Sample records for observations measurements modelling

  1. Made-to-measure modelling of observed galaxy dynamics

    NASA Astrophysics Data System (ADS)

    Bovy, Jo; Kawata, Daisuke; Hunt, Jason A. S.

    2018-01-01

    Amongst dynamical modelling techniques, the made-to-measure (M2M) method for modelling steady-state systems is amongst the most flexible, allowing non-parametric distribution functions in complex gravitational potentials to be modelled efficiently using N-body particles. Here, we propose and test various improvements to the standard M2M method for modelling observed data, illustrated using the simple set-up of a one-dimensional harmonic oscillator. We demonstrate that nuisance parameters describing the modelled system's orientation with respect to the observer - e.g. an external galaxy's inclination or the Sun's position in the Milky Way - as well as the parameters of an external gravitational field can be optimized simultaneously with the particle weights. We develop a method for sampling from the high-dimensional uncertainty distribution of the particle weights. We combine this in a Gibbs sampler with samplers for the nuisance and potential parameters to explore the uncertainty distribution of the full set of parameters. We illustrate our M2M improvements by modelling the vertical density and kinematics of F-type stars in Gaia DR1. The novel M2M method proposed here allows full probabilistic modelling of steady-state dynamical systems, allowing uncertainties on the non-parametric distribution function and on nuisance parameters to be taken into account when constraining the dark and baryonic masses of stellar systems.

  2. Solar particle events observed at Mars: dosimetry measurements and model calculations

    NASA Astrophysics Data System (ADS)

    Cleghorn, T.; Saganti, P.; Zeitlin, C.; Cucinotta, F.

    The first solar particle events from a Martian orbit are observed with the MARIE (Martian Radiation Environment Experiment) on the 2001 Mars Odyssey space -craft that is currently in orbit and collecting the mapping data of the red planet. These solar particle events observed at Mars during March and April 2002, are correlated with the GOES-8 and ACE satellite data from the same time period at Earth orbits. Dosimetry measurements for the Mars orbit from the period of March 13t h through April 29t h . Particle count rate and the corresponding dose rate enhancements were observed on March 16t h through 20t h and on April 22n d corresponding to solar particle events that were observed at Earth orbit on March 16t h through 21s t and beginning on April 21s t respectively. The model calculations with the HZETRN (High Z=atomic number and high Energy Transport) code estimated the background GCR (Galactic Cosmic Rays) dose rates. The dose rates observed by the MARIE instrument are within 10% of the model calculations. Dosimetry measurements and model calculation will be presented.

  3. A Hilbert Space Representation of Generalized Observables and Measurement Processes in the ESR Model

    NASA Astrophysics Data System (ADS)

    Sozzo, Sandro; Garola, Claudio

    2010-12-01

    The extended semantic realism ( ESR) model recently worked out by one of the authors embodies the mathematical formalism of standard (Hilbert space) quantum mechanics in a noncontextual framework, reinterpreting quantum probabilities as conditional instead of absolute. We provide here a Hilbert space representation of the generalized observables introduced by the ESR model that satisfy a simple physical condition, propose a generalization of the projection postulate, and suggest a possible mathematical description of the measurement process in terms of evolution of the compound system made up of the measured system and the measuring apparatus.

  4. The Asian Tropopause Aerosol Layer: Balloon-Borne Measurements, Satellite Observations and Modeling Approaches

    NASA Technical Reports Server (NTRS)

    Fairlie, T. D.; Vernier, J.-P.; Natarajan, M.; Deshler, Terry; Liu, H.; Wegner, T.; Baker, N.; Gadhavi, H.; Jayaraman, A.; Pandit, A.; hide

    2016-01-01

    Satellite observations and numerical modeling studies have demonstrated that the Asian Summer Monsoon (ASM) can provide a conduit for gas-phase pollutants in south Asia to reach the lower stratosphere. Now, observations from the CALIPSO satellite have revealed the Asian Tropopause Aerosol Layer (ATAL), a summertime accumulation of aerosols associated with ASM anticyclone, in the upper troposphere and lower stratosphere (UTLS). The ATAL has potential implications for regional cloud properties, climate, and chemical processes in the UTLS. Here, we show in situ measurements from balloon-borne instrumentation, aircraft and satellite observations, combined with trajectory and chemical transport model (CTM) simulations to explore the origin, composition, physical and optical properties of aerosols in the ATAL. In particular, we show balloon-based observations from our BATAL-2015 field campaign to India and Saudi Arabia in summer 2015, including in situ backscatter measurements from COBALD instruments, and some of the first observations of size and volatility of aerosols in the ATAL layer using optical particle counters (OPCs). Back trajectory calculations initialized from CALIPSO observations point to deep convection over North India as a principal source of ATAL aerosols. Available aircraft observations suggest significant sulfur and carbonaceous contributions to the ATAL, which is supported by simulations using the GEOS-Chem CTM. Source elimination studies conducted with the GEOS-Chem indicate that 80-90% of ATAL aerosols originate from south Asian sources, in contrast with some earlier studies.

  5. Model-Observation "Data Cubes" for the DOE Atmospheric Radiation Measurement Program's LES ARM Symbiotic Simulation and Observation (LASSO) Workflow

    NASA Astrophysics Data System (ADS)

    Vogelmann, A. M.; Gustafson, W. I., Jr.; Toto, T.; Endo, S.; Cheng, X.; Li, Z.; Xiao, H.

    2015-12-01

    The Department of Energy's Atmospheric Radiation Measurement (ARM) Climate Research Facilities' Large-Eddy Simulation (LES) ARM Symbiotic Simulation and Observation (LASSO) Workflow is currently being designed to provide output from routine LES to complement its extensive observations. The modeling portion of the LASSO workflow is presented by Gustafson et al., which will initially focus on shallow convection over the ARM megasite in Oklahoma, USA. This presentation describes how the LES output will be combined with observations to construct multi-dimensional and dynamically consistent "data cubes", aimed at providing the best description of the atmospheric state for use in analyses by the community. The megasite observations are used to constrain large-eddy simulations that provide a complete spatial and temporal coverage of observables and, further, the simulations also provide information on processes that cannot be observed. Statistical comparisons of model output with their observables are used to assess the quality of a given simulated realization and its associated uncertainties. A data cube is a model-observation package that provides: (1) metrics of model-observation statistical summaries to assess the simulations and the ensemble spread; (2) statistical summaries of additional model property output that cannot be or are very difficult to observe; and (3) snapshots of the 4-D simulated fields from the integration period. Searchable metrics are provided that characterize the general atmospheric state to assist users in finding cases of interest, such as categorization of daily weather conditions and their specific attributes. The data cubes will be accompanied by tools designed for easy access to cube contents from within the ARM archive and externally, the ability to compare multiple data streams within an event as well as across events, and the ability to use common grids and time sampling, where appropriate.

  6. Using satellite observations in performance evaluation for regulatory air quality modeling: Comparison with ground-level measurements

    NASA Astrophysics Data System (ADS)

    Odman, M. T.; Hu, Y.; Russell, A.; Chai, T.; Lee, P.; Shankar, U.; Boylan, J.

    2012-12-01

    Regulatory air quality modeling, such as State Implementation Plan (SIP) modeling, requires that model performance meets recommended criteria in the base-year simulations using period-specific, estimated emissions. The goal of the performance evaluation is to assure that the base-year modeling accurately captures the observed chemical reality of the lower troposphere. Any significant deficiencies found in the performance evaluation must be corrected before any base-case (with typical emissions) and future-year modeling is conducted. Corrections are usually made to model inputs such as emission-rate estimates or meteorology and/or to the air quality model itself, in modules that describe specific processes. Use of ground-level measurements that follow approved protocols is recommended for evaluating model performance. However, ground-level monitoring networks are spatially sparse, especially for particulate matter. Satellite retrievals of atmospheric chemical properties such as aerosol optical depth (AOD) provide spatial coverage that can compensate for the sparseness of ground-level measurements. Satellite retrievals can also help diagnose potential model or data problems in the upper troposphere. It is possible to achieve good model performance near the ground, but have, for example, erroneous sources or sinks in the upper troposphere that may result in misleading and unrealistic responses to emission reductions. Despite these advantages, satellite retrievals are rarely used in model performance evaluation, especially for regulatory modeling purposes, due to the high uncertainty in retrievals associated with various contaminations, for example by clouds. In this study, 2007 was selected as the base year for SIP modeling in the southeastern U.S. Performance of the Community Multiscale Air Quality (CMAQ) model, at a 12-km horizontal resolution, for this annual simulation is evaluated using both recommended ground-level measurements and non-traditional satellite

  7. Diffusion measurement from observed transverse beam echoes

    DOE PAGES

    Sen, Tanaji; Fischer, Wolfram

    2017-01-09

    For this research, we study the measurement of transverse diffusion through beam echoes. We revisit earlier observations of echoes in RHIC and apply an updated theoretical model to these measurements. We consider three possible models for the diffusion coefficient and show that only one is consistent with measured echo amplitudes and pulse widths. This model allows us to parameterize the diffusion coefficients as functions of bunch charge. We demonstrate that echoes can be used to measure diffusion much quicker than present methods and could be useful to a variety of hadron synchrotrons.

  8. Model selection for marginal regression analysis of longitudinal data with missing observations and covariate measurement error.

    PubMed

    Shen, Chung-Wei; Chen, Yi-Hau

    2015-10-01

    Missing observations and covariate measurement error commonly arise in longitudinal data. However, existing methods for model selection in marginal regression analysis of longitudinal data fail to address the potential bias resulting from these issues. To tackle this problem, we propose a new model selection criterion, the Generalized Longitudinal Information Criterion, which is based on an approximately unbiased estimator for the expected quadratic error of a considered marginal model accounting for both data missingness and covariate measurement error. The simulation results reveal that the proposed method performs quite well in the presence of missing data and covariate measurement error. On the contrary, the naive procedures without taking care of such complexity in data may perform quite poorly. The proposed method is applied to data from the Taiwan Longitudinal Study on Aging to assess the relationship of depression with health and social status in the elderly, accommodating measurement error in the covariate as well as missing observations. © The Author 2015. Published by Oxford University Press. All rights reserved. For permissions, please e-mail: journals.permissions@oup.com.

  9. Observability and synchronization of neuron models.

    PubMed

    Aguirre, Luis A; Portes, Leonardo L; Letellier, Christophe

    2017-10-01

    Observability is the property that enables recovering the state of a dynamical system from a reduced number of measured variables. In high-dimensional systems, it is therefore important to make sure that the variable recorded to perform the analysis conveys good observability of the system dynamics. The observability of a network of neuron models depends nontrivially on the observability of the node dynamics and on the topology of the network. The aim of this paper is twofold. First, to perform a study of observability using four well-known neuron models by computing three different observability coefficients. This not only clarifies observability properties of the models but also shows the limitations of applicability of each type of coefficients in the context of such models. Second, to study the emergence of phase synchronization in networks composed of neuron models. This is done performing multivariate singular spectrum analysis which, to the best of the authors' knowledge, has not been used in the context of networks of neuron models. It is shown that it is possible to detect phase synchronization: (i) without having to measure all the state variables, but only one (that provides greatest observability) from each node and (ii) without having to estimate the phase.

  10. Evaluation of Two Methods for Modeling Measurement Errors When Testing Interaction Effects with Observed Composite Scores

    ERIC Educational Resources Information Center

    Hsiao, Yu-Yu; Kwok, Oi-Man; Lai, Mark H. C.

    2018-01-01

    Path models with observed composites based on multiple items (e.g., mean or sum score of the items) are commonly used to test interaction effects. Under this practice, researchers generally assume that the observed composites are measured without errors. In this study, we reviewed and evaluated two alternative methods within the structural…

  11. Sensor Web Dynamic Measurement Techniques and Adaptive Observing Strategies

    NASA Technical Reports Server (NTRS)

    Talabac, Stephen J.

    2004-01-01

    Sensor Web observing systems may have the potential to significantly improve our ability to monitor, understand, and predict the evolution of rapidly evolving, transient, or variable environmental features and events. This improvement will come about by integrating novel data collection techniques, new or improved instruments, emerging communications technologies and protocols, sensor mark-up languages, and interoperable planning and scheduling systems. In contrast to today's observing systems, "event-driven" sensor webs will synthesize real- or near-real time measurements and information from other platforms and then react by reconfiguring the platforms and instruments to invoke new measurement modes and adaptive observation strategies. Similarly, "model-driven" sensor webs will utilize environmental prediction models to initiate targeted sensor measurements or to use a new observing strategy. The sensor web concept contrasts with today's data collection techniques and observing system operations concepts where independent measurements are made by remote sensing and in situ platforms that do not share, and therefore cannot act upon, potentially useful complementary sensor measurement data and platform state information. This presentation describes NASA's view of event-driven and model-driven Sensor Webs and highlights several research and development activities at the Goddard Space Flight Center.

  12. A new technique for measuring aerosols with moonlight observations and a sky background model

    NASA Astrophysics Data System (ADS)

    Jones, Amy; Noll, Stefan; Kausch, Wolfgang; Kimeswenger, Stefan; Szyszka, Ceszary; Unterguggenberger, Stefanie

    2014-05-01

    There have been an ample number of studies on aerosols in urban, daylight conditions, but few for remote, nocturnal aerosols. We have developed a new technique for investigating such aerosols using our sky background model and astronomical observations. With a dedicated observing proposal we have successfully tested this technique for nocturnal, remote aerosol studies. This technique relies on three requirements: (a) sky background model, (b) observations taken with scattered moonlight, and (c) spectrophotometric standard star observations for flux calibrations. The sky background model was developed for the European Southern Observatory and is optimized for the Very Large Telescope at Cerro Paranal in the Atacama desert in Chile. This is a remote location with almost no urban aerosols. It is well suited for studying remote background aerosols that are normally difficult to detect. Our sky background model has an uncertainty of around 20 percent and the scattered moonlight portion is even more accurate. The last two requirements are having astronomical observations with moonlight and of standard stars at different airmasses, all during the same night. We had a dedicated observing proposal at Cerro Paranal with the instrument X-Shooter to use as a case study for this method. X-Shooter is a medium resolution, echelle spectrograph which covers the wavelengths from 0.3 to 2.5 micrometers. We observed plain sky at six different distances (7, 13, 20, 45, 90, and 110 degrees) to the Moon for three different Moon phases (between full and half). Also direct observations of spectrophotometric standard stars were taken at two different airmasses for each night to measure the extinction curve via the Langley method. This is an ideal data set for testing this technique. The underlying assumption is that all components, other than the atmospheric conditions (specifically aerosols and airglow), can be calculated with the model for the given observing parameters. The scattered

  13. Supporting observation campaigns with high resolution modeling

    NASA Astrophysics Data System (ADS)

    Klocke, Daniel; Brueck, Matthias; Voigt, Aiko

    2017-04-01

    High resolution simulation in support of measurement campaigns offers a promising and emerging way to create large-scale context for small-scale observations of clouds and precipitation processes. As these simulation include the coupling of measured small-scale processes with the circulation, they also help to integrate the research communities from modeling and observations and allow for detailed model evaluations against dedicated observations. In connection with the measurement campaign NARVAL (August 2016 and December 2013) simulations with a grid-spacing of 2.5 km for the tropical Atlantic region (9000x3300 km), with local refinement to 1.2 km for the western part of the domain, were performed using the icosahedral non-hydrostatic (ICON) general circulation model. These simulations are again used to drive large eddy resolving simulations with the same model for selected days in the high definition clouds and precipitation for advancing climate prediction (HD(CP)2) project. The simulations are presented with the focus on selected results showing the benefit for the scientific communities doing atmospheric measurements and numerical modeling of climate and weather. Additionally, an outlook will be given on how similar simulations will support the NAWDEX measurement campaign in the North Atlantic and AC3 measurement campaign in the Arctic.

  14. A Primer on Observational Measurement.

    PubMed

    Girard, Jeffrey M; Cohn, Jeffrey F

    2016-08-01

    Observational measurement plays an integral role in a variety of scientific endeavors within biology, psychology, sociology, education, medicine, and marketing. The current article provides an interdisciplinary primer on observational measurement; in particular, it highlights recent advances in observational methodology and the challenges that accompany such growth. First, we detail the various types of instrument that can be used to standardize measurements across observers. Second, we argue for the importance of validity in observational measurement and provide several approaches to validation based on contemporary validity theory. Third, we outline the challenges currently faced by observational researchers pertaining to measurement drift, observer reactivity, reliability analysis, and time/expense. Fourth, we describe recent advances in computer-assisted measurement, fully automated measurement, and statistical data analysis. Finally, we identify several key directions for future observational research to explore.

  15. Characterizing the Asian Tropopause Aerosol Layer (ATAL) Using Satellite Observations, Balloon Measurements and a Chemical Transport Model

    NASA Technical Reports Server (NTRS)

    Fairlie, T. D.; Vernier, J.-P.; Liu, H.; Deshler, T.; Natarajan, M.; Bedka, K.; Wegner, T.; Baker, N.; Gadhavi, H.; Ratnam, M. V.; hide

    2016-01-01

    Satellite observations and numerical modeling studies have demonstrated that the Asian Summer Monsoon (ASM) provide a conduit for gas-phase pollutants in south Asia to reach the lower stratosphere. Now, observations from the CALIPSO satellite have revealed the Asian Tropopause Aerosol Layer (ATAL), a summertime accumulation of aerosols in the upper troposphere and lower stratosphere (UTLS), associated with the ASM anticyclone. The ATAL has potential implications for regional cloud properties, climate, and chemical processes in the UTLS. Here, we show in situ measurements from balloon-borne instruments, aircraft, and satellite observations, together with trajectory and chemical transport model (CTM) simulations to explore the origin, composition, physical, and optical properties of aerosols in the ATAL. In particular, we show balloon-data from our BATAL-2015 field campaign to India and Saudi Arabia in summer 2015, which includes in situ backscatter measurements from COBALD instruments, and the first observations of size and volatility of aerosols in the ATAL layer using optical particle counters (OPCs). Back trajectory calculations initialized from CALIPSO observations point to deep convection over North India as a principal source of ATAL aerosols. Available aircraft observations suggest significant sulfur and carbonaceous components to the ATAL, which is supported by simulations using the GEOS-Chem CTM. Source elimination studies conducted with the GEOS-Chem indicate that ATAL aerosols originate primary from south Asian sources, in contrast with some earlier studies.

  16. Air Modeling - Observational Meteorological Data

    EPA Pesticide Factsheets

    Observed meteorological data for use in air quality modeling consist of physical parameters that are measured directly by instrumentation, and include temperature, dew point, wind direction, wind speed, cloud cover, cloud layer(s), ceiling height,

  17. Exploring the Accretion Model of M87 and 3C 84 with the Faraday Rotation Measure Observations

    NASA Astrophysics Data System (ADS)

    Li, Ya-Ping; Yuan, Feng; Xie, Fu-Guo

    2016-10-01

    Low-luminosity active galactic nuclei (LLAGNs) are believed to be powered by an accretion-jet model, consisting of an inner advection-dominated accretion flow (ADAF), an outer truncated standard thin disk, and a jet; however, model degeneracy still exists in this framework. For example, the X-ray emission can originate from either the ADAF or the jet. The aim of the present work is to check these models with the Faraday rotation measure (RM) observations recently detected for two LLAGNs, M87 and 3C 84, in the sub-mm band. For M87, we find that the RM predicted by the model in which the X-ray emission originates from the ADAF is larger than the observed upper limit of RM by over two orders of magnitude, while the model in which the X-ray emission originates from the jet predicts a RM lower than the observed upper limit. For 3C 84, the sub-mm emission is found to be dominated by the jet component, while the Faraday screen is attributed to the ADAFs. This scenario can naturally explain the observed external origin of the RM and why the RM is found to be stable during a two-year interval although the sub-mm emission increases at the same period.

  18. Apollo 11 and 16 Soil Bi-directional Solar Reflectance Measurements, Models and LRO Diviner Observations

    NASA Astrophysics Data System (ADS)

    Foote, E. J.; Paige, D. A.; Shepard, M. K.; Johnson, J. R.; Biggar, S. F.; Greenhagen, B. T.; Allen, C.

    2010-12-01

    We have compared laboratory solar reflectance measurements of Apollo 11 and 16 soil samples to Lunar Reconnaissance Orbiter (LRO) Diviner orbital albedo measurements at the Apollo landing sites. The soil samples are two representative end member samples from the moon, low albedo lunar maria (sample 10084) and high albedo lunar highlands (sample 68810). Bidirectional reflectance distribution function (BRDF) measurements of the soil samples were conducted at Bloomsburg University (BUG) and at the University of Arizona [1,2]. We collected two different types of BUG datasets: a standard set of BRDF measurements at incidence angles of 0-60°, emission angles of 0-80°, and phase angles of 3-140°, and a high-incidence angle set of measurements along and perpendicular to the principal plane at incidence angles of 0-75° and phase angles of 3-155°. The BUG measurements generated a total of 765 data points in four different filters 450, 550, 750 and 950 nm. The Blacklab measurements were acquired at incidence angles of 60-88°, emission angles 60-82°, and phase angles of 17-93° at wavelengths of 455, 554, 699, 949nm. The BUG data were fit to two BRDF models: Hapke’s model [3] as described by Johnson et al, 2010 [4], and a simplified empirical function. The fact that both approaches can satisfactorily fit the BUG data is not unexpected, given the similarities between the functions and their input parameters, and the fact that the BRDF for dark lunar soil is dominated by the single scattering phase functions of the individual soil particles. To compare our lunar sample measurements with LRO Diviner data [5], we selected all daytime observations acquired during the first year of operation within 3 km square boxes centered at the landing sites. We compared Diviner Channel 1 (0.3 - 3 µm) Lambert albedos with model calculated Lambert albedos of the lunar samples at the same photometric angles. In general, we found good agreement between the laboratory and Diviner

  19. Observers' measurements in premetric electrodynamics: Time and radar length

    NASA Astrophysics Data System (ADS)

    Gürlebeck, Norman; Pfeifer, Christian

    2018-04-01

    The description of an observer's measurement in general relativity and the standard model of particle physics is closely related to the spacetime metric. In order to understand and interpret measurements, which test the metric structure of the spacetime, like the classical Michelson-Morley, Ives-Stilwell, Kennedy-Thorndike experiments or frequency comparison experiments in general, it is necessary to describe them in theories, which go beyond the Lorentzian metric structure. However, this requires a description of an observer's measurement without relying on a metric. We provide such a description of an observer's measurement of the fundamental quantities time and length derived from a premetric perturbation of Maxwell's electrodynamics and a discussion on how these measurements influence classical relativistic observables like time dilation and length contraction. Most importantly, we find that the modification of electrodynamics influences the measurements at two instances: the propagation of light is altered as well as the observer's proper time normalization. When interpreting the results of a specific experiment, both effects cannot be disentangled, in general, and have to be taken into account.

  20. HOx Observation and Model Comparison During INTEX-A 2004

    NASA Technical Reports Server (NTRS)

    Ren, Xinrong; Olson, Jennifer R.; Crawford, James H.; Brune, William H.; Mao, Jingqiu; Long, Robert B.; Chen, Zhong; Chen, Gao; Avery, Melody A.; Sachse, Glen W.; hide

    2008-01-01

    OH and HO2 were measured with the Airborne Tropospheric Hydrogen Oxides Sensor (ATHOS) as part of a large measurement suite from the NASA DC-8 aircraft during the Intercontinental Chemical Transport Experiment - A (INTEX-A). This mission, which was conducted mainly over North America and the western Atlantic Ocean in summer 2004, was an excellent test of atmospheric oxidation chemistry. Throughout the troposphere, observed OH was generally 0.60 of the modeled OH; below 8 km, observed HO2 was generally 0.78 of modeled HO2. If the over-prediction of tropospheric OH is not due to an instrument calibration error, then it implied less global tropospheric oxidation capacity and longer lifetimes for gases like methane and methyl chloroform than currently thought. This discrepancy falls well outside uncertainties in both the OH measurement and rate coefficients for known reactions and points to a large unknown OH loss. If the modeled OH is forced to agree with observed values by introducing of an undefined OH loss that removed HOx (HOx=OH+HO2), the observed and modeled HO2 and HO2/OH ratios are largely reconciled within the measurement uncertainty. HO2 behavior above 8 km was markedly different. The observed-to-modeled ratio correlating with NO. The observed-to-modeled HO2 ratio increased from approximately 1 at 8 km to more than approximately 2.5 at 11 km with the observed-to-modeled ratio correlating with NO. The observed-to-modeled HO2 and NO were both considerably greater than observations from previous campaigns. In addition, the observed-to-modeled HO2/OH, which is sensitive to cycling reactions between OH and HO2, increased from approximately 1.2 at 8 km to almost 4 above 11 km. In contrast to the lower atmosphere, these discrepancies above 8 km suggest a large unknown HOx source and additional reactants that cycle HOx from OH to HO2. In the continental planetary boundary layer, the OH observed-to-modeled ratio increased from 0.6 when isoprene was less than 0.1 ppbv

  1. EXPLORING THE ACCRETION MODEL OF M87 AND 3C 84 WITH THE FARADAY ROTATION MEASURE OBSERVATIONS

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Li, Ya-Ping; Yuan, Feng; Xie, Fu-Guo, E-mail: fyuan@shao.ac.cn

    2016-10-20

    Low-luminosity active galactic nuclei (LLAGNs) are believed to be powered by an accretion-jet model, consisting of an inner advection-dominated accretion flow (ADAF), an outer truncated standard thin disk, and a jet; however, model degeneracy still exists in this framework. For example, the X-ray emission can originate from either the ADAF or the jet. The aim of the present work is to check these models with the Faraday rotation measure (RM) observations recently detected for two LLAGNs, M87 and 3C 84, in the sub-mm band. For M87, we find that the RM predicted by the model in which the X-ray emissionmore » originates from the ADAF is larger than the observed upper limit of RM by over two orders of magnitude, while the model in which the X-ray emission originates from the jet predicts a RM lower than the observed upper limit. For 3C 84, the sub-mm emission is found to be dominated by the jet component, while the Faraday screen is attributed to the ADAFs. This scenario can naturally explain the observed external origin of the RM and why the RM is found to be stable during a two-year interval although the sub-mm emission increases at the same period.« less

  2. Observation and numerical modeling of tidal dune dynamics

    NASA Astrophysics Data System (ADS)

    Doré, Arnaud; Bonneton, Philippe; Marieu, Vincent; Garlan, Thierry

    2018-05-01

    Tidal sand dune dynamics is observed for two tidal cycles in the Arcachon tidal inlet, southwest France. An array of instruments is deployed to measure bathymetric and current variations along dune profiles. Based on the measurements, dune crest horizontal and vertical displacements are quantified and show important dynamics in phase with tidal currents. We observed superimposed ripples on the dune stoss side and front, migrating and changing polarity as tidal currents reverse. A 2D RANS numerical model is used to simulate the morphodynamic evolution of a flat non-cohesive sand bed submitted to a tidal current. The model reproduces the bed evolution until a field of sand bedforms is obtained that are comparable with observed superimposed ripples in terms of geometrical dimensions and dynamics. The model is then applied to simulate the dynamics of a field of large sand dunes of similar size as the dunes observed in situ. In both cases, simulation results compare well with measurements qualitatively and quantitatively. This research allows for a better understanding of tidal sand dune and superimposed ripple morphodynamics and opens new perspectives for the use of numerical models to predict their evolution.

  3. Aerosol Absorption in the Atmosphere: Perspectives from Global Model, Ground-Based Measurements, and Field Observations

    NASA Technical Reports Server (NTRS)

    Chin, Mian; Dubovik, Oleg; Holben, Brent; Torres, Omar; Anderson, Tad; Quinn, Patricia; Ginoux, Paul

    2004-01-01

    Aerosol absorption in the atmosphere poses a major uncertainty in assessing the aerosol climate effects. This uncertainty arises from the poorly quantified aerosol sources, especially black carbon emissions, and our limited knowledge of aerosol mixing state and optical properties. Here we use a global model GOCART to simulate atmospheric aerosols, including sulfate, black carbon, organic carbon, dust, and sea salt. We compare the model calculated total aerosol optical thickness, extinction, and absorption with those quantities from the ground-based sun photometer measurements from AERONET, satellite retrievals from the TOMS instrument, and field observations from ACE-Asia. We will examine the most sensitive factors in determining the aerosol absorption. and the consequences of assessing the aerosol radiative forcing and atmospheric heating associated with those factors.

  4. Aerosol Absorption in the Atmosphere: Perspectives from Global Model, Ground-Based Measurements, and Field Observations

    NASA Technical Reports Server (NTRS)

    Chin, Mian; Dubovik, Oleg; Holben, Brent; Anderson, Tad; Quinn, Patricia; Duncan, Bryan; Ginoux, Paul

    2003-01-01

    Aerosol absorption in the atmosphere poses a major uncertainty in assessing the aerosol climate effects. This uncertainty arises from the poorly quantified aerosol sources, especially black carbon emissions, and our limited knowledge of aerosol mixing state and optical properties. Here we use a global model GOCART to simulate atmospheric aerosols, including sulfate, black carbon, organic carbon, dust, and sea salt. We compare the model calculated total aerosol optical thickness, extinction, and absorption with those quantities from the ground-based sun photometer measurements from AERONET at several different wavelengths and the field observations from ACE-Asia. We will examine what are the most sensitive factors in determining the aerosol absorption, and the consequences of assessing the aerosol radiative forcing and atmospheric heating associated with those factors.

  5. Aerosol Absorption in the Atmosphere: Perspectives from Global Model, Ground-Based Measurements, and Field Observations

    NASA Technical Reports Server (NTRS)

    Chin, Main; Dubovik, Oleg; Holben, Brent; Anderson, Tad; Quinn, Patricia; Duncan, Bryan; Ginoux, Paul

    2004-01-01

    Aerosol absorption in the atmosphere poses a major uncertainty in assessing the aerosol climate effects. This uncertainty arises from the poorly quantified aerosol sources, especially black carbon emissions, and our limited knowledge of aerosol mixing state and optical properties. Here we use a global model GOCART to simulate atmospheric aerosols, including sulfate, black carbon, organic carbon, dust, and sea salt. We compare the model calculated total aerosol optical thickness, extinction, and absorption with those quantities from the ground-based sun photometer measurements from AERONET at several different wavelengths and the field observations from ACE-Asia. We will examine the most sensitive factors in determining the aerosol absorption, and the consequences of assessing the aerosol radiative forcing and atmospheric heating associated with those factors.

  6. Constraining Cosmological Models with Different Observations

    NASA Astrophysics Data System (ADS)

    Wei, J. J.

    2016-07-01

    With the observations of Type Ia supernovae (SNe Ia), scientists discovered that the Universe is experiencing an accelerated expansion, and then revealed the existence of dark energy in 1998. Since the amazing discovery, cosmology has became a hot topic in the physical research field. Cosmology is a subject that strongly depends on the astronomical observations. Therefore, constraining different cosmological models with all kinds of observations is one of the most important research works in the modern cosmology. The goal of this thesis is to investigate cosmology using the latest observations. The observations include SNe Ia, Type Ic Super Luminous supernovae (SLSN Ic), Gamma-ray bursts (GRBs), angular diameter distance of galaxy cluster, strong gravitational lensing, and age measurements of old passive galaxies, etc. In Chapter 1, we briefly review the research background of cosmology, and introduce some cosmological models. Then we summarize the progress on cosmology from all kinds of observations in more details. In Chapter 2, we present the results of our studies on the supernova cosmology. The main difficulty with the use of SNe Ia as standard candles is that one must optimize three or four nuisance parameters characterizing SN luminosities simultaneously with the parameters of an expansion model of the Universe. We have confirmed that one should optimize all of the parameters by carrying out the method of maximum likelihood estimation in any situation where the parameters include an unknown intrinsic dispersion. The commonly used method, which estimates the dispersion by requiring the reduced χ^{2} to equal unity, does not take into account all possible variances among the parameters. We carry out such a comparison of the standard ΛCDM cosmology and the R_{h}=ct Universe using the SN Legacy Survey sample of 252 SN events, and show that each model fits its individually reduced data very well. Moreover, it is quite evident that SLSNe Ic may be useful

  7. Observers' Agreement on Measurements in Fiberoptic Endoscopic Evaluation of Swallowing.

    PubMed

    Pilz, Walmari; Vanbelle, Sophie; Kremer, Bernd; van Hooren, Michel R; van Becelaere, Tine; Roodenburg, Nel; Baijens, Laura W J

    2016-04-01

    This study analyzed the effect that dysphagia etiology, different observers, and bolus consistency might have on the level of agreement for measurements in FEES images reached by independent versus consensus panel rating. Sixty patients were included and divided into two groups according to dysphagia etiology: neurological or head and neck oncological. All patients underwent standardized FEES examination using thin and thick liquid consistencies. Two observers scored the same exams, first independently and then in a consensus panel. Four ordinal FEES variables were analyzed. Statistical analysis was performed using a linear weighted kappa coefficient and Bayesian multilevel model. Intra- and interobserver agreement on FEES measurements ranged from 0.76 to 0.93 and from 0.61 to 0.88, respectively. Dysphagia etiology did not influence observers' agreement level. However, bolus consistency resulted in decreased interobserver agreement for all measured FEES variables during thin liquid swallows. When rating on the consensus panel, the observers deviated considerably from the scores they had previously given on the independent rating task. Observer agreement on measurements in FEES exams was influenced by bolus consistency, not by dysphagia etiology. Therefore, observer agreement on FEES measurements should be analyzed by taking bolus consistency into account, as it might affect the interpretation of the outcome. Identifying factors that might influence agreement levels could lead to better understanding of the rating process and assist in developing a more precise measurement scale that would ensure higher levels of observer agreement for measurements in FEES exams.

  8. Solar particle events observed at Mars: dosimetry measurements and model calculations.

    PubMed

    Cleghorn, Timothy F; Saganti, Premkumar B; Zeitlin, Cary J; Cucinotta, Francis A

    2004-01-01

    During the period from March 13, 2002 to mid-September, 2002, six solar particle events (SPE) were observed by the MARIE instrument onboard the Odyssey Spacecraft in Martian Orbit. These events were observed also by the GOES 8 satellite in Earth orbit, and thus represent the first time that the same SPE have been observed at these separate locations. The characteristics of these SPE are examined, given that the active regions of the solar disc from which the event originated can usually be identified. The dose rates at Martian orbit are calculated, both for the galactic and solar components of the ionizing particle radiation environment. The dose rates due to galactic cosmic rays (GCR) agree well with the HZETRN model calculations. Published by Elsevier Ltd on behalf of COSPAR.

  9. Solar particle events observed at Mars: dosimetry measurements and model calculations

    NASA Technical Reports Server (NTRS)

    Cleghorn, Timothy F.; Saganti, Premkumar B.; Zeitlin, Cary J.; Cucinotta, Francis A.

    2004-01-01

    During the period from March 13, 2002 to mid-September, 2002, six solar particle events (SPE) were observed by the MARIE instrument onboard the Odyssey Spacecraft in Martian Orbit. These events were observed also by the GOES 8 satellite in Earth orbit, and thus represent the first time that the same SPE have been observed at these separate locations. The characteristics of these SPE are examined, given that the active regions of the solar disc from which the event originated can usually be identified. The dose rates at Martian orbit are calculated, both for the galactic and solar components of the ionizing particle radiation environment. The dose rates due to galactic cosmic rays (GCR) agree well with the HZETRN model calculations. Published by Elsevier Ltd on behalf of COSPAR.

  10. Observations and Measurements Design Patterns within INSPIRE

    NASA Astrophysics Data System (ADS)

    Schleidt, K.; Cox, S.; Grellet, S.; Lowe, D.; Lutz, M.; Portele, C.; Sarretta, A.; Ventouras, S.

    2012-04-01

    Several INSPIRE spatial data themes have been specified so that their scope, in addition to classical geographic information, includes measured, modelled or simulated data. The FprEN ISO 19156 standard on Observations and Measurements (O&M) was designed for the explicit purpose of creating application schemas for such data, and thus shall be used in INSPIRE as a basis for developing data models for these themes. The following INSPIRE themes have identified O&M as integrally relevant to their thematic domain and are including elements of O&M in their data specifications: • Geology • Oceanographic geographical features • Atmospheric conditions and Meteorological geographical features • Environmental monitoring facilities • Soil In addition to these themes, several other INSPIRE themes have been identified to which observational information, while not at the core of the data specification, is relevant. Some examples of this are the INSPIRE theme "Species distribution", where primary occurrence data could be provided together with the aggregate distribution, as well as "Industrial and production facilities", where the provision of emissions data on such facilities would be useful for various environmental reporting obligations. While the O&M standard provides a generic framework for the provision of measurement data, it is also kept very abstract, and there are many ways of implementing the core structures in specific application schemas. In order to assure the consistent application of the O&M classes and properties across different INSPIRE themes, a cross-thematic working group on the use of O&M in INSPIRE has been convened. This group has analysed the requirements towards O&M within INSPIRE, identified the types of O&M design patterns required in INSPIRE and developed both additional classes identified as necessary within INSPIRE as well as guidelines detailing how this standard is to be used within INSPIRE. Some examples for these additional classes are

  11. Evaluation of Multiclass Model Observers in PET LROC Studies

    NASA Astrophysics Data System (ADS)

    Gifford, H. C.; Kinahan, P. E.; Lartizien, C.; King, M. A.

    2007-02-01

    A localization ROC (LROC) study was conducted to evaluate nonprewhitening matched-filter (NPW) and channelized NPW (CNPW) versions of a multiclass model observer as predictors of human tumor-detection performance with PET images. Target localization is explicitly performed by these model observers. Tumors were placed in the liver, lungs, and background soft tissue of a mathematical phantom, and the data simulation modeled a full-3D acquisition mode. Reconstructions were performed with the FORE+AWOSEM algorithm. The LROC study measured observer performance with 2D images consisting of either coronal, sagittal, or transverse views of the same set of cases. Versions of the CNPW observer based on two previously published difference-of-Gaussian channel models demonstrated good quantitative agreement with human observers. One interpretation of these results treats the CNPW observer as a channelized Hotelling observer with implicit internal noise

  12. Detecting influential observations in nonlinear regression modeling of groundwater flow

    USGS Publications Warehouse

    Yager, Richard M.

    1998-01-01

    Nonlinear regression is used to estimate optimal parameter values in models of groundwater flow to ensure that differences between predicted and observed heads and flows do not result from nonoptimal parameter values. Parameter estimates can be affected, however, by observations that disproportionately influence the regression, such as outliers that exert undue leverage on the objective function. Certain statistics developed for linear regression can be used to detect influential observations in nonlinear regression if the models are approximately linear. This paper discusses the application of Cook's D, which measures the effect of omitting a single observation on a set of estimated parameter values, and the statistical parameter DFBETAS, which quantifies the influence of an observation on each parameter. The influence statistics were used to (1) identify the influential observations in the calibration of a three-dimensional, groundwater flow model of a fractured-rock aquifer through nonlinear regression, and (2) quantify the effect of omitting influential observations on the set of estimated parameter values. Comparison of the spatial distribution of Cook's D with plots of model sensitivity shows that influential observations correspond to areas where the model heads are most sensitive to certain parameters, and where predicted groundwater flow rates are largest. Five of the six discharge observations were identified as influential, indicating that reliable measurements of groundwater flow rates are valuable data in model calibration. DFBETAS are computed and examined for an alternative model of the aquifer system to identify a parameterization error in the model design that resulted in overestimation of the effect of anisotropy on horizontal hydraulic conductivity.

  13. Multiple Indicators, Multiple Causes Measurement Error Models

    PubMed Central

    Tekwe, Carmen D.; Carter, Randy L.; Cullings, Harry M.; Carroll, Raymond J.

    2014-01-01

    Multiple Indicators, Multiple Causes Models (MIMIC) are often employed by researchers studying the effects of an unobservable latent variable on a set of outcomes, when causes of the latent variable are observed. There are times however when the causes of the latent variable are not observed because measurements of the causal variable are contaminated by measurement error. The objectives of this paper are: (1) to develop a novel model by extending the classical linear MIMIC model to allow both Berkson and classical measurement errors, defining the MIMIC measurement error (MIMIC ME) model, (2) to develop likelihood based estimation methods for the MIMIC ME model, (3) to apply the newly defined MIMIC ME model to atomic bomb survivor data to study the impact of dyslipidemia and radiation dose on the physical manifestations of dyslipidemia. As a by-product of our work, we also obtain a data-driven estimate of the variance of the classical measurement error associated with an estimate of the amount of radiation dose received by atomic bomb survivors at the time of their exposure. PMID:24962535

  14. Models and Measurements Intercomparison 2

    NASA Technical Reports Server (NTRS)

    Park, Jae H. (Editor); Ko, Malcolm K. W. (Editor); Jackman, Charles H. (Editor); Plumb, R. Alan (Editor); Kaye, Jack A. (Editor); Sage, Karen H. (Editor)

    1999-01-01

    Models and Measurement Intercomparison II (MM II) summarizes the intercomparison of results from model simulations and observations of stratospheric species. Representatives from twenty-three modeling groups using twenty-nine models participated in these MM II exercises between 1996 and 1999. Twelve of the models were two- dimensional zonal-mean models while seventeen were three-dimensional models. This was an international effort as seven were from outside the United States. Six transport experiments and five chemistry experiments were designed for various models. Models participating in the transport experiments performed simulations of chemically inert tracers providing diagnostics for transport. The chemistry experiments involved simulating the distributions of chemically active trace cases including ozone. The model run conditions for dynamics and chemistry were prescribed in order to minimize the factors that caused differences in the models. The report includes a critical review of the results by the participants and a discussion of the causes of differences between modeled and measured results as well as between results from different models, A sizable effort went into preparation of the database of the observations. This included a new climatology for ozone. The report should help in evaluating the results from various predictive models for assessing humankind perturbations of the stratosphere.

  15. Testing Viable f(T) Models with Current Observations

    NASA Astrophysics Data System (ADS)

    Xu, Bing; Yu, Hongwei; Wu, Puxun

    2018-03-01

    We perform observational tests on the f(T) gravity with the BAO data (including the BOSS DR 12 galaxy sample, the DR12 Lyα-Forests measurement, the new eBOSS DR14 quasar sample, the 6dFGS, and the SDSS), the CMB distance priors from the Planck 2015, the SNIa data from the joint light-curve analysis, the latest H(z) data, and the local value of the Hubble constant. Six different f(T) models are investigated. Furthermore, the ΛCDM is also considered. All models are compared by using the Akaike information criteria (AIC) and the Bayesian information criteria (BIC). Our results show that the ΛCDM remains to be the most favored model by current observations. However, there are also the Hubble constant tension between the Planck measurements and the local Universe observations and the tension between the CMB data and the H(z) data in the ΛCDM. For f(T) models considered in this paper, half, which can reduce to the ΛCDM, have values of {{χ }2}\\min smaller than that of the ΛCDM and can relieve the tensions existing in the ΛCDM. However, they are punished slightly by the BIC due to one extra parameter. Two of six f(T) models, in which the crossing of the phantom divide line can be realized for the equation of state of the effective dark energy and this crossing is shown in this paper to be favored by current observations, are punished by the information criteria. In addition, we find that the logarithmic f(T) model is excluded by cosmological observations.

  16. Research Opportunities from Emerging Atmospheric Observing and Modeling Capabilities.

    NASA Astrophysics Data System (ADS)

    Dabberdt, Walter F.; Schlatter, Thomas W.

    1996-02-01

    The Second Prospectus Development Team (PDT-2) of the U.S. Weather Research Program was charged with identifying research opportunities that are best matched to emerging operational and experimental measurement and modeling methods. The overarching recommendation of PDT-2 is that inputs for weather forecast models can best be obtained through the use of composite observing systems together with adaptive (or targeted) observing strategies employing both in situ and remote sensing. Optimal observing systems and strategies are best determined through a three-part process: observing system simulation experiments, pilot field measurement programs, and model-assisted data sensitivity experiments. Furthermore, the mesoscale research community needs easy and timely access to the new operational and research datasets in a form that can readily be reformatted into existing software packages for analysis and display. The value of these data is diminished to the extent that they remain inaccessible.The composite observing system of the future must combine synoptic observations, routine mobile observations, and targeted observations, as the current or forecast situation dictates. High costs demand fuller exploitation of commercial aircraft, meteorological and navigation [Global Positioning System (GPS)] satellites, and Doppler radar. Single observing systems must be assessed in the context of a composite system that provides complementary information. Maintenance of the current North American rawinsonde network is critical for progress in both research-oriented and operational weather forecasting.Adaptive sampling strategies are designed to improve large-scale and regional weather prediction but they will also improve diagnosis and prediction of flash flooding, air pollution, forest fire management, and other environmental emergencies. Adaptive measurements can be made by piloted or unpiloted aircraft. Rawinsondes can be launched and satellites can be programmed to make

  17. Measurement of evapotranspiration with combined reflective and thermal infrared radiance observations

    NASA Technical Reports Server (NTRS)

    Hope, Allen S.

    1993-01-01

    The broad goal of the research summarized in this report was 'To facilitate the evaluation of regional evapotranspiration (ET) through the combined use of solar reflective and thermal infrared radiance observations.' The specific objectives stated by Goward and Hope (1986) were to: (1) investigate the nature of the relationship between surface temperature (T(sub S)) and the normalized difference vegetation index (NDVI) and develop an understanding of this relationship in terms of energy exchange processes, particularly latent flux heat (LE); (2) develop procedures to estimate large area LE using combined T(sub S) and NDVI observations obtained from AVHRR data; and (3) determine whether measurements derived from satellite observations relate directly to measurements made at the surface or from aircraft platforms. Both empirical and modeling studies were used to develop an understanding of the T(sub S)-NDVI relationship. Most of the modeling was based on the Tergra model as originally proposed by Goward. This model, and modified versions developed in this project, simulates the flows of water and energy in the soil-plant-atmosphere system using meteorological, soil and vegetation inputs. Model outputs are the diurnal course of soil moisture, T(sub S), LE and the other individual components of the surface energy balance.

  18. Development of an observational measure of healthcare worker hand-hygiene behaviour: the hand-hygiene observation tool (HHOT).

    PubMed

    McAteer, J; Stone, S; Fuller, C; Charlett, A; Cookson, B; Slade, R; Michie, S

    2008-03-01

    Previous observational measures of healthcare worker (HCW) hand-hygiene behaviour (HHB) fail to provide adequate standard operating procedures (SOPs), accounts of inter-rater agreement testing or evidence of sensitivity to change. This study reports the development of an observational tool in a way that addresses these deficiencies. Observational categories were developed systematically, guided by a clinical guideline, previous measures and pilot hand-hygiene behaviour observations (HHOs). The measure, a simpler version of the Geneva tool, consists of HHOs (before and after low-risk, high-risk or unobserved contact), HHBs (soap, alcohol hand rub, no action, unknown), and type of HCW. Inter-observer agreement for each category was assessed by observation of 298 HHOs and HHBs by two independent observers on acute elderly and intensive care units. Raw agreement (%) and Kappa were 77% and 0.68 for HHB; 83% and 0.77 for HHO; and 90% and 0.77 for HCW. Inter-observer agreement for overall compliance of a group of HCWs was assessed by observation of 1191 HHOs and HHBs by two pairs of independent observers. Overall agreement was good (intraclass correlation coefficient = 0.79). Sensitivity to change was examined by autoregressive time-series modelling of longitudinal observations for 8 months on the intensive therapy unit during an Acinetobacter baumannii outbreak and subsequent strengthening of infection control measures. Sensitivity to change was demonstrated by a rise in compliance from 80 to 98% with an odds ratio of increased compliance of 7.00 (95% confidence interval: 4.02-12.2) P < 0.001.

  19. Advancing an Information Model for Environmental Observations

    NASA Astrophysics Data System (ADS)

    Horsburgh, J. S.; Aufdenkampe, A. K.; Hooper, R. P.; Lehnert, K. A.; Schreuders, K.; Tarboton, D. G.; Valentine, D. W.; Zaslavsky, I.

    2011-12-01

    Observational data are fundamental to hydrology and water resources, and the way they are organized, described, and shared either enables or inhibits the analyses that can be performed using the data. The CUAHSI Hydrologic Information System (HIS) project is developing cyberinfrastructure to support hydrologic science by enabling better access to hydrologic data. HIS is composed of three major components. HydroServer is a software stack for publishing time series of hydrologic observations on the Internet as well as geospatial data using standards-based web feature, map, and coverage services. HydroCatalog is a centralized facility that catalogs the data contents of individual HydroServers and enables search across them. HydroDesktop is a client application that interacts with both HydroServer and HydroCatalog to discover, download, visualize, and analyze hydrologic observations published on one or more HydroServers. All three components of HIS are founded upon an information model for hydrologic observations at stationary points that specifies the entities, relationships, constraints, rules, and semantics of the observational data and that supports its data services. Within this information model, observations are described with ancillary information (metadata) about the observations to allow them to be unambiguously interpreted and used, and to provide traceable heritage from raw measurements to useable information. Physical implementations of this information model include the Observations Data Model (ODM) for storing hydrologic observations, Water Markup Language (WaterML) for encoding observations for transmittal over the Internet, the HydroCatalog metadata catalog database, and the HydroDesktop data cache database. The CUAHSI HIS and this information model have now been in use for several years, and have been deployed across many different academic institutions as well as across several national agency data repositories. Additionally, components of the HIS

  20. Multiple indicators, multiple causes measurement error models

    DOE PAGES

    Tekwe, Carmen D.; Carter, Randy L.; Cullings, Harry M.; ...

    2014-06-25

    Multiple indicators, multiple causes (MIMIC) models are often employed by researchers studying the effects of an unobservable latent variable on a set of outcomes, when causes of the latent variable are observed. There are times, however, when the causes of the latent variable are not observed because measurements of the causal variable are contaminated by measurement error. The objectives of this study are as follows: (i) to develop a novel model by extending the classical linear MIMIC model to allow both Berkson and classical measurement errors, defining the MIMIC measurement error (MIMIC ME) model; (ii) to develop likelihood-based estimation methodsmore » for the MIMIC ME model; and (iii) to apply the newly defined MIMIC ME model to atomic bomb survivor data to study the impact of dyslipidemia and radiation dose on the physical manifestations of dyslipidemia. Finally, as a by-product of our work, we also obtain a data-driven estimate of the variance of the classical measurement error associated with an estimate of the amount of radiation dose received by atomic bomb survivors at the time of their exposure.« less

  1. Multiple indicators, multiple causes measurement error models

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Tekwe, Carmen D.; Carter, Randy L.; Cullings, Harry M.

    Multiple indicators, multiple causes (MIMIC) models are often employed by researchers studying the effects of an unobservable latent variable on a set of outcomes, when causes of the latent variable are observed. There are times, however, when the causes of the latent variable are not observed because measurements of the causal variable are contaminated by measurement error. The objectives of this study are as follows: (i) to develop a novel model by extending the classical linear MIMIC model to allow both Berkson and classical measurement errors, defining the MIMIC measurement error (MIMIC ME) model; (ii) to develop likelihood-based estimation methodsmore » for the MIMIC ME model; and (iii) to apply the newly defined MIMIC ME model to atomic bomb survivor data to study the impact of dyslipidemia and radiation dose on the physical manifestations of dyslipidemia. Finally, as a by-product of our work, we also obtain a data-driven estimate of the variance of the classical measurement error associated with an estimate of the amount of radiation dose received by atomic bomb survivors at the time of their exposure.« less

  2. Improving Snow Modeling by Assimilating Observational Data Collected by Citizen Scientists

    NASA Astrophysics Data System (ADS)

    Crumley, R. L.; Hill, D. F.; Arendt, A. A.; Wikstrom Jones, K.; Wolken, G. J.; Setiawan, L.

    2017-12-01

    Modeling seasonal snow pack in alpine environments includes a multiplicity of challenges caused by a lack of spatially extensive and temporally continuous observational datasets. This is partially due to the difficulty of collecting measurements in harsh, remote environments where extreme gradients in topography exist, accompanied by large model domains and inclement weather. Engaging snow enthusiasts, snow professionals, and community members to participate in the process of data collection may address some of these challenges. In this study, we use SnowModel to estimate seasonal snow water equivalence (SWE) in the Thompson Pass region of Alaska while incorporating snow depth measurements collected by citizen scientists. We develop a modeling approach to assimilate hundreds of snow depth measurements from participants in the Community Snow Observations (CSO) project (www.communitysnowobs.org). The CSO project includes a mobile application where participants record and submit geo-located snow depth measurements while working and recreating in the study area. These snow depth measurements are randomly located within the model grid at irregular time intervals over the span of four months in the 2017 water year. This snow depth observation dataset is converted into a SWE dataset by employing an empirically-based, bulk density and SWE estimation method. We then assimilate this data using SnowAssim, a sub-model within SnowModel, to constrain the SWE output by the observed data. Multiple model runs are designed to represent an array of output scenarios during the assimilation process. An effort to present model output uncertainties is included, as well as quantification of the pre- and post-assimilation divergence in modeled SWE. Early results reveal pre-assimilation SWE estimations are consistently greater than the post-assimilation estimations, and the magnitude of divergence increases throughout the snow pack evolution period. This research has implications beyond the

  3. Assessing Model Fitting of Megamaser Disks with Simulated Observations

    NASA Astrophysics Data System (ADS)

    Han, Jiwon; Braatz, James; Pesce, Dominic

    2018-01-01

    The Megamaser Cosmology Project (MCP) measures the Hubble Constant by determining distances to galaxies with observations of 22 GHz H20 megamasers. The megamasers arise in the circumnuclear accretion disks of active galaxies. In this research, we aim to improve the estimation of systematic errors in MCP measurements. Currently, the MCP fits a disk model to the observed maser data with a Markov Chain Monte Carlo (MCMC) code. The disk model is described by up to 14 global parameters, including up to 6 that describe the disk warping. We first assess the model by generating synthetic datasets in which the locations and dynamics of the maser spots are exactly known, and fitting the model to these data. By doing so, we can also test the effects of unmodeled substructure on the estimated uncertainties. Furthermore, in order to gain better understanding of the physics behind accretion disk warping, we develop a physics-driven model for the warp and test it with the MCMC approach.

  4. A Comparison Between Gravity Wave Momentum Fluxes in Observations and Climate Models

    NASA Technical Reports Server (NTRS)

    Geller, Marvin A.; Alexadner, M. Joan; Love, Peter T.; Bacmeister, Julio; Ern, Manfred; Hertzog, Albert; Manzini, Elisa; Preusse, Peter; Sato, Kaoru; Scaife, Adam A.; hide

    2013-01-01

    For the first time, a formal comparison is made between gravity wave momentum fluxes in models and those derived from observations. Although gravity waves occur over a wide range of spatial and temporal scales, the focus of this paper is on scales that are being parameterized in present climate models, sub-1000-km scales. Only observational methods that permit derivation of gravity wave momentum fluxes over large geographical areas are discussed, and these are from satellite temperature measurements, constant-density long-duration balloons, and high-vertical-resolution radiosonde data. The models discussed include two high-resolution models in which gravity waves are explicitly modeled, Kanto and the Community Atmosphere Model, version 5 (CAM5), and three climate models containing gravity wave parameterizations,MAECHAM5, Hadley Centre Global Environmental Model 3 (HadGEM3), and the Goddard Institute for Space Studies (GISS) model. Measurements generally show similar flux magnitudes as in models, except that the fluxes derived from satellite measurements fall off more rapidly with height. This is likely due to limitations on the observable range of wavelengths, although other factors may contribute. When one accounts for this more rapid fall off, the geographical distribution of the fluxes from observations and models compare reasonably well, except for certain features that depend on the specification of the nonorographic gravity wave source functions in the climate models. For instance, both the observed fluxes and those in the high-resolution models are very small at summer high latitudes, but this is not the case for some of the climate models. This comparison between gravity wave fluxes from climate models, high-resolution models, and fluxes derived from observations indicates that such efforts offer a promising path toward improving specifications of gravity wave sources in climate models.

  5. Surface Runoff Estimation Using SMOS Observations, Rain-gauge Measurements and Satellite Precipitation Estimations. Comparison with Model Predictions

    NASA Astrophysics Data System (ADS)

    Garcia Leal, Julio A.; Lopez-Baeza, Ernesto; Khodayar, Samiro; Estrela, Teodoro; Fidalgo, Arancha; Gabaldo, Onofre; Kuligowski, Robert; Herrera, Eddy

    Surface runoff is defined as the amount of water that originates from precipitation, does not infiltrates due to soil saturation and therefore circulates over the surface. A good estimation of runoff is useful for the design of draining systems, structures for flood control and soil utilisation. For runoff estimation there exist different methods such as (i) rational method, (ii) isochrone method, (iii) triangular hydrograph, (iv) non-dimensional SCS hydrograph, (v) Temez hydrograph, (vi) kinematic wave model, represented by the dynamics and kinematics equations for a uniforme precipitation regime, and (vii) SCS-CN (Soil Conservation Service Curve Number) model. This work presents a way of estimating precipitation runoff through the SCS-CN model, using SMOS (Soil Moisture and Ocean Salinity) mission soil moisture observations and rain-gauge measurements, as well as satellite precipitation estimations. The area of application is the Jucar River Basin Authority area where one of the objectives is to develop the SCS-CN model in a spatial way. The results were compared to simulations performed with the 7-km COSMO-CLM (COnsortium for Small-scale MOdelling, COSMO model in CLimate Mode) model. The use of SMOS soil moisture as input to the COSMO-CLM model will certainly improve model simulations.

  6. Characterisation of Central-African emissions based on MAX-DOAS measurements, satellite observations and model simulations over Bujumbura, Burundi.

    NASA Astrophysics Data System (ADS)

    Gielen, Clio; Hendrick, Francois; Pinardi, Gaia; De Smedt, Isabelle; Stavrakou, Trissevgeni; Yu, Huan; Fayt, Caroline; Hermans, Christian; Bauwens, Maité; Ndenzako, Eugene; Nzohabonayo, Pierre; Akimana, Rachel; Niyonzima, Sébastien; Müller, Jean-Francois; Van Roozendael, Michel

    2016-04-01

    Central Africa is known for its strong biogenic, pyrogenic, and to a lesser extent anthropogenic emissions. Satellite observations of species like nitrogen dioxide (NO2) and formaldehyde (HCHO), as well as inverse modelling results have shown that there are large uncertainties associated with the emissions in this region. There is thus a need for additional measurements, especially from the ground, in order to better characterise the biomass-burning and biogenic products emitted in this area. We present MAX-DOAS measurements of NO2, HCHO, and aerosols performed in Central Africa, in the city of Bujumbura, Burundi (3°S, 29°E, 850m). A MAX-DOAS instrument has been operating at this location by BIRA-IASB since late 2013. Aerosol-extinction and trace-gases vertical profiles are retrieved by applying the optimal-estimation-based profiling tool bePRO to the measured O4, NO2 and HCHO slant-column densities. The MAX-DOAS vertical columns and profiles are used for investigating the diurnal and seasonal cycles of NO2, HCHO, and aerosols. Regarding the aerosols, the retrieved AODs are compared to co-located AERONET sun photometer measurements for verification purpose, while in the case of NO2 and HCHO, the MAX-DOAS vertical columns and profiles are used for validating GOME-2 and OMI satellite observations. To characterise the biomass-burning and biogenic emissions in the Bujumbura region, the trace gases and aerosol MAX-DOAS retrievals are used in combination to MODIS fire counts/radiative-power and GOME-2/OMI NO2 and HCHO satellite data, as well as simulations from the NOAA backward trajectory model HYSPLIT. First results show that HCHO seasonal variation around local noon is driven by the alternation of rain and dry periods, the latter being associated with intense biomass-burning agricultural activities and forest fires in the south/south-east and transport from this region to Bujumbura. In contrast, NO2 is seen to depend mainly on local emissions close to the city, due

  7. Ozone distributions over southern Lake Michigan: comparisons between ferry-based observations, shoreline-based DOAS observations and model forecasts

    NASA Astrophysics Data System (ADS)

    Cleary, P. A.; Fuhrman, N.; Schulz, L.; Schafer, J.; Fillingham, J.; Bootsma, H.; McQueen, J.; Tang, Y.; Langel, T.; McKeen, S.; Williams, E. J.; Brown, S. S.

    2015-05-01

    Air quality forecast models typically predict large summertime ozone abundances over water relative to land in the Great Lakes region. While each state bordering Lake Michigan has dedicated monitoring systems, offshore measurements have been sparse, mainly executed through specific short-term campaigns. This study examines ozone abundances over Lake Michigan as measured on the Lake Express ferry, by shoreline differential optical absorption spectroscopy (DOAS) observations in southeastern Wisconsin and as predicted by the Community Multiscale Air Quality (CMAQ) model. From 2008 to 2009 measurements of O3, SO2, NO2 and formaldehyde were made in the summertime by DOAS at a shoreline site in Kenosha, WI. From 2008 to 2010 measurements of ambient ozone were conducted on the Lake Express, a high-speed ferry that travels between Milwaukee, WI, and Muskegon, MI, up to six times daily from spring to fall. Ferry ozone observations over Lake Michigan were an average of 3.8 ppb higher than those measured at shoreline in Kenosha, with little dependence on position of the ferry or temperature and with greatest differences during evening and night. Concurrent 1-48 h forecasts from the CMAQ model in the upper Midwestern region surrounding Lake Michigan were compared to ferry ozone measurements, shoreline DOAS measurements and Environmental Protection Agency (EPA) station measurements. The bias of the model O3 forecast was computed and evaluated with respect to ferry-based measurements. Trends in the bias with respect to location and time of day were explored showing non-uniformity in model bias over the lake. Model ozone bias was consistently high over the lake in comparison to land-based measurements, with highest biases for 25-48 h after initialization.

  8. Correlation between human observer performance and model observer performance in differential phase contrast CT

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Li, Ke; Garrett, John; Chen, Guang-Hong

    2013-11-15

    Purpose: With the recently expanding interest and developments in x-ray differential phase contrast CT (DPC-CT), the evaluation of its task-specific detection performance and comparison with the corresponding absorption CT under a given radiation dose constraint become increasingly important. Mathematical model observers are often used to quantify the performance of imaging systems, but their correlations with actual human observers need to be confirmed for each new imaging method. This work is an investigation of the effects of stochastic DPC-CT noise on the correlation of detection performance between model and human observers with signal-known-exactly (SKE) detection tasks.Methods: The detectabilities of different objectsmore » (five disks with different diameters and two breast lesion masses) embedded in an experimental DPC-CT noise background were assessed using both model and human observers. The detectability of the disk and lesion signals was then measured using five types of model observers including the prewhitening ideal observer, the nonprewhitening (NPW) observer, the nonprewhitening observer with eye filter and internal noise (NPWEi), the prewhitening observer with eye filter and internal noise (PWEi), and the channelized Hotelling observer (CHO). The same objects were also evaluated by four human observers using the two-alternative forced choice method. The results from the model observer experiment were quantitatively compared to the human observer results to assess the correlation between the two techniques.Results: The contrast-to-detail (CD) curve generated by the human observers for the disk-detection experiments shows that the required contrast to detect a disk is inversely proportional to the square root of the disk size. Based on the CD curves, the ideal and NPW observers tend to systematically overestimate the performance of the human observers. The NPWEi and PWEi observers did not predict human performance well either, as the slopes of

  9. Observation model and parameter partials for the JPL geodetic GPS modeling software GPSOMC

    NASA Technical Reports Server (NTRS)

    Sovers, O. J.; Border, J. S.

    1988-01-01

    The physical models employed in GPSOMC and the modeling module of the GIPSY software system developed at JPL for analysis of geodetic Global Positioning Satellite (GPS) measurements are described. Details of the various contributions to range and phase observables are given, as well as the partial derivatives of the observed quantities with respect to model parameters. A glossary of parameters is provided to enable persons doing data analysis to identify quantities in the current report with their counterparts in the computer programs. There are no basic model revisions, with the exceptions of an improved ocean loading model and some new options for handling clock parametrization. Such misprints as were discovered were corrected. Further revisions include modeling improvements and assurances that the model description is in accord with the current software.

  10. Understanding Rasch Measurement: Rasch Models Overview.

    ERIC Educational Resources Information Center

    Wright, Benjamin D.; Mok, Magdalena

    2000-01-01

    Presents an overview of Rasch measurement models that begins with a conceptualization of continuous experiences often captured as discrete observations. Discusses the mathematical properties of the Rasch family of models that allow the transformation of discrete deterministic counts into continuous probabilistic abstractions. Also discusses six of…

  11. Nighttime reactive nitrogen measurements from stratospheric infrared thermal emission observations

    NASA Technical Reports Server (NTRS)

    Abbas, Mian M.; Kunde, Virgil G.; Brasunas, J. C.; Herman, J. R.; Massie, Steven T.

    1991-01-01

    IR thermal emission spectra of the earth's atmosphere in the 700-2000/cm region were obtained with a cryogenically cooled high-resolution interferometer spectrometer on a balloon flight from Palestine, Texas, on September 15-16, 1986. The observations exhibit spectral features of a number of stratospheric constituents, including important species of the reactive nitrogen family. An analysis of the observed data for simultaneously measured vertical distributions of O3, H2O, N2O, NO2, N2O5, HNO3, and ClONO2 is presented. These measurements permit the first direct determination of the nighttime total reactive nitrogen concentrations, and the partitioning of the important elements of the NO(x) family. Comparisons of the total reactive nitrogen budget are made with the measurements by the ATMOS experiment and with the predictions of one-dimensional and two-dimensional photochemical models.

  12. Observations and Models of Highly Intermittent Phytoplankton Distributions

    PubMed Central

    Mandal, Sandip; Locke, Christopher; Tanaka, Mamoru; Yamazaki, Hidekatsu

    2014-01-01

    The measurement of phytoplankton distributions in ocean ecosystems provides the basis for elucidating the influences of physical processes on plankton dynamics. Technological advances allow for measurement of phytoplankton data to greater resolution, displaying high spatial variability. In conventional mathematical models, the mean value of the measured variable is approximated to compare with the model output, which may misinterpret the reality of planktonic ecosystems, especially at the microscale level. To consider intermittency of variables, in this work, a new modelling approach to the planktonic ecosystem is applied, called the closure approach. Using this approach for a simple nutrient-phytoplankton model, we have shown how consideration of the fluctuating parts of model variables can affect system dynamics. Also, we have found a critical value of variance of overall fluctuating terms below which the conventional non-closure model and the mean value from the closure model exhibit the same result. This analysis gives an idea about the importance of the fluctuating parts of model variables and about when to use the closure approach. Comparisons of plot of mean versus standard deviation of phytoplankton at different depths, obtained using this new approach with real observations, give this approach good conformity. PMID:24787740

  13. A Community Data Model for Hydrologic Observations

    NASA Astrophysics Data System (ADS)

    Tarboton, D. G.; Horsburgh, J. S.; Zaslavsky, I.; Maidment, D. R.; Valentine, D.; Jennings, B.

    2006-12-01

    The CUAHSI Hydrologic Information System project is developing information technology infrastructure to support hydrologic science. Hydrologic information science involves the description of hydrologic environments in a consistent way, using data models for information integration. This includes a hydrologic observations data model for the storage and retrieval of hydrologic observations in a relational database designed to facilitate data retrieval for integrated analysis of information collected by multiple investigators. It is intended to provide a standard format to facilitate the effective sharing of information between investigators and to facilitate analysis of information within a single study area or hydrologic observatory, or across hydrologic observatories and regions. The observations data model is designed to store hydrologic observations and sufficient ancillary information (metadata) about the observations to allow them to be unambiguously interpreted and used and provide traceable heritage from raw measurements to usable information. The design is based on the premise that a relational database at the single observation level is most effective for providing querying capability and cross dimension data retrieval and analysis. This premise is being tested through the implementation of a prototype hydrologic observations database, and the development of web services for the retrieval of data from and ingestion of data into the database. These web services hosted by the San Diego Supercomputer center make data in the database accessible both through a Hydrologic Data Access System portal and directly from applications software such as Excel, Matlab and ArcGIS that have Standard Object Access Protocol (SOAP) capability. This paper will (1) describe the data model; (2) demonstrate the capability for representing diverse data in the same database; (3) demonstrate the use of the database from applications software for the performance of hydrologic analysis

  14. Thermal Infrared Observations and Thermophysical Modeling of Phobos

    NASA Astrophysics Data System (ADS)

    Smith, Nathan Michael; Edwards, Christopher Scott; Mommert, Michael; Trilling, David E.; Glotch, Timothy

    2016-10-01

    Mars-observing spacecraft have the opportunity to study Phobos from Mars orbit, and have produced a sizeable record of observations using the same instruments that study the surface of the planet below. However, these observations are generally infrequent, acquired only rarely over each mission.Using observations gathered by Mars Global Surveyor's (MGS) Thermal Emission Spectrometer (TES), we can investigate the fine layer of regolith that blankets Phobos' surface, and characterize its thermal properties. The mapping of TES observations to footprints on the Phobos surface has not previously been undertaken, and must consider the orientation and position of both MGS and Phobos, and TES's pointing mirror angle. Approximately 300 fully resolved observations are available covering a significant subset of Phobos' surface at a variety of scales.The properties of the surface regolith, such as grain size, density, and conductivity, determine how heat is absorbed, transferred, and reradiated to space. Thermophysical modeling allows us to simulate these processes and predict, for a given set of assumed parameters, how the observed thermal infrared spectra will appear. By comparing models to observations, we can constrain the properties of the regolith, and see how these properties vary with depth, as well as regionally across the Phobos surface. These constraints are key to understanding how Phobos formed and evolved over time, which in turn will help inform the environment and processes that shaped the solar system as a whole.We have developed a thermophysical model of Phobos adapted from a model used for unresolved observations of asteroids. The model has been modified to integrate thermal infrared flux across each observed portion of Phobos. It will include the effects of surface roughness, temperature-dependent conductivity, as well as radiation scattered, reflected, and thermally emitted from the Martian surface. Combining this model with the newly-mapped TES

  15. Study on individual stochastic model of GNSS observations for precise kinematic applications

    NASA Astrophysics Data System (ADS)

    Próchniewicz, Dominik; Szpunar, Ryszard

    2015-04-01

    The proper definition of mathematical positioning model, which is defined by functional and stochastic models, is a prerequisite to obtain the optimal estimation of unknown parameters. Especially important in this definition is realistic modelling of stochastic properties of observations, which are more receiver-dependent and time-varying than deterministic relationships. This is particularly true with respect to precise kinematic applications which are characterized by weakening model strength. In this case, incorrect or simplified definition of stochastic model causes that the performance of ambiguity resolution and accuracy of position estimation can be limited. In this study we investigate the methods of describing the measurement noise of GNSS observations and its impact to derive precise kinematic positioning model. In particular stochastic modelling of individual components of the variance-covariance matrix of observation noise performed using observations from a very short baseline and laboratory GNSS signal generator, is analyzed. Experimental test results indicate that the utilizing the individual stochastic model of observations including elevation dependency and cross-correlation instead of assumption that raw measurements are independent with the same variance improves the performance of ambiguity resolution as well as rover positioning accuracy. This shows that the proposed stochastic assessment method could be a important part in complex calibration procedure of GNSS equipment.

  16. "Evaluations" of Observables Versus Measurements in Quantum Theory

    NASA Astrophysics Data System (ADS)

    Nisticò, Giuseppe; Sestito, Angela

    2016-03-01

    In Quantum Physics there are circumstances where the direct measurement of a given observable encounters difficulties; in some of these cases, however, its value can be "evaluated", i.e. it can be inferred by measuring another observable characterized by perfect correlation with the observable of interest. Though an evaluation is often interpreted as a measurement of the evaluated observable, we prove that the two concepts cannot be identified in Quantum Physics, because the identification yields contradictions. Then, we establish the conceptual status of evaluations in Quantum Theory and how they are related to measurements.

  17. Probing quantumness with joint continuous measurements of non-commuting qubit observables

    NASA Astrophysics Data System (ADS)

    Garcia-Pintos, Luis Pedro; Dressel, Justin

    In this talk we consider continuous weak measurements as a means to probe foundational issues in quantum mechanics. We consider the simultaneous monitoring of two noncommuting observables-as recently implemented by the Siddiqi group at UC Berkeley. Contrary to naive expectation, the output of such experiment can be used to simultaneously track the approximate observable dynamics. Despite this seeming realism, we also show that the readouts violate macrorealistic Leggett-Garg inequalities for arbitrarily short temporal correlations, and that the derived inequalities are manifestly violated even in the absence of Hamiltonian evolution. Such violations should indicate the failure of at least one postulate of macrorealism: either physical quantities do not have well defined values at all times, or the measurement process itself disturbs what is being measured. Despite this macrorealism violation, we construct a realistic, but epistemically restricted, model that perfectly emulates both the qubit evolution and the observed noisy signals, thus also emulating the violations.

  18. Observation model and parameter partials for the JPL geodetic (GPS) modeling software 'GPSOMC'

    NASA Technical Reports Server (NTRS)

    Sovers, O. J.

    1990-01-01

    The physical models employed in GPSOMC, the modeling module of the GIPSY software system developed at JPL for analysis of geodetic Global Positioning Satellite (GPS) measurements are described. Details of the various contributions to range and phase observables are given, as well as the partial derivatives of the observed quantities with respect to model parameters. A glossary of parameters is provided to enable persons doing data analysis to identify quantities with their counterparts in the computer programs. The present version is the second revision of the original document which it supersedes. The modeling is expanded to provide the option of using Cartesian station coordinates; parameters for the time rates of change of universal time and polar motion are also introduced.

  19. NACP Synthesis: Evaluating modeled carbon state and flux variables against multiple observational constraints (Invited)

    NASA Astrophysics Data System (ADS)

    Thornton, P. E.; Nacp Site Synthesis Participants

    2010-12-01

    The North American Carbon Program (NACP) synthesis effort includes an extensive intercomparison of modeled and observed ecosystem states and fluxes preformed with multiple models across multiple sites. The participating models span a range of complexity and intended application, while the participating sites cover a broad range of natural and managed ecosystems in North America, from the subtropics to arctic tundra, and coastal to interior climates. A unique characteristic of this collaborative effort is that multiple independent observations are available at all sites: fluxes are measured with the eddy covariance technique, and standard biometric and field sampling methods provide estimates of standing stock and annual production in multiple categories. In addition, multiple modeling approaches are employed to make predictions at each site, varying, for example, in the use of diagnostic vs. prognostic leaf area index. Given multiple independent observational constraints and multiple classes of model, we evaluate the internal consistency of observations at each site, and use this information to extend previously derived estimates of uncertainty in the flux observations. Model results are then compared with all available observations and models are ranked according to their consistency with each type of observation (high frequency flux measurement, carbon stock, annual production). We demonstrate a range of internal consistency across the sites, and show that some models which perform well against one observational metric perform poorly against others. We use this analysis to construct a hypothesis for combining eddy covariance, biometrics, and other standard physiological and ecological measurements which, as data collection proceeded over several years, would present an increasingly challenging target for next generation models.

  20. Observed and modelled “chemical weather” during ESCOMPTE

    NASA Astrophysics Data System (ADS)

    Dufour, A.; Amodei, M.; Ancellet, G.; Peuch, V.-H.

    2005-03-01

    The new MOdèle de Chimie Atmosphérique à Grande Echelle (MOCAGE) three-dimensional multiscale chemistry and transport model (CTM) has been applied to study heavy pollution episodes observed during the ESCOMPTE experiment. The model considers the troposphere and lower stratosphere, and allows the possibility of zooming from the planetary scale down to the regional scale over limited area subdomains. Like this, it generates its own time-dependent chemical boundary conditions in the vertical and in the horizontal. This paper focuses on the evaluation and quantification of uncertainties related to chemical and transport modelling during two intensive observing periods, IOP2 and IOP4 (June 20-26 and July 10-14, 2001, respectively). Simulations are compared to the database of four-dimensional observations, which includes ground-based sites and aircraft measurements, radiosoundings, and quasi-continuous measurements of ozone by LIDARs. Thereby, the observed and modelled day-to-day variabilities in air composition both at the surface and in the vertical have been assessed. Then, three sensitivity studies are conducted concerning boundary conditions, accuracy of the emission dataset, and representation of chemistry. Firstly, to go further in the analysis of chemical boundary conditions, results from the standard grid nesting set-up and altered configurations, relying on climatologies, are compared. Along with other recent studies, this work advocates the systematic coupling of limited-area models with global CTMs, even for regional air quality studies or forecasts. Next, we evaluate the benefits of using the detailed high-resolution emissions inventory of ESCOMPTE: improvements are noticeable both on ozone reactivity and on the concentrations of various species of the ozone photochemical cycle especially primary ones. Finally, we provide some insights on the comparison of two simulations differing only by the parameterisation of chemistry and using two state

  1. Inter-observer variability in fetal biometric measurements.

    PubMed

    Kilani, Rami; Aleyadeh, Wesam; Atieleh, Luay Abu; Al Suleimat, Abdul Mane; Khadra, Maysa; Hawamdeh, Hassan M

    2018-02-01

    To evaluate inter-observer variability and reproducibility of ultrasound measurements for fetal biometric parameters. A prospective cohort study was implemented in two tertiary care hospitals in Amman, Jordan; Prince Hamza Hospital and Albashir Hospital. 192 women with a singleton pregnancy at a gestational age of 18-36 weeks were the participants in the study. Transabdominal scans for fetal biometric parameter measurement were performed on study participants from the period of November 2014 to March 2015. Women who agreed to participate in the study were administered two ultrasound scans for head circumference, abdominal circumference and femur length. The correlation coefficient was calculated. Bland-Altman plots were used to analyze the degree of measurement agreement between observers. Limits of agreement ± 2 SD for the differences in fetal biometry measurements in proportions of the mean of the measurements were derived. Main outcome measures examine the reproducibility of fetal biometric measurements by different observers. High inter-observer inter-class correlation coefficient (ICC) was found for femur length (0.990) and abdominal circumference (0.996) where Bland-Altman plots showed high degrees of agreement. The highest degrees of agreement were noted in the measurement of abdominal circumference followed by head circumference. The lowest degree of agreement was found for femur length measurement. We used a paired-sample t-test and found that the mean difference between duplicate measurements was not significant (P > 0.05). Biometric fetal parameter measurements may be reproducible by different operators in the clinical setting with similar results. Fetal head circumference, abdominal circumference and femur length were highly reproducible. Large organized studies are needed to ensure accurate fetal measurements due to the important clinical implications of inaccurate measurements. Copyright © 2018. Published by Elsevier B.V.

  2. Geocoronal Balmer α line profile observations and forward-model analysis

    NASA Astrophysics Data System (ADS)

    Mierkiewicz, E. J.; Bishop, J.; Roesler, F. L.; Nossal, S. M.

    2006-05-01

    High spectral resolution geocoronal Balmer α line profile observations from Pine Bluff Observatory (PBO) are presented in the context of forward-model analysis. Because Balmer series column emissions depend significantly on multiple scattering, retrieval of hydrogen parameters of general aeronomic interest from these observations (e.g., the hydrogen column abundance) currently requires a forward modeling approach. This capability is provided by the resonance radiative transfer code LYAO_RT. We have recently developed a parametric data-model comparison search procedure employing an extensive grid of radiative transport model input parameters (defining a 6-dimensional parameter space) to map-out bounds for feasible forward model retrieved atomic hydrogen density distributions. We applied this technique to same-night (March, 2000) ground-based Balmer α data from PBO and geocoronal Lyman β measurements from the Espectrógrafo Ultravioleta extremo para la Radiación Difusa (EURD) instrument on the Spanish satellite MINISAT-1 (provided by J.F. Gómez and C. Morales of the Laboratorio de Astrofisica Espacial y Física Fundamental, INTA, Madrid, Spain) in order to investigate the modeling constraints imposed by two sets of independent geocoronal intensity measurements, both of which rely on astronomical calibration methods. In this poster we explore extending this analysis to the line profile information also contained in the March 2000 PBO Balmer α data set. In general, a decrease in the Doppler width of the Balmer α emission with shadow altitude is a persistent feature in every night of PBO observations in which a wide range of shadow altitudes are observed. Preliminary applications of the LYAO_RT code, which includes the ability to output Doppler line profiles for both the singly and multiply scattered contributions to the Balmer α emission line, displays good qualitative agreement with regard to geocoronal Doppler width trends observed from PBO. Model-data Balmer

  3. Modeling a Full Coronal Loop Observed with Hinode EIS and SDO AIA

    NASA Technical Reports Server (NTRS)

    Alexander, Caroline; Winebarger, Amy R.

    2015-01-01

    Physical parameters measured from an observation of a coronal loop from Gupta et al. (2015) using Hinode/EIS and SDO/AIA were used as input for the hydrodynamic, impulsively heating NRLSOFM 1-­d loop model. The model was run at eight different energy inputs and used the measured quantities of temperature (0.73 MK), density (10(sup 8.5)cm(sup -3) and minimum loop lifetime to evaluate the success of the model at recreating the observations. The loop was measured by us to have an unprojected length of 236 Mm and was assumed to be almost perpendicular to the solar surface (tilt of 3.5 degrees) and have a dipolar geometry. Our results show that two of our simulation runs (with input energies of 0.01 and 0.02 ergs cm(sup -3)S(sup -1) closely match the temperature/density combination exhibited by the loop observation. However, our simulated loops only remain in the temperature sensitive region of the Mg 278.4 Angstrom filter for 500 and 800 seconds respectively which is less than the 1200 seconds that the loop is observed for with EIS in order to make the temperature/density measurements over the loop's entire length. This leads us to conclude that impulsive heating of a single loop is not complex enough to explain this observation. Additional steady heating or a collection of additional strands along the line-­of-­sight would help to align the simulation with the observation.

  4. Predicting detection performance with model observers: Fourier domain or spatial domain?

    PubMed

    Chen, Baiyu; Yu, Lifeng; Leng, Shuai; Kofler, James; Favazza, Christopher; Vrieze, Thomas; McCollough, Cynthia

    2016-02-27

    The use of Fourier domain model observer is challenged by iterative reconstruction (IR), because IR algorithms are nonlinear and IR images have noise texture different from that of FBP. A modified Fourier domain model observer, which incorporates nonlinear noise and resolution properties, has been proposed for IR and needs to be validated with human detection performance. On the other hand, the spatial domain model observer is theoretically applicable to IR, but more computationally intensive than the Fourier domain method. The purpose of this study is to compare the modified Fourier domain model observer to the spatial domain model observer with both FBP and IR images, using human detection performance as the gold standard. A phantom with inserts of various low contrast levels and sizes was repeatedly scanned 100 times on a third-generation, dual-source CT scanner at 5 dose levels and reconstructed using FBP and IR algorithms. The human detection performance of the inserts was measured via a 2-alternative-forced-choice (2AFC) test. In addition, two model observer performances were calculated, including a Fourier domain non-prewhitening model observer and a spatial domain channelized Hotelling observer. The performance of these two mode observers was compared in terms of how well they correlated with human observer performance. Our results demonstrated that the spatial domain model observer correlated well with human observers across various dose levels, object contrast levels, and object sizes. The Fourier domain observer correlated well with human observers using FBP images, but overestimated the detection performance using IR images.

  5. Predicting detection performance with model observers: Fourier domain or spatial domain?

    PubMed Central

    Chen, Baiyu; Yu, Lifeng; Leng, Shuai; Kofler, James; Favazza, Christopher; Vrieze, Thomas; McCollough, Cynthia

    2016-01-01

    The use of Fourier domain model observer is challenged by iterative reconstruction (IR), because IR algorithms are nonlinear and IR images have noise texture different from that of FBP. A modified Fourier domain model observer, which incorporates nonlinear noise and resolution properties, has been proposed for IR and needs to be validated with human detection performance. On the other hand, the spatial domain model observer is theoretically applicable to IR, but more computationally intensive than the Fourier domain method. The purpose of this study is to compare the modified Fourier domain model observer to the spatial domain model observer with both FBP and IR images, using human detection performance as the gold standard. A phantom with inserts of various low contrast levels and sizes was repeatedly scanned 100 times on a third-generation, dual-source CT scanner at 5 dose levels and reconstructed using FBP and IR algorithms. The human detection performance of the inserts was measured via a 2-alternative-forced-choice (2AFC) test. In addition, two model observer performances were calculated, including a Fourier domain non-prewhitening model observer and a spatial domain channelized Hotelling observer. The performance of these two mode observers was compared in terms of how well they correlated with human observer performance. Our results demonstrated that the spatial domain model observer correlated well with human observers across various dose levels, object contrast levels, and object sizes. The Fourier domain observer correlated well with human observers using FBP images, but overestimated the detection performance using IR images. PMID:27239086

  6. Individual Colorimetric Observer Model

    PubMed Central

    Asano, Yuta; Fairchild, Mark D.; Blondé, Laurent

    2016-01-01

    This study proposes a vision model for individual colorimetric observers. The proposed model can be beneficial in many color-critical applications such as color grading and soft proofing to assess ranges of color matches instead of a single average match. We extended the CIE 2006 physiological observer by adding eight additional physiological parameters to model individual color-normal observers. These eight parameters control lens pigment density, macular pigment density, optical densities of L-, M-, and S-cone photopigments, and λmax shifts of L-, M-, and S-cone photopigments. By identifying the variability of each physiological parameter, the model can simulate color matching functions among color-normal populations using Monte Carlo simulation. The variabilities of the eight parameters were identified through two steps. In the first step, extensive reviews of past studies were performed for each of the eight physiological parameters. In the second step, the obtained variabilities were scaled to fit a color matching dataset. The model was validated using three different datasets: traditional color matching, applied color matching, and Rayleigh matches. PMID:26862905

  7. Observational attachment theory-based parenting measures predict children's attachment narratives independently from social learning theory-based measures.

    PubMed

    Matias, Carla; O'Connor, Thomas G; Futh, Annabel; Scott, Stephen

    2014-01-01

    Conceptually and methodologically distinct models exist for assessing quality of parent-child relationships, but few studies contrast competing models or assess their overlap in predicting developmental outcomes. Using observational methodology, the current study examined the distinctiveness of attachment theory-based and social learning theory-based measures of parenting in predicting two key measures of child adjustment: security of attachment narratives and social acceptance in peer nominations. A total of 113 5-6-year-old children from ethnically diverse families participated. Parent-child relationships were rated using standard paradigms. Measures derived from attachment theory included sensitive responding and mutuality; measures derived from social learning theory included positive attending, directives, and criticism. Child outcomes were independently-rated attachment narrative representations and peer nominations. Results indicated that Attachment theory-based and Social Learning theory-based measures were modestly correlated; nonetheless, parent-child mutuality predicted secure child attachment narratives independently of social learning theory-based measures; in contrast, criticism predicted peer-nominated fighting independently of attachment theory-based measures. In young children, there is some evidence that attachment theory-based measures may be particularly predictive of attachment narratives; however, no single model of measuring parent-child relationships is likely to best predict multiple developmental outcomes. Assessment in research and applied settings may benefit from integration of different theoretical and methodological paradigms.

  8. Observations and Modelling of the Zodiacal Light

    NASA Astrophysics Data System (ADS)

    Kelsall, T.

    1994-12-01

    The DIRBE instrument on the COBE satellite performed a full-sky survey in ten bands covering the spectral range from 1.25 to 240 microns, and made measurements of the polarization from 1.25 to 3.5 microns. These observations provide a wealth of data on the radiations from the interplanetary dust cloud (IPD). The presentation covers the observations, the model-independent findings, and the results from the extensive efforts of the DIRBE team to model the IPD. Emphasis is placed on describing the importance of correctly accounting for the IPD contribution to the observed-sky signal for the purpose of detecting the cosmic infrared background. (*) The NASA/Goddard Space Flight Center (GSFC) is responsible for the design, development, and operation of the COBE mission. GSFC is also responsible for the development of the analysis software and for the production of the mission data sets. Scientific guidance is provided by the COBE Science Working Group. The COBE program is supported by the Astrophysics Division of NASA's Office of Space Science.

  9. Uncertainty modelling of real-time observation of a moving object: photogrammetric measurements

    NASA Astrophysics Data System (ADS)

    Ulrich, Thomas

    2015-04-01

    Photogrametric systems are widely used in the field of industrial metrology to measure kinematic tasks such as tracking robot movements. In order to assess spatiotemporal deviations of a kinematic movement, it is crucial to have a reliable uncertainty of the kinematic measurements. Common methods to evaluate the uncertainty in kinematic measurements include approximations specified by the manufactures, various analytical adjustment methods and Kalman filters. Here a hybrid system estimator in conjunction with a kinematic measurement model is applied. This method can be applied to processes which include various types of kinematic behaviour, constant velocity, variable acceleration or variable turn rates. Additionally, it has been shown that the approach is in accordance with GUM (Guide to the Expression of Uncertainty in Measurement). The approach is compared to the Kalman filter using simulated data to achieve an overall error calculation. Furthermore, the new approach is used for the analysis of a rotating system as this system has both a constant and a variable turn rate. As the new approach reduces overshoots it is more appropriate for analysing kinematic processes than the Kalman filter. In comparison with the manufacturer’s approximations, the new approach takes account of kinematic behaviour, with an improved description of the real measurement process. Therefore, this approach is well-suited to the analysis of kinematic processes with unknown changes in kinematic behaviour.

  10. Observed Parenting Behavior with Teens: Measurement Invariance and Predictive Validity Across Race

    PubMed Central

    Skinner, Martie L.; MacKenzie, Elizabeth P.; Haggerty, Kevin P.; Hill, Karl G.; Roberson, Kendra C.

    2011-01-01

    Previous reports supporting measurement equality between European American and African American families have often focused on self-reported risk factors or observed parent behavior with young children. This study examines equality of measurement of observer ratings of parenting behavior with adolescents during structured tasks; mean levels of observed parenting; and predictive validity of teen self-reports of antisocial behaviors and beliefs using a sample of 163 African American and 168 European American families. Multiple-group confirmatory factor analyses supported measurement invariance across ethnic groups for 4 measures of observed parenting behavior: prosocial rewards, psychological costs, antisocial rewards, and problem solving. Some mean-level differences were found: African American parents exhibited lower levels of prosocial rewards, higher levels of psychological costs, and lower problem solving when compared to European Americans. No significant mean difference was found in rewards for antisocial behavior. Multigroup structural equation models suggested comparable relationships across race (predictive validity) between parenting constructs and youth antisocial constructs (i.e., drug initiation, positive drug attitudes, antisocial attitudes, problem behaviors) in all but one of the tested relationships. This study adds to existing evidence that family-based interventions targeting parenting behaviors can be generalized to African American families. PMID:21787057

  11. Modeling COSMO-SkyMed measurements of precipitating clouds over the sea using simultaneous weather radar observations

    NASA Astrophysics Data System (ADS)

    Roberto, N.; Baldini, L.; Facheris, L.; Chandrasekar, V.

    2014-07-01

    Several satellite missions employing X-band synthetic aperture radar (SAR) have been activated to provide high-resolution images of normalized radar cross-sections (NRCS) on land and ocean for numerous applications. Rainfall and wind affect the sea surface roughness and consequently the NRCS from the combined effects of corrugation due to impinging raindrops and surface wind. X-band frequencies are sensitive to precipitation: intense convective cells result in irregularly bright and dark patches in SAR images, masking changes in surface NRCS. Several works have modeled SAR images of intense precipitation over land; less adequately investigated is the precipitation effect over the sea surface. These images are analyzed in this study by modeling both the scattering and attenuation of radiation by hydrometeors in the rain cells and the NRCS surface changes using weather radar precipitation estimates as input. The reconstruction of X-band SAR returns in precipitating clouds is obtained by the joint utilization of volume reflectivity and attenuation, the latter estimated by coupling ground-based radar measurements and an electromagnetic model to predict the sea surface NRCS. Radar signatures of rain cells were investigated using X-band SAR images collected from the COSMO-SkyMed constellation of the Italian Space Agency. Two case studies were analyzed. The first occurred over the sea off the coast of Louisiana (USA) in summer 2010 with COSMO-SkyMed (CSK®) ScanSar mode monitoring of the Deepwater Horizon oil spill. Simultaneously, the NEXRAD S-band Doppler radar (KLIX) located in New Orleans was scanning the same portion of ocean. The second case study occurred in Liguria (Italy) on November 4, 2011, during an extraordinary flood event. The same events were observed by the Bric della Croce C-band dual polarization radar located close to Turin (Italy). The polarimetric capability of the ground radars utilized allows discrimination of the composition of the precipitation

  12. Performance characteristics of a visual-search human-model observer with sparse PET image data

    NASA Astrophysics Data System (ADS)

    Gifford, Howard C.

    2012-02-01

    As predictors of human performance in detection-localization tasks, statistical model observers can have problems with tasks that are primarily limited by target contrast or structural noise. Model observers with a visual-search (VS) framework may provide a more reliable alternative. This framework provides for an initial holistic search that identifies suspicious locations for analysis by a statistical observer. A basic VS observer for emission tomography focuses on hot "blobs" in an image and uses a channelized nonprewhitening (CNPW) observer for analysis. In [1], we investigated this model for a contrast-limited task with SPECT images; herein, a statisticalnoise limited task involving PET images is considered. An LROC study used 2D image slices with liver, lung and soft-tissue tumors. Human and model observers read the images in coronal, sagittal and transverse display formats. The study thus measured the detectability of tumors in a given organ as a function of display format. The model observers were applied under several task variants that tested their response to structural noise both at the organ boundaries alone and over the organs as a whole. As measured by correlation with the human data, the VS observer outperformed the CNPW scanning observer.

  13. Measurement and modeling of moist processes

    NASA Technical Reports Server (NTRS)

    Cotton, William; Starr, David; Mitchell, Kenneth; Fleming, Rex; Koch, Steve; Smith, Steve; Mailhot, Jocelyn; Perkey, Don; Tripoli, Greg

    1993-01-01

    The keynote talk summarized five years of work simulating observed mesoscale convective systems with the RAMS (Regional Atmospheric Modeling System) model. Excellent results are obtained when simulating squall line or other convective systems that are strongly forced by fronts or other lifting mechanisms. Less highly forced systems are difficult to model. The next topic in this colloquium was measurement of water vapor and other constituents of the hydrologic cycle. Impressive accuracy was shown measuring water vapor with both the airborne DIAL (Differential Absorption Lidar) system and the the ground-based Raman Lidar. NMC's plans for initializing land water hydrology in mesoscale models was presented before water vapor measurement concepts for GCIP were discussed. The subject of using satellite data to provide mesoscale moisture and wind analyses was next. Recent activities in modeling of moist processes in mesoscale systems was reported on. These modeling activities at the Canadian Atmospheric Environment Service (AES) used a hydrostatic, variable-resolution grid model. Next the spatial resolution effects of moisture budgets was discussed; in particular, the effects of temporal resolution on heat and moisture budgets for cumulus parameterization. The conclusion of this colloquium was on modeling scale interaction processes.

  14. Observational Constraints for Modeling Diffuse Molecular Clouds

    NASA Astrophysics Data System (ADS)

    Federman, S. R.

    2014-02-01

    Ground-based and space-borne observations of diffuse molecular clouds suggest a number of areas where further improvements to modeling efforts is warranted. I will highlight those that have the widest applicability. The range in CO fractionation caused by selective isotope photodissociation, in particular the large 12C16O/13C16O ratios observed toward stars in Ophiuchus, is not reproduced well by current models. Our ongoing laboratory measurements of oscillator strengths and predissociation rates for Rydberg transitions in CO isotopologues may help clarify the situtation. The CH+ abundance continues to draw attention. Small scale structure seen toward ζ Per may provide additional constraints on the possible synthesis routes. The connection between results from optical transitions and those from radio and sub-millimeter wave transitions requires further effort. A study of OH+ and OH toward background stars reveals that these species favor different environments. This brings to focus the need to model each cloud along the line of sight separately, and to allow the physical conditions to vary within an individual cloud, in order to gain further insight into the chemistry. Now that an extensive set of data on molecular excitation is available, the models should seek to reproduce these data to place further constraints on the modeling results.

  15. PARAGON: A Systematic, Integrated Approach to Aerosol Observation and Modeling

    NASA Technical Reports Server (NTRS)

    Diner, David J.; Kahn, Ralph A.; Braverman, Amy J.; Davies, Roger; Martonchik, John V.; Menzies, Robert T.; Ackerman, Thomas P.; Seinfeld, John H.; Anderson, Theodore L.; Charlson, Robert J.; hide

    2004-01-01

    Aerosols are generated and transformed by myriad processes operating across many spatial and temporal scales. Evaluation of climate models and their sensitivity to changes, such as in greenhouse gas abundances, requires quantifying natural and anthropogenic aerosol forcings and accounting for other critical factors, such as cloud feedbacks. High accuracy is required to provide sufficient sensitivity to perturbations, separate anthropogenic from natural influences, and develop confidence in inputs used to support policy decisions. Although many relevant data sources exist, the aerosol research community does not currently have the means to combine these diverse inputs into an integrated data set for maximum scientific benefit. Bridging observational gaps, adapting to evolving measurements, and establishing rigorous protocols for evaluating models are necessary, while simultaneously maintaining consistent, well understood accuracies. The Progressive Aerosol Retrieval and Assimilation Global Observing Network (PARAGON) concept represents a systematic, integrated approach to global aerosol Characterization, bringing together modern measurement and modeling techniques, geospatial statistics methodologies, and high-performance information technologies to provide the machinery necessary for achieving a comprehensive understanding of how aerosol physical, chemical, and radiative processes impact the Earth system. We outline a framework for integrating and interpreting observations and models and establishing an accurate, consistent and cohesive long-term data record.

  16. Optimal observation network design for conceptual model discrimination and uncertainty reduction

    NASA Astrophysics Data System (ADS)

    Pham, Hai V.; Tsai, Frank T.-C.

    2016-02-01

    This study expands the Box-Hill discrimination function to design an optimal observation network to discriminate conceptual models and, in turn, identify a most favored model. The Box-Hill discrimination function measures the expected decrease in Shannon entropy (for model identification) before and after the optimal design for one additional observation. This study modifies the discrimination function to account for multiple future observations that are assumed spatiotemporally independent and Gaussian-distributed. Bayesian model averaging (BMA) is used to incorporate existing observation data and quantify future observation uncertainty arising from conceptual and parametric uncertainties in the discrimination function. In addition, the BMA method is adopted to predict future observation data in a statistical sense. The design goal is to find optimal locations and least data via maximizing the Box-Hill discrimination function value subject to a posterior model probability threshold. The optimal observation network design is illustrated using a groundwater study in Baton Rouge, Louisiana, to collect additional groundwater heads from USGS wells. The sources of uncertainty creating multiple groundwater models are geological architecture, boundary condition, and fault permeability architecture. Impacts of considering homoscedastic and heteroscedastic future observation data and the sources of uncertainties on potential observation areas are analyzed. Results show that heteroscedasticity should be considered in the design procedure to account for various sources of future observation uncertainty. After the optimal design is obtained and the corresponding data are collected for model updating, total variances of head predictions can be significantly reduced by identifying a model with a superior posterior model probability.

  17. Modelling Ground Based X- and Ku-Band Observations of Tundra Snow

    NASA Astrophysics Data System (ADS)

    Kasurak, A.; King, J. M.; Kelly, R. E.

    2012-12-01

    As part of a radar-based remote sensing field experiment in Churchill, Manitoba ground based Ku- and X-band scatterometers were deployed to observe changing tundra snowpack conditions from November 2010 to March 2011. The research is part of the validation effort for the Cold Regions Hydrology High-resolution Observatory (CoReH2O) mission, a candidate in the European Space Agency's Earth Explorer program. This paper focuses on the local validation of the semi-empirical radiative transfer (sRT) model proposed for use in snow property retrievals as part of the CoReH2O mission. In this validation experiment, sRT was executed in the forward mode, simulating backscatter to assess the ability of the model. This is a necessary precursor to any inversion attempt. Two experiments are considered, both conducted in a hummocky tundra environment with shallow snow cover. In both cases, scatterometer observations were acquired over a field of view of approximately 10 by 20 meters. In the first experiment, radar observations were made of a snow field and then repeated after the snow had been removed. A ground-based scanning LiDAR system was used to characterize the spatial variability of snow depth through measurements of the snow and ground surface. Snow properties were determined in the field of view from two snow pits, 12 density core measurements, and Magnaprobe snow depth measurements. In the second experiment, a site was non-destructively observed from November through March, with snow properties measured out-of-scene, to characterize the snow evolution response. The model results from sRT fit the form of the observations from the two scatterometer field experiments but do not capture the backscatter magnitude. A constant offset for the season of 5 dB for X-band co- and cross-polarization response was required to match observations, in addition to a 3 dB X- and Ku-band co-polarization offset after the 6th of December. To explain these offsets, it is recognized that the two

  18. Assimilating uncertain, dynamic and intermittent streamflow observations in hydrological models

    NASA Astrophysics Data System (ADS)

    Mazzoleni, Maurizio; Alfonso, Leonardo; Chacon-Hurtado, Juan; Solomatine, Dimitri

    2015-09-01

    Catastrophic floods cause significant socio-economical losses. Non-structural measures, such as real-time flood forecasting, can potentially reduce flood risk. To this end, data assimilation methods have been used to improve flood forecasts by integrating static ground observations, and in some cases also remote sensing observations, within water models. Current hydrologic and hydraulic research works consider assimilation of observations coming from traditional, static sensors. At the same time, low-cost, mobile sensors and mobile communication devices are becoming also increasingly available. The main goal and innovation of this study is to demonstrate the usefulness of assimilating uncertain streamflow observations that are dynamic in space and intermittent in time in the context of two different semi-distributed hydrological model structures. The developed method is applied to the Brue basin, where the dynamic observations are imitated by the synthetic observations of discharge. The results of this study show how model structures and sensors locations affect in different ways the assimilation of streamflow observations. In addition, it proves how assimilation of such uncertain observations from dynamic sensors can provide model improvements similar to those of streamflow observations coming from a non-optimal network of static physical sensors. This can be a potential application of recent efforts to build citizen observatories of water, which can make the citizens an active part in information capturing, evaluation and communication, helping simultaneously to improvement of model-based flood forecasting.

  19. Global and regional ecosystem modeling: comparison of model outputs and field measurements

    NASA Astrophysics Data System (ADS)

    Olson, R. J.; Hibbard, K.

    2003-04-01

    The Ecosystem Model-Data Intercomparison (EMDI) Workshops provide a venue for global ecosystem modeling groups to compare model outputs against measurements of net primary productivity (NPP). The objective of EMDI Workshops is to evaluate model performance relative to observations in order to improve confidence in global model projections terrestrial carbon cycling. The questions addressed by EMDI include: How does the simulated NPP compare with the field data across biome and environmental gradients? How sensitive are models to site-specific climate? Does additional mechanistic detail in models result in a better match with field measurements? How useful are the measures of NPP for evaluating model predictions? How well do models represent regional patterns of NPP? Initial EMDI results showed general agreement between model predictions and field measurements but with obvious differences that indicated areas for potential data and model improvement. The effort was built on the development and compilation of complete and consistent databases for model initialization and comparison. Database development improves the data as well as models; however, there is a need to incorporate additional observations and model outputs (LAI, hydrology, etc.) for comprehensive analyses of biogeochemical processes and their relationships to ecosystem structure and function. EMDI initialization and NPP data sets are available from the Oak Ridge National Laboratory Distributed Active Archive Center http://www.daac.ornl.gov/. Acknowledgements: This work was partially supported by the International Geosphere-Biosphere Programme - Data and Information System (IGBP-DIS); the IGBP-Global Analysis, Interpretation and Modelling Task Force (GAIM); the National Center for Ecological Analysis and Synthesis (NCEAS); and the National Aeronautics and Space Administration (NASA) Terrestrial Ecosystem Program. Oak Ridge National Laboratory is managed by UT-Battelle LLC for the U.S. Department of

  20. UHECR mass composition measurement at Telescope Array via stereoscopic observation

    NASA Astrophysics Data System (ADS)

    Stroman, Thomas; Telescope Array Collaboration

    2015-04-01

    The masses of primary ultra-high-energy cosmic-ray (UHECR) nuclei cannot be measured directly on an individual basis, but constraints on the chemical composition can be inferred from the distributions of observable properties. The atmospheric slant depth at which a UHECR-induced extensive air shower reaches its maximum number of particles, Xmax, is particularly sensitive to the mass of the incident nucleus, occurring earlier in the shower's longitudinal development for heavier nuclei at a given energy. The Telescope Array in west-central Utah, the northern hemisphere's largest UHECR detector, is equipped for accurate Xmax and energy measurements via stereoscopic fluorescence observation. Using data from seven years of operation, we will present Xmax distributions at several energies E >10 18 . 2eV , and compare them to distributions predicted by detailed detector simulations under an assortment of assumed UHECR compositions and high-energy hadronic interaction models.

  1. Measurements in Quantum Mechanics and von NEUMANN's Model

    NASA Astrophysics Data System (ADS)

    Mello, Pier A.; Johansen, Lars M.

    2010-12-01

    Many textbooks on Quantum Mechanics are not very precise as to the meaning of making a measurement: as a consequence, they frequently make assertions which are not based on a dynamical description of the measurement process. A model proposed by von Neumann allows a dynamical description of measurement in Quantum Mechanics, including the measuring instrument in the formalism. In this article we apply von Neumann's model to illustrate the measurement of an observable by means of a measuring instrument and show how various results, which are sometimens postulated without a dynamical basis, actually emerge. We also investigate the more complex, intriguing and fundamental problem of two successive measurements in Quantum Mechanics, extending von Neumann's model to two measuring instruments. We present a description which allows obtaining, in a unified way, various results that have been given in the literature.

  2. Science-Grade Observing Systems as Process Observatories: Mapping and Understanding Nonlinearity and Multiscale Memory with Models and Observations

    NASA Astrophysics Data System (ADS)

    Barros, A. P.; Wilson, A. M.; Miller, D. K.; Tao, J.; Genereux, D. P.; Prat, O.; Petersen, W. A.; Brunsell, N. A.; Petters, M. D.; Duan, Y.

    2015-12-01

    Using the planet as a study domain and collecting observations over unprecedented ranges of spatial and temporal scales, NASA's EOS (Earth Observing System) program was an agent of transformational change in Earth Sciences over the last thirty years. The remarkable space-time organization and variability of atmospheric and terrestrial moist processes that emerged from the analysis of comprehensive satellite observations provided much impetus to expand the scope of land-atmosphere interaction studies in Hydrology and Hydrometeorology. Consequently, input and output terms in the mass and energy balance equations evolved from being treated as fluxes that can be used as boundary conditions, or forcing, to being viewed as dynamic processes of a coupled system interacting at multiple scales. Measurements of states or fluxes are most useful if together they map, reveal and/or constrain the underlying physical processes and their interactions. This can only be accomplished through an integrated observing system designed to capture the coupled physics, including nonlinear feedbacks and tipping points. Here, we first review and synthesize lessons learned from hydrometeorology studies in the Southern Appalachians and in the Southern Great Plains using both ground-based and satellite observations, physical models and data-assimilation systems. We will specifically focus on mapping and understanding nonlinearity and multiscale memory of rainfall-runoff processes in mountainous regions. It will be shown that beyond technical rigor, variety, quantity and duration of measurements, the utility of observing systems is determined by their interpretive value in the context of physical models to describe the linkages among different observations. Second, we propose a framework for designing science-grade and science-minded process-oriented integrated observing and modeling platforms for hydrometeorological studies.

  3. Canonical Naimark extension for generalized measurements involving sets of Pauli quantum observables chosen at random

    NASA Astrophysics Data System (ADS)

    Sparaciari, Carlo; Paris, Matteo G. A.

    2013-01-01

    We address measurement schemes where certain observables Xk are chosen at random within a set of nondegenerate isospectral observables and then measured on repeated preparations of a physical system. Each observable has a probability zk to be measured, with ∑kzk=1, and the statistics of this generalized measurement is described by a positive operator-valued measure. This kind of scheme is referred to as quantum roulettes, since each observable Xk is chosen at random, e.g., according to the fluctuating value of an external parameter. Here we focus on quantum roulettes for qubits involving the measurements of Pauli matrices, and we explicitly evaluate their canonical Naimark extensions, i.e., their implementation as indirect measurements involving an interaction scheme with a probe system. We thus provide a concrete model to realize the roulette without destroying the signal state, which can be measured again after the measurement or can be transmitted. Finally, we apply our results to the description of Stern-Gerlach-like experiments on a two-level system.

  4. Ordinal probability effect measures for group comparisons in multinomial cumulative link models.

    PubMed

    Agresti, Alan; Kateri, Maria

    2017-03-01

    We consider simple ordinal model-based probability effect measures for comparing distributions of two groups, adjusted for explanatory variables. An "ordinal superiority" measure summarizes the probability that an observation from one distribution falls above an independent observation from the other distribution, adjusted for explanatory variables in a model. The measure applies directly to normal linear models and to a normal latent variable model for ordinal response variables. It equals Φ(β/2) for the corresponding ordinal model that applies a probit link function to cumulative multinomial probabilities, for standard normal cdf Φ and effect β that is the coefficient of the group indicator variable. For the more general latent variable model for ordinal responses that corresponds to a linear model with other possible error distributions and corresponding link functions for cumulative multinomial probabilities, the ordinal superiority measure equals exp(β)/[1+exp(β)] with the log-log link and equals approximately exp(β/2)/[1+exp(β/2)] with the logit link, where β is the group effect. Another ordinal superiority measure generalizes the difference of proportions from binary to ordinal responses. We also present related measures directly for ordinal models for the observed response that need not assume corresponding latent response models. We present confidence intervals for the measures and illustrate with an example. © 2016, The International Biometric Society.

  5. Observing Traveling Ionospheric Disturbances Caused by Tsunamis Using GPS TEC Measurements

    NASA Technical Reports Server (NTRS)

    Galvan, David A.; Komjathy, Attila; Hickey, Michael; Foster, James; Mannucci, Anthony J.

    2010-01-01

    Ground-based Global Positioning System (GPS) measurements of ionospheric Total Electron Content (TEC) show variations consistent with atmospheric internal gravity waves caused by ocean tsunamis following two recent seismic events: the American Samoa earthquake of September 29, 2009, and the Chile earthquake of February 27, 2010. Fluctuations in TEC correlated in time, space, and wave properties with these tsunamis were observed in TEC estimates processed using JPL's Global Ionospheric Mapping Software. These TEC estimates were band-pass filtered to remove ionospheric TEC variations with wavelengths and periods outside the typical range of internal gravity waves caused by tsunamis. Observable variations in TEC appear correlated with the tsunamis in certain locations, but not in others. Where variations are observed, the typical amplitude tends to be on the order of 1% of the background TEC value. Variations with amplitudes 0.1 - 0.2 TECU are observable with periods and timing affiliated with the tsunami. These observations are compared to estimates of expected tsunami-driven TEC variations produced by Embry Riddle Aeronautical University's Spectral Full Wave Model, an atmosphere-ionosphere coupling model, and found to be in good agreement in some locations, though there are cases when the model predicts an observable tsunami-driven signature and none is observed. These TEC variations are not always seen when a tsunami is present, but in these two events the regions where a strong ocean tsunami was observed did coincide with clear TEC observations, while a lack of clear TEC observations coincided with smaller tsunami amplitudes. There exists the potential to apply these detection techniques to real-time GPS TEC data, providing estimates of tsunami speed and amplitude that may be useful for early warning systems.

  6. The Inherent Uncertainty of In-Situ Observations and its Implications for Modeling Evapotranspiration

    NASA Astrophysics Data System (ADS)

    Alfieri, J. G.

    2012-12-01

    In-situ observations are essential to a broad range of applications including the development, calibration, and validation of both the numerical and remote sensing-based models. For example, observational data is requisite in order to evaluate the skill of these models both to represent the complex biogeophysical processes regulating evapotranspiration (ET) and to predict the magnitude of the moisture flux. As such, by propagating into these subsequent activities, any uncertainty or errors associated with the observational data have the potential to adversely impact the accuracy and utility of these models. It is, therefore, critical that the factors driving measurement uncertainty are fully understood so that the steps can be taken to account for its effects and mitigate its impact on subsequent analyses. Field measurements of ET can be collected using a variety of techniques including eddy covariance (EC), lysimetry (LY), and scintillometry (SC). Each of these methods is underpinned by a unique set of theoretical considerations and practical constraints; and, as a result, each method is susceptible to differing types of systematic and random error. Since the uncertainty associated with the field measurements is predicated on how well numerous factors - for example, environmental conditions - adhere to those prescribed by the underlying assumptions, the quality of in-situ observations collected via the differing methods can vary significantly both over time and from site-to-site. Using data from both site studies and large field campaigns, such as IHOP_2002 and BEAREX08, the sources of uncertainty in field observations will be discussed. The impact of measurement uncertainty on model validation will also be illustrated.

  7. Observation of the diphoton decay of the Higgs boson and measurement of its properties.

    PubMed

    Khachatryan, V; Sirunyan, A M; Tumasyan, A; Adam, W; Bergauer, T; Dragicevic, M; Erö, J; Fabjan, C; Friedl, M; Frühwirth, R; Ghete, V M; Hartl, C; Hörmann, N; Hrubec, J; Jeitler, M; Kiesenhofer, W; Knünz, V; Krammer, M; Krätschmer, I; Liko, D; Mikulec, I; Rabady, D; Rahbaran, B; Rohringer, H; Schöfbeck, R; Strauss, J; Taurok, A; Treberer-Treberspurg, W; Waltenberger, W; Wulz, C-E; Mossolov, V; Shumeiko, N; Suarez Gonzalez, J; Alderweireldt, S; Bansal, M; Bansal, S; Cornelis, T; De Wolf, E A; Janssen, X; Knutsson, A; Luyckx, S; Ochesanu, S; Roland, B; Rougny, R; Van De Klundert, M; Van Haevermaet, H; Van Mechelen, P; Van Remortel, N; Van Spilbeeck, A; Blekman, F; Blyweert, S; D'Hondt, J; Daci, N; Heracleous, N; Keaveney, J; Lowette, S; Maes, M; Olbrechts, A; Python, Q; Strom, D; Tavernier, S; Van Doninck, W; Van Mulders, P; Van Onsem, G P; Villella, I; Caillol, C; Clerbaux, B; De Lentdecker, G; Dobur, D; Favart, L; Gay, A P R; Grebenyuk, A; Léonard, A; Mohammadi, A; Perniè, L; Reis, T; Seva, T; Thomas, L; Vander Velde, C; Vanlaer, P; Wang, J; Adler, V; Beernaert, K; Benucci, L; Cimmino, A; Costantini, S; Crucy, S; Dildick, S; Fagot, A; Garcia, G; Mccartin, J; Ocampo Rios, A A; Ryckbosch, D; Salva Diblen, S; Sigamani, M; Strobbe, N; Thyssen, F; Tytgat, M; Yazgan, E; Zaganidis, N; Basegmez, S; Beluffi, C; Bruno, G; Castello, R; Caudron, A; Ceard, L; Da Silveira, G G; Delaere, C; du Pree, T; Favart, D; Forthomme, L; Giammanco, A; Hollar, J; Jez, P; Komm, M; Lemaitre, V; Nuttens, C; Pagano, D; Perrini, L; Pin, A; Piotrzkowski, K; Popov, A; Quertenmont, L; Selvaggi, M; Vidal Marono, M; Vizan Garcia, J M; Beliy, N; Caebergs, T; Daubie, E; Hammad, G H; Júnior, W L Aldá; Alves, G A; Correa Martins Junior, M; Martins, T Dos Reis; Pol, M E; Carvalho, W; Chinellato, J; Custódio, A; Da Costa, E M; De Jesus Damiao, D; De Oliveira Martins, C; Fonseca De Souza, S; Malbouisson, H; Matos Figueiredo, D; Mundim, L; Nogima, H; Prado Da Silva, W L; Santaolalla, J; Santoro, A; Sznajder, A; Tonelli Manganote, E J; Vilela Pereira, A; Bernardes, C A; Fernandez Perez Tomei, T R; Gregores, E M; Mercadante, P G; Novaes, S F; Padula, Sandra S; Aleksandrov, A; Genchev, V; Iaydjiev, P; Marinov, A; Piperov, S; Rodozov, M; Sultanov, G; Vutova, M; Dimitrov, A; Glushkov, I; Hadjiiska, R; Kozhuharov, V; Litov, L; Pavlov, B; Petkov, P; Bian, J G; Chen, G M; Chen, H S; Chen, M; Du, R; Jiang, C H; Liang, D; Liang, S; Plestina, R; Tao, J; Wang, X; Wang, Z; Asawatangtrakuldee, C; Ban, Y; Guo, Y; Li, Q; Li, W; Liu, S; Mao, Y; Qian, S J; Wang, D; Zhang, L; Zou, W; Avila, C; Chaparro Sierra, L F; Florez, C; Gomez, J P; Gomez Moreno, B; Sanabria, J C; Godinovic, N; Lelas, D; Polic, D; Puljak, I; Antunovic, Z; Kovac, M; Brigljevic, V; Kadija, K; Luetic, J; Mekterovic, D; Sudic, L; Attikis, A; Mavromanolakis, G; Mousa, J; Nicolaou, C; Ptochos, F; Razis, P A; Bodlak, M; Finger, M; Finger, M; Assran, Y; Mahmoud, M A; Radi, A; Kadastik, M; Murumaa, M; Raidal, M; Tiko, A; Eerola, P; Fedi, G; Voutilainen, M; 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Smith, J G; Stenson, K; Ulmer, K A; Wagner, S R; Alexander, J; Chatterjee, A; Chu, J; Dittmer, S; Eggert, N; Mirman, N; Nicolas Kaufman, G; Patterson, J R; Ryd, A; Salvati, E; Skinnari, L; Sun, W; Teo, W D; Thom, J; Thompson, J; Tucker, J; Weng, Y; Winstrom, L; Wittich, P; Winn, D; Abdullin, S; Albrow, M; Anderson, J; Apollinari, G; Bauerdick, L A T; Beretvas, A; Berryhill, J; Bhat, P C; Burkett, K; Butler, J N; Cheung, H W K; Chlebana, F; Cihangir, S; Elvira, V D; Fisk, I; Freeman, J; Gao, Y; Gottschalk, E; Gray, L; Green, D; Grünendahl, S; Gutsche, O; Hanlon, J; Hare, D; Harris, R M; Hirschauer, J; Hooberman, B; Jindariani, S; Johnson, M; Joshi, U; Kaadze, K; Klima, B; Kreis, B; Kwan, S; Linacre, J; Lincoln, D; Lipton, R; Liu, T; Lykken, J; Maeshima, K; Marraffino, J M; Martinez Outschoorn, V I; Maruyama, S; Mason, D; McBride, P; Mishra, K; Mrenna, S; Musienko, Y; Nahn, S; Newman-Holmes, C; O'Dell, V; Prokofyev, O; Sexton-Kennedy, E; Sharma, S; Soha, A; Spalding, W J; Spiegel, L; Taylor, L; Tkaczyk, S; Tran, N V; Uplegger, L; Vaandering, E W; Vidal, R; Whitbeck, A; Whitmore, J; Yang, F; Acosta, D; Avery, P; Bourilkov, D; Carver, M; Cheng, T; Curry, D; Das, S; De Gruttola, M; Di Giovanni, G P; Field, R D; Fisher, M; Furic, I K; Hugon, J; Konigsberg, J; Korytov, A; Kypreos, T; Low, J F; Matchev, K; Milenovic, P; Mitselmakher, G; Muniz, L; Rinkevicius, A; Shchutska, L; Skhirtladze, N; Snowball, M; Yelton, J; Zakaria, M; Hewamanage, S; Linn, S; Markowitz, P; Martinez, G; Rodriguez, J L; Adams, T; Askew, A; Bochenek, J; Diamond, B; Haas, J; Hagopian, S; Hagopian, V; Johnson, K F; Prosper, H; Veeraraghavan, V; Weinberg, M; Baarmand, M M; Hohlmann, M; Kalakhety, H; Yumiceva, F; Adams, M R; Apanasevich, L; Bazterra, V E; Berry, D; Betts, R R; Bucinskaite, I; Cavanaugh, R; Evdokimov, O; Gauthier, L; Gerber, C E; Hofman, D J; Khalatyan, S; Kurt, P; Moon, D H; O'Brien, C; Silkworth, C; Turner, P; Varelas, N; Albayrak, E A; Bilki, B; Clarida, W; Dilsiz, K; Duru, F; Haytmyradov, M; Merlo, J-P; Mermerkaya, H; Mestvirishvili, A; Moeller, A; Nachtman, J; Ogul, H; Onel, Y; Ozok, F; Penzo, A; Rahmat, R; Sen, S; Tan, P; Tiras, E; Wetzel, J; Yetkin, T; Yi, K; Barnett, B A; Blumenfeld, B; Bolognesi, S; Fehling, D; Gritsan, A V; Maksimovic, P; Martin, C; Swartz, M; Baringer, P; Bean, A; Benelli, G; Bruner, C; Gray, J; Kenny, R P; Malek, M; Murray, M; Noonan, D; Sanders, S; Sekaric, J; Stringer, R; Wang, Q; Wood, J S; Barfuss, A F; Chakaberia, I; Ivanov, A; Khalil, S; Makouski, M; Maravin, Y; Saini, L K; Shrestha, S; Svintradze, I; Gronberg, J; Lange, D; Rebassoo, F; Wright, D; Baden, A; Calvert, B; Eno, S C; Gomez, J A; Hadley, N J; Kellogg, R G; Kolberg, T; Lu, Y; Marionneau, M; Mignerey, A C; Pedro, K; Skuja, A; Tonjes, M B; Tonwar, S C; Apyan, A; Barbieri, R; Bauer, G; Busza, W; Cali, I A; Chan, M; Di Matteo, L; Dutta, V; Gomez Ceballos, G; Goncharov, M; Gulhan, D; Klute, M; Lai, Y S; Lee, Y-J; Levin, A; Luckey, P D; Ma, T; Paus, C; Ralph, D; Roland, C; Roland, G; Stephans, G S F; Stöckli, F; Sumorok, K; Velicanu, D; Veverka, J; Wyslouch, B; Yang, M; Yoon, A S; Zanetti, M; Zhukova, V; Dahmes, B; De Benedetti, A; Gude, A; Kao, S C; Klapoetke, K; Kubota, Y; Mans, J; Pastika, N; Rusack, R; Singovsky, A; Tambe, N; Turkewitz, J; Acosta, J G; Cremaldi, L M; Kroeger, R; Oliveros, S; Perera, L; Sanders, D A; Summers, D; Avdeeva, E; Bloom, K; Bose, S; Claes, D R; Dominguez, A; Gonzalez Suarez, R; Keller, J; Knowlton, D; Kravchenko, I; Lazo-Flores, J; Malik, S; Meier, F; Snow, G R; Dolen, J; Godshalk, A; Iashvili, I; Jain, S; Kharchilava, A; Kumar, A; Rappoccio, S; Alverson, G; Barberis, E; Baumgartel, D; Chasco, M; Haley, J; Massironi, A; Nash, D; Orimoto, T; Trocino, D; Wood, D; Zhang, J; Anastassov, A; Hahn, K A; Kubik, A; Lusito, L; Mucia, N; Odell, N; Pollack, B; Pozdnyakov, A; Schmitt, M; Stoynev, S; Sung, K; Velasco, M; Won, S; Brinkerhoff, A; Chan, K M; Drozdetskiy, A; Hildreth, M; Jessop, C; Karmgard, D J; Kellams, N; Lannon, K; Luo, W; Lynch, S; Marinelli, N; Pearson, T; Planer, M; Ruchti, R; Valls, N; Wayne, M; Wolf, M; Woodard, A; Antonelli, L; Brinson, J; Bylsma, B; Durkin, L S; Flowers, S; Hill, C; Hughes, R; Kotov, K; Ling, T Y; Puigh, D; Rodenburg, M; Smith, G; Vuosalo, C; Winer, B L; Wolfe, H; Wulsin, H W; Driga, O; Elmer, P; Hebda, P; Hunt, A; Koay, S A; Lujan, P; Marlow, D; Medvedeva, T; Mooney, M; Olsen, J; Piroué, P; Quan, X; Saka, H; Stickland, D; Tully, C; Werner, J S; Zenz, S C; Zuranski, A; Brownson, E; Mendez, H; Ramirez Vargas, J E; Alagoz, E; Barnes, V E; Benedetti, D; Bolla, G; Bortoletto, D; De Mattia, M; Hu, Z; Jha, M K; Jones, M; Jung, K; Kress, M; Leonardo, N; Lopes Pegna, D; Maroussov, V; Merkel, P; Miller, D H; Neumeister, N; Radburn-Smith, B C; Shi, X; Shipsey, I; Silvers, D; Svyatkovskiy, A; Wang, F; Xie, W; Xu, L; Yoo, H D; Zablocki, J; Zheng, Y; Parashar, N; Stupak, J; Adair, A; Akgun, B; Ecklund, K M; Geurts, F J M; Li, W; Michlin, B; Padley, B P; Redjimi, R; Roberts, J; Zabel, J; Betchart, B; Bodek, A; Covarelli, R; de Barbaro, P; Demina, R; Eshaq, Y; Ferbel, T; Garcia-Bellido, A; Goldenzweig, P; Han, J; Harel, A; Khukhunaishvili, A; Petrillo, G; Vishnevskiy, D; Ciesielski, R; Demortier, L; Goulianos, K; Lungu, G; Mesropian, C; Arora, S; Barker, A; Chou, J P; Contreras-Campana, C; Contreras-Campana, E; Duggan, D; Ferencek, D; Gershtein, Y; Gray, R; Halkiadakis, E; Hidas, D; Lath, A; Panwalkar, S; Park, M; Patel, R; Salur, S; Schnetzer, S; Somalwar, S; Stone, R; Thomas, S; Thomassen, P; Walker, M; Rose, K; Spanier, S; York, A; Bouhali, O; Eusebi, R; Flanagan, W; Gilmore, J; Kamon, T; Khotilovich, V; Krutelyov, V; Montalvo, R; Osipenkov, I; Pakhotin, Y; Perloff, A; Roe, J; Rose, A; Safonov, A; Sakuma, T; Suarez, I; Tatarinov, A; Akchurin, N; Cowden, C; Damgov, J; Dragoiu, C; Dudero, P R; Faulkner, J; Kovitanggoon, K; Kunori, S; Lee, S W; Libeiro, T; Volobouev, I; Appelt, E; Delannoy, A G; Greene, S; Gurrola, A; Johns, W; Maguire, C; Mao, Y; Melo, A; Sharma, M; Sheldon, P; Snook, B; Tuo, S; Velkovska, J; Arenton, M W; Boutle, S; Cox, B; Francis, B; Goodell, J; Hirosky, R; Ledovskoy, A; Li, H; Lin, C; Neu, C; Wood, J; Harr, R; Karchin, P E; Kottachchi Kankanamge Don, C; Lamichhane, P; Sturdy, J; Belknap, D A; Carlsmith, D; Cepeda, M; Dasu, S; Duric, S; Friis, E; Hall-Wilton, R; Herndon, M; Hervé, A; Klabbers, P; Lanaro, A; Lazaridis, C; Levine, A; Loveless, R; Mohapatra, A; Ojalvo, I; Perry, T; Pierro, G A; Polese, G; Ross, I; Sarangi, T; Savin, A; Smith, W H; Woods, N

    Observation of the diphoton decay mode of the recently discovered Higgs boson and measurement of some of its properties are reported. The analysis uses the entire dataset collected by the CMS experiment in proton-proton collisions during the 2011 and 2012 LHC running periods. The data samples correspond to integrated luminosities of 5.1[Formula: see text]at [Formula: see text] and 19.7[Formula: see text]at 8[Formula: see text] . A clear signal is observed in the diphoton channel at a mass close to 125[Formula: see text] with a local significance of [Formula: see text], where a significance of [Formula: see text] is expected for the standard model Higgs boson. The mass is measured to be [Formula: see text] , and the best-fit signal strength relative to the standard model prediction is [Formula: see text][Formula: see text][Formula: see text]. Additional measurements include the signal strength modifiers associated with different production mechanisms, and hypothesis tests between spin-0 and spin-2 models.

  8. Integration of Local Observations into the One Dimensional Fog Model PAFOG

    NASA Astrophysics Data System (ADS)

    Thoma, Christina; Schneider, Werner; Masbou, Matthieu; Bott, Andreas

    2012-05-01

    The numerical prediction of fog requires a very high vertical resolution of the atmosphere. Owing to a prohibitive computational effort of high resolution three dimensional models, operational fog forecast is usually done by means of one dimensional fog models. An important condition for a successful fog forecast with one dimensional models consists of the proper integration of observational data into the numerical simulations. The goal of the present study is to introduce new methods for the consideration of these data in the one dimensional radiation fog model PAFOG. First, it will be shown how PAFOG may be initialized with observed visibilities. Second, a nudging scheme will be presented for the inclusion of measured temperature and humidity profiles in the PAFOG simulations. The new features of PAFOG have been tested by comparing the model results with observations of the German Meteorological Service. A case study will be presented that reveals the importance of including local observations in the model calculations. Numerical results obtained with the modified PAFOG model show a distinct improvement of fog forecasts regarding the times of fog formation, dissipation as well as the vertical extent of the investigated fog events. However, model results also reveal that a further improvement of PAFOG might be possible if several empirical model parameters are optimized. This tuning can only be realized by comprehensive comparisons of model simulations with corresponding fog observations.

  9. Deployment and Evaluation of an Observations Data Model

    NASA Astrophysics Data System (ADS)

    Horsburgh, J. S.; Tarboton, D. G.; Zaslavsky, I.; Maidment, D. R.; Valentine, D.

    2007-12-01

    Environmental observations are fundamental to hydrology and water resources, and the way these data are organized and manipulated either enables or inhibits the analyses that can be performed. The CUAHSI Hydrologic Information System project is developing information technology infrastructure to support hydrologic science. This includes an Observations Data Model (ODM) that provides a new and consistent format for the storage and retrieval of environmental observations in a relational database designed to facilitate integrated analysis of large datasets collected by multiple investigators. Within this data model, observations are stored with sufficient ancillary information (metadata) about the observations to allow them to be unambiguously interpreted and used, and to provide traceable heritage from raw measurements to useable information. The design is based upon a relational database model that exposes each single observation as a record, taking advantage of the capability in relational database systems for querying based upon data values and enabling cross dimension data retrieval and analysis. This data model has been deployed, as part of the HIS Server, at the WATERS Network test bed observatories across the U.S where it serves as a repository for real time data in the observatory information system. The ODM holds the data that is then made available to investigators and the public through web services and the Data Access System for Hydrology (DASH) map based interface. In the WATERS Network test bed settings the ODM has been used to ingest, analyze and publish data from a variety of sources and disciplines. This paper will present an evaluation of the effectiveness of this initial deployment and the revisions that are being instituted to address shortcomings. The ODM represents a new, systematic way for hydrologists, scientists, and engineers to organize and share their data and thereby facilitate a fuller integrated understanding of water resources based on

  10. UV solar irradiance in observations and the NRLSSI and SATIRE-S models

    NASA Astrophysics Data System (ADS)

    Yeo, K. L.; Ball, W. T.; Krivova, N. A.; Solanki, S. K.; Unruh, Y. C.; Morrill, J.

    2015-08-01

    Total solar irradiance and UV spectral solar irradiance has been monitored since 1978 through a succession of space missions. This is accompanied by the development of models aimed at replicating solar irradiance by relating the variability to solar magnetic activity. The Naval Research Laboratory Solar Spectral Irradiance (NRLSSI) and Spectral And Total Irradiance REconstruction for the Satellite era (SATIRE-S) models provide the most comprehensive reconstructions of total and spectral solar irradiance over the period of satellite observation currently available. There is persistent controversy between the various measurements and models in terms of the wavelength dependence of the variation over the solar cycle, with repercussions on our understanding of the influence of UV solar irradiance variability on the stratosphere. We review the measurement and modeling of UV solar irradiance variability over the period of satellite observation. The SATIRE-S reconstruction is consistent with spectral solar irradiance observations where they are reliable. It is also supported by an independent, empirical reconstruction of UV spectral solar irradiance based on Upper Atmosphere Research Satellite/Solar Ultraviolet Spectral Irradiance Monitor measurements from an earlier study. The weaker solar cycle variability produced by NRLSSI between 300 and 400 nm is not evident in any available record. We show that although the method employed to construct NRLSSI is principally sound, reconstructed solar cycle variability is detrimentally affected by the uncertainty in the SSI observations it draws upon in the derivation. Based on our findings, we recommend, when choosing between the two models, the use of SATIRE-S for climate studies.

  11. Stratospheric Temperature Changes: Observations and Model Simulations

    NASA Technical Reports Server (NTRS)

    Ramaswamy, V.; Chanin, M.-L.; Angell, J.; Barnett, J.; Gaffen, D.; Gelman, M.; Keckhut, P.; Koshelkov, Y.; Labitzke, K.; Lin, J.-J. R.

    1999-01-01

    This paper reviews observations of stratospheric temperatures that have been made over a period of several decades. Those observed temperatures have been used to assess variations and trends in stratospheric temperatures. A wide range of observation datasets have been used, comprising measurements by radiosonde (1940s to the present), satellite (1979 - present), lidar (1979 - present) and rocketsonde (periods varying with location, but most terminating by about the mid-1990s). In addition, trends have also been assessed from meteorological analyses, based on radiosonde and/or satellite data, and products based on assimilating observations into a general circulation model. Radiosonde and satellite data indicate a cooling trend of the annual-mean lower stratosphere since about 1980. Over the period 1979-1994, the trend is 0.6K/decade. For the period prior to 1980, the radiosonde data exhibit a substantially weaker long-term cooling trend. In the northern hemisphere, the cooling trend is about 0.75K/decade in the lower stratosphere, with a reduction in the cooling in mid-stratosphere (near 35 km), and increased cooling in the upper stratosphere (approximately 2 K per decade at 50 km). Model simulations indicate that the depletion of lower stratospheric ozone is the dominant factor in the observed lower stratospheric cooling. In the middle and upper stratosphere both the well-mixed greenhouse gases (such as CO) and ozone changes contribute in an important manner to the cooling.

  12. Experiments with data assimilation in comprehensive air quality models: Impacts on model predictions and observation requirements (Invited)

    NASA Astrophysics Data System (ADS)

    Mathur, R.

    2009-12-01

    Emerging regional scale atmospheric simulation models must address the increasing complexity arising from new model applications that treat multi-pollutant interactions. Sophisticated air quality modeling systems are needed to develop effective abatement strategies that focus on simultaneously controlling multiple criteria pollutants as well as use in providing short term air quality forecasts. In recent years the applications of such models is continuously being extended to address atmospheric pollution phenomenon from local to hemispheric spatial scales over time scales ranging from episodic to annual. The need to represent interactions between physical and chemical atmospheric processes occurring at these disparate spatial and temporal scales requires the use of observation data beyond traditional in-situ networks so that the model simulations can be reasonably constrained. Preliminary applications of assimilation of remote sensing and aloft observations within a comprehensive regional scale atmospheric chemistry-transport modeling system will be presented: (1) A methodology is developed to assimilate MODIS aerosol optical depths in the model to represent the impacts long-range transport associated with the summer 2004 Alaskan fires on surface-level regional fine particulate matter (PM2.5) concentrations across the Eastern U.S. The episodic impact of this pollution transport event on PM2.5 concentrations over the eastern U.S. during mid-July 2004, is quantified through the complementary use of the model with remotely-sensed, aloft, and surface measurements; (2) Simple nudging experiments with limited aloft measurements are performed to identify uncertainties in model representations of physical processes and assess the potential use of such measurements in improving the predictive capability of atmospheric chemistry-transport models. The results from these early applications will be discussed in context of uncertainties in the model and in the remote sensing

  13. Observing Tsunamis in the Ionosphere Using Ground Based GPS Measurements

    NASA Technical Reports Server (NTRS)

    Galvan, D. A.; Komjathy, A.; Song, Y. Tony; Stephens, P.; Hickey, M. P.; Foster, J.

    2011-01-01

    Ground-based Global Positioning System (GPS) measurements of ionospheric Total Electron Content (TEC) show variations consistent with atmospheric internal gravity waves caused by ocean tsunamis following recent seismic events, including the Tohoku tsunami of March 11, 2011. We observe fluctuations correlated in time, space, and wave properties with this tsunami in TEC estimates processed using JPL's Global Ionospheric Mapping Software. These TEC estimates were band-pass filtered to remove ionospheric TEC variations with periods outside the typical range of internal gravity waves caused by tsunamis. Observable variations in TEC appear correlated with the Tohoku tsunami near the epicenter, at Hawaii, and near the west coast of North America. Disturbance magnitudes are 1-10% of the background TEC value. Observations near the epicenter are compared to estimates of expected tsunami-driven TEC variations produced by Embry Riddle Aeronautical University's Spectral Full Wave Model, an atmosphere-ionosphere coupling model, and found to be in good agreement. The potential exists to apply these detection techniques to real-time GPS TEC data, providing estimates of tsunami speed and amplitude that may be useful for future early warning systems.

  14. Models of the Jovian Ring and Comparisions With Observations

    NASA Astrophysics Data System (ADS)

    Juhasz, A.; Horanyi, M.

    2008-12-01

    A number of in situ and remote sensing observations of the Jovian ring system exist so we can now combine observations from Voyager, Pioneer, Galileo and Cassini, as well as ground based and HST measurements. In this presentation we will compare this large body of observations to available theoretical models of the dust dynamics in the Jovian ring. Common to all models (Burns et al., 1985, 2001 ; Horanyi et al.,1996, 2004) is the basic idea that dust is being continuously produced due to micro-meteoroid bombardment of the moons in this region. Also, the spatial distribution of dust in the halo region inward of the main ring is generally accepted to be a consequence of electrodynamic perturbations acting on small charged dust particles. However, in the suggested theoretical models the time scale for orbital evolution is drastically differ. Burns et al. argues, that in the main ring, dust particles evolve inward very slowly due to Poynting-Robertson drag. A typical micron sized grain is predicted to orbit Jupiter for 104 years before crashing into the atmosphere of Jupiter. Horanyi et al. argues that the radial transport is due to resonant charge variations, dictated by the plasma density distribution. In this model grains are transported on a time scale that is orders of magnitude shorter than predicted by PR drag. Here we use both of these models to generate brightness distributions and predict optical depth distributions for same geometries and wavelengths as that of the observations. Quantitative comparisons of the modeled and the real observations lead us to the conclusion that the dust transport in ring/halo region at Jupiter is mainly due to resonant charge variation.

  15. An Evaluation of Cosmological Models from the Expansion and Growth of Structure Measurements

    DOE PAGES

    Zhai, Zhongxu; Blanton, Michael; Slosar, Anze; ...

    2017-12-01

    Here, we compare a large suite of theoretical cosmological models to observational data from the cosmic microwave background, baryon acoustic oscillation measurements of expansion, Type Ia supernova measurements of expansion, redshift space distortion measurements of the growth of structure, and the local Hubble constant. Our theoretical models include parametrizations of dark energy as well as physical models of dark energy and modified gravity. We determine the constraints on the model parameters, incorporating the redshift space distortion data directly in the analysis. To determine whether models can be ruled out, we evaluate the p-value (the probability under the model of obtainingmore » data as bad or worse than the observed data). In our comparison, we find the well-known tension of H 0 with the other data; no model resolves this tension successfully. Among the models we consider, the large-scale growth of structure data does not affect the modified gravity models as a category particularly differently from dark energy models; it matters for some modified gravity models but not others, and the same is true for dark energy models. We compute predicted observables for each model under current observational constraints, and identify models for which future observational constraints will be particularly informative.« less

  16. An Evaluation of Cosmological Models from the Expansion and Growth of Structure Measurements

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Zhai, Zhongxu; Blanton, Michael; Slosar, Anze

    Here, we compare a large suite of theoretical cosmological models to observational data from the cosmic microwave background, baryon acoustic oscillation measurements of expansion, Type Ia supernova measurements of expansion, redshift space distortion measurements of the growth of structure, and the local Hubble constant. Our theoretical models include parametrizations of dark energy as well as physical models of dark energy and modified gravity. We determine the constraints on the model parameters, incorporating the redshift space distortion data directly in the analysis. To determine whether models can be ruled out, we evaluate the p-value (the probability under the model of obtainingmore » data as bad or worse than the observed data). In our comparison, we find the well-known tension of H 0 with the other data; no model resolves this tension successfully. Among the models we consider, the large-scale growth of structure data does not affect the modified gravity models as a category particularly differently from dark energy models; it matters for some modified gravity models but not others, and the same is true for dark energy models. We compute predicted observables for each model under current observational constraints, and identify models for which future observational constraints will be particularly informative.« less

  17. An Evaluation of Cosmological Models from the Expansion and Growth of Structure Measurements

    NASA Astrophysics Data System (ADS)

    Zhai, Zhongxu; Blanton, Michael; Slosar, Anže; Tinker, Jeremy

    2017-12-01

    We compare a large suite of theoretical cosmological models to observational data from the cosmic microwave background, baryon acoustic oscillation measurements of expansion, Type Ia supernova measurements of expansion, redshift space distortion measurements of the growth of structure, and the local Hubble constant. Our theoretical models include parametrizations of dark energy as well as physical models of dark energy and modified gravity. We determine the constraints on the model parameters, incorporating the redshift space distortion data directly in the analysis. To determine whether models can be ruled out, we evaluate the p-value (the probability under the model of obtaining data as bad or worse than the observed data). In our comparison, we find the well-known tension of H 0 with the other data; no model resolves this tension successfully. Among the models we consider, the large-scale growth of structure data does not affect the modified gravity models as a category particularly differently from dark energy models; it matters for some modified gravity models but not others, and the same is true for dark energy models. We compute predicted observables for each model under current observational constraints, and identify models for which future observational constraints will be particularly informative.

  18. Observer Agreement for Measurements in Videolaryngostroboscopy.

    PubMed

    Brunings, Jan Wouter; Vanbelle, Sophie; Akkermans, Annemarie; Heemskerk, Nienke M M; Kremer, Bernd; Stokroos, Robert J; Baijens, Laura W J

    2017-11-06

    This study evaluated the levels of intraobserver and interobserver agreement for measurements of visuoperceptual variables in videolaryngostroboscopic examinations and compared the observers' behavior during independent versus consensus panel rating. This is a retrospective study. This study was conducted in a single-center tertiary care facility. Sixty-four patients with dysphonia of heterogeneous etiology were included. All subjects underwent a standardized videolaryngostroboscopic examination. Two experienced and trained observers scored exactly the same examinations, first independently and then on a consensus panel. Specific visuoperceptual variables and the clinical diagnosis (as recommended by the Committee on Phoniatrics and the Phonosurgery Committee of the European Laryngological Society and advised by the American Speech-Language-Hearing Association) were scored. Descriptive and kappa statistics were used. In general, intraobserver agreement was better than agreement between observers for measurements of several variables. The intrapanel observer agreement levels were slightly higher than the intraobserver agreement levels on the independent rating task. When rating on the consensus panel, the observers deviated considerably from the scores they had previously given on the independent rating task. Observer agreement in videolaryngostroboscopic assessment has important implications not only for the diagnosis and treatment of dysphonic patients but also for the interpretation of the results of scientific studies using videolaryngostroboscopic outcome parameters. The identification of factors that can influence the levels of observer agreement can provide a better understanding of the rating process and its limitations. The results of this study suggest that future research could achieve better agreement levels by rating the visuoperceptual variables in a panel setting. Copyright © 2017 The Voice Foundation. Published by Elsevier Inc. All rights reserved.

  19. Experimental evaluation of nonclassical correlations between measurement outcomes and target observable in a quantum measurement

    NASA Astrophysics Data System (ADS)

    Iinuma, Masataka; Suzuki, Yutaro; Nii, Taiki; Kinoshita, Ryuji; Hofmann, Holger F.

    2016-03-01

    In general, it is difficult to evaluate measurement errors when the initial and final conditions of the measurement make it impossible to identify the correct value of the target observable. Ozawa proposed a solution based on the operator algebra of observables which has recently been used in experiments investigating the error-disturbance trade-off of quantum measurements. Importantly, this solution makes surprisingly detailed statements about the relations between measurement outcomes and the unknown target observable. In the present paper, we investigate this relation by performing a sequence of two measurements on the polarization of a photon, so that the first measurement commutes with the target observable and the second measurement is sensitive to a complementary observable. While the initial measurement can be evaluated using classical statistics, the second measurement introduces the effects of quantum correlations between the noncommuting physical properties. By varying the resolution of the initial measurement, we can change the relative contribution of the nonclassical correlations and identify their role in the evaluation of the quantum measurement. It is shown that the most striking deviation from classical expectations is obtained at the transition between weak and strong measurements, where the competition between different statistical effects results in measurement values well outside the range of possible eigenvalues.

  20. Parental modelling of eating behaviours: observational validation of the Parental Modelling of Eating Behaviours scale (PARM).

    PubMed

    Palfreyman, Zoe; Haycraft, Emma; Meyer, Caroline

    2015-03-01

    Parents are important role models for their children's eating behaviours. This study aimed to further validate the recently developed Parental Modelling of Eating Behaviours Scale (PARM) by examining the relationships between maternal self-reports on the PARM with the modelling practices exhibited by these mothers during three family mealtime observations. Relationships between observed maternal modelling and maternal reports of children's eating behaviours were also explored. Seventeen mothers with children aged between 2 and 6 years were video recorded at home on three separate occasions whilst eating a meal with their child. Mothers also completed the PARM, the Children's Eating Behaviour Questionnaire and provided demographic information about themselves and their child. Findings provided validation for all three PARM subscales, which were positively associated with their observed counterparts on the observational coding scheme (PARM-O). The results also indicate that habituation to observations did not change the feeding behaviours displayed by mothers. In addition, observed maternal modelling was significantly related to children's food responsiveness (i.e., their interest in and desire for foods), enjoyment of food, and food fussiness. This study makes three important contributions to the literature. It provides construct validation for the PARM measure and provides further observational support for maternal modelling being related to lower levels of food fussiness and higher levels of food enjoyment in their children. These findings also suggest that maternal feeding behaviours remain consistent across repeated observations of family mealtimes, providing validation for previous research which has used single observations. Copyright © 2014 Elsevier Ltd. All rights reserved.

  1. Parameter Estimation and Model Selection for Indoor Environments Based on Sparse Observations

    NASA Astrophysics Data System (ADS)

    Dehbi, Y.; Loch-Dehbi, S.; Plümer, L.

    2017-09-01

    This paper presents a novel method for the parameter estimation and model selection for the reconstruction of indoor environments based on sparse observations. While most approaches for the reconstruction of indoor models rely on dense observations, we predict scenes of the interior with high accuracy in the absence of indoor measurements. We use a model-based top-down approach and incorporate strong but profound prior knowledge. The latter includes probability density functions for model parameters and sparse observations such as room areas and the building footprint. The floorplan model is characterized by linear and bi-linear relations with discrete and continuous parameters. We focus on the stochastic estimation of model parameters based on a topological model derived by combinatorial reasoning in a first step. A Gauss-Markov model is applied for estimation and simulation of the model parameters. Symmetries are represented and exploited during the estimation process. Background knowledge as well as observations are incorporated in a maximum likelihood estimation and model selection is performed with AIC/BIC. The likelihood is also used for the detection and correction of potential errors in the topological model. Estimation results are presented and discussed.

  2. Recent solar extreme ultraviolet irradiance observations and modeling: A review

    NASA Technical Reports Server (NTRS)

    Tobiska, W. Kent

    1993-01-01

    For more than 90 years, solar extreme ultraviolet (EUV) irradiance modeling has progressed from empirical blackbody radiation formulations, through fudge factors, to typically measured irradiances and reference spectra was well as time-dependent empirical models representing continua and line emissions. A summary of recent EUV measurements by five rockets and three satellites during the 1980s is presented along with the major modeling efforts. The most significant reference spectra are reviewed and threee independently derived empirical models are described. These include Hinteregger's 1981 SERF1, Nusinov's 1984 two-component, and Tobiska's 1990/1991/SERF2/EUV91 flux models. They each provide daily full-disk broad spectrum flux values from 2 to 105 nm at 1 AU. All the models depend to one degree or another on the long time series of the Atmosphere Explorer E (AE-E) EUV database. Each model uses ground- and/or space-based proxies to create emissions from solar atmospheric regions. Future challenges in EUV modeling are summarized including the basic requirements of models, the task of incorporating new observations and theory into the models, the task of comparing models with solar-terrestrial data sets, and long-term goals and modeling objectives. By the late 1990s, empirical models will potentially be improved through the use of proposed solar EUV irradiance measurements and images at selected wavelengths that will greatly enhance modeling and predictive capabilities.

  3. Measurement Uncertainty Relations for Discrete Observables: Relative Entropy Formulation

    NASA Astrophysics Data System (ADS)

    Barchielli, Alberto; Gregoratti, Matteo; Toigo, Alessandro

    2018-02-01

    We introduce a new information-theoretic formulation of quantum measurement uncertainty relations, based on the notion of relative entropy between measurement probabilities. In the case of a finite-dimensional system and for any approximate joint measurement of two target discrete observables, we define the entropic divergence as the maximal total loss of information occurring in the approximation at hand. For fixed target observables, we study the joint measurements minimizing the entropic divergence, and we prove the general properties of its minimum value. Such a minimum is our uncertainty lower bound: the total information lost by replacing the target observables with their optimal approximations, evaluated at the worst possible state. The bound turns out to be also an entropic incompatibility degree, that is, a good information-theoretic measure of incompatibility: indeed, it vanishes if and only if the target observables are compatible, it is state-independent, and it enjoys all the invariance properties which are desirable for such a measure. In this context, we point out the difference between general approximate joint measurements and sequential approximate joint measurements; to do this, we introduce a separate index for the tradeoff between the error of the first measurement and the disturbance of the second one. By exploiting the symmetry properties of the target observables, exact values, lower bounds and optimal approximations are evaluated in two different concrete examples: (1) a couple of spin-1/2 components (not necessarily orthogonal); (2) two Fourier conjugate mutually unbiased bases in prime power dimension. Finally, the entropic incompatibility degree straightforwardly generalizes to the case of many observables, still maintaining all its relevant properties; we explicitly compute it for three orthogonal spin-1/2 components.

  4. Measured and modeled dry deposition velocities over the ESCOMPTE area

    NASA Astrophysics Data System (ADS)

    Michou, M.; Laville, P.; Serça, D.; Fotiadi, A.; Bouchou, P.; Peuch, V.-H.

    2005-03-01

    Measurements of the dry deposition velocity of ozone have been made by the eddy correlation method during ESCOMPTE (Etude sur Site pour COntraindre les Modèles de Pollution atmosphérique et de Transport d'Emissions). The strong local variability of natural ecosystems was sampled over several weeks in May, June and July 2001 for four sites with varying surface characteristics. The sites included a maize field, a Mediterranean forest, a Mediterranean shrub-land, and an almost bare soil. Measurements of nitrogen oxide deposition fluxes by the relaxed eddy correlation method have also been carried out at the same bare soil site. An evaluation of the deposition velocities computed by the surface module of the multi-scale Chemistry and Transport Model MOCAGE is presented. This module relies on a resistance approach, with a detailed treatment of the stomatal contribution to the surface resistance. Simulations at the finest model horizontal resolution (around 10 km) are compared to observations. If the seasonal variations are in agreement with the literature, comparisons between raw model outputs and observations, at the different measurement sites and for the specific observing periods, are contrasted. As the simulated meteorology at the scale of 10 km nicely captures the observed situations, the default set of surface characteristics (averaged at the resolution of a grid cell) appears to be one of the main reasons for the discrepancies found with observations. For each case, sensitivity studies have been performed in order to see the impact of adjusting the surface characteristics to the observed ones, when available. Generally, a correct agreement with the observations of deposition velocities is obtained. This advocates for a sub-grid scale representation of surface characteristics for the simulation of dry deposition velocities over such a complex area. Two other aspects appear in the discussion. Firstly, the strong influence of the soil water content to the plant

  5. Anchoring Atmospheric Density Models Using Observed Shuttle Plume Emissions

    NASA Astrophysics Data System (ADS)

    Dimpfl, W. L.; Bernstien, L. S.

    2010-12-01

    Atmospheric number densities at a given low-earth orbit (LEO) altitude can vary by more than an order of magnitude, depending on such parameters as diurnal variations and solar activity. The MSIS atmospheric model, which includes these dependent variables as input, is reported as being accurate to ±15%. Improvement to such models requires accurate direct atmospheric measurement. Here, a means of anchoring atmospheric models is offered through measuring the size and shape of atomic line or molecular band radiance resulting from the atmospheric interaction from rocket engine plumes or gas releases in LEO. Many discrete line or band emissions, ranging from the infrared to the ultraviolet may be suitable. For this purpose we are focusing on NH(A→X), centered at 316 nm. This emission is seen in the plumes of the Shuttle Orbiter PRCS engines, is expected in the plume of any amine fueled engine, and can be observed from remote sensors in space or on the ground. The atmospheric interaction of gas releases or plumes from spacecraft in LEO are understood by comparison of observed radiance with that predicted by Direct Simulation Monte Carlo (DSMC) models. The recent Extended Variable Hard Sphere (EVHS) improvements in treating hyperthermal collisions has produced exceptional agreement between measured and modeled steady-state Space Shuttle OMS and PRCS 190-250 nm Cameron band plume radiance from CO(a→X), which is understood to result from a combination of two- and three-step mechanisms. Radiance from NH(A→X) in far field plumes is understood to result from a simpler single-step process of the reaction of a minor plume species with atomic oxygen, making it more suitable for use in determining atmospheric density. It is recommended that direct retrofire burns of amine fueled engines be imaged in a narrow band from remote sensors to reveal atmospheric number density. In principal the simple measurement of the distance between the engine exit and the peak in the steady

  6. Nonlinearity analysis of measurement model for vision-based optical navigation system

    NASA Astrophysics Data System (ADS)

    Li, Jianguo; Cui, Hutao; Tian, Yang

    2015-02-01

    In the autonomous optical navigation system based on line-of-sight vector observation, nonlinearity of measurement model is highly correlated with the navigation performance. By quantitatively calculating the degree of nonlinearity of the focal plane model and the unit vector model, this paper focuses on determining which optical measurement model performs better. Firstly, measurement equations and measurement noise statistics of these two line-of-sight measurement models are established based on perspective projection co-linearity equation. Then the nonlinear effects of measurement model on the filter performance are analyzed within the framework of the Extended Kalman filter, also the degrees of nonlinearity of two measurement models are compared using the curvature measure theory from differential geometry. Finally, a simulation of star-tracker-based attitude determination is presented to confirm the superiority of the unit vector measurement model. Simulation results show that the magnitude of curvature nonlinearity measurement is consistent with the filter performance, and the unit vector measurement model yields higher estimation precision and faster convergence properties.

  7. Can standard cosmological models explain the observed Abell cluster bulk flow?

    NASA Technical Reports Server (NTRS)

    Strauss, Michael A.; Cen, Renyue; Ostriker, Jeremiah P.; Laure, Tod R.; Postman, Marc

    1995-01-01

    Lauer and Postman (LP) observed that all Abell clusters with redshifts less than 15,000 km/s appear to be participating in a bulk flow of 689 km/s with respect to the cosmic microwave background. We find this result difficult to reconcile with all popular models for large-scale structure formation that assume Gaussian initial conditions. This conclusion is based on Monte Carlo realizations of the LP data, drawn from large particle-mesh N-body simulations for six different models of the initial power spectrum (standard, tilted, and Omega(sub 0) = 0.3 cold dark matter, and two variants of the primordial baryon isocurvature model). We have taken special care to treat properly the longest-wavelength components of the power spectra. The simulations are sampled, 'observed,' and analyzed as identically as possible to the LP cluster sample. Large-scale bulk flows as measured from clusters in the simulations are in excellent agreement with those measured from the grid: the clusters do not exhibit any strong velocity bias on large scales. Bulk flows with amplitude as large as that reported by LP are not uncommon in the Monte Carlo data stes; the distribution of measured bulk flows before error bias subtraction is rougly Maxwellian, with a peak around 400 km/s. However the chi squared of the observed bulk flow, taking into account the anisotropy of the error ellipsoid, is much more difficult to match in the simulations. The models examined are ruled out at confidence levels between 94% and 98%.

  8. A core observational data model for enhancing the interoperability of ontologically annotated environmental data

    NASA Astrophysics Data System (ADS)

    Schildhauer, M.; Bermudez, L. E.; Bowers, S.; Dibner, P. C.; Gries, C.; Jones, M. B.; McGuinness, D. L.; Cao, H.; Cox, S. J.; Kelling, S.; Lagoze, C.; Lapp, H.; Madin, J.

    2010-12-01

    Research in the environmental sciences often requires accessing diverse data, collected by numerous data providers over varying spatiotemporal scales, incorporating specialized measurements from a range of instruments. These measurements are typically documented using idiosyncratic, disciplinary specific terms, and stored in management systems ranging from desktop spreadsheets to the Cloud, where the information is often further decomposed or stylized in unpredictable ways. This situation creates major informatics challenges for broadly discovering, interpreting, and merging the data necessary for integrative earth science research. A number of scientific disciplines have recognized these issues, and been developing semantically enhanced data storage frameworks, typically based on ontologies, to enable communities to better circumscribe and clarify the content of data objects within their domain of practice. There is concern, however, that cross-domain compatibility of these semantic solutions could become problematic. We describe here our efforts to address this issue by developing a core, unified Observational Data Model, that should greatly facilitate interoperability among the semantic solutions growing organically within diverse scientific domains. Observational Data Models have emerged independently from several distinct scientific communities, including the biodiversity sciences, ecology, evolution, geospatial sciences, and hydrology, to name a few. Informatics projects striving for data integration within each of these domains had converged on identifying "observations" and "measurements" as fundamental abstractions that provide useful "templates" through which scientific data can be linked— at the structural, composited, or even cell value levels— to domain terms stored in ontologies or other forms of controlled vocabularies. The Scientific Observations Network, SONet (http://sonet.ecoinformatics.org) brings together a number of these observational

  9. Measurement of Form-Factor-Independent Observables in the Decay B0→K*0μ+μ-

    NASA Astrophysics Data System (ADS)

    Aaij, R.; Adeva, B.; Adinolfi, M.; Adrover, C.; Affolder, A.; Ajaltouni, Z.; Albrecht, J.; Alessio, F.; Alexander, M.; Ali, S.; Alkhazov, G.; Alvarez Cartelle, P.; Alves, A. A., Jr.; Amato, S.; Amerio, S.; Amhis, Y.; Anderlini, L.; Anderson, J.; Andreassen, R.; Andrews, J. E.; Appleby, R. B.; Aquines Gutierrez, O.; Archilli, F.; Artamonov, A.; Artuso, M.; Aslanides, E.; Auriemma, G.; Baalouch, M.; Bachmann, S.; Back, J. J.; Baesso, C.; Balagura, V.; Baldini, W.; Barlow, R. J.; Barschel, C.; Barsuk, S.; Barter, W.; Bauer, Th.; Bay, A.; Beddow, J.; Bedeschi, F.; Bediaga, I.; Belogurov, S.; Belous, K.; Belyaev, I.; Ben-Haim, E.; Bencivenni, G.; Benson, S.; Benton, J.; Berezhnoy, A.; Bernet, R.; Bettler, M.-O.; van Beuzekom, M.; Bien, A.; Bifani, S.; Bird, T.; Bizzeti, A.; Bjørnstad, P. M.; Blake, T.; Blanc, F.; Blouw, J.; Blusk, S.; Bocci, V.; Bondar, A.; Bondar, N.; Bonivento, W.; Borghi, S.; Borgia, A.; Bowcock, T. J. V.; Bowen, E.; Bozzi, C.; Brambach, T.; van den Brand, J.; Bressieux, J.; Brett, D.; Britsch, M.; Britton, T.; Brook, N. H.; Brown, H.; Burducea, I.; Bursche, A.; Busetto, G.; Buytaert, J.; Cadeddu, S.; Callot, O.; Calvi, M.; Calvo Gomez, M.; Camboni, A.; Campana, P.; Campora Perez, D.; Carbone, A.; Carboni, G.; Cardinale, R.; Cardini, A.; Carranza-Mejia, H.; Carson, L.; Carvalho Akiba, K.; Casse, G.; Castillo Garcia, L.; Cattaneo, M.; Cauet, Ch.; Cenci, R.; Charles, M.; Charpentier, Ph.; Chen, P.; Chiapolini, N.; Chrzaszcz, M.; Ciba, K.; Cid Vidal, X.; Ciezarek, G.; Clarke, P. E. L.; Clemencic, M.; Cliff, H. V.; Closier, J.; Coca, C.; Coco, V.; Cogan, J.; Cogneras, E.; Collins, P.; Comerma-Montells, A.; Contu, A.; Cook, A.; Coombes, M.; Coquereau, S.; Corti, G.; Couturier, B.; Cowan, G. A.; Craik, D. C.; Cunliffe, S.; Currie, R.; D'Ambrosio, C.; David, P.; David, P. N. Y.; Davis, A.; De Bonis, I.; De Bruyn, K.; De Capua, S.; De Cian, M.; De Miranda, J. M.; De Paula, L.; De Silva, W.; De Simone, P.; Decamp, D.; Deckenhoff, M.; Del Buono, L.; Déléage, N.; Derkach, D.; Deschamps, O.; Dettori, F.; Di Canto, A.; Dijkstra, H.; Dogaru, M.; Donleavy, S.; Dordei, F.; Dosil Suárez, A.; Dossett, D.; Dovbnya, A.; Dupertuis, F.; Durante, P.; Dzhelyadin, R.; Dziurda, A.; Dzyuba, A.; Easo, S.; Egede, U.; Egorychev, V.; Eidelman, S.; van Eijk, D.; Eisenhardt, S.; Eitschberger, U.; Ekelhof, R.; Eklund, L.; El Rifai, I.; Elsasser, Ch.; Falabella, A.; Färber, C.; Fardell, G.; Farinelli, C.; Farry, S.; Ferguson, D.; Fernandez Albor, V.; Ferreira Rodrigues, F.; Ferro-Luzzi, M.; Filippov, S.; Fiore, M.; Fitzpatrick, C.; Fontana, M.; Fontanelli, F.; Forty, R.; Francisco, O.; Frank, M.; Frei, C.; Frosini, M.; Furcas, S.; Furfaro, E.; Gallas Torreira, A.; Galli, D.; Gandelman, M.; Gandini, P.; Gao, Y.; Garofoli, J.; Garosi, P.; Garra Tico, J.; Garrido, L.; Gaspar, C.; Gauld, R.; Gersabeck, E.; Gersabeck, M.; Gershon, T.; Ghez, Ph.; Gibson, V.; Giubega, L.; Gligorov, V. V.; Göbel, C.; Golubkov, D.; Golutvin, A.; Gomes, A.; Gorbounov, P.; Gordon, H.; Gotti, C.; Grabalosa Gándara, M.; Graciani Diaz, R.; Granado Cardoso, L. A.; Graugés, E.; Graziani, G.; Grecu, A.; Greening, E.; Gregson, S.; Griffith, P.; Grünberg, O.; Gui, B.; Gushchin, E.; Guz, Yu.; Gys, T.; Hadjivasiliou, C.; Haefeli, G.; Haen, C.; Haines, S. C.; Hall, S.; Hamilton, B.; Hampson, T.; Hansmann-Menzemer, S.; Harnew, N.; Harnew, S. T.; Harrison, J.; Hartmann, T.; He, J.; Head, T.; Heijne, V.; Hennessy, K.; Henrard, P.; Hernando Morata, J. A.; van Herwijnen, E.; Hess, M.; Hicheur, A.; Hicks, E.; Hill, D.; Hoballah, M.; Hombach, C.; Hopchev, P.; Hulsbergen, W.; Hunt, P.; Huse, T.; Hussain, N.; Hutchcroft, D.; Hynds, D.; Iakovenko, V.; Idzik, M.; Ilten, P.; Jacobsson, R.; Jaeger, A.; Jans, E.; Jaton, P.; Jawahery, A.; Jing, F.; John, M.; Johnson, D.; Jones, C. R.; Joram, C.; Jost, B.; Kaballo, M.; Kandybei, S.; Kanso, W.; Karacson, M.; Karbach, T. M.; Kenyon, I. R.; Ketel, T.; Keune, A.; Khanji, B.; Kochebina, O.; Komarov, I.; Koopman, R. F.; Koppenburg, P.; Korolev, M.; Kozlinskiy, A.; Kravchuk, L.; Kreplin, K.; Kreps, M.; Krocker, G.; Krokovny, P.; Kruse, F.; Kucharczyk, M.; Kudryavtsev, V.; Kurek, K.; Kvaratskheliya, T.; La Thi, V. N.; Lacarrere, D.; Lafferty, G.; Lai, A.; Lambert, D.; Lambert, R. W.; Lanciotti, E.; Lanfranchi, G.; Langenbruch, C.; Latham, T.; Lazzeroni, C.; Le Gac, R.; van Leerdam, J.; Lees, J.-P.; Lefèvre, R.; Leflat, A.; Lefrançois, J.; Leo, S.; Leroy, O.; Lesiak, T.; Leverington, B.; Li, Y.; Li Gioi, L.; Liles, M.; Lindner, R.; Linn, C.; Liu, B.; Liu, G.; Lohn, S.; Longstaff, I.; Lopes, J. H.; Lopez-March, N.; Lu, H.; Lucchesi, D.; Luisier, J.; Luo, H.; Machefert, F.; Machikhiliyan, I. V.; Maciuc, F.; Maev, O.; Malde, S.; Manca, G.; Mancinelli, G.; Maratas, J.; Marconi, U.; Marino, P.; Märki, R.; Marks, J.; Martellotti, G.; Martens, A.; Martín Sánchez, A.; Martinelli, M.; Martinez Santos, D.; Martins Tostes, D.; Martynov, A.; Massafferri, A.; Matev, R.; Mathe, Z.; Matteuzzi, C.; Maurice, E.; Mazurov, A.; McCarthy, J.; McNab, A.; McNulty, R.; McSkelly, B.; Meadows, B.; Meier, F.; Meissner, M.; Merk, M.; Milanes, D. A.; Minard, M.-N.; Molina Rodriguez, J.; Monteil, S.; Moran, D.; Morawski, P.; Mordà, A.; Morello, M. J.; Mountain, R.; Mous, I.; Muheim, F.; Müller, K.; Muresan, R.; Muryn, B.; Muster, B.; Naik, P.; Nakada, T.; Nandakumar, R.; Nasteva, I.; Needham, M.; Neubert, S.; Neufeld, N.; Nguyen, A. D.; Nguyen, T. D.; Nguyen-Mau, C.; Nicol, M.; Niess, V.; Niet, R.; Nikitin, N.; Nikodem, T.; Nomerotski, A.; Novoselov, A.; Oblakowska-Mucha, A.; Obraztsov, V.; Oggero, S.; Ogilvy, S.; Okhrimenko, O.; Oldeman, R.; Orlandea, M.; Otalora Goicochea, J. M.; Owen, P.; Oyanguren, A.; Pal, B. K.; Palano, A.; Palczewski, T.; Palutan, M.; Panman, J.; Papanestis, A.; Pappagallo, M.; Parkes, C.; Parkinson, C. J.; Passaleva, G.; Patel, G. D.; Patel, M.; Patrick, G. N.; Patrignani, C.; Pavel-Nicorescu, C.; Pazos Alvarez, A.; Pellegrino, A.; Penso, G.; Pepe Altarelli, M.; Perazzini, S.; Perez Trigo, E.; Pérez-Calero Yzquierdo, A.; Perret, P.; Perrin-Terrin, M.; Pescatore, L.; Pesen, E.; Petridis, K.; Petrolini, A.; Phan, A.; Picatoste Olloqui, E.; Pietrzyk, B.; Pilař, T.; Pinci, D.; Playfer, S.; Plo Casasus, M.; Polci, F.; Polok, G.; Poluektov, A.; Polycarpo, E.; Popov, A.; Popov, D.; Popovici, B.; Potterat, C.; Powell, A.; Prisciandaro, J.; Pritchard, A.; Prouve, C.; Pugatch, V.; Puig Navarro, A.; Punzi, G.; Qian, W.; Rademacker, J. H.; Rakotomiaramanana, B.; Rangel, M. S.; Raniuk, I.; Rauschmayr, N.; Raven, G.; Redford, S.; Reid, M. M.; dos Reis, A. C.; Ricciardi, S.; Richards, A.; Rinnert, K.; Rives Molina, V.; Roa Romero, D. A.; Robbe, P.; Roberts, D. A.; Rodrigues, E.; Rodriguez Perez, P.; Roiser, S.; Romanovsky, V.; Romero Vidal, A.; Rouvinet, J.; Ruf, T.; Ruffini, F.; Ruiz, H.; Ruiz Valls, P.; Sabatino, G.; Saborido Silva, J. J.; Sagidova, N.; Sail, P.; Saitta, B.; Salustino Guimaraes, V.; Sanmartin Sedes, B.; Sannino, M.; Santacesaria, R.; Santamarina Rios, C.; Santovetti, E.; Sapunov, M.; Sarti, A.; Satriano, C.; Satta, A.; Savrie, M.; Savrina, D.; Schaack, P.; Schiller, M.; Schindler, H.; Schlupp, M.; Schmelling, M.; Schmidt, B.; Schneider, O.; Schopper, A.; Schune, M.-H.; Schwemmer, R.; Sciascia, B.; Sciubba, A.; Seco, M.; Semennikov, A.; Senderowska, K.; Sepp, I.; Serra, N.; Serrano, J.; Seyfert, P.; Shapkin, M.; Shapoval, I.; Shatalov, P.; Shcheglov, Y.; Shears, T.; Shekhtman, L.; Shevchenko, O.; Shevchenko, V.; Shires, A.; Silva Coutinho, R.; Sirendi, M.; Skwarnicki, T.; Smith, N. A.; Smith, E.; Smith, J.; Smith, M.; Sokoloff, M. D.; Soler, F. J. P.; Soomro, F.; Souza, D.; Souza De Paula, B.; Spaan, B.; Sparkes, A.; Spradlin, P.; Stagni, F.; Stahl, S.; Steinkamp, O.; Stevenson, S.; Stoica, S.; Stone, S.; Storaci, B.; Straticiuc, M.; Straumann, U.; Subbiah, V. K.; Sun, L.; Swientek, S.; Syropoulos, V.; Szczekowski, M.; Szczypka, P.; Szumlak, T.; T'Jampens, S.; Teklishyn, M.; Teodorescu, E.; Teubert, F.; Thomas, C.; Thomas, E.; van Tilburg, J.; Tisserand, V.; Tobin, M.; Tolk, S.; Tonelli, D.; Topp-Joergensen, S.; Torr, N.; Tournefier, E.; Tourneur, S.; Tran, M. T.; Tresch, M.; Tsaregorodtsev, A.; Tsopelas, P.; Tuning, N.; Ubeda Garcia, M.; Ukleja, A.; Urner, D.; Ustyuzhanin, A.; Uwer, U.; Vagnoni, V.; Valenti, G.; Vallier, A.; Van Dijk, M.; Vazquez Gomez, R.; Vazquez Regueiro, P.; Vázquez Sierra, C.; Vecchi, S.; Velthuis, J. J.; Veltri, M.; Veneziano, G.; Vesterinen, M.; Viaud, B.; Vieira, D.; Vilasis-Cardona, X.; Vollhardt, A.; Volyanskyy, D.; Voong, D.; Vorobyev, A.; Vorobyev, V.; Voß, C.; Voss, H.; Waldi, R.; Wallace, C.; Wallace, R.; Wandernoth, S.; Wang, J.; Ward, D. R.; Watson, N. K.; Webber, A. D.; Websdale, D.; Whitehead, M.; Wicht, J.; Wiechczynski, J.; Wiedner, D.; Wiggers, L.; Wilkinson, G.; Williams, M. P.; Williams, M.; Wilson, F. F.; Wimberley, J.; Wishahi, J.; Wislicki, W.; Witek, M.; Wotton, S. A.; Wright, S.; Wu, S.; Wyllie, K.; Xie, Y.; Xing, Z.; Yang, Z.; Young, R.; Yuan, X.; Yushchenko, O.; Zangoli, M.; Zavertyaev, M.; Zhang, F.; Zhang, L.; Zhang, W. C.; Zhang, Y.; Zhelezov, A.; Zhokhov, A.; Zhong, L.; Zvyagin, A.

    2013-11-01

    We present a measurement of form-factor-independent angular observables in the decay B0→K*(892)0μ+μ-. The analysis is based on a data sample corresponding to an integrated luminosity of 1.0fb-1, collected by the LHCb experiment in pp collisions at a center-of-mass energy of 7 TeV. Four observables are measured in six bins of the dimuon invariant mass squared q2 in the range 0.1model is found for 23 of the 24 measurements. A local discrepancy, corresponding to 3.7 Gaussian standard deviations is observed in one q2 bin for one of the observables. Considering the 24 measurements as independent, the probability to observe such a discrepancy, or larger, in one is 0.5%.

  10. Entanglement measures based on observable correlations

    NASA Astrophysics Data System (ADS)

    Luo, Shunlong

    2008-06-01

    By regarding quantum states as communication channels and using observable correlations quantitatively expressed by mutual information, we introduce a hierarchy of entanglement measures that includes the entanglement of formation as a particular instance. We compare the maximal and minimal measures and indicate the conceptual advantages of the minimal measure over the entanglement of formation. We reveal a curious feature of the entanglement of formation by showing that it can exceed the quantum mutual information, which is usually regarded as a theoretical measure of total correlations. This places the entanglement of formation in a broader scenario, highlights its peculiarity in relation to pure-state ensembles, and introduces a competing definition with intrinsic informational significance.

  11. Probability distributions of molecular observables computed from Markov models. II. Uncertainties in observables and their time-evolution

    NASA Astrophysics Data System (ADS)

    Chodera, John D.; Noé, Frank

    2010-09-01

    Discrete-state Markov (or master equation) models provide a useful simplified representation for characterizing the long-time statistical evolution of biomolecules in a manner that allows direct comparison with experiments as well as the elucidation of mechanistic pathways for an inherently stochastic process. A vital part of meaningful comparison with experiment is the characterization of the statistical uncertainty in the predicted experimental measurement, which may take the form of an equilibrium measurement of some spectroscopic signal, the time-evolution of this signal following a perturbation, or the observation of some statistic (such as the correlation function) of the equilibrium dynamics of a single molecule. Without meaningful error bars (which arise from both approximation and statistical error), there is no way to determine whether the deviations between model and experiment are statistically meaningful. Previous work has demonstrated that a Bayesian method that enforces microscopic reversibility can be used to characterize the statistical component of correlated uncertainties in state-to-state transition probabilities (and functions thereof) for a model inferred from molecular simulation data. Here, we extend this approach to include the uncertainty in observables that are functions of molecular conformation (such as surrogate spectroscopic signals) characterizing each state, permitting the full statistical uncertainty in computed spectroscopic experiments to be assessed. We test the approach in a simple model system to demonstrate that the computed uncertainties provide a useful indicator of statistical variation, and then apply it to the computation of the fluorescence autocorrelation function measured for a dye-labeled peptide previously studied by both experiment and simulation.

  12. Comparison of dark energy models: A perspective from the latest observational data

    NASA Astrophysics Data System (ADS)

    Li, Miao; Li, Xiaodong; Zhang, Xin

    2010-09-01

    We compare some popular dark energy models under the assumption of a flat universe by using the latest observational data including the type Ia supernovae Constitution compilation, the baryon acoustic oscillation measurement from the Sloan Digital Sky Survey, the cosmic microwave background measurement given by the seven-year Wilkinson Microwave Anisotropy Probe observations and the determination of H 0 from the Hubble Space Telescope. Model comparison statistics such as the Bayesian and Akaike information criteria are applied to assess the worth of the models. These statistics favor models that give a good fit with fewer parameters. Based on this analysis, we find that the simplest cosmological constant model that has only one free parameter is still preferred by the current data. For other dynamical dark energy models, we find that some of them, such as the α dark energy, constant w, generalized Chaplygin gas, Chevalliear-Polarski-Linder parametrization, and holographic dark energy models, can provide good fits to the current data, and three of them, namely, the Ricci dark energy, agegraphic dark energy, and Dvali-Gabadadze-Porrati models, are clearly disfavored by the data.

  13. A Modeling Framework for Inference of Surface Emissions Using Mobile Observations

    NASA Astrophysics Data System (ADS)

    Fasoli, B.; Mitchell, L.; Crosman, E.; Mendoza, D. L.; Lin, J. C.

    2016-12-01

    Our ability to quantify surface emissions depends on the precision of observations and the spatial density of measurement networks. Mobile measurement techniques offer a cost effective strategy for quantifying atmospheric conditions over space without requiring a dense network of in-situ sites. However, interpretation of these data and inversion of dispersed measurements to estimate surface emissions can be difficult. We introduce a framework using the Stochastic Time-Inverted Lagrangian Transport (STILT) model that assimilates both spatially resolved observations and an emissions inventory to better estimate surface fluxes. Salt Lake City is a unique laboratory for the study of urban carbon emissions. It is the only U.S. city that utilizes light-rail trains to continuously measure high frequency carbon dioxide (CO2) and methane (CH4); it is home to one of the longest and most spatially resolved high precision CO2 measurement networks (air.utah.edu); and it is one of four cities in the world for which the Hestia anthropogenic emissions inventory has been produced which characterizes CO2 emissions at the scale of individual buildings and roadways. Using these data and modeling resources, we evaluate spatially resolved CO2 measurements and transported CO2 emissions on hourly timescales at a dense spatial resolution across Salt Lake City.

  14. Metrological challenges for measurements of key climatological observables Part 2: oceanic salinity

    NASA Astrophysics Data System (ADS)

    Pawlowicz, R.; Feistel, R.; McDougall, T. J.; Ridout, P.; Seitz, S.; Wolf, H.

    2016-02-01

    Salinity is a key variable in the modelling and observation of ocean circulation and ocean-atmosphere fluxes of heat and water. In this paper, we examine the climatological relevance of ocean salinity, noting fundamental deficiencies in the definition of this key observable, and its lack of a secure foundation in the International System of Units, the SI. The metrological history of salinity is reviewed, problems with its current definitions and measurement practices are analysed, and options for future improvements are discussed in conjunction with the recent seawater standard TEOS-10.

  15. Consistency Between Convection Allowing Model Output and Passive Microwave Satellite Observations

    NASA Astrophysics Data System (ADS)

    Bytheway, J. L.; Kummerow, C. D.

    2018-01-01

    Observations from the Global Precipitation Measurement (GPM) core satellite were used along with precipitation forecasts from the High Resolution Rapid Refresh (HRRR) model to assess and interpret differences between observed and modeled storms. Using a feature-based approach, precipitating objects were identified in both the National Centers for Environmental Prediction Stage IV multisensor precipitation product and HRRR forecast at lead times of 1, 2, and 3 h at valid times corresponding to GPM overpasses. Precipitating objects were selected for further study if (a) the observed feature occurred entirely within the swath of the GPM Microwave Imager (GMI) and (b) the HRRR model predicted it at all three forecast lead times. Output from the HRRR model was used to simulate microwave brightness temperatures (Tbs), which were compared to those observed by the GMI. Simulated Tbs were found to have biases at both the warm and cold ends of the distribution, corresponding to the stratiform/anvil and convective areas of the storms, respectively. Several experiments altered both the simulation microphysics and hydrometeor classification in order to evaluate potential shortcomings in the model's representation of precipitating clouds. In general, inconsistencies between observed and simulated brightness temperatures were most improved when transferring snow water content to supercooled liquid hydrometeor classes.

  16. Updated observational constraints on quintessence dark energy models

    NASA Astrophysics Data System (ADS)

    Durrive, Jean-Baptiste; Ooba, Junpei; Ichiki, Kiyotomo; Sugiyama, Naoshi

    2018-02-01

    The recent GW170817 measurement favors the simplest dark energy models, such as a single scalar field. Quintessence models can be classified in two classes, freezing and thawing, depending on whether the equation of state decreases towards -1 or departs from it. In this paper, we put observational constraints on the parameters governing the equations of state of tracking freezing, scaling freezing, and thawing models using updated data, from the Planck 2015 release, joint light-curve analysis, and baryonic acoustic oscillations. Because of the current tensions on the value of the Hubble parameter H0, unlike previous authors, we let this parameter vary, which modifies significantly the results. Finally, we also derive constraints on neutrino masses in each of these scenarios.

  17. Long-term observations of tropospheric ozone: GAW Measurement Guidelines

    NASA Astrophysics Data System (ADS)

    Tarasova, Oksana; Galbally, Ian E.; Schultz, Martin G.

    2013-04-01

    The Global Atmosphere Watch (GAW) Programme of the World Meteorological Organization (WMO) coordinates long-term observations of the chemical composition and physical properties of the atmosphere which are relevant for understanding of atmospheric chemistry and climate change. Atmospheric observations of reactive gases (tropospheric ozone, carbon monoxide, volatile organic compounds and nitrogen oxides) coordinated by the GAW Programme complement local and regional scale air quality monitoring efforts. As part of the GAW quality assurance (QA) system detailed measurement guidelines for atmospheric trace species are developed by international expert teams at irregular intervals. The most recent report focuses on continuous in-situ measurements of ozone in the troposphere, performed in particular at continental or island sites with altitudes ranging from sea level to mountain tops. Data Quality Objectives (DQOs) are defined for different applications of the data (e.g. trend analysis and verification of global model forecasts). These DQOs include a thorough discussion of the tolerable level of measurement uncertainty and data completeness. The guidelines present the best practices and practical arrangements adopted by the GAW Programme in order to enable the GAW station network to approach or achieve the defined tropospheric ozone DQOs. The document includes information on the selection of station and measurement locations, required skills and training of staff, recommendations on the measurement technique and the necessary equipment to perform highest quality measurements, rules for conducting the measurements, preparing the data and archiving them, and more. Much emphasis is given to discussions about how to ensure the quality of the data through tracing calibrations back to primary standards, proper calibration and data analysis, etc. In the GAW Programme the QA system is implemented through Central Facilities (Central Calibration Laboratories, World and Regional

  18. Examination of Observation Impacts derived from OSEs and Adjoint Models

    NASA Technical Reports Server (NTRS)

    Gelaro, Ronald

    2008-01-01

    With the adjoint of a data assimilation system, the impact of any or all assimilated observations on measures of forecast skill can be estimated accurately and efficiently. The approach allows aggregation of results in terms of individual data types, channels or locations, all computed simultaneously. In this study, adjoint-based estimates of observation impact are compared with results from standard observing system experiments (OSEs) in the NASA Goddard Earth Observing System Model, Version 5 (GEOS-5) GEOS-5 system. The two approaches are shown to provide unique, but complimentary, information. Used together, they reveal both redundancies and dependencies between observing system impacts as observations are added or removed. Understanding these dependencies poses a major challenge for optimizing the use of the current observational network and defining requirements for future observing systems.

  19. Total solar eclipse effects on VLF signals: Observations and modeling

    NASA Astrophysics Data System (ADS)

    Clilverd, Mark A.; Rodger, Craig J.; Thomson, Neil R.; Lichtenberger, János; Steinbach, Péter; Cannon, Paul; Angling, Matthew J.

    During the total solar eclipse observed in Europe on August 11, 1999, measurements were made of the amplitude and phase of four VLF transmitters in the frequency range 16-24 kHz. Five receiver sites were set up, and significant variations in phase and amplitude are reported for 17 paths, more than any previously during an eclipse. Distances from transmitter to receiver ranged from 90 to 14,510 km, although the majority were <2000 km. Typically, positive amplitude changes were observed throughout the whole eclipse period on path lengths <2000 km, while negative amplitude changes were observed on paths >10,000 km. Negative phase changes were observed on most paths, independent of path length. Although there was significant variation from path to path, the typical changes observed were ~3 dB and ~50°. The changes observed were modeled using the Long Wave Propagation Capability waveguide code. Maximum eclipse effects occurred when the Wait inverse scale height parameter β was 0.5 km-1 and the effective ionospheric height parameter H' was 79 km, compared with β=0.43km-1 and H'=71km for normal daytime conditions. The resulting changes in modeled amplitude and phase show good agreement with the majority of the observations. The modeling undertaken provides an interpretation of why previous estimates of height change during eclipses have shown such a range of values. A D region gas-chemistry model was compared with electron concentration estimates inferred from the observations made during the solar eclipse. Quiet-day H' and β parameters were used to define the initial ionospheric profile. The gas-chemistry model was then driven only by eclipse-related solar radiation levels. The calculated electron concentration values at 77 km altitude throughout the period of the solar eclipse show good agreement with the values determined from observations at all times, which suggests that a linear variation in electron production rate with solar ionizing radiation is reasonable

  20. Effect of simultaneous model observation and self-modeling of volleyball skill acquisition.

    PubMed

    Barzouka, Karolina; Bergeles, Nikolaos; Hatziharistos, Dimitris

    2007-02-01

    This study examined the effect of feedback with simultaneous skilled model observation and self-modeling on volleyball skill acquisition. 53 pupils 12 to 15 years old formed two experimental groups and one control group who followed an intervention program with 12 practice sessions for acquisition and retention of how to receive a ball. Groups received different types of feedback before and in the middle of each practice session. Reception performance outcome (score) and technique in every group were assessed before and at the end of the intervention program and during the retention phase. A 3 (Group) x 3 (Measurement Period) multivariate analysis of variance with repeated measures was applied to investigate differences. Results showed equivalent improvement in all three groups at the end of the intervention program. In conclusion, types of augmented feedback from the physical education teacher are effective in acquisition and retention of the skill for reception in volleyball.

  1. Evaluation of Aerosol-cloud Interaction in the GISS Model E Using ARM Observations

    NASA Technical Reports Server (NTRS)

    DeBoer, G.; Bauer, S. E.; Toto, T.; Menon, Surabi; Vogelmann, A. M.

    2013-01-01

    Observations from the US Department of Energy's Atmospheric Radiation Measurement (ARM) program are used to evaluate the ability of the NASA GISS ModelE global climate model in reproducing observed interactions between aerosols and clouds. Included in the evaluation are comparisons of basic meteorology and aerosol properties, droplet activation, effective radius parameterizations, and surface-based evaluations of aerosol-cloud interactions (ACI). Differences between the simulated and observed ACI are generally large, but these differences may result partially from vertical distribution of aerosol in the model, rather than the representation of physical processes governing the interactions between aerosols and clouds. Compared to the current observations, the ModelE often features elevated droplet concentrations for a given aerosol concentration, indicating that the activation parameterizations used may be too aggressive. Additionally, parameterizations for effective radius commonly used in models were tested using ARM observations, and there was no clear superior parameterization for the cases reviewed here. This lack of consensus is demonstrated to result in potentially large, statistically significant differences to surface radiative budgets, should one parameterization be chosen over another.

  2. Modeling the Footprint and Equivalent Radiance Transfer Path Length for Tower-Based Hemispherical Observations of Chlorophyll Fluorescence

    PubMed Central

    Liu, Xinjie; Liu, Liangyun; Hu, Jiaochan; Du, Shanshan

    2017-01-01

    The measurement of solar-induced chlorophyll fluorescence (SIF) is a new tool for estimating gross primary production (GPP). Continuous tower-based spectral observations together with flux measurements are an efficient way of linking the SIF to the GPP. Compared to conical observations, hemispherical observations made with cosine-corrected foreoptic have a much larger field of view and can better match the footprint of the tower-based flux measurements. However, estimating the equivalent radiation transfer path length (ERTPL) for hemispherical observations is more complex than for conical observations and this is a key problem that needs to be addressed before accurate retrieval of SIF can be made. In this paper, we first modeled the footprint of hemispherical spectral measurements and found that, under convective conditions with light winds, 90% of the total radiation came from an FOV of width 72°, which in turn covered 75.68% of the source area of the flux measurements. In contrast, conical spectral observations covered only 1.93% of the flux footprint. Secondly, using theoretical considerations, we modeled the ERTPL of the hemispherical spectral observations made with cosine-corrected foreoptic and found that the ERTPL was approximately equal to twice the sensor height above the canopy. Finally, the modeled ERTPL was evaluated using a simulated dataset. The ERTPL calculated using the simulated data was about 1.89 times the sensor’s height above the target surface, which was quite close to the results for the modeled ERTPL. Furthermore, the SIF retrieved from atmospherically corrected spectra using the modeled ERTPL fitted well with the reference values, giving a relative root mean square error of 18.22%. These results show that the modeled ERTPL was reasonable and that this method is applicable to tower-based hemispherical observations of SIF. PMID:28509843

  3. Inverse modeling of CO2 sources and sinks using satellite observations of CO2 from TES and surface flask measurements

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Nassar, Ray; Jones, DBA; Kulawik, SS

    2011-01-01

    We infer CO2 surface fluxes using satellite observations of mid-tropospheric CO2 from the Tropospheric Emission Spectrometer (TES) and measurements of CO2 from surface flasks in a time-independent inversion analysis based on the GEOS-Chem model. Using TES CO2 observations over oceans, spanning 40 S 40 N, we find that the horizontal and vertical coverage of the TES and flask data are complementary. This complementarity is demonstrated by combining the datasets in a joint inversion, which provides better constraints than from either dataset alone, when a posteriori CO2 distributions are evaluated against independent ship and aircraft CO2 data. In particular, the jointmore » inversion offers improved constraints in the tropics where surface measurements are sparse, such as the tropical forests of South America. Aggregating the annual surface-to-atmosphere fluxes from the joint inversion for the year 2006 yields 1.13 0.21 PgC for the global ocean, 2.77 0.20 PgC for the global land biosphere and 3.90 0.29 PgC for the total global natural flux (defined as the sum of all biospheric, oceanic, and biomass burning contributions but excluding CO2 emissions from fossil fuel combustion). These global ocean and global land fluxes are shown to be near the median of the broad range of values from other inversion results for 2006. To achieve these results, a bias in TES CO2 in the Southern Hemisphere was assessed and corrected using aircraft flask data, and we demonstrate that our results have low sensitivity to variations in the bias correction approach. Overall, this analysis suggests that future carbon data assimilation systems can benefit by integrating in situ and satellite observations of CO2 and that the vertical information provided by satellite observations of mid-tropospheric CO2 combined with measurements of surface CO2, provides an important additional constraint for flux inversions.« less

  4. Location- and lesion-dependent estimation of background tissue complexity for anthropomorphic model observer

    NASA Astrophysics Data System (ADS)

    Avanaki, Ali R. N.; Espig, Kathryn; Knippel, Eddie; Kimpe, Tom R. L.; Xthona, Albert; Maidment, Andrew D. A.

    2016-03-01

    In this paper, we specify a notion of background tissue complexity (BTC) as perceived by a human observer that is suited for use with model observers. This notion of BTC is a function of image location and lesion shape and size. We propose four unsupervised BTC estimators based on: (i) perceived pre- and post-lesion similarity of images, (ii) lesion border analysis (LBA; conspicuous lesion should be brighter than its surround), (iii) tissue anomaly detection, and (iv) mammogram density measurement. The latter two are existing methods we adapt for location- and lesion-dependent BTC estimation. To validate the BTC estimators, we ask human observers to measure BTC as the visibility threshold amplitude of an inserted lesion at specified locations in a mammogram. Both human-measured and computationally estimated BTC varied with lesion shape (from circular to oval), size (from small circular to larger circular), and location (different points across a mammogram). BTCs measured by different human observers are correlated (ρ=0.67). BTC estimators are highly correlated to each other (0.84observers (ρ<=0.81). With change in lesion shape or size, estimated BTC by LBA changes in the same direction as human-measured BTC. A generalization of proposed methods for viewing breast tomosynthesis sequences in cine mode is outlined. The proposed estimators, as-is or customized to a specific human observer, may be used to construct a BTC-aware model observer, with applications such as optimization of contrast-enhanced medical imaging systems, and creation of a diversified image dataset with characteristics of a desired population.

  5. Observing System Simulations for ASCENDS: Synthesizing Science Measurement Requirements (Invited)

    NASA Astrophysics Data System (ADS)

    Kawa, S. R.; Baker, D. F.; Schuh, A. E.; Crowell, S.; Rayner, P. J.; Hammerling, D.; Michalak, A. M.; Wang, J. S.; Eluszkiewicz, J.; Ott, L.; Zaccheo, T.; Abshire, J. B.; Browell, E. V.; Moore, B.; Crisp, D.

    2013-12-01

    The measurement of atmospheric CO2 from space using active (lidar) sensing techniques has several potentially significant advantages in comparison to current and planned passive CO2 instruments. Application of this new technology aims to advance CO2 measurement capability and carbon cycle science into the next decade. The NASA Active Sensing of Carbon Emissions, Nights, Days, and Seasons (ASCENDS) mission has been recommended by the US National Academy of Sciences Decadal Survey for the next generation of space-based CO2 observing systems. ASCENDS is currently planned for launch in 2022. Several possible lidar instrument approaches have been demonstrated in airborne campaigns and the results indicate that such sensors are quite feasible. Studies are now underway to evaluate performance requirements for space mission implementation. Satellite CO2 observations must be highly precise and unbiased in order to accurately infer global carbon source/sink fluxes. Measurement demands are likely to further increase in the wake of GOSAT, OCO-2, and enhanced ground-based in situ and remote sensing CO2 data. The objective of our work is to quantitatively and consistently evaluate the measurement capabilities and requirements for ASCENDS in the context of advancing our knowledge of carbon flux distributions and their dependence on underlying physical processes. Considerations include requirements for precision, relative accuracy, spatial/temporal coverage and resolution, vertical information content, interferences, and possibly the tradeoffs among these parameters, while at the same time framing a mission that can be implemented within a constrained budget. Here, we attempt to synthesize the results of observing system simulation studies, commissioned by the ASCENDS Science Requirements Definition Team, into a coherent set of mission performance guidelines. A variety of forward and inverse model frameworks are employed to reduce the potential dependence of the results on model

  6. Global Atmosphere Watch Workshop on Measurement-Model ...

    EPA Pesticide Factsheets

    The World Meteorological Organization’s (WMO) Global Atmosphere Watch (GAW) Programme coordinates high-quality observations of atmospheric composition from global to local scales with the aim to drive high-quality and high-impact science while co-producing a new generation of products and services. In line with this vision, GAW’s Scientific Advisory Group for Total Atmospheric Deposition (SAG-TAD) has a mandate to produce global maps of wet, dry and total atmospheric deposition for important atmospheric chemicals to enable research into biogeochemical cycles and assessments of ecosystem and human health effects. The most suitable scientific approach for this activity is the emerging technique of measurement-model fusion for total atmospheric deposition. This technique requires global-scale measurements of atmospheric trace gases, particles, precipitation composition and precipitation depth, as well as predictions of the same from global/regional chemical transport models. The fusion of measurement and model results requires data assimilation and mapping techniques. The objective of the GAW Workshop on Measurement-Model Fusion for Global Total Atmospheric Deposition (MMF-GTAD), an initiative of the SAG-TAD, was to review the state-of-the-science and explore the feasibility and methodology of producing, on a routine retrospective basis, global maps of atmospheric gas and aerosol concentrations as well as wet, dry and total deposition via measurement-model

  7. Comparison of land surface humidity between observations and CMIP5 models

    NASA Astrophysics Data System (ADS)

    Dunn, Robert J. H.; Willett, Kate M.; Ciavarella, Andrew; Stott, Peter A.

    2017-08-01

    We compare the latest observational land surface humidity dataset, HadISDH, with the latest generation of climate models extracted from the CMIP5 archive and the ERA-Interim reanalysis over the period 1973 to present. The globally averaged behaviour of HadISDH and ERA-Interim are very similar in both humidity measures and air temperature, on decadal and interannual timescales. The global average relative humidity shows a gradual increase from 1973 to 2000, followed by a steep decline in recent years. The observed specific humidity shows a steady increase in the global average during the early period but in the later period it remains approximately constant. None of the CMIP5 models or experiments capture the observed behaviour of the relative or specific humidity over the entire study period. When using an atmosphere-only model, driven by observed sea surface temperatures and radiative forcing changes, the behaviour of regional average temperature and specific humidity are better captured, but there is little improvement in the relative humidity. Comparing the observed climatologies with those from historical model runs shows that the models are generally cooler everywhere, are drier and less saturated in the tropics and extra-tropics, and have comparable moisture levels but are more saturated in the high latitudes. The spatial pattern of linear trends is relatively similar between the models and HadISDH for temperature and specific humidity, but there are large differences for relative humidity, with less moistening shown in the models over the tropics and very little at high latitudes. The observed drying in mid-latitudes is present at a much lower magnitude in the CMIP5 models. Relationships between temperature and humidity anomalies (T-q and T-rh) show good agreement for specific humidity between models and observations, and between the models themselves, but much poorer for relative humidity. The T-q correlation from the models is more steeply positive than

  8. Inverse modelling of radionuclide release rates using gamma dose rate observations

    NASA Astrophysics Data System (ADS)

    Hamburger, Thomas; Stohl, Andreas; von Haustein, Christoph; Thummerer, Severin; Wallner, Christian

    2014-05-01

    Severe accidents in nuclear power plants such as the historical accident in Chernobyl 1986 or the more recent disaster in the Fukushima Dai-ichi nuclear power plant in 2011 have drastic impacts on the population and environment. The hazardous consequences reach out on a national and continental scale. Environmental measurements and methods to model the transport and dispersion of the released radionuclides serve as a platform to assess the regional impact of nuclear accidents - both, for research purposes and, more important, to determine the immediate threat to the population. However, the assessments of the regional radionuclide activity concentrations and the individual exposure to radiation dose underlie several uncertainties. For example, the accurate model representation of wet and dry deposition. One of the most significant uncertainty, however, results from the estimation of the source term. That is, the time dependent quantification of the released spectrum of radionuclides during the course of the nuclear accident. The quantification of the source terms of severe nuclear accidents may either remain uncertain (e.g. Chernobyl, Devell et al., 1995) or rely on rather rough estimates of released key radionuclides given by the operators. Precise measurements are mostly missing due to practical limitations during the accident. Inverse modelling can be used to realise a feasible estimation of the source term (Davoine and Bocquet, 2007). Existing point measurements of radionuclide activity concentrations are therefore combined with atmospheric transport models. The release rates of radionuclides at the accident site are then obtained by improving the agreement between the modelled and observed concentrations (Stohl et al., 2012). The accuracy of the method and hence of the resulting source term depends amongst others on the availability, reliability and the resolution in time and space of the observations. Radionuclide activity concentrations are observed on a

  9. Analysis and modeling of tropical convection observed by CYGNSS

    NASA Astrophysics Data System (ADS)

    Lang, T. J.; Li, X.; Roberts, J. B.; Mecikalski, J. R.

    2017-12-01

    The Cyclone Global Navigation Satellite System (CYGNSS) is a multi-satellite constellation that utilizes Global Positioning System (GPS) reflectometry to retrieve near-surface wind speeds over the ocean. While CYGNSS is primarily aimed at measuring wind speeds in tropical cyclones, our research has established that the mission may also provide valuable insight into the relationships between wind-driven surface fluxes and general tropical oceanic convection. Currently, we are examining organized tropical convection using a mixture of CYGNSS level 1 through level 3 data, IMERG (Integrated Multi-satellite Retrievals for Global Precipitation Measurement), and other ancillary datasets (including buoys, GPM level 1 and 2 data, as well as ground-based radar). In addition, observing system experiments (OSEs) are being performed using hybrid three-dimensional variational assimilation to ingest CYGNSS observations into a limited-domain, convection-resolving model. Our focus for now is on case studies of convective evolution, but we will also report on progress toward statistical analysis of convection sampled by CYGNSS. Our working hypothesis is that the typical mature phase of organized tropical convection is marked by the development of a sharp gust-front boundary from an originally spatially broader but weaker wind speed change associated with precipitation. This increase in the wind gradient, which we demonstrate is observable by CYGNSS, likely helps to focus enhanced turbulent fluxes of convection-sustaining heat and moisture near the leading edge of the convective system where they are more easily ingested by the updraft. Progress on the testing and refinement of this hypothesis, using a mixture of observations and modeling, will be reported.

  10. Observation of the diphoton decay of the Higgs boson and measurement of its properties

    DOE PAGES

    Khachatryan, A. M.

    2014-10-15

    Observation of the diphoton decay mode of the recently discovered Higgs boson and measurement of some of its properties are reported. The analysis uses the entire dataset collected by the CMS experiment in proton-proton collisions during the 2011 and 2012 LHC running periods. The data samples correspond to integrated luminosities of 5.1fb -1 at √s=7 TeV and 19.7fb -1 at 8TeV. A clear signal is observed in the diphoton channel at a mass close to 125GeV with a local significance of 5.7σ, where a significance of 5.2σ is expected for the standard model Higgs boson. The mass is measured tomore » be 124.70 ± 0.34 GeV = 124.70 ± 0.31(stat) ± 0.15(syst) GeV, and the best-fit signal strength relative to the standard model prediction is 1.14 +0.26 –0.23 = 1.14 ± 0.21(stat) +0.09 –0.05(syst) +0.13 –0.09(theo). Thus, additional measurements include the signal strength modifiers associated with different production mechanisms, and hypothesis tests between spin-0 and spin-2 models.« less

  11. Intercomparison of middle-atmospheric wind in observations and models

    NASA Astrophysics Data System (ADS)

    Rüfenacht, Rolf; Baumgarten, Gerd; Hildebrand, Jens; Schranz, Franziska; Matthias, Vivien; Stober, Gunter; Lübken, Franz-Josef; Kämpfer, Niklaus

    2018-04-01

    Wind profile information throughout the entire upper stratosphere and lower mesosphere (USLM) is important for the understanding of atmospheric dynamics but became available only recently, thanks to developments in remote sensing techniques and modelling approaches. However, as wind measurements from these altitudes are rare, such products have generally not yet been validated with (other) observations. This paper presents the first long-term intercomparison of wind observations in the USLM by co-located microwave radiometer and lidar instruments at Andenes, Norway (69.3° N, 16.0° E). Good correspondence has been found at all altitudes for both horizontal wind components for nighttime as well as daylight conditions. Biases are mostly within the random errors and do not exceed 5-10 m s-1, which is less than 10 % of the typically encountered wind speeds. Moreover, comparisons of the observations with the major reanalyses and models covering this altitude range are shown, in particular with the recently released ERA5, ECMWF's first reanalysis to cover the whole USLM region. The agreement between models and observations is very good in general, but temporally limited occurrences of pronounced discrepancies (up to 40 m s-1) exist. In the article's Appendix the possibility of obtaining nighttime wind information about the mesopause region by means of microwave radiometry is investigated.

  12. Halo Coronal Mass Ejections: Comparing Observations and Models

    NASA Technical Reports Server (NTRS)

    Gilbert, Holly; Orlove, Matthew; SaintCyr, O.; Mays, L.; Gopalswamy, N.

    2011-01-01

    Since 1996, the SOHO LASCO coronagraphs have detected "halo" CMEs that appear to be directed toward Earth, but information about the size and speed of these events seen face-on has been limited. From a single vantage point along the Sun-Earth line, the primary limitation has been ambiguity in fitting the cone model (or other forward-modeling techniques, e.g., Thernisian et al., 2006). But in the past few years, the STEREO mission has provided a view of Earth-directed events from the side. These events offer the opportunity to compare measurements (width and speed) of halo CMEs observed by STEREO with models that derive halo CME properties. We report here results of such a comparison on a large sample of LASCO CMEs in the STEREO era.

  13. Which measurement strategies to improve spatial erosion and deposition patterns modelling?

    NASA Astrophysics Data System (ADS)

    Pineux, Nathalie; Maugnard, Alexandre; Swerts, Gilles; Bielders, Charles; Degré, Aurore

    2014-05-01

    Validation of the erosion models requires field data. To date, many authors continue to highlight the paucity of accurate field observations and long-term enough studies. The fields observations are often put aside because these measures are difficult to obtain: weighty experimental devices, climatic dependence, … Hence the models are evolving and propose refined calculation procedures including for instance the calculation of landscape evolution. The need of field data therefore increases and new measuring strategies should arise. In the centre of Belgium we choose an agricultural watershed quite representative of the local context. It covers 124 ha of loamy soil with more than 90% of arable land and a weak proportion of forest and artificial lands. The slope ranges between 0 and 9%. Instrumentation on the watershed includes meteorological observations and discharge measurement coupled with water sampling at different outlets. The weather data (radiation, temperature, wind velocity, relative humidity and rainfall) and discharge measurement (comparison between Doppler and pressure sensors) will allow us to model the hydrological behaviour of the catchment. Rainfall readings (tipping buckets) are completed with erosivity readings (disdrometer). Erosivity, together with soil data, land use and agricultural practices observations on field, will be used as entry in the Landsoil model. The sediment samplings at 3 points in the catchment will give an insight of the sediment delivery of 3 subcatchments. The Landsoil model calculates the evolution of the DTM through time. This cannot be compared to measurements at the outlet and requires further data collection. Older elevation data and/or archaeological data are a possible source of information even if their precision remains scarce in our context. 1950's soil surveys are on the contrary really informative since they detail the horizons depth in a spatial way and can be compared to new observation across the watershed

  14. Rotational Motions from Teleseismic Events - Modelling and Observations

    NASA Astrophysics Data System (ADS)

    Schuberth, B.; Igel, H.; Wassermann, J.; Cochard, A.; Schreiber, U.

    2004-12-01

    Currently only ring lasers technology is capable of recording rotational motions resulting from earthquakes with a sensitivity and frequency band that are interesting for broadband seismology. One of those instruments is located at the Geodetic observatory in Wettzell/Germany. Here we present theoretical studies of rotational motions simulated with different Earth models and comparisons with several observations at the Wettzell ring laser. The 3-D global simulations were performed with the Spectral Element Method (Komatitsch and Tromp 2002a,b), that was modified to also allow the output of rotational seismograms. The Earth models used in these simulations range from simple radially symmetric ones, such as PREM, to more complex models including 3D velocity structures, attenuation and geometric effects like topography and bathymetry. Thus, by comparison of the theoretical rotation rates with the ring laser data we show how the results converge to the observed rotation rates when using more realistic Earth models. In a second step we compare rotation rates to the transverse component of translational acceleration both obtained from simulations with 3D velocity structures in crust and mantle. As expected from theory - under the assumption of plane wave propagation - those two signals should be in phase and scale linearly with the phase velocity. Using this relation, it is possible to determine the local phase velocity of transverse signals from collocated measurments of rotations and transverse accelerations. We compare the estimated phase velocities with those observed in a temporary seismic array installed around the ring laser.

  15. Pitfalls in alignment of observation models resolved using PROV as an upper ontology

    NASA Astrophysics Data System (ADS)

    Cox, S. J. D.

    2015-12-01

    A number of models for observation metadata have been developed in the earth and environmental science communities, including OGC's Observations and Measurements (O&M), the ecosystems community's Extensible Observation Ontology (OBOE), the W3C's Semantic Sensor Network Ontology (SSNO), and the CUAHSI/NSF Observations Data Model v2 (ODM2). In order to combine data formalized in the various models, mappings between these must be developed. In some cases this is straightforward: since ODM2 took O&M as its starting point, their terminology is almost completely aligned. In the eco-informatics world observations are almost never made in isolation of other observations, so OBOE pays particular attention to groupings, with multiple atomic 'Measurements' in each oboe:Observation which does not have a result of its own and thus plays a different role to an om:Observation. And while SSN also adopted terminology from O&M, mapping is confounded by the fact that SSN uses DOLCE as its foundation and places ssn:Observations as 'Social Objects' which are explicitly disjoint from 'Events', while O&M is formalized as part of the ISO/TC 211 harmonised (UML) model and sees om:Observations as value assignment activities. Foundational ontologies (such as BFO, GFO, UFO or DOLCE) can provide a framework for alignment, but different upper ontologies can be based in profoundly different worldviews and use of incommensurate frameworks can confound rather than help. A potential resolution is provided by comparing recent studies that align SSN and O&M, respectively, with the PROV-O ontology. PROV-O provides just three base classes: Entity, Activity and Agent. om:Observation is sub-classed from prov:Activity, while ssn:Observation is sub-classed from prov:Entity. This confirms that, despite the same name, om:Observation and ssn:Observation denote different aspects of the observation process: the observation event, and the record of the observation event, respectively. Alignment with the simple

  16. ANALYSIS AND MODELING OF TWO FLARE LOOPS OBSERVED BY AIA AND EIS

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Li, Y.; Ding, M. D.; Qiu, J.

    2012-10-10

    We analyze and model an M1.0 flare observed by SDO/AIA and Hinode/EIS to investigate how flare loops are heated and evolve subsequently. The flare is composed of two distinctive loop systems observed in extreme ultraviolet (EUV) images. The UV 1600 A emission at the feet of these loops exhibits a rapid rise, followed by enhanced emission in different EUV channels observed by the Atmospheric Imaging Assembly (AIA) and the EUV Imaging Spectrometer (EIS). Such behavior is indicative of impulsive energy deposit and the subsequent response in overlying coronal loops that evolve through different temperatures. Using the method we recently developed,more » we infer empirical heating functions from the rapid rise of the UV light curves for the two loop systems, respectively, treating them as two big loops with cross-sectional area of 5'' by 5'', and compute the plasma evolution in the loops using the EBTEL model. We compute the synthetic EUV light curves, which, with the limitation of the model, reasonably agree with observed light curves obtained in multiple AIA channels and EIS lines: they show the same evolution trend and their magnitudes are comparable by within a factor of two. Furthermore, we also compare the computed mean enthalpy flow velocity with the Doppler shift measurements by EIS during the decay phase of the two loops. Our results suggest that the two different loops with different heating functions as inferred from their footpoint UV emission, combined with their different lengths as measured from imaging observations, give rise to different coronal plasma evolution patterns captured both in the model and in observations.« less

  17. Networked high-speed auroral observations combined with radar measurements for multi-scale insights

    NASA Astrophysics Data System (ADS)

    Hirsch, M.; Semeter, J. L.

    2015-12-01

    Networks of ground-based instruments to study terrestrial aurora for the purpose of analyzing particle precipitation characteristics driving the aurora have been established. Additional funding is pouring into future ground-based auroral observation networks consisting of combinations of tossable, portable, and fixed installation ground-based legacy equipment. Our approach to this problem using the High Speed Tomography (HiST) system combines tightly-synchronized filtered auroral optical observations capturing temporal features of order 10 ms with supporting measurements from incoherent scatter radar (ISR). ISR provides a broader spatial context up to order 100 km laterally on one minute time scales, while our camera field of view (FOV) is chosen to be order 10 km at auroral altitudes in order to capture 100 m scale lateral auroral features. The dual-scale observations of ISR and HiST fine-scale optical observations may be coupled through a physical model using linear basis functions to estimate important ionospheric quantities such as electron number density in 3-D (time, perpendicular and parallel to the geomagnetic field).Field measurements and analysis using HiST and PFISR are presented from experiments conducted at the Poker Flat Research Range in central Alaska. Other multiscale configuration candidates include supplementing networks of all-sky cameras such as THEMIS with co-locations of HiST-like instruments to fuse wide FOV measurements with the fine-scale HiST precipitation characteristic estimates. Candidate models for this coupling include GLOW and TRANSCAR. Future extensions of this work may include incorporating line of sight total electron count estimates from ground-based networks of GPS receivers in a sensor fusion problem.

  18. Theory and observations: Model simulations of the period 1955-1985

    NASA Technical Reports Server (NTRS)

    Isaksen, Ivar S. A.; Eckman, R.; Lacis, A.; Ko, Malcolm K. W.; Prather, M.; Pyle, J.; Rodhe, H.; Stordal, Frode; Stolarski, R. S.; Turco, R. P.

    1989-01-01

    The main objective of the theoretical studies presented here is to apply models of stratospheric chemistry and transport in order to understand the processes that control stratospheric ozone and that are responsible for the observed variations. The model calculations are intended to simulate the observed behavior of atmospheric ozone over the past three decades (1955-1985), for which there exists a substantial record of both ground-based and, more recently, satellite measurements. Ozone concentrations in the atmosphere vary on different time scales and for several different causes. The models described here were designed to simulate the effect on ozone of changes in the concentration of such trace gases as CFC, CH4, N2O, and CO2. Changes from year to year in ultraviolet radiation associated with the solar cycle are also included in the models. A third source of variability explicitly considered is the sporadic introduction of large amounts of NO sub x into the stratosphere during atmospheric nuclear tests.

  19. Observation and mass measurement of the baryon Xib-.

    PubMed

    Aaltonen, T; Abulencia, A; Adelman, J; Affolder, T; Akimoto, T; Albrow, M G; Amerio, S; Amidei, D; Anastassov, A; Anikeev, K; Annovi, A; Antos, J; Aoki, M; Apollinari, G; Arisawa, T; Artikov, A; Ashmanskas, W; Attal, A; Aurisano, A; Azfar, F; Azzi-Bacchetta, P; Azzurri, P; Bacchetta, N; Badgett, W; Barbaro-Galtieri, A; Barnes, V E; Barnett, B A; Baroiant, S; Bartsch, V; Bauer, G; Beauchemin, P-H; Bedeschi, F; Behari, S; Bellettini, G; Bellinger, J; Belloni, A; Benjamin, D; Beretvas, A; Beringer, J; Berry, T; Bhatti, A; Binkley, M; Bisello, D; Bizjak, I; Blair, R E; Blocker, C; Blumenfeld, B; Bocci, A; Bodek, A; Boisvert, V; Bolla, G; Bolshov, A; Bortoletto, D; Boudreau, J; Boveia, A; Brau, B; Brigliadori, L; Bromberg, C; Brubaker, E; Budagov, J; Budd, H S; Budd, S; Burkett, K; Busetto, G; Bussey, P; Buzatu, A; Byrum, K L; Cabrera, S; Campanelli, M; Campbell, M; Canelli, F; Canepa, A; Carrillo, S; Carlsmith, D; Carosi, R; Carron, S; Casal, B; Casarsa, M; Castro, A; Catastini, P; Cauz, D; Cavalli-Sforza, M; Cerri, A; Cerrito, L; Chang, S H; Chen, Y C; Chertok, M; Chiarelli, G; Chlachidze, G; Chlebana, F; Cho, I; Cho, K; Chokheli, D; Chou, J P; Choudalakis, G; Chuang, S H; Chung, K; Chung, W H; Chung, Y S; Cilijak, M; Ciobanu, C I; Ciocci, M A; Clark, A; Clark, D; Coca, M; Compostella, G; Convery, M E; Conway, J; Cooper, B; Copic, K; Cordelli, M; Cortiana, G; Crescioli, F; Cuenca Almenar, C; Cuevas, J; Culbertson, R; Cully, J C; DaRonco, S; Datta, M; D'Auria, S; Davies, T; Dagenhart, D; de Barbaro, P; De Cecco, S; Deisher, A; De Lentdecker, G; De Lorenzo, G; Dell'Orso, M; Delli Paoli, F; Demortier, L; Deng, J; Deninno, M; De Pedis, D; Derwent, P F; Di Giovanni, G P; Dionisi, C; Di Ruzza, B; Dittmann, J R; D'Onofrio, M; Dörr, C; Donati, S; Dong, P; Donini, J; Dorigo, T; Dube, S; Efron, J; Erbacher, R; Errede, D; Errede, S; Eusebi, R; Fang, H C; Farrington, S; Fedorko, I; Fedorko, W T; Feild, R G; Feindt, M; Fernandez, J P; Field, R; Flanagan, G; Forrest, R; Forrester, S; Franklin, M; Freeman, J C; Furic, I; Gallinaro, M; Galyardt, J; Garcia, J E; Garberson, F; Garfinkel, A F; Gay, C; Gerberich, H; Gerdes, D; Giagu, S; Giannetti, P; Gibson, K; Gimmell, J L; Ginsburg, C; Giokaris, N; Giordani, M; Giromini, P; Giunta, M; Giurgiu, G; Glagolev, V; Glenzinski, D; Gold, M; Goldschmidt, N; Goldstein, J; Golossanov, A; Gomez, G; Gomez-Ceballos, G; Goncharov, M; González, O; Gorelov, I; Goshaw, A T; Goulianos, K; Gresele, A; Grinstein, S; Grosso-Pilcher, C; Group, R C; Grundler, U; Guimaraes da Costa, J; Gunay-Unalan, Z; Haber, C; Hahn, K; Hahn, S R; Halkiadakis, E; Hamilton, A; Han, B-Y; Han, J Y; Handler, R; Happacher, F; Hara, K; Hare, D; Hare, M; Harper, S; Harr, R F; Harris, R M; Hartz, M; Hatakeyama, K; Hauser, J; Hays, C; Heck, M; Heijboer, A; Heinemann, B; Heinrich, J; Henderson, C; Herndon, M; Heuser, J; Hidas, D; Hill, C S; Hirschbuehl, D; Hocker, A; Holloway, A; Hou, S; Houlden, M; Hsu, S-C; Huffman, B T; Hughes, R E; Husemann, U; Huston, J; Incandela, J; Introzzi, G; Iori, M; Ivanov, A; Iyutin, B; James, E; Jang, D; Jayatilaka, B; Jeans, D; Jeon, E J; Jindariani, S; Johnson, W; Jones, M; Joo, K K; Jun, S Y; Jung, J E; Junk, T R; Kamon, T; Karchin, P E; Kato, Y; Kemp, Y; Kephart, R; Kerzel, U; Khotilovich, V; Kilminster, B; Kim, D H; Kim, H S; Kim, J E; Kim, M J; Kim, S B; Kim, S H; Kim, Y K; Kimura, N; Kirsch, L; Klimenko, S; Klute, M; Knuteson, B; Ko, B R; Kondo, K; Kong, D J; Konigsberg, J; Korytov, A; Kotwal, A V; Kraan, A C; Kraus, J; Kreps, M; Kroll, J; Krumnack, N; Kruse, M; Krutelyov, V; Kubo, T; Kuhlmann, S E; Kuhr, T; Kulkarni, N P; Kusakabe, Y; Kwang, S; Laasanen, A T; Lai, S; Lami, S; Lammel, S; Lancaster, M; Lander, R L; Lannon, K; Lath, A; Latino, G; Lazzizzera, I; LeCompte, T; Lee, J; Lee, J; Lee, Y J; Lee, S W; Lefèvre, R; Leonardo, N; Leone, S; Levy, S; Lewis, J D; Lin, C; Lin, C S; Lindgren, M; Lipeles, E; Lister, A; Litvintsev, D O; Liu, T; Lockyer, N S; Loginov, A; Loreti, M; Lu, R-S; Lucchesi, D; Lujan, P; Lukens, P; Lungu, G; Lyons, L; Lys, J; Lysak, R; Lytken, E; Mack, P; MacQueen, D; Madrak, R; Maeshima, K; Makhoul, K; Maki, T; Maksimovic, P; Malde, S; Malik, S; Manca, G; Manousakis, A; Margaroli, F; Marginean, R; Marino, C; Marino, C P; Martin, A; Martin, M; Martin, V; Martínez, M; Martínez-Ballarín, R; Maruyama, T; Mastrandrea, P; Masubuchi, T; Matsunaga, H; Mattson, M E; Mazini, R; Mazzanti, P; McFarland, K S; McIntyre, P; McNulty, R; Mehta, A; Mehtala, P; Menzemer, S; Menzione, A; Merkel, P; Mesropian, C; Messina, A; Miao, T; Miladinovic, N; Miles, J; Miller, R; Mills, C; Milnik, M; Mitra, A; Mitselmakher, G; Miyamoto, A; Moed, S; Moggi, N; Mohr, B; Moon, C S; Moore, R; Morello, M; Movilla Fernandez, P; Mülmenstädt, J; Mukherjee, A; Muller, Th; Mumford, R; Murat, P; Mussini, M; Nachtman, J; Nagano, A; Naganoma, J; Nakamura, K; Nakano, I; Napier, A; Necula, V; Neu, C; Neubauer, M S; Nielsen, J; Nodulman, L; Norniella, O; Nurse, E; Oh, S H; Oh, Y D; Oksuzian, I; Okusawa, T; Oldeman, R; Orava, R; Osterberg, K; Pagliarone, C; Palencia, E; Papadimitriou, V; Papaikonomou, A; Paramonov, A A; Parks, B; Pashapour, S; Patrick, J; Pauletta, G; Paulini, M; Paus, C; Pellett, D E; Penzo, A; Phillips, T J; Piacentino, G; Piedra, J; Pinera, L; Pitts, K; Plager, C; Pondrom, L; Portell, X; Poukhov, O; Pounder, N; Prakoshyn, F; Pronko, A; Proudfoot, J; Ptohos, F; Punzi, G; Pursley, J; Rademacker, J; Rahaman, A; Ramakrishnan, V; Ranjan, N; Redondo, I; Reisert, B; Rekovic, V; Renton, P; Rescigno, M; Richter, S; Rimondi, F; Ristori, L; Robson, A; Rodrigo, T; Rogers, E; Rolli, S; Roser, R; Rossi, M; Rossin, R; Roy, P; Ruiz, A; Russ, J; Rusu, V; Saarikko, H; Safonov, A; Sakumoto, W K; Salamanna, G; Saltó, O; Santi, L; Sarkar, S; Sartori, L; Sato, K; Savard, P; Savoy-Navarro, A; Scheidle, T; Schlabach, P; Schmidt, E E; Schmidt, M P; Schmitt, M; Schwarz, T; Scodellaro, L; Scott, A L; Scribano, A; Scuri, F; Sedov, A; Seidel, S; Seiya, Y; Semenov, A; Sexton-Kennedy, L; Sfyrla, A; Shalhout, S Z; Shapiro, M D; Shears, T; Shepard, P F; Sherman, D; Shimojima, M; Shochet, M; Shon, Y; Shreyber, I; Sidoti, A; Sinervo, P; Sisakyan, A; Slaughter, A J; Slaunwhite, J; Sliwa, K; Smith, J R; Snider, F D; Snihur, R; Soderberg, M; Soha, A; Somalwar, S; Sorin, V; Spalding, J; Spinella, F; Spreitzer, T; Squillacioti, P; Stanitzki, M; Staveris-Polykalas, A; St Denis, R; Stelzer, B; Stelzer-Chilton, O; Stentz, D; Strologas, J; Stuart, D; Suh, J S; Sukhanov, A; Sun, H; Suslov, I; Suzuki, T; Taffard, A; Takashima, R; Takeuchi, Y; Tanaka, R; Tecchio, M; Teng, P K; Terashi, K; Thom, J; Thompson, A S; Thomson, E; Tipton, P; Tiwari, V; Tkaczyk, S; Toback, D; Tokar, S; Tollefson, K; Tomura, T; Tonelli, D; Torre, S; Torretta, D; Tourneur, S; Trischuk, W; Tsuno, S; Tu, Y; Turini, N; Ukegawa, F; Uozumi, S; Vallecorsa, S; van Remortel, N; Varganov, A; Vataga, E; Vazquez, F; Velev, G; Vellidis, C; Veramendi, G; Veszpremi, V; Vidal, M; Vidal, R; Vila, I; Vilar, R; Vine, T; Vogel, M; Vollrath, I; Volobouev, I; Volpi, G; Würthwein, F; Wagner, P; Wagner, R G; Wagner, R L; Wagner, J; Wagner, W; Wallny, R; Wang, S M; Warburton, A; Waters, D; Weinberger, M; Wester, W C; Whitehouse, B; Whiteson, D; Wicklund, A B; Wicklund, E; Williams, G; Williams, H H; Wilson, P; Winer, B L; Wittich, P; Wolbers, S; Wolfe, C; Wright, T; Wu, X; Wynne, S M; Yagil, A; Yamamoto, K; Yamaoka, J; Yamashita, T; Yang, C; Yang, U K; Yang, Y C; Yao, W M; Yeh, G P; Yoh, J; Yorita, K; Yoshida, T; Yu, G B; Yu, I; Yu, S S; Yun, J C; Zanello, L; Zanetti, A; Zaw, I; Zhang, X; Zhou, J; Zucchelli, S

    2007-08-03

    We report the observation and measurement of the mass of the bottom, strange baryon Xi(b)- through the decay chain Xi(b)- -->J/psiXi-, where J/psi-->mu+mu-, Xi- -->Lambdapi-, and Lambda-->ppi-. A signal is observed whose probability of arising from a background fluctuation is 6.6 x 10(-15), or 7.7 Gaussian standard deviations. The Xi(b)- mass is measured to be 5792.9+/-2.5(stat) +/- 1.7(syst) MeV/c2.

  20. Optical properties of soot particles: measurement - model comparison

    NASA Astrophysics Data System (ADS)

    Forestieri, S.; Lambe, A. T.; Lack, D.; Massoli, P.; Cross, E. S.; Dubey, M.; Mazzoleni, C.; Olfert, J.; Freedman, A.; Davidovits, P.; Onasch, T. B.; Cappa, C. D.

    2013-12-01

    Soot, a product of incomplete combustion, plays an important role in the earth's climate system through the absorption and scattering of solar radiation. In order to accurately model the direct radiative impact of black carbon (BC), the refractive index and shape dependent scattering and absorption characteristics must be known. At present, the assumed shape remains highly uncertain because BC particles are fractal-like, being agglomerates of smaller (20-40 nm) spherules, yet traditional optical models such as Mie theory typically assume a spherical particle morphology. To investigate the ability of various optical models to reproduce observed BC optical properties, we measured light absorption and extinction coefficients of methane and ethylene flame soot particles. Optical properties were measured by multiple instruments: absorption by a dual cavity ringdown photoacoustic spectrometer (CRD-PAS), absorption and scattering by a 3-wavelength photoacoustic/nephelometer spectrometer (PASS-3) and extinction and scattering by a cavity attenuated phase shift spectrometer (CAPS). Soot particle mass was quantified using a centrifugal particle mass analyzer (CPMA) and mobility size was measured with a scanning mobility particle sizer (SMPS). Measurements were made for nascent soot particles and for collapsed soot particles following coating with dioctyl sebacate or sulfuric acid and thermal denuding to remove the coating. Wavelength-dependent refractive indices for the sampled particles were derived by fitting the observed absorption and extinction cross-sections to spherical particle Mie theory and Rayleigh-Debye-Gans theory. The Rayleigh-Debye-Gans approximation assumes that the absorption properties of soot are dictated by the individual spherules and neglects interaction between them. In general, Mie theory reproduces the observed absorption and extinction cross-sections for particles with volume equivalent diameters (VED) < ~160 nm, but systematically predicts lower

  1. New Interview and Observation Measures of the Broader Autism Phenotype: Impressions of Interviewee Measure

    ERIC Educational Resources Information Center

    Pickles, A.; Parr, J. R.; Rutter, M. L.; De Jonge, M. V.; Wallace, S.; Le Couteur, A. S.; van Engeland, H.; Wittemeyer, K.; McConachie, H.; Roge, B.; Mantoulan, C.; Pedersen, L.; Isager, T.; Poustka, F.; Bolte, S.; Bolton, P.; Weisblatt, E.; Green, J.; Papanikolaou, K.; Bailey, A. J.

    2013-01-01

    A 20 item observational measure of social functioning, the Impression of Interviewee rating scale, is one of three measures devised to assess the broader autism phenotype. The sample studied included families containing at least two individuals with autism spectrum disorder; observations were undertaken by the researcher who interviewed the…

  2. Combined constraints on global ocean primary production using observations and models

    NASA Astrophysics Data System (ADS)

    Buitenhuis, Erik T.; Hashioka, Taketo; Quéré, Corinne Le

    2013-09-01

    production is at the base of the marine food web and plays a central role for global biogeochemical cycles. Yet global ocean primary production is known to only a factor of 2, with previous estimates ranging from 38 to 65 Pg C yr-1 and no formal uncertainty analysis. Here, we present an improved global ocean biogeochemistry model that includes a mechanistic representation of photosynthesis and a new observational database of net primary production (NPP) in the ocean. We combine the model and observations to constrain particulate NPP in the ocean with statistical metrics. The PlankTOM5.3 model includes a new photosynthesis formulation with a dynamic representation of iron-light colimitation, which leads to a considerable improvement of the interannual variability of surface chlorophyll. The database includes a consistent set of 50,050 measurements of 14C primary production. The model best reproduces observations when global NPP is 58 ± 7 Pg C yr-1, with a most probable value of 56 Pg C yr-1. The most probable value is robust to the model used. The uncertainty represents 95% confidence intervals. It considers all random errors in the model and observations, but not potential biases in the observations. We show that tropical regions (23°S-23°N) contribute half of the global NPP, while NPPs in the Northern and Southern Hemispheres are approximately equal in spite of the larger ocean area in the South.

  3. Measurements of observables replaced by “evaluations” in Quantum Theory

    NASA Astrophysics Data System (ADS)

    Nisticò, Giuseppe; Sestito, Angela

    2015-07-01

    In quantum physics there are circumstances where the direct measurement of particular observables encounters difficulties; in some of these cases, however, its value can be evaluated, i.e. it can be inferred by measuring another observable characterized by perfect correlation with the observable of interest. Though an evaluation is often interpreted as a measurement of the evaluated observable, we prove that the two concepts cannot be identified in quantum physics, because the identification yields contradictions. Then, we establish the conceptual status of evaluations in Quantum Theory and the role can be ascribed to them.

  4. Vehicle-specific emissions modeling based upon on-road measurements.

    PubMed

    Frey, H Christopher; Zhang, Kaishan; Rouphail, Nagui M

    2010-05-01

    Vehicle-specific microscale fuel use and emissions rate models are developed based upon real-world hot-stabilized tailpipe measurements made using a portable emissions measurement system. Consecutive averaging periods of one to three multiples of the response time are used to compare two semiempirical physically based modeling schemes. One scheme is based on internally observable variables (IOVs), such as engine speed and manifold absolute pressure, while the other is based on externally observable variables (EOVs), such as speed, acceleration, and road grade. For NO, HC, and CO emission rates, the average R(2) ranged from 0.41 to 0.66 for the former and from 0.17 to 0.30 for the latter. The EOV models have R(2) for CO(2) of 0.43 to 0.79 versus 0.99 for the IOV models. The models are sensitive to episodic events in driving cycles such as high acceleration. Intervehicle and fleet average modeling approaches are compared; the former account for microscale variations that might be useful for some types of assessments. EOV-based models have practical value for traffic management or simulation applications since IOVs usually are not available or not used for emission estimation.

  5. Angular motion estimation using dynamic models in a gyro-free inertial measurement unit.

    PubMed

    Edwan, Ezzaldeen; Knedlik, Stefan; Loffeld, Otmar

    2012-01-01

    In this paper, we summarize the results of using dynamic models borrowed from tracking theory in describing the time evolution of the state vector to have an estimate of the angular motion in a gyro-free inertial measurement unit (GF-IMU). The GF-IMU is a special type inertial measurement unit (IMU) that uses only a set of accelerometers in inferring the angular motion. Using distributed accelerometers, we get an angular information vector (AIV) composed of angular acceleration and quadratic angular velocity terms. We use a Kalman filter approach to estimate the angular velocity vector since it is not expressed explicitly within the AIV. The bias parameters inherent in the accelerometers measurements' produce a biased AIV and hence the AIV bias parameters are estimated within an augmented state vector. Using dynamic models, the appended bias parameters of the AIV become observable and hence we can have unbiased angular motion estimate. Moreover, a good model is required to extract the maximum amount of information from the observation. Observability analysis is done to determine the conditions for having an observable state space model. For higher grades of accelerometers and under relatively higher sampling frequency, the error of accelerometer measurements is dominated by the noise error. Consequently, simulations are conducted on two models, one has bias parameters appended in the state space model and the other is a reduced model without bias parameters.

  6. Modeling and Explaining Content: Definition, Research Support, and Measurement of the "ETS"® National Observational Teaching Examination (NOTE) Assessment Series. Research Memorandum No. RM-16-07

    ERIC Educational Resources Information Center

    Stickler, Leslie; Sykes, Gary

    2016-01-01

    This report reviews the scholarly and research evidence supporting the construct labeled modeling and explaining content (MEC), which is measured via a performance assessment in the "ETS"® National Observational Teaching Examination (NOTE) assessment series. This construct involves practices at the heart of teaching that deal with how…

  7. Ionospheric Simulation System for Satellite Observations and Global Assimilative Modeling Experiments (ISOGAME)

    NASA Technical Reports Server (NTRS)

    Pi, Xiaoqing; Mannucci, Anthony J.; Verkhoglyadova, Olga P.; Stephens, Philip; Wilson, Brian D.; Akopian, Vardan; Komjathy, Attila; Lijima, Byron A.

    2013-01-01

    ISOGAME is designed and developed to assess quantitatively the impact of new observation systems on the capability of imaging and modeling the ionosphere. With ISOGAME, one can perform observation system simulation experiments (OSSEs). A typical OSSE using ISOGAME would involve: (1) simulating various ionospheric conditions on global scales; (2) simulating ionospheric measurements made from a constellation of low-Earth-orbiters (LEOs), particularly Global Navigation Satellite System (GNSS) radio occultation data, and from ground-based global GNSS networks; (3) conducting ionospheric data assimilation experiments with the Global Assimilative Ionospheric Model (GAIM); and (4) analyzing modeling results with visualization tools. ISOGAME can provide quantitative assessment of the accuracy of assimilative modeling with the interested observation system. Other observation systems besides those based on GNSS are also possible to analyze. The system is composed of a suite of software that combines the GAIM, including a 4D first-principles ionospheric model and data assimilation modules, an Internal Reference Ionosphere (IRI) model that has been developed by international ionospheric research communities, observation simulator, visualization software, and orbit design, simulation, and optimization software. The core GAIM model used in ISOGAME is based on the GAIM++ code (written in C++) that includes a new high-fidelity geomagnetic field representation (multi-dipole). New visualization tools and analysis algorithms for the OSSEs are now part of ISOGAME.

  8. Optimal Estimation with Two Process Models and No Measurements

    DTIC Science & Technology

    2015-08-01

    models will be lost if either of the models includes deterministic modeling errors. 12 5. References and Notes 1. Brown RG, Hwang PYC. Introduction to...independent process models when no measurements are present. The observer follows a derivation similar to that of the discrete time Kalman filter. A simulation...discrete time Kalman filter. A simulation example is provided in which a process model based on the dynamics of a ballistic projectile is blended with an

  9. Estimators for longitudinal latent exposure models: examining measurement model assumptions.

    PubMed

    Sánchez, Brisa N; Kim, Sehee; Sammel, Mary D

    2017-06-15

    Latent variable (LV) models are increasingly being used in environmental epidemiology as a way to summarize multiple environmental exposures and thus minimize statistical concerns that arise in multiple regression. LV models may be especially useful when multivariate exposures are collected repeatedly over time. LV models can accommodate a variety of assumptions but, at the same time, present the user with many choices for model specification particularly in the case of exposure data collected repeatedly over time. For instance, the user could assume conditional independence of observed exposure biomarkers given the latent exposure and, in the case of longitudinal latent exposure variables, time invariance of the measurement model. Choosing which assumptions to relax is not always straightforward. We were motivated by a study of prenatal lead exposure and mental development, where assumptions of the measurement model for the time-changing longitudinal exposure have appreciable impact on (maximum-likelihood) inferences about the health effects of lead exposure. Although we were not particularly interested in characterizing the change of the LV itself, imposing a longitudinal LV structure on the repeated multivariate exposure measures could result in high efficiency gains for the exposure-disease association. We examine the biases of maximum likelihood estimators when assumptions about the measurement model for the longitudinal latent exposure variable are violated. We adapt existing instrumental variable estimators to the case of longitudinal exposures and propose them as an alternative to estimate the health effects of a time-changing latent predictor. We show that instrumental variable estimators remain unbiased for a wide range of data generating models and have advantages in terms of mean squared error. Copyright © 2017 John Wiley & Sons, Ltd. Copyright © 2017 John Wiley & Sons, Ltd.

  10. Psychometric Measurement Models and Artificial Neural Networks

    ERIC Educational Resources Information Center

    Sese, Albert; Palmer, Alfonso L.; Montano, Juan J.

    2004-01-01

    The study of measurement models in psychometrics by means of dimensionality reduction techniques such as Principal Components Analysis (PCA) is a very common practice. In recent times, an upsurge of interest in the study of artificial neural networks apt to computing a principal component extraction has been observed. Despite this interest, the…

  11. Video Modeling and Observational Learning to Teach Gaming Access to Students with ASD.

    PubMed

    Spriggs, Amy D; Gast, David L; Knight, Victoria F

    2016-09-01

    The purpose of this study was to evaluate both video modeling and observational learning to teach age-appropriate recreation and leisure skills (i.e., accessing video games) to students with autism spectrum disorder. Effects of video modeling were evaluated via a multiple probe design across participants and criteria for mastery were based on these results. Secondary measures were collected on observational learning across participants and behaviors. Participants included 4 children with autism, ages 8-11, who were served in self-contained special education classrooms. Results indicated a functional relation between video modeling and increased independence in gaming; observational learning occurred for at least some steps across students. Results, implications for practitioners, limitations, and ideas for future research are discussed.

  12. Observations and modelling of the boundary layer using remotely piloted aircraft

    NASA Astrophysics Data System (ADS)

    Cayez, Gregoire; Dralet, Jean-Philippe; Seity, Yann; Momboisse, Geraud; Hattenberger, Gautier; Bronz, Murat; Roberts, Greg

    2014-05-01

    Over the past decade, the scientific community considers the RPAS (remotely piloted aircraft system) as a tool which can help to improve their knowledge of climate and atmospheric phenomena. RPAS equipped with instruments can now conduct measurements in areas that are too hazardous or remote for a manned plane. RPAS are especially adapted system for observing the atmospheric boundary layer processes at high vertical and temporal resolution. The main objectives of VOLTIGE (Vecteur d'Observation de La Troposphère pour l'Investigation et la Gestion de l'Environnement) are to study the life cycle of fog with micro-RPAS, encourage direct participation of the students on the advancement and development of novel observing systems, and assess the feasibility of deploying RPAS in Météo-France's operational network. The instrumented RPAS flights successfully observed the evolution of small-scale meteorological events. Before the arrival of the warm pseudo-front, profiles show a temperature inversion of a hundred meters, which overlaps a cold and wet atmospheric layer. Subsequent profiles show the combination of the arrival of a marine air mass as well as the arrival of a higher level warm pseudo-front. A third case study characterizes the warm sector of the disturbance. Two distinct air masses are visible on the vertical profiles, and show a dry air above an air almost saturated and slightly colder. The temperature and the relative humidity profiles show < 1 meter vertical resolution with a difference between ascent and descent profiles within ± 0.5°C and ± 6 % RH. These results comply with the Météo-France standard limits of quality control. The RPAS profiles were compared with those of the Arome forecast model (an operational model at Météo France). The temperature and wind in the Arome model profiles generally agree with those of the RPAS (less for relative humidity profiles). The Arome model also suggests transitions between air masses occurred at a higher

  13. Measuring Incompatible Observables by Exploiting Sequential Weak Values.

    PubMed

    Piacentini, F; Avella, A; Levi, M P; Gramegna, M; Brida, G; Degiovanni, I P; Cohen, E; Lussana, R; Villa, F; Tosi, A; Zappa, F; Genovese, M

    2016-10-21

    One of the most intriguing aspects of quantum mechanics is the impossibility of measuring at the same time observables corresponding to noncommuting operators, because of quantum uncertainty. This impossibility can be partially relaxed when considering joint or sequential weak value evaluation. Indeed, weak value measurements have been a real breakthrough in the quantum measurement framework that is of the utmost interest from both a fundamental and an applicative point of view. In this Letter, we show how we realized for the first time a sequential weak value evaluation of two incompatible observables using a genuine single-photon experiment. These (sometimes anomalous) sequential weak values revealed the single-operator weak values, as well as the local correlation between them.

  14. Measuring Incompatible Observables by Exploiting Sequential Weak Values

    NASA Astrophysics Data System (ADS)

    Piacentini, F.; Avella, A.; Levi, M. P.; Gramegna, M.; Brida, G.; Degiovanni, I. P.; Cohen, E.; Lussana, R.; Villa, F.; Tosi, A.; Zappa, F.; Genovese, M.

    2016-10-01

    One of the most intriguing aspects of quantum mechanics is the impossibility of measuring at the same time observables corresponding to noncommuting operators, because of quantum uncertainty. This impossibility can be partially relaxed when considering joint or sequential weak value evaluation. Indeed, weak value measurements have been a real breakthrough in the quantum measurement framework that is of the utmost interest from both a fundamental and an applicative point of view. In this Letter, we show how we realized for the first time a sequential weak value evaluation of two incompatible observables using a genuine single-photon experiment. These (sometimes anomalous) sequential weak values revealed the single-operator weak values, as well as the local correlation between them.

  15. A measurement/model comparison of ozone photochemical loss in the Antarctic ozone hole using Polar Ozone and Aerosol Measurement observations and the Match technique

    NASA Astrophysics Data System (ADS)

    Hoppel, Karl; Bevilacqua, Richard; Canty, Timothy; Salawitch, Ross; Santee, Michelle

    2005-10-01

    The Polar Ozone and Aerosol Measurement (POAM III) instrument has provided 6 years (1998 to present) of Antarctic ozone profile measurements, which detail the annual formation of the ozone hole. During the period of ozone hole formation the measurement latitude follows the edge of the polar night and presents a unique challenge for comparing with model simulations. The formation of the ozone hole has been simulated by using a photochemical box model with an ensemble of trajectories, and the results were sampled at the measurement latitude for comparison with the measured ozone. The agreement is generally good but very sensitive to the model dynamics and less sensitive to changes in the model chemistry. In order to better isolate the chemical ozone loss the Match technique was applied to 5 years of data to directly calculate ozone photochemical loss rates. The measured loss rates are specific to the high solar zenith angle conditions of the POAM-Match trajectories and are found to increase slowly from July to early August and then increase rapidly until mid-September. The Match results are sensitive to the choice of meteorological analysis used for the trajectory calculations. The ECMWF trajectories yield the smallest, and perhaps most accurate, peak loss rates that can be reproduced by a photochemical model using standard JPL 2002 kinetics, assuming reactive bromine (BrOx) of 14 pptv based solely on contributions from CH3Br and halons, and without requiring ClOx to exceed the upper limit for available inorganic chlorine of 3.7 ppbv. Larger Match ozone loss rates are found for the late August and early September period if trajectories based on UKMO and NCEP analyses are employed. Such loss rates require higher values for ClO and/or BrO than can be simulated using JPL 2002 chemical kinetics and complete activation of chlorine. In these cases, the agreement between modeled and measured loss rates is significantly improved if the model employs larger ClOOCl cross

  16. Multitime correlators in continuous measurement of qubit observables

    NASA Astrophysics Data System (ADS)

    Atalaya, Juan; Hacohen-Gourgy, Shay; Martin, Leigh S.; Siddiqi, Irfan; Korotkov, Alexander N.

    2018-02-01

    We consider multitime correlators for output signals from linear detectors, continuously measuring several qubit observables at the same time. Using the quantum Bayesian formalism, we show that for unital (symmetric) evolution in the absence of phase backaction, an N -time correlator can be expressed as a product of two-time correlators when N is even. For odd N , there is a similar factorization, which also includes a single-time average. Theoretical predictions agree well with experimental results for two detectors, which simultaneously measure noncommuting qubit observables.

  17. Linking Fine-Scale Observations and Model Output with Imagery at Multiple Scales

    NASA Astrophysics Data System (ADS)

    Sadler, J.; Walthall, C. L.

    2014-12-01

    The development and implementation of a system for seasonal worldwide agricultural yield estimates is underway with the international Group on Earth Observations GeoGLAM project. GeoGLAM includes a research component to continually improve and validate its algorithms. There is a history of field measurement campaigns going back decades to draw upon for ways of linking surface measurements and model results with satellite observations. Ground-based, in-situ measurements collected by interdisciplinary teams include yields, model inputs and factors affecting scene radiation. Data that is comparable across space and time with careful attention to calibration is essential for the development and validation of agricultural applications of remote sensing. Data management to ensure stewardship, availability and accessibility of the data are best accomplished when considered an integral part of the research. The expense and logistical challenges of field measurement campaigns can be cost-prohibitive and because of short funding cycles for research, access to consistent, stable study sites can be lost. The use of a dedicated staff for baseline data needed by multiple investigators, and conducting measurement campaigns using existing measurement networks such as the USDA Long Term Agroecosystem Research network can fulfill these needs and ensure long-term access to study sites.

  18. Sea Ice Summer Camp: Bringing Together Arctic Sea Ice Modelers and Observers

    NASA Astrophysics Data System (ADS)

    Perovich, D. K.; Holland, M. M.

    2016-12-01

    The Arctic sea ice has undergone dramatic change and numerical models project this to continue for the foreseeable future. Understanding the mechanisms behind sea ice loss and its consequences for the larger Arctic and global systems is of critical importance if we are to anticipate and plan for the future. One impediment to progress is a disconnect between the observational and modeling communities. A sea ice summer camp was held in Barrow Alaska from 26 May to 1 June 2016 to overcome this impediment and better integrate the sea ice community. The 25 participants were a mix of modelers and observers from 13 different institutions at career stages from graduate student to senior scientist. The summer camp provided an accelerated program on sea ice observations and models and also fostered future collaborative interdisciplinary activities. Each morning was spent in the classroom with a daily lecture on an aspect of modeling or remote sensing followed by practical exercises. Topics included using models to assess sensitivity, to test hypotheses and to explore sources of uncertainty in future Arctic sea ice loss. The afternoons were spent on the ice making observations. There were four observational activities; albedo observations, ice thickness measurements, ice coring and physical properties, and ice morphology surveys. The last field day consisted of a grand challenge where the group formulated a hypothesis, developed an observational and modeling strategy to test the hypothesis, and then integrated the observations and model results. The impacts of changing sea ice are being felt today in Barrow Alaska. We opened a dialog with Barrow community members to further understand these changes. This included an evening discussion with two Barrow sea ice experts and a community presentation of our work in a public lecture at the Inupiat Heritage Center.

  19. Modeling Noisy Data with Differential Equations Using Observed and Expected Matrices

    ERIC Educational Resources Information Center

    Deboeck, Pascal R.; Boker, Steven M.

    2010-01-01

    Complex intraindividual variability observed in psychology may be well described using differential equations. It is difficult, however, to apply differential equation models in psychological contexts, as time series are frequently short, poorly sampled, and have large proportions of measurement and dynamic error. Furthermore, current methods for…

  20. Evaluation of Observed and Modelled Aerosol Lifetimes Using Radioactive Tracers of Opportunity and an Ensemble of 19 Global Models

    NASA Technical Reports Server (NTRS)

    Kristiansen, N. I.; Stohl, A.; Olivie, D. J. L.; Croft, B.; Sovde, O. A.; Klein, H.; Christoudias, T.; Kunkel, D.; Leadbetter, S. J.; Lee, Y. H.; hide

    2016-01-01

    Aerosols have important impacts on air quality and climate, but the processes affecting their removal from the atmosphere are not fully understood and are poorly constrained by observations. This makes modelled aerosol lifetimes uncertain. In this study, we make use of an observational constraint on aerosol lifetimes provided by radionuclide measurements and investigate the causes of differences within a set of global models. During the Fukushima Dai-Ichi nuclear power plant accident of March 2011, the radioactive isotopes cesium-137 (Cs-137) and xenon-133 (Xe-133) were released in large quantities. Cesium attached to particles in the ambient air, approximately according to their available aerosol surface area. Cs-137 size distribution measurements taken close to the power plant suggested that accumulation mode (AM) sulfate aerosols were the main carriers of cesium. Hence, Cs-137 can be used as a proxy tracer for the AM sulfate aerosol's fate in the atmosphere. In contrast, the noble gas Xe-133 behaves almost like a passive transport tracer. Global surface measurements of the two radioactive isotopes taken over several months after the release allow the derivation of a lifetime of the carrier aerosol. We compare this to the lifetimes simulated by 19 different atmospheric transport models initialized with identical emissions of Cs-137that were assigned to an aerosol tracer with each model's default properties of AM sulfate, and Xe-133 emissions that were assigned to a passive tracer. We investigate to what extent the modelled sulfate tracer can reproduce the measurements, especially with respect to the observed loss of aerosol mass with time. Modelled Cs-137and Xe-133 concentrations sampled at the same location and times as station measurements allow a direct comparison between measured and modelled aerosol lifetime. The e-folding lifetime e, calculated from station measurement data taken between 2 and 9 weeks after the start of the emissions, is 14.3 days (95

  1. Spatial and spectral interpolation of ground-motion intensity measure observations

    USGS Publications Warehouse

    Worden, Charles; Thompson, Eric M.; Baker, Jack W.; Bradley, Brendon A.; Luco, Nicolas; Wilson, David

    2018-01-01

    Following a significant earthquake, ground‐motion observations are available for a limited set of locations and intensity measures (IMs). Typically, however, it is desirable to know the ground motions for additional IMs and at locations where observations are unavailable. Various interpolation methods are available, but because IMs or their logarithms are normally distributed, spatially correlated, and correlated with each other at a given location, it is possible to apply the conditional multivariate normal (MVN) distribution to the problem of estimating unobserved IMs. In this article, we review the MVN and its application to general estimation problems, and then apply the MVN to the specific problem of ground‐motion IM interpolation. In particular, we present (1) a formulation of the MVN for the simultaneous interpolation of IMs across space and IM type (most commonly, spectral response at different oscillator periods) and (2) the inclusion of uncertain observation data in the MVN formulation. These techniques, in combination with modern empirical ground‐motion models and correlation functions, provide a flexible framework for estimating a variety of IMs at arbitrary locations.

  2. The importance of deep, basinwide measurements in optimized Atlantic Meridional Overturning Circulation observing arrays

    NASA Astrophysics Data System (ADS)

    McCarthy, G. D.; Menary, M. B.; Mecking, J. V.; Moat, B. I.; Johns, W. E.; Andrews, M. B.; Rayner, D.; Smeed, D. A.

    2017-03-01

    The Atlantic Meridional Overturning Circulation (AMOC) is a key process in the global redistribution of heat. The AMOC is defined as the maximum of the overturning stream function, which typically occurs near 30°N in the North Atlantic. The RAPID mooring array has provided full-depth, basinwide, continuous estimates of this quantity since 2004. Motivated by both the need to deliver near real-time data and optimization of the array to reduce costs, we consider alternative configurations of the mooring array. Results suggest that the variability observed since 2004 could be reproduced by a single tall mooring on the western boundary and a mooring to 1500 m on the eastern boundary. We consider the potential future evolution of the AMOC in two generations of the Hadley Centre climate models and a suite of additional CMIP5 models. The modeling studies show that deep, basinwide measurements are essential to capture correctly the future decline of the AMOC. We conclude that, while a reduced array could be useful for estimates of the AMOC on subseasonal to decadal time scales as part of a near real-time data delivery system, extreme caution must be applied to avoid the potential misinterpretation or absence of a climate time scale AMOC decline that is a key motivation for the maintenance of these observations.Plain Language SummaryThe Atlantic Overturning Circulation is a system of ocean currents that carries heat northwards in the Atlantic. This heat is crucial to maintaining the mild climate of northwest Europe. The Overturning Circulation is predicted to slow in future in response to man-made climate change. The RAPID program is designed to <span class="hlt">measure</span> the Overturning Circulation using a number of fixed point <span class="hlt">observations</span> spanning the Atlantic between the Canary Islands and the Bahamas. We look at whether we could reduce the number of these fixed point <span class="hlt">observations</span> to continue to get accurate estimates of the overturning</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3386685','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3386685"><span>Angular Motion Estimation Using Dynamic <span class="hlt">Models</span> in a Gyro-Free Inertial <span class="hlt">Measurement</span> Unit</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Edwan, Ezzaldeen; Knedlik, Stefan; Loffeld, Otmar</p> <p>2012-01-01</p> <p>In this paper, we summarize the results of using dynamic <span class="hlt">models</span> borrowed from tracking theory in describing the time evolution of the state vector to have an estimate of the angular motion in a gyro-free inertial <span class="hlt">measurement</span> unit (GF-IMU). The GF-IMU is a special type inertial <span class="hlt">measurement</span> unit (IMU) that uses only a set of accelerometers in inferring the angular motion. Using distributed accelerometers, we get an angular information vector (AIV) composed of angular acceleration and quadratic angular velocity terms. We use a Kalman filter approach to estimate the angular velocity vector since it is not expressed explicitly within the AIV. The bias parameters inherent in the accelerometers <span class="hlt">measurements</span>' produce a biased AIV and hence the AIV bias parameters are estimated within an augmented state vector. Using dynamic <span class="hlt">models</span>, the appended bias parameters of the AIV become <span class="hlt">observable</span> and hence we can have unbiased angular motion estimate. Moreover, a good <span class="hlt">model</span> is required to extract the maximum amount of information from the <span class="hlt">observation</span>. <span class="hlt">Observability</span> analysis is done to determine the conditions for having an <span class="hlt">observable</span> state space <span class="hlt">model</span>. For higher grades of accelerometers and under relatively higher sampling frequency, the error of accelerometer <span class="hlt">measurements</span> is dominated by the noise error. Consequently, simulations are conducted on two <span class="hlt">models</span>, one has bias parameters appended in the state space <span class="hlt">model</span> and the other is a reduced <span class="hlt">model</span> without bias parameters. PMID:22778586</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1813385M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1813385M"><span>Towards real-time assimilation of crowdsourced <span class="hlt">observations</span> in hydrological <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mazzoleni, Maurizio; Verlaan, Martin; Alfonso, Leonardo; Norbiato, Daniele; Monego, Martina; Ferri, Michele; Solomatine, Dimitri</p> <p>2016-04-01</p> <p>The continued technological advances have stimulated the spread of low-cost sensors that can be used by citizens to provide crowdsourced <span class="hlt">observations</span> (CO) of different hydrological variables. An example of such low-cost sensors is a staff gauge connected to a QR code on which people can read the water level indication and send the <span class="hlt">measurement</span> via a mobile phone application. The goal of this study is to assess the combined effect of the assimilation of CO coming from a distributed network of low-cost sensors, and the existing streamflow <span class="hlt">observations</span> from physical sensors, on the performance of a semi-distributed hydrological <span class="hlt">model</span>. The methodology is applied to the Bacchiglione catchment, North East of Italy, where an early warning system is used by the Alto Adriatico Water Authority to issue forecasted water level along the river network which cross important cities such as Vicenza and Padua. In this study, forecasted precipitation values are used as input in the hydrological <span class="hlt">model</span> to estimate the simulated streamflow hydrograph used as boundary condition for the hydraulic <span class="hlt">model</span>. <span class="hlt">Observed</span> precipitation values are used to generate realistic synthetic streamflow values with various characteristics of arrival frequency and accuracy, to simulate CO coming at irregular time steps. These <span class="hlt">observations</span> are assimilated into the semi-distributed <span class="hlt">model</span> using a Kalman filter based method. The results of this study show that CO, asynchronous in time and with variable accuracy, can still improve flood prediction when integrated in hydrological <span class="hlt">models</span>. When both physical and low-cost sensors are located at the same places, the assimilation of CO gives the same <span class="hlt">model</span> improvement than the assimilation of physical <span class="hlt">observations</span> only for high number of non-intermittent sensors. However, the integration of <span class="hlt">observations</span> from low-cost sensors and single physical sensors can improve the flood prediction even when small a number of intermittent CO are available. This study is part of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1425660-enso-driven-energy-budget-perturbations-observations-cmip-models','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1425660-enso-driven-energy-budget-perturbations-observations-cmip-models"><span>ENSO-driven energy budget perturbations in <span class="hlt">observations</span> and CMIP <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Mayer, Michael; Fasullo, John T.; Trenberth, Kevin E.; ...</p> <p>2016-03-19</p> <p>Various <span class="hlt">observation</span>-based datasets are employed to robustly quantify changes in ocean heat content (OHC), anomalous ocean–atmosphere energy exchanges and atmospheric energy transports during El Niño-Southern Oscillation (ENSO). These results are used as a benchmark to evaluate the energy pathways during ENSO as simulated by coupled climate <span class="hlt">model</span> runs from the CMIP3 and CMIP5 archives. The <span class="hlt">models</span> are able to qualitatively reproduce <span class="hlt">observed</span> patterns of ENSO-related energy budget variability to some degree, but key aspects are seriously biased. Area-averaged tropical Pacific OHC variability associated with ENSO is greatly underestimated by all <span class="hlt">models</span> because of strongly biased responses of net radiation atmore » top-of-the-atmosphere to ENSO. The latter are related to biases of mean convective activity in the <span class="hlt">models</span> and project on surface energy fluxes in the eastern Pacific Intertropical Convergence Zone region. Moreover, <span class="hlt">models</span> underestimate horizontal and vertical OHC redistribution in association with the generally too weak Bjerknes feedback, leading to a <span class="hlt">modeled</span> ENSO affecting a too shallow layer of the Pacific. Vertical links between SST and OHC variability are too weak even in <span class="hlt">models</span> driven with <span class="hlt">observed</span> winds, indicating shortcomings of the ocean <span class="hlt">models</span>. Furthermore, <span class="hlt">modeled</span> teleconnections as <span class="hlt">measured</span> by tropical Atlantic OHC variability are too weak and the tropical zonal mean ENSO signal is strongly underestimated or even completely missing in most of the considered <span class="hlt">models</span>. In conclusion, results suggest that attempts to infer insight about climate sensitivity from ENSO-related variability are likely to be hampered by biases in ENSO in CMIP simulations that do not bear a clear link to future changes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140002434','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140002434"><span>Empirical STORM-E <span class="hlt">Model</span>. [I. Theoretical and <span class="hlt">Observational</span> Basis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mertens, Christopher J.; Xu, Xiaojing; Bilitza, Dieter; Mlynczak, Martin G.; Russell, James M., III</p> <p>2013-01-01</p> <p>Auroral nighttime infrared emission <span class="hlt">observed</span> by the Sounding of the Atmosphere using Broadband Emission Radiometry (SABER) instrument onboard the Thermosphere-Ionosphere-Mesosphere Energetics and Dynamics (TIMED) satellite is used to develop an empirical <span class="hlt">model</span> of geomagnetic storm enhancements to E-region peak electron densities. The empirical <span class="hlt">model</span> is called STORM-E and will be incorporated into the 2012 release of the International Reference Ionosphere (IRI). The proxy for characterizing the E-region response to geomagnetic forcing is NO+(v) volume emission rates (VER) derived from the TIMED/SABER 4.3 lm channel limb radiance <span class="hlt">measurements</span>. The storm-time response of the NO+(v) 4.3 lm VER is sensitive to auroral particle precipitation. A statistical database of storm-time to climatological quiet-time ratios of SABER-<span class="hlt">observed</span> NO+(v) 4.3 lm VER are fit to widely available geomagnetic indices using the theoretical framework of linear impulse-response theory. The STORM-E <span class="hlt">model</span> provides a dynamic storm-time correction factor to adjust a known quiescent E-region electron density peak concentration for geomagnetic enhancements due to auroral particle precipitation. Part II of this series describes the explicit development of the empirical storm-time correction factor for E-region peak electron densities, and shows comparisons of E-region electron densities between STORM-E predictions and incoherent scatter radar <span class="hlt">measurements</span>. In this paper, Part I of the series, the efficacy of using SABER-derived NO+(v) VER as a proxy for the E-region response to solar-geomagnetic disturbances is presented. Furthermore, a detailed description of the algorithms and methodologies used to derive NO+(v) VER from SABER 4.3 lm limb emission <span class="hlt">measurements</span> is given. Finally, an assessment of key uncertainties in retrieving NO+(v) VER is presented</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1815180C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1815180C"><span>Hydro-geophysical <span class="hlt">observations</span> integration in numerical <span class="hlt">model</span>: case study in Mediterranean karstic unsaturated zone (Larzac, france)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Champollion, Cédric; Fores, Benjamin; Le Moigne, Nicolas; Chéry, Jean</p> <p>2016-04-01</p> <p>Karstic hydro-systems are highly non-linear and heterogeneous but one of the main water resource in the Mediterranean area. Neither local <span class="hlt">measurements</span> in boreholes or analysis at the spring can take into account the variability of the water storage. Since a few years, ground-based geophysical <span class="hlt">measurements</span> (such as gravity, electrical resistivity or seismological data) allows following water storage in heterogeneous hydrosystems at an intermediate scale between boreholes and basin. Behind classical rigorous monitoring, the integration of geophysical data in hydrological numerical <span class="hlt">models</span> in needed for both processes interpretation and quantification. Since a few years, a karstic geophysical observatory (GEK: Géodésie de l'Environnement Karstique, OSU OREME, SNO H+) has been setup in the Mediterranean area in the south of France. The observatory is surrounding more than 250m karstified dolomite, with an unsaturated zone of ~150m thickness. At the observatory water level in boreholes, evapotranspiration and rainfall are classical hydro-meteorological <span class="hlt">observations</span> completed by continuous gravity, resistivity and seismological <span class="hlt">measurements</span>. The main objective of the study is the <span class="hlt">modelling</span> of the whole <span class="hlt">observation</span> dataset by explicit unsaturated numerical <span class="hlt">model</span> in one dimension. Hydrus software is used for the explicit <span class="hlt">modelling</span> of the water storage and transfer and links the different <span class="hlt">observations</span> (geophysics, water level, evapotranspiration) with the water saturation. Unknown hydrological parameters (permeability, porosity) are retrieved from stochastic inversions. The scale of investigation of the different <span class="hlt">observations</span> are discussed thank to the <span class="hlt">modelling</span> results. A sensibility study of the <span class="hlt">measurements</span> against the <span class="hlt">model</span> is done and key hydro-geological processes of the site are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28395353','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28395353"><span>Predicting Directly <span class="hlt">Measured</span> Trunk and Upper Arm Postures in Paper Mill Work From Administrative Data, Workers' Ratings and Posture <span class="hlt">Observations</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heiden, Marina; Garza, Jennifer; Trask, Catherine; Mathiassen, Svend Erik</p> <p>2017-03-01</p> <p>A cost-efficient approach for assessing working postures could be to build statistical <span class="hlt">models</span> for predicting results of direct <span class="hlt">measurements</span> from cheaper data, and apply these <span class="hlt">models</span> to samples in which only the latter data are available. The present study aimed to build and assess the performance of statistical <span class="hlt">models</span> predicting inclinometer-assessed trunk and arm posture among paper mill workers. Separate <span class="hlt">models</span> were built using administrative data, workers' ratings of their exposure, and <span class="hlt">observations</span> of the work from video recordings as predictors. Trunk and upper arm postures were <span class="hlt">measured</span> using inclinometry on 28 paper mill workers during three work shifts each. Simultaneously, the workers were video filmed, and their postures were assessed by <span class="hlt">observation</span> of the videos afterwards. Workers' ratings of exposure, and administrative data on staff and production during the shifts were also collected. Linear mixed <span class="hlt">models</span> were fitted for predicting inclinometer-assessed exposure variables (median trunk and upper arm angle, proportion of time with neutral trunk and upper arm posture, and frequency of periods in neutral trunk and upper arm inclination) from administrative data, workers' ratings, and <span class="hlt">observations</span>, respectively. Performance was evaluated in terms of Akaike information criterion, proportion of variance explained (R2), and standard error (SE) of the <span class="hlt">model</span> estimate. For <span class="hlt">models</span> performing well, validity was assessed by bootstrap resampling. <span class="hlt">Models</span> based on administrative data performed poorly (R2 ≤ 15%) and would not be useful for assessing posture in this population. <span class="hlt">Models</span> using workers' ratings of exposure performed slightly better (8% ≤ R2 ≤ 27% for trunk posture; 14% ≤ R2 ≤ 36% for arm posture). The best <span class="hlt">model</span> was obtained when using <span class="hlt">observational</span> data for predicting frequency of periods with neutral arm inclination. It explained 56% of the variance in the postural exposure, and its SE was 5.6. Bootstrap validation of this <span class="hlt">model</span> showed similar</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010084310','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010084310"><span>Mixing in the Extratropical Stratosphere: <span class="hlt">Model-measurements</span> Comparisons using MLM Diagnostics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ma, Jun; Waugh, Darryn W.; Douglass, Anne R.; Kawa, Stephan R.; Bhartia, P. K. (Technical Monitor)</p> <p>2001-01-01</p> <p>We evaluate transport processes in the extratropical lower stratosphere for both <span class="hlt">models</span> and <span class="hlt">measurements</span> with the help of equivalent length diagnostic from the modified Lagrangian-mean (MLM) analysis. This diagnostic is used to compare <span class="hlt">measurements</span> of long-lived tracers made by the Cryogenic Limb Array Etalon Spectrometer (CLAES) on the Upper Atmosphere Research Satellite (UARS) with simulated tracers. Simulations are produced in Chemical and Transport <span class="hlt">Models</span> (CTMs), in which meteorological fields are taken from the Goddard Earth <span class="hlt">Observing</span> System Data Assimilation System (GEOS DAS), the Middle Atmosphere Community Climate <span class="hlt">Model</span> (MACCM2), and the Geophysical Fluid Dynamics Laboratory (GFDL) "SKYHI" <span class="hlt">model</span>, respectively. Time series of isentropic equivalent length show that these <span class="hlt">models</span> are able to capture major mixing and transport properties <span class="hlt">observed</span> by CLAES, such as the formation and destruction of polar barriers, the presence of surf zones in both hemispheres. Differences between each <span class="hlt">model</span> simulation and the <span class="hlt">observation</span> are examined in light of <span class="hlt">model</span> performance. Among these differences, only the simulation driven by GEOS DAS shows one case of the "top-down" destruction of the Antarctic polar vortex, as <span class="hlt">observed</span> in the CLAES data. Additional experiments of isentropic advection of artificial tracer by GEOS DAS winds suggest that diabatic movement might have considerable contribution to the equivalent length field in the 3D CTM diagnostics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003798&hterms=Automata&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAutomata','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003798&hterms=Automata&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAutomata"><span>A Nanoflare-Based Cellular Automaton <span class="hlt">Model</span> and the <span class="hlt">Observed</span> Properties of the Coronal Plasma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lopez-Fuentes, Marcelo; Klimchuk, James Andrew</p> <p>2016-01-01</p> <p>We use the cellular automaton <span class="hlt">model</span> described in Lopez Fuentes and Klimchuk to study the evolution of coronal loop plasmas. The <span class="hlt">model</span>, based on the idea of a critical misalignment angle in tangled magnetic fields, produces nanoflares of varying frequency with respect to the plasma cooling time. We compare the results of the <span class="hlt">model</span> with active region (AR) <span class="hlt">observations</span> obtained with the Hinode/XRT and SDOAIA instruments. The comparison is based on the statistical properties of synthetic and <span class="hlt">observed</span> loop light curves. Our results show that the <span class="hlt">model</span> reproduces the main <span class="hlt">observational</span> characteristics of the evolution of the plasma in AR coronal loops. The typical intensity fluctuations have amplitudes of 10 percent - 15 percent both for the <span class="hlt">model</span> and the <span class="hlt">observations</span>. The sign of the skewness of the intensity distributions indicates the presence of cooling plasma in the loops. We also study the emission <span class="hlt">measure</span> (EM) distribution predicted by the <span class="hlt">model</span> and obtain slopes in log(EM) versus log(T) between 2.7 and 4.3, in agreement with published <span class="hlt">observational</span> values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22667445-nanoflare-based-cellular-automaton-model-observed-properties-coronal-plasma','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22667445-nanoflare-based-cellular-automaton-model-observed-properties-coronal-plasma"><span>A NANOFLARE-BASED CELLULAR AUTOMATON <span class="hlt">MODEL</span> AND THE <span class="hlt">OBSERVED</span> PROPERTIES OF THE CORONAL PLASMA</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Fuentes, Marcelo López; Klimchuk, James A., E-mail: lopezf@iafe.uba.ar</p> <p>2016-09-10</p> <p>We use the cellular automaton <span class="hlt">model</span> described in López Fuentes and Klimchuk to study the evolution of coronal loop plasmas. The <span class="hlt">model</span>, based on the idea of a critical misalignment angle in tangled magnetic fields, produces nanoflares of varying frequency with respect to the plasma cooling time. We compare the results of the <span class="hlt">model</span> with active region (AR) <span class="hlt">observations</span> obtained with the Hinode /XRT and SDO /AIA instruments. The comparison is based on the statistical properties of synthetic and <span class="hlt">observed</span> loop light curves. Our results show that the <span class="hlt">model</span> reproduces the main <span class="hlt">observational</span> characteristics of the evolution of the plasmamore » in AR coronal loops. The typical intensity fluctuations have amplitudes of 10%–15% both for the <span class="hlt">model</span> and the <span class="hlt">observations</span>. The sign of the skewness of the intensity distributions indicates the presence of cooling plasma in the loops. We also study the emission <span class="hlt">measure</span> (EM) distribution predicted by the <span class="hlt">model</span> and obtain slopes in log(EM) versus log(T) between 2.7 and 4.3, in agreement with published <span class="hlt">observational</span> values.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3818391','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3818391"><span>An overview of animal <span class="hlt">models</span> of pain: disease <span class="hlt">models</span> and outcome <span class="hlt">measures</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gregory, N; Harris, AL; Robinson, CR; Dougherty, PM; Fuchs, PN; Sluka, KA</p> <p>2013-01-01</p> <p>Pain is ultimately a perceptual phenomenon. It is built from information gathered by specialized pain receptors in tissue, modified by spinal and supraspinal mechanisms, and integrated into a discrete sensory experience with an emotional valence in the brain. Because of this, studying intact animals allows the multidimensional nature of pain to be examined. A number of animal <span class="hlt">models</span> have been developed, reflecting <span class="hlt">observations</span> that pain phenotypes are mediated by distinct mechanisms. Animal <span class="hlt">models</span> of pain are designed to mimic distinct clinical diseases to better evaluate underlying mechanisms and potential treatments. Outcome <span class="hlt">measures</span> are designed to <span class="hlt">measure</span> multiple parts of the pain experience including reflexive hyperalgesia <span class="hlt">measures</span>, sensory and affective dimensions of pain and impact of pain on function and quality of life. In this review we discuss the common methods used for inducing each of the pain phenotypes related to clinical pain syndromes, as well as the main behavioral tests for assessing pain in each <span class="hlt">model</span>. PMID:24035349</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.9186K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.9186K"><span><span class="hlt">Observational</span> uncertainty and regional climate <span class="hlt">model</span> evaluation: A pan-European perspective</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kotlarski, Sven; Szabó, Péter; Herrera, Sixto; Räty, Olle; Keuler, Klaus; Soares, Pedro M.; Cardoso, Rita M.; Bosshard, Thomas; Pagé, Christian; Boberg, Fredrik; Gutiérrez, José M.; Jaczewski, Adam; Kreienkamp, Frank; Liniger, Mark. A.; Lussana, Cristian; Szepszo, Gabriella</p> <p>2017-04-01</p> <p>Local and regional climate change assessments based on downscaling methods crucially depend on the existence of accurate and reliable <span class="hlt">observational</span> reference data. In dynamical downscaling via regional climate <span class="hlt">models</span> (RCMs) <span class="hlt">observational</span> data can influence <span class="hlt">model</span> development itself and, later on, <span class="hlt">model</span> evaluation, parameter calibration and added value assessment. In empirical-statistical downscaling, <span class="hlt">observations</span> serve as predictand data and directly influence <span class="hlt">model</span> calibration with corresponding effects on downscaled climate change projections. Focusing on the evaluation of RCMs, we here analyze the influence of uncertainties in <span class="hlt">observational</span> reference data on evaluation results in a well-defined performance assessment framework and on a European scale. For this purpose we employ three different gridded <span class="hlt">observational</span> reference grids, namely (1) the well-established EOBS dataset (2) the recently developed EURO4M-MESAN regional re-analysis, and (3) several national high-resolution and quality-controlled gridded datasets that recently became available. In terms of climate <span class="hlt">models</span> five reanalysis-driven experiments carried out by five different RCMs within the EURO-CORDEX framework are used. Two variables (temperature and precipitation) and a range of evaluation metrics that reflect different aspects of RCM performance are considered. We furthermore include an illustrative <span class="hlt">model</span> ranking exercise and relate <span class="hlt">observational</span> spread to RCM spread. The results obtained indicate a varying influence of <span class="hlt">observational</span> uncertainty on <span class="hlt">model</span> evaluation depending on the variable, the season, the region and the specific performance metric considered. Over most parts of the continent, the influence of the choice of the reference dataset for temperature is rather small for seasonal mean values and inter-annual variability. Here, <span class="hlt">model</span> uncertainty (as <span class="hlt">measured</span> by the spread between the five RCM simulations considered) is typically much larger than reference data uncertainty. For</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991SoPh..132..137C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991SoPh..132..137C"><span><span class="hlt">Modelling</span> a solar flare from X-ray, UV, and radio <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chiuderi Drago, F.; Monsignori Fossi, B. C.</p> <p>1991-03-01</p> <p>A slowly evolving, flaring loop was <span class="hlt">observed</span> by the UVSP, XRP, and HXIS instruments onboard SMM on June 10, 1980. Simultaneous radio <span class="hlt">observations</span> from Toyokawa (Japan) are also available. The SMM instruments have an angular resolution ranging from 3 to 30 arcsec by which the loop structure may be determined. It appears that these <span class="hlt">observations</span> cannot be accounted for by a single loop <span class="hlt">model</span> even assuming a variable temperature and pressure. The additional presence of a hot and tenuous isothermal plasma is necessary to explain the harder emission (HXIS). X-ray and UV data are used to fit the differential emission <span class="hlt">measure</span> as a function of temperature and a <span class="hlt">model</span> of the flare is deduced, which is then checked against radio data. An estimate of the heating function along the loop and of the total energy content of the loop is also given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.B52A..04H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.B52A..04H"><span>Carbon Cycle <span class="hlt">Model</span> Linkage Project (CCMLP): Evaluating Biogeochemical Process <span class="hlt">Models</span> with Atmospheric <span class="hlt">Measurements</span> and Field Experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heimann, M.; Prentice, I. C.; Foley, J.; Hickler, T.; Kicklighter, D. W.; McGuire, A. D.; Melillo, J. M.; Ramankutty, N.; Sitch, S.</p> <p>2001-12-01</p> <p><span class="hlt">Models</span> of biophysical and biogeochemical proceses are being used -either offline or in coupled climate-carbon cycle (C4) <span class="hlt">models</span>-to assess climate- and CO2-induced feedbacks on atmospheric CO2. <span class="hlt">Observations</span> of atmospheric CO2 concentration, and supplementary tracers including O2 concentrations and isotopes, offer unique opportunities to evaluate the large-scale behaviour of <span class="hlt">models</span>. Global patterns, temporal trends, and interannual variability of the atmospheric CO2 concentration and its seasonal cycle provide crucial benchmarks for simulations of regionally-integrated net ecosystem exchange; flux <span class="hlt">measurements</span> by eddy correlation allow a far more demanding <span class="hlt">model</span> test at the ecosystem scale than conventional indicators, such as <span class="hlt">measurements</span> of annual net primary production; and large-scale manipulations, such as the Duke Forest Free Air Carbon Enrichment (FACE) experiment, give a standard to evaluate <span class="hlt">modelled</span> phenomena such as ecosystem-level CO2 fertilization. <span class="hlt">Model</span> runs including historical changes of CO2, climate and land use allow comparison with regional-scale monthly CO2 balances as inferred from atmospheric <span class="hlt">measurements</span>. Such comparisons are providing grounds for some confidence in current <span class="hlt">models</span>, while pointing to processes that may still be inadequately treated. Current plans focus on (1) continued benchmarking of land process <span class="hlt">models</span> against flux <span class="hlt">measurements</span> across ecosystems and experimental findings on the ecosystem-level effects of enhanced CO2, reactive N inputs and temperature; (2) improved representation of land use, forest management and crop metabolism in <span class="hlt">models</span>; and (3) a strategy for the evaluation of C4 <span class="hlt">models</span> in a historical <span class="hlt">observational</span> context.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRD..119.1534W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRD..119.1534W"><span>Twomey effect <span class="hlt">observed</span> from collocated microphysical and remote sensing <span class="hlt">measurements</span> over shallow cumulus</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Werner, F.; Ditas, F.; Siebert, H.; Simmel, M.; Wehner, B.; Pilewskie, P.; Schmeissner, T.; Shaw, R. A.; Hartmann, S.; Wex, H.; Roberts, G. C.; Wendisch, M.</p> <p>2014-02-01</p> <p>Clear experimental evidence of the Twomey effect for shallow trade wind cumuli near Barbados is presented. Effective droplet radius (reff) and cloud optical thickness (τ), retrieved from helicopter-borne spectral cloud-reflected radiance <span class="hlt">measurements</span>, and spectral cloud reflectivity (γλ) are correlated with collocated in situ <span class="hlt">observations</span> of the number concentration of aerosol particles from the subcloud layer (N). N denotes the concentration of particles larger than 80 nm in diameter and represents particles in the activation mode. In situ cloud microphysical and aerosol parameters were sampled by the Airborne Cloud Turbulence <span class="hlt">Observation</span> System (ACTOS). Spectral cloud-reflected radiance data were collected by the Spectral Modular Airborne Radiation <span class="hlt">measurement</span> sysTem (SMART-HELIOS). With increasing N a shift in the probability density functions of τ and γλ toward larger values is <span class="hlt">observed</span>, while the mean values and <span class="hlt">observed</span> ranges of retrieved reff decrease. The relative susceptibilities (RS) of reff, τ, and γλ to N are derived for bins of constant liquid water path. The resulting values of RS are in the range of 0.35 for reff and τ, and 0.27 for γλ. These results are close to the maximum susceptibility possible from theory. Overall, the shallow cumuli sampled near Barbados show characteristics of homogeneous, plane-parallel clouds. Comparisons of RS derived from in situ <span class="hlt">measured</span> reff and from a microphysical parcel <span class="hlt">model</span> are in close agreement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSA41A2101F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSA41A2101F"><span>An Analysis of Ionospheric Thermal Ions Using a SIMION-based Forward Instrument <span class="hlt">Model</span>: In Situ <span class="hlt">Observations</span> of Vertical Thermal Ion Flows as <span class="hlt">Measured</span> by the MICA Sounding Rocket</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fernandes, P. A.; Lynch, K. A.; Zettergren, M. D.; Hampton, D. L.; Fisher, L. E.; Powell, S. P.</p> <p>2013-12-01</p> <p>The MICA sounding rocket launched on 19 Feb. 2012 into several discrete, localized arcs in the wake of a westward traveling surge. In situ and ground-based <span class="hlt">observations</span> provide a <span class="hlt">measured</span> response of the ionosphere to preflight and localized auroral drivers. In this presentation we focus on in situ <span class="hlt">measurements</span> of the thermal ion distribution. We <span class="hlt">observe</span> thermal ions flowing both up and down the auroral field line, with upflows concentrated in Alfvénic and downward current regions. The in situ data are compared with recent ionospheric <span class="hlt">modeling</span> efforts (Zettergren et al., this session) which show structured patterns of ion upflow and downflow consistent with these <span class="hlt">observations</span>. In the low-energy thermal plasma regime, instrument response to the <span class="hlt">measured</span> thermal ion population is very sensitive to the presence of the instrument. The plasma is shifted and accelerated in the frame of the instrument due to flows, ram, and acceleration through the payload sheath. The energies associated with these processes are large compared to the thermal energy. Rigorous quantitative analysis of the instrument response is necessary to extract the plasma properties which describe the full 3D distribution function at the instrument aperture. We introduce an instrument <span class="hlt">model</span>, developed in the commercial software package SIMION, to characterize instrument response at low energies. The instrument <span class="hlt">model</span> provides important insight into how we would modify our instrument for future missions, including fine-tuning parameters such as the analyzer sweep curve, the geometry factor, and the aperture size. We use the results from the instrument <span class="hlt">model</span> to develop a forward <span class="hlt">model</span>, from which we can extract anisotropic ion temperatures, flows, and density of the thermal plasma at the aperture. Because this plasma has transited a sheath to reach the aperture, we must account for the acceleration due to the sheath. <span class="hlt">Modeling</span> of this complex sheath is being conducted by co-author Fisher, using a PIC code</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1254571-evaluation-observed-modelled-aerosol-lifetimes-using-radioactive-tracers-opportunity-ensemble-global-models','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1254571-evaluation-observed-modelled-aerosol-lifetimes-using-radioactive-tracers-opportunity-ensemble-global-models"><span>Evaluation of <span class="hlt">observed</span> and <span class="hlt">modelled</span> aerosol lifetimes using radioactive tracers of opportunity and an ensemble of 19 global <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Kristiansen, N. I.; Stohl, A.; Olivie, D. J. L.; ...</p> <p>2016-03-17</p> <p>Aerosols have important impacts on air quality and climate, but the processes affecting their removal from the atmosphere are not fully understood and are poorly constrained by <span class="hlt">observations</span>. This makes <span class="hlt">modelled</span> aerosol lifetimes uncertain. In this study, we make use of an <span class="hlt">observational</span> constraint on aerosol lifetimes provided by radionuclide <span class="hlt">measurements</span> and investigate the causes of differences within a set of global <span class="hlt">models</span>. During the Fukushima Dai-Ichi nuclear power plant accident of March 2011, the radioactive isotopes cesium-137 ( 137Cs) and xenon-133 ( 133Xe) were released in large quantities. Cesium attached to particles in the ambient air, approximately according to theirmore » available aerosol surface area. 137Cs size distribution <span class="hlt">measurements</span> taken close to the power plant suggested that accumulation-mode (AM) sulfate aerosols were the main carriers of cesium. Hence, 137Cs can be used as a proxy tracer for the AM sulfate aerosol's fate in the atmosphere. In contrast, the noble gas 133Xe behaves almost like a passive transport tracer. Global surface <span class="hlt">measurements</span> of the two radioactive isotopes taken over several months after the release allow the derivation of a lifetime of the carrier aerosol. We compare this to the lifetimes simulated by 19 different atmospheric transport <span class="hlt">models</span> initialized with identical emissions of 137Cs that were assigned to an aerosol tracer with each <span class="hlt">model</span>'s default properties of AM sulfate, and 133Xe emissions that were assigned to a passive tracer. We investigate to what extent the <span class="hlt">modelled</span> sulfate tracer can reproduce the <span class="hlt">measurements</span>, especially with respect to the <span class="hlt">observed</span> loss of aerosol mass with time. <span class="hlt">Modelled</span> 137Cs and 133Xe concentrations sampled at the same location and times as station <span class="hlt">measurements</span> allow a direct comparison between <span class="hlt">measured</span> and <span class="hlt">modelled</span> aerosol lifetime. The e-folding lifetime τ e, calculated from station <span class="hlt">measurement</span> data taken between 2 and 9 weeks after the start of the emissions, is 14.3 days</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3077406','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3077406"><span>Bayesian <span class="hlt">Modeling</span> of Perceived Surface Slant from Actively-Generated and Passively-<span class="hlt">Observed</span> Optic Flow</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Caudek, Corrado; Fantoni, Carlo; Domini, Fulvio</p> <p>2011-01-01</p> <p>We <span class="hlt">measured</span> perceived depth from the optic flow (a) when showing a stationary physical or virtual object to <span class="hlt">observers</span> who moved their head at a normal or slower speed, and (b) when simulating the same optic flow on a computer and presenting it to stationary <span class="hlt">observers</span>. Our results show that perceived surface slant is systematically distorted, for both the active and the passive viewing of physical or virtual surfaces. These distortions are modulated by head translation speed, with perceived slant increasing directly with the local velocity gradient of the optic flow. This empirical result allows us to determine the relative merits of two alternative approaches aimed at explaining perceived surface slant in active vision: an “inverse optics” <span class="hlt">model</span> that takes head motion information into account, and a probabilistic <span class="hlt">model</span> that ignores extra-retinal signals. We compare these two approaches within the framework of the Bayesian theory. The “inverse optics” Bayesian <span class="hlt">model</span> produces veridical slant estimates if the optic flow and the head translation velocity are <span class="hlt">measured</span> with no error; because of the influence of a “prior” for flatness, the slant estimates become systematically biased as the <span class="hlt">measurement</span> errors increase. The Bayesian <span class="hlt">model</span>, which ignores the <span class="hlt">observer</span>'s motion, always produces distorted estimates of surface slant. Interestingly, the predictions of this second <span class="hlt">model</span>, not those of the first one, are consistent with our empirical findings. The present results suggest that (a) in active vision perceived surface slant may be the product of probabilistic processes which do not guarantee the correct solution, and (b) extra-retinal signals may be mainly used for a better <span class="hlt">measurement</span> of retinal information. PMID:21533197</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900053142&hterms=mahan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmahan','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900053142&hterms=mahan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmahan"><span>An improved electrothermal <span class="hlt">model</span> for the ERBE nonscanning radiometer - Comparison of predicted and <span class="hlt">measured</span> behavior during solar <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tira, Nour E.; Mahan, J. R.; Lee, Robert B., III</p> <p>1989-01-01</p> <p>The improved Earth Radiation Budget Experiment nonscanning-channels electrothermal <span class="hlt">model</span> presented is used to <span class="hlt">model</span> two types of solar <span class="hlt">observations</span>: those obtained through the solar port during solar calibration, and and those obtained during the satellite pitch-over maneuver, in which the sun is <span class="hlt">observed</span> by the radiometer while it is in earth-viewing configuration. Thermal noise has been separately studied to evaluate its contribution to the radiative energy absorbed by the active cavity. It is found that the scattering of the collimated solar radiation contributes an average of 0.071 mW during solar calibration.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A21I2258S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A21I2258S"><span>Comparison of water vapor from <span class="hlt">observations</span> and <span class="hlt">models</span> in the Asian Monsoon UTLS region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singer, C. E.; Clouser, B.; Gaeta, D. C.; Moyer, E. J.</p> <p>2017-12-01</p> <p>As part of the StratoClim campaign in July/August 2017, the Chicago Water Isotope Spectrometer (ChiWIS) made water vapor <span class="hlt">measurements</span> from the mid-troposphere through the lower stratosphere (to 21 km altitude). We compare in-situ <span class="hlt">measurements</span> with remote sensing <span class="hlt">observations</span> and <span class="hlt">model</span> projections both to validate <span class="hlt">measurements</span> and to evalute the added value of high-precision in-situ sampling. Preliminary results and comparison with other StratoClim tracer <span class="hlt">measurements</span> suggest that the UTLS region is highly structured, beyond what <span class="hlt">models</span> or satellite instruments can capture, and that ChiWIS accurately captures these variations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1712054H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1712054H"><span><span class="hlt">Observing</span> convection with satellite, radar, and lightning <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hamann, Ulrich; Nisi, Luca; Clementi, Lorenzo; Ventura, Jordi Figueras i.; Gabella, Marco; Hering, Alessandro M.; Sideris, Ioannis; Trefalt, Simona; Germann, Urs</p> <p>2015-04-01</p> <p>Heavy precipitation, hail, and wind gusts are the fundamental meteorological hazards associated with strong convection and thunderstorms. The thread is particularly severe in mountainous areas, e.g. it is estimated that on average between 50% and 80% of all weather-related damage in Switzerland is caused by strong thunderstorms (Hilker et al., 2010). Intense atmospheric convection is governed by processes that range from the synoptic to the microphysical scale and are considered to be one of the most challenging and difficult weather phenomena to predict. Even though numerical weather prediction <span class="hlt">models</span> have some skills to predict convection, in general the exact location of the convective initialization and its propagation cannot be forecasted by these <span class="hlt">models</span> with sufficient precision. Hence, there is a strong interest to improve the short-term forecast by using statistical, object oriented and/or heuristic nowcasting methods. MeteoSwiss has developed several operational nowcasting systems for this purpose such as TRT (Hering, 2008) and COALITION (Nisi, 2014). In this contribution we analyze the typical development of convection using <span class="hlt">measurements</span> of the Swiss C-band Dual Polarization Doppler weather radar network, the MSG SEVIRI satellite, and the Météorage lighting network. The <span class="hlt">observations</span> are complemented with the analysis and forecasts of the COSMO <span class="hlt">model</span>. Special attention is given to the typical evolutionary stages like the pre-convective environment, convective initiation, cloud top glaciation, start, maximum, and end of precipitation and lightning activity. The pre-convective environment is examined using instability indices derived from SEVIRI <span class="hlt">observations</span> and the COSMO forecasts. During the early development satellite <span class="hlt">observations</span> are used to <span class="hlt">observe</span> the rise of the cloud top, the growth of the cloud droplet or crystals, and the glaciation of the cloud top. SEVIRI brightness temperatures, channel differences, and temporal trends as suggested by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050139693','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050139693"><span>Earth <span class="hlt">Observing</span> System (EOS) Snow and Ice Products for <span class="hlt">Observation</span> and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hall, D.; Kaminski, M.; Cavalieri, D.; Dickinson, R.; Marquis, M.; Riggs, G.; Robinson, D.; VanWoert, M.; Wolfe, R.</p> <p>2005-01-01</p> <p>Snow and ice are the key components of the Earth's cryosphere, and their influence on the Earth's energy balance is very significant due at least in part to the large areal extent and high albedo characterizing these features. Large changes in the cryosphere have been <span class="hlt">measured</span> over the last century and especially over the past decade, and remote sensing plays a pivotal role in documenting these changes. Many of NASA's Earth <span class="hlt">Observing</span> System (EOS) products derived from instruments on the Terra, Aqua, and Ice, Cloud and land Elevation Satellite (ICESat) satellites are useful for <span class="hlt">measuring</span> changes in features that are associated with climate change. The utility of the products is continually enhanced as the length of the time series increases. To gain a more coherent view of the cryosphere and its historical and recent changes, the EOS products may be employed together, in conjunction with other sources of data, and in <span class="hlt">models</span>. To further this goal, the first EOS Snow and Ice Products Workshop was convened. The specific goals of the workshop were to provide current and prospective users of EOS snow and ice products up-to-date information on the products, their validation status and future enhancements, to help users utilize the data products through hands-on demonstrations, and to facilitate the integration of EOS products into <span class="hlt">models</span>. Oral and poster sessions representing a wide variety of snow and ice topics were held; three panels were also convened to discuss workshop themes. Panel discussions focused on data fusion and assimilation of the products into <span class="hlt">models</span>. Approximately 110 people attended, representing a wide array of interests and organizations in the cryospheric community.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H41H1543W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H41H1543W"><span>Snow mass and river flows <span class="hlt">modelled</span> using GRACE total water storage <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, S.</p> <p>2017-12-01</p> <p>Snow mass and river flow <span class="hlt">measurements</span> are difficult and less accurate in cold regions due to the hash environment. Floods in cold regions are commonly a result of snowmelt during the spring break-up. Flooding is projected to increase with climate change in many parts of the world. Forecasting floods from snowmelt remains a challenge due to scarce and quality issues in basin-scale snow <span class="hlt">observations</span> and lack of knowledge for cold region hydrological processes. This study developed a <span class="hlt">model</span> for estimating basin-level snow mass (snow water equivalent SWE) and river flows using the total water storage (TWS) <span class="hlt">observations</span> from the Gravity Recovery and Climate Experiment (GRACE) satellite mission. The SWE estimation is based on mass balance approach which is independent of in situ snow gauge <span class="hlt">observations</span>, thus largely eliminates the limitations and uncertainties with traditional in situ or remote sensing snow estimates. The <span class="hlt">model</span> forecasts river flows by simulating surface runoff from snowmelt and the corresponding baseflow from groundwater discharge. Snowmelt is predicted using a temperature index <span class="hlt">model</span>. Baseflow is predicted using a modified linear reservoir <span class="hlt">model</span>. The <span class="hlt">model</span> also quantifies the hysteresis between the snowmelt and the streamflow rates, or the lump time for water travel in the basin. The <span class="hlt">model</span> was applied to the Red River Basin, the Mackenzie River Basin, and the Hudson Bay Lowland Basins in Canada. The predicted river flows were compared with the <span class="hlt">observed</span> values at downstream hydrometric stations. The results were also compared to that for the Lower Fraser River obtained in a separate study to help better understand the roles of environmental factors in determining flood and their variations with different hydroclimatic conditions. This study advances the applications of space-based time-variable gravity <span class="hlt">measurements</span> in cold region snow mass estimation, river flow and flood forecasting. It demonstrates a relatively simple method that only needs GRACE TWS</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24769431','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24769431"><span>Reliability and validity of the Pragmatics <span class="hlt">Observational</span> <span class="hlt">Measure</span> (POM): a new <span class="hlt">observational</span> <span class="hlt">measure</span> of pragmatic language for children.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cordier, Reinie; Munro, Natalie; Wilkes-Gillan, Sarah; Speyer, Renée; Pearce, Wendy M</p> <p>2014-07-01</p> <p>There is a need for a reliable and valid assessment of childhood pragmatic language skills during peer-peer interactions. This study aimed to evaluate the psychometric properties of a newly developed pragmatic assessment, the Pragmatic <span class="hlt">Observational</span> <span class="hlt">Measure</span> (POM). The psychometric properties of the POM were investigated from <span class="hlt">observational</span> data of two studies - study 1 involved 342 children aged 5-11 years (108 children with ADHD; 108 typically developing playmates; 126 children in the control group), and study 2 involved 9 children with ADHD who attended a 7-week play-based intervention. The psychometric properties of the POM were determined based on the COnsensus-based Standards for the selection of health status <span class="hlt">Measurement</span> INstruments (COSMIN) taxonomy of psychometric properties and definitions for health-related outcomes; the Pragmatic Protocol was used as the reference tool against which the POM was evaluated. The POM demonstrated sound psychometric properties in all the reliability, validity and interpretability criteria against which it was assessed. The findings showed that the POM is a reliable and valid <span class="hlt">measure</span> of pragmatic language skills of children with ADHD between the age of 5 and 11 years and has clinical utility in identifying children with pragmatic language difficulty. Copyright © 2014 The Authors. Published by Elsevier Ltd.. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8827621','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8827621"><span>Overview of meteorological <span class="hlt">measurements</span> for aerial spray <span class="hlt">modeling</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rafferty, J E; Biltoft, C A; Bowers, J F</p> <p>1996-06-01</p> <p>The routine meteorological <span class="hlt">observations</span> made by the National Weather Service have a spatial resolution on the order of 1,000 km, whereas the resolution needed to conduct or <span class="hlt">model</span> aerial spray applications is on the order of 1-10 km. Routinely available <span class="hlt">observations</span> also do not include the detailed information on the turbulence and thermal structure of the boundary layer that is needed to predict the transport, dispersion, and deposition of aerial spray releases. This paper provides an overview of the information needed to develop the meteorological inputs for an aerial spray <span class="hlt">model</span> such as the FSCBG and discusses the different types of instruments that are available to make the necessary <span class="hlt">measurements</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=kernel&pg=3&id=EJ1121533','ERIC'); return false;" href="https://eric.ed.gov/?q=kernel&pg=3&id=EJ1121533"><span>Asymptotic Standard Errors of <span class="hlt">Observed</span>-Score Equating with Polytomous IRT <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Andersson, Björn</p> <p>2016-01-01</p> <p>In <span class="hlt">observed</span>-score equipercentile equating, the goal is to make scores on two scales or tests <span class="hlt">measuring</span> the same construct comparable by matching the percentiles of the respective score distributions. If the tests consist of different items with multiple categories for each item, a suitable <span class="hlt">model</span> for the responses is a polytomous item response…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SGeo...33..779S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SGeo...33..779S"><span><span class="hlt">Observing</span> and <span class="hlt">Modeling</span> Earth's Energy Flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stevens, Bjorn; Schwartz, Stephen E.</p> <p>2012-07-01</p> <p>This article reviews, from the authors' perspective, progress in <span class="hlt">observing</span> and <span class="hlt">modeling</span> energy flows in Earth's climate system. Emphasis is placed on the state of understanding of Earth's energy flows and their susceptibility to perturbations, with particular emphasis on the roles of clouds and aerosols. More accurate <span class="hlt">measurements</span> of the total solar irradiance and the rate of change of ocean enthalpy help constrain individual components of the energy budget at the top of the atmosphere to within ±2 W m-2. The <span class="hlt">measurements</span> demonstrate that Earth reflects substantially less solar radiation and emits more terrestrial radiation than was believed even a decade ago. Active remote sensing is helping to constrain the surface energy budget, but new estimates of downwelling surface irradiance that benefit from such methods are proving difficult to reconcile with existing precipitation climatologies. Overall, the energy budget at the surface is much more uncertain than at the top of the atmosphere. A decade of high-precision <span class="hlt">measurements</span> of the energy budget at the top of the atmosphere is providing new opportunities to track Earth's energy flows on timescales ranging from days to years, and at very high spatial resolution. The <span class="hlt">measurements</span> show that the principal limitation in the estimate of secular trends now lies in the natural variability of the Earth system itself. The forcing-feedback-response framework, which has developed to understand how changes in Earth's energy flows affect surface temperature, is reviewed in light of recent work that shows fast responses (adjustments) of the system are central to the definition of the effective forcing that results from a change in atmospheric composition. In many cases, the adjustment, rather than the characterization of the compositional perturbation (associated, for instance, with changing greenhouse gas concentrations, or aerosol burdens), limits accurate determination of the radiative forcing. Changes in clouds contribute</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980001208','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980001208"><span><span class="hlt">Observational</span> and <span class="hlt">Modeling</span> Studies of Clouds and the Hydrological Cycle</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Somerville, Richard C. J.</p> <p>1997-01-01</p> <p>Our approach involved validating parameterizations directly against <span class="hlt">measurements</span> from field programs, and using this validation to tune existing parameterizations and to guide the development of new ones. We have used a single-column <span class="hlt">model</span> (SCM) to make the link between <span class="hlt">observations</span> and parameterizations of clouds, including explicit cloud microphysics (e.g., prognostic cloud liquid water used to determine cloud radiative properties). Surface and satellite radiation <span class="hlt">measurements</span> were used to provide an initial evaluation of the performance of the different parameterizations. The results of this evaluation will then used to develop improved cloud and cloud-radiation schemes, which were tested in GCM experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61..787G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61..787G"><span>Research on navigation of satellite constellation based on an asynchronous <span class="hlt">observation</span> <span class="hlt">model</span> using X-ray pulsar</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Pengbin; Sun, Jian; Hu, Shuling; Xue, Ju</p> <p>2018-02-01</p> <p>Pulsar navigation is a promising navigation method for high-altitude orbit space tasks or deep space exploration. At present, an important reason for restricting the development of pulsar navigation is that navigation accuracy is not high due to the slow update of the <span class="hlt">measurements</span>. In order to improve the accuracy of pulsar navigation, an asynchronous <span class="hlt">observation</span> <span class="hlt">model</span> which can improve the update rate of the <span class="hlt">measurements</span> is proposed on the basis of satellite constellation which has a broad space for development because of its visibility and reliability. The simulation results show that the asynchronous <span class="hlt">observation</span> <span class="hlt">model</span> improves the positioning accuracy by 31.48% and velocity accuracy by 24.75% than that of the synchronous <span class="hlt">observation</span> <span class="hlt">model</span>. With the new Doppler effects compensation method in the asynchronous <span class="hlt">observation</span> <span class="hlt">model</span> proposed in this paper, the positioning accuracy is improved by 32.27%, and the velocity accuracy is improved by 34.07% than that of the traditional method. The simulation results show that without considering the clock error will result in a filtering divergence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29880775','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29880775"><span>Indirect <span class="hlt">Measurement</span> of Rotor Dynamic Imbalance for Control Moment Gyroscopes via Gimbal Disturbance <span class="hlt">Observer</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huang, Liya; Wu, Zhong; Wang, Kan</p> <p>2018-06-07</p> <p>The high-precision speed control of gimbal servo systems is the key to generating high-precision torque for control moment gyroscopes (CMGs) in spacecrafts. However, the control performance of gimbal servo systems may be degraded significantly by disturbances, especially a dynamic imbalance disturbance with the same frequency as the high-speed rotor. For assembled CMGs, it is very difficult to <span class="hlt">measure</span> the rotor imbalance directly by using a dynamic balancing machine. In this paper, a gimbal disturbance <span class="hlt">observer</span> is proposed to estimate the dynamic imbalance of the rotor assembled in the CMG. First, a third-order dynamical system is established to describe the disturbance dynamics of the gimbal servo system, in which the rotor dynamic imbalance torque along the gimbal axis and the other disturbances are <span class="hlt">modeled</span> to be periodic and bounded, respectively. Then, the gimbal disturbance <span class="hlt">observer</span> is designed for the third-order dynamical system by using the total disturbance as a virtual <span class="hlt">measurement</span>. Since the virtual <span class="hlt">measurement</span> is derived from the inverse dynamics of the gimbal servo system, the information of the rotor dynamic imbalance can be obtained indirectly only using the <span class="hlt">measurements</span> of gimbal speed and three-phase currents. Semi-physical experimental results demonstrate the effectiveness of the <span class="hlt">observer</span> by using a CMG simulator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080023294','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080023294"><span>A Physical <span class="hlt">Model</span> to Estimate Snowfall over Land using AMSU-B <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kim, Min-Jeong; Weinman, J. A.; Olson, W. S.; Chang, D.-E.; Skofronick-Jackson, G.; Wang, J. R.</p> <p>2008-01-01</p> <p>In this study, we present an improved physical <span class="hlt">model</span> to retrieve snowfall rate over land using brightness temperature <span class="hlt">observations</span> from the National Oceanic and Atmospheric Administration's (NOAA) Advanced Microwave Sounder Unit-B (AMSU-B) at 89 GHz, 150 GHz, 183.3 +/- 1 GHz, 183.3 +/- 3 GHz, and 183.3 +/- 7 GHz. The retrieval <span class="hlt">model</span> is applied to the New England blizzard of March 5, 2001 which deposited about 75 cm of snow over much of Vermont, New Hampshire, and northern New York. In this improved physical <span class="hlt">model</span>, prior retrieval assumptions about snowflake shape, particle size distributions, environmental conditions, and optimization methodology have been updated. Here, single scattering parameters for snow particles are calculated with the Discrete-Dipole Approximation (DDA) method instead of assuming spherical shapes. Five different snow particle <span class="hlt">models</span> (hexagonal columns, hexagonal plates, and three different kinds of aggregates) are considered. Snow particle size distributions are assumed to vary with air temperature and to follow aircraft <span class="hlt">measurements</span> described by previous studies. Brightness temperatures at AMSU-B frequencies for the New England blizzard are calculated using these DDA calculated single scattering parameters and particle size distributions. The vertical profiles of pressure, temperature, relative humidity and hydrometeors are provided by MM5 <span class="hlt">model</span> simulations. These profiles are treated as the a priori data base in the Bayesian retrieval algorithm. In algorithm applications to the blizzard data, calculated brightness temperatures associated with selected database profiles agree with AMSU-B <span class="hlt">observations</span> to within about +/- 5 K at all five frequencies. Retrieved snowfall rates compare favorably with the near-concurrent National Weather Service (NWS) radar reflectivity <span class="hlt">measurements</span>. The relationships between the NWS radar <span class="hlt">measured</span> reflectivities Z(sub e) and retrieved snowfall rate R for a given snow particle <span class="hlt">model</span> are derived by a histogram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.8274T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.8274T"><span>Evaluation of atmospheric dust prediction <span class="hlt">models</span> using ground-based <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Terradellas, Enric; María Baldasano, José; Cuevas, Emilio; Basart, Sara; Huneeus, Nicolás; Camino, Carlos; Dundar, Cinhan; Benincasa, Francesco</p> <p>2013-04-01</p> <p>An important step in numerical prediction of mineral dust is the <span class="hlt">model</span> evaluation aimed to assess its performance to forecast the atmospheric dust content and to lead to new directions in <span class="hlt">model</span> development and improvement. The first problem to address the evaluation is the scarcity of ground-based routine <span class="hlt">observations</span> intended for dust monitoring. An alternative option would be the use of satellite products. They have the advantage of a large spatial coverage and a regular availability. However, they do have numerous drawbacks that make the quantitative retrievals of aerosol-related variables difficult and imprecise. This work presents the use of different ground-based <span class="hlt">observing</span> systems for the evaluation of dust <span class="hlt">models</span> in the Regional Center for Northern Africa, Middle East and Europe of the World Meteorological Organization (WMO) Sand and Dust Storm Warning Advisory and Assessment System (SDS-WAS). The dust optical depth at 550 nm forecast by different <span class="hlt">models</span> is regularly compared with the AERONET <span class="hlt">measurements</span> of Aerosol Optical Depth (AOD) for 40 selected stations. Photometric <span class="hlt">measurements</span> are a powerful tool for remote sensing of the atmosphere allowing retrieval of aerosol properties, such as AOD. This variable integrates the contribution of different aerosol types, but may be complemented with spectral information that enables hypotheses about the nature of the particles. Comparison is restricted to cases with low Ångström exponent values in order to ensure that coarse mineral dust is the dominant aerosol type. Additionally to column dust load, it is important to evaluate dust surface concentration and dust vertical profiles. Air quality monitoring stations are the main source of data for the evaluation of surface concentration. However they are concentrated in populated and industrialized areas around the Mediterranean. In the present contribution, results of different <span class="hlt">models</span> are compared with <span class="hlt">observations</span> of PM10 from the Turkish air quality network for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20156988','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20156988"><span>Wavelet-based functional linear mixed <span class="hlt">models</span>: an application to <span class="hlt">measurement</span> error-corrected distributed lag <span class="hlt">models</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Malloy, Elizabeth J; Morris, Jeffrey S; Adar, Sara D; Suh, Helen; Gold, Diane R; Coull, Brent A</p> <p>2010-07-01</p> <p>Frequently, exposure data are <span class="hlt">measured</span> over time on a grid of discrete values that collectively define a functional <span class="hlt">observation</span>. In many applications, researchers are interested in using these <span class="hlt">measurements</span> as covariates to predict a scalar response in a regression setting, with interest focusing on the most biologically relevant time window of exposure. One example is in panel studies of the health effects of particulate matter (PM), where particle levels are <span class="hlt">measured</span> over time. In such studies, there are many more values of the functional data than <span class="hlt">observations</span> in the data set so that regularization of the corresponding functional regression coefficient is necessary for estimation. Additional issues in this setting are the possibility of exposure <span class="hlt">measurement</span> error and the need to incorporate additional potential confounders, such as meteorological or co-pollutant <span class="hlt">measures</span>, that themselves may have effects that vary over time. To accommodate all these features, we develop wavelet-based linear mixed distributed lag <span class="hlt">models</span> that incorporate repeated <span class="hlt">measures</span> of functional data as covariates into a linear mixed <span class="hlt">model</span>. A Bayesian approach to <span class="hlt">model</span> fitting uses wavelet shrinkage to regularize functional coefficients. We show that, as long as the exposure error induces fine-scale variability in the functional exposure profile and the distributed lag function representing the exposure effect varies smoothly in time, the <span class="hlt">model</span> corrects for the exposure <span class="hlt">measurement</span> error without further adjustment. Both these conditions are likely to hold in the environmental applications we consider. We examine properties of the method using simulations and apply the method to data from a study examining the association between PM, <span class="hlt">measured</span> as hourly averages for 1-7 days, and markers of acute systemic inflammation. We use the method to fully control for the effects of confounding by other time-varying predictors, such as temperature and co-pollutants.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150004052','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150004052"><span><span class="hlt">Observations</span> of Spacecraft Bearing Lubricant Redistribution Based on Thermal Conductance <span class="hlt">Measurements</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Takeuchi, Yoshimi R.; Frantz, Peter P.; Hilton, Michael R.</p> <p>2014-01-01</p> <p>The performance and life of precision ball bearings are critically dependent on maintaining a quantity of oil at the ball/race interface that is sufficient to support a robust protective film. In space applications, where parched conditions are intentionally the norm, harsh operating conditions can displace the small reserves of oil, resulting in reduced film thickness and premature wear. In the past, these effects have proven difficult to <span class="hlt">model</span> or to <span class="hlt">measure</span> experimentally. This paper describes a study addressing this challenge, where bearing thermal conductance <span class="hlt">measurements</span> are employed to infer changes in lubricant quantity at the critical rolling interfaces. In the first part of the paper, we explain how the lubricant's presence and its quantity impacts bearing thermal conductance <span class="hlt">measurements</span>. For a stationary bearing, we show that conductance is directly related to the lubricant quantity in the ball/race contacts. Hence, aspects of bearing performance related to oil quantity can be understood and insights improved with thermal conductance data. For a moving bearing, a different mechanism of heat transfer dominates and is dependent on lubricant film thickness on the ball. In the second part of the report, we discuss lubricant quantity <span class="hlt">observations</span> based on bearing thermal conductance <span class="hlt">measurements</span>. Lubricant quantity, and thus bearing thermal conductance, depends on various initial and operating conditions and is impacted further by the run-in process. A significant effect of maximum run-in speed was also <span class="hlt">observed</span>, with less oil remaining after obtaining higher speeds. Finally, we show that some of the lubricant that is displaced between the ball and race during run-in operation can be recovered during rest, and we <span class="hlt">measure</span> the rate of recovery for one example.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001SPIE.4381..225G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001SPIE.4381..225G"><span><span class="hlt">Observations</span> and <span class="hlt">model</span> predictions of water skin temperatures at MTI core site lakes and reservoirs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garrett, Alfred J.; Kurzeja, Robert J.; O'Steen, Byron L.; Parker, Matthew J.; Pendergast, Malcolm M.; Villa-Aleman, Eliel; Pagnutti, Mary A.</p> <p>2001-08-01</p> <p>The Savannah River Technology Center (SRTC) <span class="hlt">measured</span> water skin temperatures at four of the Multi-spectral Thermal Imager (MTI) core sites. The depression of the skin temperature relative to the bulk water temperature ((Delta) T) a few centimeters below the surface is a complex function of the weather conditions, turbulent mixing in the water and the bulk water temperature. <span class="hlt">Observed</span> skin temperature depressions range from near zero to more than 1.0 degree(s)C. Skin temperature depressions tend to be larger when the bulk water temperature is high, but large depressions were also <span class="hlt">observed</span> in cool bodies of water in calm conditions at night. We compared (Delta) T predictions from three <span class="hlt">models</span> (SRTC, Schlussel and Wick) against <span class="hlt">measured</span> (Delta) T's from 15 data sets taken at the MTI core sites. The SRTC and Wick <span class="hlt">models</span> performed somewhat better than the Schlussel <span class="hlt">model</span>, with RMSE and average absolute errors of about 0.2 degree(s)C, relative to 0.4 degree(s)C for the Schlussel <span class="hlt">model</span>. The average <span class="hlt">observed</span> (Delta) T for all 15 databases was -0.7 degree(s)C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.T14C..04V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.T14C..04V"><span>Linking Geomechanical <span class="hlt">Models</span> with <span class="hlt">Observations</span> of Microseismicity during CCS Operations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Verdon, J.; Kendall, J.; White, D.</p> <p>2012-12-01</p> <p>During CO2 injection for the purposes of carbon capture and storage (CCS), injection-induced fracturing of the overburden represents a key risk to storage integrity. Fractures in a caprock provide a pathway along which buoyant CO2 can rise and escape the storage zone. Therefore the ability to link field-scale geomechanical <span class="hlt">models</span> with field geophysical <span class="hlt">observations</span> is of paramount importance to guarantee secure CO2 storage. Accurate location of microseismic events identifies where brittle failure has occurred on fracture planes. This is a manifestation of the deformation induced by CO2 injection. As the pore pressure is increased during injection, effective stress is decreased, leading to inflation of the reservoir and deformation of surrounding rocks, which creates microseismicity. The deformation induced by injection can be simulated using finite-element mechanical <span class="hlt">models</span>. Such a <span class="hlt">model</span> can be used to predict when and where microseismicity is expected to occur. However, typical elements in a field scale mechanical <span class="hlt">models</span> have decameter scales, while the rupture size for microseismic events are typically of the order of 1 square meter. This means that mapping <span class="hlt">modeled</span> stress changes to predictions of microseismic activity can be challenging. Where larger scale faults have been identified, they can be included explicitly in the geomechanical <span class="hlt">model</span>. Where movement is simulated along these discrete features, it can be assumed that microseismicity will occur. However, microseismic events typically occur on fracture networks that are too small to be simulated explicitly in a field-scale <span class="hlt">model</span>. Therefore, the likelihood of microseismicity occurring must be estimated within a finite element that does not contain explicitly <span class="hlt">modeled</span> discontinuities. This can be done in a number of ways, including the utilization of <span class="hlt">measures</span> such as closeness on the stress state to predetermined failure criteria, either for planes with a defined orientation (the Mohr-Coulomb criteria) for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014A%26A...567A.110B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014A%26A...567A.110B"><span><span class="hlt">Observations</span> and NLTE <span class="hlt">modeling</span> of Ellerman bombs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berlicki, A.; Heinzel, P.</p> <p>2014-07-01</p> <p>Context. Ellerman bombs (EBs) are short-lived, compact, and spatially well localized emission structures that are <span class="hlt">observed</span> well in the wings of the hydrogen Hα line. EBs are also <span class="hlt">observed</span> in the chromospheric CaII lines and in UV continua as bright points located within active regions. Hα line profiles of EBs show a deep absorption at the line center and enhanced emission in the line wings with maxima around ±1 Å from the line center. Similar shapes of the line profiles are <span class="hlt">observed</span> for the CaII IR line at 8542 Å. In CaII H and K lines the emission peaks are much stronger, and EBs emission is also enhanced in the line center. Aims: It is generally accepted that EBs may be considered as compact microflares located in lower solar atmosphere that contribute to the heating of these low-lying regions, close to the temperature minimum of the atmosphere. However, it is still not clear where exactly the emission of EBs is formed in the solar atmosphere. High-resolution spectrophotometric <span class="hlt">observations</span> of EBs were used for determining of their physical parameters and construction of semi-empirical <span class="hlt">models</span>. Obtained <span class="hlt">models</span> allow us to determine the position of EBs in the solar atmosphere, as well as the vertical structure of the activated EB atmosphere Methods: In our analysis we used <span class="hlt">observations</span> of EBs obtained in the Hα and CaII H lines with the Dutch Open Telescope (DOT). These one-hour long simultaneous sequences obtained with high temporal and spatial resolution were used to determine the line emissions. To analyze them, we used NLTE numerical codes for the construction of grids of 243 semi-empirical <span class="hlt">models</span> simulating EBs structures. In this way, the <span class="hlt">observed</span> emission could be compared with the synthetic line spectra calculated for all such <span class="hlt">models</span>. Results: For a specific <span class="hlt">model</span> we found reasonable agreement between the <span class="hlt">observed</span> and theoretical emission and thus we consider such <span class="hlt">model</span> as a good approximation to EBs atmospheres. This <span class="hlt">model</span> is characterized by an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.2615M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.2615M"><span>Southeast Atmosphere Studies: learning from <span class="hlt">model-observation</span> syntheses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mao, Jingqiu; Carlton, Annmarie; Cohen, Ronald C.; Brune, William H.; Brown, Steven S.; Wolfe, Glenn M.; Jimenez, Jose L.; Pye, Havala O. T.; Ng, Nga Lee; Xu, Lu; McNeill, V. Faye; Tsigaridis, Kostas; McDonald, Brian C.; Warneke, Carsten; Guenther, Alex; Alvarado, Matthew J.; de Gouw, Joost; Mickley, Loretta J.; Leibensperger, Eric M.; Mathur, Rohit; Nolte, Christopher G.; Portmann, Robert W.; Unger, Nadine; Tosca, Mika; Horowitz, Larry W.</p> <p>2018-02-01</p> <p>Concentrations of atmospheric trace species in the United States have changed dramatically over the past several decades in response to pollution control strategies, shifts in domestic energy policy and economics, and economic development (and resulting emission changes) elsewhere in the world. Reliable projections of the future atmosphere require <span class="hlt">models</span> to not only accurately describe current atmospheric concentrations, but to do so by representing chemical, physical and biological processes with conceptual and quantitative fidelity. Only through incorporation of the processes controlling emissions and chemical mechanisms that represent the key transformations among reactive molecules can <span class="hlt">models</span> reliably project the impacts of future policy, energy and climate scenarios. Efforts to properly identify and implement the fundamental and controlling mechanisms in atmospheric <span class="hlt">models</span> benefit from intensive <span class="hlt">observation</span> periods, during which collocated <span class="hlt">measurements</span> of diverse, speciated chemicals in both the gas and condensed phases are obtained. The Southeast Atmosphere Studies (SAS, including SENEX, SOAS, NOMADSS and SEAC4RS) conducted during the summer of 2013 provided an unprecedented opportunity for the atmospheric <span class="hlt">modeling</span> community to come together to evaluate, diagnose and improve the representation of fundamental climate and air quality processes in <span class="hlt">models</span> of varying temporal and spatial scales.This paper is aimed at discussing progress in evaluating, diagnosing and improving air quality and climate <span class="hlt">modeling</span> using comparisons to SAS <span class="hlt">observations</span> as a guide to thinking about improvements to mechanisms and parameterizations in <span class="hlt">models</span>. The effort focused primarily on <span class="hlt">model</span> representation of fundamental atmospheric processes that are essential to the formation of ozone, secondary organic aerosol (SOA) and other trace species in the troposphere, with the ultimate goal of understanding the radiative impacts of these species in the southeast and elsewhere. Here we</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=6020695','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=6020695"><span>Southeast Atmosphere Studies: learning from <span class="hlt">model-observation</span> syntheses</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Mao, Jingqiu; Carlton, Annmarie; Cohen, Ronald C.; Brune, William H.; Brown, Steven S.; Wolfe, Glenn M.; Jimenez, Jose L.; Pye, Havala O. T.; Ng, Nga Lee; Xu, Lu; McNeill, V. Faye; Tsigaridis, Kostas; McDonald, Brian C.; Warneke, Carsten; Guenther, Alex; Alvarado, Matthew J.; de Gouw, Joost; Mickley, Loretta J.; Leibensperger, Eric M.; Mathur, Rohit; Nolte, Christopher G.; Portmann, Robert W.; Unger, Nadine; Tosca, Mika; Horowitz, Larry W.</p> <p>2018-01-01</p> <p>Concentrations of atmospheric trace species in the United States have changed dramatically over the past several decades in response to pollution control strategies, shifts in domestic energy policy and economics, and economic development (and resulting emission changes) elsewhere in the world. Reliable projections of the future atmosphere require <span class="hlt">models</span> to not only accurately describe current atmospheric concentrations, but to do so by representing chemical, physical and biological processes with conceptual and quantitative fidelity. Only through incorporation of the processes controlling emissions and chemical mechanisms that represent the key transformations among reactive molecules can <span class="hlt">models</span> reliably project the impacts of future policy, energy and climate scenarios. Efforts to properly identify and implement the fundamental and controlling mechanisms in atmospheric <span class="hlt">models</span> benefit from intensive <span class="hlt">observation</span> periods, during which collocated <span class="hlt">measurements</span> of diverse, speciated chemicals in both the gas and condensed phases are obtained. The Southeast Atmosphere Studies (SAS, including SENEX, SOAS, NOMADSS and SEAC4RS) conducted during the summer of 2013 provided an unprecedented opportunity for the atmospheric <span class="hlt">modeling</span> community to come together to evaluate, diagnose and improve the representation of fundamental climate and air quality processes in <span class="hlt">models</span> of varying temporal and spatial scales. This paper is aimed at discussing progress in evaluating, diagnosing and improving air quality and climate <span class="hlt">modeling</span> using comparisons to SAS <span class="hlt">observations</span> as a guide to thinking about improvements to mechanisms and parameterizations in <span class="hlt">models</span>. The effort focused primarily on <span class="hlt">model</span> representation of fundamental atmospheric processes that are essential to the formation of ozone, secondary organic aerosol (SOA) and other trace species in the troposphere, with the ultimate goal of understanding the radiative impacts of these species in the southeast and elsewhere. Here we</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20180002911&hterms=learning&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dlearning','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20180002911&hterms=learning&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dlearning"><span>Southeast Atmosphere Studies: Learning from <span class="hlt">Model-Observation</span> Syntheses</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mao, Jingqiu; Carlton, Annmarie; Cohen, Ronald C.; Brune, William H.; Brown, Steven S.; Wolfe, Glenn M.; Jimenez, Jose L.; Pye, Havala O. T.; Ng, Nga Lee; Xu, Lu; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20180002911'); toggleEditAbsImage('author_20180002911_show'); toggleEditAbsImage('author_20180002911_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20180002911_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20180002911_hide"></p> <p>2018-01-01</p> <p>Concentrations of atmospheric trace species in the United States have changed dramatically over the past several decades in response to pollution control strategies, shifts in domestic energy policy and economics, and economic development (and resulting emission changes) elsewhere in the world. Reliable projections of the future atmosphere require <span class="hlt">models</span> to not only accurately describe current atmospheric concentrations, but to do so by representing chemical, physical and biological processes with conceptual and quantitative fidelity. Only through incorporation of the processes controlling emissions and chemical mechanisms that represent the key transformations among reactive molecules can <span class="hlt">models</span> reliably project the impacts of future policy, energy and climate scenarios. Efforts to properly identify and implement the fundamental and controlling mechanisms in atmospheric <span class="hlt">models</span> benefit from intensive <span class="hlt">observation</span> periods, during which collocated <span class="hlt">measurements</span> of diverse, speciated chemicals in both the gas and condensed phases are obtained. The Southeast Atmosphere Studies (SAS, including SENEX, SOAS, NOMADSS and SEAC4RS) conducted during the summer of 2013 provided an unprecedented opportunity for the atmospheric <span class="hlt">modeling</span> community to come together to evaluate, diagnose and improve the representation of fundamental climate and air quality processes in <span class="hlt">models</span> of varying temporal and spatial scales. This paper is aimed at discussing progress in evaluating, diagnosing and improving air quality and climate <span class="hlt">modeling</span> using comparisons to SAS <span class="hlt">observations</span> as a guide to thinking about improvements to mechanisms and parameterizations in <span class="hlt">models</span>. The effort focused primarily on <span class="hlt">model</span> representation of fundamental atmospheric processes that are essential to the formation of ozone, secondary organic aerosol (SOA) and other trace species in the troposphere, with the ultimate goal of understanding the radiative impacts of these species in the southeast and elsewhere. Here we</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25682557','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25682557"><span>Intra- and inter-<span class="hlt">observer</span> agreement on diagnosis of Dupuytren disease, <span class="hlt">measurements</span> of severity of contracture, and disease extent.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Broekstra, Dieuwke C; Lanting, Rosanne; Werker, Paul M N; van den Heuvel, Edwin R</p> <p>2015-08-01</p> <p>Dupuytren disease (DD) is a fibrosing disease affecting the palmar aponeurosis, and is mostly treated by surgery based on <span class="hlt">measurement</span> of severity of flexion contracture of the fingers. Literature concerning the <span class="hlt">measurement</span> reliability is scarce. This study aimed to determine the intra- and inter-<span class="hlt">observer</span> agreement of four variables for diagnosing DD, determining severity of contracture, and disease extent. One of them is a new <span class="hlt">measurement</span> on the area of nodules and cords for <span class="hlt">measuring</span> the disease extent in early disease stages. An agreement study (n = 54) was performed by two trained investigators. Agreement was calculated per finger, based on an intraclass correlation coefficient (ICC) using a latent variable <span class="hlt">model</span> on subjects for diagnosis and Tubiana stage. For total passive extension deficit (TPED) and the area of nodules and cords, agreement was calculated with an ICC using a one-way random effects <span class="hlt">model</span> with subject as random effect. Inter-<span class="hlt">observer</span> agreement was very good for diagnosing DD (ICC: 95.5%-99.9%) and good to very good for classifying Tubiana stage (ICC: 73.5%-94.9%). Agreements for area and TPED were moderate (middle finger) to very good (ICC: 48.4%-98.6% and 45.0%-99.5%, respectively). Intra-<span class="hlt">observer</span> agreement was slightly higher on average than inter-<span class="hlt">observer</span> agreement. Overall, the intra- and inter-<span class="hlt">observer</span> agreement in diagnosing DD, and determining the severity of flexion contracture is high. Also, the newly introduced variable area of nodules and cords has high intra- and inter-<span class="hlt">observer</span> agreement, indicating that it is suitable to <span class="hlt">measure</span> disease extent. Copyright © 2015 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MARF46002A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MARF46002A"><span>Correlators in simultaneous <span class="hlt">measurement</span> of non-commuting qubit <span class="hlt">observables</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Atalaya, Juan; Hacohen-Gourgy, Shay; Martin, Leigh S.; Siddiqi, Irfan; Korotkov, Alexander N.</p> <p></p> <p>We consider simultaneous continuous <span class="hlt">measurement</span> of non-commuting qubit <span class="hlt">observables</span> and analyze multi-time correlators 〈i κ1 (t1) ^i κN (tN) 〉 for output signals i κ (t) from the detectors. Both informational (''spooky'') and phase backactions from cQED-type <span class="hlt">measurements</span> with phase-sensitive amplifiers are taken into account. We find an excellent agreement between analytical results and experimental data for two-time correlators of the output signals from simultaneous <span class="hlt">measurement</span> of qubit <span class="hlt">observables</span> σx and σφ =σx cosφ +σy sinφ . The correlators can be used to extract small deviations of experimental parameters, e.g., phase backaction and residual Rabi frequency. The multi-time correlators are important in analysis of Bacon-Shor error correction/detection codes, operated with continuous <span class="hlt">measurements</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMIN41C1622K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMIN41C1622K"><span>Implementing CUAHSI and SWE <span class="hlt">observation</span> data <span class="hlt">models</span> in the long-term monitoring infrastructure TERENO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klump, J. F.; Stender, V.; Schroeder, M.</p> <p>2013-12-01</p> <p>) about the data values in combination with information about the sensor systems. Also the CUAHSI <span class="hlt">model</span> is supported by a large and active international user community. The 52° North SOS data <span class="hlt">model</span> can be <span class="hlt">modeled</span> as a sub-set of the CUHASI data <span class="hlt">model</span>. In our implementation the 52° North SWE data <span class="hlt">model</span> is implemented as database views of the CUHASI <span class="hlt">model</span> to avoid redundant data storage. An essential aspect in TERENO Northeast is the use of standard OGS web services to facilitate data exchange and interoperability. A uniform treatment of sensor data can be realized through OGC Sensor Web Enablement (SWE) which makes a number of standards and interface definitions available: <span class="hlt">Observation</span> & <span class="hlt">Measurement</span> (O&M) <span class="hlt">model</span> for the description of <span class="hlt">observations</span> and <span class="hlt">measurements</span>, Sensor <span class="hlt">Model</span> Language (SensorML) for the description of sensor systems, Sensor <span class="hlt">Observation</span> Service (SOS) for obtaining sensor <span class="hlt">observations</span>, Sensor Planning Service (SPS) for tasking sensors, Web Notification Service (WNS) for asynchronous dialogues and Sensor Alert Service (SAS) for sending alerts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29029796','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29029796"><span>Robust cubature Kalman filter for GNSS/INS with missing <span class="hlt">observations</span> and colored <span class="hlt">measurement</span> noise.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cui, Bingbo; Chen, Xiyuan; Tang, Xihua; Huang, Haoqian; Liu, Xiao</p> <p>2018-01-01</p> <p>In order to improve the accuracy of GNSS/INS working in GNSS-denied environment, a robust cubature Kalman filter (RCKF) is developed by considering colored <span class="hlt">measurement</span> noise and missing <span class="hlt">observations</span>. First, an improved cubature Kalman filter (CKF) is derived by considering colored <span class="hlt">measurement</span> noise, where the time-differencing approach is applied to yield new <span class="hlt">observations</span>. Then, after analyzing the disadvantages of existing methods, the <span class="hlt">measurement</span> augment in processing colored noise is translated into processing the uncertainties of CKF, and new sigma point update framework is utilized to account for the bounded <span class="hlt">model</span> uncertainties. By reusing the diffused sigma points and approximation residual in the prediction stage of CKF, the RCKF is developed and its error performance is analyzed theoretically. Results of numerical experiment and field test reveal that RCKF is more robust than CKF and extended Kalman filter (EKF), and compared with EKF, the heading error of land vehicle is reduced by about 72.4%. Copyright © 2017 ISA. Published by Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA53C..02W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA53C..02W"><span>Constraints on vertical transport near the polar summer mesopause from PMC <span class="hlt">observations</span> and <span class="hlt">modelling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilms, H.; Rapp, M.; Kirsch, A.</p> <p>2016-12-01</p> <p>The comparison of microphysical simulations of polar mesospheric cloud properties with ground based and satellite borne <span class="hlt">observations</span> suggests that vertical wind variance imposed by gravity waves is an important prerequisite to realistically <span class="hlt">model</span> PMC properties. This paper reviews the available <span class="hlt">observational</span> evidence of vertical wind <span class="hlt">measurements</span> at the polar summer mesopause (including their frequency content). Corresponding results are compared to vertical wind variance from several global <span class="hlt">models</span> and implications for the transport of trace constituents in this altitude region are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080046997&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DH%2526M','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080046997&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DH%2526M"><span><span class="hlt">Observed</span> and <span class="hlt">Modeled</span> HOCl Profiles in the Midlatitude Stratosphere: Implication for Ozone Loss</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kovalenko, L. J.; Jucks, K. W.; Salawitch, R. J.; Toon, G. C.; Blavier, J. F.; Johnson, D. G.; Kleinbohl, A.; Livesey, N. J .; Margitan, J. J.; Pickett, H. M.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20080046997'); toggleEditAbsImage('author_20080046997_show'); toggleEditAbsImage('author_20080046997_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20080046997_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20080046997_hide"></p> <p>2007-01-01</p> <p>Vertical profiles of stratospheric HOCl calculated with a diurnal steady-state photochemical <span class="hlt">model</span> that uses currently recommended reaction rates and photolysis cross sections underestimate <span class="hlt">observed</span> profiles of HOCl obtained by two balloon-borne instruments, FIRS-2 (a far-infrared emission spectrometer) and MkIV (a mid-infrared, solar absorption spectrometer). Considerable uncertainty (a factor of two) persists in laboratory <span class="hlt">measurements</span> of the rate constant (k(sub 1)) for the reaction ClO + HO2 yields HOCl + O2. Agreement between <span class="hlt">modeled</span> and <span class="hlt">measured</span> HOCl can be attained using a value of k(sub 1) from Stimpfle et al. (1979) that is about a factor-of-two faster than the currently recommended rate constant. Comparison of <span class="hlt">modeled</span> and <span class="hlt">measured</span> HOCl suggests that <span class="hlt">models</span> using the currently recommended value for k(sub 1) may underestimate the role of the HOCl catalytic cycle for ozone depletion, important in the midlatitude lower stratosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910418A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910418A"><span>Evaluation of cloud-resolving <span class="hlt">modeling</span> of haboobs using in-situ and remotely sensed <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anisimov, Anatolii; Axisa, Duncan; Mostamandi, Suleiman; Kucera, Paul A.; Stenchikov, Georgiy</p> <p>2017-04-01</p> <p>Arabian Peninsula is one of the major dust generation regions that at present is severely under-sampled. In this study, we combine unique aircraft <span class="hlt">observations</span> of aerosol and fine-resolution simulations to better quantify dust generation and transport in deep convective storms called haboobs. The aerosol <span class="hlt">observations</span> were obtained during the "Kingdom of Saudi Arabia Assessment of Rainfall Augmentation" research program that was conducted in the Central and Southwest regions of Saudi Arabia for the years of 2006 through 2009. We ingest the <span class="hlt">observations</span> from the first phase of the project conducted in the central Arabian Peninsula near Riyadh in April 2007 and focus on the <span class="hlt">observational</span> cases when the aircraft sampled high concentrations of dust within haboobs. These data are indispensable for assessment of dust properties during periods of extreme aerosol loading. We perform cloud-resolving 2-km simulations using the coupled meteorology-chemistry WRF-Chem <span class="hlt">model</span> with 8-bin MOSAIC aerosol microphysics scheme that accounts for direct and indirect aerosol effects. The <span class="hlt">model</span> is validated using <span class="hlt">observations</span> from surface weather stations, Doppler weather radar network, AERONET stations, MODIS and SEVIRI satellite aerosol sensors. We also compare the <span class="hlt">model</span> results with recent MERRA-2 reanalysis that assimilates aerosols and chemical components. The <span class="hlt">model</span> captures the spatiotemporal variability of atmospheric circulation and aerosol properties and calculates contributions of different aerosol species. We specifically compare the simulated aerosols with the aircraft <span class="hlt">measurements</span> to evaluate the vertical extent and the structure of dust layers in haboobs. The simulated column-averaged dust size distribution compares reasonably well with AERONET and aircraft <span class="hlt">measurement</span>. Despite total aerosol optical depth in simulations and MERRA2 reanalysis are quite similar, the vertical distribution and regional dust emission fluxes in the <span class="hlt">model</span> and reanalysis differ significantly. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002SPIE.4865..190R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002SPIE.4865..190R"><span>Large-scale <span class="hlt">measurement</span> and <span class="hlt">modeling</span> of backbone Internet traffic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roughan, Matthew; Gottlieb, Joel</p> <p>2002-07-01</p> <p>There is a brewing controversy in the traffic <span class="hlt">modeling</span> community concerning how to <span class="hlt">model</span> backbone traffic. The fundamental work on self-similarity in data traffic appears to be contradicted by recent findings that suggest that backbone traffic is smooth. The traffic analysis work to date has focused on high-quality but limited-scope packet trace <span class="hlt">measurements</span>; this limits its applicability to high-speed backbone traffic. This paper uses more than one year's worth of SNMP traffic data covering an entire Tier 1 ISP backbone to address the question of how backbone network traffic should be <span class="hlt">modeled</span>. Although the limitations of SNMP <span class="hlt">measurements</span> do not permit us to comment on the fine timescale behavior of the traffic, careful analysis of the data suggests that irrespective of the variation at fine timescales, we can construct a simple traffic <span class="hlt">model</span> that captures key features of the <span class="hlt">observed</span> traffic. Furthermore, the <span class="hlt">model</span>'s parameters are <span class="hlt">measurable</span> using existing network infrastructure, making this <span class="hlt">model</span> practical in a present-day operational network. In addition to its practicality, the <span class="hlt">model</span> verifies basic statistical multiplexing results, and thus sheds deep insight into how smooth backbone traffic really is.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A13Q..08C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A13Q..08C"><span>Using aircraft and satellite <span class="hlt">observations</span> to improve regulatory air quality <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Canty, T. P.; Vinciguerra, T.; Anderson, D. C.; Carpenter, S. F.; Goldberg, D. L.; Hembeck, L.; Montgomery, L.; Liu, X.; Salawitch, R. J.; Dickerson, R. R.</p> <p>2014-12-01</p> <p>Federal and state agencies rely on EPA approved <span class="hlt">models</span> to develop attainment strategies that will bring states into compliance with the National Ambient Air Quality Standards (NAAQS). We will describe modifications to the Community Multi-Scale Air Quality (CMAQ) <span class="hlt">model</span> and Comprehensive Air Quality <span class="hlt">Model</span> with Extensions (CAMx) frameworks motivated by analysis of NASA satellite and aircraft <span class="hlt">measurements</span>. <span class="hlt">Observations</span> of tropospheric column NO2 from OMI have already led to the identification of an important deficiency in the chemical mechanisms used by <span class="hlt">models</span>; data collected during the DISCOVER-AQ field campaign has been instrumental in devising an improved representation of the chemistry of nitrogen species. Our recent work has focused on the use of: OMI <span class="hlt">observations</span> of tropospheric O3 to assess and improve the representation of boundary conditions used by AQ <span class="hlt">models</span>, OMI NO2 to derive a top down NOx emission inventory from commercial shipping vessels that affect air quality in the Eastern U.S., and OMI HCHO to assess the C5H8 emission inventories provided by bioegenic emissions <span class="hlt">models</span>. We will describe how these OMI-driven <span class="hlt">model</span> improvements are being incorporated into the State Implementation Plans (SIPs) being prepared for submission to EPA in summer 2015 and how future <span class="hlt">modeling</span> efforts may be impacted by our findings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NJPh...19f3032X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NJPh...19f3032X"><span>Optimal joint <span class="hlt">measurements</span> of complementary <span class="hlt">observables</span> by a single trapped ion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xiong, T. P.; Yan, L. L.; Ma, Z. H.; Zhou, F.; Chen, L.; Yang, W. L.; Feng, M.; Busch, P.</p> <p>2017-06-01</p> <p>The uncertainty relations, pioneered by Werner Heisenberg nearly 90 years ago, set a fundamental limitation on the joint <span class="hlt">measurability</span> of complementary <span class="hlt">observables</span>. This limitation has long been a subject of debate, which has been reignited recently due to new proposed forms of <span class="hlt">measurement</span> uncertainty relations. The present work is associated with a new error trade-off relation for compatible <span class="hlt">observables</span> approximating two incompatible <span class="hlt">observables</span>, in keeping with the spirit of Heisenberg’s original ideas of 1927. We report the first direct test and confirmation of the tight bounds prescribed by such an error trade-off relation, based on an experimental realisation of optimal joint <span class="hlt">measurements</span> of complementary <span class="hlt">observables</span> using a single ultracold {}40{{{Ca}}}+ ion trapped in a harmonic potential. Our work provides a prototypical determination of ultimate joint <span class="hlt">measurement</span> error bounds with potential applications in quantum information science for high-precision <span class="hlt">measurement</span> and information security.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26438283','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26438283"><span>Weighting climate <span class="hlt">model</span> projections using <span class="hlt">observational</span> constraints.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gillett, Nathan P</p> <p>2015-11-13</p> <p>Projected climate change integrates the net response to multiple climate feedbacks. Whereas existing long-term climate change projections are typically based on unweighted individual climate <span class="hlt">model</span> simulations, as <span class="hlt">observed</span> climate change intensifies it is increasingly becoming possible to constrain the net response to feedbacks and hence projected warming directly from <span class="hlt">observed</span> climate change. One approach scales simulated future warming based on a fit to <span class="hlt">observations</span> over the historical period, but this approach is only accurate for near-term projections and for scenarios of continuously increasing radiative forcing. For this reason, the recent Fifth Assessment Report of the Intergovernmental Panel on Climate Change (IPCC AR5) included such <span class="hlt">observationally</span> constrained projections in its assessment of warming to 2035, but used raw <span class="hlt">model</span> projections of longer term warming to 2100. Here a simple approach to weighting <span class="hlt">model</span> projections based on an <span class="hlt">observational</span> constraint is proposed which does not assume a linear relationship between past and future changes. This approach is used to weight <span class="hlt">model</span> projections of warming in 2081-2100 relative to 1986-2005 under the Representative Concentration Pathway 4.5 forcing scenario, based on an <span class="hlt">observationally</span> constrained estimate of the Transient Climate Response derived from a detection and attribution analysis. The resulting <span class="hlt">observationally</span> constrained 5-95% warming range of 0.8-2.5 K is somewhat lower than the unweighted range of 1.1-2.6 K reported in the IPCC AR5. © 2015 The Authors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS11A1249M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS11A1249M"><span><span class="hlt">Modeled</span> and <span class="hlt">Observed</span> Transitions Between Rip Currents and Alongshore Flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moulton, M.; Elgar, S.; Warner, J. C.; Raubenheimer, B.</p> <p>2014-12-01</p> <p>Predictions of rip currents, alongshore currents, and the temporal transitions between these circulation patterns are important for swimmer safety and for estimating the transport of sediments, biota, and pollutants in the nearshore. Here, field <span class="hlt">observations</span> are combined with hydrodynamic <span class="hlt">modeling</span> to determine the dominant processes that lead rip currents to turn on and off with changing waves, bathymetry, and tidal elevation. Waves, currents, mean sea levels, and bathymetry were <span class="hlt">measured</span> near and within five shore-perpendicular channels (on average 2-m deep, 30-m wide) that were dredged with the propellers of a landing craft at different times on a long straight Atlantic Ocean beach near Duck, NC in summer 2012. The circulation was <span class="hlt">measured</span> for a range of incident wave conditions and channel sizes, and included rapid transitions between strong (0.5 to 1 m/s) rip current jets flowing offshore through the channels and alongshore currents flowing across the channels with no rip currents. Meandering alongshore currents (alongshore currents combined with an offshore jet at the downstream edge of the channel) also were <span class="hlt">observed</span>. Circulation patterns near and within idealized rip channels simulated with COAWST (a three-dimensional phase-averaged <span class="hlt">model</span> that couples ROMS and SWAN) are compared with the <span class="hlt">observations</span>. In addition, the <span class="hlt">model</span> is used to investigate the hydrodynamic response to a range of wave conditions (angle, height, period) and bathymetries (channel width, depth, and length; tidal elevations; shape of sandbar or terrace). Rip current speeds are largest for the deepest perturbations, and decrease as incident wave angles become more oblique. For obliquely incident waves, the rip currents are shifted in the direction of the alongshore flow, with an increasing shift for increasing alongshore current speed or increasing bathymetric perturbation depth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AIPC..975.1132M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AIPC..975.1132M"><span><span class="hlt">Measurement</span> and <span class="hlt">Modeling</span> of Ultrasonic Pitch/catch Grain Noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Margetan, F. J.; Gray, T. A.; Thompson, R. B.</p> <p>2008-02-01</p> <p>Ultrasonic grain noise arises from the scattering of sound waves by microstructural boundaries, and can limit the detection of weakly-reflecting internal defects in metals. In some cases of practical interest, such as focused-transducer inspections of aircraft engine components, so-called "single scattering" or "independent scatterer" <span class="hlt">models</span> have proven to be reasonably accurate in predicting grain noise characteristics. In pulse/echo inspections it is difficult to experimentally assess the relative contributions of single scattering and multiple scattering, because both can generally contribute to the backscattered noise seen at any given <span class="hlt">observation</span> time. For pitch/catch inspections, however, it is relatively easy to construct inspection geometries for which single-scattered noise should be insignificant, and hence any <span class="hlt">observed</span> noise is presumably due to multiple scattering. This concept is demonstrated using pitch/catch shear-wave <span class="hlt">measurements</span> performed on a well-characterized stainless-steel specimen. The inspection geometry allows us to control the overlap volume of the intersecting radiation fields of the two transducers. As we proceed from maximally overlapping fields to zero overlap, the single-scattering contribution to the <span class="hlt">observed</span> grain noise is expected to decrease. <span class="hlt">Measurements</span> are compared to the predictions of a single-scatterer <span class="hlt">model</span>, and the relative contributions of single and multiple scattering to the <span class="hlt">observed</span> grain noise are estimated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NuPhB.929..485C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NuPhB.929..485C"><span>Fragmentation uncertainties in hadronic <span class="hlt">observables</span> for top-quark mass <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Corcella, Gennaro; Franceschini, Roberto; Kim, Doojin</p> <p>2018-04-01</p> <p>We study the Monte Carlo uncertainties due to <span class="hlt">modeling</span> of hadronization and showering in the extraction of the top-quark mass from <span class="hlt">observables</span> that use exclusive hadronic final states in top decays, such as t →anything + J / ψ or t →anything + (B →charged tracks), where B is a B-hadron. To this end, we investigate the sensitivity of the top-quark mass, determined by means of a few <span class="hlt">observables</span> already proposed in the literature as well as some new proposals, to the relevant parameters of event generators, such as HERWIG 6 and PYTHIA 8. We find that constraining those parameters at O (1%- 10%) is required to avoid a Monte Carlo uncertainty on mt greater than 500 MeV. For the sake of achieving the needed accuracy on such parameters, we examine the sensitivity of the top-quark mass <span class="hlt">measured</span> from spectral features, such as peaks, endpoints and distributions of EB, mBℓ, and some mT2-like variables. We find that restricting oneself to regions sufficiently close to the endpoints enables one to substantially decrease the dependence on the Monte Carlo parameters, but at the price of inflating significantly the statistical uncertainties. To ameliorate this situation we study how well the data on top-quark production and decay at the LHC can be utilized to constrain the showering and hadronization variables. We find that a global exploration of several calibration <span class="hlt">observables</span>, sensitive to the Monte Carlo parameters but very mildly to mt, can offer useful constraints on the parameters, as long as such quantities are <span class="hlt">measured</span> with a 1% precision.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A53M..06N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A53M..06N"><span><span class="hlt">Modeling</span> Atmospheric Transport for Greenhouse Gas <span class="hlt">Observations</span> within the Urban Dome</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nehrkorn, T.; Sargent, M. R.; Wofsy, S. C.</p> <p>2016-12-01</p> <p><span class="hlt">Observations</span> of CO2, CH4, and other greenhouse gases (GHGs) within the urban dome of major cities generally show large enhancements over background values, and large sensitivity to surface fluxes (as <span class="hlt">measured</span> by the footprints computed by Lagrangian Particle Dispersion <span class="hlt">Models</span>, LPDMs) within the urban dome. However, their use in top-down inversion studies to constrain urban emission estimates is complicated by difficulties in proper <span class="hlt">modeling</span> of the atmospheric transport. We are conducting experiments with the Weather Research and Forecast <span class="hlt">model</span> (WRF) coupled to the STILT LPDM to improve <span class="hlt">model</span> simulation of atmospheric transport on spatial scales of a few km in urban domains, because errors in transport on short time/space scales are amplified by the patchiness of GHG emissions and may engender systematic errors of simulated concentrations.We are evaluating the quality of the meteorological simulations from <span class="hlt">model</span> configurations with different resolutions and PBL packages, using both standard and non-standard (Lidar PBL height and ACARS aircraft profile) <span class="hlt">observations</span>. To take into account the effect of building scale eddies for <span class="hlt">observations</span> located on top of buildings, we are modifying the basic STILT algorithm for the computation of footprints by replacing the nominal receptor height by an effective sampling height. In addition, the footprint computations for near-field emissions make use of the vertical particle spread within the LPDM to arrive at a more appropriate estimate of mixing heights in the immediate vicinity of receptors. We present the effect of these and similar modifications on simulated concentrations and their level of agreement with <span class="hlt">observed</span> values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4638124','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4638124"><span>Multiple imputation to account for <span class="hlt">measurement</span> error in marginal structural <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Edwards, Jessie K.; Cole, Stephen R.; Westreich, Daniel; Crane, Heidi; Eron, Joseph J.; Mathews, W. Christopher; Moore, Richard; Boswell, Stephen L.; Lesko, Catherine R.; Mugavero, Michael J.</p> <p>2015-01-01</p> <p>Background Marginal structural <span class="hlt">models</span> are an important tool for <span class="hlt">observational</span> studies. These <span class="hlt">models</span> typically assume that variables are <span class="hlt">measured</span> without error. We describe a method to account for differential and non-differential <span class="hlt">measurement</span> error in a marginal structural <span class="hlt">model</span>. Methods We illustrate the method estimating the joint effects of antiretroviral therapy initiation and current smoking on all-cause mortality in a United States cohort of 12,290 patients with HIV followed for up to 5 years between 1998 and 2011. Smoking status was likely <span class="hlt">measured</span> with error, but a subset of 3686 patients who reported smoking status on separate questionnaires composed an internal validation subgroup. We compared a standard joint marginal structural <span class="hlt">model</span> fit using inverse probability weights to a <span class="hlt">model</span> that also accounted for misclassification of smoking status using multiple imputation. Results In the standard analysis, current smoking was not associated with increased risk of mortality. After accounting for misclassification, current smoking without therapy was associated with increased mortality [hazard ratio (HR): 1.2 (95% CI: 0.6, 2.3)]. The HR for current smoking and therapy (0.4 (95% CI: 0.2, 0.7)) was similar to the HR for no smoking and therapy (0.4; 95% CI: 0.2, 0.6). Conclusions Multiple imputation can be used to account for <span class="hlt">measurement</span> error in concert with methods for causal inference to strengthen results from <span class="hlt">observational</span> studies. PMID:26214338</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JHyd..408..178E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JHyd..408..178E"><span>Hydrograph matching method for <span class="hlt">measuring</span> <span class="hlt">model</span> performance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ewen, John</p> <p>2011-09-01</p> <p>SummaryDespite all the progress made over the years on developing automatic methods for analysing hydrographs and <span class="hlt">measuring</span> the performance of rainfall-runoff <span class="hlt">models</span>, automatic methods cannot yet match the power and flexibility of the human eye and brain. Very simple approaches are therefore being developed that mimic the way hydrologists inspect and interpret hydrographs, including the way that patterns are recognised, links are made by eye, and hydrological responses and errors are studied and remembered. In this paper, a dynamic programming algorithm originally designed for use in data mining is customised for use with hydrographs. It generates sets of "rays" that are analogous to the visual links made by the hydrologist's eye when linking features or times in one hydrograph to the corresponding features or times in another hydrograph. One outcome from this work is a new family of performance <span class="hlt">measures</span> called "visual" performance <span class="hlt">measures</span>. These can <span class="hlt">measure</span> differences in amplitude and timing, including the timing errors between simulated and <span class="hlt">observed</span> hydrographs in <span class="hlt">model</span> calibration. To demonstrate this, two visual performance <span class="hlt">measures</span>, one based on the Nash-Sutcliffe Efficiency and the other on the mean absolute error, are used in a total of 34 split-sample calibration-validation tests for two rainfall-runoff <span class="hlt">models</span> applied to the Hodder catchment, northwest England. The customised algorithm, called the Hydrograph Matching Algorithm, is very simple to apply; it is given in a few lines of pseudocode.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1367153-power-system-observability-dynamic-state-estimation-stability-monitoring-using-synchrophasor-measurements','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1367153-power-system-observability-dynamic-state-estimation-stability-monitoring-using-synchrophasor-measurements"><span>Power system <span class="hlt">observability</span> and dynamic state estimation for stability monitoring using synchrophasor <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sun, Kai; Qi, Junjian; Kang, Wei</p> <p>2016-08-01</p> <p>Growing penetration of intermittent resources such as renewable generations increases the risk of instability in a power grid. This paper introduces the concept of <span class="hlt">observability</span> and its computational algorithms for a power grid monitored by the wide-area <span class="hlt">measurement</span> system (WAMS) based on synchrophasors, e.g. phasor <span class="hlt">measurement</span> units (PMUs). The goal is to estimate real-time states of generators, especially for potentially unstable trajectories, the information that is critical for the detection of rotor angle instability of the grid. The paper studies the number and siting of synchrophasors in a power grid so that the state of the system can be accuratelymore » estimated in the presence of instability. An unscented Kalman filter (UKF) is adopted as a tool to estimate the dynamic states that are not directly <span class="hlt">measured</span> by synchrophasors. The theory and its computational algorithms are illustrated in detail by using a 9-bus 3-generator power system <span class="hlt">model</span> and then tested on a 140-bus 48-generator Northeast Power Coordinating Council power grid <span class="hlt">model</span>. Case studies on those two systems demonstrate the performance of the proposed approach using a limited number of synchrophasors for dynamic state estimation for stability assessment and its robustness against moderate inaccuracies in <span class="hlt">model</span> parameters.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70037277','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70037277"><span>Seasonal-scale nearshore morphological evolution: Field <span class="hlt">observations</span> and numerical <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Ruggiero, P.; Walstra, D.-J.R.; Gelfenbaum, G.; van, Ormondt M.</p> <p>2009-01-01</p> <p>A coupled waves-currents-bathymetric evolution <span class="hlt">model</span> (DELFT-3D) is compared with field <span class="hlt">measurements</span> to test hypotheses regarding the processes responsible for alongshore varying nearshore morphological changes at seasonal time scales. A 2001 field experiment, along the beaches adjacent to Grays Harbor, Washington, USA, captured the transition between the high-energy erosive conditions of winter and the low-energy beach-building conditions typical of summer. The experiment documented shoreline progradation on the order of 10-20 m and on average approximately 70 m of onshore sandbar migration during a four-month period. Significant alongshore variability was <span class="hlt">observed</span> in the morphological response of the sandbar over a 4 km reach of coast with sandbar movement ranging from 20 m of offshore migration to over 175 m of onshore bar migration, the largest seasonal-scale onshore migration event <span class="hlt">observed</span> in a natural setting. Both <span class="hlt">observations</span> and <span class="hlt">model</span> results suggest that, in the case investigated here, alongshore variations in initial bathymetry are primarily responsible for the <span class="hlt">observed</span> alongshore variable morphological changes. Alongshore varying incident hydrodynamic forcing, occasionally significant in this region due to a tidal inlet and associated ebb-tidal delta, was relatively minor during the study period and appears to play an insignificant role in the <span class="hlt">observed</span> alongshore variability in sandbar behavior at kilometer-scale. The role of fully three-dimensional cell circulation patterns in explaining the <span class="hlt">observed</span> morphological variability also appears to be minor, at least in the case investigated here. ?? 2009 Elsevier B.V.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010021174&hterms=energy+regions+Remote&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Denergy%2Bregions%2BRemote','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010021174&hterms=energy+regions+Remote&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Denergy%2Bregions%2BRemote"><span>Interannual Variability of the Tropical Energy Balance: Reconciling <span class="hlt">Observations</span> and <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Robertson, Franklin R.; Fitzjarrald, D. E.; Goodman, H. Michael (Technical Monitor)</p> <p>2000-01-01</p> <p>Since the beginning of the World Climate Research Program's Global Precipitation Climatology Project (GPCP) satellite remote sensing of precipitation has made dramatic improvements, particularly for tropical regions. Data from microwave and infrared sensors now form the most critical input to precipitation data sets and can be calibrated with surface gauges to so that the strengths of each data source can be maximized in some statistically optimal sense. Recent availability of the TRMM (Tropical Rainfall <span class="hlt">Measuring</span> Mission) has further aided in narrowing uncertainties in rainfall over the tropics and subtropics. Although climate <span class="hlt">modeling</span> efforts have long relied on space-based precipitation estimates for validation, we now are in a position to make more quantitative assessments of <span class="hlt">model</span> performance, particularly in tropical regions. An integration of the CCM3 using <span class="hlt">observed</span> SSTs as a lower boundary condition is used to examine how well this <span class="hlt">model</span> responds to ENSO forcing in terms of anomalous precipitation. An integration of the NCEP spectral <span class="hlt">model</span> used for the Reanalysis-11 effort is also examined. This integration is run with specified SSTs, but no data assimilation. Our analysis focuses on two aspects. First are the spatial anomalies that are indicative of dislocations in Hadley and Walker circulations. Second, we consider the ability of <span class="hlt">models</span> to replicate <span class="hlt">observed</span> increases in oceanic precipitation that are noted in satellite <span class="hlt">observations</span> for large ENSO events. Finally, we consider a slab ocean version of the CCM3 <span class="hlt">model</span> with prescribed ocean heat transports that mimic upwelling anomalies, but which still allows the surface energy balance to be predicted. This less restrictive experiment is used to understand why <span class="hlt">model</span> experiments with specified SSTs seem to have noticeably less interannual variability than do the satellite precipitation <span class="hlt">observations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820052253&hterms=oso&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Doso','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820052253&hterms=oso&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Doso"><span>A <span class="hlt">model</span> of a sunspot chromosphere based on OSO 8 <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lites, B. W.; Skumanich, A.</p> <p>1982-01-01</p> <p>OSO 8 spectrometer <span class="hlt">observations</span> of the H I, Mg II, and Ca II resonance lines of a large quiet sunspot during November 16-17, 1975, along with a C IV line of that event obtained by a ground-based spectrometer, are analyzed together with near-simultaneous ground-based Stokes <span class="hlt">measurements</span> to yield an umbral chromosphere and transition region <span class="hlt">model</span>. Features of this <span class="hlt">model</span> include a chromosphere that is effectively thin in the resonance lines of H I and Mg II, while being saturated in Ca II, and an upper chromospheric structure similar to that of quiet-sun <span class="hlt">models</span>. The similarity of the upper chromosphere of the sunspot umbra to the quiet-sun chromosphere suggests that the intense magnetic field plays only a passive role in the chromospheric heating mechanism, and the <span class="hlt">observations</span> cited indicate that solar-type stars with large areas of ordered magnetic flux would not necessarily exhibit extremely active chromosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150008256&hterms=kumar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D50%26Ntt%3Dkumar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150008256&hterms=kumar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D50%26Ntt%3Dkumar"><span>Land Surface Microwave Emissivity Dynamics: <span class="hlt">Observations</span>, Analysis and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tian, Yudong; Peters-Lidard, Christa D.; Harrison, Kenneth W.; Kumar, Sujay; Ringerud, Sarah</p> <p>2014-01-01</p> <p>Land surface microwave emissivity affects remote sensing of both the atmosphere and the land surface. The dynamical behavior of microwave emissivity over a very diverse sample of land surface types is studied. With seven years of satellite <span class="hlt">measurements</span> from AMSR-E, we identified various dynamical regimes of the land surface emission. In addition, we used two radiative transfer <span class="hlt">models</span> (RTMs), the Community Radiative Transfer <span class="hlt">Model</span> (CRTM) and the Community Microwave Emission <span class="hlt">Modeling</span> Platform (CMEM), to simulate land surface emissivity dynamics. With both CRTM and CMEM coupled to NASA's Land Information System, global-scale land surface microwave emissivities were simulated for five years, and evaluated against AMSR-E <span class="hlt">observations</span>. It is found that both <span class="hlt">models</span> have successes and failures over various types of land surfaces. Among them, the desert shows the most consistent underestimates (by approx. 70-80%), due to limitations of the physical <span class="hlt">models</span> used, and requires a revision in both systems. Other snow-free surface types exhibit various degrees of success and it is expected that parameter tuning can improve their performances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013012','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013012"><span>Inferring Soil Moisture Memory from Streamflow <span class="hlt">Observations</span> Using a Simple Water Balance <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Orth, Rene; Koster, Randal Dean; Seneviratne, Sonia I.</p> <p>2013-01-01</p> <p>Soil moisture is known for its integrative behavior and resulting memory characteristics. Soil moisture anomalies can persist for weeks or even months into the future, making initial soil moisture a potentially important contributor to skill in weather forecasting. A major difficulty when investigating soil moisture and its memory using <span class="hlt">observations</span> is the sparse availability of long-term <span class="hlt">measurements</span> and their limited spatial representativeness. In contrast, there is an abundance of long-term streamflow <span class="hlt">measurements</span> for catchments of various sizes across the world. We investigate in this study whether such streamflow <span class="hlt">measurements</span> can be used to infer and characterize soil moisture memory in respective catchments. Our approach uses a simple water balance <span class="hlt">model</span> in which evapotranspiration and runoff ratios are expressed as simple functions of soil moisture; optimized functions for the <span class="hlt">model</span> are determined using streamflow <span class="hlt">observations</span>, and the optimized <span class="hlt">model</span> in turn provides information on soil moisture memory on the catchment scale. The validity of the approach is demonstrated with data from three heavily monitored catchments. The approach is then applied to streamflow data in several small catchments across Switzerland to obtain a spatially distributed description of soil moisture memory and to show how memory varies, for example, with altitude and topography.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120015715','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120015715"><span>Space-based <span class="hlt">Observational</span> Constraints for 1-D Plume Rise <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Martin, Maria Val; Kahn, Ralph A.; Logan, Jennifer A.; Paguam, Ronan; Wooster, Martin; Ichoku, Charles</p> <p>2012-01-01</p> <p>We use a space-based plume height climatology derived from <span class="hlt">observations</span> made by the Multi-angle Imaging SpectroRadiometer (MISR) instrument aboard the NASA Terra satellite to evaluate the ability of a plume-rise <span class="hlt">model</span> currently embedded in several atmospheric chemical transport <span class="hlt">models</span> (CTMs) to produce accurate smoke injection heights. We initialize the plume-rise <span class="hlt">model</span> with assimilated meteorological fields from the NASA Goddard Earth <span class="hlt">Observing</span> System and estimated fuel moisture content at the location and time of the MISR <span class="hlt">measurements</span>. Fire properties that drive the plume-rise <span class="hlt">model</span> are difficult to estimate and we test the <span class="hlt">model</span> with four estimates for active fire area and four for total heat flux, obtained using empirical data and Moderate Resolution Imaging Spectroradiometer (MODIS) re radiative power (FRP) thermal anomalies available for each MISR plume. We show that the <span class="hlt">model</span> is not able to reproduce the plume heights <span class="hlt">observed</span> by MISR over the range of conditions studied (maximum r2 obtained in all configurations is 0.3). The <span class="hlt">model</span> also fails to determine which plumes are in the free troposphere (according to MISR), key information needed for atmospheric <span class="hlt">models</span> to simulate properly smoke dispersion. We conclude that embedding a plume-rise <span class="hlt">model</span> using currently available re constraints in large-scale atmospheric studies remains a difficult proposition. However, we demonstrate the degree to which the fire dynamical heat flux (related to active fire area and sensible heat flux), and atmospheric stability structure influence plume rise, although other factors less well constrained (e.g., entrainment) may also be significant. Using atmospheric stability conditions, MODIS FRP, and MISR plume heights, we offer some constraints on the main physical factors that drive smoke plume rise. We find that smoke plumes reaching high altitudes are characterized by higher FRP and weaker atmospheric stability conditions than those at low altitude, which tend to remain confined</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24669719','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24669719"><span>On <span class="hlt">modeling</span> animal movements using Brownian motion with <span class="hlt">measurement</span> error.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pozdnyakov, Vladimir; Meyer, Thomas; Wang, Yu-Bo; Yan, Jun</p> <p>2014-02-01</p> <p><span class="hlt">Modeling</span> animal movements with Brownian motion (or more generally by a Gaussian process) has a long tradition in ecological studies. The recent Brownian bridge movement <span class="hlt">model</span> (BBMM), which incorporates <span class="hlt">measurement</span> errors, has been quickly adopted by ecologists because of its simplicity and tractability. We discuss some nontrivial properties of the discrete-time stochastic process that results from <span class="hlt">observing</span> a Brownian motion with added normal noise at discrete times. In particular, we demonstrate that the <span class="hlt">observed</span> sequence of random variables is not Markov. Consequently the expected occupation time between two successively <span class="hlt">observed</span> locations does not depend on just those two <span class="hlt">observations</span>; the whole path must be taken into account. Nonetheless, the exact likelihood function of the <span class="hlt">observed</span> time series remains tractable; it requires only sparse matrix computations. The likelihood-based estimation procedure is described in detail and compared to the BBMM estimation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170006613','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170006613"><span>Answering the Call for <span class="hlt">Model</span>-Relevant <span class="hlt">Observations</span> of Aerosols and Clouds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Redemann, J.; Shinozuka, Y.; Kacenelenbogen, M.; Segal-Rozenhaimer, M.; LeBlanc, S.; Vaughan, M.; Stier, P.; Schutgens, N.</p> <p>2017-01-01</p> <p>We describe a technique for combining multiple A-Train aerosol data sets, namely MODIS spectral AOD (aerosol optical depth), OMI AAOD (absorption aerosol optical depth) and CALIOP aerosol backscatter retrievals (hereafter referred to as MOC retrievals) to estimate full spectral sets of aerosol radiative properties, and ultimately to calculate the 3-D distribution of direct aerosol radiative effects (DARE). We present MOC results using almost two years of data collected in 2007 and 2008, and show comparisons of the aerosol radiative property estimates to collocated AERONET retrievals. We compare the spatio-temporal distribution of the MOC retrievals and MOC-based calculations of seasonal clear-sky DARE to values derived from four <span class="hlt">models</span> that participated in the Phase II AeroCom <span class="hlt">model</span> intercomparison initiative. Comparisons of seasonal aerosol property to AeroCom Phase II results show generally good agreement best agreement with forcing results at TOA is found with GMI-MerraV3.We discuss the challenges in making <span class="hlt">observations</span> that really address deficiencies in <span class="hlt">models</span>, with some of the more relevant aspects being representativeness of the <span class="hlt">observations</span> for climatological states, and whether a given <span class="hlt">model-measurement</span> difference addresses a sampling or a <span class="hlt">model</span> error.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhRvD..84d3517J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhRvD..84d3517J"><span>Constraints from the CMB temperature and other common <span class="hlt">observational</span> data sets on variable dark energy density <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jetzer, Philippe; Tortora, Crescenzo</p> <p>2011-08-01</p> <p>The thermodynamic and dynamical properties of a variable dark energy <span class="hlt">model</span> with density scaling as ρx∝(1+z)m, z being the redshift, are discussed following the outline of Jetzer et al. [P. Jetzer, D. Puy, M. Signore, and C. Tortora, Gen. Relativ. Gravit. 43, 1083 (2011).GRGVA80001-770110.1007/s10714-010-1091-4]. These kinds of <span class="hlt">models</span> are proven to lead to the creation/disruption of matter and radiation, which affect the cosmic evolution of both matter and radiation components in the Universe. In particular, we have concentrated on the temperature-redshift relation of radiation, which has been constrained using a very recent collection of cosmic microwave background (CMB) temperature <span class="hlt">measurements</span> up to z˜3. For the first time, we have combined this <span class="hlt">observational</span> probe with a set of independent <span class="hlt">measurements</span> (Supernovae Ia distance moduli, CMB anisotropy, large-scale structure and <span class="hlt">observational</span> data for the Hubble parameter), which are commonly adopted to constrain dark energy <span class="hlt">models</span>. We find that, within the uncertainties, the <span class="hlt">model</span> is indistinguishable from a cosmological constant which does not exchange any particles with other components. Anyway, while temperature <span class="hlt">measurements</span> and Supernovae Ia tend to predict slightly decaying <span class="hlt">models</span>, the contrary happens if CMB data are included. Future <span class="hlt">observations</span>, in particular, <span class="hlt">measurements</span> of CMB temperature at large redshift, will allow to give firmer bounds on the effective equation of state parameter weff of this kind of dark energy <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A43H2579W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A43H2579W"><span>What is missing between <span class="hlt">model</span> and Aura MLS <span class="hlt">observations</span> in mesospheric OH?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, S.; Li, K. F.; Zeng, Z.; Sander, S. P.; Shia, R. L.; Yung, Y. L.</p> <p>2017-12-01</p> <p>Recent Aura Microwave Limb Souder <span class="hlt">observations</span> show higher mesospheric OH levels than earlier versions and previous satellite <span class="hlt">observations</span>. The current photochemical <span class="hlt">model</span> with standard chemistry is not able to accurately simulate MLS OH in the mesosphere. In particular, the <span class="hlt">model</span> significantly underestimates OH over the altitude range of 60-80km. In the standard middle atmospheric chemistry, HOx over this altitude range is controled mainly through the reactions of H2O + hv (< 205 nm) → H + OH; H + O2 + M → HO2 + M; and OH + HO2 → H2O + O2. In an attempt to resolve the <span class="hlt">model-observation</span> discrepancy, we adjust the rate coefficients of these reactions within recommended uncertainty ranges using an objective Bayesian approach. However, reasonable perturbations to these reactions are not capable of resolving the mesospheric discrepancy without introducing disagreements in other regions of the atmosphere. We explore possible new reactions in the Earth's atmosphere that are not included in current standard <span class="hlt">models</span>. Some candidate reactions and their potential impacts on mesospheric HOx chemistry will be discussed. Our results urge new laboratory studies of these candidate reactions, whose rate coefficients have never been <span class="hlt">measured</span> for the atmospheric conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.C31A0301K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.C31A0301K"><span>Local Scale Radiobrightness <span class="hlt">Modeling</span> During the Intensive <span class="hlt">Observing</span> Period-4 of the Cold Land Processes Experiment-1</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, E.; Tedesco, M.; de Roo, R.; England, A. W.; Gu, H.; Pham, H.; Boprie, D.; Graf, T.; Koike, T.; Armstrong, R.; Brodzik, M.; Hardy, J.; Cline, D.</p> <p>2004-12-01</p> <p>The NASA Cold Land Processes Field Experiment (CLPX-1) was designed to provide microwave remote sensing <span class="hlt">observations</span> and ground truth for studies of snow and frozen ground remote sensing, particularly issues related to scaling. CLPX-1 was conducted in 2002 and 2003 in Colorado, USA. One of the goals of the experiment was to test the capabilities of microwave emission <span class="hlt">models</span> at different scales. Initial forward <span class="hlt">model</span> validation work has concentrated on the Local-Scale <span class="hlt">Observation</span> Site (LSOS), a 0.8~ha study site consisting of open meadows separated by trees where the most detailed <span class="hlt">measurements</span> were made of snow depth and temperature, density, and grain size profiles. Results obtained in the case of the 3rd Intensive <span class="hlt">Observing</span> Period (IOP3) period (February, 2003, dry snow) suggest that a <span class="hlt">model</span> based on Dense Medium Radiative Transfer (DMRT) theory is able to <span class="hlt">model</span> the recorded brightness temperatures using snow parameters derived from field <span class="hlt">measurements</span>. This paper focuses on the ability of forward DMRT <span class="hlt">modelling</span>, combined with snowpack <span class="hlt">measurements</span>, to reproduce the radiobrightness signatures <span class="hlt">observed</span> by the University of Michigan's Truck-Mounted Radiometer System (TMRS) at 19 and 37~GHz during the 4th IOP (IOP4) in March, 2003. Unlike in IOP3, conditions during IOP4 include both wet and dry periods, providing a valuable test of DMRT <span class="hlt">model</span> performance. In addition, a comparison will be made for the one day of coincident <span class="hlt">observations</span> by the University of Tokyo's Ground-Based Microwave Radiometer-7 (GBMR-7) and the TMRS. The plot-scale study in this paper establishes a baseline of DMRT performance for later studies at successively larger scales. And these scaling studies will help guide the choice of future snow retrieval algorithms and the design of future Cold Lands <span class="hlt">observing</span> systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20100002945&hterms=temperature+variability&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtemperature%2Bvariability','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20100002945&hterms=temperature+variability&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtemperature%2Bvariability"><span>Soil Moisture Controls on Rainfall and Temperature Variability: A <span class="hlt">Modeler</span> Searches Through <span class="hlt">Observational</span> Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Koster, Randal</p> <p>2010-01-01</p> <p>The degree to which atmospheric processes respond to variations in soil moisture - a potentially important but largely untapped element of subseasonal to seasonal prediction - can be determined easily and directly for an atmospheric <span class="hlt">model</span> but cannot be determined directly for nature through an analysis of <span class="hlt">observations</span>. In atmospheric <span class="hlt">models</span>) directions of causality can be artificially manipulated; we can avoid difficulties associated with the fact that atmospheric variations have a much larger impact on land state variations than vice-versa. In nature) on the other hand) the dominant direction of causality (the atmosphere forcing the ground) cannot be artificially "turned off") and the statistics associated with this dominant direction overwhelm those of the feedback signal. <span class="hlt">Observational</span> data) however) do allow a number of indirect <span class="hlt">measures</span> of landatmosphere feedback. This seminar reports on a series of joint analyses of <span class="hlt">observational</span> and <span class="hlt">model</span> data designed to illuminate the degree of land-atmosphere feedback present in the real world. The indirect <span class="hlt">measures</span> do in fact suggest that feedback in nature, though small) is significant - enough to warrant the development of realistic land initialization strategies for subseasonal and seasonal forecasts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170005690','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170005690"><span>Interval Predictor <span class="hlt">Models</span> for Data with <span class="hlt">Measurement</span> Uncertainty</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lacerda, Marcio J.; Crespo, Luis G.</p> <p>2017-01-01</p> <p>An interval predictor <span class="hlt">model</span> (IPM) is a computational <span class="hlt">model</span> that predicts the range of an output variable given input-output data. This paper proposes strategies for constructing IPMs based on semidefinite programming and sum of squares (SOS). The <span class="hlt">models</span> are optimal in the sense that they yield an interval valued function of minimal spread containing all the <span class="hlt">observations</span>. Two different scenarios are considered. The first one is applicable to situations where the data is <span class="hlt">measured</span> precisely whereas the second one is applicable to data subject to known biases and <span class="hlt">measurement</span> error. In the latter case, the IPMs are designed to fully contain regions in the input-output space where the data is expected to fall. Moreover, we propose a strategy for reducing the computational cost associated with generating IPMs as well as means to simulate them. Numerical examples illustrate the usage and performance of the proposed formulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ACPD...14.5687T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ACPD...14.5687T"><span>Reconciling aerosol light extinction <span class="hlt">measurements</span> from spaceborne lidar <span class="hlt">observations</span> and in-situ <span class="hlt">measurements</span> in the Arctic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tesche, M.; Rastak, N.; Charlson, R. J.; Glantz, P.; Zieger, P.; Hansson, H.-C.</p> <p>2014-03-01</p> <p>In this study we investigate to what degree it is possible to reconcile continuously recorded particle light extinction coefficients derived from dry in-situ <span class="hlt">measurements</span> at Zeppelin station (78.92° N, 11.85° E, 475 m a.s.l.) at Ny-Ålesund, Svalbard, that are recalculated to ambient relative humidity, and simultaneous ambient <span class="hlt">observations</span> with the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) aboard the Cloud-Aerosol Lidar and Infrared Pathfinder Satellite <span class="hlt">Observations</span> (CALIPSO) satellite. To our knowledge, this represents the first study that compares spaceborne lidar <span class="hlt">measurements</span> to optical aerosol properties from short-term in-situ <span class="hlt">observations</span> (averaged over 5 h) on a case-by-case basis. Finding suitable comparison cases requires an elaborate screening and matching of the CALIOP data with respect to the location of the Zeppelin station as well as in the selection of temporal and spatial averaging intervals for both the ground-based and spaceborne <span class="hlt">observations</span>. Trustworthy reconciliation of these data cannot be achieved with the closest approach method that is often used in matching CALIOP <span class="hlt">observations</span> to those taken at ground sites due to the transport pathways of the air parcels that were sampled. The use of trajectories allowed us to establish a connection between spaceborne and ground-based <span class="hlt">observations</span> for 57 individual overpasses out of a total of 2018 that occurred in our region of interest around Svalbard (0 to 25° E; 75 to 82° N) in the considered year of 2008. Matches could only be established during winter and spring, since the low aerosol load during summer in connection with the strong solar background and the high occurrence rate of clouds strongly influences the performance and reliability of CALIOP <span class="hlt">observations</span>. Extinction coefficients in the range from 1 to 100 Mm-1 were found for successful matches with an agreement of a factor of 1.85 (median value for a range from 0.38 to 17.9) between the findings of in-situ and spaceborne</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.H51I1635L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.H51I1635L"><span>Evaluating Land-Atmosphere Moisture Feedbacks in Earth System <span class="hlt">Models</span> With Spaceborne <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levine, P. A.; Randerson, J. T.; Lawrence, D. M.; Swenson, S. C.</p> <p>2016-12-01</p> <p>We have developed a set of metrics for <span class="hlt">measuring</span> the feedback loop between the land surface moisture state and the atmosphere globally on an interannual time scale. These metrics consider both the forcing of terrestrial water storage (TWS) on subsequent atmospheric conditions as well as the response of TWS to antecedent atmospheric conditions. We designed our metrics to take advantage of more than one decade's worth of satellite <span class="hlt">observations</span> of TWS from the Gravity Recovery and Climate Experiment (GRACE) along with atmospheric variables from the Atmospheric Infrared Sounder (AIRS), the Global Precipitation Climatology Project (GPCP), and Clouds and the Earths Radiant Energy System (CERES). Metrics derived from spaceborne <span class="hlt">observations</span> were used to evaluate the strength of the feedback loop in the Community Earth System <span class="hlt">Model</span> (CESM) Large Ensemble (LENS) and in several <span class="hlt">models</span> that contributed simulations to Phase 5 of the Coupled <span class="hlt">Model</span> Intercomparison Project (CMIP5). We found that both forcing and response limbs of the feedback loop were generally stronger in tropical and temperate regions in CMIP5 <span class="hlt">models</span> and even more so in LENS compared to satellite <span class="hlt">observations</span>. Our analysis suggests that <span class="hlt">models</span> may overestimate the strength of the feedbacks between the land surface and the atmosphere, which is consistent with previous studies conducted across different spatial and temporal scales.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/928538','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/928538"><span>A comparison of water vapor quantities from <span class="hlt">model</span> short-range forecasts and ARM <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Hnilo, J J</p> <p>2006-03-17</p> <p><span class="hlt">Model</span> evolution and improvement is complicated by the lack of high quality <span class="hlt">observational</span> data. To address a major limitation of these <span class="hlt">measurements</span> the Atmospheric Radiation <span class="hlt">Measurement</span> (ARM) program was formed. For the second quarter ARM metric we will make use of new water vapor data that has become available, and called the 'Merged-sounding' value added product (referred to as OBS, within the text) at three sites: the North Slope of Alaska (NSA), Darwin Australia (DAR) and the Southern Great Plains (SGP) and compare these <span class="hlt">observations</span> to <span class="hlt">model</span> forecast data. Two time periods will be analyzed March 2000 for the SGPmore » and October 2004 for both DAR and NSA. The merged-sounding data have been interpolated to 37 pressure levels (e.g., from 1000hPa to 100hPa at 25hPa increments) and time averaged to 3 hourly data for direct comparison to our <span class="hlt">model</span> output.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ACP....15.1313V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ACP....15.1313V"><span>MAX-DOAS tropospheric nitrogen dioxide column <span class="hlt">measurements</span> compared with the Lotos-Euros air quality <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vlemmix, T.; Eskes, H. J.; Piters, A. J. M.; Schaap, M.; Sauter, F. J.; Kelder, H.; Levelt, P. F.</p> <p>2015-02-01</p> <p>A 14-month data set of MAX-DOAS (Multi-Axis Differential Optical Absorption Spectroscopy) tropospheric NO2 column <span class="hlt">observations</span> in De Bilt, the Netherlands, has been compared with the regional air quality <span class="hlt">model</span> Lotos-Euros. The <span class="hlt">model</span> was run on a 7×7 km2 grid, the same resolution as the emission inventory used. A study was performed to assess the effect of clouds on the retrieval accuracy of the MAX-DOAS <span class="hlt">observations</span>. Good agreement was found between <span class="hlt">modeled</span> and <span class="hlt">measured</span> tropospheric NO2 columns, with an average difference of less than 1% of the average tropospheric column (14.5 · 1015 molec cm-2). The comparisons show little cloud cover dependence after cloud corrections for which ceilometer data were used. Hourly differences between <span class="hlt">observations</span> and <span class="hlt">model</span> show a Gaussian behavior with a standard deviation (σ) of 5.5 · 1015 molec cm-2. For daily averages of tropospheric NO2 columns, a correlation of 0.72 was found for all <span class="hlt">observations</span>, and 0.79 for cloud free conditions. The <span class="hlt">measured</span> and <span class="hlt">modeled</span> tropospheric NO2 columns have an almost identical distribution over the wind direction. A significant difference between <span class="hlt">model</span> and <span class="hlt">measurements</span> was found for the average weekly cycle, which shows a much stronger decrease during the weekend for the <span class="hlt">observations</span>; for the diurnal cycle, the <span class="hlt">observed</span> range is about twice as large as the <span class="hlt">modeled</span> range. The results of the comparison demonstrate that averaged over a long time period, the tropospheric NO2 column <span class="hlt">observations</span> are representative for a large spatial area despite the fact that they were obtained in an urban region. This makes the MAX-DOAS technique especially suitable for validation of satellite <span class="hlt">observations</span> and air quality <span class="hlt">models</span> in urban regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004cosp...35.2031G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004cosp...35.2031G"><span>Spectrometeric <span class="hlt">measurements</span> of vertical profile and column abundance of NO2 at Zvenigorod, Russia: Fourteen years of <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gruzdev, A.; Elokhov, A.</p> <p></p> <p>Since 1990, NO2 <span class="hlt">measurements</span> are carried out at Zvenigorod Research Station (56°N, 37°E), Moscow region, with the help of zenith viewing spectrophotometer in spectral range 435-450 nm. The instrument and method of <span class="hlt">observations</span> were verified in comparison campaigns within the framework of the Network for Detection of Stratospheric Change. <span class="hlt">Measurements</span> are done during morning and evening twilight at solar zenith angles 84-96°. Slant column NO2 abundances are derived from <span class="hlt">observed</span> spectra taking into account O3 and NO2 absorption, single molecular and aerosol scattering, and the Ring effect. The NO2 abundances in the vertical column as well as vertical NO2 profiles are derived as solution of inverse mathematical problem (with Chahine method) using a spherical single scattering <span class="hlt">model</span> and a one-dimensional photochemical <span class="hlt">model</span>. Derived quantities are (1) NO2 abundances within 5-km thick layers in the stratosphere and troposphere, (2) NO2 abundance in the thin atmospheric near-surface layer and (3) columnar NO2 abundances in the troposphere (0-10 km) and the stratosphere (10-50 km) as integrals over appropriate layers. Results of <span class="hlt">measurements</span> show variability of stratospheric and tropospheric NO2 at different time scales from the diurnal to the interannual scale. Out of the period affected by the Pinatubo eruption (1992-1994), a general decline of the stratospheric column NO2 abundance is occurring, superimposed by interannual variations. A linear, statistically significant, negative annual trend of about 12% per decade has been detected for both morning and evening stratospheric column NO2 abundances. For interpretation of the <span class="hlt">observed</span> trend, a simple photochemical <span class="hlt">model</span> is used, which takes into account the <span class="hlt">observed</span> changes in N2O and stratospheric ozone abundances, and in temperature. The estimated <span class="hlt">model</span> trend of the stratospheric column NO2 abundance in the extratropical Northern Hemisphere is about -5% per decade, which is less than <span class="hlt">observed</span>. Dynamical variability</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23142894','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23142894"><span><span class="hlt">Modeling</span> and validation of photometric characteristics of space targets oriented to space-based <span class="hlt">observation</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Hongyuan; Zhang, Wei; Dong, Aotuo</p> <p>2012-11-10</p> <p>A <span class="hlt">modeling</span> and validation method of photometric characteristics of the space target was presented in order to track and identify different satellites effectively. The background radiation characteristics <span class="hlt">models</span> of the target were built based on blackbody radiation theory. The geometry characteristics of the target were illustrated by the surface equations based on its body coordinate system. The material characteristics of the target surface were described by a bidirectional reflectance distribution function <span class="hlt">model</span>, which considers the character of surface Gauss statistics and microscale self-shadow and is obtained by <span class="hlt">measurement</span> and <span class="hlt">modeling</span> in advance. The contributing surfaces of the target to <span class="hlt">observation</span> system were determined by coordinate transformation according to the relative position of the space-based target, the background radiation sources, and the <span class="hlt">observation</span> platform. Then a mathematical <span class="hlt">model</span> on photometric characteristics of the space target was built by summing reflection components of all the surfaces. Photometric characteristics simulation of the space-based target was achieved according to its given geometrical dimensions, physical parameters, and orbital parameters. Experimental validation was made based on the scale <span class="hlt">model</span> of the satellite. The calculated results fit well with the <span class="hlt">measured</span> results, which indicates the <span class="hlt">modeling</span> method of photometric characteristics of the space target is correct.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020081351','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020081351"><span>Chemistry-Transport <span class="hlt">Modeling</span> of the Satellite <span class="hlt">Observed</span> Distribution of Tropical Tropospheric Ozone</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peters, Wouter; Krol, Maarten; Dentener, Frank; Thompson, Anne M.; Leloeveld, Jos; Bhartia, P. K. (Technical Monitor)</p> <p>2002-01-01</p> <p>We have compared the 14-year record of satellite derived tropical tropospheric ozone columns (TTOC) from the NIMBUS-7 Total Ozone Mapping Spectrometer (TOMS) to TTOC calculated by a chemistry-transport <span class="hlt">model</span> (CTM). An objective <span class="hlt">measure</span> of error, based on the zonal distribution of TTOC in the tropics, is applied to perform this comparison systematically. In addition, the sensitivity of the <span class="hlt">model</span> to several key processes in the tropics is quantified to select directions for future improvements. The comparisons indicate a widespread, systematic (20%) discrepancy over the tropical Atlantic Ocean, which maximizes during austral Spring. Although independent evidence from ozonesondes shows that some of the disagreement is due to satellite over-estimate of TTOC, the Atlantic mismatch is largely due to a misrepresentation of seasonally recurring processes in the <span class="hlt">model</span>. Only minor differences between the <span class="hlt">model</span> and <span class="hlt">observations</span> over the Pacific occur, mostly due to interannual variability not captured by the <span class="hlt">model</span>. Although chemical processes determine the TTOC extent, dynamical processes dominate the TTOC distribution, as the use of actual meteorology pertaining to the year of <span class="hlt">observations</span> always leads to a better agreement with TTOC <span class="hlt">observations</span> than using a random year or a climatology. The <span class="hlt">modeled</span> TTOC is remarkably insensitive to many <span class="hlt">model</span> parameters due to efficient feedbacks in the ozone budget. Nevertheless, the simulations would profit from an improved biomass burning calendar, as well as from an increase in NOX abundances in free tropospheric biomass burning plumes. The <span class="hlt">model</span> showed the largest response to lightning NOX emissions, but systematic improvements could not be found. The use of multi-year satellite derived tropospheric data to systematically test and improve a CTM is a promising new addition to existing methods of <span class="hlt">model</span> validation, and is a first step to integrating tropospheric satellite <span class="hlt">observations</span> into global ozone <span class="hlt">modeling</span> studies. Conversely</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22572370-general-description-fission-observables-gef-model-code','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22572370-general-description-fission-observables-gef-model-code"><span>General Description of Fission <span class="hlt">Observables</span>: GEF <span class="hlt">Model</span> Code</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Schmidt, K.-H.; Jurado, B., E-mail: jurado@cenbg.in2p3.fr; Amouroux, C.</p> <p>2016-01-15</p> <p> that is consistent with the collective enhancement of the level density. The exchange of excitation energy and nucleons between the nascent fragments on the way from saddle to scission is estimated according to statistical mechanics. As a result, excitation energy and unpaired nucleons are predominantly transferred to the heavy fragment in the superfluid regime. This description reproduces some rather peculiar <span class="hlt">observed</span> features of the prompt-neutron multiplicities and of the even-odd effect in fission-fragment Z distributions. For completeness, some conventional descriptions are used for calculating pre-equilibrium emission, fission probabilities and statistical emission of neutrons and gamma radiation from the excited fragments. Preference is given to simple <span class="hlt">models</span> that can also be applied to exotic nuclei compared to more sophisticated <span class="hlt">models</span> that need precise empirical input of nuclear properties, e.g. spectroscopic information. The approach reveals a high degree of regularity and provides a considerable insight into the physics of the fission process. Fission <span class="hlt">observables</span> can be calculated with a precision that complies with the needs for applications in nuclear technology without specific adjustments to <span class="hlt">measured</span> data of individual systems. The GEF executable runs out of the box with no need for entering any empirical data. This unique feature is of valuable importance, because the number of systems and energies of potential significance for fundamental and applied science will never be possible to be <span class="hlt">measured</span>. The relevance of the approach for examining the consistency of experimental results and for evaluating nuclear data is demonstrated.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1214140J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1214140J"><span>SOA <span class="hlt">Measurements</span> vs. <span class="hlt">Models</span>: A Status Report</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jimenez, Jose-Luis; de Gouw, Joost; Hodzic, Alma</p> <p>2010-05-01</p> <p>The advent of fast and chemically-resolved organic aerosol (OA) and VOC <span class="hlt">measurements</span> in the last decade has allowed more detailed <span class="hlt">model-measurement</span> comparisons for OA and secondary OA (SOA). Large <span class="hlt">model</span> underpredictions have been reported for SOA at many locations, but this is not always the case. Here we summarize the patterns emerging from studies to date, focusing on studies that use highly time and/or chemically resolved OA <span class="hlt">measurements</span>. The <span class="hlt">model-measurement</span> comparisons exhibit clear patterns depending on the region of the atmosphere. • At least 8 studies have reported a large (x5-10) underestimation of SOA for polluted regions when using traditional <span class="hlt">models</span> (those developed until ~2006) (Heald GRL05, Volkamer GRL06, Johnson ACP06, Kleinman ACP08, Matsui JGR09, Dzepina ACP09, Hodzic ACP09, Tsimpidi ACP09). This is especially obvious when <span class="hlt">models</span> are evaluated with the ΔOA/ΔCO ratio. • Close to pollution sources, discrepancies of an order-of-magnitude in SOA lead to smaller discrepancies (often x2-3) for total OA due to the presence of primary OA (de Gouw EST09). Such OA discrepancies have been repeatedly <span class="hlt">observed</span> (e.g. Vutukuru JGR06, McKeen JGR07&09, Heald JGR07, Fast ACP09, Hodzic ACP09). • The discrepancy is reduced when recently-updated yields for aromatics (Ng ACP07) and SOA from glyoxal (Volkamer GRL07) are used, and is eliminated when using SOA formation from S/IVOC (Robinson Sci07) although with an overprediction of SOA at long aging times (Dzepina ACP09; Hodzic ACP10), especially with the Grieshop (ACP09) update of the Robison mechanism (Hodzic10). It is not clear whether the urban discrepancy is removed for the right reasons. • 4 evaluations of biogenic SOA formed in unpolluted regions find reasonable agreement between SOA from traditional <span class="hlt">models</span> and field <span class="hlt">measurements</span> (Tunved Sci06; Hodzic ACP09; Chen GRL09; Slowik ACPD09). One evaluation reports a significant underprediction (Capes ACP09), although the amount of precursor reacted was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050217203&hterms=model+atomic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dmodel%2Batomic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050217203&hterms=model+atomic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dmodel%2Batomic"><span>Martian Radiation Environment: <span class="hlt">Model</span> Calculations and Recent <span class="hlt">Measurements</span> with "MARIE"</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Saganti, P. B.; Cucinotta, F. A.; zeitlin, C. J.; Cleghorn, T. F.</p> <p>2004-01-01</p> <p>The Galactic Cosmic Ray spectra in Mars orbit were generated with the recently expanded HZETRN (High Z and Energy Transport) and QMSFRG (Quantum Multiple-Scattering theory of nuclear Fragmentation) <span class="hlt">model</span> calculations. These <span class="hlt">model</span> calculations are compared with the first eighteen months of <span class="hlt">measured</span> data from the MARIE (Martian Radiation Environment Experiment) instrument onboard the 2001 Mars Odyssey spacecraft that is currently in Martian orbit. The dose rates <span class="hlt">observed</span> by the MARIE instrument are within 10% of the <span class="hlt">model</span> calculated predictions. <span class="hlt">Model</span> calculations are compared with the MARIE <span class="hlt">measurements</span> of dose, dose-equivalent values, along with the available particle flux distribution. <span class="hlt">Model</span> calculated particle flux includes GCR elemental composition of atomic number, Z = 1-28 and mass number, A = 1-58. Particle flux calculations specific for the current MARIE mapping period are reviewed and presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1911236M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1911236M"><span>Drought Persistence in <span class="hlt">Models</span> and <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moon, Heewon; Gudmundsson, Lukas; Seneviratne, Sonia</p> <p>2017-04-01</p> <p>Many regions of the world have experienced drought events that persisted several years and caused substantial economic and ecological impacts in the 20th century. However, it remains unclear whether there are significant trends in the frequency or severity of these prolonged drought events. In particular, an important issue is linked to systematic biases in the representation of persistent drought events in climate <span class="hlt">models</span>, which impedes analysis related to the detection and attribution of drought trends. This study assesses drought persistence errors in global climate <span class="hlt">model</span> (GCM) simulations from the 5th phase of Coupled <span class="hlt">Model</span> Intercomparison Project (CMIP5), in the period of 1901-2010. The <span class="hlt">model</span> simulations are compared with five gridded <span class="hlt">observational</span> data products. The analysis focuses on two aspects: the identification of systematic biases in the <span class="hlt">models</span> and the partitioning of the spread of drought-persistence-error into four possible sources of uncertainty: <span class="hlt">model</span> uncertainty, <span class="hlt">observation</span> uncertainty, internal climate variability and the estimation error of drought persistence. We use monthly and yearly dry-to-dry transition probabilities as estimates for drought persistence with drought conditions defined as negative precipitation anomalies. For both time scales we find that most <span class="hlt">model</span> simulations consistently underestimated drought persistence except in a few regions such as India and Eastern South America. Partitioning the spread of the drought-persistence-error shows that at the monthly time scale <span class="hlt">model</span> uncertainty and <span class="hlt">observation</span> uncertainty are dominant, while the contribution from internal variability does play a minor role in most cases. At the yearly scale, the spread of the drought-persistence-error is dominated by the estimation error, indicating that the partitioning is not statistically significant, due to a limited number of considered time steps. These findings reveal systematic errors in the representation of drought persistence in current</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AtmRe.202..205S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AtmRe.202..205S"><span>Characterization of the Sahelian-Sudan rainfall based on <span class="hlt">observations</span> and regional climate <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salih, Abubakr A. M.; Elagib, Nadir Ahmed; Tjernström, Michael; Zhang, Qiong</p> <p>2018-04-01</p> <p>The African Sahel region is known to be highly vulnerable to climate variability and change. We analyze rainfall in the Sahelian Sudan in terms of distribution of rain-days and amounts, and examine whether regional climate <span class="hlt">models</span> can capture these rainfall features. Three regional <span class="hlt">models</span> namely, Regional <span class="hlt">Model</span> (REMO), Rossby Center Atmospheric <span class="hlt">Model</span> (RCA) and Regional Climate <span class="hlt">Model</span> (RegCM4), are evaluated against gridded <span class="hlt">observations</span> (Climate Research Unit, Tropical Rainfall <span class="hlt">Measuring</span> Mission, and ERA-interim reanalysis) and rain-gauge data from six arid and semi-arid weather stations across Sahelian Sudan over the period 1989 to 2008. Most of the <span class="hlt">observed</span> rain-days are characterized by weak (0.1-1.0 mm/day) to moderate (> 1.0-10.0 mm/day) rainfall, with average frequencies of 18.5% and 48.0% of the total annual rain-days, respectively. Although very strong rainfall events (> 30.0 mm/day) occur rarely, they account for a large fraction of the total annual rainfall (28-42% across the stations). The performance of the <span class="hlt">models</span> varies both spatially and temporally. RegCM4 most closely reproduces the <span class="hlt">observed</span> annual rainfall cycle, especially for the more arid locations, but all of the three <span class="hlt">models</span> fail to capture the strong rainfall events and hence underestimate its contribution to the total annual number of rain-days and rainfall amount. However, excessive moderate rainfall compensates this underestimation in the <span class="hlt">models</span> in an annual average sense. The present study uncovers some of the <span class="hlt">models</span>' limitations in skillfully reproducing the <span class="hlt">observed</span> climate over dry regions, will aid <span class="hlt">model</span> users in recognizing the uncertainties in the <span class="hlt">model</span> output and will help climate and hydrological <span class="hlt">modeling</span> communities in improving <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26317984','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26317984"><span>A Unimodal <span class="hlt">Model</span> for Double <span class="hlt">Observer</span> Distance Sampling Surveys.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Becker, Earl F; Christ, Aaron M</p> <p>2015-01-01</p> <p>Distance sampling is a widely used method to estimate animal population size. Most distance sampling <span class="hlt">models</span> utilize a monotonically decreasing detection function such as a half-normal. Recent advances in distance sampling <span class="hlt">modeling</span> allow for the incorporation of covariates into the distance <span class="hlt">model</span>, and the elimination of the assumption of perfect detection at some fixed distance (usually the transect line) with the use of double-<span class="hlt">observer</span> <span class="hlt">models</span>. The assumption of full <span class="hlt">observer</span> independence in the double-<span class="hlt">observer</span> <span class="hlt">model</span> is problematic, but can be addressed by using the point independence assumption which assumes there is one distance, the apex of the detection function, where the 2 <span class="hlt">observers</span> are assumed independent. Aerially collected distance sampling data can have a unimodal shape and have been successfully <span class="hlt">modeled</span> with a gamma detection function. Covariates in gamma detection <span class="hlt">models</span> cause the apex of detection to shift depending upon covariate levels, making this <span class="hlt">model</span> incompatible with the point independence assumption when using double-<span class="hlt">observer</span> data. This paper reports a unimodal detection <span class="hlt">model</span> based on a two-piece normal distribution that allows covariates, has only one apex, and is consistent with the point independence assumption when double-<span class="hlt">observer</span> data are utilized. An aerial line-transect survey of black bears in Alaska illustrate how this method can be applied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.A23D0207M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.A23D0207M"><span>Life Cycle of Tropical Convection and Anvil in <span class="hlt">Observations</span> and <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McFarlane, S. A.; Hagos, S. M.; Comstock, J. M.</p> <p>2011-12-01</p> <p>Tropical convective clouds are important elements of the hydrological cycle and produce extensive cirrus anvils that strongly affect the tropical radiative energy balance. To improve simulations of the global water and energy cycles and accurately predict both precipitation and cloud radiative feedbacks, <span class="hlt">models</span> need to realistically simulate the lifecycle of tropical convection, including the formation and radiative properties of ice anvil clouds. By combining remote sensing datasets from precipitation and cloud radars at the Atmospheric Radiation <span class="hlt">Measurement</span> (ARM) Darwin site with geostationary satellite data, we can develop <span class="hlt">observational</span> understanding of the lifetime of convective systems and the links between the properties of convective systems and their associated anvil clouds. The relationships between convection and anvil in <span class="hlt">model</span> simulations can then be compared to those seen in the <span class="hlt">observations</span> to identify areas for improvement in the <span class="hlt">model</span> simulations. We identify and track tropical convective systems in the Tropical Western Pacific using geostationary satellite <span class="hlt">observations</span>. We present statistics of the tropical convective systems including size, age, and intensity and classify the lifecycle stage of each system as developing, mature, or dissipating. For systems that cross over the ARM Darwin site, information on convective intensity and anvil properties are obtained from the C-Pol precipitation radar and MMCR cloud radar, respectively, and are examined as a function of the system lifecycle. Initial results from applying the convective identification and tracking algorithm to a tropical simulation from the Weather Research and Forecasting (WRF) <span class="hlt">model</span> run show that the <span class="hlt">model</span> produces reasonable overall statistics of convective systems, but details of the life cycle (such as diurnal cycle, system tracks) differ from the <span class="hlt">observations</span>. Further work will focus on the role of atmospheric temperature and moisture profiles in the <span class="hlt">model</span>'s convective life cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvC..96c4302C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvC..96c4302C"><span>Statistical approaches to lifetime <span class="hlt">measurements</span> with restricted <span class="hlt">observation</span> times</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, X. C.; Zeng, Q.; Litvinov, Yu. A.; Tu, X. L.; Walker, P. M.; Wang, M.; Wang, Q.; Yue, K.; Zhang, Y. H.</p> <p>2017-09-01</p> <p>Two generic methods based on frequentism and Bayesianism are presented in this work aiming to adequately estimate decay lifetimes from <span class="hlt">measured</span> data, while accounting for restricted <span class="hlt">observation</span> times in the <span class="hlt">measurements</span>. All the experimental scenarios that can possibly arise from the <span class="hlt">observation</span> constraints are treated systematically and formulas are derived. The methods are then tested against the decay data of bare isomeric 44+94mRu, which were <span class="hlt">measured</span> using isochronous mass spectrometry with a timing detector at the CSRe in Lanzhou, China. Applying both methods in three distinct scenarios yields six different but consistent lifetime estimates. The deduced values are all in good agreement with a prediction based on the neutral-atom value modified to take the absence of internal conversion into account. Potential applications of such methods are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMOS11B..06M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMOS11B..06M"><span>Application of a Topological Metric for Assessing Numerical Ocean <span class="hlt">Models</span> with Satellite <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morey, S. L.; Dukhovskoy, D. S.; Hiester, H. R.; Garcia-Pineda, O. G.; MacDonald, I. R.</p> <p>2015-12-01</p> <p>Satellite-based sensors provide a vast amount of <span class="hlt">observational</span> data over the world ocean. Active microwave radars <span class="hlt">measure</span> changes in sea surface height and backscattering from surface waves. Data from passive radiometers sensing emissions in multiple spectral bands can directly <span class="hlt">measure</span> surface temperature, be combined with other data sources to estimate salinity, or processed to derive estimates of optically significant quantities, such as concentrations of biochemical properties. Estimates of the hydrographic variables can be readily used for assimilation or assessment of hydrodynamic ocean <span class="hlt">models</span>. Optical data, however, have been underutilized in ocean circulation <span class="hlt">modeling</span>. Qualitative assessments of oceanic fronts and other features commonly associated with changes in optically significant quantities are often made through visual comparison. This project applies a topological approach, borrowed from the field of computer image recognition, to quantitatively evaluate ocean <span class="hlt">model</span> simulations of features that are related to quantities inferred from satellite imagery. The Modified Hausdorff Distance (MHD) provides a <span class="hlt">measure</span> of the similarity of two shapes. Examples of applications of the MHD to assess ocean circulation <span class="hlt">models</span> are presented. The first application assesses several <span class="hlt">models</span>' representation of the freshwater plume structure from the Mississippi River, which is associated with a significant expression of color, using a satellite-derived ocean color index. Even though the variables being compared (salinity and ocean color index) differ, the MHD allows contours of the fields to be compared topologically. The second application assesses simulations of surface oil transport driven by winds and ocean <span class="hlt">model</span> currents using surface oil maps derived from synthetic aperture radar backscatter data. In this case, maps of time composited oil coverage are compared between the simulations and satellite <span class="hlt">observations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ACPD...1531247W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ACPD...1531247W"><span>Atmospheric OH reactivity in central London: <span class="hlt">observations</span>, <span class="hlt">model</span> predictions and estimates of in situ ozone production</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Whalley, L. K.; Stone, D.; Bandy, B.; Dunmore, R.; Hamilton, J. F.; Hopkins, J.; Lee, J. D.; Lewis, A. C.; Heard, D. E.</p> <p>2015-11-01</p> <p>Near-continuous <span class="hlt">measurements</span> of OH reactivity in the urban background atmosphere of central London during the summer of 2012 are presented. OH reactivity behaviour is seen to be broadly dependent on airmass origin with the highest reactivity and the most pronounced diurnal profile <span class="hlt">observed</span> when air had passed over central London to the East, prior to <span class="hlt">measurement</span>. Averaged over the entire <span class="hlt">observation</span> period of 26 days, OH reactivity peaked at ~ 27 s-1 in the morning with a minimum of ~ 15 s-1 during the afternoon. A maximum OH reactivity of 116 s-1 was recorded on one day during morning rush hour. A detailed box <span class="hlt">model</span> using the Master Chemical Mechanism was used to calculate OH reactivity, and was constrained with an extended <span class="hlt">measurement</span> dataset of volatile organic compounds (VOCs) derived from GC-FID and a two-dimensional GC instrument which included heavier molecular weight (up to C12) aliphatic VOCs, oxygenated VOCs and the biogenic VOCs of α pinene and limonene. Comparison was made between <span class="hlt">observed</span> OH reactivity and <span class="hlt">modelled</span> OH reactivity using (i) a standard suite of VOC <span class="hlt">measurements</span> (C2-C8 hydrocarbons and a small selection of oxygenated VOCs) and (ii) a more comprehensive inventory including species up to C12. <span class="hlt">Modelled</span> reactivities were lower than those <span class="hlt">measured</span> (by 33 %) when only the reactivity of the standard VOC suite was considered. The difference between <span class="hlt">measured</span> and <span class="hlt">modelled</span> reactivity was improved, to within 15 %, if the reactivity of the higher VOCs (≥ C9) was also considered, with the reactivity of the biogenic compounds of α pinene and limonene and their oxidation products almost entirely responsible for this improvement. Further improvements in the <span class="hlt">model</span>'s ability to reproduce OH reactivity (to within 6 %) could be achieved if the reactivity and degradation mechanism of unassigned two-dimensional GC peaks were estimated. Neglecting the contribution of the higher VOCs (≥ C9) (particularly α pinene and limonene) and <span class="hlt">model</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18401692','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18401692"><span>The Classroom <span class="hlt">Observation</span> Schedule to <span class="hlt">Measure</span> Intentional Communication (COSMIC): an <span class="hlt">observational</span> <span class="hlt">measure</span> of the intentional communication of children with autism in an unstructured classroom setting.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pasco, Greg; Gordon, Rosanna K; Howlin, Patricia; Charman, Tony</p> <p>2008-11-01</p> <p>The Classroom <span class="hlt">Observation</span> Schedule to <span class="hlt">Measure</span> Intentional Communication (COSMIC) was devised to provide ecologically valid outcome <span class="hlt">measures</span> for a communication-focused intervention trial. Ninety-one children with autism spectrum disorder aged 6 years 10 months (SD 16 months) were videoed during their everyday snack, teaching and free play activities. Inter-rater reliability was high and relevant items showed significant associations with comparable items from concurrent Autism Diagnostic <span class="hlt">Observation</span> Schedule-Generic (Lord et al. 2000, J Autism Dev Disord 30(3):205-223) assessments. In a subsample of 28 children initial differences in rates of initiations, initiated speech/vocalisation and commenting were predictive of language and communication competence 15 months later. Results suggest that the use of <span class="hlt">observational</span> <span class="hlt">measures</span> of intentional communication in natural settings is a valuable assessment strategy for research and clinical practice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.A53D1441Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.A53D1441Z"><span>Use of High-Resolution Satellite <span class="hlt">Observations</span> to Evaluate Cloud and Precipitation Statistics from Cloud-Resolving <span class="hlt">Model</span> Simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, Y.; Tao, W.; Hou, A. Y.; Zeng, X.; Shie, C.</p> <p>2007-12-01</p> <p>The cloud and precipitation statistics simulated by 3D Goddard Cumulus Ensemble (GCE) <span class="hlt">model</span> for different environmental conditions, i.e., the South China Sea Monsoon Experiment (SCSMEX), CRYSTAL-FACE, and KAWJEX are compared with Tropical Rainfall <span class="hlt">Measuring</span> Mission (TRMM) TMI and PR rainfall <span class="hlt">measurements</span> and as well as cloud <span class="hlt">observations</span> from the Earth's Radiant Energy System (CERES) and the Moderate Resolution Imaging Spectroradiometer (MODIS) instruments. It is found that GCE is capable of simulating major convective system development and reproducing total surface rainfall amount as compared with rainfall estimated from the soundings. The <span class="hlt">model</span> presents large discrepancies in rain spectrum and vertical hydrometer profiles. The discrepancy in the precipitation field is also consistent with the cloud and radiation <span class="hlt">observations</span>. The study will focus on the effects of large scale forcing and microphysics to the simulated <span class="hlt">model</span>- <span class="hlt">observation</span> discrepancies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820049148&hterms=Non+equivalent&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DNon%2Bequivalent','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820049148&hterms=Non+equivalent&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DNon%2Bequivalent"><span>IUE <span class="hlt">observations</span> of Si and C lines and comparison with non-LTE <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kamp, L. W.</p> <p>1982-01-01</p> <p>Classical <span class="hlt">model</span> atmosphere techniques are applied to analyze IUE spectra, and to determine abundances, effective temperatures and gravities. <span class="hlt">Measurements</span> of the equivalent widths and other properties of the line profiles of 24 photospheric lines of Si II, Si III, Si IV, C II, C III and C IV are presented in the range of 1175-1725 A for seven B and two O stars. <span class="hlt">Observed</span> line profiles are compared with theoretical profiles computed using non-LTE theory and <span class="hlt">models</span>, and using line-blanketed <span class="hlt">model</span> atmospheres. Agreement is reasonably good, although strong lines are calculated to be systematically stronger than those <span class="hlt">observed</span>, while the reverse occurs for weak lines, and empirical profiles have smaller wings than theoretical profiles. It is concluded that the present theory of line formation when used with solar abundances, represents fairly well <span class="hlt">observed</span> UV photospheric lines of silicon and carbon ions in the atmospheres of main sequence stars of types B5-O9.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130004326','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130004326"><span>The Martian Dust Cycle: <span class="hlt">Observations</span> and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kahre, Melinda A.</p> <p>2013-01-01</p> <p>The dust cycle is critically important for Mars' current climate system. Suspended atmospheric dust affects the radiative balance of the atmosphere, and thus greatly influences the thermal and dynamical state of the atmosphere. Evidence for the presence of dust in the Martian atmosphere can be traced back to yellow clouds telescopically <span class="hlt">observed</span> as early as the early 19th century. The Mariner 9 orbiter arrived at Mars in November of 1971 to find a planet completely enshrouded in airborne dust. Since that time, the exchange of dust between the planet's surface and atmosphere and the role of airborne dust on Mars' weather and climate has been studied using <span class="hlt">observations</span> and numerical <span class="hlt">models</span>. The goal of this talk is to give an overview of the <span class="hlt">observations</span> and to discuss the successes and challenges associated with <span class="hlt">modeling</span> the dust cycle. Dust raising events on Mars range in size from meters to hundreds of kilometers. During some years, regional storms merge to produce hemispheric or planet encircling dust clouds that obscure the surface and raise atmospheric temperatures by tens of kelvin. The interannual variability of planet encircling dust storms is poorly understood. Although the occurrence and season of large regional and global dust storms are highly variable from one year to the next, there are many features of the dust cycle that occur year after year. A low-level dust haze is maintained during northern spring and summer, while elevated levels of atmospheric dust occur during northern autumn and winter. During years without global-scale dust storms, two peaks in total dust loading are generally <span class="hlt">observed</span>: one peak occurs before northern winter solstice and one peak occurs after northern winter solstice. Numerical <span class="hlt">modeling</span> studies attempting to interactively simulate the Martian dust cycle with general circulation <span class="hlt">models</span> (GCMs) include the lifting, transport, and sedimentation of radiatively active dust. Two dust lifting processes are commonly represented in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24961999','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24961999"><span><span class="hlt">Measuring</span> the quality of life and well-being of people with dementia: A review of <span class="hlt">observational</span> <span class="hlt">measures</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Algar, Katherine; Woods, Robert T; Windle, Gill</p> <p>2016-07-01</p> <p>The dynamic nature of psychosocial interventions implies that trying to <span class="hlt">measure</span> their effects using standardised clinical trial <span class="hlt">measures</span> may not capture their full effects. Rich and valuable data during the sessions may be missed by using standard quality of life questionnaires. This paper compares <span class="hlt">observational</span> <span class="hlt">measures</span> in the context of recording the well-being of a person with dementia during and outside of a visual arts intervention. A literature search was conducted using systematic principles of searching, screening and retrieval to identify peer-reviewed English language evaluations of research projects using <span class="hlt">observational</span> <span class="hlt">measures</span> with people with dementia. Psychometric properties, strengths and weaknesses of 11 <span class="hlt">observational</span> tools are reviewed in order to identify the most appropriate one for evaluating a visual art intervention for people with dementia. This review supports the Greater Cincinnati Chapter Well-Being <span class="hlt">Observation</span> Tool as an appropriate <span class="hlt">measure</span> to evaluate a visual art programme for people with dementia. The results of this review will help researchers plan projects to show the full range of effects for people with dementia for taking part in art sessions. © The Author(s) 2014.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22518719-nanograv-nine-year-data-set-observations-arrival-time-measurements-analysis-millisecond-pulsars','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22518719-nanograv-nine-year-data-set-observations-arrival-time-measurements-analysis-millisecond-pulsars"><span>THE NANOGRAV NINE-YEAR DATA SET: <span class="hlt">OBSERVATIONS</span>, ARRIVAL TIME <span class="hlt">MEASUREMENTS</span>, AND ANALYSIS OF 37 MILLISECOND PULSARS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Arzoumanian, Zaven; Brazier, Adam; Chatterjee, Shami</p> <p>2015-11-01</p> <p>We present high-precision timing <span class="hlt">observations</span> spanning up to nine years for 37 millisecond pulsars monitored with the Green Bank and Arecibo radio telescopes as part of the North American Nanohertz Observatory for Gravitational Waves (NANOGrav) project. We describe the <span class="hlt">observational</span> and instrumental setups used to collect the data, and methodology applied for calculating pulse times of arrival; these include novel methods for <span class="hlt">measuring</span> instrumental offsets and characterizing low signal-to-noise ratio timing results. The time of arrival data are fit to a physical timing <span class="hlt">model</span> for each source, including terms that characterize time-variable dispersion <span class="hlt">measure</span> and frequency-dependent pulse shape evolution. Inmore » conjunction with the timing <span class="hlt">model</span> fit, we have performed a Bayesian analysis of a parameterized timing noise <span class="hlt">model</span> for each source, and detect evidence for excess low-frequency, or “red,” timing noise in 10 of the pulsars. For 5 of these cases this is likely due to interstellar medium propagation effects rather than intrisic spin variations. Subsequent papers in this series will present further analysis of this data set aimed at detecting or limiting the presence of nanohertz-frequency gravitational wave signals.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Methodological%2c+AND+study&pg=2&id=EJ1042332','ERIC'); return false;" href="https://eric.ed.gov/?q=Methodological%2c+AND+study&pg=2&id=EJ1042332"><span>Alternating Renewal Process <span class="hlt">Models</span> for Behavioral <span class="hlt">Observation</span>: Simulation Methods, Software, and Validity Illustrations</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Pustejovsky, James E.; Runyon, Christopher</p> <p>2014-01-01</p> <p>Direct <span class="hlt">observation</span> recording procedures produce reductive summary <span class="hlt">measurements</span> of an underlying stream of behavior. Previous methodological studies of these recording procedures have employed simulation methods for generating random behavior streams, many of which amount to special cases of a statistical <span class="hlt">model</span> known as the alternating renewal…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013144','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013144"><span>Solar Ion Processing of Itokawa Grains: Reconciling <span class="hlt">Model</span> Predictions with Sample <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Christoffersen, Roy; Keller, L. P.</p> <p>2014-01-01</p> <p>Analytical TEM <span class="hlt">observations</span> of Itokawa grains reported to date show complex solar wind ion processing effects in the outer 30-100 nm of pyroxene and olivine grains. The effects include loss of long-range structural order, formation of isolated interval cavities or "bubbles", and other nanoscale compositional/microstructural variations. None of the effects so far described have, however, included complete ion-induced amorphization. To link the array of <span class="hlt">observed</span> relationships to grain surface exposure times, we have adapted our previous numerical <span class="hlt">model</span> for progressive solar ion processing effects in lunar regolith grains to the Itokawa samples. The <span class="hlt">model</span> uses SRIM ion collision damage and implantation calculations within a framework of a constant-deposited-energy <span class="hlt">model</span> for amorphization. Inputs include experimentally-<span class="hlt">measured</span> amorphization fluences, a Pi steradian variable ion incidence geometry required for a rotating asteroid, and a numerical flux-versus-velocity solar wind spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123.3714E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123.3714E"><span>Comparison of Global Martian Plasma <span class="hlt">Models</span> in the Context of MAVEN <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Egan, Hilary; Ma, Yingjuan; Dong, Chuanfei; Modolo, Ronan; Jarvinen, Riku; Bougher, Stephen; Halekas, Jasper; Brain, David; Mcfadden, James; Connerney, John; Mitchell, David; Jakosky, Bruce</p> <p>2018-05-01</p> <p>Global <span class="hlt">models</span> of the interaction of the solar wind with the Martian upper atmosphere have proved to be valuable tools for investigating both the escape to space of the Martian atmosphere and the physical processes controlling this complex interaction. The many <span class="hlt">models</span> currently in use employ different physical assumptions, but it can be difficult to directly compare the effectiveness of the <span class="hlt">models</span> since they are rarely run for the same input conditions. Here we present the results of a <span class="hlt">model</span> comparison activity, where five global <span class="hlt">models</span> (single-fluid MHD, multifluid MHD, multifluid electron pressure MHD, and two hybrid <span class="hlt">models</span>) were run for identical conditions corresponding to a single orbit of <span class="hlt">observations</span> from the Mars Atmosphere and Volatile EvolutioN (MAVEN) spacecraft. We find that low-altitude ion densities are very similar across all <span class="hlt">models</span> and are comparable to MAVEN ion density <span class="hlt">measurements</span> from periapsis. Plasma boundaries appear generally symmetric in all <span class="hlt">models</span> and vary only slightly in extent. Despite these similarities there are clear morphological differences in ion behavior in other regions such as the tail and southern hemisphere. These differences are <span class="hlt">observable</span> in ion escape loss maps and are necessary to understand in order to accurately use <span class="hlt">models</span> in aiding our understanding of the Martian plasma environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998AtmEn..32.4207S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998AtmEn..32.4207S"><span>Mesoscale influence on long-range transport — evidence from ETEX <span class="hlt">modelling</span> and <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sørensen, Jens Havskov; Rasmussen, Alix; Ellermann, Thomas; Lyck, Erik</p> <p></p> <p>During the first European Tracer Experiment (ETEX) tracer gas was released from a site in Brittany, France, and subsequently <span class="hlt">observed</span> over a range of 2000 km. Hourly <span class="hlt">measurements</span> were taken at the National Environmental Research Institute (NERI) located at Risø, Denmark, using two <span class="hlt">measurement</span> techniques. At this location, the <span class="hlt">observed</span> concentration time series shows a double-peak structure occurring between two and three days after the release. By using the Danish Emergency Response <span class="hlt">Model</span> of the Atmosphere (DERMA), which is developed at the Danish Meteorological Institute (DMI), simulations of the dispersion of the tracer gas have been performed. Using numerical weather-prediction data from the European Centre for Medium-Range Weather Forecast (ECMWF) by DERMA, the arrival time of the tracer is quite well predicted, so also is the duration of the passage of the plume, but the double-peak structure is not reproduced. However, using higher-resolution data from the DMI version of the HIgh Resolution Limited Area <span class="hlt">Model</span> (DMI-HIRLAM), DERMA reproduces the <span class="hlt">observed</span> structure very well. The double-peak structure is caused by the influence of a mesoscale anti-cyclonic eddy on the tracer gas plume about one day earlier.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B23B0578F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B23B0578F"><span><span class="hlt">Observations</span> and <span class="hlt">modeling</span> of methane flux in northern wetlands</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Futakuchi, Y.; Ueyama, M.; Matsumoto, Y.; Yazaki, T.; Hirano, T.; Kominami, Y.; Harazono, Y.; Igarashi, Y.</p> <p>2016-12-01</p> <p>Methane (CH4) budgets in northern wetlands vary greatly with high spatio-temporal heterogeneity. Owing to limited available data, yet, it is difficult to constrain the CH4 emission from northern wetlands. In this context, we continuously <span class="hlt">measured</span> CH4 fluxes at two northern wetlands. <span class="hlt">Measured</span> fluxes were used for constraining the new <span class="hlt">model</span> that empirically partitioned net CH4 fluxes into the processes of production, oxidation, and transport associated with ebullition, diffusion, and plant, based on the optimization technique. This study reveal the important processes related to the seasonal variations in CH4 emission with the continuous <span class="hlt">observations</span> and inverse <span class="hlt">model</span> analysis. The <span class="hlt">measurements</span> have been conducted at a Sphagnum-dominated cool temperate bog (BBY) since April 2015 using the open-path eddy covariance method and a sub-arctic forested bog on permafrost in University of Alaska Fairbanks (UAF) since May 2016 using three automated chambers by a laser-based gas analyzer (FGGA-24r-EP, Los Gatos Research Inc., USA). In BBY, daily CH4 fluxes ranged from 1.9 nmol m-2 s-1 in early spring to 97.9 nmol m-2 s-1 in mid-summer. Growing-season total CH4 flux was 13 g m-2 yr-1 in 2015. In contrast, CH4 flux at the UAF site was small (0.2 to 1.0 nmol m-2 s-1), and hardly increased since start of the <span class="hlt">observation</span>. This difference could be caused by the difference in the climate and soil conditions; mean air and soil temperature, and presence of permafrost. For BBY, the seasonal variation of CH4 emission was mostly explained by soil temperature, suggesting that the production was the important controlling process. In mid-summer when soil temperature was high, however, decrease in atmospheric pressure and increase in vegetation greenness stimulated CH4 emission probably through plant-mediated transport and form of bubble, suggesting that the transport processes were important. Based on a preliminary results by the <span class="hlt">model</span> optimization in BBY site, CH4 fluxes were strongly</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018oeps.book...79G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018oeps.book...79G"><span>Martian Ionospheric <span class="hlt">Observation</span> and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>González-Galindo, Francisco</p> <p>2018-02-01</p> <p> <span class="hlt">measurements</span> by different space missions. Numerical simulations by computational <span class="hlt">models</span> able to simulate the processes that shape the ionosphere have also been commonly employed to obtain information about this region, to provide an interpretation of the <span class="hlt">observations</span> and to fill their gaps. As a result, the Martian ionosphere is today the best known one after that of the Earth. However, there are still areas for which our knowledge is far from being complete. Examples are the details and balance of the mechanisms populating the nightside ionosphere, or a good understanding of the meteoric ionospheric layer and its variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNH23A0255O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNH23A0255O"><span>Ionospheric detection of tsunami earthquakes: <span class="hlt">observation</span>, <span class="hlt">modeling</span> and ideas for future early warning</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Occhipinti, G.; Manta, F.; Rolland, L.; Watada, S.; Makela, J. J.; Hill, E.; Astafieva, E.; Lognonne, P. H.</p> <p>2017-12-01</p> <p>Detection of ionospheric anomalies following the Sumatra and Tohoku earthquakes (e.g., Occhipinti 2015) demonstrated that ionosphere is sensitive to earthquake and tsunami propagation: ground and oceanic vertical displacement induces acoustic-gravity waves propagating within the neutral atmosphere and detectable in the ionosphere. <span class="hlt">Observations</span> supported by <span class="hlt">modelling</span> proved that ionospheric anomalies related to tsunamis are deterministic and reproducible by numerical <span class="hlt">modeling</span> via the ocean/neutral-atmosphere/ionosphere coupling mechanism (Occhipinti et al., 2008). To prove that the tsunami signature in the ionosphere is routinely detected we show here perturbations of total electron content (TEC) <span class="hlt">measured</span> by GPS and following tsunamigenic earthquakes from 2004 to 2011 (Rolland et al. 2010, Occhipinti et al., 2013), nominally, Sumatra (26 December, 2004 and 12 September, 2007), Chile (14 November, 2007), Samoa (29 September, 2009) and the recent Tohoku-Oki (11 Mars, 2011). Based on the <span class="hlt">observations</span> close to the epicenter, mainly performed by GPS networks located in Sumatra, Chile and Japan, we highlight the TEC perturbation <span class="hlt">observed</span> within the first 8 min after the seismic rupture. This perturbation contains information about the ground displacement, as well as the consequent sea surface displacement resulting in the tsunami. In addition to GNSS-TEC <span class="hlt">observations</span> close to the epicenter, new exciting <span class="hlt">measurements</span> in the far-field were performed by airglow <span class="hlt">measurement</span> in Hawaii show the propagation of the internal gravity waves induced by the Tohoku tsunami (Occhipinti et al., 2011). This revolutionary imaging technique is today supported by two new <span class="hlt">observations</span> of moderate tsunamis: Queen Charlotte (M: 7.7, 27 October, 2013) and Chile (M: 8.2, 16 September 2015). We finally detail here our recent work (Manta et al., 2017) on the case of tsunami alert failure following the Mw7.8 Mentawai event (25 October, 2010), and its twin tsunami alert response following the Mw7</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1842c0031K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1842c0031K"><span>A <span class="hlt">measurement</span> <span class="hlt">model</span> of multiple intelligence profiles of management graduates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krishnan, Heamalatha; Awang, Siti Rahmah</p> <p>2017-05-01</p> <p>In this study, developing a fit <span class="hlt">measurement</span> <span class="hlt">model</span> and identifying the best fitting items to represent Howard Gardner's nine intelligences namely, musical intelligence, bodily-kinaesthetic intelligence, mathematical/logical intelligence, visual/spatial intelligence, verbal/linguistic intelligence, interpersonal intelligence, intrapersonal intelligence, naturalist intelligence and spiritual intelligence are the main interest in order to enhance the opportunities of the management graduates for employability. In order to develop a fit <span class="hlt">measurement</span> <span class="hlt">model</span>, Structural Equation <span class="hlt">Modeling</span> (SEM) was applied. A psychometric test which is the Ability Test in Employment (ATIEm) was used as the instrument to <span class="hlt">measure</span> the existence of nine types of intelligence of 137 University Teknikal Malaysia Melaka (UTeM) management graduates for job placement purposes. The initial <span class="hlt">measurement</span> <span class="hlt">model</span> contains nine unobserved variables and each unobserved variable is <span class="hlt">measured</span> by ten <span class="hlt">observed</span> variables. Finally, the modified <span class="hlt">measurement</span> <span class="hlt">model</span> deemed to improve the Normed chi-square (NC) = 1.331; Incremental Fit Index (IFI) = 0.940 and Root Mean Square of Approximation (RMSEA) = 0.049 was developed. The findings showed that the UTeM management graduates possessed all nine intelligences either high or low. Musical intelligence, mathematical/logical intelligence, naturalist intelligence and spiritual intelligence contributed highest loadings on certain items. However, most of the intelligences such as bodily kinaesthetic intelligence, visual/spatial intelligence, verbal/linguistic intelligence interpersonal intelligence and intrapersonal intelligence possessed by UTeM management graduates are just at the borderline.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29677464','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29677464"><span>Improving the quality of preclinical research echocardiography: <span class="hlt">Observations</span>, training and guidelines for <span class="hlt">measurement</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Donner, Daniel G; Kiriazis, Helen; Du, Xiao-Jun; Marwick, Thomas H; McMullen, Julie R</p> <p>2018-04-20</p> <p>Informal training in preclinical research may be a contributor to the poor reproducibility of preclinical cardiology research and low rates of translation into clinical research and practice. Mouse echocardiography is a widely used technique to assess cardiac structure and function in drug intervention studies using disease <span class="hlt">models</span>. The inter-<span class="hlt">observer</span> variability (IOV) of clinical echocardiographic <span class="hlt">measurements</span> has been shown to improve with formalized training, but preclinical echocardiography lacks similarly critical standardization of training. The aims of this investigation were to assess the IOV of echocardiographic <span class="hlt">measurements</span> from studies in mice, and address any technical impediments to reproducibility by implementing standardized guidelines through formalized training. In this prospective, single-site, <span class="hlt">observational</span> cohort study, 13 scientists performing preclinical echocardiographic image analysis were assessed for <span class="hlt">measurement</span> of short-axis M-mode-derived dimensions and calculated left ventricular mass (LVMass). Ten M-mode images of mouse hearts acquired and analyzed by an expert researcher with a spectrum of LVMass were selected for assessment, and validated by autopsy weight. Following the initial <span class="hlt">observation</span>, a structured formal training program was introduced, and accuracy and reproducibility were re-evaluated. Mean absolute percentage error (MAPE) for Expert-calculated LVMass was 6{plus minus}4% compared to autopsy LVMass, and 25{plus minus}21% for participants before training. Standardized formal training improved participant MAPE by approximately 30% relative to expert-calculated LVMass (p<0.001). Participants initially categorized with high-range error (25-45%) improved to low-moderate error ranges (<15-25%). This report reveals an example of technical skill training insufficiency likely endemic to preclinical research and provides validated guidelines for echocardiographic <span class="hlt">measurement</span> for adaptation to formalized in-training programs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12..499M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12..499M"><span>Interplanetary plasma scintillation parameters <span class="hlt">measurements</span> retrieved from the spacecraft <span class="hlt">observations</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Molera Calvés, Guifré; Pogrebenko, S. V.; Wagner, J.; Maccaferri, G.; Colucci, G.; Kronschnabl, G.; Scilliro, F.; Bianco, G.; Pérez Ayúcar, M.; Cosmovici, C. B.</p> <p>2010-05-01</p> <p><span class="hlt">Measurement</span> of the Interplanetary Scintillations (IPS) of radio signals propagating through the plasma in the Solar System by the radio astronomical instruments is a powerful tool to characterise and study the spatial and temporal variation of the electron density in the Solar wind. Several techniques based on the <span class="hlt">observation</span> of natural and artificial radio sources have been developed during the last 50 years. Here we report our results of the IPS parameters <span class="hlt">measurement</span> based on the multi-station <span class="hlt">observations</span> of the planetary mission spacecraft. The ESA Venus Express spacecraft was <span class="hlt">observed</span> at X-band (8.4 GHz) by several European VLBI stations - Metsähovi Radio Observatory (Aalto University , FI), Medicina (INAF-RA, IT), Matera (ASI, IT), Wettzell (BKG, DE), Noto (INAF-IRA, IT) and Yebes (OAN-IGN, ES) during a 2008-2010 campaign in a framework of the PRIDE (Planetary Radio Interferometry and Doppler Experiments) project as a preparatory stage for the European Radio Astronomy VLBI facilities participation in the planned ESA planetary missions (EJSM, TESM, EVE and others). <span class="hlt">Observational</span> data were processed at Metsähovi Radio Observatory with the on-purpose developed high performance, ultra-high spectral resolution and spacecraft tracking capable software spectrometer-correlator and analysed at the Joint Institute for VLBI in Europe (JIVE, NL). High quality of acquired and analysed data enables us to study and define several parameters of the S/C signal and accompanying "ranging" tones with milli-Hz accuracy, among which the phase fluctuations of the spacecraft signal carrier line can be used to characterise the interplanetary plasma density fluctuations along the signal propagation line at different spatial and temporal scales at different Solar elongations and which exhibits a near-Kolmogorov spectrum. Such essential parameters as the phase scintillation index and bandwidth of scintillations and their dependence on the solar elongation, distance to the target</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2898131','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2898131"><span>Glass microneedles for force <span class="hlt">measurements</span>: a finite-element analysis <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ayittey, Peter N.; Walker, John S.; Rice, Jeremy J.; de Tombe, Pieter P.</p> <p>2010-01-01</p> <p>Changes in developed force (0.1–3.0 μN) <span class="hlt">observed</span> during contraction of single myofibrils in response to rapidly changing calcium concentrations can be <span class="hlt">measured</span> using glass microneedles. These microneedles are calibrated for stiffness and deflect on response to developed myofibril force. The precision and accuracy of kinetic <span class="hlt">measurements</span> are highly dependent on the structural and mechanical characteristics of the microneedles, which are generally assumed to have a linear force–deflection relationship. We present a finite-element analysis (FEA) <span class="hlt">model</span> used to simulate the effects of <span class="hlt">measurable</span> geometry on stiffness as a function of applied force and validate our <span class="hlt">model</span> with actual <span class="hlt">measured</span> needle properties. In addition, we developed a simple heuristic constitutive equation that best describes the stiffness of our range of microneedles used and define limits of geometry parameters within which our predictions hold true. Our <span class="hlt">model</span> also maps a relation between the geometry parameters and natural frequencies in air, enabling optimum parametric combinations for microneedle fabrication that would reflect more reliable force <span class="hlt">measurement</span> in fluids and physiological environments. We propose a use for this <span class="hlt">model</span> to aid in the design of microneedles to improve calibration time, reproducibility, and precision for <span class="hlt">measuring</span> myofibrillar, cellular, and supramolecular kinetic forces. PMID:19104827</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A51A0002J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A51A0002J"><span>Process-oriented <span class="hlt">Observational</span> Metrics for CMIP6 Climate <span class="hlt">Model</span> Assessments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, J. H.; Su, H.</p> <p>2016-12-01</p> <p><span class="hlt">Observational</span> metrics based on satellite <span class="hlt">observations</span> have been developed and effectively applied during post-CMIP5 <span class="hlt">model</span> evaluation and improvement projects. As new physics and parameterizations continue to be included in <span class="hlt">models</span> for the upcoming CMIP6, it is important to continue objective comparisons between <span class="hlt">observations</span> and <span class="hlt">model</span> results. This talk will summarize the process-oriented <span class="hlt">observational</span> metrics and methodologies for constraining climate <span class="hlt">models</span> with A-Train satellite <span class="hlt">observations</span> and support CMIP6 <span class="hlt">model</span> assessments. We target parameters and processes related to atmospheric clouds and water vapor, which are critically important for Earth's radiative budget, climate feedbacks, and water and energy cycles, and thus reduce uncertainties in climate <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS11A1256H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS11A1256H"><span>Surfzone alongshore advective accelerations: <span class="hlt">observations</span> and <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, J.; Raubenheimer, B.; Elgar, S.</p> <p>2014-12-01</p> <p>The sources, magnitudes, and impacts of non-linear advective accelerations on alongshore surfzone currents are investigated with <span class="hlt">observations</span> and a numerical <span class="hlt">model</span>. Previous numerical <span class="hlt">modeling</span> results have indicated that advective accelerations are an important contribution to the alongshore force balance, and are required to understand spatial variations in alongshore currents (which may result in spatially variable morphological change). However, most prior <span class="hlt">observational</span> studies have neglected advective accelerations in the alongshore force balance. Using a numerical <span class="hlt">model</span> (Delft3D) to predict optimal sensor locations, a dense array of 26 colocated current meters and pressure sensors was deployed between the shoreline and 3-m water depth over a 200 by 115 m region near Duck, NC in fall 2013. The array included 7 cross- and 3 alongshore transects. Here, <span class="hlt">observational</span> and numerical estimates of the dominant forcing terms in the alongshore balance (pressure and radiation-stress gradients) and the advective acceleration terms will be compared with each other. In addition, the numerical <span class="hlt">model</span> will be used to examine the force balance, including sources of velocity gradients, at a higher spatial resolution than possible with the instrument array. Preliminary numerical results indicate that at O(10-100 m) alongshore scales, bathymetric variations and the ensuing alongshore variations in the wave field and subsequent forcing are the dominant sources of the <span class="hlt">modeled</span> velocity gradients and advective accelerations. Additional simulations and analysis of the <span class="hlt">observations</span> will be presented. Funded by NSF and ASDR&E.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950016594','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950016594"><span>Dynamic response tests of inertial and optical wind-tunnel <span class="hlt">model</span> attitude <span class="hlt">measurement</span> devices</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Buehrle, R. D.; Young, C. P., Jr.; Burner, A. W.; Tripp, J. S.; Tcheng, P.; Finley, T. D.; Popernack, T. G., Jr.</p> <p>1995-01-01</p> <p>Results are presented for an experimental study of the response of inertial and optical wind-tunnel <span class="hlt">model</span> attitude <span class="hlt">measurement</span> systems in a wind-off simulated dynamic environment. This study is part of an ongoing activity at the NASA Langley Research Center to develop high accuracy, advanced <span class="hlt">model</span> attitude <span class="hlt">measurement</span> systems that can be used in a dynamic wind-tunnel environment. This activity was prompted by the inertial <span class="hlt">model</span> attitude sensor response <span class="hlt">observed</span> during high levels of <span class="hlt">model</span> vibration which results in a <span class="hlt">model</span> attitude <span class="hlt">measurement</span> bias error. Significant bias errors in <span class="hlt">model</span> attitude <span class="hlt">measurement</span> were found for the <span class="hlt">measurement</span> using the inertial device during wind-off dynamic testing of a <span class="hlt">model</span> system. The amount of bias present during wind-tunnel tests will depend on the amplitudes of the <span class="hlt">model</span> dynamic response and the modal characteristics of the <span class="hlt">model</span> system. Correction <span class="hlt">models</span> are presented that predict the vibration-induced bias errors to a high degree of accuracy for the vibration modes characterized in the simulated dynamic environment. The optical system results were uncorrupted by <span class="hlt">model</span> vibration in the laboratory setup.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1913099B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1913099B"><span><span class="hlt">Observing</span> atmospheric blocking with GPS radio occultation - one decade of <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brunner, Lukas; Steiner, Andrea</p> <p>2017-04-01</p> <p>Atmospheric blocking has received a lot of attention in recent years due to its impact on mid-latitude circulation and subsequently on weather extremes such as cold and warm spells. So far blocking studies have been based mainly on re-analysis data or <span class="hlt">model</span> output. However, it has been shown that blocking frequency exhibits considerable inter-<span class="hlt">model</span> spread in current climate <span class="hlt">models</span>. Here we use one decade (2006 to 2016) of satellite-based <span class="hlt">observations</span> from GPS radio occultation (RO) to analyze blocking in RO data building on work by Brunner et al. (2016). Daily fields on a 2.5°×2.5° longitude-latitude grid are calculated by applying an adequate gridding strategy to the RO <span class="hlt">measurements</span>. For blocking detection we use a standard blocking detection algorithm based on 500 hPa geopotential height (GPH) gradients. We investigate vertically resolved atmospheric variables such as GPH, temperature, and water vapor before, during, and after blocking events to increase process understanding. Moreover, utilizing the coverage of the RO data set, we investigate global blocking frequencies. The main blocking regions in the northern and southern hemisphere are identified and the (vertical) atmospheric structure linked to blocking events is compared. Finally, an inter-comparison of results from RO data to different re-analyses, such as ERA-Interim, MERRA 2, and JRA-55, is presented. Brunner, L., A. K. Steiner, B. Scherllin-Pirscher, and M. W. Jury (2016): Exploring atmospheric blocking with GPS radio occultation <span class="hlt">observations</span>. Atmos. Chem. Phys., 16, 4593-4604, doi:10.5194/acp-16-4593-2016.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910199W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910199W"><span><span class="hlt">Observation</span> and <span class="hlt">modelling</span> of fog at Cold Lake, Alberta, Canada</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Di; Boudala, Faisal; Weng, Wensong; Taylor, Peter A.; Gultepe, Ismail; Isaac, George A.</p> <p>2017-04-01</p> <p> <span class="hlt">observational</span> data indicates that the surface-based in situ <span class="hlt">measurements</span> agree well with aviation weather <span class="hlt">observation</span> METAR reports and are comparable with <span class="hlt">model</span> simulations. Both the HRDPS <span class="hlt">model</span> and microwave radiometry data indicate low level fog and cloud formation but the depths and intensities differ considerably depending on environmental conditions. Causes for this are under investigation with the high resolution 1-D boundary-layer <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1913290T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1913290T"><span><span class="hlt">Modeling</span> of snow avalanches for protection <span class="hlt">measures</span> designing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Turchaninova, Alla; Lazarev, Anton; Loginova, Ekaterina; Seliverstov, Yuri; Glazovskaya, Tatiana; Komarov, Anton</p> <p>2017-04-01</p> <p>Avalanche protection structures such as dams have to be designed using well known standard engineering procedures that differ in different countries. Our intent is to conduct a research on structural avalanche protection <span class="hlt">measures</span> designing and their reliability assessment during the operation using numerical <span class="hlt">modeling</span>. In the Khibini Mountains, Russia, several avalanche dams have been constructed at different times to protect settlements and mining. Compared with other mitigation structures dams are often less expensive to construct in mining regions. The main goal of our investigation was to test the capabilities of Swiss avalanche dynamics <span class="hlt">model</span> RAMMS and Russian methods to simulate the interaction of avalanches with mitigation structures such as catching and reflecting dams as well as to reach the <span class="hlt">observed</span> runout distances after the transition through a dam. We present the RAMMS back-calculation results of an artificially triggered and well-documented catastrophic avalanche occurred in the town of Kirovsk, Khibini Mountains in February 2016 that has unexpectedly passed through a system of two catching dams and took the lives of 3 victims. The estimated volume of an avalanche was approximately 120,000 m3. For the calculation we used a 5 m DEM including catching dams generated from field <span class="hlt">measurements</span> in summer 2015. We simulated this avalanche (occurred below 1000 m.a.s.l.) in RAMMS having taken the friction parameters (µ and ζ) from the upper altitude limit (above 1500 m.a.s.l.) from the table recommended for Switzerland (implemented into RAMMS) according to the results of our previous research. RAMMS reproduced the <span class="hlt">observed</span> avalanche behavior and runout distance. No information is available concerning the flow velocity; however, calculated values correspond in general to the values <span class="hlt">measured</span> in this avalanche track before. We applied RAMMS using an option of adding structures to DEM (including a dam in GIS) in other to test other operating catching dams in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.A41E0075S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.A41E0075S"><span>A Test of <span class="hlt">Model</span> Validation from <span class="hlt">Observed</span> Temperature Trends</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singer, S. F.</p> <p>2006-12-01</p> <p> in much reduced values of climate sensitivity; for example, the neglect of important negative feedbacks. Allowing for uncertainties in the data and for imperfect <span class="hlt">models</span>, there is only one valid conclusion from the failure of greenhouse <span class="hlt">models</span> to explain the <span class="hlt">observations</span>: The human contribution to global warming is still quite small, so that natural climate factors are dominant. This may also explain why the climate was cooling from 1940 to 1975 -- even as greenhouse-gas levels increased rapidly. An overall test for climate prediction may soon be possible by <span class="hlt">measuring</span> the ongoing rise in sea level. According to my estimates, sea level should rise by 1.5 to 2.0 cm per decade (about the same rate as in past millennia); the U.N.-IPCC (4th Assessment Report) predicts 1.4 to 4.3 cm per decade. In the New York Review of Books (July 13, 2006), however, James Hansen suggests 20 feet or more per century -- equivalent to about 60 cm or more per decade.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2873259','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2873259"><span>Cross-sectional <span class="hlt">measures</span> and <span class="hlt">modelled</span> estimates of blood alcohol levels in UK nightlife and their relationships with drinking behaviours and <span class="hlt">observed</span> signs of inebriation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2010-01-01</p> <p>Background Management of nightlife in UK cities focuses on creating safe places for individuals to drink. Little is known about intoxication levels as <span class="hlt">measuring</span> total alcohol consumption on nights out is complicated by early evening interviews missing subsequent consumption and later interviews risking individuals being too drunk to recall consumption or participate at all. Here we assess mixed survey and <span class="hlt">modelling</span> techniques as a methodological approach to examining these issues. Methods Interviews with a cross sectional sample of nightlife patrons (n = 214) recruited at different locations in three cities established alcohol consumption patterns up to the point of interview, self-assessed drunkenness and intended drinking patterns throughout the remaining night out. Researchers <span class="hlt">observed</span> individuals' behaviours to independently assess drunkenness. Breath alcohol tests and general linear <span class="hlt">modelling</span> were used to <span class="hlt">model</span> blood alcohol levels at participants' expected time of leaving nightlife settings. Results At interview 49.53% of individuals regarded themselves as drunk and 79.43% intended to consume more alcohol before returning home, with around one in ten individuals (15.38% males; 4.35% females) intending to consume >40 units (equal to 400 mls of pure alcohol). Self-assessed drunkenness, researcher <span class="hlt">observed</span> <span class="hlt">measures</span> of sobriety and blood alcohol levels all correlated well. <span class="hlt">Modelled</span> estimates for blood alcohol at time of going home suggested that 71.68% of males would be over 0.15%BAC (gms alcohol/100 mls blood). Higher blood alcohol levels were related to drinking later into the night. Conclusions UK nightlife has used substantive health and judicial resources with the aim of creating safer and later drinking environments. Survey and <span class="hlt">modelling</span> techniques together can help characterise the condition of drinkers when using and leaving these settings. Here such methods identified patrons as routinely getting drunk, with risks of drunkenness increasing over later</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24623632','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24623632"><span>Anatomical knowledge gain through a clay-<span class="hlt">modeling</span> exercise compared to live and video <span class="hlt">observations</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kooloos, Jan G M; Schepens-Franke, Annelieke N; Bergman, Esther M; Donders, Rogier A R T; Vorstenbosch, Marc A T M</p> <p>2014-01-01</p> <p>Clay <span class="hlt">modeling</span> is increasingly used as a teaching method other than dissection. The haptic experience during clay <span class="hlt">modeling</span> is supposed to correspond to the learning effect of manipulations during exercises in the dissection room involving tissues and organs. We questioned this assumption in two pretest-post-test experiments. In these experiments, the learning effects of clay <span class="hlt">modeling</span> were compared to either live <span class="hlt">observations</span> (Experiment I) or video <span class="hlt">observations</span> (Experiment II) of the clay-<span class="hlt">modeling</span> exercise. The effects of learning were <span class="hlt">measured</span> with multiple choice questions, extended matching questions, and recognition of structures on illustrations of cross-sections. Analysis of covariance with pretest scores as the covariate was used to elaborate the results. Experiment I showed a significantly higher post-test score for the <span class="hlt">observers</span>, whereas Experiment II showed a significantly higher post-test score for the clay <span class="hlt">modelers</span>. This study shows that (1) students who perform clay-<span class="hlt">modeling</span> exercises show less gain in anatomical knowledge than students who attentively <span class="hlt">observe</span> the same exercise being carried out and (2) performing a clay-<span class="hlt">modeling</span> exercise is better in anatomical knowledge gain compared to the study of a video of the recorded exercise. The most important learning effect seems to be the engagement in the exercise, focusing attention and stimulating time on task. © 2014 American Association of Anatomists.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18818655','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18818655"><span><span class="hlt">Observed</span> and <span class="hlt">modelled</span> stability of overflow across the Greenland-Scotland ridge.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Olsen, Steffen M; Hansen, Bogi; Quadfasel, Detlef; Østerhus, Svein</p> <p>2008-09-25</p> <p>Across the Greenland-Scotland ridge there is a continuous flow of cold dense water, termed 'overflow', from the Nordic seas to the Atlantic Ocean. This is a main contributor to the production of North Atlantic Deep Water that feeds the lower limb of the Atlantic meridional overturning circulation, which has been predicted to weaken as a consequence of climate change. The two main overflow branches pass the Denmark Strait and the Faroe Bank channel. Here we combine results from direct current <span class="hlt">measurements</span> in the Faroe Bank channel for 1995-2005 with an ensemble hindcast experiment for 1948-2005 using an ocean general circulation <span class="hlt">model</span>. For the overlapping period we find a convincing agreement between <span class="hlt">model</span> simulations and <span class="hlt">observations</span> on monthly to interannual timescales. Both <span class="hlt">observations</span> and <span class="hlt">model</span> data show no significant trend in volume transport. In addition, for the whole 1948-2005 period, the <span class="hlt">model</span> indicates no persistent trend in the Faroe Bank channel overflow or in the total overflow transport, in agreement with the few available historical <span class="hlt">observations</span>. Deepening isopycnals in the Norwegian Sea have tended to decrease the pressure difference across the Greenland-Scotland ridge, but this has been compensated for by the effect of changes in sea level. In contrast with earlier studies, we therefore conclude that the Faroe Bank channel overflow, and also the total overflow, did not decrease consistently from 1950 to 2005, although the <span class="hlt">model</span> does show a weakening total Atlantic meridional overturning circulation as a result of changes south of the Greenland-Scotland ridge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRD..119.8137K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRD..119.8137K"><span>Fogwater deposition <span class="hlt">modeling</span> for terrestrial ecosystems: A review of developments and <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Katata, Genki</p> <p>2014-07-01</p> <p>Recent progress in <span class="hlt">modeling</span> fogwater (and low cloud water) deposition over terrestrial ecosystems during fogwater droplet interception by vegetative surfaces is reviewed. Several types of <span class="hlt">models</span> and parameterizations for fogwater deposition are discussed with comparing assumptions, input parameter requirements, and <span class="hlt">modeled</span> processes. The relationships among deposition velocity of fogwater (Vd) in <span class="hlt">model</span> results, wind speed, and plant species structures associated with literature values are gathered for <span class="hlt">model</span> validation. Quantitative comparisons between <span class="hlt">model</span> results and <span class="hlt">observations</span> in forest environments revealed differences as large as 2 orders of magnitude, which are likely caused by uncertainties in <span class="hlt">measurement</span> techniques over heterogeneous landscapes. Results from the literature review show that Vd values ranged from 2.1 to 8.0 cm s-1 for short vegetation, whereas Vd = 7.7-92 cm s-1 and 0-20 cm s-1 for forests <span class="hlt">measured</span> by throughfall-based methods and the eddy covariance method, respectively. This review also discusses the current understanding of the impacts of fogwater deposition on atmosphere-land interactions and over complex terrain based on results from numerical studies. Lastly, future research priorities in innovative <span class="hlt">modeling</span> and <span class="hlt">observational</span> approaches for <span class="hlt">model</span> validation are outlined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMGC41A0785L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMGC41A0785L"><span>Analysis of precipitation teleconnections in CMIP <span class="hlt">models</span> as a <span class="hlt">measure</span> of <span class="hlt">model</span> fidelity in simulating precipitation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Langenbrunner, B.; Neelin, J.; Meyerson, J.</p> <p>2011-12-01</p> <p>The accurate representation of precipitation is a recurring issue in global climate <span class="hlt">models</span>, especially in the tropics. Poor skill in <span class="hlt">modeling</span> the variability and climate teleconnections associated with El Niño/Southern Oscillation (ENSO) also persisted in the latest Climate <span class="hlt">Model</span> Intercomparison Project (CMIP) campaigns. <span class="hlt">Observed</span> ENSO precipitation teleconnections provide a standard by which we can judge a given <span class="hlt">model</span>'s ability to reproduce precipitation and dynamic feedback processes originating in the tropical Pacific. Using CMIP3 Atmospheric <span class="hlt">Model</span> Intercomparison Project (AMIP) runs as a baseline, we compare precipitation teleconnections between <span class="hlt">models</span> and <span class="hlt">observations</span>, and we evaluate these results against available CMIP5 historical and AMIP runs. Using AMIP simulations restricts evaluation to the atmospheric response, as sea surface temperatures (SSTs) in AMIP are prescribed by <span class="hlt">observations</span>. We use a rank correlation between ENSO SST indices and precipitation to define teleconnections, since this method is robust to outliers and appropriate for non-Gaussian data. Spatial correlations of the <span class="hlt">modeled</span> and <span class="hlt">observed</span> teleconnections are then evaluated. We look at these correlations in regions of strong precipitation teleconnections, including equatorial S. America, the "horseshoe" region in the western tropical Pacific, and southern N. America. For each region and season, we create a "normalized projection" of a given <span class="hlt">model</span>'s teleconnection pattern onto that of the <span class="hlt">observations</span>, a metric that assesses the quality of regional pattern simulations while rewarding signals of correct sign over the region. Comparing this to an area-averaged (i.e., more generous) metric suggests <span class="hlt">models</span> do better when restrictions on exact spatial dependence are loosened and conservation constraints apply. <span class="hlt">Model</span> fidelity in regional <span class="hlt">measures</span> remains far from perfect, suggesting intrinsic issues with the <span class="hlt">models</span>' regional sensitivities in moist processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950009774','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950009774"><span>Mars Pathfinder meteorological <span class="hlt">observations</span> on the basis of results of an atmospheric global circulation <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Forget, Francois; Hourdin, F.; Talagrand, O.</p> <p>1994-01-01</p> <p>The Mars Pathfinder Meteorological Package (ASI/MET) will <span class="hlt">measure</span> the local pressure, temperature, and winds at its future landing site, somewhere between the latitudes 0 deg N and 30 deg N. Comparable <span class="hlt">measurements</span> have already been obtained at the surface of Mars by the Viking Landers at 22 deg N (VL1) and 48 deg N (VL2), providing much useful information on the martian atmosphere. In particular the pressure <span class="hlt">measurements</span> contain very instructive information on the global atmospheric circulation. At the Laboratoire de Meteorologie Dynamique (LMD), we have analyzed and simulated these <span class="hlt">measurements</span> with a martian atmospheric global circulation <span class="hlt">model</span> (GCM), which was the first to simulate the martian atmospheric circulation over more than 1 year. The <span class="hlt">model</span> is able to reproduce rather accurately many <span class="hlt">observed</span> features of the martian atmosphere, including the long- and short-period oscillations of the surface pressure <span class="hlt">observed</span> by the Viking landers. From a meteorological point of view, we think that a landing site located near or at the equator would be an interesting choice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A23D0270W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A23D0270W"><span>A Variational Inverse <span class="hlt">Model</span> Study of Amazonian Methane Emissions including <span class="hlt">Observations</span> from the AMAZONICA campaign</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilson, C. J.; Gloor, M.; Chipperfield, M.; Miller, J. B.; Gatti, L.</p> <p>2013-12-01</p> <p>Methane (CH4) is a greenhouse gas which is emitted from a range of anthropogenic and natural sources, and since the industrial revolution its mean atmospheric concentration has climbed dramatically, reaching values unprecedented in at least the past 650,000 years. CH4 produces a relatively high radiative forcing effect upon the Earth's climate, and its atmospheric lifetime of approximately 10 years makes it a more appealing target for the mitigation of climate change over short timescales than long-lived greenhouse gases such as carbon dioxide. However, the spatial and temporal variation of CH4 emissions are still not well understood, though in recent years a number of top-down and bottom-up studies have attempted to construct improved emission budgets. Some top-down studies may suffer from poor <span class="hlt">observational</span> coverage in tropical regions, however, especially in the planetary boundary layer, where the atmosphere is highly sensitive to emissions. For example, although satellite <span class="hlt">observations</span> often take a large volume of <span class="hlt">measurements</span> in tropical regions, these retrievals are not usually sensitive to concentrations at the planet's surface. Methane emissions from Amazon region, in particular, are often poorly constrained. Since emissions form this region, coming mainly from wetland and biomass burning sources, are thought to be relatively high, additional <span class="hlt">observations</span> in this region would greatly help to constrain the geographical distribution of the global CH4 emission budget. In order to provide such <span class="hlt">measurements</span>, the AMAZONICA project began to take regular flask <span class="hlt">measurements</span> of CH4 and other trace gases from aircraft over four Amazonian sites from the year 2010 onwards. We first present a forward <span class="hlt">modelling</span> study of these <span class="hlt">observations</span> of Amazonian methane for the year 2010 using the TOMCAT Chemical Transport <span class="hlt">Model</span>. The <span class="hlt">model</span> is used to attribute variations at each site to a source type and region, and also to assess the ability of our current CH4 flux estimates to</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhDT.......192W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhDT.......192W"><span>Cloud condensation nuclei in Western Colorado: <span class="hlt">Observations</span> and <span class="hlt">model</span> predictions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ward, Daniel Stewart</p> <p></p> <p>Variations in the warm cloud-active portion of atmospheric aerosols, or cloud condensation nuclei (CCN), have been shown to impact cloud droplet number concentration and subsequently cloud and precipitation processes. This issue carries special significance in western Colorado where a significant portion of the region's water resources is supplied by precipitation from winter season, orographic clouds, which are particularly sensitive to variations in CCN. Temporal and spatial variations in CCN in western Colorado were investigated using a combination of <span class="hlt">observations</span> and a new method for <span class="hlt">modeling</span> CCN. As part of the Inhibition of Snowfall by Pollution Aerosols (ISPA-III) field campaign, total particle and CCN number concentration were <span class="hlt">measured</span> for a 24-day period in Mesa Verde National Park, climatologically upwind of the San Juan Mountains. These data were combined with CCN <span class="hlt">observations</span> from Storm Peak Lab (SPL) in northwestern Colorado and from the King Air platform, flying north to south along the Western Slope. Altogether, the sampled aerosols were characteristic of a rural continental environment and the cloud-active portion varied slowly in time, and little in space. Estimates of the is hygroscopicity parameter indicated consistently low aerosol hygroscopicity typical of organic aerosol species. The <span class="hlt">modeling</span> approach included the addition of prognostic CCN to the Regional Atmospheric <span class="hlt">Modeling</span> System (RAMS). The RAMS droplet activation scheme was altered using parcel <span class="hlt">model</span> simulations to include variations in aerosol hygroscopicity, represented by K. Analysis of the parcel <span class="hlt">model</span> output and a supplemental sensitivity study showed that <span class="hlt">model</span> CCN will be sensitive to changes in aerosol hygroscopicity, but only for conditions of low supersaturation or small particle sizes. Aerosol number, size distribution median radius, and hygroscopicity (represented by the K parameter) in RAMS were constrained by nudging to forecasts of these quantities from the Weather</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMSM31B2291M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMSM31B2291M"><span>Experimental <span class="hlt">Observations</span> and Theoretical <span class="hlt">Modeling</span> of VLF Scattering During LEP Events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mitchell, M. F.; Moore, R. C.</p> <p>2012-12-01</p> <p>Recent experimental <span class="hlt">observations</span> of very low frequency (VLF) scattering during lightning-induced election precipitation (LEP) events are presented. A spread spectrum analysis technique is applied to these <span class="hlt">observations</span>, demonstrating a significant dependence on frequency. For LEP events, the scattered field amplitude and phase both exhibit strong frequency dependence, as do the event onset delays (relative to the causative lightning flash) and the event onset durations. The experimental <span class="hlt">observations</span> are compared with the predictions of an Earth-ionosphere waveguide propagation and scattering <span class="hlt">model</span>. The Long-Wave Propagation Capability (LWPC) code is used to demonstrate that the scattered field amplitude and phase depend sensitively on the electrical properties of the scattering body and the ionosphere between the scatterer and the receiver. The <span class="hlt">observed</span> frequency-dependent onset times and durations, on the other hand, are attributed to the scattering source characteristics. These <span class="hlt">measurements</span> can also be used to study radiation belt dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.2911K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.2911K"><span><span class="hlt">Model</span> Evaluation with Multi-wavelength Satellite <span class="hlt">Observations</span> Using a Neural Network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kolassa, Jana; Jimenez, Carlos; Aires, Filipe</p> <p>2013-04-01</p> <p> linked to the retrieved SM uncertainties. The proposed methodology can also be used to evaluate the quality of the <span class="hlt">model</span> forcings: two soil moisture fields from ORCHIDEE using WATCH (Weedon et al., 2011) and ERA-interim (Balsamo et al., 2010) forcings were analysed. It was shown that the WATCH forcing data are more optimal, underlining the importance of forcing data for the accuracy of <span class="hlt">model</span> predictions (Kolassa et al., in press, 2012). References Aires, F., Prigent, C., and Rossow, W.B. (2005), Sensitivity of satellite microwave and infrared <span class="hlt">observations</span> to soil moisture at a global scale: 2. Global statistical relationships, J. Geophys. Res., 110, D11103, doi:10.1029/2004JD005094. Aires, F., O. Aznay, C. Prigent, M. Paul, F. Bernardo, Synergetic multi-wavelegnth remote sensing versus a posteriori combination of retrieved products: Application for the retrieval of atmospheric profiles using MetOp <span class="hlt">measurements</span>, J. Geophys. Res., 2011 Balsamo, G., Viterbo, P., Beljaars, A., van den Hurk, B., Hirschi, M., Betts, A. and Scipa,l K. (2009) A Revised Hydrology for the ECMWF <span class="hlt">Model</span>: Verification from Field Site to Terrestrial Water Storage and Impact in the Integrated Forecast System, J. Hydrol., 10, 623-643 Balsamo, G., Boussetta, S., Lopez, P., and Ferranti, L. (2010), Evaluation of ERA-Interim and ERA- Interim-GPCP-rescaled precipitation over the U.S.A., ERA-Report Series, 5, pp. 10. Best, M. J., M. Pryor, D. B. Clark, G. G. Rooney, R .L. H. Essery, C. B. Ménard, J. M. Edwards, M. A. Hendry, A. Porson, N. Gedney, L. M. Mercado, S. Sitch, E. Blyth, O. Boucher, P. M. Cox, C. S. B. Grimmond, and R. J. Harding (2011), The Joint UK Land Environment Simulator (JULES), <span class="hlt">model</span> description - Part 1: Energy and water fluxes, Geosci. <span class="hlt">Model</span> Dev., 4 Jimenez, C., Clark, D., Kolassa, J., Aires, F., Prigent, C., and Blyth, E. (2012), A joint analysis of <span class="hlt">modeled</span> soil moisture fields and satellite <span class="hlt">observations</span> (2012), J. Geophys. Res., Kolassa, J., Aires, F., Polcher, J., Prigent, C., and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.4764L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.4764L"><span>Identification of AR(I)MA processes for <span class="hlt">modelling</span> temporal correlations of GPS <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luo, X.; Mayer, M.; Heck, B.</p> <p>2009-04-01</p> <p>In many geodetic applications <span class="hlt">observations</span> of the Global Positioning System (GPS) are routinely processed by means of the least-squares method. However, this algorithm delivers reliable estimates of unknown parameters und realistic accuracy <span class="hlt">measures</span> only if both the functional and stochastic <span class="hlt">models</span> are appropriately defined within GPS data processing. One deficiency of the stochastic <span class="hlt">model</span> used in many GPS software products consists in neglecting temporal correlations of GPS <span class="hlt">observations</span>. In practice the knowledge of the temporal stochastic behaviour of GPS <span class="hlt">observations</span> can be improved by analysing time series of residuals resulting from the least-squares evaluation. This paper presents an approach based on the theory of autoregressive (integrated) moving average (AR(I)MA) processes to <span class="hlt">model</span> temporal correlations of GPS <span class="hlt">observations</span> using time series of <span class="hlt">observation</span> residuals. A practicable integration of AR(I)MA <span class="hlt">models</span> in GPS data processing requires the determination of the order parameters of AR(I)MA processes at first. In case of GPS, the identification of AR(I)MA processes could be affected by various factors impacting GPS positioning results, e.g. baseline length, multipath effects, <span class="hlt">observation</span> weighting, or weather variations. The influences of these factors on AR(I)MA identification are empirically analysed based on a large amount of representative residual time series resulting from differential GPS post-processing using 1-Hz <span class="hlt">observation</span> data collected within the permanent SAPOS® (Satellite Positioning Service of the German State Survey) network. Both short and long time series are <span class="hlt">modelled</span> by means of AR(I)MA processes. The final order parameters are determined based on the whole residual database; the corresponding empirical distribution functions illustrate that multipath and weather variations seem to affect the identification of AR(I)MA processes much more significantly than baseline length and <span class="hlt">observation</span> weighting. Additionally, the <span class="hlt">modelling</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1913118M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1913118M"><span>Effect of citizen engagement levels in flood forecasting by assimilating crowdsourced <span class="hlt">observations</span> in hydrological <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mazzoleni, Maurizio; Cortes Arevalo, Juliette; Alfonso, Leonardo; Wehn, Uta; Norbiato, Daniele; Monego, Martina; Ferri, Michele; Solomatine, Dimitri</p> <p>2017-04-01</p> <p>In the past years, a number of methods have been proposed to reduce uncertainty in flood prediction by means of <span class="hlt">model</span> updating techniques. Traditional physical <span class="hlt">observations</span> are usually integrated into hydrological and hydraulic <span class="hlt">models</span> to improve <span class="hlt">model</span> performances and consequent flood predictions. Nowadays, low-cost sensors can be used for crowdsourced <span class="hlt">observations</span>. Different type of social sensors can <span class="hlt">measure</span>, in a more distributed way, physical variables such as precipitation and water level. However, these crowdsourced <span class="hlt">observations</span> are not integrated into a real-time fashion into water-system <span class="hlt">models</span> due to their varying accuracy and random spatial-temporal coverage. We assess the effect in <span class="hlt">model</span> performance due to the assimilation of crowdsourced <span class="hlt">observations</span> of water level. Our method consists in (1) implementing a Kalman filter into a cascade of hydrological and hydraulic <span class="hlt">models</span>. (2) defining <span class="hlt">observation</span> errors depending on the type of sensor either physical or social. Randomly distributed errors are based on accuracy ranges that slightly improve according to the citizens' expertise level. (3) Using a simplified social <span class="hlt">model</span> to realistically represent citizen engagement levels based on population density and citizens' motivation scenarios. To test our method, we synthetically derive crowdsourced <span class="hlt">observations</span> for different citizen engagement levels from a distributed network of physical and social sensors. The <span class="hlt">observations</span> are assimilated during a particular flood event occurred in the Bacchiglione catchment, Italy. The results of this study demonstrate that sharing crowdsourced water level <span class="hlt">observations</span> (often motivated by a feeling of belonging to a community of friends) can help in improving flood prediction. On the other hand, a growing participation of individual citizens or weather enthusiasts sharing hydrological <span class="hlt">observations</span> in cities can help to improve <span class="hlt">model</span> performance. This study is a first step to assess the effects of crowdsourced <span class="hlt">observations</span> in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1612113L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1612113L"><span>ODM2 (<span class="hlt">Observation</span> Data <span class="hlt">Model</span>): The EarthChem Use Case</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lehnert, Kerstin; Song, Lulin; Hsu, Leslie; Horsburgh, Jeffrey S.; Aufdenkampe, Anthony K.; Mayorga, Emilio; Tarboton, David; Zaslavsky, Ilya</p> <p>2014-05-01</p> <p>PetDB is an online data system that was created in the late 1990's to serve online a synthesis of published geochemical and petrological data of igneous and metamorphic rocks. PetDB has today reached a volume of 2.5 million analytical values for nearly 70,000 rock samples. PetDB's data <span class="hlt">model</span> (Lehnert et al., G-Cubed 2000) was designed to store sample-based <span class="hlt">observational</span> data generated by the analysis of rocks, together with a wide range of metadata documenting provenance of the samples, analytical procedures, data quality, and data source. Attempts to store additional types of geochemical data such as time-series data of seafloor hydrothermal springs and volcanic gases, depth-series data for marine sediments and soils, and mineral or mineral inclusion data revealed the limitations of the schema: the inability to properly record sample hierarchies (for example, a garnet that is included in a diamond that is included in a xenolith that is included in a kimberlite rock sample), inability to properly store time-series data, inability to accommodate classification schemes other than rock lithologies, deficiencies of identifying and documenting datasets that are not part of publications. In order to overcome these deficiencies, PetDB has been developing a new data schema using the ODM2 information <span class="hlt">model</span> (ODM=<span class="hlt">Observation</span> Data <span class="hlt">Model</span>). The development of ODM2 is a collaborative project that leverages the experience of several existing information representations, including PetDB and EarthChem, and the CUAHSI HIS <span class="hlt">Observations</span> Data <span class="hlt">Model</span> (ODM), as well as the general specification for encoding <span class="hlt">observational</span> data called <span class="hlt">Observations</span> and <span class="hlt">Measurements</span> (O&M) to develop a uniform information <span class="hlt">model</span> that seamlessly manages spatially discrete, feature-based earth <span class="hlt">observations</span> from environmental samples and sample fractions as well as in-situ sensors, and to test its initial implementation in a variety of user scenarios. The O&M <span class="hlt">model</span>, adopted as an international standard by the Open</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017BGeo...14.1419F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017BGeo...14.1419F"><span><span class="hlt">Observing</span> and <span class="hlt">modelling</span> phytoplankton community structure in the North Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ford, David A.; van der Molen, Johan; Hyder, Kieran; Bacon, John; Barciela, Rosa; Creach, Veronique; McEwan, Robert; Ruardij, Piet; Forster, Rodney</p> <p>2017-03-01</p> <p>Phytoplankton form the base of the marine food chain, and knowledge of phytoplankton community structure is fundamental when assessing marine biodiversity. Policy makers and other users require information on marine biodiversity and other aspects of the marine environment for the North Sea, a highly productive European shelf sea. This information must come from a combination of <span class="hlt">observations</span> and <span class="hlt">models</span>, but currently the coastal ocean is greatly under-sampled for phytoplankton data, and outputs of phytoplankton community structure from <span class="hlt">models</span> are therefore not yet frequently validated. This study presents a novel set of in situ <span class="hlt">observations</span> of phytoplankton community structure for the North Sea using accessory pigment analysis. The <span class="hlt">observations</span> allow a good understanding of the patterns of surface phytoplankton biomass and community structure in the North Sea for the <span class="hlt">observed</span> months of August 2010 and 2011. Two physical-biogeochemical ocean <span class="hlt">models</span>, the biogeochemical components of which are different variants of the widely used European Regional Seas Ecosystem <span class="hlt">Model</span> (ERSEM), were then validated against these and other <span class="hlt">observations</span>. Both <span class="hlt">models</span> were a good match for sea surface temperature <span class="hlt">observations</span>, and a reasonable match for remotely sensed ocean colour <span class="hlt">observations</span>. However, the two <span class="hlt">models</span> displayed very different phytoplankton community structures, with one better matching the in situ <span class="hlt">observations</span> than the other. Nonetheless, both <span class="hlt">models</span> shared some similarities with the <span class="hlt">observations</span> in terms of spatial features and inter-annual variability. An initial comparison of the formulations and parameterizations of the two <span class="hlt">models</span> suggests that diversity between the parameter settings of <span class="hlt">model</span> phytoplankton functional types, along with formulations which promote a greater sensitivity to changes in light and nutrients, is key to capturing the <span class="hlt">observed</span> phytoplankton community structure. These findings will help inform future <span class="hlt">model</span> development, which should be coupled</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960008865','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960008865"><span>ATLAS-3 correlative <span class="hlt">measurement</span> opportunities with UARS and surface <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harrison, Edwin F.; Denn, Fred M.; Gibson, Gary G.</p> <p>1995-01-01</p> <p>The third ATmospheric Laboratory for Applications and Science (ATLAS-3) mission was flown aboard the Space Shuttle launched on November 3, 1994. The mission length was approximately 10 days and 22 hours. The ATLAS-3 Earth-viewing instruments provided a large number of <span class="hlt">measurements</span> which were nearly coincident with <span class="hlt">observations</span> from experiments on the Upper Atmosphere Research Satellite (UARS). Based on ATLAS-3 instrument operating schedules, simulations were performed to determine when and where correlative <span class="hlt">measurements</span> occurred between ATLAS and UARS instruments, and between ATLAS and surface <span class="hlt">observations</span>. Results of these orbital and instrument simulations provide valuable information for scientists to compare <span class="hlt">measurements</span> between various instruments on the two satellites and at selected surface sites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654239-gravitational-wave-observations-may-constrain-gamma-ray-burst-models-case-gw150914gbm','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654239-gravitational-wave-observations-may-constrain-gamma-ray-burst-models-case-gw150914gbm"><span>GRAVITATIONAL-WAVE <span class="hlt">OBSERVATIONS</span> MAY CONSTRAIN GAMMA-RAY BURST <span class="hlt">MODELS</span>: THE CASE OF GW150914–GBM</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Veres, P.; Preece, R. D.; Goldstein, A.</p> <p></p> <p>The possible short gamma-ray burst (GRB) <span class="hlt">observed</span> by Fermi /GBM in coincidence with the first gravitational-wave (GW) detection offers new ways to test GRB prompt emission <span class="hlt">models</span>. GW <span class="hlt">observations</span> provide previously inaccessible physical parameters for the black hole central engine such as its horizon radius and rotation parameter. Using a minimum jet launching radius from the Advanced LIGO <span class="hlt">measurement</span> of GW 150914, we calculate photospheric and internal shock <span class="hlt">models</span> and find that they are marginally inconsistent with the GBM data, but cannot be definitely ruled out. Dissipative photosphere <span class="hlt">models</span>, however, have no problem explaining the <span class="hlt">observations</span>. Based on the peakmore » energy and the <span class="hlt">observed</span> flux, we find that the external shock <span class="hlt">model</span> gives a natural explanation, suggesting a low interstellar density (∼10{sup −3} cm{sup −3}) and a high Lorentz factor (∼2000). We only speculate on the exact nature of the system producing the gamma-rays, and study the parameter space of a generic Blandford–Znajek <span class="hlt">model</span>. If future joint <span class="hlt">observations</span> confirm the GW–short-GRB association we can provide similar but more detailed tests for prompt emission <span class="hlt">models</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.B24B..06F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.B24B..06F"><span>Informing Carbon Dynamics in the Community Land <span class="hlt">Model</span> with <span class="hlt">Observations</span> from Across Timescales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fox, A. M.; Hoar, T. J.</p> <p>2014-12-01</p> <p>Correct simulation of carbon dynamics in Earth System <span class="hlt">Models</span> is required to accurately predict both short and long-term land carbon-cycle climate and concentration feedbacks. As new <span class="hlt">model</span> structures and parameterizations of increasing complexity are introduced there is an ever present need for data to inform these developments, either indirectly through benchmarking activities, or directly through <span class="hlt">model</span>-data fusion techniques. Here we briefly describe a very rich source of data that will come from the National Ecological Observatory Network (NEON), a continental-scale facility that will collect freely available biogeochemical and biophysical data from 60 sites representative of a full range of ecosystems across the USA over 30 years. Relevant data at each site include a full suite of micrometeorology <span class="hlt">measurements</span>, profiles of CO2 and H2O vapor isotopes, soil temperature, moisture and CO2 flux, fine root images, and plot-based NPP, leaf area and litterfall estimates. This is accompanied by Lidar and hyperspectral derived biomass, leaf area and canopy chemistry at < 1m resolution of 100s km2. Critically, these <span class="hlt">observations</span> are well calibrated and highly standardized across sites allowing comparisons, whilst plot and site selection has been designed to optimize representativeness and spatial scaling opportunities. To illustrate the potential utility of these data in constraining <span class="hlt">models</span>, we show the range of Community Land <span class="hlt">Model</span> (CLM) output at NEON site locations, and in <span class="hlt">model</span>-space look at a number of different functional responses that characterize the <span class="hlt">model</span> in space and time and could be tested with data. These <span class="hlt">observations</span> can be used most directly through a data assimilation (DA) system and we demonstrate how we have developed support for CLM within the Data Assimilation Research Testbed (DART) that uses ensemble techniques for state estimation. Using an <span class="hlt">observing</span> system experiment, we investigate how infrequent <span class="hlt">observations</span> of carbon stocks constrain <span class="hlt">model</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050180617','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050180617"><span>Comparison of Histograms for Use in Cloud <span class="hlt">Observation</span> and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Green, Lisa; Xu, Kuan-Man</p> <p>2005-01-01</p> <p>Cloud <span class="hlt">observation</span> and cloud <span class="hlt">modeling</span> data can be presented in histograms for each characteristic to be <span class="hlt">measured</span>. Combining information from single-cloud histograms yields a summary histogram. Summary histograms can be compared to each other to reach conclusions about the behavior of an ensemble of clouds in different places at different times or about the accuracy of a particular cloud <span class="hlt">model</span>. As in any scientific comparison, it is necessary to decide whether any apparent differences are statistically significant. The usual methods of deciding statistical significance when comparing histograms do not apply in this case because they assume independent data. Thus, a new method is necessary. The proposed method uses the Euclidean distance metric and bootstrapping to calculate the significance level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.1346W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.1346W"><span>Low degree Earth's gravity coefficients determined from different space geodetic <span class="hlt">observations</span> and climate <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wińska, Małgorzata; Nastula, Jolanta</p> <p>2017-04-01</p> <p>Large scale mass redistribution and its transport within the Earth system causes changes in the Earth's rotation in space, gravity field and Earth's ellipsoid shape. These changes are <span class="hlt">observed</span> in the ΔC21, ΔS21, and ΔC20 spherical harmonics gravity coefficients, which are proportional to the mass load-induced Earth rotational excitations. In this study, linear trend, decadal, inter-annual, and seasonal variations of low degree spherical harmonics coefficients of Earth's gravity field, determined from different space geodetic techniques, Gravity Recovery and Climate Experiment (GRACE), satellite laser ranging (SLR), Global Navigation Satellite System (GNSS), Earth rotation, and climate <span class="hlt">models</span>, are examined. In this way, the contribution of each <span class="hlt">measurement</span> technique to interpreting the low degree surface mass density of the Earth is shown. Especially, we evaluate an usefulness of several climate <span class="hlt">models</span> from the Coupled <span class="hlt">Model</span> Intercomparison Project phase 5 (CMIP5) to determine the low degree Earth's gravity coefficients using GRACE satellite <span class="hlt">observations</span>. To do that, Terrestrial Water Storage (TWS) changes from several CMIP5 climate <span class="hlt">models</span> are determined and then these simulated data are compared with the GRACE <span class="hlt">observations</span>. Spherical harmonics ΔC21, ΔS21, and ΔC20 changes are calculated as the sum of atmosphere and ocean mass effect (GAC values) taken from GRACE and a land surface hydrological estimate from the selected CMIP5 climate <span class="hlt">models</span>. Low degree Stokes coefficients of the surface mass density determined from GRACE, SLR, GNSS, Earth rotation <span class="hlt">measurements</span> and climate <span class="hlt">models</span> are compared to each other in order to assess their consistency. The comparison is done by using different types of statistical and signal processing methods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21067783','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21067783"><span>SAR <span class="hlt">observation</span> and <span class="hlt">model</span> tracking of an oil spill event in coastal waters.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cheng, Yongcun; Li, Xiaofeng; Xu, Qing; Garcia-Pineda, Oscar; Andersen, Ole Baltazar; Pichel, William G</p> <p>2011-02-01</p> <p>Oil spills are a major contributor to marine pollution. The objective of this work is to simulate the oil spill trajectory of oil released from a pipeline leaking in the Gulf of Mexico with the GNOME (General NOAA Operational <span class="hlt">Modeling</span> Environment) <span class="hlt">model</span>. The <span class="hlt">model</span> was developed by NOAA (National Oceanic and Atmospheric Administration) to investigate the effects of different pollutants and environmental conditions on trajectory results. Also, a Texture-Classifying Neural Network Algorithm (TCNNA) was used to delineate ocean oil slicks from synthetic aperture radar (SAR) <span class="hlt">observations</span>. During the simulation, ocean currents from NCOM (Navy Coastal Ocean <span class="hlt">Model</span>) outputs and surface wind data <span class="hlt">measured</span> by an NDBC (National Data Buoy Center) buoy are used to drive the GNOME <span class="hlt">model</span>. The results show good agreement between the simulated trajectory of the oil spill and synchronous <span class="hlt">observations</span> from the European ENVISAT ASAR (Advanced Synthetic Aperture Radar) and the Japanese ALOS (Advanced Land <span class="hlt">Observing</span> Satellite) PALSAR (Phased Array L-band Synthetic Aperture Radar) images. Based on experience with past marine oil spills, about 63.0% of the oil will float and 18.5% of the oil will evaporate and disperse. In addition, the effects from uncertainty of ocean currents and the diffusion coefficient on the trajectory results are also studied. Copyright © 2010 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRA..121..589A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRA..121..589A"><span><span class="hlt">Observations</span> and <span class="hlt">modeling</span> of the ionospheric gravity and diamagnetic current systems from CHAMP and Swarm <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alken, P.</p> <p>2016-01-01</p> <p>The CHAMP and Swarm satellites, which provide high-quality magnetic field <span class="hlt">measurements</span> in low-altitude polar orbits, are ideally suited for investigating ionospheric current systems. In this study, we focus on the F region low-latitude gravity and diamagnetic currents which are prominent in the equatorial ionization anomaly (EIA) region in the North and South Hemisphere. During its 10 year mission, CHAMP has sampled nearly the entire altitude range of the EIA, offering the opportunity to study these currents from above, inside, and below their source region. The Swarm constellation offers the unique opportunity to study near-simultaneous <span class="hlt">measurements</span> of the current systems at different longitudinal separations. In this study, we present new <span class="hlt">observations</span> of these current systems, investigate their seasonal and local time dependence, investigate the use of in situ electron density <span class="hlt">measurements</span> as a proxy for the magnetic perturbations, and compute the longitudinal self correlation of these currents. We find that these currents are strongest during spring and fall, produce nighttime magnetic fields at satellite altitude of up to 5-7 nT during solar maximum, 2-3 nT during solar minimum, and are highly correlated with in situ electron density <span class="hlt">measurements</span>. We also find these currents are self-correlated above 70% up to 15° longitude in both hemispheres during the evening.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGC13H..03F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGC13H..03F"><span><span class="hlt">Observed</span> heavy precipitation increase confirms theory and early <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fischer, E. M.; Knutti, R.</p> <p>2016-12-01</p> <p>Environmental phenomena are often first <span class="hlt">observed</span>, and then explained or simulated quantitatively. The complexity and diversity of processes, the range of scales involved, and the lack of first principles to describe many processes make it challenging to predict conditions beyond the ones <span class="hlt">observed</span>. Here we use the intensification of heavy precipitation as a counterexample, where seemingly complex and potentially computationally intractable processes to first order manifest themselves in simple ways: the intensification of heavy precipitation is now emerging in the <span class="hlt">observed</span> record across many regions of the world, confirming both theory and a variety of <span class="hlt">model</span> predictions made decades ago, before robust evidence arose from <span class="hlt">observations</span>. We here compare heavy precipitation changes over Europe and the contiguous United States across station series and gridded <span class="hlt">observations</span>, theoretical considerations and multi-<span class="hlt">model</span> ensembles of GCMs and RCMs. We demonstrate that the <span class="hlt">observed</span> heavy precipitation intensification aggregated over large areas agrees remarkably well with Clausius-Clapeyron scaling. The <span class="hlt">observed</span> changes in heavy precipitation are consistent yet somewhat larger than predicted by very coarse resolution GCMs in the 1980s and simulated by the newest generation of GCMs and RCMs. For instance the number of days with very heavy precipitation over Europe has increased by about 45% in <span class="hlt">observations</span> (years 1981-2013 compared to 1951-1980) and by about 25% in the <span class="hlt">model</span> average in both GCMs and RCMs, although with substantial spread across <span class="hlt">models</span> and locations. As the anthropogenic climate signal strengthens, there will be more opportunities to test climate predictions for other variables against <span class="hlt">observations</span> and across a hierarchy of different <span class="hlt">models</span> and theoretical concepts. *Fischer, E.M., and R. Knutti, 2016, <span class="hlt">Observed</span> heavy precipitation increase confirms theory and early <span class="hlt">models</span>, Nature Climate Change, in press.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NJPh...18j3045S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NJPh...18j3045S"><span><span class="hlt">Observation</span> of non-classical correlations in sequential <span class="hlt">measurements</span> of photon polarization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suzuki, Yutaro; Iinuma, Masataka; Hofmann, Holger F.</p> <p>2016-10-01</p> <p>A sequential <span class="hlt">measurement</span> of two non-commuting quantum <span class="hlt">observables</span> results in a joint probability distribution for all output combinations that can be explained in terms of an initial joint quasi-probability of the non-commuting <span class="hlt">observables</span>, modified by the resolution errors and back-action of the initial <span class="hlt">measurement</span>. Here, we show that the error statistics of a sequential <span class="hlt">measurement</span> of photon polarization performed at different <span class="hlt">measurement</span> strengths can be described consistently by an imaginary correlation between the statistics of resolution and back-action. The experimental setup was designed to realize variable strength <span class="hlt">measurements</span> with well-controlled imaginary correlation between the statistical errors caused by the initial <span class="hlt">measurement</span> of diagonal polarizations, followed by a precise <span class="hlt">measurement</span> of the horizontal/vertical polarization. We perform the experimental characterization of an elliptically polarized input state and show that the same complex joint probability distribution is obtained at any <span class="hlt">measurement</span> strength.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRD..119.5719P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRD..119.5719P"><span>Long-term changes in lower tropospheric baseline ozone concentrations: Comparing chemistry-climate <span class="hlt">models</span> and <span class="hlt">observations</span> at northern midlatitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Parrish, D. D.; Lamarque, J.-F.; Naik, V.; Horowitz, L.; Shindell, D. T.; Staehelin, J.; Derwent, R.; Cooper, O. R.; Tanimoto, H.; Volz-Thomas, A.; Gilge, S.; Scheel, H.-E.; Steinbacher, M.; Fröhlich, M.</p> <p>2014-05-01</p> <p>Two recent papers have quantified long-term ozone (O3) changes <span class="hlt">observed</span> at northern midlatitude sites that are believed to represent baseline (here understood as representative of continental to hemispheric scales) conditions. Three chemistry-climate <span class="hlt">models</span> (NCAR CAM-chem, GFDL-CM3, and GISS-E2-R) have calculated retrospective tropospheric O3 concentrations as part of the Atmospheric Chemistry and Climate <span class="hlt">Model</span> Intercomparison Project and Coupled <span class="hlt">Model</span> Intercomparison Project Phase 5 <span class="hlt">model</span> intercomparisons. We present an approach for quantitative comparisons of <span class="hlt">model</span> results with <span class="hlt">measurements</span> for seasonally averaged O3 concentrations. There is considerable qualitative agreement between the <span class="hlt">measurements</span> and the <span class="hlt">models</span>, but there are also substantial and consistent quantitative disagreements. Most notably, <span class="hlt">models</span> (1) overestimate absolute O3 mixing ratios, on average by 5 to 17 ppbv in the year 2000, (2) capture only 50% of O3 changes <span class="hlt">observed</span> over the past five to six decades, and little of <span class="hlt">observed</span> seasonal differences, and (3) capture 25 to 45% of the rate of change of the long-term changes. These disagreements are significant enough to indicate that only limited confidence can be placed on estimates of present-day radiative forcing of tropospheric O3 derived from <span class="hlt">modeled</span> historic concentration changes and on predicted future O3 concentrations. Evidently our understanding of tropospheric O3, or the incorporation of chemistry and transport processes into current chemical climate <span class="hlt">models</span>, is incomplete. <span class="hlt">Modeled</span> O3 trends approximately parallel estimated trends in anthropogenic emissions of NOx, an important O3 precursor, while <span class="hlt">measured</span> O3 changes increase more rapidly than these emission estimates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A21A2136N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A21A2136N"><span>Estimating vertical profiles of water-cloud droplet effective radius from SWIR satellite <span class="hlt">measurements</span> via a statistical <span class="hlt">model</span> derived from CloudSat <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagao, T. M.; Murakami, H.; Nakajima, T. Y.</p> <p>2017-12-01</p> <p>This study proposes an algorithm to estimate vertical profiles of cloud droplet effective radius (CDER-VP) for water clouds from shortwave infrared (SWIR) <span class="hlt">measurements</span> of Himawari-8/AHI via a statistical <span class="hlt">model</span> of CDER-VP derived from CloudSat <span class="hlt">observation</span>. Several similar algorithms in previous studies utilize a spectral radiance matching on the assumption of simultaneous <span class="hlt">observations</span> of CloudSat and Aqua/MODIS. However, our algorithm does not assume simultaneous <span class="hlt">observations</span> with CloudSat. First, in advance, a database (DB) of CDER-VP is prepared by the following procedure: TOA radiances at 0.65, 2.3 and 10.4-μm bands of the AHI are simulated using CDER-VP and cloud optical depth vertical profile (COD-VP) contained in the CloudSat 2B-CWC-RVOD and 2B-TAU products. Cloud optical thickness (COT), Column-CDER and cloud top height (CTH) are retrieved from the simulated radiances using a traditional retrieval algorithm with vertically homogeneous cloud <span class="hlt">model</span> (1-SWIR VHC method). The CDER-VP is added to the DB by using the COT and Column-CDER retrievals as a key of the DB. Then by using principal component (PC) analysis, up to three PC vectors of the CDER-VPs in the DB are extracted. Next, the algorithm retrieves CDER-VP from actual AHI <span class="hlt">measurements</span> by the following procedure: First, COT, Column-CDER and CTH are retrieved from TOA radiances at 0.65, 2.3 and 10.4-μm bands of the AHI using by 1-SWIR VHC method. Then, the PC vectors of CDER-VP is fetched from the DB using the COT and Column-CDER retrievals as the key of the DB. Finally, using coefficients of the PC vectors of CDER-VP as variables for retrieval, CDER-VP, COT and CTH are retrieved from TOA radiances at 0.65, 1.6, 2.3, 3.9 and 10.4-μm bands of the AHI based on optimal estimation method with iterative radiative transfer calculation. The simulation result showed the CDER-VP retrieval errors were almost smaller than 3 - 4 μm. The CDER retrieval errors at the cloud base were almost larger than the others (e</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990111727&hterms=hack&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dhack','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990111727&hterms=hack&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dhack"><span>Absorption of Solar Radiation by Clouds: <span class="hlt">Observations</span> Versus <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cess, R. D.; Zhang, M. H.; Minnis, P.; Corsetti, L.; Dutton, E. G.; Forgan, B. W.; Garber, D. P.; Gates, W. L.; Hack, J. J.; Harrison, E. F.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_19990111727'); toggleEditAbsImage('author_19990111727_show'); toggleEditAbsImage('author_19990111727_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_19990111727_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_19990111727_hide"></p> <p>1995-01-01</p> <p>There has been a long history of unexplained anomalous absorption of solar radiation by clouds. Collocated satellite and surface <span class="hlt">measurements</span> of solar radiation at five geographically diverse locations showed significant solar absorption by clouds, resulting in about 25 watts per square meter more global-mean absorption by the cloudy atmosphere than predicted by theoretical <span class="hlt">models</span>. It has often been suggested that tropospheric aerosols could increase cloud absorption. But these aerosols are temporally and spatially heterogeneous, whereas the <span class="hlt">observed</span> cloud absorption is remarkably invariant with respect to season and location. Although its physical cause is unknown, enhanced cloud absorption substantially alters our understanding of the atmosphere's energy budget.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870000256&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsonar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870000256&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsonar"><span>Mathematical <span class="hlt">Models</span> for Doppler <span class="hlt">Measurements</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lear, William M.</p> <p>1987-01-01</p> <p>Error analysis increases precision of navigation. Report presents improved mathematical <span class="hlt">models</span> of analysis of Doppler <span class="hlt">measurements</span> and <span class="hlt">measurement</span> errors of spacecraft navigation. To take advantage of potential navigational accuracy of Doppler <span class="hlt">measurements</span>, precise equations relate <span class="hlt">measured</span> cycle count to position and velocity. Drifts and random variations in transmitter and receiver oscillator frequencies taken into account. Mathematical <span class="hlt">models</span> also adapted to aircraft navigation, radar, sonar, lidar, and interferometry.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED567240.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED567240.pdf"><span>Latent Class <span class="hlt">Models</span> for Teacher <span class="hlt">Observation</span> Data</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Halpin, Peter F.</p> <p>2016-01-01</p> <p>Recent research on multiple <span class="hlt">measures</span> of teaching effectiveness has redefined the role of in-classroom <span class="hlt">observations</span> in teacher evaluation systems. In particular, most states now mandate that teachers are <span class="hlt">observed</span> on multiple occasions during the school year, and it is increasingly common that multiple raters are utilized across the different rating…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080045496&hterms=Qbo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DQbo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080045496&hterms=Qbo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DQbo"><span><span class="hlt">Modeling</span> the <span class="hlt">Observed</span> QBO and Inter-Annual Variations of the Diurnal Tide in the Mesosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mayr, Hans G.; Mengel, John G.; Huang, F. T.</p> <p>2006-01-01</p> <p>In the current version of the Numerical Spectral <span class="hlt">Model</span> (NSM), the Quasi-biennial Oscillation (QBO) is generated primarily by small-scale gravity waves (GW) from Hines' Doppler Spread Parameterization (DSP). The <span class="hlt">model</span> does not have topography, and the planetary waves are solely generated by instabilities. We discuss a 3D <span class="hlt">modeling</span> study that describes the QBO extending from the stratosphere into the upper mesosphere, where the oscillation produces significant inter-annual variations in the diurnal tide. The numerical results are compared with temperature <span class="hlt">measurements</span> from the SABER (TIMED) and MLS (UARS) instruments obtained by Huang et al. (2006). With a GW source that peaks at the Equator and is taken to be isotropic and independent of season, the NSM generates a QBO with variable periods around 26 months and zonal wind amplitudes of almost 25 m/s at 30 km. As reported earlier, the NSM reproduces the <span class="hlt">observed</span> equinoctial maxima in the diurnal tide at altitudes around 95 km. The <span class="hlt">modeled</span> QBO modulates the tide such that the seasonal amplitude maxima can vary from one year to another by as much as 30%. To shed light on the underlying mechanisms, the relative importance of the advection terms are discussed, and they are shown to be important in the stratosphere. At altitudes above 80 km, however, the QBO-related inter-annual variations of the tide are generated primarily by GW momentum deposition. In qualitative agreement with the SABER <span class="hlt">measurements</span>, the <span class="hlt">model</span> generates distinct zonal-mean QBO temperature variations in the stratosphere and mesosphere. In the stratosphere, the computed amplitudes are not much smaller than those <span class="hlt">observed</span>, and the rate of downward propagation at the Equator is reproduced. The <span class="hlt">modeled</span> temperature amplitudes in the mesosphere, however, are much smaller than those <span class="hlt">observed</span>. The <span class="hlt">observed</span> and computed temperature variations of the QBO peak at the Equator but extend with phase reversals to high latitudes, in contrast to the zonal winds that are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ESD.....9..593B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ESD.....9..593B"><span>Steering operational synergies in terrestrial <span class="hlt">observation</span> networks: opportunity for advancing Earth system dynamics <span class="hlt">modelling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baatz, Roland; Sullivan, Pamela L.; Li, Li; Weintraub, Samantha R.; Loescher, Henry W.; Mirtl, Michael; Groffman, Peter M.; Wall, Diana H.; Young, Michael; White, Tim; Wen, Hang; Zacharias, Steffen; Kühn, Ingolf; Tang, Jianwu; Gaillardet, Jérôme; Braud, Isabelle; Flores, Alejandro N.; Kumar, Praveen; Lin, Henry; Ghezzehei, Teamrat; Jones, Julia; Gholz, Henry L.; Vereecken, Harry; Van Looy, Kris</p> <p>2018-05-01</p> <p>Advancing our understanding of Earth system dynamics (ESD) depends on the development of <span class="hlt">models</span> and other analytical tools that apply physical, biological, and chemical data. This ambition to increase understanding and develop <span class="hlt">models</span> of ESD based on site <span class="hlt">observations</span> was the stimulus for creating the networks of Long-Term Ecological Research (LTER), Critical Zone Observatories (CZOs), and others. We organized a survey, the results of which identified pressing gaps in data availability from these networks, in particular for the future development and evaluation of <span class="hlt">models</span> that represent ESD processes, and provide insights for improvement in both data collection and <span class="hlt">model</span> integration. From this survey overview of data applications in the context of LTER and CZO research, we identified three challenges: (1) widen application of terrestrial <span class="hlt">observation</span> network data in Earth system <span class="hlt">modelling</span>, (2) develop integrated Earth system <span class="hlt">models</span> that incorporate process representation and data of multiple disciplines, and (3) identify complementarity in <span class="hlt">measured</span> variables and spatial extent, and promoting synergies in the existing <span class="hlt">observational</span> networks. These challenges lead to perspectives and recommendations for an improved dialogue between the <span class="hlt">observation</span> networks and the ESD <span class="hlt">modelling</span> community, including co-location of sites in the existing networks and further formalizing these recommendations among these communities. Developing these synergies will enable cross-site and cross-network comparison and synthesis studies, which will help produce insights around organizing principles, classifications, and general rules of coupling processes with environmental conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA33B..05G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA33B..05G"><span>Anticipated <span class="hlt">Observation</span> of Waves and Tides by the GOLD Mission Using a GCM and GLOW <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Greer, K.; Solomon, S. C.; Rusch, D. W.</p> <p>2017-12-01</p> <p>One of the major scientific objectives of the GOLD mission is to address the significance of atmospheric waves and tides propagating from below on the thermospheric temperature structure. Here we examine the modes of tides and spectrum of waves that will be <span class="hlt">observed</span> by GOLD in geostationary orbit. The GOLD instrument is an imaging spectrograph that will <span class="hlt">measure</span> the Earth's emissions from 132 to 162 nm. These <span class="hlt">measurements</span> will be used to image thermospheric temperature and composition near 160 km on the dayside disk at half-hour time scales. TIE-GCM is used to produce a realistic <span class="hlt">model</span> atmosphere, where different wave and tidal components can be easily extracted, and GLobal AirglOW (GLOW) <span class="hlt">model</span> produces the emissions in the spectral bands <span class="hlt">observed</span> by GOLD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=teacher+AND+observation&pg=5&id=EJ1134283','ERIC'); return false;" href="https://eric.ed.gov/?q=teacher+AND+observation&pg=5&id=EJ1134283"><span>Validating an <span class="hlt">Observation</span> Protocol to <span class="hlt">Measure</span> Special Education Teacher Effectiveness</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Johnson, Evelyn S.; Semmelroth, Carrie L.</p> <p>2015-01-01</p> <p>This study used Kane's (2013) Interpretation/Use Argument (IUA) to <span class="hlt">measure</span> validity on the Recognizing Effective Special Education Teachers (RESET) <span class="hlt">observation</span> tool. The RESET <span class="hlt">observation</span> tool is designed to evaluate special education teacher effectiveness using evidence-based instructional practices as the basis for evaluation. In alignment with…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29057596','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29057596"><span>The Anaclitic-Introjective Depression Assessment: Development and preliminary validity of an <span class="hlt">observer</span>-rated <span class="hlt">measure</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rost, Felicitas; Luyten, Patrick; Fonagy, Peter</p> <p>2018-03-01</p> <p>The two-configurations <span class="hlt">model</span> developed by Blatt and colleagues offers a comprehensive conceptual and empirical framework for understanding depression. This <span class="hlt">model</span> suggests that depressed patients struggle, at different developmental levels, with issues related to dependency (anaclitic issues) or self-definition (introjective issues), or a combination of both. This paper reports three studies on the development and preliminary validation of the Anaclitic-Introjective Depression Assessment, an <span class="hlt">observer</span>-rated assessment tool of impairments in relatedness and self-definition in clinical depression based on the item pool of the Shedler-Westen Assessment Procedure. Study 1 describes the development of the <span class="hlt">measure</span> using expert consensus rating and Q-methodology. Studies 2 and 3 report the assessment of its psychometric properties, preliminary reliability, and validity in a sample of 128 patients diagnosed with treatment-resistant depression. Four naturally occurring clusters of depressed patients were identified using Q-factor analysis, which, overall, showed meaningful and theoretically expected relationships with anaclitic/introjective prototypes as formulated by experts, as well as with clinical, social, occupational, global, and relational functioning. Taken together, findings reported in this paper provide preliminary evidence for the reliability and validity of the Anaclitic-Introjective Depression Assessment, an <span class="hlt">observer</span>-rated <span class="hlt">measure</span> that allows the detection of important nuanced differentiations between and within anaclitic and introjective depression. Copyright © 2017 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IJMPA..3046004K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IJMPA..3046004K"><span><span class="hlt">Measurements</span> of jet-related <span class="hlt">observables</span> at the LHC</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kokkas, P.</p> <p>2015-11-01</p> <p>During the first years of the LHC operation a large amount of jet data was recorded by the ATLAS and CMS experiments. In this review several <span class="hlt">measurements</span> of jet-related <span class="hlt">observables</span> are presented, such as multi-jet rates and cross sections, ratios of jet cross sections, jet shapes and event shape <span class="hlt">observables</span>. All results presented here are based on jet data collected at a centre-of-mass energy of 7 TeV. Data are compared to various Monte Carlo generators, as well as to theoretical next-to-leading-order calculations allowing a test of perturbative Quantum Chromodynamics in a previously unexplored energy region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1394462','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1394462"><span>Virtual <span class="hlt">Observation</span> System for Earth System <span class="hlt">Model</span>: An Application to ACME Land <span class="hlt">Model</span> Simulations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Wang, Dali; Yuan, Fengming; Hernandez, Benjamin</p> <p></p> <p>Investigating and evaluating physical-chemical-biological processes within an Earth system <span class="hlt">model</span> (EMS) can be very challenging due to the complexity of both <span class="hlt">model</span> design and software implementation. A virtual <span class="hlt">observation</span> system (VOS) is presented to enable interactive <span class="hlt">observation</span> of these processes during system simulation. Based on advance computing technologies, such as compiler-based software analysis, automatic code instrumentation, and high-performance data transport, the VOS provides run-time <span class="hlt">observation</span> capability, in-situ data analytics for Earth system <span class="hlt">model</span> simulation, <span class="hlt">model</span> behavior adjustment opportunities through simulation steering. A VOS for a terrestrial land <span class="hlt">model</span> simulation within the Accelerated Climate <span class="hlt">Modeling</span> for Energy <span class="hlt">model</span> is also presentedmore » to demonstrate the implementation details and system innovations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1394462-virtual-observation-system-earth-system-model-application-acme-land-model-simulations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1394462-virtual-observation-system-earth-system-model-application-acme-land-model-simulations"><span>Virtual <span class="hlt">Observation</span> System for Earth System <span class="hlt">Model</span>: An Application to ACME Land <span class="hlt">Model</span> Simulations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wang, Dali; Yuan, Fengming; Hernandez, Benjamin; ...</p> <p>2017-01-01</p> <p>Investigating and evaluating physical-chemical-biological processes within an Earth system <span class="hlt">model</span> (EMS) can be very challenging due to the complexity of both <span class="hlt">model</span> design and software implementation. A virtual <span class="hlt">observation</span> system (VOS) is presented to enable interactive <span class="hlt">observation</span> of these processes during system simulation. Based on advance computing technologies, such as compiler-based software analysis, automatic code instrumentation, and high-performance data transport, the VOS provides run-time <span class="hlt">observation</span> capability, in-situ data analytics for Earth system <span class="hlt">model</span> simulation, <span class="hlt">model</span> behavior adjustment opportunities through simulation steering. A VOS for a terrestrial land <span class="hlt">model</span> simulation within the Accelerated Climate <span class="hlt">Modeling</span> for Energy <span class="hlt">model</span> is also presentedmore » to demonstrate the implementation details and system innovations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..12213495H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..12213495H"><span>Constraints on Meteoric Smoke Composition and Meteoric Influx Using SOFIE <span class="hlt">Observations</span> With <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hervig, Mark E.; Brooke, James S. A.; Feng, Wuhu; Bardeen, Charles G.; Plane, John M. C.</p> <p>2017-12-01</p> <p>The composition of meteoric smoke particles in the mesosphere is constrained using <span class="hlt">measurements</span> from the Solar Occultation For Ice Experiment (SOFIE) in conjunction with <span class="hlt">models</span>. Comparing the multiwavelength <span class="hlt">observations</span> with <span class="hlt">models</span> suggests smoke compositions of magnetite, wüstite, magnesiowüstite, or iron-rich olivine. Smoke compositions of pure pyroxene, hematite, iron-poor olivine, magnesium silicate, and silica are excluded, although this may be because these materials have weak signatures at the SOFIE wavelengths. Information concerning smoke composition allows the SOFIE extinction <span class="hlt">measurements</span> to be converted to smoke volume density. Comparing the <span class="hlt">observed</span> volume density with <span class="hlt">model</span> results for varying meteoric influx (MI) provides constraints on the ablated fraction of incoming meteoric material. The results indicate a global ablated MI of 3.3 ± 1.9 t d-1, which represents only iron, magnesium, and possibly silica, given the smoke compositions indicated here. Considering the optics and iron content of individual smoke compositions gives an ablated Fe influx of 1.8 ± 0.9 t d-1. Finally, the global total meteoric influx (ablated plus surviving) is estimated to be 30 ± 18 t d-1, when considering the present results and a recent description of the speciation of meteoric material.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AMT....11..949V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AMT....11..949V"><span>Characterization of smoke and dust episode over West Africa: comparison of MERRA-2 <span class="hlt">modeling</span> with multiwavelength Mie-Raman lidar <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Veselovskii, Igor; Goloub, Philippe; Podvin, Thierry; Tanre, Didier; da Silva, Arlindo; Colarco, Peter; Castellanos, Patricia; Korenskiy, Mikhail; Hu, Qiaoyun; Whiteman, David N.; Pérez-Ramírez, Daniel; Augustin, Patrick; Fourmentin, Marc; Kolgotin, Alexei</p> <p>2018-02-01</p> <p><span class="hlt">Observations</span> of multiwavelength Mie-Raman lidar taken during the SHADOW field campaign are used to analyze a smoke-dust episode over West Africa on 24-27 December 2015. For the case considered, the dust layer extended from the ground up to approximately 2000 m while the elevated smoke layer occurred in the 2500-4000 m range. The profiles of lidar <span class="hlt">measured</span> backscattering, extinction coefficients, and depolarization ratios are compared with the vertical distribution of aerosol parameters provided by the Modern-Era Retrospective Analysis for Research and Applications, version 2 (MERRA-2). The MERRA-2 <span class="hlt">model</span> simulated the correct location of the near-surface dust and elevated smoke layers. The values of <span class="hlt">modeled</span> and <span class="hlt">observed</span> aerosol extinction coefficients at both 355 and 532 nm are also rather close. In particular, for the episode reported, the mean value of difference between the <span class="hlt">measured</span> and <span class="hlt">modeled</span> extinction coefficients at 355 nm is 0.01 km-1 with SD of 0.042 km-1. The <span class="hlt">model</span> predicts significant concentration of dust particles inside the elevated smoke layer, which is supported by an increased depolarization ratio of 15 % <span class="hlt">observed</span> in the center of this layer. The <span class="hlt">modeled</span> at 355 nm the lidar ratio of 65 sr in the near-surface dust layer is close to the <span class="hlt">observed</span> value (70 ± 10) sr. At 532 nm, however, the simulated lidar ratio (about 40 sr) is lower than <span class="hlt">measurements</span> (55 ± 8 sr). The results presented demonstrate that the lidar and <span class="hlt">model</span> data are complimentary and the synergy of <span class="hlt">observations</span> and <span class="hlt">models</span> is a key to improve the aerosols characterization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1715322S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1715322S"><span><span class="hlt">Measuring</span> the World: How theory follows <span class="hlt">observation</span> (Alexander von Humboldt Medal)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Savenije, Hubert H. G.</p> <p>2015-04-01</p> <p>I started my professional career as a hydrologist working for the government of Mozambique. I was responsible for overseeing the hydrological network, the operational hydrology and answering specific questions related to water resources availability and the occurrence of floods. In the late 1970s and early 1980s, the use of telecommunication and computers was still very limited. We had to work with handbooks, lecture notes and consultancy reports, but mostly with our brains. The key to answering a specific question was to go into the field and <span class="hlt">observe</span>. We <span class="hlt">measured</span> as much as we could to understand the processes that we <span class="hlt">observed</span>. I didn't know it at the time, but this perfectly fits in the tradition of Von Humboldt. During my time in Mozambique I surveyed during and after extreme floods, such as the 1984 flood caused by the tropical cyclone Demoina. I surveyed the geometry, hydraulics and salt intrusion of 4 major Mozambican estuaries. And I <span class="hlt">measured</span> the quality and the quantity of the flows draining onto these estuaries. Having only limited access to the literature, it was a survey without much theoretical guidance. This maybe slowed us down a bit, and sometimes led to inefficient approaches, but scientifically it was a gold mine. Not being biased by established theories is a great advantage. One does not follow onto the well-trodden, but sometimes erroneous, paths of others. After working for 6 years in Mozambique I joined an international consultant, for whom I worked for 6 years in many different countries in Asia, Africa and South America. Although the access to literature and other people's experience was better, I continued the practice of <span class="hlt">observing</span> before believing. These 12 years of doing hydrology in practice formed the basis for the development of my own theories on hydrological processes, salt intrusion in estuaries, tidal hydraulics and even atmospheric moisture recycling. So when I started on my PhD at the age of 38, I made a completely different start</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMEP33B0778L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMEP33B0778L"><span><span class="hlt">Model</span> Improvement by Assimilating <span class="hlt">Observations</span> of Storm-Induced Coastal Change</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Long, J. W.; Plant, N. G.; Sopkin, K.</p> <p>2010-12-01</p> <p>Discrete, large scale, meteorological events such as hurricanes can cause wide-spread destruction of coastal islands, habitats, and infrastructure. The effects can vary significantly along the coast depending on the configuration of the coastline, variable dune elevations, changes in geomorphology (sandy beach vs. marshland), and alongshore variations in storm hydrodynamic forcing. There are two primary methods of determining the changing state of a coastal system. Process-based numerical <span class="hlt">models</span> provide highly resolved (in space and time) representations of the dominant dynamics in a physical system but must employ certain parameterizations due to computational limitations. The predictive capability may also suffer from the lack of reliable initial or boundary conditions. On the other hand, <span class="hlt">observations</span> of coastal topography before and after the storm allow the direct quantification of cumulative storm impacts. Unfortunately these <span class="hlt">measurements</span> suffer from instrument noise and a lack of necessary temporal resolution. This research focuses on the combination of these two pieces of information to make more reliable forecasts of storm-induced coastal change. Of primary importance is the development of a data assimilation strategy that is efficient, applicable for use with highly nonlinear <span class="hlt">models</span>, and able to quantify the remaining forecast uncertainty based on the reliability of each individual piece of information used in the assimilation process. We concentrate on an event time-scale and estimate/update unobserved <span class="hlt">model</span> information (boundary conditions, free parameters, etc.) by assimilating direct <span class="hlt">observations</span> of coastal change with those simulated by the <span class="hlt">model</span>. The data assimilation can help estimate spatially varying quantities (e.g. friction coefficients) that are often <span class="hlt">modeled</span> as homogeneous and identify processes inadequately characterized in the <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM52A..04W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM52A..04W"><span>Application of New Chorus Wave <span class="hlt">Model</span> from Van Allen Probe <span class="hlt">Observations</span> in Earth's Radiation Belt <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, D.; Shprits, Y.; Spasojevic, M.; Zhu, H.; Aseev, N.; Drozdov, A.; Kellerman, A. C.</p> <p>2017-12-01</p> <p>In situ satellite <span class="hlt">observations</span>, theoretical studies and <span class="hlt">model</span> simulations suggested that chorus waves play a significant role in the dynamic evolution of relativistic electrons in the Earth's radiation belts. In this study, we developed new wave frequency and amplitude <span class="hlt">models</span> that depend on Magnetic Local Time (MLT)-, L-shell, latitude- and geomagnetic conditions indexed by Kp for upper-band and lower-band chorus waves using <span class="hlt">measurements</span> from the Electric and Magnetic Field Instrument Suite and Integrated Science (EMFISIS) instrument onboard the Van Allen Probes. Utilizing the quasi-linear full diffusion code, we calculated corresponding diffusion coefficients in each MLT sector (1 hour resolution) for upper-band and lower-band chorus waves according to the new developed wave <span class="hlt">models</span>. Compared with former parameterizations of chorus waves, the new parameterizations result in differences in diffusion coefficients that depend on energy and pitch angle. Utilizing obtained diffusion coefficients, lifetime of energetic electrons is parameterized accordingly. In addition, to investigate effects of obtained diffusion coefficients in different MLT sectors and under different geomagnetic conditions, we performed simulations using four-dimensional Versatile Electron Radiation Belt simulations and validated results against <span class="hlt">observations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A52C..08P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A52C..08P"><span>Stochastic behaviour of tropical convection in <span class="hlt">observations</span> and a multicloud <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peters, K.; Jakob, C.; Davies, L.; Kumar, V.; Khouider, B.; Majda, A.</p> <p>2012-12-01</p> <p>The feasibility of using a stochastic multicloud <span class="hlt">model</span> (SMCM, Khouider et al. (2010)) to represent <span class="hlt">observed</span> tropical convection over a northern Australia coastal site is investigated. In the SMCM, area fractions of three cloud types associated with tropical convection (congestus, deep convection and stratiform) are derived employing a coarse grained birth-death process which is evolved in time using a Markov chain Monte Carlo method. Here, we force the SMCM with an <span class="hlt">observed</span> large-scale atmospheric state to assess the feasibility of applying the <span class="hlt">model</span>'s underlying design concept to simulate <span class="hlt">observed</span> tropical convection. The <span class="hlt">observational</span> dataset we use here represents the best estimate of the atmospheric state for a 190x190 km2 area centered over Darwin, Australia (Jakob et al., 2011). Cloud area fractions are derived from CPOL radar following Steiner et al. (1995). We use different combinations of predictors derived from the <span class="hlt">observations</span> (e.g. CAPE, low-level CAPE, moisture convergence, mid-tropospheric relative humidity) to obtain the evolution of the cloud ensemble as simulated by the SMCM. We find that the diagnostic performance of the SMCM depends strongly on the predictor choice and that it performs remarkably well when initiation and maintenance of convection are prescribed to depend on <span class="hlt">measures</span> related to changes in low-level moisture. This is an encouraging result on the road towards a novel convection parameterization, aimed at overcoming the difficulties of current deterministic convection parameterizations in representing the high variability in simulated tropical convection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150023378&hterms=fingerprints&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfingerprints','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150023378&hterms=fingerprints&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfingerprints"><span>External Influences on <span class="hlt">Modeled</span> and <span class="hlt">Observed</span> Cloud Trends</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marvel, Kate; Zelinka, Mark; Klein, Stephen A.; Bonfils, Celine; Caldwell, Peter; Doutriaux, Charles; Santer, Benjamin D.; Taylor, Karl E.</p> <p>2015-01-01</p> <p>Understanding the cloud response to external forcing is a major challenge for climate science. This crucial goal is complicated by intermodel differences in simulating present and future cloud cover and by <span class="hlt">observational</span> uncertainty. This is the first formal detection and attribution study of cloud changes over the satellite era. Presented herein are CMIP5 (Coupled <span class="hlt">Model</span> Intercomparison Project - Phase 5) <span class="hlt">model</span>-derived fingerprints of externally forced changes to three cloud properties: the latitudes at which the zonally averaged total cloud fraction (CLT) is maximized or minimized, the zonal average CLT at these latitudes, and the height of high clouds at these latitudes. By considering simultaneous changes in all three properties, the authors define a coherent multivariate fingerprint of cloud response to external forcing and use <span class="hlt">models</span> from phase 5 of CMIP (CMIP5) to calculate the average time to detect these changes. It is found that given perfect satellite cloud <span class="hlt">observations</span> beginning in 1983, the <span class="hlt">models</span> indicate that a detectable multivariate signal should have already emerged. A search is then made for signals of external forcing in two <span class="hlt">observational</span> datasets: ISCCP (International Satellite Cloud Climatology Project) and PATMOS-x (Advanced Very High Resolution Radiometer (AVHRR) Pathfinder Atmospheres - Extended). The datasets are both found to show a poleward migration of the zonal CLT pattern that is incompatible with forced CMIP5 <span class="hlt">models</span>. Nevertheless, a detectable multivariate signal is predicted by <span class="hlt">models</span> over the PATMOS-x time period and is indeed present in the dataset. Despite persistent <span class="hlt">observational</span> uncertainties, these results present a strong case for continued efforts to improve these existing satellite <span class="hlt">observations</span>, in addition to planning for new missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22220517-correlation-between-model-observer-human-observer-performance-ct-imaging-when-lesion-location-uncertain','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22220517-correlation-between-model-observer-human-observer-performance-ct-imaging-when-lesion-location-uncertain"><span>Correlation between <span class="hlt">model</span> <span class="hlt">observer</span> and human <span class="hlt">observer</span> performance in CT imaging when lesion location is uncertain</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Leng, Shuai; Yu, Lifeng; Zhang, Yi</p> <p>2013-08-15</p> <p>Purpose: The purpose of this study was to investigate the correlation between <span class="hlt">model</span> <span class="hlt">observer</span> and human <span class="hlt">observer</span> performance in CT imaging for the task of lesion detection and localization when the lesion location is uncertain.Methods: Two cylindrical rods (3-mm and 5-mm diameters) were placed in a 35 × 26 cm torso-shaped water phantom to simulate lesions with −15 HU contrast at 120 kV. The phantom was scanned 100 times on a 128-slice CT scanner at each of four dose levels (CTDIvol = 5.7, 11.4, 17.1, and 22.8 mGy). Regions of interest (ROIs) around each lesion were extracted to generate imagesmore » with signal-present, with each ROI containing 128 × 128 pixels. Corresponding ROIs of signal-absent images were generated from images without lesion mimicking rods. The location of the lesion (rod) in each ROI was randomly distributed by moving the ROIs around each lesion. Human <span class="hlt">observer</span> studies were performed by having three trained <span class="hlt">observers</span> identify the presence or absence of lesions, indicating the lesion location in each image and scoring confidence for the detection task on a 6-point scale. The same image data were analyzed using a channelized Hotelling <span class="hlt">model</span> <span class="hlt">observer</span> (CHO) with Gabor channels. Internal noise was added to the decision variables for the <span class="hlt">model</span> <span class="hlt">observer</span> study. Area under the curve (AUC) of ROC and localization ROC (LROC) curves were calculated using a nonparametric approach. The Spearman's rank order correlation between the average performance of the human <span class="hlt">observers</span> and the <span class="hlt">model</span> <span class="hlt">observer</span> performance was calculated for the AUC of both ROC and LROC curves for both the 3- and 5-mm diameter lesions.Results: In both ROC and LROC analyses, AUC values for the <span class="hlt">model</span> <span class="hlt">observer</span> agreed well with the average values across the three human <span class="hlt">observers</span>. The Spearman's rank order correlation values for both ROC and LROC analyses for both the 3- and 5-mm diameter lesions were all 1.0, indicating perfect rank ordering agreement of the figures of merit (AUC) between</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA616081','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA616081"><span><span class="hlt">Modeling</span> Navigation System Performance of a Satellite-<span class="hlt">Observing</span> Star Tracker Tightly Integrated with an Inertial <span class="hlt">Measurement</span> Unit</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-03-26</p> <p>tracker, an Inertial <span class="hlt">Measurement</span> Unit (IMU), and a barometric altimeter using an Extended Kalman Filter (EKF). <span class="hlt">Models</span> of each of these components are...Positioning 15 2.5 Detector Device Improvement . . . . . . . . . . . . . . . 15 2.6 Kalman Filter . . . . . . . . . . . . . . . . . . . . . . . . 17 2.6.1...Extended Kalman Filter . . . . . . . . . . . . . 17 2.7 System Properties . . . . . . . . . . . . . . . . . . . . . 21 2.8 Sun Exitance</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....16.2109W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....16.2109W"><span>Atmospheric OH reactivity in central London: <span class="hlt">observations</span>, <span class="hlt">model</span> predictions and estimates of in situ ozone production</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Whalley, Lisa K.; Stone, Daniel; Bandy, Brian; Dunmore, Rachel; Hamilton, Jacqueline F.; Hopkins, James; Lee, James D.; Lewis, Alastair C.; Heard, Dwayne E.</p> <p>2016-02-01</p> <p>Near-continuous <span class="hlt">measurements</span> of hydroxyl radical (OH) reactivity in the urban background atmosphere of central London during the summer of 2012 are presented. OH reactivity behaviour is seen to be broadly dependent on air mass origin, with the highest reactivity and the most pronounced diurnal profile <span class="hlt">observed</span> when air had passed over central London to the east, prior to <span class="hlt">measurement</span>. Averaged over the entire <span class="hlt">observation</span> period of 26 days, OH reactivity peaked at ˜ 27 s-1 in the morning, with a minimum of ˜ 15 s-1 during the afternoon. A maximum OH reactivity of 116 s-1 was recorded on one day during morning rush hour. A detailed box <span class="hlt">model</span> using the Master Chemical Mechanism was used to calculate OH reactivity, and was constrained with an extended <span class="hlt">measurement</span> data set of volatile organic compounds (VOCs) derived from a gas chromatography flame ionisation detector (GC-FID) and a two-dimensional GC instrument which included heavier molecular weight (up to C12) aliphatic VOCs, oxygenated VOCs and the biogenic VOCs α-pinene and limonene. Comparison was made between <span class="hlt">observed</span> OH reactivity and <span class="hlt">modelled</span> OH reactivity using (i) a standard suite of VOC <span class="hlt">measurements</span> (C2-C8 hydrocarbons and a small selection of oxygenated VOCs) and (ii) a more comprehensive inventory including species up to C12. <span class="hlt">Modelled</span> reactivities were lower than those <span class="hlt">measured</span> (by 33 %) when only the reactivity of the standard VOC suite was considered. The difference between <span class="hlt">measured</span> and <span class="hlt">modelled</span> reactivity was improved, to within 15 %, if the reactivity of the higher VOCs (⩾ C9) was also considered, with the reactivity of the biogenic compounds of α-pinene and limonene and their oxidation products almost entirely responsible for this improvement. Further improvements in the <span class="hlt">model</span>'s ability to reproduce OH reactivity (to within 6 %) could be achieved if the reactivity and degradation mechanism of unassigned two-dimensional GC peaks were estimated. Neglecting the contribution of the higher VOCs (⩾ C</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.H51H1617T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.H51H1617T"><span>Improving River Flow Predictions from the NOAA NCRFC Forecasting <span class="hlt">Model</span> by Incorporating Satellite <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tuttle, S. E.; Jacobs, J. M.; Restrepo, P. J.; Deweese, M. M.; Connelly, B.; Buan, S.</p> <p>2016-12-01</p> <p>The NOAA National Weather Service North Central River Forecast Center (NCRFC) is responsible for issuing river flow forecasts for parts of the Upper Mississippi, Great Lakes, and Hudson Bay drainages, including the Red River of the North basin (RRB). The NCRFC uses an operational hydrologic <span class="hlt">modeling</span> infrastructure called the Community Hydrologic Prediction System (CHPS) for its operational forecasts, which currently links the SNOW-17 snow accumulation and ablation <span class="hlt">model</span>, to the Sacramento-Soil Moisture Accounting (SAC-SMA) rainfall-runoff <span class="hlt">model</span>, to a number of hydrologic and hydraulic flow routing <span class="hlt">models</span>. The operational <span class="hlt">model</span> is lumped and requires only area-averaged precipitation and air temperature as inputs. NCRFC forecasters use <span class="hlt">observational</span> data of hydrological state variables as a source of supplemental information during forecasting, and can use professional judgment to modify the <span class="hlt">model</span> states in real time. In a few recent years (e.g. 2009, 2013), the RRB exhibited unexpected anomalous hydrologic behavior, resulting in overestimation of peak flood discharge by up to 70% and highlighting the need for <span class="hlt">observations</span> with high temporal and spatial coverage. Unfortunately, <span class="hlt">observations</span> of hydrological states (e.g. soil moisture, snow water equivalent (SWE)) are relatively scarce in the RRB. Satellite remote sensing can fill this need. We use Minnesota's Buffalo River watershed within the RRB as a test case and update the operational CHPS <span class="hlt">model</span> using modifications based on satellite <span class="hlt">observations</span>, including AMSR-E SWE and SMOS soil moisture estimates. We evaluate the added forecasting skill of the satellite-enhanced <span class="hlt">model</span> compared to <span class="hlt">measured</span> streamflow using hindcasts from 2010-2013.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23618498','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23618498"><span>Satellite <span class="hlt">observations</span> and <span class="hlt">modeling</span> of oil spill trajectories in the Bohai Sea.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xu, Qing; Li, Xiaofeng; Wei, Yongliang; Tang, Zeyan; Cheng, Yongcun; Pichel, William G</p> <p>2013-06-15</p> <p>On June 4 and 17, 2011, separate oil spill accidents occurred at two oil platforms in the Bohai Sea, China. The oil spills were subsequently <span class="hlt">observed</span> on different types of satellite images including SAR (Synthetic Aperture Radar), Chinese HJ-1-B CCD and NASA MODIS. To illustrate the fate of the oil spills, we performed two numerical simulations to simulate the trajectories of the oil spills with the GNOME (General NOAA Operational <span class="hlt">Modeling</span> Environment) <span class="hlt">model</span>. For the first time, we drive the GNOME with currents obtained from an operational ocean <span class="hlt">model</span> (NCOM, Navy Coastal Ocean <span class="hlt">Model</span>) and surface winds from operational scatterometer <span class="hlt">measurements</span> (ASCAT, the Advanced Scatterometer). Both data sets are freely and openly available. The initial oil spill location inputs to the <span class="hlt">model</span> are based on the detected oil spill locations from the SAR images acquired on June 11 and 14. Three oil slicks are tracked simultaneously and our results show good agreement between <span class="hlt">model</span> simulations and subsequent satellite <span class="hlt">observations</span> in the semi-enclosed shallow sea. Moreover, GNOME simulation shows that the number of 'splots', which denotes the extent of spilled oil, is a vital factor for GNOME running stability when the number is less than 500. Therefore, oil spill area information obtained from satellite sensors, especially SAR, is an important factor for setting up the initial <span class="hlt">model</span> conditions. Copyright © 2013 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.G11C..04M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.G11C..04M"><span>Improvements in GRACE Gravity Field Determination through Stochastic <span class="hlt">Observation</span> <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McCullough, C.; Bettadpur, S. V.</p> <p>2016-12-01</p> <p>Current unconstrained Release 05 GRACE gravity field solutions from the Center for Space Research (CSR RL05) assume random <span class="hlt">observation</span> errors following an independent multivariate Gaussian distribution. This <span class="hlt">modeling</span> of <span class="hlt">observations</span>, a simplifying assumption, fails to account for long period, correlated errors arising from inadequacies in the background force <span class="hlt">models</span>. Fully <span class="hlt">modeling</span> the errors inherent in the <span class="hlt">observation</span> equations, through the use of a full <span class="hlt">observation</span> covariance (<span class="hlt">modeling</span> colored noise), enables optimal combination of GPS and inter-satellite range-rate data and obviates the need for estimating kinematic empirical parameters during the solution process. Most importantly, fully <span class="hlt">modeling</span> the <span class="hlt">observation</span> errors drastically improves formal error estimates of the spherical harmonic coefficients, potentially enabling improved uncertainty quantification of scientific results derived from GRACE and optimizing combinations of GRACE with independent data sets and a priori constraints.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...613A..74P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...613A..74P"><span>Broadband radio spectro-polarimetric <span class="hlt">observations</span> of high-Faraday-rotation-<span class="hlt">measure</span> AGN</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasetto, Alice; Carrasco-González, Carlos; O'Sullivan, Shane; Basu, Aritra; Bruni, Gabriele; Kraus, Alex; Curiel, Salvador; Mack, Karl-Heinz</p> <p>2018-06-01</p> <p>We present broadband polarimetric <span class="hlt">observations</span> of a sample of high-Faraday-rotation-<span class="hlt">measure</span> (high-RM) active galactic nuclei (AGN) using the Karl. G. Jansky Very Large Array (JVLA) telescope from 1 to 2 GHz, and 4 to 12 GHz. The sample (14 sources) consists of very compact sources (linear resolution smaller than ≈5 kpc) that are unpolarized at 1.4 GHz in the NRAO VLA Sky Survey (NVSS). Total intensity data have been <span class="hlt">modeled</span> using a combination of synchrotron components, revealing complex structure in their radio spectra. Depolarization <span class="hlt">modeling</span>, through the so-called qu-fitting (the <span class="hlt">modeling</span> of the fractional quantities of the Stokes Q and U parameters), has been performed on the polarized data using an equation that attempts to simplify the process of fitting many different depolarization <span class="hlt">models</span>. These <span class="hlt">models</span> can be divided into two major categories: external depolarization (ED) and internal depolarization (ID) <span class="hlt">models</span>. Understanding which of the two mechanisms is the most representative would help the qualitative understanding of the AGN jet environment and whether it is embedded in a dense external magneto-ionic medium or if it is the jet-wind that causes the high RM and strong depolarization. This could help to probe the jet magnetic field geometry (e.g., helical or otherwise). This new high-sensitivity data shows a complicated behavior in the total intensity and polarization radio spectrum of individual sources. We <span class="hlt">observed</span> the presence of several synchrotron components and Faraday components in their total intensity and polarized spectra. For the majority of our targets (12 sources), the depolarization seems to be caused by a turbulent magnetic field. Thus, our main selection criteria (lack of polarization at 1.4 GHz in the NVSS) result in a sample of sources with very large RMs and depolarization due to turbulent magnetic fields local to the source. These broadband JVLA data reveal the complexity of the polarization properties of this class of radio sources</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AtmEn..48..165F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AtmEn..48..165F"><span>Validation of the FALL3D ash dispersion <span class="hlt">model</span> using <span class="hlt">observations</span> of the 2010 Eyjafjallajökull volcanic ash clouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Folch, A.; Costa, A.; Basart, S.</p> <p>2012-03-01</p> <p>During April-May 2010 volcanic ash clouds from the Icelandic Eyjafjallajökull volcano reached Europe causing an unprecedented disruption of the EUR/NAT region airspace. Civil aviation authorities banned all flight operations because of the threat posed by volcanic ash to modern turbine aircraft. New quantitative airborne ash mass concentration thresholds, still under discussion, were adopted for discerning regions contaminated by ash. This has implications for ash dispersal <span class="hlt">models</span> routinely used to forecast the evolution of ash clouds. In this new context, quantitative <span class="hlt">model</span> validation and assessment of the accuracies of current state-of-the-art <span class="hlt">models</span> is of paramount importance. The passage of volcanic ash clouds over central Europe, a territory hosting a dense network of meteorological and air quality observatories, generated a quantity of <span class="hlt">observations</span> unusual for volcanic clouds. From the ground, the cloud was <span class="hlt">observed</span> by aerosol lidars, lidar ceilometers, sun photometers, other remote-sensing instruments and in-situ collectors. From the air, sondes and multiple aircraft <span class="hlt">measurements</span> also took extremely valuable in-situ and remote-sensing <span class="hlt">measurements</span>. These <span class="hlt">measurements</span> constitute an excellent database for <span class="hlt">model</span> validation. Here we validate the FALL3D ash dispersal <span class="hlt">model</span> by comparing <span class="hlt">model</span> results with ground and airplane-based <span class="hlt">measurements</span> obtained during the initial 14-23 April 2010 Eyjafjallajökull explosive phase. We run the <span class="hlt">model</span> at high spatial resolution using as input hourly-averaged <span class="hlt">observed</span> heights of the eruption column and the total grain size distribution reconstructed from field <span class="hlt">observations</span>. <span class="hlt">Model</span> results are then compared against remote ground-based and in-situ aircraft-based <span class="hlt">measurements</span>, including lidar ceilometers from the German Meteorological Service, aerosol lidars and sun photometers from EARLINET and AERONET networks, and flight missions of the German DLR Falcon aircraft. We find good quantitative agreement, with an error similar to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.3828H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.3828H"><span>Inverse <span class="hlt">modelling</span> of radionuclide release rates using gamma dose rate <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hamburger, Thomas; Evangeliou, Nikolaos; Stohl, Andreas; von Haustein, Christoph; Thummerer, Severin; Wallner, Christian</p> <p>2015-04-01</p> <p>Severe accidents in nuclear power plants such as the historical accident in Chernobyl 1986 or the more recent disaster in the Fukushima Dai-ichi nuclear power plant in 2011 have drastic impacts on the population and environment. <span class="hlt">Observations</span> and dispersion <span class="hlt">modelling</span> of the released radionuclides help to assess the regional impact of such nuclear accidents. <span class="hlt">Modelling</span> the increase of regional radionuclide activity concentrations, which results from nuclear accidents, underlies a multiplicity of uncertainties. One of the most significant uncertainties is the estimation of the source term. That is, the time dependent quantification of the released spectrum of radionuclides during the course of the nuclear accident. The quantification of the source term may either remain uncertain (e.g. Chernobyl, Devell et al., 1995) or rely on estimates given by the operators of the nuclear power plant. Precise <span class="hlt">measurements</span> are mostly missing due to practical limitations during the accident. The release rates of radionuclides at the accident site can be estimated using inverse <span class="hlt">modelling</span> (Davoine and Bocquet, 2007). The accuracy of the method depends amongst others on the availability, reliability and the resolution in time and space of the used <span class="hlt">observations</span>. Radionuclide activity concentrations are <span class="hlt">observed</span> on a relatively sparse grid and the temporal resolution of available data may be low within the order of hours or a day. Gamma dose rates, on the other hand, are <span class="hlt">observed</span> routinely on a much denser grid and higher temporal resolution and provide therefore a wider basis for inverse <span class="hlt">modelling</span> (Saunier et al., 2013). We present a new inversion approach, which combines an atmospheric dispersion <span class="hlt">model</span> and <span class="hlt">observations</span> of radionuclide activity concentrations and gamma dose rates to obtain the source term of radionuclides. We use the Lagrangian particle dispersion <span class="hlt">model</span> FLEXPART (Stohl et al., 1998; Stohl et al., 2005) to <span class="hlt">model</span> the atmospheric transport of the released radionuclides. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E.471D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E.471D"><span>The Geolocation <span class="hlt">model</span> for lunar-based Earth <span class="hlt">observation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ding, Yixing; Liu, Guang; Ren, Yuanzhen; Ye, Hanlin; Guo, Huadong; Lv, Mingyang</p> <p>2016-07-01</p> <p>In recent years, people are more and more aware of that the earth need to treated as an entirety, and consequently to be <span class="hlt">observed</span> in a holistic, systematic and multi-scale view. However, the interaction mechanism between the Earth's inner layers and outer layers is still unclear. Therefore, we propose to <span class="hlt">observe</span> the Earth's inner layers and outer layers instantaneously on the Moon which may be helpful to the studies in climatology, meteorology, seismology, etc. At present, the Moon has been proved to be an irreplaceable platform for Earth's outer layers <span class="hlt">observation</span>. Meanwhile, some discussions have been made in lunar-based <span class="hlt">observation</span> of the Earth's inner layers, but the geolocation <span class="hlt">model</span> of lunar-based <span class="hlt">observation</span> has not been specified yet. In this paper, we present a geolocation <span class="hlt">model</span> based on transformation matrix. The <span class="hlt">model</span> includes six coordinate systems: The telescope coordinate system, the lunar local coordinate system, the lunar-reference coordinate system, the selenocentric inertial coordinate system, the geocentric inertial coordinate system and the geo-reference coordinate system. The parameters, lncluding the position of the Sun, the Earth, the Moon, the libration and the attitude of the Earth, can be acquired from the Ephemeris. By giving an elevation angle and an azimuth angle of the lunar-based telescope, this <span class="hlt">model</span> links the image pixel to the ground point uniquely.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1201353-insights-from-modeling-observational-evaluation-precipitating-continental-cumulus-event-observed-during-mc3e-field-campaign','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1201353-insights-from-modeling-observational-evaluation-precipitating-continental-cumulus-event-observed-during-mc3e-field-campaign"><span>Insights from <span class="hlt">modeling</span> and <span class="hlt">observational</span> evaluation of a precipitating continental cumulus event <span class="hlt">observed</span> during the MC3E field campaign</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Mechem, David B.; Giangrande, Scott E.; Wittman, Carly S.; ...</p> <p>2015-03-13</p> <p>A case of shallow cumulus and precipitating cumulus congestus sampled at the Atmospheric Radiation <span class="hlt">Measurement</span> (ARM) Program Southern Great Plains (SGP) supersite is analyzed using a multi-sensor <span class="hlt">observational</span> approach and numerical simulation. <span class="hlt">Observations</span> from a new radar suite surrounding the facility are used to characterize the evolving statistical behavior of the precipitating cloud system. This is accomplished using distributions of different <span class="hlt">measures</span> of cloud geometry and precipitation properties. Large-eddy simulation (LES) with size-resolved (bin) microphysics is employed to determine the forcings most important in producing the salient aspects of the cloud system captured in the radar <span class="hlt">observations</span>. Our emphasis ismore » on assessing the importance of time-varying vs. steady-state large-scale forcing on the <span class="hlt">model</span>'s ability to reproduce the evolutionary behavior of the cloud system. Additional consideration is given to how the characteristic spatial scale and homogeneity of the forcing imposed on the simulation influences the evolution of cloud system properties. Results indicate that several new scanning radar estimates such as distributions of cloud top are useful to differentiate the value of time-varying (or at least temporally well-matched) forcing on LES solution fidelity.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984InISJ..65...11L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984InISJ..65...11L"><span><span class="hlt">Observations</span> of tip vortex cavitation inception from a <span class="hlt">model</span> marine propeller</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lodha, R. K.; Arakeri, V. H.</p> <p>1984-01-01</p> <p>Cavitation inception characteristics of a <span class="hlt">model</span> marine propeller having three blades, developed area ratio of 0.34 and at three different pitch to diameter ratios of 0.62, 0.83 and 1.0 are reported. The dominant type of cavitation <span class="hlt">observed</span> at inception was the tip vortex type. The <span class="hlt">measured</span> magnitude of inception index is found to agree well with a proposed correlation due to Strasberg. Performance calculations of the propeller based on combined vortex and blade element theory are also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004MeScT..15.1185M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004MeScT..15.1185M"><span>Exhaust pressure pulsation <span class="hlt">observation</span> from turbocharger instantaneous speed <span class="hlt">measurement</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Macián, V.; Luján, J. M.; Bermúdez, V.; Guardiola, C.</p> <p>2004-06-01</p> <p>In internal combustion engines, instantaneous exhaust pressure <span class="hlt">measurements</span> are difficult to perform in a production environment. The high temperature of the exhaust manifold and its pulsating character make its application to exhaust gas recirculation control algorithms impossible. In this paper an alternative method for estimating the exhaust pressure pulsation is presented. A numerical <span class="hlt">model</span> is built which enables the exhaust pressure pulses to be predicted from instantaneous turbocharger speed <span class="hlt">measurements</span>. Although the <span class="hlt">model</span> is data based, a theoretical description of the process is also provided. This combined approach makes it possible to export the <span class="hlt">model</span> for different engine operating points. Also, compressor contribution in the turbocharger speed pulsation is discussed extensively. The compressor contribution is initially neglected, and effects of this simplified approach are analysed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=reliability&pg=7&id=EJ1006173','ERIC'); return false;" href="https://eric.ed.gov/?q=reliability&pg=7&id=EJ1006173"><span>An Examination of the Reliability of a New <span class="hlt">Observation</span> <span class="hlt">Measure</span> for Autism Spectrum Disorders: The Autism Spectrum Disorder <span class="hlt">Observation</span> for Children</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Neal, Daniene; Matson, Johnny L.; Belva, Brian C.</p> <p>2013-01-01</p> <p>The "autism spectrum disorder <span class="hlt">observation</span> for children" ("ASD-OC") is a newly created 54-item <span class="hlt">observation</span> <span class="hlt">measure</span> for autism spectrum disorders (ASD). Due to the fact that many of the ASD <span class="hlt">observation</span> <span class="hlt">measures</span> currently available do not have established psychometric properties and require extensive time and training to administer, the "ASD-OC"…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.6951G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.6951G"><span>Arctic chlorine activation and ozone depletion: Comparison of chemistry transport <span class="hlt">models</span> with satellite <span class="hlt">observations</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grooß, J.-U.; Wegner, T.; Müller, R.; Chipperfield, M. P.; Feng, W.; Santee, M. L.</p> <p>2009-04-01</p> <p>The accurate simulation of Arctic stratospheric ozone depletion has been an issue for two decades. However, there are still notable quantitative discrepancies between the <span class="hlt">models</span> and <span class="hlt">observations</span>. We show results from the SLIMCAT and CLaMS 3D chemistry-transport <span class="hlt">models</span> that differ in some aspects of simulated chlorine activation and descent in the polar vortex. Consequently, the estimates of accumulated ozone depletion in the polar vortex for these two <span class="hlt">models</span> in cold Arctic winters still largely disagree. As shown recently by Santee et al. (JGR, 2008) using MLS and ACE data, the extent of chlorine activation for the cold Arctic winter of 2004/2005 within the basic SLIMCAT <span class="hlt">model</span> is overestimated with the likely consequence of too much simulated ozone depletion. In contrast, the CLaMS simulation for the same winter shows too little chlorine activation compared to <span class="hlt">observations</span>, and therefore likely too little loss. For SLIMCAT the version used by Santee et al. has been updated to replace the equilibrium treatment of NAT PSCs with a Lagrangian microphysical scheme. This leads to smaller regions of NAT particles and less denitrification, in better agreement with <span class="hlt">observations</span>. The impact of this on the <span class="hlt">modeled</span> extent of chlorine activation will be discussed. For CLaMS we have changed the parameterization of heterogeneous reactions on liquid aerosols from Carslaw et al. to that of Shi et al. (2001), with which chlorine activation on liquid aerosol becomes more efficient. In turn, the simulated chlorine activation agrees better with the <span class="hlt">observations</span>. The impact of these <span class="hlt">model</span> changes on chlorine activation and ozone loss will be assessed and remaining <span class="hlt">model-observation</span> discrepancies will be discussed in terms of different <span class="hlt">model</span> formulations. We will also show the impact of recent lab <span class="hlt">measurements</span> of Cl2O2 absorption cross sections by von Hobe et al. (2009) on the simulated ozone depletion. References: von Hobe, M., F. Stroh, H. Beckers, T. Benter, and H. Willner, The UV</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010062494&hterms=inorganic+chemistry&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dinorganic%2Bchemistry','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010062494&hterms=inorganic+chemistry&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dinorganic%2Bchemistry"><span>Inorganic Chlorine Partitioning in the Summer Lower Stratosphere: <span class="hlt">Modeled</span> and <span class="hlt">Measured</span> [ClONO2/HCl] During POLARIS</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Voss, P. B.; Stimpfle, R. M.; Cohen, R. C.; Hanisco, T. F.; Bonne, G. P.; Perkins, K. K.; Lanzendorf, E. J.; Anderson, J. G.; Salawitch, R. J.</p> <p>2001-01-01</p> <p>We examine inorganic chlorine (Cly) partitioning in the summer lower stratosphere using in situ ER-2 aircraft <span class="hlt">observations</span> made during the Photochemistry of Ozone Loss in the Arctic Region in Summer (POLARIS) campaign. New steady state and numerical <span class="hlt">models</span> estimate [ClONO2]/[HCl] using currently accepted photochemistry. These <span class="hlt">models</span> are tightly constrained by <span class="hlt">observations</span> with OH (parameterized as a function of solar zenith angle) substituting for <span class="hlt">modeled</span> HO2 chemistry. We find that inorganic chlorine photochemistry alone overestimates <span class="hlt">observed</span> [ClONO2]/[HCl] by approximately 55-60% at mid and high latitudes. On the basis of POLARIS studies of the inorganic chlorine budget, [ClO]/[ClONO2], and an intercomparison with balloon <span class="hlt">observations</span>, the most direct explanation for the <span class="hlt">model-measurement</span> discrepancy in Cly partitioning is an error in the reactions, rate constants, and <span class="hlt">measured</span> species concentrations linking HCl and ClO (simulated [ClO]/[HCl] too high) in combination with a possible systematic error in the ER-2 ClONO2 <span class="hlt">measurement</span> (too low). The high precision of our simulation (+/-15% 1-sigma for [ClONO2]/[HCl], which is compared with <span class="hlt">observations</span>) increases confidence in the <span class="hlt">observations</span>, photolysis calculations, and laboratory rate constants. These results, along with other findings, should lead to improvements in both the accuracy and precision of stratospheric photochemical <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=teacher+AND+observation&pg=2&id=EJ1100448','ERIC'); return false;" href="https://eric.ed.gov/?q=teacher+AND+observation&pg=2&id=EJ1100448"><span>Classroom Composition and <span class="hlt">Measured</span> Teacher Performance: What Do Teacher <span class="hlt">Observation</span> Scores Really <span class="hlt">Measure</span>?</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Steinberg, Matthew P.; Garrett, Rachel</p> <p>2016-01-01</p> <p>As states and districts implement more rigorous teacher evaluation systems, <span class="hlt">measures</span> of teacher performance are increasingly being used to support instruction and inform retention decisions. Classroom <span class="hlt">observations</span> take a central role in these systems, accounting for the majority of teacher ratings upon which accountability decisions are based.…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120001768','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120001768"><span>Ares I Scale <span class="hlt">Model</span> Acoustic Test Instrumentation for Acoustic and Pressure <span class="hlt">Measurements</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vargas, Magda B.; Counter, Douglas</p> <p>2011-01-01</p> <p>Ares I Scale <span class="hlt">Model</span> Acoustic Test (ASMAT) is a 5% scale <span class="hlt">model</span> test of the Ares I vehicle, launch pad and support structures conducted at MSFC to verify acoustic and ignition environments and evaluate water suppression systems Test design considerations 5% <span class="hlt">measurements</span> must be scaled to full scale requiring high frequency <span class="hlt">measurements</span> Users had different frequencies of interest Acoustics: 200 - 2,000 Hz full scale equals 4,000 - 40,000 Hz <span class="hlt">model</span> scale Ignition Transient: 0 - 100 Hz full scale equals 0 - 2,000 Hz <span class="hlt">model</span> scale Environment exposure Weather exposure: heat, humidity, thunderstorms, rain, cold and snow Test environments: Plume impingement heat and pressure, and water deluge impingement Several types of sensors were used to <span class="hlt">measure</span> the environments Different instrument mounts were used according to the location and exposure to the environment This presentation addresses the <span class="hlt">observed</span> effects of the selected sensors and mount design on the acoustic and pressure <span class="hlt">measurements</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/920860','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/920860"><span>Considerations on the Use of 3-D Geophysical <span class="hlt">Models</span> to Predict Test Ban Monitoring <span class="hlt">Observables</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Harris, D B; Zucca, J J; McCallen, D B</p> <p>2007-07-09</p> <p>The use of 3-D geophysical <span class="hlt">models</span> to predict nuclear test ban monitoring <span class="hlt">observables</span> (phase travel times, amplitudes, dispersion, etc.) is widely anticipated to provide improvements in the basic seismic monitoring functions of detection, association, location, discrimination and yield estimation. A number of questions arise when contemplating a transition from 1-D, 2-D and 2.5-D <span class="hlt">models</span> to constructing and using 3-D <span class="hlt">models</span>, among them: (1) Can a 3-D geophysical <span class="hlt">model</span> or a collection of 3-D <span class="hlt">models</span> provide <span class="hlt">measurably</span> improved predictions of seismic monitoring <span class="hlt">observables</span> over existing 1-D <span class="hlt">models</span>, or 2-D and 2 1/2-D <span class="hlt">models</span> currently under development? (2) Is a single modelmore » that can predict all <span class="hlt">observables</span> achievable, or must separate <span class="hlt">models</span> be devised for each <span class="hlt">observable</span>? How should joint inversion of disparate <span class="hlt">observable</span> data be performed, if required? (3) What are the options for <span class="hlt">model</span> representation? Are multi-resolution <span class="hlt">models</span> essential? How does representation affect the accuracy and speed of <span class="hlt">observable</span> predictions? (4) How should <span class="hlt">model</span> uncertainty be estimated, represented and how should it be used? Are stochastic <span class="hlt">models</span> desirable? (5) What data types should be used to construct the <span class="hlt">models</span>? What quality control regime should be established? (6) How will 3-D <span class="hlt">models</span> be used in operations? Will significant improvements in the basic monitoring functions result from the use of 3-D <span class="hlt">models</span>? Will the calculation of <span class="hlt">observables</span> through 3-D <span class="hlt">models</span> be fast enough for real-time use or must a strategy of pre-computation be employed? (7) What are the theoretical limits to 3-D <span class="hlt">model</span> development (resolution, uncertainty) and performance in predicting monitoring <span class="hlt">observables</span>? How closely can those limits be approached with projected data availability, station distribution and inverse methods? (8) What priorities should be placed on the acquisition of event ground truth information, deployment of new stations, development of new inverse techniques, exploitation of large</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070009922','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070009922"><span>Evaluating Clouds in Long-Term Cloud-Resolving <span class="hlt">Model</span> Simulations with <span class="hlt">Observational</span> Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zeng, Xiping; Tao, Wei-Kuo; Zhang, Minghua; Peters-Lidard, Christa; Lang, Stephen; Simpson, Joanne; Kumar, Sujay; Xie, Shaocheng; Eastman, Joseph L.; Shie, Chung-Lin; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20070009922'); toggleEditAbsImage('author_20070009922_show'); toggleEditAbsImage('author_20070009922_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20070009922_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20070009922_hide"></p> <p>2006-01-01</p> <p>Two 20-day, continental midlatitude cases are simulated with a three-dimensional (3D) cloud-resolving <span class="hlt">model</span> (CRM) and compared to Atmospheric Radiation <span class="hlt">Measurement</span> (ARM) data. This evaluation of long-term cloud-resolving <span class="hlt">model</span> simulations focuses on the evaluation of clouds and surface fluxes. All numerical experiments, as compared to <span class="hlt">observations</span>, simulate surface precipitation well but over-predict clouds, especially in the upper troposphere. The sensitivity of cloud properties to dimensionality and other factors is studied to isolate the origins of the over prediction of clouds. Due to the difference in buoyancy damping between 2D and 3D <span class="hlt">models</span>, surface precipitation fluctuates rapidly with time, and spurious dehumidification occurs near the tropopause in the 2D CRM. Surface fluxes from a land data assimilation system are compared with ARM <span class="hlt">observations</span>. They are used in place of the ARM surface fluxes to test the sensitivity of simulated clouds to surface fluxes. Summertime simulations show that surface fluxes from the assimilation system bring about a better simulation of diurnal cloud variation in the lower troposphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070030218','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070030218"><span>Evaluation of a Cloud Resolving <span class="hlt">Model</span> Using TRMM <span class="hlt">Observations</span> for Multiscale <span class="hlt">Modeling</span> Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Posselt, Derek J.; L'Ecuyer, Tristan; Tao, Wei-Kuo; Hou, Arthur Y.; Stephens, Graeme L.</p> <p>2007-01-01</p> <p>The climate change simulation community is moving toward use of global cloud resolving <span class="hlt">models</span> (CRMs), however, current computational resources are not sufficient to run global CRMs over the hundreds of years necessary to produce climate change estimates. As an intermediate step between conventional general circulation <span class="hlt">models</span> (GCMs) and global CRMs, many climate analysis centers are embedding a CRM in each grid cell of a conventional GCM. These Multiscale <span class="hlt">Modeling</span> Frameworks (MMFs) represent a theoretical advance over the use of conventional GCM cloud and convection parameterizations, but have been shown to exhibit an overproduction of precipitation in the tropics during the northern hemisphere summer. In this study, simulations of clouds, precipitation, and radiation over the South China Sea using the CRM component of the NASA Goddard MMF are evaluated using retrievals derived from the instruments aboard the Tropical Rainfall <span class="hlt">Measuring</span> Mission (TRMM) satellite platform for a 46-day time period that spans 5 May - 20 June 1998. The NASA Goddard Cumulus Ensemble (GCE) <span class="hlt">model</span> is forced with <span class="hlt">observed</span> largescale forcing derived from soundings taken during the intensive <span class="hlt">observing</span> period of the South China Sea Monsoon Experiment. It is found that the GCE configuration used in the NASA Goddard MMF responds too vigorously to the imposed large-scale forcing, accumulating too much moisture and producing too much cloud cover during convective phases, and overdrying the atmosphere and suppressing clouds during monsoon break periods. Sensitivity experiments reveal that changes to ice cloud microphysical parameters have a relatively large effect on simulated clouds, precipitation, and radiation, while changes to grid spacing and domain length have little effect on simulation results. The results motivate a more detailed and quantitative exploration of the sources and magnitude of the uncertainty associated with specified cloud microphysical parameters in the CRM components of MMFs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H12C..03T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H12C..03T"><span>Process-based <span class="hlt">model</span> with flood control <span class="hlt">measures</span> towards more realistic global flood <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, Q.; Zhang, X.; Wang, Y.; Mu, M.; Lv, A.; Li, Z.</p> <p>2017-12-01</p> <p>In the profoundly human-influenced era, the Anthropocene, increased amount of land was developed in flood plains and many flood control <span class="hlt">measures</span> were implemented to protect people and infrastructures placed in the flood-prone areas. These human influences (for example, dams and dykes) have altered peak streamflow and flood risk, and are already an integral part of flood. However, most of the process-based flood <span class="hlt">models</span> have yet to taken into account the human influences. In this study, we used a hydrological <span class="hlt">model</span> together with an advanced hydrodynamic <span class="hlt">model</span> to assess flood risk at the Baiyangdian catchment. The Baiyangdian Lake is the largest shallow freshwater lake in North China, and it was used as a flood storage area in the past. A new development hub for the Beijing-Tianjin-Hebei economic triangle, namely the Xiongan new area, was recently established in the flood-prone area around the lake. The shuttle radar topography mission (SRTM) digital elevation <span class="hlt">model</span> (DEMs) was used to parameterize the hydrodynamic <span class="hlt">model</span> simulation, and the inundation estimates were compared with published flood maps and <span class="hlt">observed</span> inundation area during the extreme historical flood events. A simple scheme was carried out to consider the impacts of flood control <span class="hlt">measures</span>, including the reservoirs in the headwaters and the dykes to be built. By comparing <span class="hlt">model</span> simulations with and without the influences of flood control <span class="hlt">measures</span>, we demonstrated the importance of human influences in altering the inundated area and depth under design flood conditions. Based on the SRTM DEM and dam and reservoir data in the Global Reservoir and Dam (GRanD) database, we further discuss the potential to develop a global flood <span class="hlt">model</span> with human influences.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhRvD..84g2005A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhRvD..84g2005A"><span><span class="hlt">Measurement</span> of the neutrino component of an antineutrino beam <span class="hlt">observed</span> by a nonmagnetized detector</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aguilar-Arevalo, A. A.; Anderson, C. E.; Brice, S. J.; Brown, B. C.; Bugel, L.; Conrad, J. M.; Dharmapalan, R.; Djurcic, Z.; Fleming, B. T.; Ford, R.; Garcia, F. G.; Garvey, G. T.; Grange, J.; Green, J. A.; Imlay, R.; Johnson, R. A.; Karagiorgi, G.; Katori, T.; Kobilarcik, T.; Linden, S. K.; Louis, W. C.; Mahn, K. B. M.; Marsh, W.; Mauger, C.; Metcalf, W.; Mills, G. B.; Mirabal, J.; Moore, C. D.; Mousseau, J.; Nelson, R. H.; Nguyen, V.; Nienaber, P.; Nowak, J. A.; Osmanov, B.; Patch, A.; Pavlovic, Z.; Perevalov, D.; Polly, C. C.; Ray, H.; Roe, B. P.; Russell, A. D.; Shaevitz, M. H.; Sorel, M.; Spitz, J.; Stancu, I.; Stefanski, R. J.; Tayloe, R.; Tzanov, M.; van de Water, R. G.; Wascko, M. O.; White, D. H.; Wilking, M. J.; Zeller, G. P.; Zimmerman, E. D.</p> <p>2011-10-01</p> <p>Two methods are employed to <span class="hlt">measure</span> the neutrino flux of the antineutrino-mode beam <span class="hlt">observed</span> by the MiniBooNE detector. The first method compares data to simulated event rates in a high-purity νμ-induced charged-current single π+ (CC1π+) sample while the second exploits the difference between the angular distributions of muons created in νμ and ν¯μ charged-current quasielastic (CCQE) interactions. The results from both analyses indicate the prediction of the neutrino flux component of the predominately antineutrino beam is overestimated—the CC1π+ analysis indicates the predicted νμ flux should be scaled by 0.76±0.11, while the CCQE angular fit yields 0.65±0.23. The energy spectrum of the flux prediction is checked by repeating the analyses in bins of reconstructed neutrino energy, and the results show that the spectral shape is well-<span class="hlt">modeled</span>. These analyses are a demonstration of techniques for <span class="hlt">measuring</span> the neutrino contamination of antineutrino beams <span class="hlt">observed</span> by future nonmagnetized detectors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A31B0023W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A31B0023W"><span>Estimating Amazonian methane emissions through 4D-Var inverse <span class="hlt">modelling</span> with satellite <span class="hlt">observations</span> from GOSAT and IASI</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilson, C. J.; Chipperfield, M.; Gloor, M.; McNorton, J.; Miller, J. B.; Gatti, L. V.; Siddans, R.; Bloom, A. A.; Basso, L. S.; Boesch, H.; Parker, R.; Monks, S. A.</p> <p>2015-12-01</p> <p>Methane (CH4) is emitted from a range of anthropogenic and natural sources, and since the industrial revolution its mean atmospheric concentration has climbed dramatically. CH4 produces a relatively high radiative forcing effect upon the Earth's climate, and its atmospheric lifetime of approximately 10 years makes it an appealing target for the mitigation of climate change. However, the spatial and temporal variation of CH4 emissions are not well understood, though in recent years a number of top-down and bottom-up studies have attempted to construct improved emission budgets. However, some top-down studies suffer from poor <span class="hlt">observational</span> coverage near the Amazon basin, particularly in the planetary boundary layer. Since emissions from this region, coming mainly from wetland and burning sources, are thought to be relatively high, additional <span class="hlt">observations</span> in this region would greatly help to constrain the geographical distribution of the global CH4 emission budget. To this end, regular flask <span class="hlt">measurements</span> of CH4 and other trace gases have been taken during flights over four Amazonian sites since 2010, as part of the AMAZONICA project. The GOSAT has been used to retrieve global column-average CH4 concentrations since mid-2009, whilst IASI, on-board Metop-A, has also been <span class="hlt">measuring</span> atmospheric CH4 concentrations since its launch in 2006. We present an assessment of Amazonian methane emissions for 2010 and 2011 using the TOMCAT Chemical Transport <span class="hlt">Model</span> and the new variational inverse <span class="hlt">model</span>, INVICAT. These <span class="hlt">models</span> are used to attribute methane variations at each Amazon site to a source type and region, to assess the ability of our current CH4 flux estimates to reproduce these <span class="hlt">observations</span> and to produce improved posterior emission estimates through assimilation of atmospheric <span class="hlt">observations</span>. This study represents the first use of the INVICAT scheme to constrain emissions of any atmospheric trace gas. Whilst there is generally good agreement between the <span class="hlt">model</span> and the</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70048387','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70048387"><span>A hybrid double-<span class="hlt">observer</span> sightability <span class="hlt">model</span> for aerial surveys</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Griffin, Paul C.; Lubow, Bruce C.; Jenkins, Kurt J.; Vales, David J.; Moeller, Barbara J.; Reid, Mason; Happe, Patricia J.; Mccorquodale, Scott M.; Tirhi, Michelle J.; Schaberi, Jim P.; Beirne, Katherine</p> <p>2013-01-01</p> <p>Raw counts from aerial surveys make no correction for undetected animals and provide no estimate of precision with which to judge the utility of the counts. Sightability <span class="hlt">modeling</span> and double-<span class="hlt">observer</span> (DO) <span class="hlt">modeling</span> are 2 commonly used approaches to account for detection bias and to estimate precision in aerial surveys. We developed a hybrid DO sightability <span class="hlt">model</span> (<span class="hlt">model</span> MH) that uses the strength of each approach to overcome the weakness in the other, for aerial surveys of elk (Cervus elaphus). The hybrid approach uses detection patterns of 2 independent <span class="hlt">observer</span> pairs in a helicopter and telemetry-based detections of collared elk groups. Candidate MH <span class="hlt">models</span> reflected hypotheses about effects of recorded covariates and unmodeled heterogeneity on the separate front-seat <span class="hlt">observer</span> pair and back-seat <span class="hlt">observer</span> pair detection probabilities. Group size and concealing vegetation cover strongly influenced detection probabilities. The pilot's previous experience participating in aerial surveys influenced detection by the front pair of <span class="hlt">observers</span> if the elk group was on the pilot's side of the helicopter flight path. In 9 surveys in Mount Rainier National Park, the raw number of elk counted was approximately 80–93% of the abundance estimated by <span class="hlt">model</span> MH. Uncorrected ratios of bulls per 100 cows generally were low compared to estimates adjusted for detection bias, but ratios of calves per 100 cows were comparable whether based on raw survey counts or adjusted estimates. The hybrid method was an improvement over commonly used alternatives, with improved precision compared to sightability <span class="hlt">modeling</span> and reduced bias compared to DO <span class="hlt">modeling</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.A14D..06J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.A14D..06J"><span>SOA <span class="hlt">Measurements</span> vs. <span class="hlt">Models</span>: a Status Report</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jimenez, J. L.; de Gouw, J. A.</p> <p>2009-12-01</p> <p>The advent of fast and more detailed organic aerosol (OA) and VOC <span class="hlt">measurements</span> in the last decade has allowed clearer <span class="hlt">model-measurement</span> comparisons for OA and secondary OA (SOA). Here we summarize the patterns emerging from studies to date. <li>At least 8 studies have reported a large (x5-10) underestimation of SOA for polluted regions when using traditional <span class="hlt">models</span> (those developed until ~2006) (Heald GRL05, Volkamer GRL06, Johnson ACP06, Kleinman ACP08, Matsui JGR09, Dzepina ACP09, Hodzic ACP09, Tsimpidi ACP09). This is especially obvious when <span class="hlt">models</span> are evaluated with the ΔOA/ΔCO ratio. <li>Close to pollution sources, discrepancies of an order-of-magnitude in SOA lead to smaller discrepancies (often x2-3) for total OA due to the presence of primary OA (de Gouw EST09). Such OA discrepancies have been repeatedly <span class="hlt">observed</span> (e.g. Vutukuru JGR06, McKeen JGR07&09, Heald JGR07, Fast ACP09, Hodzic ACP09). <li>The discrepancy is reduced when recently-updated yields for aromatics (Ng ACP07) and SOA from glyoxal (Volkamer GRL07) are used, and is eliminated when using SOA formation from S/IVOC (Robinson Sci07) although with an overprediction of SOA at long aging times (Dzepina ACP09; Hodzic ACP09b). It is not clear whether the urban discrepancy is removed for the right reasons. <li>4 evaluations of biogenic SOA formed in unpolluted regions find reasonable agreement between SOA from traditional <span class="hlt">models</span> and field <span class="hlt">measurements</span> (Tunved Sci06; Hodzic ACP09; Chen GRL09; Slowik ACPD09). One evaluation reports a significant underprediction (Capes ACP09), although the amount of precursor reacted was difficult to ascertain for that case. The difference with the systematic underprediction <span class="hlt">observed</span> for anthropogenic SOA may be due to the lack of primary S/IVOC in biogenic emissions, or to other reasons (NOx, SO2, POA, etc.). <li>Comparisons for biogenic SOA formed in polluted regions are more complex. Several studies have reported a lack of clear influence of biogenic VOCs in SOA</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20100029638&hterms=kessler&qs=N%3D0%26Ntk%3DAuthor-Name%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dkessler','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20100029638&hterms=kessler&qs=N%3D0%26Ntk%3DAuthor-Name%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dkessler"><span>Updating the NASA LEO Orbital Debris Environment <span class="hlt">Model</span> with Recent Radar and Optical <span class="hlt">Observations</span> and in Situ <span class="hlt">Measurements</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liou, J.-C.; Anz-Meador, P.; Matney, M. J.; Kessler, D. J.; Theall, J.; Johnson, N. L.</p> <p>2000-01-01</p> <p>The Low Earth Orbit (LEO, between 200 and 2000 km altitudes) debris environment has been constantly <span class="hlt">measured</span> by NASA Johnson Space Center's Liquid Mirror Telescope (LMT) since 1996 (Africano et al. 1999, NASA JSC-28826) and by Haystack and Haystack Auxiliary radars at MIT Lincoln Laboratory since 1990 (Settecerri et al. 1999, NASA JSC-28744). Debris particles as small as 3 mm can be detected by the radars and as small as 3 cm can be <span class="hlt">measured</span> by LMT. Objects about 10 cm in diameter and greater are tracked and catalogued by the US Space Surveillance Network. Much smaller (down to several micrometers) natural and debris particle populations can be estimated based on in situ <span class="hlt">measurements</span>, such as Long Duration Exposure Facility, and based on analyses of returned surfaces, such as Hubble Space Telescope solar arrays, European Retrievable Carrier, and Space Shuttles. To increase our understanding of the current LEO debris environment, the Orbital Debris Program Office at NASA JSC has initiated an effort to improve and update the ORDEM96 <span class="hlt">model</span> (Kessler et al. 1996, NASA TM-104825) utilizing the recently available data. This paper gives an overview of the new NASA orbital debris engineering <span class="hlt">model</span>, ORDEM2000.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED319794.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED319794.pdf"><span><span class="hlt">Measurement</span> <span class="hlt">Model</span> Specification Error in LISREL Structural Equation <span class="hlt">Models</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Baldwin, Beatrice; Lomax, Richard</p> <p></p> <p>This LISREL study examines the robustness of the maximum likelihood estimates under varying degrees of <span class="hlt">measurement</span> <span class="hlt">model</span> misspecification. A true <span class="hlt">model</span> containing five latent variables (two endogenous and three exogenous) and two indicator variables per latent variable was used. <span class="hlt">Measurement</span> <span class="hlt">model</span> misspecification considered included errors of…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=bill+AND+gates&pg=3&id=EJ1051313','ERIC'); return false;" href="https://eric.ed.gov/?q=bill+AND+gates&pg=3&id=EJ1051313"><span>The Stability of <span class="hlt">Observational</span> and Student Survey <span class="hlt">Measures</span> of Teaching Effectiveness</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Polikoff, Morgan S.</p> <p>2015-01-01</p> <p>Responding to federal policy and recent research, states and districts have developed and begun implementing multiple-<span class="hlt">measure</span> teacher evaluation systems. These systems generally include <span class="hlt">observational</span> and/or student survey <span class="hlt">measures</span> of instructional quality alongside <span class="hlt">measures</span> of teachers' contributions to student learning (e.g., value-added models…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A53I..02L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A53I..02L"><span>Toward a Tighter Coupling between <span class="hlt">Models</span> and <span class="hlt">Observations</span> of Arctic Energy Balance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>L'Ecuyer, T. S.</p> <p>2016-12-01</p> <p>The Arctic climate is changing more rapidly than almost anywhere else on Earth owing to a number of unique feedbacks that locally amplify the effects of increased greenhouse gas concentrations. While the basic theory behind these feedback mechanisms has been known for a long time, current climate <span class="hlt">models</span> still struggle to capture <span class="hlt">observed</span> rates of sea ice decline and ice sheet melt. This may be explained, at least partially, by a lack of <span class="hlt">observational</span> constraints on cloud and precipitation processes owing to the challenges of making sustained, high quality atmospheric <span class="hlt">measurements</span> in this inhospitable region. This presentation will introduce a new multi-satellite, multi-<span class="hlt">model</span> combined Arctic dataset for probing the state of the Arctic climate and documenting and improving prediction <span class="hlt">models</span>. Recent satellite-based reconstructions of the Arctic energy budget and its annual cycle contained within this dataset will used to demonstrate that many climate <span class="hlt">models</span> exhibit significant biases in several key energy flows in the region. These biases, in turn, lead to discrepancies in both the magnitude and seasonality of the implied heat transport into the Arctic from lower latitudes. The potential impacts of these biases on the surface mass balance of the Greenland Ice Sheet will be explored. New estimates of downwelling radiative fluxes that explicitly account for the effects of super-cooled liquid water <span class="hlt">observed</span> by new active satellite sensors will be used to drive a regional ice sheet <span class="hlt">model</span> to assess the sensitivity of ice sheet dynamical processes to uncertainties in surface radiation balance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1336080-fingerprints-riming-event-cloud-radar-doppler-spectra-observations-modeling','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1336080-fingerprints-riming-event-cloud-radar-doppler-spectra-observations-modeling"><span>Fingerprints of a riming event on cloud radar Doppler spectra: <span class="hlt">observations</span> and <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Kalesse, Heike; Szyrmer, Wanda; Kneifel, Stefan; ...</p> <p>2016-03-09</p> <p>In this paper, Radar Doppler spectra <span class="hlt">measurements</span> are exploited to study a riming event when precipitating ice from a seeder cloud sediment through a supercooled liquid water (SLW) layer. The focus is on the "golden sample" case study for this type of analysis based on <span class="hlt">observations</span> collected during the deployment of the Atmospheric Radiation <span class="hlt">Measurement</span> Program's (ARM) mobile facility AMF2 at Hyytiälä, Finland, during the Biogenic Aerosols – Effects on Clouds and Climate (BAECC) field campaign. The presented analysis of the height evolution of the radar Doppler spectra is a state-of-the-art retrieval with profiling cloud radars in SLW layers beyondmore » the traditional use of spectral moments. Dynamical effects are considered by following the particle population evolution along slanted tracks that are caused by horizontal advection of the cloud under wind shear conditions. In the SLW layer, the identified liquid peak is used as an air motion tracer to correct the Doppler spectra for vertical air motion and the ice peak is used to study the radar profiles of rimed particles. A 1-D steady-state bin microphysical <span class="hlt">model</span> is constrained using the SLW and air motion profiles and cloud top radar <span class="hlt">observations</span>. The <span class="hlt">observed</span> radar moment profiles of the rimed snow can be simulated reasonably well by the <span class="hlt">model</span>, but not without making several assumptions about the ice particle concentration and the relative role of deposition and aggregation. In conclusion, this suggests that in situ <span class="hlt">observations</span> of key ice properties are needed to complement the profiling radar <span class="hlt">observations</span> before process-oriented studies can effectively evaluate ice microphysical parameterizations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvA..91c2110K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvA..91c2110K"><span>Classicality condition on a system <span class="hlt">observable</span> in a quantum <span class="hlt">measurement</span> and a relative-entropy conservation law</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuramochi, Yui; Ueda, Masahito</p> <p>2015-03-01</p> <p>We consider the information flow on a system <span class="hlt">observable</span> X corresponding to a positive-operator-valued <span class="hlt">measure</span> under a quantum <span class="hlt">measurement</span> process Y described by a completely positive instrument from the viewpoint of the relative entropy. We establish a sufficient condition for the relative-entropy conservation law which states that the average decrease in the relative entropy of the system <span class="hlt">observable</span> X equals the relative entropy of the <span class="hlt">measurement</span> outcome of Y , i.e., the information gain due to <span class="hlt">measurement</span>. This sufficient condition is interpreted as an assumption of classicality in the sense that there exists a sufficient statistic in a joint successive <span class="hlt">measurement</span> of Y followed by X such that the probability distribution of the statistic coincides with that of a single <span class="hlt">measurement</span> of X for the premeasurement state. We show that in the case when X is a discrete projection-valued <span class="hlt">measure</span> and Y is discrete, the classicality condition is equivalent to the relative-entropy conservation for arbitrary states. The general theory on the relative-entropy conservation is applied to typical quantum <span class="hlt">measurement</span> <span class="hlt">models</span>, namely, quantum nondemolition <span class="hlt">measurement</span>, destructive sharp <span class="hlt">measurements</span> on two-level systems, a photon counting, a quantum counting, homodyne and heterodyne <span class="hlt">measurements</span>. These examples except for the nondemolition and photon-counting <span class="hlt">measurements</span> do not satisfy the known Shannon-entropy conservation law proposed by Ban [M. Ban, J. Phys. A: Math. Gen. 32, 1643 (1999), 10.1088/0305-4470/32/9/012], implying that our approach based on the relative entropy is applicable to a wider class of quantum <span class="hlt">measurements</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRD..120.5693P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRD..120.5693P"><span><span class="hlt">Measuring</span> and <span class="hlt">modeling</span> the lifetime of nitrous oxide including its variability</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prather, Michael J.; Hsu, Juno; DeLuca, Nicole M.; Jackman, Charles H.; Oman, Luke D.; Douglass, Anne R.; Fleming, Eric L.; Strahan, Susan E.; Steenrod, Stephen D.; Søvde, O. Amund; Isaksen, Ivar S. A.; Froidevaux, Lucien; Funke, Bernd</p> <p>2015-06-01</p> <p>The lifetime of nitrous oxide, the third-most-important human-emitted greenhouse gas, is based to date primarily on <span class="hlt">model</span> studies or scaling to other gases. This work calculates a semiempirical lifetime based on Microwave Limb Sounder satellite <span class="hlt">measurements</span> of stratospheric profiles of nitrous oxide, ozone, and temperature; laboratory cross-section data for ozone and molecular oxygen plus kinetics for O(1D); the <span class="hlt">observed</span> solar spectrum; and a simple radiative transfer <span class="hlt">model</span>. The result is 116 ± 9 years. The <span class="hlt">observed</span> monthly-to-biennial variations in lifetime and tropical abundance are well matched by four independent chemistry-transport <span class="hlt">models</span> driven by reanalysis meteorological fields for the period of <span class="hlt">observation</span> (2005-2010), but all these <span class="hlt">models</span> overestimate the lifetime due to lower abundances in the critical loss region near 32 km in the tropics. These <span class="hlt">models</span> plus a chemistry-climate <span class="hlt">model</span> agree on the nitrous oxide feedback factor on its own lifetime of 0.94 ± 0.01, giving N2O perturbations an effective residence time of 109 years. Combining this new empirical lifetime with <span class="hlt">model</span> estimates of residence time and preindustrial lifetime (123 years) adjusts our best estimates of the human-natural balance of emissions today and improves the accuracy of projected nitrous oxide increases over this century.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017IJAEO..58..278H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017IJAEO..58..278H"><span>Vegetation chlorophyll estimates in the Amazon from multi-angle MODIS <span class="hlt">observations</span> and canopy reflectance <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hilker, Thomas; Galvão, Lênio Soares; Aragão, Luiz E. O. C.; de Moura, Yhasmin M.; do Amaral, Cibele H.; Lyapustin, Alexei I.; Wu, Jin; Albert, Loren P.; Ferreira, Marciel José; Anderson, Liana O.; dos Santos, Victor A. H. F.; Prohaska, Neill; Tribuzy, Edgard; Barbosa Ceron, João Vitor; Saleska, Scott R.; Wang, Yujie; de Carvalho Gonçalves, José Francisco; de Oliveira Junior, Raimundo Cosme; Cardoso Rodrigues, João Victor Figueiredo; Garcia, Maquelle Neves</p> <p>2017-06-01</p> <p>As a preparatory study for future hyperspectral missions that can <span class="hlt">measure</span> canopy chemistry, we introduce a novel approach to investigate whether multi-angle Moderate Resolution Imaging Spectroradiometer (MODIS) data can be used to generate a preliminary database with long-term estimates of chlorophyll. MODIS monthly chlorophyll estimates between 2000 and 2015, derived from a fully coupled canopy reflectance <span class="hlt">model</span> (ProSAIL), were inspected for consistency with eddy covariance fluxes, tower-based hyperspectral images and chlorophyll <span class="hlt">measurements</span>. MODIS chlorophyll estimates from the inverse <span class="hlt">model</span> showed strong seasonal variations across two flux-tower sites in central and eastern Amazon. Marked increases in chlorophyll concentrations were <span class="hlt">observed</span> during the early dry season. Remotely sensed chlorophyll concentrations were correlated to field <span class="hlt">measurements</span> (r2 = 0.73 and r2 = 0.98) but the data deviated from the 1:1 line with root mean square errors (RMSE) ranging from 0.355 μg cm-2 (Tapajós tower) to 0.470 μg cm-2 (Manaus tower). The chlorophyll estimates were consistent with flux tower <span class="hlt">measurements</span> of photosynthetically active radiation (PAR) and net ecosystem productivity (NEP). We also applied ProSAIL to mono-angle hyperspectral <span class="hlt">observations</span> from a camera installed on a tower to scale <span class="hlt">modeled</span> chlorophyll pigments to MODIS <span class="hlt">observations</span> (r2 = 0.73). Chlorophyll pigment concentrations (ChlA+B) were correlated to changes in the amount of young and mature leaf area per month (0.59 ≤ r2 ≤ 0.64). Increases in MODIS <span class="hlt">observed</span> ChlA+B were preceded by increased PAR during the dry season (0.61 ≤ r2 ≤ 0.62) and followed by changes in net carbon uptake. We conclude that, at these two sites, changes in LAI, coupled with changes in leaf chlorophyll, are comparable with seasonality of plant productivity. Our results allowed the preliminary development of a 15-year time series of chlorophyll estimates over the Amazon to support canopy chemistry studies using future</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1240689-measuring-seeds-ion-outflow-auroral-sounding-rocket-observations-low-altitude-ion-heating-circulation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1240689-measuring-seeds-ion-outflow-auroral-sounding-rocket-observations-low-altitude-ion-heating-circulation"><span><span class="hlt">Measuring</span> the seeds of ion outflow: auroral sounding rocket <span class="hlt">observations</span> of low-altitude ion heating and circulation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Fernandes, P. A.; Lynch, K. A.; Zettergren, M.; ...</p> <p>2016-01-25</p> <p>Here, we present an analysis of in situ <span class="hlt">measurements</span> from the MICA (Magnetosphere-Ionosphere Coupling in the Alfvén Resonator) nightside auroral sounding rocket with comparisons to a multifluid ionospheric <span class="hlt">model</span>. MICA made <span class="hlt">observations</span> at altitudes below 325 km of the thermal ion kinetic particle distributions that are the origins of ion outflow. Late flight, in the vicinity of an auroral arc, we <span class="hlt">observe</span> frictional processes controlling the ion temperature. Upflow of these cold ions is attributed to either the ambipolar field resulting from the heated electrons or possibly to ion-neutral collisions. We <span class="hlt">measure</span> E →xB → convection away from the arcmore » (poleward) and downflows of hundreds of m s -1 poleward of this arc, indicating small-scale low-altitude plasma circulation. In the early flight we <span class="hlt">observe</span> DC electromagnetic Poynting flux and associated ELF wave activity influencing the thermal ion temperature in regions of Alfvénic aurora. We <span class="hlt">observe</span> enhanced, anisotropic ion temperatures which we conjecture are caused by transverse heating by wave-particle interactions (WPI) even at these low altitudes. Throughout this region we <span class="hlt">observe</span> several hundred m s -1 upflow of the bulk thermal ions colocated with WPI; however, the mirror force is negligible at these low energies; thus, the upflow is attributed to ambipolar fields (or possibly neutral upwelling drivers). Moreover, the low-altitude MICA <span class="hlt">observations</span> serve to inform future ionospheric <span class="hlt">modeling</span> and simulations of (a) the need to consider the effects of heating by WPI at altitudes lower than previously considered viable and (b) the occurrence of structured and localized upflows/downflows below where higher-altitude heating rocesses are expected.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1240689','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1240689"><span><span class="hlt">Measuring</span> the seeds of ion outflow: auroral sounding rocket <span class="hlt">observations</span> of low-altitude ion heating and circulation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Fernandes, P. A.; Lynch, K. A.; Zettergren, M.</p> <p></p> <p>Here, we present an analysis of in situ <span class="hlt">measurements</span> from the MICA (Magnetosphere-Ionosphere Coupling in the Alfvén Resonator) nightside auroral sounding rocket with comparisons to a multifluid ionospheric <span class="hlt">model</span>. MICA made <span class="hlt">observations</span> at altitudes below 325 km of the thermal ion kinetic particle distributions that are the origins of ion outflow. Late flight, in the vicinity of an auroral arc, we <span class="hlt">observe</span> frictional processes controlling the ion temperature. Upflow of these cold ions is attributed to either the ambipolar field resulting from the heated electrons or possibly to ion-neutral collisions. We <span class="hlt">measure</span> E →xB → convection away from the arcmore » (poleward) and downflows of hundreds of m s -1 poleward of this arc, indicating small-scale low-altitude plasma circulation. In the early flight we <span class="hlt">observe</span> DC electromagnetic Poynting flux and associated ELF wave activity influencing the thermal ion temperature in regions of Alfvénic aurora. We <span class="hlt">observe</span> enhanced, anisotropic ion temperatures which we conjecture are caused by transverse heating by wave-particle interactions (WPI) even at these low altitudes. Throughout this region we <span class="hlt">observe</span> several hundred m s -1 upflow of the bulk thermal ions colocated with WPI; however, the mirror force is negligible at these low energies; thus, the upflow is attributed to ambipolar fields (or possibly neutral upwelling drivers). Moreover, the low-altitude MICA <span class="hlt">observations</span> serve to inform future ionospheric <span class="hlt">modeling</span> and simulations of (a) the need to consider the effects of heating by WPI at altitudes lower than previously considered viable and (b) the occurrence of structured and localized upflows/downflows below where higher-altitude heating rocesses are expected.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26521723','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26521723"><span>Fuzzy <span class="hlt">model</span>-based <span class="hlt">observers</span> for fault detection in CSTR.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ballesteros-Moncada, Hazael; Herrera-López, Enrique J; Anzurez-Marín, Juan</p> <p>2015-11-01</p> <p>Under the vast variety of fuzzy <span class="hlt">model</span>-based <span class="hlt">observers</span> reported in the literature, what would be the properone to be used for fault detection in a class of chemical reactor? In this study four fuzzy <span class="hlt">model</span>-based <span class="hlt">observers</span> for sensor fault detection of a Continuous Stirred Tank Reactor were designed and compared. The designs include (i) a Luenberger fuzzy <span class="hlt">observer</span>, (ii) a Luenberger fuzzy <span class="hlt">observer</span> with sliding modes, (iii) a Walcott-Zak fuzzy <span class="hlt">observer</span>, and (iv) an Utkin fuzzy <span class="hlt">observer</span>. A negative, an oscillating fault signal, and a bounded random noise signal with a maximum value of ±0.4 were used to evaluate and compare the performance of the fuzzy <span class="hlt">observers</span>. The Utkin fuzzy <span class="hlt">observer</span> showed the best performance under the tested conditions. Copyright © 2015 ISA. Published by Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ACP.....5.3093D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ACP.....5.3093D"><span>3-D microphysical <span class="hlt">model</span> studies of Arctic denitrification: comparison with <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davies, S.; Mann, G. W.; Carslaw, K. S.; Chipperfield, M. P.; Kettleborough, J. A.; Santee, M. L.; Oelhaf, H.; Wetzel, G.; Sasano, Y.; Sugita, T.</p> <p>2005-11-01</p> <p>Simulations of Arctic denitrification using a 3-D chemistry-microphysics transport <span class="hlt">model</span> are compared with <span class="hlt">observations</span> for the winters 1994/95, 1996/97 and 1999/2000. The <span class="hlt">model</span> of Denitrification by Lagrangian Particle Sedimentation (DLAPSE) couples the full chemical scheme of the 3-D chemical transport <span class="hlt">model</span>, SLIMCAT, with a nitric acid trihydrate (NAT) growth and sedimentation scheme. We use <span class="hlt">observations</span> from the Microwave Limb Sounder (MLS) and Improved Limb Atmospheric Sounder (ILAS) satellite instruments, the balloon-borne Michelsen Interferometer for Passive Atmospheric Sounding (MIPAS-B), and the in situ NOy instrument on-board the ER-2. As well as directly comparing <span class="hlt">model</span> results with <span class="hlt">observations</span>, we also assess the extent to which these <span class="hlt">observations</span> are able to validate the <span class="hlt">modelling</span> approach taken. For instance, in 1999/2000 the <span class="hlt">model</span> captures the temporal development of denitrification <span class="hlt">observed</span> by the ER-2 from late January into March. However, in this winter the vortex was already highly denitrified by late January so the <span class="hlt">observations</span> do not provide a strong constraint on the <span class="hlt">modelled</span> rate of denitrification. The <span class="hlt">model</span> also reproduces the MLS <span class="hlt">observations</span> of denitrification in early February 2000. In 1996/97 the <span class="hlt">model</span> captures the timing and magnitude of denitrification as <span class="hlt">observed</span> by ILAS, although the lack of <span class="hlt">observations</span> north of ~67° N in the beginning of February make it difficult to constrain the actual timing of onset. The comparison for this winter does not support previous conclusions that denitrification must be caused by an ice-mediated process. In 1994/95 the <span class="hlt">model</span> notably underestimates the magnitude of denitrification <span class="hlt">observed</span> during a single balloon flight of the MIPAS-B instrument. Agreement between <span class="hlt">model</span> and MLS HNO3 at 68 hPa in mid-February 1995 is significantly better. Sensitivity tests show that a 1.5 K overall decrease in vortex temperatures, or a factor 4 increase in assumed NAT nucleation rates, produce the best statistical</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ACPD....5..347D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ACPD....5..347D"><span>3-D microphysical <span class="hlt">model</span> studies of Arctic denitrification: comparison with <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davies, S.; Mann, G. W.; Carslaw, K. S.; Chipperfield, M. P.; Kettleborough, J. A.; Santee, M. L.; Oelhaf, H.; Wetzel, G.; Sasano, Y.; Sugita, T.</p> <p>2005-01-01</p> <p>Simulations of Arctic denitrification using a 3-D chemistry-microphysics transport <span class="hlt">model</span> are compared with <span class="hlt">observations</span> for the winters 1994/1995, 1996/1997 and 1999/2000. The <span class="hlt">model</span> of Denitrification by Lagrangian Particle Sedimentation (DLAPSE) couples the full chemical scheme of the 3-D chemical transport <span class="hlt">model</span>, SLIMCAT, with a nitric acid trihydrate (NAT) growth and sedimentation scheme. We use <span class="hlt">observations</span> from the Microwave Limb Sounder (MLS) and Improved Limb Atmospheric Sounder (ILAS) satellite instruments, the balloon-borne Michelsen Interferometer for Passive Atmospheric Sounding (MIPAS-B), and the in situ NOy instrument on-board the ER-2. As well as directly comparing <span class="hlt">model</span> results with <span class="hlt">observations</span>, we also assess the extent to which these <span class="hlt">observations</span> are able to validate the <span class="hlt">modelling</span> approach taken. For instance, in 1999/2000 the <span class="hlt">model</span> captures the temporal development of denitrification <span class="hlt">observed</span> by the ER-2 from late January into March. However, in this winter the vortex was already highly denitrified by late January so the <span class="hlt">observations</span> do not provide a strong constraint on the <span class="hlt">modelled</span> rate of denitrification. The <span class="hlt">model</span> also reproduces the MLS <span class="hlt">observations</span> of denitrification in early February 2000. In 1996/1997 the <span class="hlt">model</span> captures the timing and magnitude of denitrification as <span class="hlt">observed</span> by ILAS, although the lack of <span class="hlt">observations</span> north of ~67° N make it difficult to constrain the actual timing of onset. The comparison for this winter does not support previous conclusions that denitrification must be caused by an ice-mediated process. In 1994/1995 the <span class="hlt">model</span> notably underestimates the magnitude of denitrification <span class="hlt">observed</span> during a single balloon flight of the MIPAS-B instrument. Agreement between <span class="hlt">model</span> and MLS HNO3 at 68 hPa in mid-February 1995 was significantly better. Sensitivity tests show that a 1.5 K overall decrease in vortex temperatures or a factor 4 increase in assumed NAT nucleation rates produce the best statistical fit to MLS <span class="hlt">observations</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4199927','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4199927"><span><span class="hlt">Observational</span> <span class="hlt">Measures</span> of Implementer Fidelity for a School-based Preventive Intervention: Development, Reliability and Validity</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Cross, Wendi; West, Jennifer; Wyman, Peter A.; Schmeelk-Cone, Karen; Xia, Yinglin; Tu, Xin; Teisl, Michael; Brown, C. Hendricks; Forgatch, Marion</p> <p>2014-01-01</p> <p>Current <span class="hlt">measures</span> of implementer fidelity often fail to adequately <span class="hlt">measure</span> core constructs of adherence and competence, and their relationship to outcomes can be mixed. To address these limitations, we used <span class="hlt">observational</span> methods to assess these constructs and their relationships to proximal outcomes in a randomized trial of a school-based preventive intervention (Rochester Resilience Project) designed to strengthen emotion self-regulation skills in 1st–3rd graders with elevated aggressive-disruptive behaviors. Within the intervention group (n = 203), a subsample (n = 76) of students was selected to reflect the overall sample. Implementers were 10 paraprofessionals. Videotaped <span class="hlt">observations</span> of three lessons from Year 1 of the intervention (14 lessons) were coded for each implementer-child dyad on Adherence (content) and Competence (quality). Using multi-level <span class="hlt">modeling</span> we examined how much of the variance in the fidelity <span class="hlt">measures</span> was attributed to implementer and to the child within implementer. Both <span class="hlt">measures</span> had large and significant variance accounted for by implementer (Competence, 68%; Adherence, 41%); child within implementer did not account for significant variance indicating that ratings reflected stable qualities of the implementer rather than the child. Raw Adherence and Competence scores shared 46% of variance (r = .68). Controlling for baseline differences and age, the amount (Adherence) and quality (Competence) of program delivered predicted children’s enhanced response to the intervention on both child and parent reports after six months, but not on teacher report of externalizing behavior. Our findings support the use of multiple <span class="hlt">observations</span> for <span class="hlt">measuring</span> fidelity and that adherence and competence are important components of fidelity which could be assessed by many programs using these methods. PMID:24736951</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29768698','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29768698"><span>Financial Viability of Emergency Department <span class="hlt">Observation</span> Unit Billing <span class="hlt">Models</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Baugh, Christopher W; Suri, Pawan; Caspers, Christopher G; Granovsky, Michael A; Neal, Keith; Ross, Michael A</p> <p>2018-05-16</p> <p>Outpatients receive <span class="hlt">observation</span> services to determine the need for inpatient admission. These services are usually provided without the use of condition-specific protocols and in an unstructured manner, scattered throughout a hospital in areas typically designated for inpatient care. Emergency department <span class="hlt">observation</span> units (EDOUs) use protocolized care to offer an efficient alternative with shorter lengths of stay, lower costs and higher patient satisfaction. EDOU growth is limited by existing policy barriers that prevent a "two-service" <span class="hlt">model</span> of separate professional billing for both emergency and <span class="hlt">observation</span> services. The majority of EDOUs use the "one-service" <span class="hlt">model</span>, where a single composite professional fee is billed for both emergency and <span class="hlt">observation</span> services. The financial implications of these <span class="hlt">models</span> are not well understood. We created a Monte Carlo simulation by building a <span class="hlt">model</span> that reflects current clinical practice in the United States and uses inputs gathered from the most recently available peer-reviewed literature, national survey and payer data. Using this simulation, we <span class="hlt">modeled</span> annual staffing costs and payments for professional services under two common <span class="hlt">models</span> of care in an EDOU. We also <span class="hlt">modeled</span> cash flows over a continuous range of daily EDOU patient encounters to illustrate the dynamic relationship between costs and revenue over various staffing levels. We estimate the mean (±SD) annual net cash flow to be a net loss of $315,382 ±$89,635 in the one-service <span class="hlt">model</span> and a net profit of $37,569 ±$359,583 in the two-service <span class="hlt">model</span>. The two-service <span class="hlt">model</span> is financially sustainable at daily billable encounters above 20 while in the one-service <span class="hlt">model</span>, costs exceed revenue regardless of encounter count. Physician cost per hour and daily patient encounters had the most significant impact on <span class="hlt">model</span> estimates. In the one-service <span class="hlt">model</span>, EDOU staffing costs exceed payments at all levels of patient encounters, making a hospital subsidy necessary to create a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017InAgr..31..231S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017InAgr..31..231S"><span><span class="hlt">Observed</span> and <span class="hlt">modelled</span> solar radiation components in sugarcane crop grown under tropical conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Santos, Marcos A. dos; Souza, José L. de; Lyra, Gustavo B.; Teodoro, Iêdo; Ferreira, Ricardo A.; Santos Almeida, Alexsandro C. dos; Lyra, Guilherme B.; Souza, Renan C. de; Lemes, Marco A. Maringolo</p> <p>2017-04-01</p> <p>The net radiation over vegetated surfaces is one of the major input variables in many <span class="hlt">models</span> of soil evaporation, evapotranspiration as well as leaf wetness duration. In the literature there are relatively few studies on net radiation over sugarcane crop in tropical climates. The main objective of the present study was to assess the solar radiation components <span class="hlt">measured</span> and <span class="hlt">modelled</span> for two crop stages of a sugarcane crop in the region of Rio Largo, Alagoas, North-eastern Brazil. The <span class="hlt">measurements</span> of the radiation components were made with a net radiometer during the dry and rainy seasons and two <span class="hlt">models</span> were used to estimate net radiation: the Ortega-Farias <span class="hlt">model</span> and the Monteith and Unsworth <span class="hlt">model</span>. The highest values of net radiation were <span class="hlt">observed</span> at the crop development stage, due mainly to the high indices of incoming solar radiation. The daily average albedos of sugarcane at the crop development and mid-season stages were 0.16 and 0.20, respectively. Both <span class="hlt">models</span> showed a better fit for the crop development stage than for the mid-season stage. When they were inter-compared, Monteith and Unsworth <span class="hlt">model</span> was more efficient than Ortega-Farias <span class="hlt">model</span>, despite the dispersion of their simulated radiation components which was similar.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870020417','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870020417"><span><span class="hlt">Measurement</span>-based reliability/performability <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hsueh, Mei-Chen</p> <p>1987-01-01</p> <p><span class="hlt">Measurement</span>-based <span class="hlt">models</span> based on real error-data collected on a multiprocessor system are described. <span class="hlt">Model</span> development from the raw error-data to the estimation of cumulative reward is also described. A workload/reliability <span class="hlt">model</span> is developed based on low-level error and resource usage data collected on an IBM 3081 system during its normal operation in order to evaluate the resource usage/error/recovery process in a large mainframe system. Thus, both normal and erroneous behavior of the system are <span class="hlt">modeled</span>. The results provide an understanding of the different types of errors and recovery processes. The <span class="hlt">measured</span> data show that the holding times in key operational and error states are not simple exponentials and that a semi-Markov process is necessary to <span class="hlt">model</span> the system behavior. A sensitivity analysis is performed to investigate the significance of using a semi-Markov process, as opposed to a Markov process, to <span class="hlt">model</span> the <span class="hlt">measured</span> system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFMOS62E..08S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFMOS62E..08S"><span>Surfzone Currents Over Irregular Bathymetry: Drifter <span class="hlt">Observations</span> and Numerical <span class="hlt">Model</span> Results</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmidt, W. E.; Slinn, D. N.; Guza, R. T.</p> <p>2002-12-01</p> <p>Surfzone currents on alongshore variable bathymetry were <span class="hlt">observed</span> with recently developed GPS-tracked drifters and numerically <span class="hlt">modeled</span> with the time-dependent, nonlinear shallow water equations. These currents, forced by alongshore inhomogeneous pressure and radiation stress gradients, contain flow features difficult to resolve with fixed instrument arrays, such as rips, eddies, and meanders. Drifters were repeatedly released and recovered near Scripps Beach, La Jolla, California, in July 2000, 2001, and 2002. The most recent deployment of 10 drifters yielded about 32 hours of drifter data for each 5 hour deployment day. Offshore wave heights were moderate, between 0.3-1.0 m. The bathymetry, <span class="hlt">measured</span> over a 600-700 m alongshore span with a GPS- and sonar-equipped jetski (2001 and 2002 deployments), was alongshore inhomogeneous primarily where an irregularly shaped bar-trough feature spanned the surf zone. The <span class="hlt">model</span> simulations suggest that the alongshore inhomogeneous bathymetry strongly influences the location and strength of the <span class="hlt">observed</span> flow features. Research supported by the California Sea Grant College Program and the Office of Naval Research.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820006118','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820006118"><span><span class="hlt">Observational</span> data needs useful for <span class="hlt">modeling</span> the coma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Huebner, W. F.; Giguere, P. T.</p> <p>1981-01-01</p> <p>A computer <span class="hlt">model</span> of comet comae is described; results from assumed composition of frozen gases are summarized and compared to coma <span class="hlt">observations</span>. Restrictions on relative abundance of some frozen constituents are illustrated. <span class="hlt">Modeling</span>, when tightly coupled to <span class="hlt">observational</span> data, can be important for comprehensive analysis of <span class="hlt">observations</span>, for predicting undetected molecular species and for improved understanding of coma and nucleus. To accomplish this, total gas production rates and relative elemental abundances of H:C:N:O:S are needed as a function of heliocentric distance of the comet. Also needed are relative column densitites and column density profiles with well defined diaphragm range and pointing position on the coma. Production rates are less desirable since they are <span class="hlt">model</span> dependent. Total number (or upper limits) of molecules in the coma and analysis of unidentified spectral lines are needed also.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5550725','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5550725"><span>A New Strategy in <span class="hlt">Observer</span> <span class="hlt">Modeling</span> for Greenhouse Cucumber Seedling Growth</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Qiu, Quan; Zheng, Chenfei; Wang, Wenping; Qiao, Xiaojun; Bai, He; Yu, Jingquan; Shi, Kai</p> <p>2017-01-01</p> <p>State <span class="hlt">observer</span> is an essential component in computerized control loops for greenhouse-crop systems. However, the current accomplishments of <span class="hlt">observer</span> <span class="hlt">modeling</span> for greenhouse-crop systems mainly focus on mass/energy balance, ignoring physiological responses of crops. As a result, state <span class="hlt">observers</span> for crop physiological responses are rarely developed, and control operations are typically made based on experience rather than actual crop requirements. In addition, existing <span class="hlt">observer</span> <span class="hlt">models</span> require a large number of parameters, leading to heavy computational load and poor application feasibility. To address these problems, we present a new state <span class="hlt">observer</span> <span class="hlt">modeling</span> strategy that takes both environmental information and crop physiological responses into consideration during the <span class="hlt">observer</span> <span class="hlt">modeling</span> process. Using greenhouse cucumber seedlings as an instance, we sample 10 physiological parameters of cucumber seedlings at different time point during the exponential growth stage, and employ them to build growth state <span class="hlt">observers</span> together with 8 environmental parameters. Support vector machine (SVM) acts as the mathematical tool for <span class="hlt">observer</span> <span class="hlt">modeling</span>. Canonical correlation analysis (CCA) is used to select the dominant environmental and physiological parameters in the <span class="hlt">modeling</span> process. With the dominant parameters, simplified <span class="hlt">observer</span> <span class="hlt">models</span> are built and tested. We conduct contrast experiments with different input parameter combinations on simplified and un-simplified <span class="hlt">observers</span>. Experimental results indicate that physiological information can improve the prediction accuracies of the growth state <span class="hlt">observers</span>. Furthermore, the simplified <span class="hlt">observer</span> <span class="hlt">models</span> can give equivalent or even better performance than the un-simplified ones, which verifies the feasibility of CCA. The current study can enable state <span class="hlt">observers</span> to reflect crop requirements and make them feasible for applications with simplified shapes, which is significant for developing intelligent greenhouse control systems for modern</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28848565','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28848565"><span>A New Strategy in <span class="hlt">Observer</span> <span class="hlt">Modeling</span> for Greenhouse Cucumber Seedling Growth.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Qiu, Quan; Zheng, Chenfei; Wang, Wenping; Qiao, Xiaojun; Bai, He; Yu, Jingquan; Shi, Kai</p> <p>2017-01-01</p> <p>State <span class="hlt">observer</span> is an essential component in computerized control loops for greenhouse-crop systems. However, the current accomplishments of <span class="hlt">observer</span> <span class="hlt">modeling</span> for greenhouse-crop systems mainly focus on mass/energy balance, ignoring physiological responses of crops. As a result, state <span class="hlt">observers</span> for crop physiological responses are rarely developed, and control operations are typically made based on experience rather than actual crop requirements. In addition, existing <span class="hlt">observer</span> <span class="hlt">models</span> require a large number of parameters, leading to heavy computational load and poor application feasibility. To address these problems, we present a new state <span class="hlt">observer</span> <span class="hlt">modeling</span> strategy that takes both environmental information and crop physiological responses into consideration during the <span class="hlt">observer</span> <span class="hlt">modeling</span> process. Using greenhouse cucumber seedlings as an instance, we sample 10 physiological parameters of cucumber seedlings at different time point during the exponential growth stage, and employ them to build growth state <span class="hlt">observers</span> together with 8 environmental parameters. Support vector machine (SVM) acts as the mathematical tool for <span class="hlt">observer</span> <span class="hlt">modeling</span>. Canonical correlation analysis (CCA) is used to select the dominant environmental and physiological parameters in the <span class="hlt">modeling</span> process. With the dominant parameters, simplified <span class="hlt">observer</span> <span class="hlt">models</span> are built and tested. We conduct contrast experiments with different input parameter combinations on simplified and un-simplified <span class="hlt">observers</span>. Experimental results indicate that physiological information can improve the prediction accuracies of the growth state <span class="hlt">observers</span>. Furthermore, the simplified <span class="hlt">observer</span> <span class="hlt">models</span> can give equivalent or even better performance than the un-simplified ones, which verifies the feasibility of CCA. The current study can enable state <span class="hlt">observers</span> to reflect crop requirements and make them feasible for applications with simplified shapes, which is significant for developing intelligent greenhouse control systems for modern</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999JGR...10419881C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999JGR...10419881C"><span>Latitudinally dependent Trimpi effects: <span class="hlt">Modeling</span> and <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Clilverd, Mark A.; Yeo, Richard F.; Nunn, David; Smith, Andy J.</p> <p>1999-09-01</p> <p><span class="hlt">Modeling</span> studies show that the exclusion of the propagating VLF wave from the ionospheric region results in the decline of Trimpi magnitude with patch altitude. In large <span class="hlt">models</span> such as Long Wave Propagation Capability (LWPC) this exclusion does not occur inherently in the code, and high-altitude precipitation <span class="hlt">modeling</span> can produce results that are not consistent with <span class="hlt">observations</span> from ground-based experiments. The introduction to LWPC of realistic wave attenuation of the height gain functions in the ionosphere solves these computational problems. This work presents the first <span class="hlt">modeling</span> of (Born) Trimpi scattering at long ranges, taking into account global inhomogeneities and continuous mode conversion along all paths, by employing the full conductivity perturbation matrix. The application of the more realistic height gain functions allows the prediction of decreasing Trimpi activity with increasing latitude, primarily through the mechanism of excluding the VLF wave from regions of high conductivity and scattering efficiency. Ground-based <span class="hlt">observations</span> from Faraday and Rothera, Antarctica, in September and October 1995 of Trimpi occurring on the NPM (Hawaii) path provide data that are consistent with these predictions. Latitudinal variations in Trimpi occurrence near L=2.5, with a significant decrease of about 70% occurrence between L=2.4 and L=2.8, have been <span class="hlt">observed</span> at higher L shell resolution than in previous studies (i.e., 2<L<3).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010074719','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010074719"><span>Comparison of Columnar Water Vapor <span class="hlt">Measurements</span> During The Fall 1997 ARM Intensive <span class="hlt">Observation</span> Period: Solar Transmittance Methods</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schmid, B.; Michalsky, J. J.; Slater, D. W.; Barnard, J. C.; Halthore, R. N.; Liljegren, J. C.; Holben, B. N.; Eck, T. F.; Livingston, J. M.; Russell, P. B.</p> <p>2000-01-01</p> <p>In the fall of 1997, during an Intensive <span class="hlt">Observation</span> Period (IOP), the Atmospheric Radiation <span class="hlt">Measurement</span> (ARM) program conducted a study of water vapor abundance <span class="hlt">measurement</span> at its Southern Great Plains (SGP) site. Among a large number of instruments, four sun-tracking radiometers were present to <span class="hlt">measure</span> the columnar water vapor (CWV). All four solar radiometers retrieve CWV by <span class="hlt">measuring</span> total solar transmittance in the 0.94-gm water vapor absorption band and subtracting contributions due to Rayleigh, ozone and aerosol transmittances. The aerosol optical depth comparisons among the same four radiometers has been presented elsewhere (Geophys. Res. Lett., 26, 17, 2725-2728, 1999). We have used three different methods to retrieve CWV. In a first round of comparison no attempt was made to standardize on the same radiative transfer <span class="hlt">model</span> and its underlying water vapor spectroscopy. In the second round of comparison we used the same line-by-line code (which includes recently corrected H2O spectroscopy) to retrieve CAN from all four suntracking radiometers. This decreased the mean CWV by 8% or 13%. The spread of 8% in the solar radiometer results found when using the same <span class="hlt">model</span> is an indication of the other-than-<span class="hlt">model</span> uncertainties involved in determining CWV from solar transmittance <span class="hlt">measurements</span> with current instrumentation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1413327S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1413327S"><span>Wave-induced boundary-layer separation: A case study comparing airborne <span class="hlt">observations</span> and results from a mesoscale <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Strauss, L.; Serafin, S.; Grubišić, V.</p> <p>2012-04-01</p> <p>Wave-induced boundary-layer separation (BLS) results from the adverse-pressure gradient forces that are exerted on the atmospheric boundary-layer by internal gravity waves in flow over orography. BLS has received significant attention in recent years, particularly so, because it is a key ingredient in the formation of atmospheric rotors. Traditionally depicted as horizontal eddies in the lee of mountain ranges, rotors originate from the interaction between internal gravity waves and the atmospheric boundary-layer. Our study focuses on the first <span class="hlt">observationally</span> documented case of wave-induced BLS, which occurred on 26 Jan 2006 in the lee of the Medicine Bow Mountains in SE Wyoming (USA). <span class="hlt">Observations</span> from the University of Wyoming King Air (UWKA) aircraft, in particular, the remote sensing <span class="hlt">measurements</span> with the Wyoming Cloud Radar (WCR), reveal strong wave activity, downslope winds in excess of 30 m/s, and near-surface flow reversal in the lee of the mountain range. The fine resolution of WCR data (on the order of 40x40 m2 for two-dimensional velocity fields) exhibits fine-scale vortical structures ("subrotors") which are embedded within the main rotor zone. Our case study intends to complete the characterisation of the <span class="hlt">observed</span> boundary-layer separation event. <span class="hlt">Modelling</span> of the event with the mesoscale Weather Research and Forecast <span class="hlt">Model</span> (WRF) provides insight into the mesoscale triggers of wave-induced BLS and turbulence generation. Indeed, the mesoscale <span class="hlt">model</span> underpins the expected concurrence of the essential processes (gravity waves, wave breaking, downslope windstorms, etc.) leading to BLS. To exploit the recorded in situ and radar data to their full extent, a quantitative evaluation of the structure and intensity of turbulence is conducted by means of a power spectral analysis of the vertical wind component, <span class="hlt">measured</span> along the flight track. An intercomparison of <span class="hlt">observational</span> and <span class="hlt">modelling</span> results serves the purpose of <span class="hlt">model</span> verification and can shed some more</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120001749','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120001749"><span>Ares I Scale <span class="hlt">Model</span> Acoustic Tests Instrumentation for Acoustic and Pressure <span class="hlt">Measurements</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vargas, Magda B.; Counter, Douglas D.</p> <p>2011-01-01</p> <p>The Ares I Scale <span class="hlt">Model</span> Acoustic Test (ASMAT) was a development test performed at the Marshall Space Flight Center (MSFC) East Test Area (ETA) Test Stand 116. The test article included a 5% scale Ares I vehicle <span class="hlt">model</span> and tower mounted on the Mobile Launcher. Acoustic and pressure data were <span class="hlt">measured</span> by approximately 200 instruments located throughout the test article. There were four primary ASMAT instrument suites: ignition overpressure (IOP), lift-off acoustics (LOA), ground acoustics (GA), and spatial correlation (SC). Each instrumentation suite incorporated different sensor <span class="hlt">models</span> which were selected based upon <span class="hlt">measurement</span> requirements. These requirements included the type of <span class="hlt">measurement</span>, exposure to the environment, instrumentation check-outs and data acquisition. The sensors were attached to the test article using different mounts and brackets dependent upon the location of the sensor. This presentation addresses the <span class="hlt">observed</span> effect of the sensors and mounts on the acoustic and pressure <span class="hlt">measurements</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5891330','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5891330"><span>Confronting weather and climate <span class="hlt">models</span> with <span class="hlt">observational</span> data from soil moisture networks over the United States</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Dirmeyer, Paul A.; Wu, Jiexia; Norton, Holly E.; Dorigo, Wouter A.; Quiring, Steven M.; Ford, Trenton W.; Santanello, Joseph A.; Bosilovich, Michael G.; Ek, Michael B.; Koster, Randal D.; Balsamo, Gianpaolo; Lawrence, David M.</p> <p>2018-01-01</p> <p>Four land surface <span class="hlt">models</span> in uncoupled and coupled configurations are compared to <span class="hlt">observations</span> of daily soil moisture from 19 networks in the conterminous United States to determine the viability of such comparisons and explore the characteristics of <span class="hlt">model</span> and <span class="hlt">observational</span> data. First, <span class="hlt">observations</span> are analyzed for error characteristics and representation of spatial and temporal variability. Some networks have multiple stations within an area comparable to <span class="hlt">model</span> grid boxes; for those we find that aggregation of stations before calculation of statistics has little effect on estimates of variance, but soil moisture memory is sensitive to aggregation. Statistics for some networks stand out as unlike those of their neighbors, likely due to differences in instrumentation, calibration and maintenance. Buried sensors appear to have less random error than near-field remote sensing techniques, and heat dissipation sensors show less temporal variability than other types. <span class="hlt">Model</span> soil moistures are evaluated using three metrics: standard deviation in time, temporal correlation (memory) and spatial correlation (length scale). <span class="hlt">Models</span> do relatively well in capturing large-scale variability of metrics across climate regimes, but poorly reproduce <span class="hlt">observed</span> patterns at scales of hundreds of kilometers and smaller. Uncoupled land <span class="hlt">models</span> do no better than coupled <span class="hlt">model</span> configurations, nor do reanalyses outperform free-running <span class="hlt">models</span>. Spatial decorrelation scales are found to be difficult to diagnose. Using data for <span class="hlt">model</span> validation, calibration or data assimilation from multiple soil moisture networks with different types of sensors and <span class="hlt">measurement</span> techniques requires great caution. Data from <span class="hlt">models</span> and <span class="hlt">observations</span> should be put on the same spatial and temporal scales before comparison. PMID:29645013</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170003079','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170003079"><span>Confronting Weather and Climate <span class="hlt">Models</span> with <span class="hlt">Observational</span> Data from Soil Moisture Networks over the United States</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dirmeyer, Paul A.; Wu, Jiexia; Norton, Holly E.; Dorigo, Wouter A.; Quiring, Steven M.; Ford, Trenton W.; Santanello, Joseph A., Jr.; Bosilovich, Michael G.; Ek, Michael B.; Koster, Randal Dean; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003079'); toggleEditAbsImage('author_20170003079_show'); toggleEditAbsImage('author_20170003079_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003079_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003079_hide"></p> <p>2016-01-01</p> <p>Four land surface <span class="hlt">models</span> in uncoupled and coupled configurations are compared to <span class="hlt">observations</span> of daily soil moisture from 19 networks in the conterminous United States to determine the viability of such comparisons and explore the characteristics of <span class="hlt">model</span> and <span class="hlt">observational</span> data. First, <span class="hlt">observations</span> are analyzed for error characteristics and representation of spatial and temporal variability. Some networks have multiple stations within an area comparable to <span class="hlt">model</span> grid boxes; for those we find that aggregation of stations before calculation of statistics has little effect on estimates of variance, but soil moisture memory is sensitive to aggregation. Statistics for some networks stand out as unlike those of their neighbors, likely due to differences in instrumentation, calibration and maintenance. Buried sensors appear to have less random error than near-field remote sensing techniques, and heat dissipation sensors show less temporal variability than other types. <span class="hlt">Model</span> soil moistures are evaluated using three metrics: standard deviation in time, temporal correlation (memory) and spatial correlation (length scale). <span class="hlt">Models</span> do relatively well in capturing large-scale variability of metrics across climate regimes, but poorly reproduce <span class="hlt">observed</span> patterns at scales of hundreds of kilometers and smaller. Uncoupled land <span class="hlt">models</span> do no better than coupled <span class="hlt">model</span> configurations, nor do reanalyses out perform free-running <span class="hlt">models</span>. Spatial decorrelation scales are found to be difficult to diagnose. Using data for <span class="hlt">model</span> validation, calibration or data assimilation from multiple soil moisture networks with different types of sensors and <span class="hlt">measurement</span> techniques requires great caution. Data from <span class="hlt">models</span> and <span class="hlt">observations</span> should be put on the same spatial and temporal scales before comparison.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29645013','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29645013"><span>Confronting weather and climate <span class="hlt">models</span> with <span class="hlt">observational</span> data from soil moisture networks over the United States.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dirmeyer, Paul A; Wu, Jiexia; Norton, Holly E; Dorigo, Wouter A; Quiring, Steven M; Ford, Trenton W; Santanello, Joseph A; Bosilovich, Michael G; Ek, Michael B; Koster, Randal D; Balsamo, Gianpaolo; Lawrence, David M</p> <p>2016-04-01</p> <p>Four land surface <span class="hlt">models</span> in uncoupled and coupled configurations are compared to <span class="hlt">observations</span> of daily soil moisture from 19 networks in the conterminous United States to determine the viability of such comparisons and explore the characteristics of <span class="hlt">model</span> and <span class="hlt">observational</span> data. First, <span class="hlt">observations</span> are analyzed for error characteristics and representation of spatial and temporal variability. Some networks have multiple stations within an area comparable to <span class="hlt">model</span> grid boxes; for those we find that aggregation of stations before calculation of statistics has little effect on estimates of variance, but soil moisture memory is sensitive to aggregation. Statistics for some networks stand out as unlike those of their neighbors, likely due to differences in instrumentation, calibration and maintenance. Buried sensors appear to have less random error than near-field remote sensing techniques, and heat dissipation sensors show less temporal variability than other types. <span class="hlt">Model</span> soil moistures are evaluated using three metrics: standard deviation in time, temporal correlation (memory) and spatial correlation (length scale). <span class="hlt">Models</span> do relatively well in capturing large-scale variability of metrics across climate regimes, but poorly reproduce <span class="hlt">observed</span> patterns at scales of hundreds of kilometers and smaller. Uncoupled land <span class="hlt">models</span> do no better than coupled <span class="hlt">model</span> configurations, nor do reanalyses outperform free-running <span class="hlt">models</span>. Spatial decorrelation scales are found to be difficult to diagnose. Using data for <span class="hlt">model</span> validation, calibration or data assimilation from multiple soil moisture networks with different types of sensors and <span class="hlt">measurement</span> techniques requires great caution. Data from <span class="hlt">models</span> and <span class="hlt">observations</span> should be put on the same spatial and temporal scales before comparison.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1806n0001S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1806n0001S"><span>An approach based on Hierarchical Bayesian Graphical <span class="hlt">Models</span> for <span class="hlt">measurement</span> interpretation under uncertainty</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Skataric, Maja; Bose, Sandip; Zeroug, Smaine; Tilke, Peter</p> <p>2017-02-01</p> <p>It is not uncommon in the field of non-destructive evaluation that multiple <span class="hlt">measurements</span> encompassing a variety of modalities are available for analysis and interpretation for determining the underlying states of nature of the materials or parts being tested. Despite and sometimes due to the richness of data, significant challenges arise in the interpretation manifested as ambiguities and inconsistencies due to various uncertain factors in the physical properties (inputs), environment, <span class="hlt">measurement</span> device properties, human errors, and the <span class="hlt">measurement</span> data (outputs). Most of these uncertainties cannot be described by any rigorous mathematical means, and <span class="hlt">modeling</span> of all possibilities is usually infeasible for many real time applications. In this work, we will discuss an approach based on Hierarchical Bayesian Graphical <span class="hlt">Models</span> (HBGM) for the improved interpretation of complex (multi-dimensional) problems with parametric uncertainties that lack usable physical <span class="hlt">models</span>. In this setting, the input space of the physical properties is specified through prior distributions based on domain knowledge and expertise, which are represented as Gaussian mixtures to <span class="hlt">model</span> the various possible scenarios of interest for non-destructive testing applications. Forward <span class="hlt">models</span> are then used offline to generate the expected distribution of the proposed <span class="hlt">measurements</span> which are used to train a hierarchical Bayesian network. In Bayesian analysis, all <span class="hlt">model</span> parameters are treated as random variables, and inference of the parameters is made on the basis of posterior distribution given the <span class="hlt">observed</span> data. Learned parameters of the posterior distribution obtained after the training can therefore be used to build an efficient classifier for differentiating new <span class="hlt">observed</span> data in real time on the basis of pre-trained <span class="hlt">models</span>. We will illustrate the implementation of the HBGM approach to ultrasonic <span class="hlt">measurements</span> used for cement evaluation of cased wells in the oil industry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1417280-evaluation-cloud-resolving-model-simulations-midlatitude-cirrus-arm-train-observations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1417280-evaluation-cloud-resolving-model-simulations-midlatitude-cirrus-arm-train-observations"><span>Evaluation of cloud-resolving <span class="hlt">model</span> simulations of midlatitude cirrus with ARM and A-train <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Muhlbauer, A.; Ackerman, T. P.; Lawson, R. P.; ...</p> <p>2015-07-14</p> <p>Cirrus clouds are ubiquitous in the upper troposphere and still constitute one of the largest uncertainties in climate predictions. Our paper evaluates cloud-resolving <span class="hlt">model</span> (CRM) and cloud system-resolving <span class="hlt">model</span> (CSRM) simulations of a midlatitude cirrus case with comprehensive <span class="hlt">observations</span> collected under the auspices of the Atmospheric Radiation <span class="hlt">Measurements</span> (ARM) program and with spaceborne <span class="hlt">observations</span> from the National Aeronautics and Space Administration A-train satellites. The CRM simulations are driven with periodic boundary conditions and ARM forcing data, whereas the CSRM simulations are driven by the ERA-Interim product. Vertical profiles of temperature, relative humidity, and wind speeds are reasonably well simulated bymore » the CSRM and CRM, but there are remaining biases in the temperature, wind speeds, and relative humidity, which can be mitigated through nudging the <span class="hlt">model</span> simulations toward the <span class="hlt">observed</span> radiosonde profiles. Simulated vertical velocities are underestimated in all simulations except in the CRM simulations with grid spacings of 500 m or finer, which suggests that turbulent vertical air motions in cirrus clouds need to be parameterized in general circulation <span class="hlt">models</span> and in CSRM simulations with horizontal grid spacings on the order of 1 km. The simulated ice water content and ice number concentrations agree with the <span class="hlt">observations</span> in the CSRM but are underestimated in the CRM simulations. The underestimation of ice number concentrations is consistent with the overestimation of radar reflectivity in the CRM simulations and suggests that the <span class="hlt">model</span> produces too many large ice particles especially toward the cloud base. Simulated cloud profiles are rather insensitive to perturbations in the initial conditions or the dimensionality of the <span class="hlt">model</span> domain, but the treatment of the forcing data has a considerable effect on the outcome of the <span class="hlt">model</span> simulations. Despite considerable progress in <span class="hlt">observations</span> and microphysical parameterizations</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070031231&hterms=tropospheric+ozone&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtropospheric%2Bozone','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070031231&hterms=tropospheric+ozone&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtropospheric%2Bozone"><span>Tropospheric Ozone Determined from Aura OMI and MLS: Evaluation of <span class="hlt">Measurements</span> and Comparison with the Global <span class="hlt">Modeling</span> Initiative's Chemical Transport <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ziemke, J. R.; Chandra, S.; Duncan, B. N.; Froidevaux, L.; Bhartia, P. K.; Levelt, P. F.; Waters, J. W.</p> <p>2006-01-01</p> <p>Ozone <span class="hlt">measurements</span> from the OMI and MLS instruments on board the Aura satellite are used for deriving global distributions of tropospheric column ozone (TCO). TCO is determined using the tropospheric ozone residual method which involves subtracting <span class="hlt">measurements</span> of MLS stratospheric column ozone (SCO) from OMI total column ozone after adjusting for intercalibration differences of the two instruments using the convective-cloud differential method. The derived TCO field, which covers one complete year of mostly continuous daily <span class="hlt">measurements</span> from late August 2004 through August 2005, is used for studying the regional and global pollution on a timescale of a few days to months. The seasonal and zonal characteristics of the <span class="hlt">observed</span> TCO fields are also compared with TCO fields derived from the Global <span class="hlt">Modeling</span> Initiative's Chemical Transport <span class="hlt">Model</span>. The <span class="hlt">model</span> and <span class="hlt">observations</span> show interesting similarities with respect to zonal and seasonal variations. However, there are notable differences, particularly over the vast region of the Saharan desert.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4469187','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4469187"><span>Evaluating <span class="hlt">Measurement</span> of Dynamic Constructs: Defining a <span class="hlt">Measurement</span> <span class="hlt">Model</span> of Derivatives</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Estabrook, Ryne</p> <p>2015-01-01</p> <p>While <span class="hlt">measurement</span> evaluation has been embraced as an important step in psychological research, evaluating <span class="hlt">measurement</span> structures with longitudinal data is fraught with limitations. This paper defines and tests a <span class="hlt">measurement</span> <span class="hlt">model</span> of derivatives (MMOD), which is designed to assess the <span class="hlt">measurement</span> structure of latent constructs both for analyses of between-person differences and for the analysis of change. Simulation results indicate that MMOD outperforms existing <span class="hlt">models</span> for multivariate analysis and provides equivalent fit to data generation <span class="hlt">models</span>. Additional simulations show MMOD capable of detecting differences in between-person and within-person factor structures. <span class="hlt">Model</span> features, applications and future directions are discussed. PMID:24364383</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMED24B..06V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMED24B..06V"><span>CrowdWater - Can people <span class="hlt">observe</span> what <span class="hlt">models</span> need?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Meerveld, I. H. J.; Seibert, J.; Vis, M.; Etter, S.; Strobl, B.</p> <p>2017-12-01</p> <p>CrowdWater (www.crowdwater.ch) is a citizen science project that explores the usefulness of crowd-sourced data for hydrological <span class="hlt">model</span> calibration and prediction. Hydrological <span class="hlt">models</span> are usually calibrated based on <span class="hlt">observed</span> streamflow data but it is likely easier for people to estimate relative stream water levels, such as the water level above or below a rock, than streamflow. Relative stream water levels may, therefore, be a more suitable variable for citizen science projects than streamflow. In order to test this assumption, we held surveys near seven different sized rivers in Switzerland and asked more than 450 volunteers to estimate the water level class based on a picture with a virtual staff gauge. The results show that people can generally estimate the relative water level well, although there were also a few outliers. We also asked the volunteers to estimate streamflow based on the stick method. The median estimated streamflow was close to the <span class="hlt">observed</span> streamflow but the spread in the streamflow estimates was large and there were very large outliers, suggesting that crowd-based streamflow data is highly uncertain. In order to determine the potential value of water level class data for <span class="hlt">model</span> calibration, we converted streamflow time series for 100 catchments in the US to stream level class time series and used these to calibrate the HBV <span class="hlt">model</span>. The <span class="hlt">model</span> was then validated using the streamflow data. The results of this <span class="hlt">modeling</span> exercise show that stream level class data are useful for constraining a simple runoff <span class="hlt">model</span>. Time series of only two stream level classes, e.g. above or below a rock in the stream, were already informative, especially when the class boundary was chosen towards the highest stream levels. There was hardly any improvement in <span class="hlt">model</span> performance when more than five water level classes were used. This suggests that if crowd-sourced stream level <span class="hlt">observations</span> are available for otherwise ungauged catchments, these data can be used to constrain</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999PhDT.........2R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999PhDT.........2R"><span><span class="hlt">Observation</span> and <span class="hlt">modelling</span> of urban dew</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Richards, Katrina</p> <p></p> <p>Despite its relevance to many aspects of urban climate and to several practical questions, urban dew has largely been ignored. Here, simple <span class="hlt">observations</span> an out-of-doors scale <span class="hlt">model</span>, and numerical simulation are used to investigate patterns of dewfall and surface moisture (dew + guttation) in urban environments. <span class="hlt">Observations</span> and <span class="hlt">modelling</span> were undertaken in Vancouver, B.C., primarily during the summers of 1993 and 1996. Surveys at several scales (0.02-25 km) show that the main controls on dew are weather, location and site configuration (geometry and surface materials). Weather effects are discussed using an empirical factor, FW . Maximum dew accumulation (up to ~ 0.2 mm per night) is seen on nights with moist air and high FW , i.e., cloudless conditions with light winds. Favoured sites are those with high Ysky and surfaces which cool rapidly after sunset, e.g., grass and well insulated roofs. A 1/8-scale <span class="hlt">model</span> is designed, constructed, and run at an out-of-doors site to study dew patterns in an urban residential landscape which consists of house lots, a street and an open grassed park. The Internal Thermal Mass (ITM) approach is used to scale the thermal inertia of buildings. The <span class="hlt">model</span> is validated using data from full-scale sites in Vancouver. Patterns in the <span class="hlt">model</span> agree with those seen at the full-scale, i.e., dew distribution is governed by weather, site geometry and substrate conditions. Correlation is shown between Ysky and surface moisture accumulation. The feasibility of using a numerical <span class="hlt">model</span> to simulate urban dew is investigated using a modified version of a rural dew <span class="hlt">model</span>. Results for simple isolated surfaces-a deciduous tree leaf and an asphalt shingle roof-show promise, especially for built surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29041509','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29041509"><span><span class="hlt">Measurement</span> system and <span class="hlt">model</span> for simultaneously <span class="hlt">measuring</span> 6DOF geometric errors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhao, Yuqiong; Zhang, Bin; Feng, Qibo</p> <p>2017-09-04</p> <p>A <span class="hlt">measurement</span> system to simultaneously <span class="hlt">measure</span> six degree-of-freedom (6DOF) geometric errors is proposed. The <span class="hlt">measurement</span> method is based on a combination of mono-frequency laser interferometry and laser fiber collimation. A simpler and more integrated optical configuration is designed. To compensate for the <span class="hlt">measurement</span> errors introduced by error crosstalk, element fabrication error, laser beam drift, and nonparallelism of two <span class="hlt">measurement</span> beam, a unified <span class="hlt">measurement</span> <span class="hlt">model</span>, which can improve the <span class="hlt">measurement</span> accuracy, is deduced and established using the ray-tracing method. A numerical simulation using the optical design software Zemax is conducted, and the results verify the correctness of the <span class="hlt">model</span>. Several experiments are performed to demonstrate the feasibility and effectiveness of the proposed system and <span class="hlt">measurement</span> <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920063154&hterms=modulation+reactions+chemical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dmodulation%2Breactions%2Bchemical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920063154&hterms=modulation+reactions+chemical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dmodulation%2Breactions%2Bchemical"><span>FAGE <span class="hlt">measurements</span> of tropospheric HO with <span class="hlt">measurements</span> and <span class="hlt">model</span> of interferences</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hard, T. M.; Mehrabzadeh, A. A.; Chan, C. Y.; O'Brien, R. J.</p> <p>1992-01-01</p> <p>Ambient HO <span class="hlt">measurements</span> by low-pressure laser-excited fluorescence with chemical modulation, and supporting ozone and water-vapor data, are presented for periods in May and August 1987. The <span class="hlt">observed</span> peak daytime ambient HO concentrations are in the range (2.5 to 8) x 10 exp 6 molecules/cu cm and show small negative offsets due to photochemical interference. Direct <span class="hlt">measurements</span> of the interference at fixed (O3) give the dependence on ambient (H2O) and on the modulating reagent (isobutane). At ambient (O3) = 30 ppb and 10 torr H2O, with excitation and detection at a total pressure of 4 torr, the net interference is equal to (HO) = -1.3 x 10 exp 6 molecules/cu cm. Production of HO by the reaction of isobutane with O(1D) accounts for the negative interference. Quenching of HO fluorescence by the modulating reagent contributes a smaller positive term to the interference; kinetic <span class="hlt">measurements</span> of the quenching rate coefficient are reported. The experimental interference results are compared with a detailed kinetic <span class="hlt">model</span> of HO production, excitation, relaxation, and detection; reasonable agreement is found.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040081263','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040081263"><span>Bio-Optical <span class="hlt">Measurement</span> and <span class="hlt">Modeling</span> of the California Current and Southern Oceans</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mitchell, B. Gregg; Mitchell, B. Greg</p> <p>2003-01-01</p> <p>The SIMBIOS project's principal goals are to validate standard or experimental ocean color products through detailed bio-optical and biogeochemical <span class="hlt">measurements</span>, and to combine Ocean optical <span class="hlt">observations</span> with <span class="hlt">modeling</span> to contribute to satellite vicarious radiometric calibration and algorithm development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRD..11715310B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRD..11715310B"><span>Methane airborne <span class="hlt">measurements</span> and comparison to global <span class="hlt">models</span> during BARCA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Beck, Veronika; Chen, Huilin; Gerbig, Christoph; Bergamaschi, Peter; Bruhwiler, Lori; Houweling, Sander; Röckmann, Thomas; Kolle, Olaf; Steinbach, Julia; Koch, Thomas; Sapart, Célia J.; van der Veen, Carina; Frankenberg, Christian; Andreae, Meinrat O.; Artaxo, Paulo; Longo, Karla M.; Wofsy, Steven C.</p> <p>2012-08-01</p> <p>Tropical regions, especially the Amazon region, account for large emissions of methane (CH4). Here, we present CH4 <span class="hlt">observations</span> from two airborne campaigns conducted within the BARCA (Balanço Atmosférico Regional de Carbono na Amazônia) project in the Amazon basin in November 2008 (end of the dry season) and May 2009 (end of the wet season). We performed continuous <span class="hlt">measurements</span> of CH4 onboard an aircraft for the first time in the Amazon region, covering the whole Amazon basin with over 150 vertical profiles between altitudes of 500 m and 4000 m. The <span class="hlt">observations</span> support the finding of previous ground-based, airborne, and satellite <span class="hlt">measurements</span> that the Amazon basin is a large source of atmospheric CH4. Isotope analysis verified that the majority of emissions can be attributed to CH4 emissions from wetlands, while urban CH4 emissions could be also traced back to biogenic origin. A comparison of five TM5 based global CH4 inversions with the <span class="hlt">observations</span> clearly indicates that the inversions using SCIAMACHY <span class="hlt">observations</span> represent the BARCA <span class="hlt">observations</span> best. The calculated CH4 flux estimate obtained from the mismatch between <span class="hlt">observations</span> and TM5-<span class="hlt">modeled</span> CH4 fields ranges from 36 to 43 mg m-2 d-1 for the Amazon lowland region.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18..227L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18..227L"><span>Ultraviolet radiation <span class="hlt">modelling</span> from ground-based and satellite <span class="hlt">measurements</span> on Reunion Island, southern tropics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lamy, Kévin; Portafaix, Thierry; Brogniez, Colette; Godin-Beekmann, Sophie; Bencherif, Hassan; Morel, Béatrice; Pazmino, Andrea; Metzger, Jean Marc; Auriol, Frédérique; Deroo, Christine; Duflot, Valentin; Goloub, Philippe; Long, Charles N.</p> <p>2018-01-01</p> <p>Surface ultraviolet radiation (SUR) is not an increasing concern after the implementation of the Montreal Protocol and the recovery of the ozone layer (Morgenstern et al., 2008). However, large uncertainties remain in the prediction of future changes of SUR (Bais et al., 2015). Several studies pointed out that UV-B impacts the biosphere (Erickson et al., 2015), especially the aquatic system, which plays a central part in the biogeochemical cycle (Hader et al., 2007). It can affect phytoplankton productivity (Smith and Cullen, 1995). This influence can result in either positive or negative feedback on climate (Zepp et al., 2007). Global circulation <span class="hlt">model</span> simulations predict an acceleration of the Brewer-Dobson circulation over the next century (Butchart, 2014), which would lead to a decrease in ozone levels in the tropics and an enhancement at higher latitudes (Hegglin and Shepherd, 2009). Reunion Island is located in the tropics (21° S, 55° E), in a part of the world where the amount of ozone in the ozone column is naturally low. In addition, this island is mountainous and the marine atmosphere is often clean with low aerosol concentrations. Thus, <span class="hlt">measurements</span> show much higher SUR than at other sites at the same latitude or at midlatitudes. Ground-based <span class="hlt">measurements</span> of SUR have been taken on Reunion Island by a Bentham DTMc300 spectroradiometer since 2009. This instrument is affiliated with the Network for the Detection of Atmospheric Composition Change (NDACC). In order to quantify the future evolution of SUR in the tropics, it is necessary to validate a <span class="hlt">model</span> against present <span class="hlt">observations</span>. This study is designed to be a preliminary parametric and sensitivity study of SUR <span class="hlt">modelling</span> in the tropics. We developed a local parameterisation using the Tropospheric Ultraviolet and Visible <span class="hlt">Model</span> (TUV; Madronich, 1993) and compared the output of TUV to multiple years of Bentham spectral <span class="hlt">measurements</span>. This comparison started in early 2009 and continued until 2016. Only</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.S43A1966G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.S43A1966G"><span>Trampoline Effect: <span class="hlt">Observations</span> and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guyer, R.; Larmat, C. S.; Ulrich, T. J.</p> <p>2009-12-01</p> <p>The Iwate-Miyagi earthquake at site IWTH25 (14 June 2008) had large, asymmetric at surface vertical accelerations prompting the sobriquet trampoline effect (Aoi et. al. 2008). In addition the surface acceleration record showed long-short waiting time correlations and vertical-horizontal acceleration correlations. A lumped element <span class="hlt">model</span>, deduced from the equations of continuum elasticity, is employed to describe the behavior at this site in terms of a surface layer and substrate. Important ingredients in the <span class="hlt">model</span> are the nonlinear vertical coupling between the surface layer and the substrate and the nonlinear horizontal frictional coupling between the surface layer and the substrate. The <span class="hlt">model</span> produces results in qualitative accord with <span class="hlt">observations</span>: acceleration asymmetry, Fourier spectrum, waiting time correlations and vertical acceleration-horizontal acceleration correlations. [We gratefully acknowledge the support of the U. S. Department of Energy through the LANL/LDRD Program for this work].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.8189B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.8189B"><span><span class="hlt">Observation</span>- and <span class="hlt">model</span>-based estimates of particulate dry nitrogen deposition to the oceans</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baker, Alex R.; Kanakidou, Maria; Altieri, Katye E.; Daskalakis, Nikos; Okin, Gregory S.; Myriokefalitakis, Stelios; Dentener, Frank; Uematsu, Mitsuo; Sarin, Manmohan M.; Duce, Robert A.; Galloway, James N.; Keene, William C.; Singh, Arvind; Zamora, Lauren; Lamarque, Jean-Francois; Hsu, Shih-Chieh; Rohekar, Shital S.; Prospero, Joseph M.</p> <p>2017-07-01</p> <p>Anthropogenic nitrogen (N) emissions to the atmosphere have increased significantly the deposition of nitrate (NO3-) and ammonium (NH4+) to the surface waters of the open ocean, with potential impacts on marine productivity and the global carbon cycle. Global-scale understanding of the impacts of N deposition to the oceans is reliant on our ability to produce and validate <span class="hlt">models</span> of nitrogen emission, atmospheric chemistry, transport and deposition. In this work, ˜ 2900 <span class="hlt">observations</span> of aerosol NO3- and NH4+ concentrations, acquired from sampling aboard ships in the period 1995-2012, are used to assess the performance of <span class="hlt">modelled</span> N concentration and deposition fields over the remote ocean. Three ocean regions (the eastern tropical North Atlantic, the northern Indian Ocean and northwest Pacific) were selected, in which the density and distribution of <span class="hlt">observational</span> data were considered sufficient to provide effective comparison to <span class="hlt">model</span> products. All of these study regions are affected by transport and deposition of mineral dust, which alters the deposition of N, due to uptake of nitrogen oxides (NOx) on mineral surfaces. Assessment of the impacts of atmospheric N deposition on the ocean requires atmospheric chemical transport <span class="hlt">models</span> to report deposition fluxes; however, these fluxes cannot be <span class="hlt">measured</span> over the ocean. <span class="hlt">Modelling</span> studies such as the Atmospheric Chemistry and Climate <span class="hlt">Model</span> Intercomparison Project (ACCMIP), which only report deposition flux, are therefore very difficult to validate for dry deposition. Here, the available <span class="hlt">observational</span> data were averaged over a 5° × 5° grid and compared to ACCMIP dry deposition fluxes (ModDep) of oxidised N (NOy) and reduced N (NHx) and to the following parameters from the Tracer <span class="hlt">Model</span> 4 of the Environmental Chemical Processes Laboratory (TM4): ModDep for NOy, NHx and particulate NO3- and NH4+, and surface-level particulate NO3- and NH4+ concentrations. As a <span class="hlt">model</span> ensemble, ACCMIP can be expected to be more robust than</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29151838','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29151838"><span><span class="hlt">Observation</span>- and <span class="hlt">Model</span>-Based Estimates of Particulate Dry Nitrogen Deposition to the Oceans.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Baker, Alex R; Kanakidou, Maria; Altieri, Katye E; Daskalakis, Nikos; Okin, Gregory S; Myriokefalitakis, Stelios; Dentener, Frank; Uematsu, Mitsuo; Sarin, Manmohan M; Duce, Robert A; Galloway, James N; Keene, William C; Singh, Arvind; Zamora, Lauren; Lamarque, Jean-Francois; Hsu, Shih-Chieh; Rohekar, Shital S; Prospero, Joseph M</p> <p>2017-01-01</p> <p>Anthropogenic nitrogen (N) emissions to the atmosphere have increased significantly the deposition of nitrate (NO 3 - ) and ammonium (NH 4 + ) to the surface waters of the open ocean, with potential impacts on marine productivity and the global carbon cycle. Global-scale understanding of the impacts of N deposition to the oceans is reliant on our ability to produce and validate <span class="hlt">models</span> of nitrogen emission, atmospheric chemistry, transport and deposition. In this work, ~2900 <span class="hlt">observations</span> of aerosol NO 3 - and NH 4 + concentrations, acquired from sampling aboard ships in the period 1995 - 2012, are used to assess the performance of <span class="hlt">modelled</span> N concentration and deposition fields over the remote ocean. Three ocean regions (the eastern tropical North Atlantic, the northern Indian Ocean and northwest Pacific) were selected, in which the density and distribution of <span class="hlt">observational</span> data were considered sufficient to provide effective comparison to <span class="hlt">model</span> products. All of these study regions are affected by transport and deposition of mineral dust, which alters the deposition of N, due to uptake of nitrogen oxides (NO x ) on mineral surfaces. Assessment of the impacts of atmospheric N deposition on the ocean requires atmospheric chemical transport <span class="hlt">models</span> to report deposition fluxes, however these fluxes cannot be <span class="hlt">measured</span> over the ocean. <span class="hlt">Modelling</span> studies such as the Atmospheric Chemistry and Climate <span class="hlt">Model</span> Intercomparison Project (ACCMIP), which only report deposition flux are therefore very difficult to validate for dry deposition. Here the available <span class="hlt">observational</span> data were averaged over a 5° × 5° grid and compared to ACCMIP dry deposition fluxes (ModDep) of oxidised N (NO y ) and reduced N (NH x ) and to the following parameters from the TM4-ECPL (TM4) <span class="hlt">model</span>: ModDep for NO y , NH x and particulate NO 3 - and NH 4 + , and surface-level particulate NO 3 - and NH 4 + concentrations. As a <span class="hlt">model</span> ensemble, ACCMIP can be expected to be more robust than TM4, while TM4 gives</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=%22Observation+Protocol%22&id=EJ1122583','ERIC'); return false;" href="https://eric.ed.gov/?q=%22Observation+Protocol%22&id=EJ1122583"><span>An Exploratory Factor Analysis of the Sheltered Instruction <span class="hlt">Observation</span> Protocol as an Evaluation Tool to <span class="hlt">Measure</span> Teaching Effectiveness</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Polat, Nihat; Cepik, Saban</p> <p>2016-01-01</p> <p>To narrow the achievement gap between English language learners (ELLs) and their native-speaking peers in K-12 settings in the United States, effective instructional <span class="hlt">models</span> must be identified. However, identifying valid <span class="hlt">observation</span> protocols that can <span class="hlt">measure</span> the effectiveness of specially designed instructional practices is not an easy task. This…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100017177','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100017177"><span>Assimilation of Satellite-Derived Skin Temperature <span class="hlt">Observations</span> into Land Surface <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reichle, Rolf H.; Kumar, Sujay V.; Mahanama, P. P.; Koster, Randal D.; Liu, Q.</p> <p>2010-01-01</p> <p>Land surface (or "skin") temperature (LST) lies at the heart of the surface energy balance and is a key variable in weather and climate <span class="hlt">models</span>. Here we assimilate LST retrievals from the International Satellite Cloud Climatology Project (ISCCP) into the Noah and Catchment (CLSM) land surface <span class="hlt">models</span> using an ensemble-based, off-line land data assimilation system. LST is described very differently in the two <span class="hlt">models</span>. A priori scaling and dynamic bias estimation approaches are applied because satellite and <span class="hlt">model</span> LST typically exhibit different mean values and variability. Performance is <span class="hlt">measured</span> against 27 months of in situ <span class="hlt">measurements</span> from the Coordinated Energy and Water Cycle <span class="hlt">Observations</span> Project at 48 stations. LST estimates from Noah and CLSM without data assimilation ("open loop") are comparable to each other and superior to that of ISCCP retrievals. For LST, RMSE values are 4.9 K (CLSM), 5.6 K (Noah), and 7.6 K (ISCCP), and anomaly correlation coefficients (R) are 0.62 (CLSM), 0.61 (Noah), and 0.52 (ISCCP). Assimilation of ISCCP retrievals provides modest yet statistically significant improvements (over open loop) of up to 0.7 K in RMSE and 0.05 in anomaly R. The skill of surface turbulent flux estimates from the assimilation integrations is essentially identical to the corresponding open loop skill. Noah assimilation estimates of ground heat flux, however, can be significantly worse than open loop estimates. Provided the assimilation system is properly adapted to each land <span class="hlt">model</span>, the benefits from the assimilation of LST retrievals are comparable for both <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1812685E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1812685E"><span>The combination of satellite <span class="hlt">observation</span> techniques for sequential ionosphere VTEC <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Erdogan, Eren; Limberger, Marco; Schmidt, Michael; Seitz, Florian; Dettmering, Denise; Börger, Klaus; Brandert, Sylvia; Görres, Barbara; Kersten, Wilhelm F.; Bothmer, Volker; Hinrichs, Johannes; Venzmer, Malte; Mrotzek, Niclas</p> <p>2016-04-01</p> <p>The project OPTIMAP is a joint initiative by the Bundeswehr GeoInformation Centre (BGIC), the German Space Situational Awareness Centre (GSSAC), the German Geodetic Research Institute of the Technical University of Munich (DGFI-TUM) and the Institute for Astrophysics at the University of Göttingen (IAG). The main goal is to develop an operational tool for ionospheric mapping and prediction (OPTIMAP). A key feature of the project is the combination of different satellite <span class="hlt">observation</span> techniques to improve the spatio-temporal data coverage and the sensitivity for selected target parameters. In the current status, information about the vertical total electron content (VTEC) is derived from the dual frequency signal processing of four techniques: (1) Terrestrial <span class="hlt">observations</span> of GPS and GLONASS ensure the high-resolution coverage of continental regions, (2) the satellite altimetry mission Jason-2 is taken into account to provide VTEC in nadir direction along the satellite tracks over the oceans, (3) GPS radio occultations to Formosat-3/COSMIC are exploited for the retrieval of electron density profiles that are integrated to obtain VTEC and (4) Jason-2 carrier-phase <span class="hlt">observations</span> tracked by the on-board DORIS receiver are processed to determine the relative VTEC. All <span class="hlt">measurements</span> are sequentially pre-processed in hourly batches serving as input data of a Kalman filter (KF) for <span class="hlt">modeling</span> the global VTEC distribution. The KF runs in a predictor-corrector mode allowing for the sequential processing of the <span class="hlt">measurements</span> where update steps are performed with one-minute sampling in the current configuration. The spatial VTEC distribution is represented by B-spline series expansions, i.e., the corresponding B-spline series coefficients together with additional technique-dependent unknowns such as Differential Code Biases and Intersystem Biases are estimated by the KF. As a preliminary solution, the prediction <span class="hlt">model</span> to propagate the filter state through time is defined by a random</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUSM.G33B..04R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUSM.G33B..04R"><span>Regional Geoid <span class="hlt">Modeling</span> Compared to Ocean Surface <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roman, D. R.; Saleh, J.; Wang, Y. M.</p> <p>2007-05-01</p> <p>Aerogravity over a limited coastal region of the northern Gulf of Mexico enhanced and rectified the local gravity field signal. In turn, these data improved the derived geoid height <span class="hlt">model</span> based on comparison with dynamic ocean topography (DOT) and tide gage information at eleven stations. Additionally, lidar <span class="hlt">observations</span> were analyzed along nearly 50 profiles to estimate the reliability of these <span class="hlt">models</span> into the offshore region. The overall comparison shows dm-level agreement between the various geoid and DOT <span class="hlt">models</span> and ocean surface <span class="hlt">observations</span>. An approximate 30 cm bias must still be explained; however, the results of this study point to the potential for further cooperative studies between oceanographers and geodesists.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PTEP.2018d3B08N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PTEP.2018d3B08N"><span>Analysis of angular <span class="hlt">observables</span> of Λ_b \\to Λ (\\to pπ)μ+μ- decay in the standard and Z^' <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nasrullah, Aqsa; Jamil Aslam, M.; Shafaq, Saba</p> <p>2018-04-01</p> <p>In 2015, the LHCb collaboration <span class="hlt">measured</span> the differential branching ratio d{B}/dq^2, the lepton- and hadron-side forward-backward asymmetries, denoted by A^ℓ_FB and A^{Λ}_FB, respectively, in the range 15 < q^2(=s) < 20 GeV^2 with 3 fb^{-1} of data. Motivated by these <span class="hlt">measurements</span>, we perform an analysis of q^2-dependent Λ_b \\to Λ (\\to p π ) μ^+μ^- angular <span class="hlt">observables</span> at large- and low- recoil in the standard <span class="hlt">model</span> (SM) and in a family non-universal Z^' <span class="hlt">model</span>. The exclusive Λb\\to Λ transition is governed by the form factors, and in the present study we use the recently performed high-precision lattice QCD calculations that have well-controlled uncertainties, especially in the 15 < s < 20 GeV^2 bin. Using the full four-folded angular distribution of Λ_b \\to Λ (\\to p π ) μ^+μ^- decay, first of all we focus on calculations of the experimentally <span class="hlt">measured</span> d{B}/ds, A^ℓ_FB, and A^{Λ}_FB in the SM and compare their numerical values with the <span class="hlt">measurements</span> in appropriate bins of s. In case of a possible discrepancy between the SM prediction and the <span class="hlt">measurements</span>, we try to see if these can be accommodated though the extra neutral Z^' boson. We find that in the dimuon momentum range 15 < s < 20 GeV^2 the value of d{B}/ds and central value of A^ℓ_FB in the Z^' <span class="hlt">model</span> is compatible with the <span class="hlt">measured</span> values. In addition, the fraction of longitudinal polarization of the dimuon FL was <span class="hlt">measured</span> to be 0.61^{+0.11}_{-0.14}± 0.03 in 15 < s < 20 GeV^2 at the LHCb. We find that in this bin the value found in the Z^' <span class="hlt">model</span> is close to the <span class="hlt">observed</span> values. After comparing the results of these <span class="hlt">observables</span>, we have proposed other <span class="hlt">observables</span> such as {α}i and α^{(')}i with i =θ_{ℓ}, θ_{Λ}, φ,L, U and coefficients of different foldings P_{1, \\ldots, 9} in different bins of s in the SM and Z^' <span class="hlt">model</span>. We illustrate that the experimental <span class="hlt">observations</span> of the s-dependent angular <span class="hlt">observables</span> calculated here in several bins of s can help to test the predictions of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150000350','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150000350"><span>Long-Term Changes in Lower Tropospheric Baseline Ozone Concentrations:. [Comparing Chemistry-Climate <span class="hlt">Models</span> and <span class="hlt">Observations</span> at Northern Mid-Latitudes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parrish, D. D.; Lamarque, J.-F.; Naik, V.; Horowitz, L.; Shindell, D. T.; Staehelin, J.; Derwent, R.; Cooper, O. R.; Tanimoto, H.; Volz-Thomas, A.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20150000350'); toggleEditAbsImage('author_20150000350_show'); toggleEditAbsImage('author_20150000350_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20150000350_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20150000350_hide"></p> <p>2014-01-01</p> <p>Two recent papers have quantified long-term ozone (O3) changes <span class="hlt">observed</span> at northernmidlatitude sites that are believed to represent baseline (here understood as representative of continental to hemispheric scales) conditions. Three chemistry-climate <span class="hlt">models</span> (NCAR CAM-chem, GFDL-CM3, and GISS-E2-R) have calculated retrospective tropospheric O3 concentrations as part of the Atmospheric Chemistry and Climate <span class="hlt">Model</span> Intercomparison Project and Coupled <span class="hlt">Model</span> Intercomparison Project Phase 5 <span class="hlt">model</span> intercomparisons. We present an approach for quantitative comparisons of <span class="hlt">model</span> results with <span class="hlt">measurements</span> for seasonally averaged O3 concentrations. There is considerable qualitative agreement between the <span class="hlt">measurements</span> and the <span class="hlt">models</span>, but there are also substantial and consistent quantitative disagreements. Most notably, <span class="hlt">models</span> (1) overestimate absolute O3 mixing ratios, on average by approximately 5 to 17 ppbv in the year 2000, (2) capture only approximately 50% of O3 changes <span class="hlt">observed</span> over the past five to six decades, and little of <span class="hlt">observed</span> seasonal differences, and (3) capture approximately 25 to 45% of the rate of change of the long-term changes. These disagreements are significant enough to indicate that only limited confidence can be placed on estimates of present-day radiative forcing of tropospheric O3 derived from <span class="hlt">modeled</span> historic concentration changes and on predicted future O3 concentrations. Evidently our understanding of tropospheric O3, or the incorporation of chemistry and transport processes into current chemical climate <span class="hlt">models</span>, is incomplete. <span class="hlt">Modeled</span> O3 trends approximately parallel estimated trends in anthropogenic emissions of NO(sub x), an important O3 precursor, while <span class="hlt">measured</span> O3 changes increase more rapidly than these emission estimates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A11E0065S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A11E0065S"><span><span class="hlt">Modeling</span> Trace Pollutants in the North Atlantic Free Troposphere and Comparisons with <span class="hlt">Observed</span> Pollutant Concentrations at Pico</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sanyal, S.; Wuebbles, D. J.; Olsen, S. C.; Mazzoleni, L. R.; Mazzoleni, C.; Helmig, D.; Fialho, P. J.</p> <p>2016-12-01</p> <p>This study focuses on <span class="hlt">modeling</span> free tropospheric aerosol and co-pollutants after trans-Atlantic transport of North American air pollution to the Pico Mountain Observatory (PMO) using the 3D global chemistry climate <span class="hlt">model</span> CAM-Chem (version 4) and analyzing the <span class="hlt">model</span> simulations relative to in-situ summertime <span class="hlt">measurements</span> of carbon monoxide (CO), ozone (O3) and black carbon (BC) at the Pico Mountain Observatory (PMO) located in the Azores, Portugal from 2009 - 2011. The elevation of PMO ( 2225m above mean sea level) and steep slope of the surrounding mountain put the station above the regional marine boundary layer, enabling frequent sampling of free tropospheric air. Because of its unique location, air sampled at the station is rarely affected by local emissions or the ocean, and represents air masses transported over long distances to the site. The study used the Community Atmosphere <span class="hlt">Model</span> CAM4, which is a part of the Community Earth System <span class="hlt">model</span> version 1 (CESM1). HYSPLIT backward trajectories ran using the web-based portal READY was used to study airflow trajectory at PMO and showed that more than 50% of the air mass originated from North America. The <span class="hlt">model</span> simulations were compared with <span class="hlt">observational</span> data (from April - September) at PMO for the years 2009 through 2011. The fire data for the USA and Canada was compiled from the reports of National Interagency Coordination Center and Canadian Wildland Fire Information System, respectively. Time series analyses and orthogonal regression were used to compare <span class="hlt">model</span> simulations with <span class="hlt">observations</span>. The comparison shows simulations give a good representation of the <span class="hlt">observations</span>, e.g., the mean concentration of CO in 2009 is 91.76 ppb and 95.05 ppb respectively from the simulation and the <span class="hlt">observations</span>. <span class="hlt">Observed</span> elevated pollutant concentrations also coincide with the maxima captured by the simulations. To assess the impact of North American outflow on pollution at PMO, scatter technique was used to calculate enhancement</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....16.4451Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....16.4451Z"><span>Global <span class="hlt">observations</span> and <span class="hlt">modeling</span> of atmosphere-surface exchange of elemental mercury: a critical review</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Wei; Lin, Che-Jen; Wang, Xun; Sommar, Jonas; Fu, Xuewu; Feng, Xinbin</p> <p>2016-04-01</p> <p>Reliable quantification of air-surface fluxes of elemental Hg vapor (Hg0) is crucial for understanding mercury (Hg) global biogeochemical cycles. There have been extensive <span class="hlt">measurements</span> and <span class="hlt">modeling</span> efforts devoted to estimating the exchange fluxes between the atmosphere and various surfaces (e.g., soil, canopies, water, snow, etc.) in the past three decades. However, large uncertainties remain due to the complexity of Hg0 bidirectional exchange, limitations of flux quantification techniques and challenges in <span class="hlt">model</span> parameterization. In this study, we provide a critical review on the state of science in the atmosphere-surface exchange of Hg0. Specifically, the advancement of flux quantification techniques, mechanisms in driving the air-surface Hg exchange and <span class="hlt">modeling</span> efforts are presented. Due to the semi-volatile nature of Hg0 and redox transformation of Hg in environmental media, Hg deposition and evasion are influenced by multiple environmental variables including seasonality, vegetative coverage and its life cycle, temperature, light, moisture, atmospheric turbulence and the presence of reactants (e.g., O3, radicals, etc.). However, the effects of these processes on flux have not been fundamentally and quantitatively determined, which limits the accuracy of flux <span class="hlt">modeling</span>. We compile an up-to-date global <span class="hlt">observational</span> flux database and discuss the implication of flux data on the global Hg budget. Mean Hg0 fluxes obtained by micrometeorological <span class="hlt">measurements</span> do not appear to be significantly greater than the fluxes <span class="hlt">measured</span> by dynamic flux chamber methods over unpolluted surfaces (p = 0.16, one-tailed, Mann-Whitney U test). The spatiotemporal coverage of existing Hg0 flux <span class="hlt">measurements</span> is highly heterogeneous with large data gaps existing in multiple continents (Africa, South Asia, Middle East, South America and Australia). The magnitude of the evasion flux is strongly enhanced by human activities, particularly at contaminated sites. Hg0 flux <span class="hlt">observations</span> in East</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..APR.Y4004L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..APR.Y4004L"><span><span class="hlt">Measuring</span> the radius of PSR J0437 -4715 using NICER <span class="hlt">observations</span> of X-ray oscillations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lamb, Frederick; Miller, M. Coleman</p> <p>2017-01-01</p> <p>The Neutron Star Interior Composition Explorer (NICER) will launch early in 2017. Its first scientific objective is to precisely and reliably <span class="hlt">measure</span> the radius of several neutron stars, thereby constraining the properties of cold matter at supranuclear densities. This will be done by fitting energy-dependent waveform <span class="hlt">models</span> to the <span class="hlt">observed</span> thermal X-ray waveforms of selected rotation-powered millisecond pulsars. A key target is the 174-Hz pulsar PSR J0437 -4715. Using synthetic waveform data and Bayesian methods, we have estimated the precisions with which its mass M and radius R can be <span class="hlt">measured</span> by NICER. When generating the synthetic data, we assumed M = 1 . 4M⊙ and R = 13 km. When generating the data and when analyzing it, we assumed the X-ray spectrum and radiation beaming pattern given by <span class="hlt">models</span> with cool hydrogen atmospheres and two hot spots. Assuming NICER <span class="hlt">observations</span> lasting a total of 1.0 Msec, current knowledge of M and the distance, and knowledge of the pulsar's spin axis to within 1°, the 1 σ credible region in R extends from 11.83 to 13.73 km (7.4%) and in M, from 1.307 to 1.567 M⊙ (9.1%). Marginalizing over M, we find the 1 σ credible interval for R alone extends from 12.62 to 13.68 km (4%).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040111048','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040111048"><span>ISS Plasma Interaction: <span class="hlt">Measurements</span> and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barsamian, H.; Mikatarian, R.; Alred, J.; Minow, J.; Koontz, S.</p> <p>2004-01-01</p> <p>Ionospheric plasma interaction effects on the International Space Station are discussed in the following paper. The large structure and high voltage arrays of the ISS represent a complex system interacting with LEO plasma. Discharge current <span class="hlt">measurements</span> made by the Plasma Contactor Units and potential <span class="hlt">measurements</span> made by the Floating Potential Probe delineate charging and magnetic induction effects on the ISS. Based on theoretical and physical understanding of the interaction phenomena, a <span class="hlt">model</span> of ISS plasma interaction has been developed. The <span class="hlt">model</span> includes magnetic induction effects, interaction of the high voltage solar arrays with ionospheric plasma, and accounts for other conductive areas on the ISS. Based on these phenomena, the Plasma Interaction <span class="hlt">Model</span> has been developed. Limited verification of the <span class="hlt">model</span> has been performed by comparison of Floating Potential Probe <span class="hlt">measurement</span> data to simulations. The ISS plasma interaction <span class="hlt">model</span> will be further tested and verified as <span class="hlt">measurements</span> from the Floating Potential <span class="hlt">Measurement</span> Unit become available, and construction of the ISS continues.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150007895','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150007895"><span>Investigating the Differential Emission <span class="hlt">Measure</span> and Energetics of Microflares with Combined SDO/AIA and RHESSI <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Inglis, A. R.; Christe, S.</p> <p>2014-01-01</p> <p>An important question in solar physics is whether solar microflares, the smallest currently <span class="hlt">observable</span> flare events in X-rays, possess the same energetic properties as large flares. Recent surveys have suggested that microflares may be less efficient particle accelerators than large flares, and hence contribute less non-thermal energy, which may have implications for coronal heating mechanisms. We therefore explore the energetic properties of microflares by combining EUV and X-ray <span class="hlt">measurements</span>. We present forward-fitting differential emission <span class="hlt">measure</span> (DEM) analysis of 10 microflares. The fitting is constrained by combining, for the first time, high-temperature Reuven Ramaty High Energy Solar Spectroscopic Imager (RHESSI) <span class="hlt">observations</span> and flux data from the Solar Dynamics Observatory (SDO) Atmospheric Imaging Assembly (AIA). Two fitting <span class="hlt">models</span> are tested for the DEM; a Gaussian distribution and a uniform DEM profile. A Gaussian fit proved unable to explain the <span class="hlt">observations</span> for any of the studied microflares. However, 8 of 10 events studied were reasonably fit by a uniform DEM profile. Hence microflare plasma can be considered to be significantly multi-thermal, and may not be significantly peaked or contain resolvable fine structure, within the uncertainties of the <span class="hlt">observational</span> instruments. The thermal and non-thermal energy is estimated for each microflare, comparing the energy budget with an isothermal plasma assumption. From the multi-thermal fits the minimum non-thermal energy content was found to average approximately 30% of the estimated thermal energy. By comparison, under an isothermal <span class="hlt">model</span> the non-thermal and thermal energy estimates were generally comparable. Hence, multi-thermal plasma is an important consideration for solar microflares that substantially alters their thermal and non-thermal energy content.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.3102A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.3102A"><span>Consistent radiative transfer <span class="hlt">modeling</span> of active and passive <span class="hlt">observations</span> of precipitation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Adams, Ian</p> <p>2016-04-01</p> <p>Spaceborne platforms such as the Tropical Rainfall <span class="hlt">Measurement</span> Mission (TRMM) and the Global Precipitation <span class="hlt">Measurement</span> (GPM) mission exploit a combination of active and passive sensors to provide a greater understanding of the three-dimensional structure of precipitation. While "operationalized" retrieval algorithms require fast forward <span class="hlt">models</span>, the ability to perform higher fidelity simulations is necessary in order to understand the physics of remote sensing problems by testing assumptions and developing parameterizations for the fast <span class="hlt">models</span>. To ensure proper synergy between active and passive <span class="hlt">modeling</span>, forward <span class="hlt">models</span> must be consistent when <span class="hlt">modeling</span> the responses of radars and radiometers. This work presents a self-consistent transfer <span class="hlt">model</span> for simulating radar reflectivities and millimeter wave brightness temperatures for precipitating scenes. To accomplish this, we extended the Atmospheric Radiative Transfer Simulator (ARTS) version 2.3 to solve the radiative transfer equation for active sensors and multiple scattering conditions. Early versions of ARTS (1.1) included a passive Monte Carlo solver, and ARTS is capable of handling atmospheres of up to three dimensions with ellipsoidal planetary geometries. The modular nature of ARTS facilitates extensibility, and the well-developed ray-tracing tools are suited for implementation of Monte Carlo algorithms. Finally, since ARTS handles the full Stokes vector, co- and cross-polarized reflectivity products are possible for scenarios that include nonspherical particles, with or without preferential alignment. The accuracy of the forward <span class="hlt">model</span> will be demonstrated with precipitation events <span class="hlt">observed</span> by TRMM and GPM, and the effects of multiple scattering will be detailed. The three-dimensional nature of the radiative transfer <span class="hlt">model</span> will be useful for understanding the effects of nonuniform beamfill and multiple scattering for spatially heterogeneous precipitation events. The targets of this forward <span class="hlt">model</span> are GPM (the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150021052','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150021052"><span>Assimilation of Precipitation <span class="hlt">Measurement</span> Missions Microwave Radiance <span class="hlt">Observations</span> With GEOS-5</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jin, Jianjun; Kim, Min-Jeong; McCarty, Will; Akella, Santha; Gu, Wei</p> <p>2015-01-01</p> <p>The Global Precipitation Mission (GPM) Core Observatory satellite was launched in February, 2014. The GPM Microwave Imager (GMI) is a conically scanning radiometer <span class="hlt">measuring</span> 13 channels ranging from 10 to 183 GHz and sampling between 65 S 65 N. This instrument is a successor to the Tropical Rainfall <span class="hlt">Measurement</span> Mission (TRMM) Microwave Imager (TMI), which has <span class="hlt">observed</span> 9 channels at frequencies ranging 10 to 85 GHz between 40 S 40 N since 1997. This presentation outlines the base procedures developed to assimilate GMI and TMI radiances in clear-sky conditions, including quality control methods, thinning decisions, and the estimation of, <span class="hlt">observation</span> errors. This presentation also shows the impact of these <span class="hlt">observations</span> when they are incorporated into the GEOS-5 atmospheric data assimilation system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010cosp...38.1411S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38.1411S"><span>The Martian airglow: <span class="hlt">observations</span> by Mars Express and kinetic <span class="hlt">modelling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simon, Cyril; Leblanc, François; Gronoff, Guillaume; Witasse, Olivier; Lilensten, Jean; Barthelemy, Mathieu; Bertaux, Jean-Loup</p> <p></p> <p>The photoemissions on Mars are the result of physical chemistry reactions in the upper atmo-sphere that depend on the planet's plasma environment. They arise on the dayside from UV photo-excitation (Barth et al., 1971) and on the nightside from chemical reactions and electron precipitation above regions of strong crustal magnetism (Bertaux et al., 2005). The physics of airglow generation at Mars is discussed both in terms of <span class="hlt">observations</span> (satellites) and <span class="hlt">models</span> (especially transport codes). A review of <span class="hlt">observations</span> made by SPICAM, the UV spectrometer onboard Mars Express, is first presented. The Cameron bands of CO(a - X), the CO+ (A - X) 2 doublet at 289.0 nm and the trans-auroral line of OI (297.2 nm) are mainly seen on the dayside. On the nightside both Cameron emissions and NO(C - X and A - X) emissions are present. In a second step, an updated airglow <span class="hlt">model</span> has been developed and compared to the latest SPICAM data. Several interesting implications are highlighted regarding neutral atmosphere variations for the dayglow (Simon et al., 2009) and electron precipitation mechanisms at the origin of the auroral intensities <span class="hlt">measured</span> by SPICAM in conjunction with the particle detector ASPERA and the radar MARSIS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1816026P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1816026P"><span>Aerosol classification using EARLINET <span class="hlt">measurements</span> for an intensive <span class="hlt">observational</span> period</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Papagiannopoulos, Nikolaos; Mona, Lucia; Pappalardo, Gelsomina</p> <p>2016-04-01</p> <p>ACTRIS (Aerosols, Clouds and Trace gases Research Infrastructure Network) organized an intensive <span class="hlt">observation</span> period during summer 2012. This campaign aimed at the provision of advanced <span class="hlt">observations</span> of physical and chemical aerosol properties, at the delivery of information about the 3D distribution of European atmospheric aerosols, and at the monitoring of Saharan dust intrusions events. EARLINET (European Aerosol Research Lidar Network) participated in the ACTRIS campaign through the addition of <span class="hlt">measurements</span> according to the EARLINET schedule as well as daily lidar-profiling <span class="hlt">measurements</span> around sunset by 11 selected lidar stations for the period from 8 June - 17 July. EARLINET <span class="hlt">observations</span> during this almost two-month period are used to characterize the optical properties and vertical distribution of long-range transported aerosol over the broader area of Mediterranean basin. The lidar <span class="hlt">measurements</span> of aerosol intensive parameters (lidar ratio, depolarization, Angstrom exponents) are shown to vary with location and aerosol type. A methodology based on EARLINET <span class="hlt">observations</span> of frequently <span class="hlt">observed</span> aerosol types is used to classify aerosols into seven separate types. The summertime Mediterranean basin is prone to African dust aerosols. Two major dust events were studied. The first episode occurred from the 18 to 21 of the June and the second one lasted from 28 June to 6 July. The lidar ratio within the dust layer was found to be wavelength independent with mean values of 58±14 sr at 355 nm and 57±11 sr at 532 nm. For the particle linear depolarization ratio, mean values of 0.27±0.04 at 532 nm have been found. Acknowledgements. The financial support for EARLINET in the ACTRIS Research Infrastructure Project by the European Union's Horizon 2020 research and innovation programme under grant agreement no. 654169 and previously under grant agreement no. 262254 in the Seventh Framework Programme (FP7/2007-2013) is gratefully acknowledged.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MARF46008C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MARF46008C"><span>Simultaneous continuous <span class="hlt">measurement</span> of non-commuting <span class="hlt">observables</span> and correlation in qubit trajectories</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chantasri, Areeya; Jordan, Andrew</p> <p></p> <p>We consider the continuous quantum <span class="hlt">measurement</span> of two or more non-commuting <span class="hlt">observables</span> of a single qubit. Examples are presented for the <span class="hlt">measurement</span> of two <span class="hlt">observables</span> which can be mapped to two <span class="hlt">measurement</span> axes on the Bloch sphere; a special case being the <span class="hlt">measurement</span> along the X and Z bases. The qubit dynamics is described by the stochastic master equations which include the effect of decoherence and <span class="hlt">measurement</span> inefficiencies. We investigate the qubit trajectories, their most likely paths, and their correlation functions using the stochastic path integral formalism. The correlation functions in qubit trajectories can be derived exactly for a special case and perturbatively for general cases. The theoretical predictions are compared with numerical simulations, as well as with trajectory data from the transmon superconducting qubit experiments.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.......186G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.......186G"><span><span class="hlt">Observations</span> and <span class="hlt">Modeling</span> of Merging Galaxy Clusters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Golovich, Nathan Ryan</p> <p></p> <p>Context: Galaxy clusters grow hierarchically with continuous accretion bookended by major merging events that release immense gravitational potential energy (as much as ˜1065 erg). This energy creates an environment for rich astrophysics. Precise <span class="hlt">measurements</span> of the dark matter halo, intracluster medium, and galaxy population have resulted in a number of important results including dark matter constraints and explanations of the generation of cosmic rays. However, since the timescale of major mergers (˜several Gyr) relegates <span class="hlt">observations</span> of individual systems to mere snapshots, these results are difficult to understand under a consistent dynamical framework. While computationally expensive simulations are vital in this regard, the vastness of parameter space has necessitated simulations of idealized mergers that are unlikely to capture the full richness. Merger speeds, geometries, and timescales each have a profound consequential effect, but even these simple dynamical properties of the mergers are often poorly understood. A method to identify and constrain the best systems for probing the rich astrophysics of merging clusters is needed. Such a method could then be utilized to prioritize <span class="hlt">observational</span> follow up and best inform proper exploration of dynamical phase space. Task: In order to identify and <span class="hlt">model</span> a large number of systems, in this dissertation, we compile an ensemble of major mergers each containing radio relics. We then complete a pan-chromatic study of these 29 systems including wide field optical photometry, targeted optical spectroscopy of member galaxies, radio, and X-ray <span class="hlt">observations</span>. We use the optical <span class="hlt">observations</span> to <span class="hlt">model</span> the galaxy substructure and estimate line of sight motion. In conjunction with the radio and X-ray data, these substructure <span class="hlt">models</span> helped elucidate the most likely merger scenario for each system and further constrain the dynamical properties of each system. We demonstrate the power of this technique through detailed analyses</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1225771-measuring-modeling-lifetime-nitrous-oxide-including-its-variability','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1225771-measuring-modeling-lifetime-nitrous-oxide-including-its-variability"><span><span class="hlt">Measuring</span> and <span class="hlt">modeling</span> the lifetime of nitrous oxide including its variability</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Prather, Michael J.; Hsu, Juno; DeLuca, Nicole M.; ...</p> <p>2015-05-14</p> <p>The lifetime of nitrous oxide, the third-most-important human-emitted greenhouse gas, is based to date primarily on <span class="hlt">model</span> studies or scaling to other gases. This work calculates a semiempirical lifetime based on Microwave Limb Sounder satellite <span class="hlt">measurements</span> of stratospheric profiles of nitrous oxide, ozone, and temperature; laboratory cross-section data for ozone and molecular oxygen plus kinetics for O( 1D); the <span class="hlt">observed</span> solar spectrum; and a simple radiative transfer <span class="hlt">model</span>. The result is 116 ± 9 years. The <span class="hlt">observed</span> monthly-to-biennial variations in lifetime and tropical abundance are well matched by four independent chemistry-transport <span class="hlt">models</span> driven by reanalysis meteorological fields for the periodmore » of <span class="hlt">observation</span> (2005–2010), but all these <span class="hlt">models</span> overestimate the lifetime due to lower abundances in the critical loss region near 32 km in the tropics. These <span class="hlt">models</span> plus a chemistry-climate <span class="hlt">model</span> agree on the nitrous oxide feedback factor on its own lifetime of 0.94 ± 0.01, giving N 2O perturbations an effective residence time of 109 years. Combining this new empirical lifetime with <span class="hlt">model</span> estimates of residence time and preindustrial lifetime (123 years) adjusts our best estimates of the human-natural balance of emissions today and improves the accuracy of projected nitrous oxide increases over this century.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....1711273B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....1711273B"><span>Higher <span class="hlt">measured</span> than <span class="hlt">modeled</span> ozone production at increased NOx levels in the Colorado Front Range</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baier, Bianca C.; Brune, William H.; Miller, David O.; Blake, Donald; Long, Russell; Wisthaler, Armin; Cantrell, Christopher; Fried, Alan; Heikes, Brian; Brown, Steven; McDuffie, Erin; Flocke, Frank; Apel, Eric; Kaser, Lisa; Weinheimer, Andrew</p> <p>2017-09-01</p> <p>Chemical <span class="hlt">models</span> must correctly calculate the ozone formation rate, P(O3), to accurately predict ozone levels and to test mitigation strategies. However, air quality <span class="hlt">models</span> can have large uncertainties in P(O3) calculations, which can create uncertainties in ozone forecasts, especially during the summertime when P(O3) is high. One way to test mechanisms is to compare <span class="hlt">modeled</span> P(O3) to direct <span class="hlt">measurements</span>. During summer 2014, the <span class="hlt">Measurement</span> of Ozone Production Sensor (MOPS) directly <span class="hlt">measured</span> net P(O3) in Golden, CO, approximately 25 km west of Denver along the Colorado Front Range. Net P(O3) was compared to rates calculated by a photochemical box <span class="hlt">model</span> that was constrained by <span class="hlt">measurements</span> of other chemical species and that used a lumped chemical mechanism and a more explicit one. Median <span class="hlt">observed</span> P(O3) was up to a factor of 2 higher than that <span class="hlt">modeled</span> during early morning hours when nitric oxide (NO) levels were high and was similar to <span class="hlt">modeled</span> P(O3) for the rest of the day. While all interferences and offsets in this new method are not fully understood, simulations of these possible uncertainties cannot explain the <span class="hlt">observed</span> P(O3) behavior. <span class="hlt">Modeled</span> and <span class="hlt">measured</span> P(O3) and peroxy radical (HO2 and RO2) discrepancies <span class="hlt">observed</span> here are similar to those presented in prior studies. While a missing atmospheric organic peroxy radical source from volatile organic compounds co-emitted with NO could be one plausible solution to the P(O3) discrepancy, such a source has not been identified and does not fully explain the peroxy radical <span class="hlt">model</span>-data mismatch. If the MOPS accurately depicts atmospheric P(O3), then these results would imply that P(O3) in Golden, CO, would be NOx-sensitive for more of the day than what is calculated by <span class="hlt">models</span>, extending the NOx-sensitive P(O3) regime from the afternoon further into the morning. These results could affect ozone reduction strategies for the region surrounding Golden and possibly other areas that do not comply with national ozone regulations</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.6726C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.6726C"><span>On the importance of <span class="hlt">measurement</span> error correlations in data assimilation for integrated hydrological <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Camporese, Matteo; Botto, Anna</p> <p>2017-04-01</p> <p>Data assimilation is becoming increasingly popular in hydrological and earth system <span class="hlt">modeling</span>, as it allows us to integrate multisource <span class="hlt">observation</span> data in <span class="hlt">modeling</span> predictions and, in doing so, to reduce uncertainty. For this reason, data assimilation has been recently the focus of much attention also for physically-based integrated hydrological <span class="hlt">models</span>, whereby multiple terrestrial compartments (e.g., snow cover, surface water, groundwater) are solved simultaneously, in an attempt to tackle environmental problems in a holistic approach. Recent examples include the joint assimilation of water table, soil moisture, and river discharge <span class="hlt">measurements</span> in catchment <span class="hlt">models</span> of coupled surface-subsurface flow using the ensemble Kalman filter (EnKF). One of the typical assumptions in these studies is that the <span class="hlt">measurement</span> errors are uncorrelated, whereas in certain situations it is reasonable to believe that some degree of correlation occurs, due for example to the fact that a pair of sensors share the same soil type. The goal of this study is to show if and how the <span class="hlt">measurement</span> error correlations between different <span class="hlt">observation</span> data play a significant role on assimilation results in a real-world application of an integrated hydrological <span class="hlt">model</span>. The <span class="hlt">model</span> CATHY (CATchment HYdrology) is applied to reproduce the hydrological dynamics <span class="hlt">observed</span> in an experimental hillslope. The physical <span class="hlt">model</span>, located in the Department of Civil, Environmental and Architectural Engineering of the University of Padova (Italy), consists of a reinforced concrete box containing a soil prism with maximum height of 3.5 m, length of 6 m, and width of 2 m. The hillslope is equipped with sensors to monitor the pressure head and soil moisture responses to a series of generated rainfall events applied onto a 60 cm thick sand layer overlying a sandy clay soil. The <span class="hlt">measurement</span> network is completed by two tipping bucket flow gages to <span class="hlt">measure</span> the two components (subsurface and surface) of the outflow. By collecting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012IJQI...1041012E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012IJQI...1041012E"><span>Proliferation of <span class="hlt">Observables</span> and <span class="hlt">Measurement</span> in Quantum-Classical Hybrids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Elze, Hans-Thomas</p> <p>2012-01-01</p> <p>Following a review of quantum-classical hybrid dynamics, we discuss the ensuing proliferation of <span class="hlt">observables</span> and relate it to <span class="hlt">measurements</span> of (would-be) quantum mechanical degrees of freedom performed by (would-be) classical ones (if they were separable). Hybrids consist in coupled classical (CL) and quantum mechanical (QM) objects. Numerous consistency requirements for their description have been discussed and are fulfilled here. We summarize a representation of quantum mechanics in terms of classical analytical mechanics which is naturally extended to QM-CL hybrids. This framework allows for superposition, separable, and entangled states originating in the QM sector, admits experimenter's "Free Will", and is local and nonsignaling. Presently, we study the set of hybrid <span class="hlt">observables</span>, which is larger than the Cartesian product of QM and CL <span class="hlt">observables</span> of its components; yet it is smaller than a corresponding product of all-classical <span class="hlt">observables</span>. Thus, quantumness and classicality infect each other.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950016767','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950016767"><span><span class="hlt">Observations</span> of the magnetopause current layer: Cases with no boundary layer and tests of recent <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Eastman, Timothy E.</p> <p>1995-01-01</p> <p>Evidence for the probable existence of magnetospheric boundary layers was first presented by Hones, et al. (1972), based on VELA satellite plasma <span class="hlt">observations</span> (no magnetic field <span class="hlt">measurements</span> were obtained). This magnetotail boundary layer is now known to be the tailward extension of the high-latitude boundary layer or plasma mantle (first uniquely identified using HEOS 2 plasma and field <span class="hlt">observations</span> by Rosenbauer et al., 1975) and the low-latitude boundary layer (first uniquely identified using IMP 6 plasma and field <span class="hlt">observations</span> by Eastman et al., 1976). The magnetospheric boundary layer is the region of magnetosheath-like plasma located Earthward of, but generally contiguous with the magnetopause. This boundary layer is typically identified by comparing low-energy (less than 10 keV) ion spectra across the magnetopause. Low-energy electron <span class="hlt">measurements</span> are also useful for identifying the boundary layer because the shocked solar wind or magnetosheath has a characteristic spectral signature for electrons as well. However, there are magnetopause crossings where low-energy electrons might suggest a depletion layer outside the magnetopause even though the traditional field-rotation signature indicates that this same region is a boundary layer Earthward of the current layer. Our analyses avoided crossings which exhibit such ambiguities. Pristine magnetopause crossings are magnetopause crossings for which the current layer is well defined and for which there is no adjoining magnetospheric boundary layer as defined above. Although most magnetopause <span class="hlt">models</span> to date apply to such crossings, few comparisons between such theory and <span class="hlt">observations</span> of pristine magnetopause crossings have been made because most crossings have an associated magnetospheric boundary layer which significantly affects the applicable boundary conditions for the magnetopause current layer. Furthermore, almost no <span class="hlt">observational</span> studies of magnetopause microstructure have been done even though key</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26429240','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26429240"><span><span class="hlt">Measurement</span> with microscopic MRI and simulation of flow in different aneurysm <span class="hlt">models</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Edelhoff, Daniel; Walczak, Lars; Frank, Frauke; Heil, Marvin; Schmitz, Inge; Weichert, Frank; Suter, Dieter</p> <p>2015-10-01</p> <p>The impact and the development of aneurysms depend to a significant degree on the exchange of liquid between the regular vessel and the pathological extension. A better understanding of this process will lead to improved prediction capabilities. The aim of the current study was to investigate fluid-exchange in aneurysm <span class="hlt">models</span> of different complexities by combining microscopic magnetic resonance <span class="hlt">measurements</span> with numerical simulations. In order to evaluate the accuracy and applicability of these methods, the fluid-exchange process between the unaltered vessel lumen and the aneurysm phantoms was analyzed quantitatively using high spatial resolution. Magnetic resonance flow imaging was used to visualize fluid-exchange in two different <span class="hlt">models</span> produced with a 3D printer. One <span class="hlt">model</span> of an aneurysm was based on histological findings. The flow distribution in the different <span class="hlt">models</span> was <span class="hlt">measured</span> on a microscopic scale using time of flight magnetic resonance imaging. The whole experiment was simulated using fast graphics processing unit-based numerical simulations. The obtained simulation results were compared qualitatively and quantitatively with the magnetic resonance imaging <span class="hlt">measurements</span>, taking into account flow and spin-lattice relaxation. The results of both presented methods compared well for the used aneurysm <span class="hlt">models</span> and the chosen flow distributions. The results from the fluid-exchange analysis showed comparable characteristics concerning <span class="hlt">measurement</span> and simulation. Similar symmetry behavior was <span class="hlt">observed</span>. Based on these results, the amount of fluid-exchange was calculated. Depending on the geometry of the <span class="hlt">models</span>, 7% to 45% of the liquid was exchanged per second. The result of the numerical simulations coincides well with the experimentally determined velocity field. The rate of fluid-exchange between vessel and aneurysm was well-predicted. Hence, the results obtained by simulation could be validated by the experiment. The <span class="hlt">observed</span> deviations can be caused by the noise</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22482332-measurement-microscopic-mri-simulation-flow-different-aneurysm-models','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22482332-measurement-microscopic-mri-simulation-flow-different-aneurysm-models"><span><span class="hlt">Measurement</span> with microscopic MRI and simulation of flow in different aneurysm <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Edelhoff, Daniel, E-mail: daniel.edelhoff@tu-dortmund.de; Frank, Frauke; Heil, Marvin</p> <p>2015-10-15</p> <p>Purpose: The impact and the development of aneurysms depend to a significant degree on the exchange of liquid between the regular vessel and the pathological extension. A better understanding of this process will lead to improved prediction capabilities. The aim of the current study was to investigate fluid-exchange in aneurysm <span class="hlt">models</span> of different complexities by combining microscopic magnetic resonance <span class="hlt">measurements</span> with numerical simulations. In order to evaluate the accuracy and applicability of these methods, the fluid-exchange process between the unaltered vessel lumen and the aneurysm phantoms was analyzed quantitatively using high spatial resolution. Methods: Magnetic resonance flow imaging was usedmore » to visualize fluid-exchange in two different <span class="hlt">models</span> produced with a 3D printer. One <span class="hlt">model</span> of an aneurysm was based on histological findings. The flow distribution in the different <span class="hlt">models</span> was <span class="hlt">measured</span> on a microscopic scale using time of flight magnetic resonance imaging. The whole experiment was simulated using fast graphics processing unit-based numerical simulations. The obtained simulation results were compared qualitatively and quantitatively with the magnetic resonance imaging <span class="hlt">measurements</span>, taking into account flow and spin–lattice relaxation. Results: The results of both presented methods compared well for the used aneurysm <span class="hlt">models</span> and the chosen flow distributions. The results from the fluid-exchange analysis showed comparable characteristics concerning <span class="hlt">measurement</span> and simulation. Similar symmetry behavior was <span class="hlt">observed</span>. Based on these results, the amount of fluid-exchange was calculated. Depending on the geometry of the <span class="hlt">models</span>, 7% to 45% of the liquid was exchanged per second. Conclusions: The result of the numerical simulations coincides well with the experimentally determined velocity field. The rate of fluid-exchange between vessel and aneurysm was well-predicted. Hence, the results obtained by simulation could be validated by the experiment</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25685433','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25685433"><span>Comparison of COSMIC <span class="hlt">measurements</span> with the IRI-2007 <span class="hlt">model</span> over the eastern Mediterranean region.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vryonides, P; Haralambous, H</p> <p>2013-05-01</p> <p>This paper presents a comparison of the International Reference Ionosphere (IRI-2007) <span class="hlt">model</span> over the eastern Mediterranean region with peak ionospheric characteristics (foF2-hmF2) and electron density profiles <span class="hlt">measured</span> by FORMOSAT-3/COSMIC satellites in terms of GPS radio occultation technique and the Cyprus digisonde. In the absence of systematic ionosonde <span class="hlt">measurements</span> over this area, COSMIC <span class="hlt">measurements</span> provide an opportunity to perform such a study by considering <span class="hlt">observations</span> for year 2010 to investigate the behaviour of the IRI-2007 <span class="hlt">model</span> over the eastern Mediterranean area.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1377489-multi-scale-comparison-modeled-observed-seasonal-methane-emissions-northern-wetlands','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1377489-multi-scale-comparison-modeled-observed-seasonal-methane-emissions-northern-wetlands"><span>A multi-scale comparison of <span class="hlt">modeled</span> and <span class="hlt">observed</span> seasonal methane emissions in northern wetlands</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Xu, Xiyan; Riley, William J.; Koven, Charles D.; ...</p> <p>2016-09-13</p> <p>Wetlands are the largest global natural methane (CH 4) source, and emissions between 50 and 70° N latitude contribute 10-30 % to this source. Predictive capability of land <span class="hlt">models</span> for northern wetland CH 4 emissions is still low due to limited site <span class="hlt">measurements</span>, strong spatial and temporal variability in emissions, and complex hydrological and biogeochemical dynamics. To explore this issue, we compare wetland CH 4 emission predictions from the Community Land <span class="hlt">Model</span> 4.5 (CLM4.5-BGC) with site- to regional-scale <span class="hlt">observations</span>. A comparison of the CH 4 fluxes with eddy flux data highlighted needed changes to the <span class="hlt">model</span>'s estimate of aerenchyma area,more » which we implemented and tested. The <span class="hlt">model</span> modification substantially reduced biases in CH 4 emissions when compared with CarbonTracker CH 4 predictions. CLM4.5 CH 4 emission predictions agree well with growing season (May–September) CarbonTracker Alaskan regional-level CH 4 predictions and site-level <span class="hlt">observations</span>. However, CLM4.5 underestimated CH 4 emissions in the cold season (October–April). The monthly atmospheric CH 4 mole fraction enhancements due to wetland emissions are also assessed using the Weather Research and Forecasting-Stochastic Time-Inverted Lagrangian Transport (WRF-STILT) <span class="hlt">model</span> coupled with daily emissions from CLM4.5 and compared with aircraft CH 4 mole fraction <span class="hlt">measurements</span> from the Carbon in Arctic Reservoirs Vulnerability Experiment (CARVE) campaign. Both the tower and aircraft analyses confirm the underestimate of cold-season CH 4 emissions by CLM4.5. The greatest uncertainties in predicting the seasonal CH 4 cycle are from the wetland extent, cold-season CH 4 production and CH 4 transport processes. We recommend more cold-season experimental studies in high-latitude systems, which could improve the understanding and parameterization of ecosystem structure and function during this period. Predicted CH 4 emissions remain uncertain, but we show here that benchmarking against <span class="hlt">observations</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1377489','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1377489"><span>A multi-scale comparison of <span class="hlt">modeled</span> and <span class="hlt">observed</span> seasonal methane emissions in northern wetlands</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Xu, Xiyan; Riley, William J.; Koven, Charles D.</p> <p></p> <p>Wetlands are the largest global natural methane (CH 4) source, and emissions between 50 and 70° N latitude contribute 10-30 % to this source. Predictive capability of land <span class="hlt">models</span> for northern wetland CH 4 emissions is still low due to limited site <span class="hlt">measurements</span>, strong spatial and temporal variability in emissions, and complex hydrological and biogeochemical dynamics. To explore this issue, we compare wetland CH 4 emission predictions from the Community Land <span class="hlt">Model</span> 4.5 (CLM4.5-BGC) with site- to regional-scale <span class="hlt">observations</span>. A comparison of the CH 4 fluxes with eddy flux data highlighted needed changes to the <span class="hlt">model</span>'s estimate of aerenchyma area,more » which we implemented and tested. The <span class="hlt">model</span> modification substantially reduced biases in CH 4 emissions when compared with CarbonTracker CH 4 predictions. CLM4.5 CH 4 emission predictions agree well with growing season (May–September) CarbonTracker Alaskan regional-level CH 4 predictions and site-level <span class="hlt">observations</span>. However, CLM4.5 underestimated CH 4 emissions in the cold season (October–April). The monthly atmospheric CH 4 mole fraction enhancements due to wetland emissions are also assessed using the Weather Research and Forecasting-Stochastic Time-Inverted Lagrangian Transport (WRF-STILT) <span class="hlt">model</span> coupled with daily emissions from CLM4.5 and compared with aircraft CH 4 mole fraction <span class="hlt">measurements</span> from the Carbon in Arctic Reservoirs Vulnerability Experiment (CARVE) campaign. Both the tower and aircraft analyses confirm the underestimate of cold-season CH 4 emissions by CLM4.5. The greatest uncertainties in predicting the seasonal CH 4 cycle are from the wetland extent, cold-season CH 4 production and CH 4 transport processes. We recommend more cold-season experimental studies in high-latitude systems, which could improve the understanding and parameterization of ecosystem structure and function during this period. Predicted CH 4 emissions remain uncertain, but we show here that benchmarking against <span class="hlt">observations</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=coding+AND+sheet&pg=4&id=ED231502','ERIC'); return false;" href="https://eric.ed.gov/?q=coding+AND+sheet&pg=4&id=ED231502"><span>Development of an <span class="hlt">Observational</span> Scale to <span class="hlt">Measure</span> Social Competence in Young Children.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Porter, Robin</p> <p></p> <p>An <span class="hlt">observational</span> instrument was developed to <span class="hlt">measure</span> social competence in kindergarten classrooms. Social competence was specified in terms of four broad behavioral categories: obedience, cooperation, interaction, and autonomy. Each category was further particularized in terms of <span class="hlt">observable</span> behaviors. Initial 5-minute <span class="hlt">observations</span> using the…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PMB....63g5011A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PMB....63g5011A"><span>A simple parametric <span class="hlt">model</span> <span class="hlt">observer</span> for quality assurance in computer tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anton, M.; Khanin, A.; Kretz, T.; Reginatto, M.; Elster, C.</p> <p>2018-04-01</p> <p><span class="hlt">Model</span> <span class="hlt">observers</span> are mathematical classifiers that are used for the quality assessment of imaging systems such as computer tomography. The quality of the imaging system is quantified by means of the performance of a selected <span class="hlt">model</span> <span class="hlt">observer</span>. For binary classification tasks, the performance of the <span class="hlt">model</span> <span class="hlt">observer</span> is defined by the area under its ROC curve (AUC). Typically, the AUC is estimated by applying the <span class="hlt">model</span> <span class="hlt">observer</span> to a large set of training and test data. However, the recording of these large data sets is not always practical for routine quality assurance. In this paper we propose as an alternative a parametric <span class="hlt">model</span> <span class="hlt">observer</span> that is based on a simple phantom, and we provide a Bayesian estimation of its AUC. It is shown that a limited number of repeatedly recorded images (10–15) is already sufficient to obtain results suitable for the quality assessment of an imaging system. A MATLAB® function is provided for the calculation of the results. The performance of the proposed <span class="hlt">model</span> <span class="hlt">observer</span> is compared to that of the established channelized Hotelling <span class="hlt">observer</span> and the nonprewhitening matched filter for simulated images as well as for images obtained from a low-contrast phantom on an x-ray tomography scanner. The results suggest that the proposed parametric <span class="hlt">model</span> <span class="hlt">observer</span>, along with its Bayesian treatment, can provide an efficient, practical alternative for the quality assessment of CT imaging systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930067430&hterms=models+linear&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmodels%2Blinear','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930067430&hterms=models+linear&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmodels%2Blinear"><span>Linear system identification via backward-time <span class="hlt">observer</span> <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Juang, Jer-Nan; Phan, Minh</p> <p>1993-01-01</p> <p>This paper presents an algorithm to identify a state-space <span class="hlt">model</span> of a linear system using a backward-time approach. The procedure consists of three basic steps. First, the Markov parameters of a backward-time <span class="hlt">observer</span> are computed from experimental input-output data. Second, the backward-time <span class="hlt">observer</span> Markov parameters are decomposed to obtain the backward-time system Markov parameters (backward-time pulse response samples) from which a backward-time state-space <span class="hlt">model</span> is realized using the Eigensystem Realization Algorithm. Third, the obtained backward-time state space <span class="hlt">model</span> is converted to the usual forward-time representation. Stochastic properties of this approach will be discussed. Experimental results are given to illustrate when and to what extent this concept works.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=129661','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=129661"><span>Evaluation of the Clinical LOINC (Logical <span class="hlt">Observation</span> Identifiers, Names, and Codes) Semantic Structure as a Terminology <span class="hlt">Model</span> for Standardized Assessment <span class="hlt">Measures</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bakken, Suzanne; Cimino, James J.; Haskell, Robert; Kukafka, Rita; Matsumoto, Cindi; Chan, Garrett K.; Huff, Stanley M.</p> <p>2000-01-01</p> <p>Objective: The purpose of this study was to test the adequacy of the Clinical LOINC (Logical <span class="hlt">Observation</span> Identifiers, Names, and Codes) semantic structure as a terminology <span class="hlt">model</span> for standardized assessment <span class="hlt">measures</span>. Methods: After extension of the definitions, 1,096 items from 35 standardized assessment instruments were dissected into the elements of the Clinical LOINC semantic structure. An additional coder dissected at least one randomly selected item from each instrument. When multiple scale types occurred in a single instrument, a second coder dissected one randomly selected item representative of each scale type. Results: The results support the adequacy of the Clinical LOINC semantic structure as a terminology <span class="hlt">model</span> for standardized assessments. Using the revised definitions, the coders were able to dissect into the elements of Clinical LOINC all the standardized assessment items in the sample instruments. Percentage agreement for each element was as follows: component, 100 percent; property, 87.8 percent; timing, 82.9 percent; system/sample, 100 percent; scale, 92.6 percent; and method, 97.6 percent. Discussion: This evaluation was an initial step toward the representation of standardized assessment items in a manner that facilitates data sharing and re-use. Further clarification of the definitions, especially those related to time and property, is required to improve inter-rater reliability and to harmonize the representations with similar items already in LOINC. PMID:11062226</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/948516','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/948516"><span>A Comparison of Water Vapor Quantities from <span class="hlt">Model</span> Short-Range Forecasts and ARM <span class="hlt">Observations</span> (in English; Croatian)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Hnilo, J.</p> <p>2006-03-17</p> <p><span class="hlt">Model</span> evolution and improvement is complicated by the lack of high quality <span class="hlt">observational</span> data. To address a major limitation of these <span class="hlt">measurements</span> the Atmospheric Radiation <span class="hlt">Measurement</span> (ARM) program was formed. For the second quarter ARM metric we will make use of new water vapor data that has become available, and called the “Mergedsounding” value added product (referred to as OBS, within the text) at three sites: the North Slope of Alaska (NSA), Darwin Australia (DAR) and the Southern Great Plains (SGP) and compare these <span class="hlt">observations</span> to <span class="hlt">model</span> forecast data. Two time periods will be analyzed March 2000 for the SGPmore » and October 2004 for both DAR and NSA. The merged-sounding data have been interpolated to 37 pressure levels (e.g., from 1000hPa to 100hPa at 25hPa increments) and time averaged to 3 hourly data for direct comparison to our <span class="hlt">model</span> output.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000109960&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D40%26Ntt%3DRussell','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000109960&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D40%26Ntt%3DRussell"><span>Comparison of Columnar Water Vapor <span class="hlt">Measurements</span> During The Fall 1997 ARM Intensive <span class="hlt">Observation</span> Period: Optical Methods</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schmid, Beat; Michalsky, J.; Slater, D.; Barnard, J.; Halthore, R.; Liljegren, J.; Holben, B.; Eck, T.; Livingston, J.; Russell, P.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20000109960'); toggleEditAbsImage('author_20000109960_show'); toggleEditAbsImage('author_20000109960_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20000109960_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20000109960_hide"></p> <p>2000-01-01</p> <p>In the fall of 1997 the Atmospheric Radiation <span class="hlt">Measurement</span> (ARM program conducted an intensive <span class="hlt">Observation</span> Period (IOP) to study water vapor at its Southern Great Plains (SGP) site. Among the large number of instruments, four sun-tracking radiometers were present to <span class="hlt">measure</span> the columnar water vapor (CWV). All four solar radiometers retrieve CWV by <span class="hlt">measuring</span> solar transmittance in the 0.94-micrometer water vapor absorption band. As one of the steps in the CWV retrievals the aerosol component is subtracted from the total transmittance, in the 0.94-micrometer band. The aerosol optical depth comparisons among the same four radiometers are presented elsewhere. We have used three different methods to retrieve CWV. Without attempting to standardize on the same radiative transfer <span class="hlt">model</span> and its underlying water vapor spectroscopy we found the CWV to agree within 0.13 cm (rms) for CWV values ranging from 1 to 5 cm. Preliminary results obtained when using the same updated radiative transfer <span class="hlt">model</span> with updated spectroscopy for all instruments will also be shown. Comparisons to the microwave radiometer results will be included in the comparisons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040089037&hterms=wheat&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dwheat','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040089037&hterms=wheat&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dwheat"><span>Growing wheat in Biosphere 2 under elevated CO2: <span class="hlt">observations</span> and <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tubiello, F. N.; Mahato, T.; Morton, T.; Druitt, J. W.; Volk, T.; Marino, B. D.</p> <p>1999-01-01</p> <p>Spring wheat (Triticum aestivum L., cv. Yecora Rojo) was grown in the intensive agricultural biome (IAB) of Biosphere 2 during the l995-l996 winter/spring season. Environmental conditions were characterized by a day/night temperature regime of 27/17 degrees C, relative humidity (RH) levels around 45%, mean atmospheric CO2 concentration of 450 ppmv, and natural light conditions with mean intensities about half of outside levels. Weekly samples of above-ground plant matter were collected throughout the growing season and phenological events recorded. A computer <span class="hlt">model</span>, CERES-Wheat, previously tested under both field and controlled conditions, was used to simulate the <span class="hlt">observed</span> crop growth and to help in data analysis. We found that CERES-Wheat simulated the data collected at Biosphere 2 to within 10% of <span class="hlt">observed</span>, thus suggesting that wheat growth inside the IAB was comparable to that documented in other environments. The <span class="hlt">model</span> predicts phenological stages and final dry matter (DM) production within l0% of the <span class="hlt">observed</span> data. <span class="hlt">Measured</span> DM production rates, normalized for light absorbed by the crop. suggested photosynthetic efficiencies intermediate between those <span class="hlt">observed</span> under optimal field conditions and those recorded in NASA-Controlled Ecological Life-Support Systems (CELSS). We suggest that such a difference can be explained primarily in terms of low light levels inside the IAB, with additional effects due to elevated CO2 concentrations and diffuse light fractions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMNH21C1828O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMNH21C1828O"><span>Internal Gravity Wave Induced by the Queen Charlotte Event (27 October 2012, Mw 7.8): Airglow <span class="hlt">Observation</span> and <span class="hlt">Modeling</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Occhipinti, G.; Bablet, A.; Makela, J. J.</p> <p>2015-12-01</p> <p>The detection of the tsunami related internal gravity waves (IGWtsuna) by airglow camera has been recently validated by <span class="hlt">observation</span> (Makela et al., 2011) and <span class="hlt">modeling</span> (Occhipinti et al., 2011) in the case of the Tohoku event (11 March 2011, Mw 9.0). The airglow is <span class="hlt">measuring</span> the photon emission at 630 nm, indirectly linked to the plasma density of O2+ (Link & Cogger, 1988) and it is commonly used to detect transient event in the ionosphere (Kelley et al., 2002, Makela et al., 2009, Miller et al., 2009). The <span class="hlt">modeling</span> of the IGWtsuna clearly reproduced the pattern of the airglow <span class="hlt">measurement</span> <span class="hlt">observed</span> over Hawaii and the comparison between the <span class="hlt">observation</span> and the <span class="hlt">modeling</span> allows to recognize the wave form and allow to explain the IGWtsuna arriving before the tsunami wavefront at the sea level (Occhipinti et al., 2011). Approaching the Hawaiian archipelagos the tsunami propagation is slowed down (reduction of the sea depth), instead, the IGWtsuna, propagating in the atmosphere/ionosphere, conserves its speed. In this work, we present the <span class="hlt">modeling</span> of the new airglow <span class="hlt">observation</span> following the Queen Charlotte event (27 October 2012, Mw 7.8) that has been recently detected, proving that the technique can be generalized for smaller events. Additionally, the effect of the wind on the IGWtsuna, already evocated in the past, is included in the <span class="hlt">modeling</span> to better reproduce the airglow <span class="hlt">observations</span>. All ref. here @ www.ipgp.fr/~ninto</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AIPC.1703e0009K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AIPC.1703e0009K"><span>Intracochlear pressure <span class="hlt">measurements</span> in scala media inform <span class="hlt">models</span> of cochlear mechanics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kale, Sushrut; Olson, Elizabeth S.</p> <p>2015-12-01</p> <p>In the classic view of cochlear mechanics, the cochlea is comprised of two identical fluid chambers separated by the cochlear partition (CP). In this view the traveling wave pressures in the two chambers mirror each other; they are equal in magnitude and opposite in phase. A fast pressure mode adds approximately uniformly. More recent <span class="hlt">models</span> of cochlear mechanics take into account the structural complexity of the CP and the resulting additional mechanical modes would lead to distinct (non-symmetric) patterns of pressure and motion on the two sides of the CP. However, there was little to no physiological data that explored these predictions. To this aim, we <span class="hlt">measured</span> intracochlear fluid pressure in scala media (SM), including <span class="hlt">measurements</span> close to the sensory tissue, using miniaturized pressure sensors (˜ 80 μm outer diameter). <span class="hlt">Measurements</span> were made in-vivo from the basal cochlear turn in gerbils. SM pressure was <span class="hlt">measured</span> at two longitudinal locations in different preparations. In a subset of the experiments SM and ST (scala tympani) pressures were <span class="hlt">measured</span> at the same longitudinal location. Traveling wave pressures were <span class="hlt">observed</span> in both SM and ST, and showed the relative phase predicted by the classical theory. In addition, SM pressure showed spatial variations that had not been <span class="hlt">observed</span> in ST, which points to a relatively complex CP motion on the SM side. These data both underscore the first-order validity of the classic cochlear traveling wave <span class="hlt">model</span>, and open a new view to CP mechanics.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4150295','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4150295"><span>A perspective on sustained marine <span class="hlt">observations</span> for climate <span class="hlt">modelling</span> and prediction</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Dunstone, Nick J.</p> <p>2014-01-01</p> <p>Here, I examine some of the many varied ways in which sustained global ocean <span class="hlt">observations</span> are used in numerical <span class="hlt">modelling</span> activities. In particular, I focus on the use of ocean <span class="hlt">observations</span> to initialize predictions in ocean and climate <span class="hlt">models</span>. Examples are also shown of how <span class="hlt">models</span> can be used to assess the impact of both current ocean <span class="hlt">observations</span> and to simulate that of potential new ocean <span class="hlt">observing</span> platforms. The ocean has never been better <span class="hlt">observed</span> than it is today and similarly ocean <span class="hlt">models</span> have never been as capable at representing the real ocean as they are now. However, there remain important unanswered questions that can likely only be addressed via future improvements in ocean <span class="hlt">observations</span>. In particular, ocean <span class="hlt">observing</span> systems need to respond to the needs of the burgeoning field of near-term climate predictions. Although new ocean <span class="hlt">observing</span> platforms promise exciting new discoveries, there is a delicate balance to be made between their funding and that of the current ocean <span class="hlt">observing</span> system. Here, I identify the need to secure long-term funding for ocean <span class="hlt">observing</span> platforms as they mature, from a mainly research exercise to an operational system for sustained <span class="hlt">observation</span> over climate change time scales. At the same time, considerable progress continues to be made via ship-based <span class="hlt">observing</span> campaigns and I highlight some that are dedicated to addressing uncertainties in key ocean <span class="hlt">model</span> parametrizations. The use of ocean <span class="hlt">observations</span> to understand the prominent long time scale changes <span class="hlt">observed</span> in the North Atlantic is another focus of this paper. The exciting first decade of monitoring of the Atlantic meridional overturning circulation by the RAPID-MOCHA array is highlighted. The use of ocean and climate <span class="hlt">models</span> as tools to further probe the drivers of variability seen in such time series is another exciting development. I also discuss the need for a concerted combined effort from climate <span class="hlt">models</span> and ocean <span class="hlt">observations</span> in order to understand the current slow</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25157195','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25157195"><span>A perspective on sustained marine <span class="hlt">observations</span> for climate <span class="hlt">modelling</span> and prediction.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dunstone, Nick J</p> <p>2014-09-28</p> <p>Here, I examine some of the many varied ways in which sustained global ocean <span class="hlt">observations</span> are used in numerical <span class="hlt">modelling</span> activities. In particular, I focus on the use of ocean <span class="hlt">observations</span> to initialize predictions in ocean and climate <span class="hlt">models</span>. Examples are also shown of how <span class="hlt">models</span> can be used to assess the impact of both current ocean <span class="hlt">observations</span> and to simulate that of potential new ocean <span class="hlt">observing</span> platforms. The ocean has never been better <span class="hlt">observed</span> than it is today and similarly ocean <span class="hlt">models</span> have never been as capable at representing the real ocean as they are now. However, there remain important unanswered questions that can likely only be addressed via future improvements in ocean <span class="hlt">observations</span>. In particular, ocean <span class="hlt">observing</span> systems need to respond to the needs of the burgeoning field of near-term climate predictions. Although new ocean <span class="hlt">observing</span> platforms promise exciting new discoveries, there is a delicate balance to be made between their funding and that of the current ocean <span class="hlt">observing</span> system. Here, I identify the need to secure long-term funding for ocean <span class="hlt">observing</span> platforms as they mature, from a mainly research exercise to an operational system for sustained <span class="hlt">observation</span> over climate change time scales. At the same time, considerable progress continues to be made via ship-based <span class="hlt">observing</span> campaigns and I highlight some that are dedicated to addressing uncertainties in key ocean <span class="hlt">model</span> parametrizations. The use of ocean <span class="hlt">observations</span> to understand the prominent long time scale changes <span class="hlt">observed</span> in the North Atlantic is another focus of this paper. The exciting first decade of monitoring of the Atlantic meridional overturning circulation by the RAPID-MOCHA array is highlighted. The use of ocean and climate <span class="hlt">models</span> as tools to further probe the drivers of variability seen in such time series is another exciting development. I also discuss the need for a concerted combined effort from climate <span class="hlt">models</span> and ocean <span class="hlt">observations</span> in order to understand the current slow</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMIN21D0070F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMIN21D0070F"><span>Obs4MIPS: Satellite <span class="hlt">Observations</span> for <span class="hlt">Model</span> Evaluation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferraro, R.; Waliser, D. E.; Gleckler, P. J.</p> <p>2017-12-01</p> <p>This poster will review the current status of the obs4MIPs project, whose purpose is to provide a limited collection of well-established and documented datasets for comparison with Earth system <span class="hlt">models</span> (https://www.earthsystemcog.org/projects/obs4mips/). These datasets have been reformatted to correspond with the CMIP5 <span class="hlt">model</span> output requirements, and include technical documentation specifically targeted for their use in <span class="hlt">model</span> output evaluation. The project holdings now exceed 120 datasets with <span class="hlt">observations</span> that directly correspond to CMIP5 <span class="hlt">model</span> output variables, with new additions in response to the CMIP6 experiments. With the growth in climate <span class="hlt">model</span> output data volume, it is increasing more difficult to bring the <span class="hlt">model</span> output and the <span class="hlt">observations</span> together to do evaluations. The positioning of the obs4MIPs datasets within the Earth System Grid Federation (ESGF) allows for the use of currently available and planned online tools within the ESGF to perform analysis using <span class="hlt">model</span> output and <span class="hlt">observational</span> datasets without necessarily downloading everything to a local workstation. This past year, obs4MIPs has updated its submission guidelines to closely align with changes in the CMIP6 experiments, and is implementing additional indicators and ancillary data to allow users to more easily determine the efficacy of an obs4MIPs dataset for specific evaluation purposes. This poster will present the new guidelines and indicators, and update the list of current obs4MIPs holdings and their connection to the ESGF evaluation and analysis tools currently available, and being developed for the CMIP6 experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AtmRe.197....1T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AtmRe.197....1T"><span>Global precipitation <span class="hlt">measurements</span> for validating climate <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tapiador, F. J.; Navarro, A.; Levizzani, V.; García-Ortega, E.; Huffman, G. J.; Kidd, C.; Kucera, P. A.; Kummerow, C. D.; Masunaga, H.; Petersen, W. A.; Roca, R.; Sánchez, J.-L.; Tao, W.-K.; Turk, F. J.</p> <p>2017-11-01</p> <p>The advent of global precipitation data sets with increasing temporal span has made it possible to use them for validating climate <span class="hlt">models</span>. In order to fulfill the requirement of global coverage, existing products integrate satellite-derived retrievals from many sensors with direct ground <span class="hlt">observations</span> (gauges, disdrometers, radars), which are used as reference for the satellites. While the resulting product can be deemed as the best-available source of quality validation data, awareness of the limitations of such data sets is important to avoid extracting wrong or unsubstantiated conclusions when assessing climate <span class="hlt">model</span> abilities. This paper provides guidance on the use of precipitation data sets for climate research, including <span class="hlt">model</span> validation and verification for improving physical parameterizations. The strengths and limitations of the data sets for climate <span class="hlt">modeling</span> applications are presented, and a protocol for quality assurance of both <span class="hlt">observational</span> databases and <span class="hlt">models</span> is discussed. The paper helps elaborating the recent IPCC AR5 acknowledgment of large <span class="hlt">observational</span> uncertainties in precipitation <span class="hlt">observations</span> for climate <span class="hlt">model</span> validation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B13J..05L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B13J..05L"><span>Quantifying Fire Impact on Alaskan Tundra from Satellite <span class="hlt">Observations</span> and Field <span class="hlt">Measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Loboda, T. V.; Chen, D.; He, J.; Jenkins, L. K.</p> <p>2017-12-01</p> <p>Wildfire is a major disturbance agent in Alaskan tundra. The frequency and extent of fire events obtained from paleo, management, and satellite records may yet underestimate the scope of tundra fire impact. Field <span class="hlt">measurements</span>, collected within the NASA's ABoVE campaign, revealed unexpectedly shallow organic soils ( 15 cm) across all sampled sites of the Noatak valley with no significant difference between recently burned and unburned sites. In typical small and medium-sized tundra burns vegetation recovers rapidly and scars are not discernable in 30 m optical satellite imagery by the end of the first post-fire season. However, field <span class="hlt">observations</span> indicate that vegetation and subsurface characteristics within fire scars of different ages vary across the landscape. In this study we develop linkages between fire-induced changes to tundra and satellite-based <span class="hlt">observations</span> from optical, thermal, and microwave imagers to enable extrapolation of in-situ <span class="hlt">observations</span> to cover the full extent of Alaskan tundra. Our results show that recent ( 30 years) fire history can be reconstructed from optical <span class="hlt">observations</span> (R2 0.65, p<0.001) within a specific narrow temporal window or thermal signatures (R2 0.54, p < 0.001), in both cases controlled for slope and southern exposure. Using microwave SAR imagery fire history can be determined for 4 years post fire primarily due to increased soil moisture at burned sites. Field <span class="hlt">measurements</span> suggest that the relatively quick SAR signal dissipation results from more even distribution of surface moisture through the soil column with increases in Active Layer Thickness (ALT). Similar to previous long-term field studies we find an increase in shrub fraction and shrub height within burns over time at the landscape scale; however, the strength and significance of the relationship between shrub fraction and time since fire is governed by burn severity with more severe burns predictably (p < 0.01) resulting in higher post-fire shrub cover. Although</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A24C..07L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A24C..07L"><span><span class="hlt">Observations</span> and <span class="hlt">Model</span> Simulations of Orographic Mixed-Phase Clouds at Mountain Range Site</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lohmann, U.; Henneberg, O. C.; Henneberger, J.</p> <p>2014-12-01</p> <p>Aerosol-cloud interactions constitute the highest uncertainties in forcing estimation. Especially uncertainties due to mixed clouds (MPCs) have a large impact on the radiative balance and precipitation prediction. Due to Wegener-Bergeron-Findeisen-process (WBF) which describes glaciation of MPCs due to the lower saturation over ice than over water, MPCs are mostly expected as short lived clouds. In contrast to the theory of the WBF, in-situ <span class="hlt">measurements</span> have shown that MPCs can persist over longer time. But only a small number of <span class="hlt">measurements</span> of MPCs is available. In addition <span class="hlt">modeling</span> studies about MPCs are difficult as their processes of the three-phase-system are on the micro scale and therefore not resolved in <span class="hlt">models</span>. We present <span class="hlt">measurements</span> obtained at the high-altitude research station Jungfraujoch (JFJ, 3580 m asl) in the Swiss Alps partly taken during the CLoud-Aerosol Interaction Experiments (CLACE). During the winter season, the JFJ has a high frequency of super-cooled clouds and is considered representative for being in the free troposphere. In-situ <span class="hlt">measurements</span> of the microstructure of MPCs have been obtained with the digital imager HOLIMO, that delivers phase-resolved size distributions, concentrations, and water contents. The data set of MPCs at JFJ shows that for northerly wind cases partially-glaciated MPCs are more frequently <span class="hlt">observed</span> than for southerly wind cases. The higher frequency of these intermediate states of MPCs suggests either higher updraft velocities, and therefore higher water-vapor supersaturations, or the absence of sufficiently high IN concentrations to quickly glaciate the MPC. Because of the limitation of in-situ information, i.e. point <span class="hlt">measurements</span> and missing <span class="hlt">measurements</span> of vertical velocities at JFJ, the mechanism of the long persistence of MPCs cannot be fully understood. Therefore, in addition to <span class="hlt">measurements</span> we will investigate the JFJ region with a <span class="hlt">model</span> study with the non-hydrostatic <span class="hlt">model</span> COSMO-ART-M7. Combination of km</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880066225&hterms=Abreu&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAbreu%252C%2Bc.','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880066225&hterms=Abreu&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAbreu%252C%2Bc."><span>The auroral 6300 A emission - <span class="hlt">Observations</span> and <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Solomon, Stanley C.; Hays, Paul B.; Abreu, Vincent J.</p> <p>1988-01-01</p> <p>A tomographic inversion is used to analyze <span class="hlt">measurements</span> of the auroral atomic oxygen emission line at 6300 A made by the atmosphere explorer visible airglow experiment. A comparison is made between emission altitude profiles and the results from an electron transport and chemical reaction <span class="hlt">model</span>. <span class="hlt">Measurements</span> of the energetic electron flux, neutral composition, ion composition, and electron density are incorporated in the <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMAE21A0229D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMAE21A0229D"><span>Comparison between <span class="hlt">model</span> predictions and <span class="hlt">observations</span> of ELF radio atmospherics generated by rocket-triggered lightning</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dupree, N. A.; Moore, R. C.</p> <p>2011-12-01</p> <p><span class="hlt">Model</span> predictions of the ELF radio atmospheric generated by rocket-triggered lightning are compared with <span class="hlt">observations</span> performed at Arrival Heights, Antarctica. The ability to infer source characteristics using <span class="hlt">observations</span> at great distances may prove to greatly enhance the understanding of lightning processes that are associated with the production of transient luminous events (TLEs) as well as other ionospheric effects associated with lightning. The <span class="hlt">modeling</span> of the sferic waveform is carried out using a modified version of the Long Wavelength Propagation Capability (LWPC) code developed by the Naval Ocean Systems Center over a period of many years. LWPC is an inherently narrowband propagation code that has been modified to predict the broadband response of the Earth-ionosphere waveguide to an impulsive lightning flash while preserving the ability of LWPC to account for an inhomogeneous waveguide. ELF <span class="hlt">observations</span> performed at Arrival Heights, Antarctica during rocket-triggered lightning experiments at the International Center for Lightning Research and Testing (ICLRT) located at Camp Blanding, Florida are presented. The lightning current waveforms directly <span class="hlt">measured</span> at the base of the lightning channel (at the ICLRT) are used together with LWPC to predict the sferic waveform <span class="hlt">observed</span> at Arrival Heights under various ionospheric conditions. This paper critically compares <span class="hlt">observations</span> with <span class="hlt">model</span> predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1379757-measurements-top-quark-spin-observables-overline-events-using-dilepton-final-states-sqrt-tev-pp-collisions-atlas-detector','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1379757-measurements-top-quark-spin-observables-overline-events-using-dilepton-final-states-sqrt-tev-pp-collisions-atlas-detector"><span><span class="hlt">Measurements</span> of top quark spin <span class="hlt">observables</span> in $$ t\\overline{t} $$ events using dilepton final states in $$ \\sqrt{s}=8 $$ TeV pp collisions with the ATLAS detector</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Aaboud, M.; Aad, G.; Abbott, B.; ...</p> <p>2017-03-22</p> <p><span class="hlt">Measurements</span> of top quark spin <span class="hlt">observables</span> in tt¯ events are presented based on 20.2 fb –1 of √s = 8 TeV proton-proton collisions recorded with the ATLAS detector at the LHC. The analysis is performed in the dilepton final state, characterised by the presence of two isolated leptons (electrons or muons). There are 15 <span class="hlt">observables</span>, each sensitive to a different coefficient of the spin density matrix of tt¯ production, which are <span class="hlt">measured</span> independently. Ten of these <span class="hlt">observables</span> are <span class="hlt">measured</span> for the first time. All of them are corrected for detector resolution and acceptance effects back to the parton and stable-particlemore » levels. The <span class="hlt">measured</span> values of the <span class="hlt">observables</span> at parton level are compared to Standard <span class="hlt">Model</span> predictions at next-to-leading order in QCD. The corrected distributions at stable-particle level are presented and the means of the distributions are compared to Monte Carlo predictions. No significant deviation from the Standard <span class="hlt">Model</span> is <span class="hlt">observed</span> for any <span class="hlt">observable</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1379757','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1379757"><span><span class="hlt">Measurements</span> of top quark spin <span class="hlt">observables</span> in $$ t\\overline{t} $$ events using dilepton final states in $$ \\sqrt{s}=8 $$ TeV pp collisions with the ATLAS detector</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Aaboud, M.; Aad, G.; Abbott, B.</p> <p></p> <p><span class="hlt">Measurements</span> of top quark spin <span class="hlt">observables</span> in tt¯ events are presented based on 20.2 fb –1 of √s = 8 TeV proton-proton collisions recorded with the ATLAS detector at the LHC. The analysis is performed in the dilepton final state, characterised by the presence of two isolated leptons (electrons or muons). There are 15 <span class="hlt">observables</span>, each sensitive to a different coefficient of the spin density matrix of tt¯ production, which are <span class="hlt">measured</span> independently. Ten of these <span class="hlt">observables</span> are <span class="hlt">measured</span> for the first time. All of them are corrected for detector resolution and acceptance effects back to the parton and stable-particlemore » levels. The <span class="hlt">measured</span> values of the <span class="hlt">observables</span> at parton level are compared to Standard <span class="hlt">Model</span> predictions at next-to-leading order in QCD. The corrected distributions at stable-particle level are presented and the means of the distributions are compared to Monte Carlo predictions. No significant deviation from the Standard <span class="hlt">Model</span> is <span class="hlt">observed</span> for any <span class="hlt">observable</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4104P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4104P"><span>How to misinterpret photosynthesis <span class="hlt">measurements</span> and develop incorrect ecosystem <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prentice, Iain Colin</p> <p>2017-04-01</p> <p>It is becoming widely accepted than current land ecosystem <span class="hlt">models</span> (dynamic global vegetation <span class="hlt">models</span> and land-surface <span class="hlt">models</span>) rest on shaky foundations and are in need of rebuilding, taking advantage of huge data resources that were hardly conceivable when these <span class="hlt">models</span> were first developed. It has also become almost a truism that next-generation <span class="hlt">model</span> development should involve observationalists, experimentalists and <span class="hlt">modellers</span> working more closely together. What is currently lacking, however, is open discussion of specific problems in the structure of current <span class="hlt">models</span>, and how they might have arisen. Such a discussion is important if the same mistakes are not to be perpetuated in a new generation of <span class="hlt">models</span>. I will focus on the central processes governing leaf-level gas exchange, which powers the land carbon and water cycles. I will show that a broad area of confusion exists - as much in the empirical ecophysiological literature as in <span class="hlt">modelling</span> research - concerning the interpretation of gas-exchange <span class="hlt">measurements</span> and (especially) their scaling up from the narrow temporal and spatial scales of laboratory <span class="hlt">measurements</span> to the broad-scale research questions linked to global environmental change. In particular, I will provide examples (drawing on a variety of published and unpublished <span class="hlt">observations</span>) that illustrate the benefits of taking a "plant-centred" view, showing how consideration of optimal acclimation challenges many (often untstated) assumptions about the relationship of plant and ecosystem processes to environmental variation. (1) Photosynthesis is usually <span class="hlt">measured</span> at light saturation (implying Rubisco limitation), leading to temperature and CO2 responses that are completely different from those of gross primary production (GPP) under field conditions. (2) The actual rate of electron transport under field conditions depends strongly on the intrinsic quantum efficiency, which is temperature-independent (within a broad range) and unrelated to the maximum electron</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004cosp...35.1656D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004cosp...35.1656D"><span>ISS <span class="hlt">Observations</span> of the Trapped Proton Anisotropic Effect: A Comparison with <span class="hlt">Model</span> Calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dachev, T.; Atwell, W.; Semones, E.; Tomov, B.; Reddell, B.</p> <p></p> <p>Space radiation <span class="hlt">measurements</span> were made on the International Space Station (ISS) with the Bulgarian Liulin-E094 instrument, which contains 4 Mobile Dosimetry Unit (MDU), and the NASA Tissue Equivalent Proportional Counter (TEPC) during 2001. Four MDUs were placed at fixed locations: one unit (MDU #1) in the ISS "Unity" Node-1 and three (MDU #2-#4) units were located in the US Laboratory module. The MDU #2 and the TEPC were located in the US Laboratory module Human Research Facility (rack #1, port side). Space radiation flight <span class="hlt">measurements</span> were obtained during the time period May 11 - July 26, 2001. In this paper we discuss the flight <span class="hlt">observed</span> asymmetries in different detectors on the ascending and descending parts of the ISS orbits. The differences are described by the development of a shielding <span class="hlt">model</span> using combinatorial geometry and 3-D visualization and the orientation and placement of the five detectors at the locations within the ISS. Shielding distributions were generated for the combined ISS and detector shielding <span class="hlt">models</span>. The AP8MAX and AE8MAX trapped radiation <span class="hlt">models</span> were used to compute the daily absorbed dose for the five detectors and are compared with the flight <span class="hlt">measurements</span>. In addition, the trapped proton anisotropy (East-West effect) was computed for the individual passes through the South Atlantic Anomaly based on the Badhwar-Konradi anisotropy <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=internal+AND+factors+AND+theory&pg=4&id=EJ1069081','ERIC'); return false;" href="https://eric.ed.gov/?q=internal+AND+factors+AND+theory&pg=4&id=EJ1069081"><span><span class="hlt">Measuring</span> Afterschool Program Quality Using Setting-Level <span class="hlt">Observational</span> Approaches</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Oh, Yoonkyung; Osgood, D. Wayne; Smith, Emilie P.</p> <p>2015-01-01</p> <p>The importance of afterschool hours for youth development is widely acknowledged, and afterschool settings have recently received increasing attention as an important venue for youth interventions, bringing a growing need for reliable and valid <span class="hlt">measures</span> of afterschool quality. This study examined the extent to which the two <span class="hlt">observational</span> tools,…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26404626','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26404626"><span>Clinical Complexity in Medicine: A <span class="hlt">Measurement</span> <span class="hlt">Model</span> of Task and Patient Complexity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Islam, R; Weir, C; Del Fiol, G</p> <p>2016-01-01</p> <p>Complexity in medicine needs to be reduced to simple components in a way that is comprehensible to researchers and clinicians. Few studies in the current literature propose a <span class="hlt">measurement</span> <span class="hlt">model</span> that addresses both task and patient complexity in medicine. The objective of this paper is to develop an integrated approach to understand and <span class="hlt">measure</span> clinical complexity by incorporating both task and patient complexity components focusing on the infectious disease domain. The <span class="hlt">measurement</span> <span class="hlt">model</span> was adapted and modified for the healthcare domain. Three clinical infectious disease teams were <span class="hlt">observed</span>, audio-recorded and transcribed. Each team included an infectious diseases expert, one infectious diseases fellow, one physician assistant and one pharmacy resident fellow. The transcripts were parsed and the authors independently coded complexity attributes. This baseline <span class="hlt">measurement</span> <span class="hlt">model</span> of clinical complexity was modified in an initial set of coding processes and further validated in a consensus-based iterative process that included several meetings and email discussions by three clinical experts from diverse backgrounds from the Department of Biomedical Informatics at the University of Utah. Inter-rater reliability was calculated using Cohen's kappa. The proposed clinical complexity <span class="hlt">model</span> consists of two separate components. The first is a clinical task complexity <span class="hlt">model</span> with 13 clinical complexity-contributing factors and 7 dimensions. The second is the patient complexity <span class="hlt">model</span> with 11 complexity-contributing factors and 5 dimensions. The <span class="hlt">measurement</span> <span class="hlt">model</span> for complexity encompassing both task and patient complexity will be a valuable resource for future researchers and industry to <span class="hlt">measure</span> and understand complexity in healthcare.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1214851G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1214851G"><span>Probabilistic calibration of the SPITFIRE fire spread <span class="hlt">model</span> using Earth <span class="hlt">observation</span> data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gomez-Dans, Jose; Wooster, Martin; Lewis, Philip; Spessa, Allan</p> <p>2010-05-01</p> <p>There is a great interest in understanding how fire affects vegetation distribution and dynamics in the context of global vegetation <span class="hlt">modelling</span>. A way to include these effects is through the development of embedded fire spread <span class="hlt">models</span>. However, fire is a complex phenomenon, thus difficult to <span class="hlt">model</span>. Statistical <span class="hlt">models</span> based on fire return intervals, or fire danger indices need large amounts of data for calibration, and are often prisoner to the epoch they were calibrated to. Mechanistic <span class="hlt">models</span>, such as SPITFIRE, try to <span class="hlt">model</span> the complete fire phenomenon based on simple physical rules, making these <span class="hlt">models</span> mostly independent of calibration data. However, the processes expressed in <span class="hlt">models</span> such as SPITFIRE require many parameters. These parametrisations are often reliant on site-specific experiments, or in some other cases, paremeters might not be <span class="hlt">measured</span> directly. Additionally, in many cases, changes in temporal and/or spatial resolution result in parameters becoming effective. To address the difficulties with parametrisation and the often-used fitting methodologies, we propose using a probabilistic framework to calibrate some areas of the SPITFIRE fire spread <span class="hlt">model</span>. We calibrate the <span class="hlt">model</span> against Earth <span class="hlt">Observation</span> (EO) data, a global and ever-expanding source of relevant data. We develop a methodology that tries to incorporate the limitations of the EO data, reasonable prior values for parameters and that results in distributions of parameters, which can be used to infer uncertainty due to parameter estimates. Additionally, the covariance structure of parameters and <span class="hlt">observations</span> is also derived, whcih can help inform data gathering efforts and <span class="hlt">model</span> development, respectively. For this work, we focus on Southern African savannas, an important ecosystem for fire studies, and one with a good amount of EO data relevnt to fire studies. As calibration datasets, we use burned area data, estimated number of fires and vegetation moisture dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DPS....4921402H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DPS....4921402H"><span>Testing Planetary Volcanism <span class="hlt">Models</span> with Multi-Wavelength Near Infrared <span class="hlt">Observations</span> of Kilauea Flows and Fountains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Howell, Robert R.; Radebaugh, Jani; M. C Lopes, Rosaly; Kerber, Laura; Solomonidou, Anezina; Watkins, Bryn</p> <p>2017-10-01</p> <p>Using remote sensing of planetary volcanism on objects such as Io to determine eruption conditions is challenging because the emitting region is typically not resolved and because exposed lava cools so quickly. A <span class="hlt">model</span> of the cooling rate and eruption mechanism is typically used to predict the amount of surface area at different temperatures, then that areal distribution is convolved with a Planck blackbody emission curve, and the predicted spectra is compared with <span class="hlt">observation</span>. Often the broad nature of the Planck curve makes interpretation non-unique. However different eruption mechanisms (for example cooling fire fountain droplets vs. cooling flows) have very different area vs. temperature distributions which can often be characterized by simple power laws. Furthermore different composition magmas have significantly different upper limit cutoff temperatures. In order to test these <span class="hlt">models</span> in August 2016 and May 2017 we obtained spatially resolved <span class="hlt">observations</span> of spreading Kilauea pahoehoe flows and fire fountains using a three-wavelength near-infrared prototype camera system. We have <span class="hlt">measured</span> the area vs. temperature distribution for the flows and find that over a relatively broad temperature range the distribution does follow a power law matching the theoretical predictions. As one approaches the solidus temperature the <span class="hlt">observed</span> area drops below the simple <span class="hlt">model</span> predictions by an amount that seems to vary inversely with the vigor of the spreading rate. At these highest temperatures the simple <span class="hlt">models</span> are probably inadequate. It appears necessary to <span class="hlt">model</span> the visco-elastic stretching of the very thin crust which covers even the most recently formed surfaces. That deviation between <span class="hlt">observations</span> and the simple <span class="hlt">models</span> may be particularly important when using such remote sensing <span class="hlt">observations</span> to determine magma eruption temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSEC44D1293B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSEC44D1293B"><span>Integrating <span class="hlt">observational</span> and <span class="hlt">modelling</span> systems for the management of the Great Barrier Reef</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baird, M. E.; Jones, E. M.; Margvelashvili, N.; Mongin, M.; Rizwi, F.; Robson, B.; Schroeder, T.; Skerratt, J.; Steven, A. D.; Wild-Allen, K.</p> <p>2016-02-01</p> <p><span class="hlt">Observational</span> and <span class="hlt">modelling</span> systems provide two sources of knowledge that must be combined to provide a more complete view than either <span class="hlt">observations</span> or <span class="hlt">models</span> alone can provide. Here we describe the eReefs coupled hydrodynamic, sediment and biogeochemical <span class="hlt">model</span> that has been developed for the Great Barrier Reef; and the multiple <span class="hlt">observations</span> that are used to constrain the <span class="hlt">model</span>. Two contrasting examples of <span class="hlt">model</span> - <span class="hlt">observational</span> integration are highlighted. First we explore the carbon chemistry of the waters above the reef, for which <span class="hlt">observations</span> are accurate, but expensive and therefore sparse, while <span class="hlt">model</span> behaviour is highly skilful. For carbon chemistry, <span class="hlt">observations</span> are used to constrain <span class="hlt">model</span> parameterisation and quantify <span class="hlt">model</span> error, with the <span class="hlt">model</span> output itself providing the most useable knowledge for management purposes. In contrast, ocean colour provides inaccurate, but cheap and spatially and temporally extensive <span class="hlt">observations</span>. Thus <span class="hlt">observations</span> are best combined with the <span class="hlt">model</span> in a data assimilating framework, where a custom-designed optical <span class="hlt">model</span> has been developed for the purposes of incorporating ocean colour <span class="hlt">observations</span>. The future management of Great Barrier Reef water quality will be based on an integration of <span class="hlt">observing</span> and <span class="hlt">modelling</span> systems, providing the most robust information available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3892862','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3892862"><span>An <span class="hlt">Observability</span> Metric for Underwater Vehicle Localization Using Range <span class="hlt">Measurements</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Arrichiello, Filippo; Antonelli, Gianluca; Aguiar, Antonio Pedro; Pascoal, Antonio</p> <p>2013-01-01</p> <p>The paper addresses <span class="hlt">observability</span> issues related to the general problem of single and multiple Autonomous Underwater Vehicle (AUV) localization using only range <span class="hlt">measurements</span>. While an AUV is submerged, localization devices, such as Global Navigation Satellite Systems, are ineffective, due to the attenuation of electromagnetic waves. AUV localization based on dead reckoning techniques and the use of affordable motion sensor units is also not practical, due to divergence caused by sensor bias and drift. For these reasons, localization systems often build on trilateration algorithms that rely on the <span class="hlt">measurements</span> of the ranges between an AUV and a set of fixed transponders using acoustic devices. Still, such solutions are often expensive, require cumbersome calibration procedures and only allow for AUV localization in an area that is defined by the geometrical arrangement of the transponders. A viable alternative for AUV localization that has recently come to the fore exploits the use of complementary information on the distance from the AUV to a single transponder, together with information provided by on-board resident motion sensors, such as, for example, depth, velocity and acceleration <span class="hlt">measurements</span>. This concept can be extended to address the problem of relative localization between two AUVs equipped with acoustic sensors for inter-vehicle range <span class="hlt">measurements</span>. Motivated by these developments, in this paper, we show that both the problems of absolute localization of a single vehicle and the relative localization of multiple vehicles can be treated using the same mathematical framework, and tailoring concepts of <span class="hlt">observability</span> derived for nonlinear systems, we analyze how the performance in localization depends on the types of motion imparted to the AUVs. For this effect, we propose a well-defined <span class="hlt">observability</span> metric and validate its usefulness, both in simulation and by carrying out experimental tests with a real marine vehicle during which the performance of an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=true+AND+experimental&pg=6&id=EJ1026147','ERIC'); return false;" href="https://eric.ed.gov/?q=true+AND+experimental&pg=6&id=EJ1026147"><span>The Effect of <span class="hlt">Observation</span> Length and Presentation Order on the Reliability and Validity of an <span class="hlt">Observational</span> <span class="hlt">Measure</span> of Teaching Quality</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Mashburn, Andrew J.; Meyer, J. Patrick; Allen, Joseph P.; Pianta, Robert C.</p> <p>2014-01-01</p> <p><span class="hlt">Observational</span> methods are increasingly being used in classrooms to evaluate the quality of teaching. Operational procedures for <span class="hlt">observing</span> teachers are somewhat arbitrary in existing <span class="hlt">measures</span> and vary across different instruments. To study the effect of different <span class="hlt">observation</span> procedures on score reliability and validity, we conducted an experimental…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.B43F0359L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.B43F0359L"><span>The synergistic use of <span class="hlt">models</span> and <span class="hlt">observations</span>: understanding the mechanisms behind <span class="hlt">observed</span> biomass dynamics at 14 Amazonian field sites and the implications for future biomass change</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levine, N. M.; Galbraith, D.; Christoffersen, B. J.; Imbuzeiro, H. A.; Restrepo-Coupe, N.; Malhi, Y.; Saleska, S. R.; Costa, M. H.; Phillips, O.; Andrade, A.; Moorcroft, P. R.</p> <p>2011-12-01</p> <p>The Amazonian rainforests play a vital role in global water, energy and carbon cycling. The sensitivity of this system to natural and anthropogenic disturbances therefore has important implications for the global climate. Some global <span class="hlt">models</span> have predicted large-scale forest dieback and the savannization of Amazonia over the next century [Meehl et al., 2007]. While several studies have demonstrated the sensitivity of dynamic global vegetation <span class="hlt">models</span> to changes in temperature, precipitation, and dry season length [e.g. Galbraith et al., 2010; Good et al., 2011], the ability of these <span class="hlt">models</span> to accurately reproduce ecosystem dynamics of present-day transitional or low biomass tropical forests has not been demonstrated. A <span class="hlt">model</span>-data intercomparison was conducted with four state-of-the-art terrestrial ecosystem <span class="hlt">models</span> to evaluate the ability of these <span class="hlt">models</span> to accurately represent structure, function, and long-term biomass dynamics over a range of Amazonian ecosystems. Each <span class="hlt">modeling</span> group conducted a series of simulations for 14 sites including mature forest, transitional forest, savannah, and agricultural/pasture sites. All <span class="hlt">models</span> were run using standard physical parameters and the same initialization procedure. <span class="hlt">Model</span> results were compared against forest inventory and dendrometer data in addition to flux tower <span class="hlt">measurements</span>. While the <span class="hlt">models</span> compared well against field <span class="hlt">observations</span> for the mature forest sites, significant differences were <span class="hlt">observed</span> between predicted and <span class="hlt">measured</span> ecosystem structure and dynamics for the transitional forest and savannah sites. The length of the dry season and soil sand content were good predictors of <span class="hlt">model</span> performance. In addition, for the big leaf <span class="hlt">models</span>, <span class="hlt">model</span> performance was highest for sites dominated by late successional trees and lowest for sites with predominantly early and mid-successional trees. This study provides insight into tropical forest function and sensitivity to environmental conditions that will aid in predictions of the</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P51D..06B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P51D..06B"><span>The Formation of Lunar Impact Basins: <span class="hlt">Observational</span> Constraints from LRO Datasets and Comparisons with <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baker, D. M. H.; Head, J. W., III</p> <p>2016-12-01</p> <p>Impact basins provide windows into the subsurface and through time on a planetary body. However, meaningful geologic interpretations rely on a detailed understanding of their formation and the origin of basin materials. Data from the Lunar Reconnaissance Orbiter (LRO) have been critical to advancing our understanding of the formation of impact basins. We present a number of recent <span class="hlt">observations</span>, including <span class="hlt">measurements</span> of basin morphometry, mineralogy, and gravity anomalies, which provide a framework for constraining current formation <span class="hlt">models</span>. Image data from the LRO Wide Angle Camera (WAC) and altimetry data from the Lunar Orbiter Laser Altimeter (LOLA) were used to refine the recognition of both fresh and degraded impact basins, including their ring structures. Analyses of gravity anomalies from the GRAIL mission show that mantle uplifts confined within the inner basin rings are characteristics that basins acquire from the onset. We used LOLA data to also make new <span class="hlt">measurements</span> of basin morphometry. Small basins possessing two concentric rings ("peak-ring basins") have unique topographic signatures, consisting of inner depressions bounded by a peak ring and a higher annulus that grades to steeper wall material. LRO Narrow Angle Camera (NAC) images and Diviner rock abundance maps were used to identify boulder-rich outcrops in basin rings, which focused mineralogical analyses using Moon Mineralogy Mapper hyperspectral data. Crystalline plagioclase and candidate shock plagioclase outcrops were found to be abundant within basins of all sizes. These <span class="hlt">observations</span> combined with crater scaling laws and lunar crustal thickness constrain the depth of origin of basin peak rings to be near the maximum depth of excavation. Comparisons between iSALE numerical <span class="hlt">models</span> and <span class="hlt">observations</span> show important consistencies and inconsistencies that can help to refine current <span class="hlt">models</span>. In particular, improvements in the match between <span class="hlt">observed</span> and <span class="hlt">modeled</span> morphometry of craters transitional</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120002859','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120002859"><span>An OSSE on Mesoscale <span class="hlt">Model</span> Assimilation of Simulated HIRAD-<span class="hlt">Observed</span> Hurricane Surface Winds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Albers, Cerese; Miller, Timothy; Uhlhorn, Eric; Krishnamurti, T. N.</p> <p>2012-01-01</p> <p>The hazards of landfalling hurricanes are well known, but progress on improving the intensity forecasts of these deadly storms at landfall has been slow. Many cite a lack of high-resolution data sets taken inside the core of a hurricane, and the lack of reliable <span class="hlt">measurements</span> in extreme conditions near the surface of hurricanes, as possible reasons why even the most state-of-the-art forecasting <span class="hlt">models</span> cannot seem to forecast intensity changes better. The Hurricane Imaging Radiometer (HIRAD) is a new airborne microwave remote sensor for <span class="hlt">observing</span> hurricanes, and is operated and researched by NASA Marshall Space Flight Center in partnership with the NOAA Atlantic Oceanographic and Meteorological Laboratory/Hurricane Research Division, the University of Central Florida, the University of Michigan, and the University of Alabama in Huntsville. This instrument?s purpose is to study the wind field of a hurricane, specifically <span class="hlt">observing</span> surface wind speeds and rain rates, in what has traditionally been the most difficult areas for other instruments to study; the high wind and heavy rain regions. Dr. T. N. Krishnamurti has studied various data assimilation techniques for hurricane and monsoon rain rates, and this study builds off of results obtained from utilizing his style of physical initializations of rainfall <span class="hlt">observations</span>, but obtaining reliable <span class="hlt">observations</span> in heavy rain regions has always presented trouble to our research of high-resolution rainfall forecasting. Reliable data from these regions at such a high resolution and wide swath as HIRAD provides is potentially very valuable to mesoscale forecasting of hurricane intensity. This study shows how the data assimilation technique of Ensemble Kalman Filtering (EnKF) in the Weather Research and Forecasting (WRF) <span class="hlt">model</span> can be used to incorporate wind, and later rain rate, data into a mesoscale <span class="hlt">model</span> forecast of hurricane intensity. The study makes use of an <span class="hlt">Observing</span> System Simulation Experiment (OSSE) with a simulated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10136E..0PL','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10136E..0PL"><span>Foveated <span class="hlt">model</span> <span class="hlt">observers</span> to predict human performance in 3D images</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lago, Miguel A.; Abbey, Craig K.; Eckstein, Miguel P.</p> <p>2017-03-01</p> <p>We evaluate 3D search requires <span class="hlt">model</span> <span class="hlt">observers</span> that take into account the peripheral human visual processing (foveated <span class="hlt">models</span>) to predict human <span class="hlt">observer</span> performance. We show that two different 3D tasks, free search and location-known detection, influence the relative human visual detectability of two signals of different sizes in synthetic backgrounds mimicking the noise found in 3D digital breast tomosynthesis. One of the signals resembled a microcalcification (a small and bright sphere), while the other one was designed to look like a mass (a larger Gaussian blob). We evaluated current standard <span class="hlt">models</span> <span class="hlt">observers</span> (Hotelling; Channelized Hotelling; non-prewhitening matched filter with eye filter, NPWE; and non-prewhitening matched filter <span class="hlt">model</span>, NPW) and showed that they incorrectly predict the relative detectability of the two signals in 3D search. We propose a new <span class="hlt">model</span> <span class="hlt">observer</span> (3D Foveated Channelized Hotelling <span class="hlt">Observer</span>) that incorporates the properties of the visual system over a large visual field (fovea and periphery). We show that the foveated <span class="hlt">model</span> <span class="hlt">observer</span> can accurately predict the rank order of detectability of the signals in 3D images for each task. Together, these results motivate the use of a new generation of foveated <span class="hlt">model</span> <span class="hlt">observers</span> for predicting image quality for search tasks in 3D imaging modalities such as digital breast tomosynthesis or computed tomography.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.884a2060N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.884a2060N"><span>Comparison of conventional study <span class="hlt">model</span> <span class="hlt">measurements</span> and 3D digital study <span class="hlt">model</span> <span class="hlt">measurements</span> from laser scanned dental impressions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nugrahani, F.; Jazaldi, F.; Noerhadi, N. A. I.</p> <p>2017-08-01</p> <p>The field of orthodontics is always evolving,and this includes the use of innovative technology. One type of orthodontic technology is the development of three-dimensional (3D) digital study <span class="hlt">models</span> that replace conventional study <span class="hlt">models</span> made by stone. This study aims to compare the mesio-distal teeth width, intercanine width, and intermolar width <span class="hlt">measurements</span> between a 3D digital study <span class="hlt">model</span> and a conventional study <span class="hlt">model</span>. Twelve sets of upper arch dental impressions were taken from subjects with non-crowding teeth. The impressions were taken twice, once with alginate and once with polivinylsiloxane. The alginate impressions used in the conventional study <span class="hlt">model</span> and the polivinylsiloxane impressions were scanned to obtain the 3D digital study <span class="hlt">model</span>. Scanning was performed using a laser triangulation scanner device assembled by the School of Electrical Engineering and Informatics at the Institut Teknologi Bandung and David Laser Scan software. For the conventional <span class="hlt">model</span>, themesio-distal width, intercanine width, and intermolar width were <span class="hlt">measured</span> using digital calipers; in the 3D digital study <span class="hlt">model</span> they were <span class="hlt">measured</span> using software. There were no significant differences between the mesio-distal width, intercanine width, and intermolar width <span class="hlt">measurments</span> between the conventional and 3D digital study <span class="hlt">models</span> (p>0.05). Thus, <span class="hlt">measurements</span> using 3D digital study <span class="hlt">models</span> are as accurate as those obtained from conventional study <span class="hlt">models</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1413641E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1413641E"><span>Impacts of uncertainties in weather and streamflow <span class="hlt">observations</span> in calibration and evaluation of an elevation distributed HBV-<span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Engeland, K.; Steinsland, I.; Petersen-Øverleir, A.; Johansen, S.</p> <p>2012-04-01</p> <p>The aim of this study is to assess the uncertainties in streamflow simulations when uncertainties in both <span class="hlt">observed</span> inputs (precipitation and temperature) and streamflow <span class="hlt">observations</span> used in the calibration of the hydrological <span class="hlt">model</span> are explicitly accounted for. To achieve this goal we applied the elevation distributed HBV <span class="hlt">model</span> operating on daily time steps to a small catchment in high elevation in Southern Norway where the seasonal snow cover is important. The uncertainties in precipitation inputs were quantified using conditional simulation. This procedure accounts for the uncertainty related to the density of the precipitation network, but neglects uncertainties related to <span class="hlt">measurement</span> bias/errors and eventual elevation gradients in precipitation. The uncertainties in temperature inputs were quantified using a Bayesian temperature interpolation procedure where the temperature lapse rate is re-estimated every day. The uncertainty in the lapse rate was accounted for whereas the sampling uncertainty related to network density was neglected. For every day a random sample of precipitation and temperature inputs were drawn to be applied as inputs to the hydrologic <span class="hlt">model</span>. The uncertainties in <span class="hlt">observed</span> streamflow were assessed based on the uncertainties in the rating curve <span class="hlt">model</span>. A Bayesian procedure was applied to estimate the probability for rating curve <span class="hlt">models</span> with 1 to 3 segments and the uncertainties in their parameters. This method neglects uncertainties related to errors in <span class="hlt">observed</span> water levels. Note that one rating curve was drawn to make one realisation of a whole time series of streamflow, thus the rating curve errors lead to a systematic bias in the streamflow <span class="hlt">observations</span>. All these uncertainty sources were linked together in both calibration and evaluation of the hydrologic <span class="hlt">model</span> using a DREAM based MCMC routine. Effects of having less information (e.g. missing one streamflow <span class="hlt">measurement</span> for defining the rating curve or missing one precipitation station</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663544-atmosphere-models-from-inversion-fe-nm-observations-application-solar-irradiance-studies','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663544-atmosphere-models-from-inversion-fe-nm-observations-application-solar-irradiance-studies"><span>1D Atmosphere <span class="hlt">Models</span> from Inversion of Fe i 630 nm <span class="hlt">Observations</span> with an Application to Solar Irradiance Studies</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Cristaldi, Alice; Ermolli, Ilaria, E-mail: alice.cristaldi@oaroma.inaf.it</p> <p></p> <p>Present-day semi-empirical <span class="hlt">models</span> of solar irradiance (SI) variations reconstruct SI changes <span class="hlt">measured</span> on timescales greater than a day by using spectra computed in one dimensional atmosphere <span class="hlt">models</span> (1D <span class="hlt">models</span>), which are representative of various solar surface features. Various recent studies have pointed out, however, that the spectra synthesized in 1D <span class="hlt">models</span> do not reflect the radiative emission of the inhomogenous atmosphere revealed by high-resolution solar <span class="hlt">observations</span>. We aimed to derive <span class="hlt">observation</span>-based atmospheres from such <span class="hlt">observations</span> and test their accuracy for SI estimates. We analyzed spectropolarimetric data of the Fe i 630 nm line pair in photospheric regions that are representativemore » of the granular quiet-Sun pattern (QS) and of small- and large-scale magnetic features, both bright and dark with respect to the QS. The data were taken on 2011 August 6, with the CRisp Imaging Spectropolarimeter at the Swedish Solar Telescope, under excellent seeing conditions. We derived atmosphere <span class="hlt">models</span> of the <span class="hlt">observed</span> regions from data inversion with the SIR code. We studied the sensitivity of results to spatial resolution and temporal evolution, and discuss the obtained atmospheres with respect to several 1D <span class="hlt">models</span>. The atmospheres derived from our study agree well with most of the 1D <span class="hlt">models</span> we compare our results with, both qualitatively and quantitatively (within 10%), except for pore regions. Spectral synthesis computations of the atmosphere obtained from the QS <span class="hlt">observations</span> return an SI between 400 and 2400 nm that agrees, on average, within 2.2% with standard reference <span class="hlt">measurements</span>, and within −0.14% with the SI computed on the QS atmosphere employed by the most advanced semi-empirical <span class="hlt">model</span> of SI variations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110007823','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110007823"><span>Satellite <span class="hlt">Observations</span> and Chemistry Climate <span class="hlt">Models</span> - A Meandering Path Towards Better Predictions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Douglass, Anne R.</p> <p>2011-01-01</p> <p>Knowledge of the chemical and dynamical processes that control the stratospheric ozone layer has grown rapidly since the 1970s, when ideas that depletion of the ozone layer due to human activity were put forth. The concept of ozone depletion due to anthropogenic chlorine increase is simple; quantification of the effect is much more difficult. The future of stratospheric ozone is complicated because ozone is expected to increase for two reasons: the slow decrease in anthropogenic chlorine due to the Montreal Protocol and its amendments and stratospheric cooling caused by increases in carbon dioxide and other greenhouse gases. Prediction of future ozone levels requires three-dimensional <span class="hlt">models</span> that represent physical, photochemical and radiative processes, i.e., chemistry climate <span class="hlt">models</span> (CCMs). While laboratory kinetic and photochemical data are necessary inputs for a CCM, atmospheric <span class="hlt">measurements</span> are needed both to reveal physical and chemical processes and for comparison with simulations to test the conceptual <span class="hlt">model</span> that CCMs represent. Global <span class="hlt">measurements</span> are available from various satellites including but not limited to the LIMS and TOMS instruments on Nimbus 7 (1979 - 1993), and various instruments on the Upper Atmosphere Research Satellite (1991 - 2005), Envisat (2002 - ongoing), Sci-Sat (2003 - ongoing) and Aura (2004 - ongoing). Every successful satellite instrument requires a physical concept for the <span class="hlt">measurement</span>, knowledge of physical chemical properties of the molecules to be <span class="hlt">measured</span>, and stellar engineering to design an instrument that will survive launch and operate for years with no opportunity for repair but providing enough information that trend information can be separated from any instrument change. The on-going challenge is to use <span class="hlt">observations</span> to decrease uncertainty in prediction. This talk will focus on two applications. The first considers transport diagnostics and implications for prediction of the eventual demise of the Antarctic ozone hole</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040171655&hterms=sensitivity+scale&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsensitivity%2Bscale','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040171655&hterms=sensitivity+scale&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsensitivity%2Bscale"><span>Comparison of Local Scale <span class="hlt">Measured</span> and <span class="hlt">Modeled</span> Brightness Temperatures and Snow Parameters from the CLPX 2003 by Means of a Dense Medium Radiative Transfer Theory <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tedescol, Marco; Kim, Edward J.; Cline, Don; Graf, Tobias; Koike, Toshio; Armstrong, Richard; Brodzik, Mary J.; Hardy, Janet</p> <p>2004-01-01</p> <p>Microwave remote sensing offers distinct advantages for <span class="hlt">observing</span> the cryosphere. Solar illumination is not required, and spatial and temporal coverage are excellent from polar-orbiting satellites. Passive microwave <span class="hlt">measurements</span> are sensitive to the two most useful physical quantities for many hydrological applications: physical temperature and water content/state. Sensitivity to the latter is a direct result of the microwave sensitivity to the dielectric properties of natural media, including snow, ice, soil (frozen or thawed), and vegetation. These considerations are factors motivating the development of future cryospheric satellite remote sensing missions, continuing and improving on a 26-year microwave <span class="hlt">measurement</span> legacy. Perhaps the biggest issues regarding the use of such satellite <span class="hlt">measurements</span> involve how to relate parameter values at spatial scales as small as a hectare to <span class="hlt">observations</span> with sensor footprints that may be up to 25 x 25 km. The NASA Cold-land Processes Field Experiment (CLPX) generated a dataset designed to enhance understanding of such scaling issues. CLPX <span class="hlt">observations</span> were made in February (dry snow) and March (wet snow), 2003 in Colorado, USA, at scales ranging from plot scale to 25 x 25 km satellite footprints. Of interest here are passive microwave <span class="hlt">observations</span> from ground-based, airborne, and satellite sensors, as well as meteorological and snowpack <span class="hlt">measurements</span> that will enable studies of the effects of spatial heterogeneity of surface conditions on the <span class="hlt">observations</span>. Prior to performing such scaling studies, an evaluation of snowpack forward <span class="hlt">modelling</span> at the plot scale (least heterogeneous scale) is in order. This is the focus of this paper. Many forward <span class="hlt">models</span> of snow signatures (brightness temperatures) have been developed over the years. It is now recognized that a dense medium radiative transfer (DMRT) treatment represents a high degree of physical fidelity for snow <span class="hlt">modeling</span>, yet dense medium <span class="hlt">models</span> are particularly sensitive to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GMD....11...77S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GMD....11...77S"><span>The Cloud Feedback <span class="hlt">Model</span> Intercomparison Project <span class="hlt">Observational</span> Simulator Package: Version 2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Swales, Dustin J.; Pincus, Robert; Bodas-Salcedo, Alejandro</p> <p>2018-01-01</p> <p>The Cloud Feedback <span class="hlt">Model</span> Intercomparison Project <span class="hlt">Observational</span> Simulator Package (COSP) gathers together a collection of <span class="hlt">observation</span> proxies or <q>satellite simulators</q> that translate <span class="hlt">model</span>-simulated cloud properties to synthetic <span class="hlt">observations</span> as would be obtained by a range of satellite <span class="hlt">observing</span> systems. This paper introduces COSP2, an evolution focusing on more explicit and consistent separation between host <span class="hlt">model</span>, coupling infrastructure, and individual <span class="hlt">observing</span> proxies. Revisions also enhance flexibility by allowing for <span class="hlt">model</span>-specific representation of sub-grid-scale cloudiness, provide greater clarity by clearly separating tasks, support greater use of shared code and data including shared inputs across simulators, and follow more uniform software standards to simplify implementation across a wide range of platforms. The complete package including a testing suite is freely available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16219419','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16219419"><span>Near and far field contamination <span class="hlt">modeling</span> in a large scale enclosure: Fire Dynamics Simulator comparisons with <span class="hlt">measured</span> <span class="hlt">observations</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ryder, Noah L; Schemel, Christopher F; Jankiewicz, Sean P</p> <p>2006-03-17</p> <p>The occurrence of a fire, no matter how small, often exposes objects to significant levels of contamination from the products of combustion. The production and dispersal of these contaminants has been an issue of relevance in the field of fire science for many years, though little work has been done to examine the contamination levels accumulated within an enclosure some time after an incident. This phenomenon is of great importance when considering the consequences associated with even low level contamination of sensitive materials, such as food, pharmaceuticals, clothing, electrical equipment, etc. Not only does such exposure present a localized hazard, but also the shipment of contaminated goods places distant recipients at risk. It is the intent of this paper to use a well-founded computational fluid dynamic (CFD) program, the Fire Dynamics Simulator (FDS), a large eddy simulation (LES) code developed by National Institute of Standards and Technology (NIST), to <span class="hlt">model</span> smoke dispersion in order to assess the subject of air contamination and post fire surface contamination in a warehouse facility. <span class="hlt">Measured</span> results are then compared with the results from the FDS <span class="hlt">model</span>. Two components are examined: the production rate of contaminates and the trajectory of contaminates caused by the forced ventilation conditions. Each plays an important role in determining the extent to which the products of combustion are dispersed and the levels to which products are exposed to the contaminants throughout the enclosure. The <span class="hlt">model</span> results indicate a good first-order approximation to the <span class="hlt">measured</span> surface contamination levels. The proper application of the FDS <span class="hlt">model</span> can provide a cost and time efficient means of evaluating contamination levels within a defined volume.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760009796','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760009796"><span><span class="hlt">Measures</span> and <span class="hlt">models</span> for angular correlation and angular-linear correlation. [correlation of random variables</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Johnson, R. A.; Wehrly, T.</p> <p>1976-01-01</p> <p>Population <span class="hlt">models</span> for dependence between two angular <span class="hlt">measurements</span> and for dependence between an angular and a linear <span class="hlt">observation</span> are proposed. The method of canonical correlations first leads to new population and sample <span class="hlt">measures</span> of dependence in this latter situation. An example relating wind direction to the level of a pollutant is given. Next, applied to pairs of angular <span class="hlt">measurements</span>, the method yields previously proposed sample <span class="hlt">measures</span> in some special cases and a new sample <span class="hlt">measure</span> in general.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Icar..258..402K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Icar..258..402K"><span><span class="hlt">Modeling</span> of the energetic ion <span class="hlt">observations</span> in the vicinity of Rhea and Dione</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kotova, Anna; Roussos, Elias; Krupp, Norbert; Dandouras, Iannis</p> <p>2015-09-01</p> <p>During several flybys of the Cassini spacecraft by the saturnian moons Rhea and Dione the energetic particle detector MIMI/LEMMS <span class="hlt">measured</span> a significant reduction of energetic ion fluxes (20-300 keV) in their vicinity, which is caused by the absorption of those ions at the moon surfaces. In order to simulate the <span class="hlt">observed</span> depletion profiles we developed an energetic particle tracer, which can be used to simulate the charged particle trajectories considering different <span class="hlt">models</span> of the saturnian magnetosphere. This particle tracer is using an adaptive fourth order Gauss Runge-Kutta calculation method and its background magnetospheric <span class="hlt">model</span> can be varied from that of a simple dipole, to a more complex one that includes also non-dipolar perturbations. The electromagnetic environment of each local, moon-magnetosphere interaction region is <span class="hlt">modeled</span> through a hybrid plasma simulation code. Using this energetic particle tracer we explore which of these magnetospheric characteristics are more important in shaping the MIMI/LEMMS ion profiles. We also examine if MIMI/LEMMS responds primarily to protons (as typically assumed in many studies) or also to heavier ions, using calibration information, <span class="hlt">observations</span> of the energy flux spectrum by the MIMI/CHEMS instrument (on board of Cassini as well) and different simulation results. Our results show that MIMI/LEMMS indeed <span class="hlt">measures</span> heavier ions as well. Also we discovered that wrapping of magnetic field lines, even if it caused local perturbations only about few percent of the background magnetic field, can cause <span class="hlt">measurable</span> changes in the spatial and energy distribution of fluxes <span class="hlt">measured</span> by MIMI/LEMMS. These results are important for correct interpretation of MIMI/LEMMS data, and offer capabilities for a precise in-flight instruments' cross-calibration. Besides that, our simulation approach can be employed in similar environments (Titan, Enceladus, jovian moons, etc.) for constraining the magnetic topology of their interaction region and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DPS....4910506B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DPS....4910506B"><span>High resolution 3D global climate <span class="hlt">modeling</span> of Pluto's atmosphere to interpret New Horizons <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bertrand, Tanguy; Forget, Francois; New Horizons Science Team</p> <p>2017-10-01</p> <p>We use the LMD Global Climate <span class="hlt">Model</span> (GCM) of Pluto's atmosphere to interpret New Horizons <span class="hlt">observations</span> and simulate the Pluto climate system. The <span class="hlt">model</span> takes into account the cycles of N2, CH4, CO and organic haze. It is described in details in Forget et al., 2017. In order to ensure our simulations, sensitive to our initial conditions, correctly describe reality, we initialize the 3D <span class="hlt">model</span> with a set of subsurface temperatures and ice distribution, which converged toward steady state after thousands of years simulated with a 2D version of the <span class="hlt">model</span> (Bertrand and Forget, 2016).We identify three “realistic” simulations which differ by their spatial distribution of N2 ice in 2015 but remain consistent with the evolution of the surface pressure (Sicardy et al., 2016) and the amount of atmospheric methane <span class="hlt">observed</span> on Pluto (Lellouch et al., 2015). We perform a comprehensive characterization of Pluto’s atmosphere in 2015 using these simulations. Near surface winds can be compared to wind streaks on Pluto, while the simulated waves and thermal structure can be compared to the New Horizons occultations <span class="hlt">measurements</span> (Hinson et al., 2017).In particular, we demonstrate the sensitivity of the general circulation to the distribution of N2 ice on the surface. Our latest results suggest that Pluto’s atmosphere undergoes retrograde rotation, a unique circulation regime in the Solar System, induced by the condensation-sublimation of N2 in the Sputnik Planitia basin. In Sputnik Planitia, the near-surface winds favor a deposition of haze particles in the northern and western part of the ice cap, which helps to interpret the different colors <span class="hlt">observed</span>. The GCM also shows that several atmospheric phenomena are at the origin of the cold boundary layer <span class="hlt">observed</span> deep in the Sputnik Planitia basin, in particular the sublimation of N2, effects of topography and the supply of cold air by winds. This allows us to understand the near-surface differences <span class="hlt">observed</span> between the entry and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.475.4170A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.475.4170A"><span>COCOA code for creating mock <span class="hlt">observations</span> of star cluster <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Askar, Abbas; Giersz, Mirek; Pych, Wojciech; Dalessandro, Emanuele</p> <p>2018-04-01</p> <p>We introduce and present results from the COCOA (Cluster simulatiOn Comparison with <span class="hlt">ObservAtions</span>) code that has been developed to create idealized mock photometric <span class="hlt">observations</span> using results from numerical simulations of star cluster evolution. COCOA is able to present the output of realistic numerical simulations of star clusters carried out using Monte Carlo or N-body codes in a way that is useful for direct comparison with photometric <span class="hlt">observations</span>. In this paper, we describe the COCOA code and demonstrate its different applications by utilizing globular cluster (GC) <span class="hlt">models</span> simulated with the MOCCA (MOnte Carlo Cluster simulAtor) code. COCOA is used to synthetically <span class="hlt">observe</span> these different GC <span class="hlt">models</span> with optical telescopes, perform point spread function photometry, and subsequently produce <span class="hlt">observed</span> colour-magnitude diagrams. We also use COCOA to compare the results from synthetic <span class="hlt">observations</span> of a cluster <span class="hlt">model</span> that has the same age and metallicity as the Galactic GC NGC 2808 with <span class="hlt">observations</span> of the same cluster carried out with a 2.2 m optical telescope. We find that COCOA can effectively simulate realistic <span class="hlt">observations</span> and recover photometric data. COCOA has numerous scientific applications that maybe be helpful for both theoreticians and <span class="hlt">observers</span> that work on star clusters. Plans for further improving and developing the code are also discussed in this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AdRS...11..347V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AdRS...11..347V"><span>Application of postured human <span class="hlt">model</span> for SAR <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vuchkovikj, M.; Munteanu, I.; Weiland, T.</p> <p>2013-07-01</p> <p>In the last two decades, the increasing number of electronic devices used in day-to-day life led to a growing interest in the study of the electromagnetic field interaction with biological tissues. The design of medical devices and wireless communication devices such as mobile phones benefits a lot from the bio-electromagnetic simulations in which digital human <span class="hlt">models</span> are used. The digital human <span class="hlt">models</span> currently available have an upright position which limits the research activities in realistic scenarios, where postured human bodies must be considered. For this reason, a software application called "BodyFlex for CST STUDIO SUITE" was developed. In its current version, this application can deform the voxel-based human <span class="hlt">model</span> named HUGO (Dipp GmbH, 2010) to allow the generation of common postures that people use in normal life, ensuring the continuity of tissues and conserving the mass to an acceptable level. This paper describes the enhancement of the "BodyFlex" application, which is related to the movements of the forearm and the wrist of a digital human <span class="hlt">model</span>. One of the electromagnetic applications in which the forearm and the wrist movement of a voxel based human <span class="hlt">model</span> has a significant meaning is the <span class="hlt">measurement</span> of the specific absorption rate (SAR) when a <span class="hlt">model</span> is exposed to a radio frequency electromagnetic field produced by a mobile phone. Current SAR <span class="hlt">measurements</span> of the exposure from mobile phones are performed with the SAM (Specific Anthropomorphic Mannequin) phantom which is filled with a dispersive but homogeneous material. We are interested what happens with the SAR values if a realistic inhomogeneous human <span class="hlt">model</span> is used. To this aim, two human <span class="hlt">models</span>, a homogeneous and an inhomogeneous one, in two simulation scenarios are used, in order to examine and <span class="hlt">observe</span> the differences in the results for the SAR values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28175325','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28175325"><span>Adolescents' <span class="hlt">Observations</span> of Parent Pain Behaviors: Preliminary <span class="hlt">Measure</span> Validation and Test of Social Learning Theory in Pediatric Chronic Pain.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stone, Amanda L; Walker, Lynn S</p> <p>2017-01-01</p> <p>Evaluate psychometric properties of a <span class="hlt">measure</span> of adolescents’ <span class="hlt">observations</span> of parental pain behaviors and use this <span class="hlt">measure</span> to test hypotheses regarding pain-specific social learning. We created a proxy-report of the Patient Reported Outcomes <span class="hlt">Measurement</span> Information System (PROMIS) Pain Behavior–Short Form (PPB) for adolescents to report on parental pain behaviors, which we labeled the PPB-Proxy. Adolescents (n = 138, mean age = 14.20) with functional abdominal pain completed the PPB-Proxy and a parent completed the PPB. Adolescents and their parents completed <span class="hlt">measures</span> of pain and disability during the adolescent’s clinic visit for abdominal pain. Adolescents subsequently completed a 7-day pain diary period. The PPB-Proxy moderately correlated with the PPB, evidencing that adolescents <span class="hlt">observe</span> and can report on parental pain behaviors. Both the PPB-Proxy and PPB significantly correlated with adolescents’ pain-related disability. Parental <span class="hlt">modeling</span> of pain behaviors could represent an important target for assessment and treatment in pediatric chronic pain patients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.5260S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.5260S"><span>Comparing soil moisture memory in satellite <span class="hlt">observations</span> and <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stacke, Tobias; Hagemann, Stefan; Loew, Alexander</p> <p>2013-04-01</p> <p>A major obstacle to a correct parametrization of soil processes in large scale global land surface <span class="hlt">models</span> is the lack of long term soil moisture <span class="hlt">observations</span> for large parts of the globe. Currently, a compilation of soil moisture data derived from a range of satellites is released by the ESA Climate Change Initiative (ECV_SM). Comprising the period from 1978 until 2010, it provides the opportunity to compute climatological relevant statistics on a quasi-global scale and to compare these to the output of climate <span class="hlt">models</span>. Our study is focused on the investigation of soil moisture memory in satellite <span class="hlt">observations</span> and <span class="hlt">models</span>. As a proxy for memory we compute the autocorrelation length (ACL) of the available satellite data and the uppermost soil layer of the <span class="hlt">models</span>. Additional to the ECV_SM data, AMSR-E soil moisture is used as <span class="hlt">observational</span> estimate. Simulated soil moisture fields are taken from ERA-Interim reanalysis and generated with the land surface <span class="hlt">model</span> JSBACH, which was driven with quasi-<span class="hlt">observational</span> meteorological forcing data. The satellite data show ACLs between one week and one month for the greater part of the land surface while the <span class="hlt">models</span> simulate a longer memory of up to two months. Some pattern are similar in <span class="hlt">models</span> and <span class="hlt">observations</span>, e.g. a longer memory in the Sahel Zone and the Arabian Peninsula, but the <span class="hlt">models</span> are not able to reproduce regions with a very short ACL of just a few days. If the long term seasonality is subtracted from the data the memory is strongly shortened, indicating the importance of seasonal variations for the memory in most regions. Furthermore, we analyze the change of soil moisture memory in the different soil layers of the <span class="hlt">models</span> to investigate to which extent the surface soil moisture includes information about the whole soil column. A first analysis reveals that the ACL is increasing for deeper layers. However, its increase is stronger in the soil moisture anomaly than in its absolute values and the first even exceeds the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017A%26A...604A.124M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017A%26A...604A.124M"><span>Understanding EROS2 <span class="hlt">observations</span> toward the spiral arms within a classical Galactic <span class="hlt">model</span> framework</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moniez, M.; Sajadian, S.; Karami, M.; Rahvar, S.; Ansari, R.</p> <p>2017-08-01</p> <p>Aims: EROS (Expérience de Recherche d'Objets Sombres) has searched for microlensing toward four directions in the Galactic plane away from the Galactic center. The interpretation of the catalog optical depth is complicated by the spread of the source distance distribution. We compare the EROS microlensing <span class="hlt">observations</span> with Galactic <span class="hlt">models</span> (including the Besançon <span class="hlt">model</span>), tuned to fit the EROS source catalogs, and take into account all <span class="hlt">observational</span> data such as the microlensing optical depth, the Einstein crossing durations, and the color and magnitude distributions of the catalogued stars. Methods: We simulated EROS-like source catalogs using the HIgh-Precision PARallax COllecting Satellite (Hipparcos) database, the Galactic mass distribution, and an interstellar extinction table. Taking into account the EROS star detection efficiency, we were able to produce simulated color-magnitude diagrams that fit the <span class="hlt">observed</span> diagrams. This allows us to estimate average microlensing optical depths and event durations that are directly comparable with the <span class="hlt">measured</span> values. Results: Both the Besançon <span class="hlt">model</span> and our Galactic <span class="hlt">model</span> allow us to fully understand the EROS color-magnitude data. The average optical depths and mean event durations calculated from these <span class="hlt">models</span> are in reasonable agreement with the <span class="hlt">observations</span>. Varying the Galactic structure parameters through simulation, we were also able to deduce contraints on the kinematics of the disk, the disk stellar mass function (at a few kpc distance from the Sun), and the maximum contribution of a thick disk of compact objects in the Galactic plane (Mthick< 5 - 7 × 1010M⊙ at 95%, depending on the <span class="hlt">model</span>). We also show that the microlensing data toward one of our monitored directions are significantly sensitive to the Galactic bar parameters, although much larger statistics are needed to provide competitive constraints. Conclusions: Our simulation gives a better understanding of the lens and source spatial distributions in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.8633D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.8633D"><span>Comparison of land-surface humidity between <span class="hlt">observations</span> and CMIP5 <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dunn, Robert; Willett, Kate; Ciavarella, Andrew; Stott, Peter; Jones, Gareth</p> <p>2017-04-01</p> <p>We compare the latest <span class="hlt">observational</span> land-surface humidity dataset, HadISDH, with the CMIP5 <span class="hlt">model</span> archive spatially and temporally over the period 1973-2015. None of the CMIP5 <span class="hlt">models</span> or experiments capture the <span class="hlt">observed</span> temporal behaviour of the globally averaged relative or specific humidity over the entire study period. When using an atmosphere-only <span class="hlt">model</span>, driven by <span class="hlt">observed</span> sea-surface temperatures and radiative forcing changes, the behaviour of regional average temperature and specific humidity are better captured, but there is little improvement in the relative humidity. Comparing the <span class="hlt">observed</span> and historical <span class="hlt">model</span> climatologies show that the <span class="hlt">models</span> are generally cooler everywhere, are drier and less saturated in the tropics and extra tropics, and have comparable moisture levels but are more saturated in the high latitudes. The spatial pattern of linear trends are relatively similar between the <span class="hlt">models</span> and HadISDH for temperature and specific humidity, but there are large differences for relative humidity, with less moistening shown in the <span class="hlt">models</span> over the Tropics, and very little at high atitudes. The <span class="hlt">observed</span> temporal behaviour appears to be a robust climate feature rather than <span class="hlt">observational</span> error. It has been previously documented and is theoretically consistent with faster warming rates over land compared to oceans. Thus, the poor replication in the <span class="hlt">models</span>, especially in the atmosphere only <span class="hlt">model</span>, leads to questions over future projections of impacts related to changes in surface relative humidity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5381A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5381A"><span>AirSWOT <span class="hlt">observations</span> versus hydrodynamic <span class="hlt">model</span> outputs of water surface elevation and slope in a multichannel river</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Altenau, Elizabeth H.; Pavelsky, Tamlin M.; Moller, Delwyn; Lion, Christine; Pitcher, Lincoln H.; Allen, George H.; Bates, Paul D.; Calmant, Stéphane; Durand, Michael; Neal, Jeffrey C.; Smith, Laurence C.</p> <p>2017-04-01</p> <p>Anabranching rivers make up a large proportion of the world's major rivers, but quantifying their flow dynamics is challenging due to their complex morphologies. Traditional in situ <span class="hlt">measurements</span> of water levels collected at gauge stations cannot capture out of bank flows and are limited to defined cross sections, which presents an incomplete picture of water fluctuations in multichannel systems. Similarly, current remotely sensed <span class="hlt">measurements</span> of water surface elevations (WSEs) and slopes are constrained by resolutions and accuracies that limit the visibility of surface waters at global scales. Here, we present new <span class="hlt">measurements</span> of river WSE and slope along the Tanana River, AK, acquired from AirSWOT, an airborne analogue to the Surface Water and Ocean Topography (SWOT) mission. Additionally, we compare the AirSWOT <span class="hlt">observations</span> to hydrodynamic <span class="hlt">model</span> outputs of WSE and slope simulated across the same study area. Results indicate AirSWOT errors are significantly lower than <span class="hlt">model</span> outputs. When compared to field <span class="hlt">measurements</span>, RMSE for AirSWOT <span class="hlt">measurements</span> of WSEs is 9.0 cm when averaged over 1 km squared areas and 1.0 cm/km for slopes along 10 km reaches. Also, AirSWOT can accurately reproduce the spatial variations in slope critical for characterizing reach-scale hydraulics, while <span class="hlt">model</span> outputs of spatial variations in slope are very poor. Combining AirSWOT and future SWOT <span class="hlt">measurements</span> with hydrodynamic <span class="hlt">models</span> can result in major improvements in <span class="hlt">model</span> simulations at local to global scales. Scientists can use AirSWOT <span class="hlt">measurements</span> to constrain <span class="hlt">model</span> parameters over long reach distances, improve understanding of the physical processes controlling the spatial distribution of <span class="hlt">model</span> parameters, and validate <span class="hlt">models</span>' abilities to reproduce spatial variations in slope. Additionally, AirSWOT and SWOT <span class="hlt">measurements</span> can be assimilated into lower-complexity <span class="hlt">models</span> to try and approach the accuracies achieved by higher-complexity <span class="hlt">models</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1345147-detection-solar-like-oscillations-observational-constraints-stellar-models-cyg-brightest-star-observed-kepler-mission','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1345147-detection-solar-like-oscillations-observational-constraints-stellar-models-cyg-brightest-star-observed-kepler-mission"><span>Detection of Solar-Like Oscillations, <span class="hlt">Observational</span> Constraints, and Stellar <span class="hlt">Models</span> for θ Cyg, the Brightest Star <span class="hlt">Observed</span> by the Kepler Mission</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Guzik, Joyce Ann; Houdek, G.; Chaplin, W. J.; ...</p> <p>2016-10-21</p> <p>θ Cygni is an F3 spectral type magnitude V = 4.48 main-sequence star that was the brightest star <span class="hlt">observed</span> by the original Kepler spacecraft mission. Short-cadence (58.8 s) photometric data using a custom aperture were first obtained during Quarter 6 (2010 June–September) and subsequently in Quarters 8 and 12–17. We present analyses of solar-like oscillations based on Q6 and Q8 data, identifying angular degree l = 0, 1, and 2 modes with frequencies of 1000–2700 μHz, a large frequency separation of 83.9 ± 0.4 μHz, and maximum oscillation amplitude at frequency ν max = 1829 ± 54 μHz. We alsomore » present analyses of new ground-based spectroscopic <span class="hlt">observations</span>, which, combined with interferometric angular diameter <span class="hlt">measurements</span>, give T eff = 6697 ± 78 K, radius 1.49 ± 0.03 R ⊙, [Fe/H] = $-$0.02 ± 0.06 dex, and log g = 4.23 ± 0.03. We calculate stellar <span class="hlt">models</span> matching these constraints using the Yale Rotating Evolution Code and the Asteroseismic <span class="hlt">Modeling</span> Portal. The best-fit <span class="hlt">models</span> have masses of 1.35–1.39 M ⊙ and ages of 1.0–1.6 Gyr. θ Cyg's T eff and log g place it cooler than the red edge of the γ Doradus instability region established from pre-Kepler ground-based <span class="hlt">observations</span>, but just at the red edge derived from pulsation <span class="hlt">modeling</span>. Lastly, the pulsation <span class="hlt">models</span> show γ Dor gravity modes driven by the convective blocking mechanism, with frequencies of 1–3 cycles per day (11 to 33 μHz). However, gravity modes were not seen in Kepler data; one signal at 1.776 cycles per day (20.56 μHz) may be attributable to a faint, possibly background, binary.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A21C0037Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A21C0037Q"><span>Evaluation of multi-<span class="hlt">model</span> aerosol distributions over East Asia using in-situ and satellite <span class="hlt">observations</span> during summer 2008</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Quennehen, B.; Raut, J.; Law, K.; Ancellet, G.; Bazureau, A.; Thomas, J.; Daskalakis, N.; Kim, S.; Zhu, T.</p> <p>2013-12-01</p> <p>As part of the EU ECLIPSE (Evaluating the CLimate and air quality ImPacts of Short-livEd pollutants) project, which aims to quantify the climate impact of short lived climate forcers (SLCFs), including aerosols, black carbon and ozone, the WRF-Chem regional and six global (ECHAM6, EMEP, HadGEM, OsloCTM, NORESM, TM4) <span class="hlt">models</span> are evaluated using <span class="hlt">observations</span> in East-Asia. Simulations are compared at horizontal and vertical scales to satellite <span class="hlt">observations</span>, as well as data from field campaigns which took place in summer 2008, and from long-term <span class="hlt">measurement</span> stations. <span class="hlt">Models</span> were run with the same emissions, namely, the ECLIPSE anthropogenic (based on the GAINS <span class="hlt">model</span>), GFED 3.1 fire and RCP 6.0 ship and aircraft emissions for 2008. The initial and boundary conditions for the WRF-Chem regional <span class="hlt">model</span> were specified from the TM4 global chemical transport <span class="hlt">model</span>. Firstly, this study evaluates the ability of the <span class="hlt">models</span> to simulate aerosol physical, optical and chemical properties at a large scale, both horizontally and vertically, using monthly mean satellite <span class="hlt">observations</span> such as CALIPSO, MODIS and IASI. Secondly, <span class="hlt">model</span> daily and hourly results are evaluated at more regional/local scales using ground-based data and <span class="hlt">measurements</span> from summer 2008 intensive campaigns, including aircraft data (CAPMEX and CAREBEIJING). In this study, we assess aerosol total concentrations and size distributions simulated by the <span class="hlt">model</span>. The radiative impact of anthropogenic aerosol layers has already been investigated but less is known about the influence of vertical layering in the atmosphere. Pollution layers have different radiative impacts whether they are below or above clouds and in that sense, a better understanding of their spatial and vertical extent is critical. Information about pollution layers and cloud optical properties and locations over East-Asia are determined using <span class="hlt">observations</span> from IASI for trace gases and CALIPSO for aerosols. The radiative impact of the aerosol layers is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT.........6V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT.........6V"><span><span class="hlt">Observing</span> and <span class="hlt">modeling</span> dynamics in terrestrial gross primary productivity and phenology from remote sensing: An assessment using in-situ <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Verma, Manish K.</p> <p></p> <p>-situ and remote sensing time series. However, the Richards function captured <span class="hlt">observed</span> asymmetric dynamics that were not captured by the other functions. The timing of key phenophase transitions derived using the Richards function therefore agreed best with <span class="hlt">observations</span>. This suggests that ecosystem <span class="hlt">models</span> and remote-sensing algorithms would benefit from using the Richards function to represent phenological dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015A%26C....12...73P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015A%26C....12...73P"><span>Montblanc1: GPU accelerated radio interferometer <span class="hlt">measurement</span> equations in support of Bayesian inference for radio <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Perkins, S. J.; Marais, P. C.; Zwart, J. T. L.; Natarajan, I.; Tasse, C.; Smirnov, O.</p> <p>2015-09-01</p> <p>We present Montblanc, a GPU implementation of the Radio interferometer <span class="hlt">measurement</span> equation (RIME) in support of the Bayesian inference for radio <span class="hlt">observations</span> (BIRO) technique. BIRO uses Bayesian inference to select sky <span class="hlt">models</span> that best match the visibilities <span class="hlt">observed</span> by a radio interferometer. To accomplish this, BIRO evaluates the RIME multiple times, varying sky <span class="hlt">model</span> parameters to produce multiple <span class="hlt">model</span> visibilities. χ2 values computed from the <span class="hlt">model</span> and <span class="hlt">observed</span> visibilities are used as likelihood values to drive the Bayesian sampling process and select the best sky <span class="hlt">model</span>. As most of the elements of the RIME and χ2 calculation are independent of one another, they are highly amenable to parallel computation. Additionally, Montblanc caters for iterative RIME evaluation to produce multiple χ2 values. Modified <span class="hlt">model</span> parameters are transferred to the GPU between each iteration. We implemented Montblanc as a Python package based upon NVIDIA's CUDA architecture. As such, it is easy to extend and implement different pipelines. At present, Montblanc supports point and Gaussian morphologies, but is designed for easy addition of new source profiles. Montblanc's RIME implementation is performant: On an NVIDIA K40, it is approximately 250 times faster than MEQTREES on a dual hexacore Intel E5-2620v2 CPU. Compared to the OSKAR simulator's GPU-implemented RIME components it is 7.7 and 12 times faster on the same K40 for single and double-precision floating point respectively. However, OSKAR's RIME implementation is more general than Montblanc's BIRO-tailored RIME. Theoretical analysis of Montblanc's dominant CUDA kernel suggests that it is memory bound. In practice, profiling shows that is balanced between compute and memory, as much of the data required by the problem is retained in L1 and L2 caches.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1347994-mhd-modeling-diii-low-torque-qh-mode-discharge-comparison-observations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1347994-mhd-modeling-diii-low-torque-qh-mode-discharge-comparison-observations"><span>MHD <span class="hlt">modeling</span> of a DIII-D low-torque QH-mode discharge and comparison to <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>King, Jacob R.; Kruger, S. E.; Burrell, K. H.; ...</p> <p>2017-03-07</p> <p>Extended-MHD <span class="hlt">modeling</span> of DIII-D tokamak quiescent H-mode (QH-mode) discharges with nonlinear NIMROD simulations saturates into a turbulent state but does not saturate when the steady-state flow inferred from <span class="hlt">measurements</span> is not included. This is consistent with the experimental <span class="hlt">observations</span> of the quiescent regime on DIII-D. The simulation with flow develops into a saturated turbulent state where the n Φ = 1 and 2 toroidal modes become dominant through an inverse cascade. Each mode in the range of n Φ = 1–5 is dominant at a different time. Consistent with experimental <span class="hlt">observations</span> during QH-mode, the simulated state leads to large particlemore » transport relative to the thermal transport. Analysis shows that the amplitude and phase of the density and temperature perturbations differ resulting in greater fluctuation-induced convective particle transport relative to the convective thermal transport. As a result, comparison to magnetic-coil <span class="hlt">measurements</span> shows that rotation frequencies differ between the simulation and experiment, which indicates that more sophisticated extended-MHD two-fluid <span class="hlt">modeling</span> is required.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1347994','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1347994"><span>MHD <span class="hlt">modeling</span> of a DIII-D low-torque QH-mode discharge and comparison to <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>King, Jacob R.; Kruger, S. E.; Burrell, K. H.</p> <p></p> <p>Extended-MHD <span class="hlt">modeling</span> of DIII-D tokamak quiescent H-mode (QH-mode) discharges with nonlinear NIMROD simulations saturates into a turbulent state but does not saturate when the steady-state flow inferred from <span class="hlt">measurements</span> is not included. This is consistent with the experimental <span class="hlt">observations</span> of the quiescent regime on DIII-D. The simulation with flow develops into a saturated turbulent state where the n Φ = 1 and 2 toroidal modes become dominant through an inverse cascade. Each mode in the range of n Φ = 1–5 is dominant at a different time. Consistent with experimental <span class="hlt">observations</span> during QH-mode, the simulated state leads to large particlemore » transport relative to the thermal transport. Analysis shows that the amplitude and phase of the density and temperature perturbations differ resulting in greater fluctuation-induced convective particle transport relative to the convective thermal transport. As a result, comparison to magnetic-coil <span class="hlt">measurements</span> shows that rotation frequencies differ between the simulation and experiment, which indicates that more sophisticated extended-MHD two-fluid <span class="hlt">modeling</span> is required.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PMB....61.2109G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PMB....61.2109G"><span>Collimator optimization and collimator-detector response compensation in myocardial perfusion SPECT using the ideal <span class="hlt">observer</span> with and without <span class="hlt">model</span> mismatch and an anthropomorphic <span class="hlt">model</span> <span class="hlt">observer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghaly, Michael; Links, Jonathan M.; Frey, Eric C.</p> <p>2016-03-01</p> <p>The collimator is the primary factor that determines the spatial resolution and noise tradeoff in myocardial perfusion SPECT images. In this paper, the goal was to find the collimator that optimizes the image quality in terms of a perfusion defect detection task. Since the optimal collimator could depend on the level of approximation of the collimator-detector response (CDR) compensation <span class="hlt">modeled</span> in reconstruction, we performed this optimization for the cases of <span class="hlt">modeling</span> the full CDR (including geometric, septal penetration and septal scatter responses), the geometric CDR, or no <span class="hlt">model</span> of the CDR. We evaluated the performance on the detection task using three <span class="hlt">model</span> <span class="hlt">observers</span>. Two <span class="hlt">observers</span> operated on data in the projection domain: the Ideal <span class="hlt">Observer</span> (IO) and IO with <span class="hlt">Model</span>-Mismatch (IO-MM). The third <span class="hlt">observer</span> was an anthropomorphic Channelized Hotelling <span class="hlt">Observer</span> (CHO), which operated on reconstructed images. The projection-domain <span class="hlt">observers</span> have the advantage that they are computationally less intensive. The IO has perfect knowledge of the image formation process, i.e. it has a perfect <span class="hlt">model</span> of the CDR. The IO-MM takes into account the mismatch between the true (complete and accurate) <span class="hlt">model</span> and an approximate <span class="hlt">model</span>, e.g. one that might be used in reconstruction. We evaluated the utility of these projection domain <span class="hlt">observers</span> in optimizing instrumentation parameters. We investigated a family of 8 parallel-hole collimators, spanning a wide range of resolution and sensitivity tradeoffs, using a population of simulated projection (for the IO and IO-MM) and reconstructed (for the CHO) images that included background variability. We simulated anterolateral and inferior perfusion defects with variable extents and severities. The area under the ROC curve was estimated from the IO, IO-MM, and CHO test statistics and served as the figure-of-merit. The optimal collimator for the IO had a resolution of 9-11 mm FWHM at 10 cm, which is poorer resolution than typical collimators</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1418345-using-arm-observations-evaluate-climate-model-simulations-land-atmosphere-coupling-southern-great-plains','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1418345-using-arm-observations-evaluate-climate-model-simulations-land-atmosphere-coupling-southern-great-plains"><span>Using ARM <span class="hlt">Observations</span> to Evaluate Climate <span class="hlt">Model</span> Simulations of Land-Atmosphere Coupling on the U.S. Southern Great Plains</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Phillips, Thomas J.; Klein, Stephen A.; Ma, Hsi -Yen</p> <p></p> <p>Several independent <span class="hlt">measurements</span> of warm-season soil moisture and surface atmospheric variables recorded at the ARM Southern Great Plains (SGP) research facility are used to estimate the terrestrial component of land-atmosphere coupling (LAC) strength and its regional uncertainty. The <span class="hlt">observations</span> reveal substantial variation in coupling strength, as estimated from three soil moisture <span class="hlt">measurements</span> at a single site, as well as across six other sites having varied soil and land cover types. The <span class="hlt">observational</span> estimates then serve as references for evaluating SGP terrestrial coupling strength in the Community Atmospheric <span class="hlt">Model</span> coupled to the Community Land <span class="hlt">Model</span>. These coupled <span class="hlt">model</span> components are operatedmore » in both a free-running mode and in a controlled configuration, where the atmospheric and land states are reinitialized daily, so that they do not drift very far from <span class="hlt">observations</span>. Although the controlled simulation deviates less from the <span class="hlt">observed</span> surface climate than its free-running counterpart, the terrestrial LAC in both configurations is much stronger and displays less spatial variability than the SGP <span class="hlt">observational</span> estimates. Preliminary investigation of vegetation leaf area index (LAI) substituted for soil moisture suggests that the overly strong coupling between <span class="hlt">model</span> soil moisture and surface atmospheric variables is associated with too much evaporation from bare ground and too little from the vegetation cover. Lastly, these results imply that <span class="hlt">model</span> surface characteristics such as LAI, as well as the physical parameterizations involved in the coupling of the land and atmospheric components, are likely to be important sources of the problematical LAC behaviors.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1418345-using-arm-observations-evaluate-climate-model-simulations-land-atmosphere-coupling-southern-great-plains','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1418345-using-arm-observations-evaluate-climate-model-simulations-land-atmosphere-coupling-southern-great-plains"><span>Using ARM <span class="hlt">Observations</span> to Evaluate Climate <span class="hlt">Model</span> Simulations of Land-Atmosphere Coupling on the U.S. Southern Great Plains</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Phillips, Thomas J.; Klein, Stephen A.; Ma, Hsi -Yen; ...</p> <p>2017-10-13</p> <p>Several independent <span class="hlt">measurements</span> of warm-season soil moisture and surface atmospheric variables recorded at the ARM Southern Great Plains (SGP) research facility are used to estimate the terrestrial component of land-atmosphere coupling (LAC) strength and its regional uncertainty. The <span class="hlt">observations</span> reveal substantial variation in coupling strength, as estimated from three soil moisture <span class="hlt">measurements</span> at a single site, as well as across six other sites having varied soil and land cover types. The <span class="hlt">observational</span> estimates then serve as references for evaluating SGP terrestrial coupling strength in the Community Atmospheric <span class="hlt">Model</span> coupled to the Community Land <span class="hlt">Model</span>. These coupled <span class="hlt">model</span> components are operatedmore » in both a free-running mode and in a controlled configuration, where the atmospheric and land states are reinitialized daily, so that they do not drift very far from <span class="hlt">observations</span>. Although the controlled simulation deviates less from the <span class="hlt">observed</span> surface climate than its free-running counterpart, the terrestrial LAC in both configurations is much stronger and displays less spatial variability than the SGP <span class="hlt">observational</span> estimates. Preliminary investigation of vegetation leaf area index (LAI) substituted for soil moisture suggests that the overly strong coupling between <span class="hlt">model</span> soil moisture and surface atmospheric variables is associated with too much evaporation from bare ground and too little from the vegetation cover. Lastly, these results imply that <span class="hlt">model</span> surface characteristics such as LAI, as well as the physical parameterizations involved in the coupling of the land and atmospheric components, are likely to be important sources of the problematical LAC behaviors.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007epsc.conf..568T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007epsc.conf..568T"><span>Characterising Hot-Jupiters' atmospheres with <span class="hlt">observations</span> and <span class="hlt">modelling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tinetti, G.</p> <p>2007-08-01</p> <p>Exoplanet transit photometry and spectroscopy are currently the best techniques to probe the atmospheres of extrasolar worlds. The best targets to be <span class="hlt">observed</span> with these methods, are the planets that orbit very close to their parent star, both because their probability to transit grows and their atmospheres are warmer and more expanded, hence easier to probe. These characteristics are met by the so called Hot-Jupiters, massive low-density gaseous planets orbiting very close-in. Phase-curves allow to <span class="hlt">observe</span> the change in brightness in the combined light of the planet-star system, also for non-transiting exoplanets. We review here the most crucial <span class="hlt">observations</span> performed with the Hubble and Spitzer Space Telescopes at multiple wavelenghts, and the most successful <span class="hlt">models</span> proposed in the literature to plan and interpret those <span class="hlt">observations</span>. In particular we will focus on most recent <span class="hlt">observations</span> and <span class="hlt">modelling</span> claiming the detection of water vapour in the atmospheres of these planets. Further into the future, the JamesWebb Space Telescope will allow to probe the atmospheres of smaller size-planets with the same techniques. We briefly report here the results expected for hot and warm Neptunes, or transiting terrestrial planets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvL.114h1303M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvL.114h1303M"><span><span class="hlt">Observing</span> Inflationary Reheating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martin, Jérôme; Ringeval, Christophe; Vennin, Vincent</p> <p>2015-02-01</p> <p>Reheating is the epoch which connects inflation to the subsequent hot big-bang phase. Conceptually very important, this era is, however, <span class="hlt">observationally</span> poorly known. We show that the current Planck satellite <span class="hlt">measurements</span> of the cosmic microwave background (CMB) anisotropies constrain the kinematic properties of the reheating era for most of the inflationary <span class="hlt">models</span>. This result is obtained by deriving the marginalized posterior distributions of the reheating parameter for about 200 <span class="hlt">models</span> of slow-roll inflation. Weighted by the statistical evidence of each <span class="hlt">model</span> to explain the data, we show that the Planck 2013 <span class="hlt">measurements</span> induce an average reduction of the posterior-to-prior volume by 40%. Making some additional assumptions on reheating, such as specifying a mean equation of state parameter, or focusing the analysis on peculiar scenarios, can enhance or reduce this constraint. Our study also indicates that the Bayesian evidence of a <span class="hlt">model</span> can substantially be affected by the reheating properties. The precision of the current CMB data is therefore such that estimating the <span class="hlt">observational</span> performance of a <span class="hlt">model</span> now requires incorporating information about its reheating history.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004SPIE.5320...91Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004SPIE.5320...91Y"><span>Adhesion monitoring of skin grafts by photoacoustic <span class="hlt">measurement</span>: experiment using rat allograft <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yamazaki, Mutsuo; Sato, Shunichi; Saito, Daizo; Okada, Yoshiaki; Ashida, Hiroshi; Obara, Minoru</p> <p>2004-07-01</p> <p>Adhesion monitoring of grafted skins is very important in successful treatment of severe burns and traumas. However, current diagnosis of skin grafting is usually done by visual <span class="hlt">observation</span>, which is not reliable and gives no quantitative information on the skin graft adhesion. When the grafted skin adheres well, neovascularities will be generated in the grafted skin tissue, and therefore adhesion may be monitored by detecting the neovascularities. In this study, we attempted to <span class="hlt">measure</span> photoacoustic signals originate from the neovascularities by irradiating the grafted skins with 532-nm nanosecond light pulses in rat autograft and allograft <span class="hlt">models</span>. The <span class="hlt">measurement</span> showed that immediately after skin grafting, photoacoustic signal originate from the blood in the dermis was negligibly small, while 6 - 24 hours after skin grafting, signal was <span class="hlt">observed</span> from the dermis in the graft. We did not <span class="hlt">observe</span> a significant difference between the signals from the autograft and the allograft <span class="hlt">models</span>. These results indicate that neovascularization would take place within 6 hours after skin grafting, and the rejection reaction would make little effect on adhesion within early hours after grafting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA....13207E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA....13207E"><span>On the use of tower-flux <span class="hlt">measurements</span> to assess the performance of global ecosystem <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El Maayar, M.; Kucharik, C.</p> <p>2003-04-01</p> <p>Global ecosystem <span class="hlt">models</span> are important tools for the study of biospheric processes and their responses to environmental changes. Such <span class="hlt">models</span> typically translate knowledge, gained from local <span class="hlt">observations</span>, into estimates of regional or even global outcomes of ecosystem processes. A typical test of ecosystem <span class="hlt">models</span> consists of comparing their output against tower-flux <span class="hlt">measurements</span> of land surface-atmosphere exchange of heat and mass. To perform such tests, <span class="hlt">models</span> are typically run using detailed information on soil properties (texture, carbon content,...) and vegetation structure <span class="hlt">observed</span> at the experimental site (e.g., vegetation height, vegetation phenology, leaf photosynthetic characteristics,...). In global simulations, however, earth's vegetation is typically represented by a limited number of plant functional types (PFT; group of plant species that have similar physiological and ecological characteristics). For each PFT (e.g., temperate broadleaf trees, boreal conifer evergreen trees,...), which can cover a very large area, a set of typical physiological and physical parameters are assigned. Thus, a legitimate question arises: How does the performance of a global ecosystem <span class="hlt">model</span> run using detailed site-specific parameters compare with the performance of a less detailed global version where generic parameters are attributed to a group of vegetation species forming a PFT? To answer this question, we used a multiyear dataset, <span class="hlt">measured</span> at two forest sites with contrasting environments, to compare seasonal and interannual variability of surface-atmosphere exchange of water and carbon predicted by the Integrated BIosphere Simulator-Dynamic Global Vegetation <span class="hlt">Model</span>. Two types of simulations were, thus, performed: a) Detailed runs: <span class="hlt">observed</span> vegetation characteristics (leaf area index, vegetation height,...) and soil carbon content, in addition to climate and soil type, are specified for <span class="hlt">model</span> run; and b) Generic runs: when only <span class="hlt">observed</span> climates and soil types at the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC21E0980P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC21E0980P"><span>An '<span class="hlt">Observational</span> Large Ensemble' to compare <span class="hlt">observed</span> and <span class="hlt">modeled</span> temperature trend uncertainty due to internal variability.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poppick, A. N.; McKinnon, K. A.; Dunn-Sigouin, E.; Deser, C.</p> <p>2017-12-01</p> <p>Initial condition climate <span class="hlt">model</span> ensembles suggest that regional temperature trends can be highly variable on decadal timescales due to characteristics of internal climate variability. Accounting for trend uncertainty due to internal variability is therefore necessary to contextualize recent <span class="hlt">observed</span> temperature changes. However, while the variability of trends in a climate <span class="hlt">model</span> ensemble can be evaluated directly (as the spread across ensemble members), internal variability simulated by a climate <span class="hlt">model</span> may be inconsistent with <span class="hlt">observations</span>. <span class="hlt">Observation</span>-based methods for assessing the role of internal variability on trend uncertainty are therefore required. Here, we use a statistical resampling approach to assess trend uncertainty due to internal variability in historical 50-year (1966-2015) winter near-surface air temperature trends over North America. We compare this estimate of trend uncertainty to simulated trend variability in the NCAR CESM1 Large Ensemble (LENS), finding that uncertainty in wintertime temperature trends over North America due to internal variability is largely overestimated by CESM1, on average by a factor of 32%. Our <span class="hlt">observation</span>-based resampling approach is combined with the forced signal from LENS to produce an '<span class="hlt">Observational</span> Large Ensemble' (OLENS). The members of OLENS indicate a range of spatially coherent fields of temperature trends resulting from different sequences of internal variability consistent with <span class="hlt">observations</span>. The smaller trend variability in OLENS suggests that uncertainty in the historical climate change signal in <span class="hlt">observations</span> due to internal variability is less than suggested by LENS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Prediction&pg=5&id=EJ988907','ERIC'); return false;" href="https://eric.ed.gov/?q=Prediction&pg=5&id=EJ988907"><span>Relationships of <span class="hlt">Measurement</span> Error and Prediction Error in <span class="hlt">Observed</span>-Score Regression</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Moses, Tim</p> <p>2012-01-01</p> <p>The focus of this paper is assessing the impact of <span class="hlt">measurement</span> errors on the prediction error of an <span class="hlt">observed</span>-score regression. <span class="hlt">Measures</span> are presented and described for decomposing the linear regression's prediction error variance into parts attributable to the true score variance and the error variances of the dependent variable and the predictor…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030066199&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcorona','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030066199&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcorona"><span>The Solar Chromosphere/Corona Interface. I; FUV-EUV <span class="hlt">Observations</span> and <span class="hlt">Modeling</span> of Unresolved Coronal Funnels</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Martinez-Galarce, D. S.; Walker, A. B. C.; Barbee, T. W., II; Hoover, R. B.</p> <p>2003-01-01</p> <p>A coronal funnel <span class="hlt">model</span>, developed by Rabin (199l), was tested against a calibrated spectroheliogram recorded in 171 - 175 Angstrom bandpass. This image was recorded on board a sounding rocket experiment flown on 1994 November 3, called the Multi-Spectral Solar Telescope Array, II (MSSTA II), MSSTA, a joint project of Stanford University, the NASA Marshall Space Flight Center and the Lawrence Livermore National Laboratory, is an <span class="hlt">observing</span> platform composed of a set of normal-incidence, multilayer-coated optics designed to obtain narrow bandpass, high resolution images (1 - 3 arc sec) at selected FUV, EUV and soft X-ray wavelengths (44 Angstroms - 1550 Angstroms). Using full-disk images centered at 1550 Angstroms (C IV) and 173 Angstroms (FE IX/X), the funnel <span class="hlt">model</span>, which is based on coronal back-heating, was tested against the data incorporating <span class="hlt">observed</span> constraints on global coverage and <span class="hlt">measured</span> flux. Found, was a class of funnel <span class="hlt">models</span> that could account for the quiescent, globally diffuse and unresolved emission seen in the 171 - 175 Angstrom bandpass, where the funnels are assumed to be rooted in the C IV supergranular network. These <span class="hlt">models</span>, when incorporated with the Chianti spectral code, suggest that this emission is mostly of upper transition region origin and primarily composed of FE IX plasma. The funnels are found to have constrictions, Gamma approx. 6 - 20, which is in good agreement with the <span class="hlt">observations</span>. Further, the fitted <span class="hlt">models</span> simultaneously satisfy global areal constraints seen in both images; namely, that a global network of funnels must cover approx. 70 - 95 % of the total solar surface area seen in the 171 - 175 Angstrom image, and = 45 % of the disk area seen in the 1550 Angstrom bandpass. These findings support the configuration of the EUV magnetic network as suggested by Reeves et af. (1974) and put forth in more detail by Gabriel (1976). Furthermore, the <span class="hlt">models</span> are in good agreement with differential emission <span class="hlt">measure</span> estimates made of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...838L..20H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...838L..20H"><span>Dusty Winds in Active Galactic Nuclei: Reconciling <span class="hlt">Observations</span> with <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hönig, Sebastian F.; Kishimoto, Makoto</p> <p>2017-04-01</p> <p>This Letter presents a revised radiative transfer <span class="hlt">model</span> for the infrared (IR) emission of active galactic nuclei (AGNs). While current <span class="hlt">models</span> assume that the IR is emitted from a dusty torus in the equatorial plane of the AGNs, spatially resolved <span class="hlt">observations</span> indicate that the majority of the IR emission from ≲100 pc in many AGNs originates from the polar region, contradicting classical torus <span class="hlt">models</span>. The new <span class="hlt">model</span> CAT3D-WIND builds upon the suggestion that the dusty gas around the AGNs consists of an inflowing disk and an outflowing wind. Here, it is demonstrated that (1) such disk+wind <span class="hlt">models</span> cover overall a similar parameter range of <span class="hlt">observed</span> spectral features in the IR as classical clumpy torus <span class="hlt">models</span>, e.g., the silicate feature strengths and mid-IR spectral slopes, (2) they reproduce the 3-5 μm bump <span class="hlt">observed</span> in many type 1 AGNs unlike torus <span class="hlt">models</span>, and (3) they are able to explain polar emission features seen in IR interferometry, even for type 1 AGNs at relatively low inclination, as demonstrated for NGC3783. These characteristics make it possible to reconcile radiative transfer <span class="hlt">models</span> with <span class="hlt">observations</span> and provide further evidence of a two-component parsec-scale dusty medium around AGNs: the disk gives rise to the 3-5 μm near-IR component, while the wind produces the mid-IR emission. The <span class="hlt">model</span> SEDs will be made available for download.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654422-dusty-winds-active-galactic-nuclei-reconciling-observations-models','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654422-dusty-winds-active-galactic-nuclei-reconciling-observations-models"><span>Dusty Winds in Active Galactic Nuclei: Reconciling <span class="hlt">Observations</span> with <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Hönig, Sebastian F.; Kishimoto, Makoto, E-mail: S.Hoenig@soton.ac.uk</p> <p>2017-04-01</p> <p>This Letter presents a revised radiative transfer <span class="hlt">model</span> for the infrared (IR) emission of active galactic nuclei (AGNs). While current <span class="hlt">models</span> assume that the IR is emitted from a dusty torus in the equatorial plane of the AGNs, spatially resolved <span class="hlt">observations</span> indicate that the majority of the IR emission from ≲100 pc in many AGNs originates from the polar region, contradicting classical torus <span class="hlt">models</span>. The new <span class="hlt">model</span> CAT3D-WIND builds upon the suggestion that the dusty gas around the AGNs consists of an inflowing disk and an outflowing wind. Here, it is demonstrated that (1) such disk+wind <span class="hlt">models</span> cover overall amore » similar parameter range of <span class="hlt">observed</span> spectral features in the IR as classical clumpy torus <span class="hlt">models</span>, e.g., the silicate feature strengths and mid-IR spectral slopes, (2) they reproduce the 3–5 μ m bump <span class="hlt">observed</span> in many type 1 AGNs unlike torus <span class="hlt">models</span>, and (3) they are able to explain polar emission features seen in IR interferometry, even for type 1 AGNs at relatively low inclination, as demonstrated for NGC3783. These characteristics make it possible to reconcile radiative transfer <span class="hlt">models</span> with <span class="hlt">observations</span> and provide further evidence of a two-component parsec-scale dusty medium around AGNs: the disk gives rise to the 3–5 μ m near-IR component, while the wind produces the mid-IR emission. The <span class="hlt">model</span> SEDs will be made available for download.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150023372&hterms=Garcia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D30%26Ntt%3DR%2BGarcia','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150023372&hterms=Garcia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D30%26Ntt%3DR%2BGarcia"><span>Predicting the Mineral Composition of Dust Aerosols. Part 2; <span class="hlt">Model</span> Evaluation and Identification of Key Processes with <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Perlwitz, J. P.; Garcia-Pando, C. Perez; Miller, R. L.</p> <p>2015-01-01</p> <p>A global compilation of nearly sixty <span class="hlt">measurement</span> studies is used to evaluate two methods of simulating the mineral composition of dust aerosols in an Earth system <span class="hlt">model</span>. Both methods are based upon a Mean Mineralogical Table (MMT) that relates the soil mineral fractions to a global atlas of arid soil type. The Soil Mineral Fraction (SMF) method assumes that the aerosol mineral fractions match the fractions of the soil. The MMT is based upon soil <span class="hlt">measurements</span> after wet sieving, a process that destroys aggregates of soil particles that would have been emitted from the original, undisturbed soil. The second method approximately reconstructs the emitted aggregates. This <span class="hlt">model</span> is referred to as the Aerosol Mineral Fraction (AMF) method because the mineral fractions of the aerosols differ from those of the wet-sieved parent soil, partly due to reaggregation. The AMF method remedies some of the deficiencies of the SMF method in comparison to <span class="hlt">observations</span>. Only the AMF method exhibits phyllosilicate mass at silt sizes, where they are abundant according to <span class="hlt">observations</span>. In addition, the AMF quartz fraction of silt particles is in better agreement with <span class="hlt">measured</span> values, in contrast to the overestimated SMF fraction. <span class="hlt">Measurements</span> at distinct clay and silt particle sizes are shown to be more useful for evaluation of the <span class="hlt">models</span>, in contrast to the sum over all particles sizes that is susceptible to compensating errors, as illustrated by the SMF experiment. <span class="hlt">Model</span> errors suggest that allocation of the emitted silt fraction of each mineral into the corresponding transported size categories is an important remaining source of uncertainty. Evaluation of both <span class="hlt">models</span> and the MMT is hindered by the limited number of size-resolved <span class="hlt">measurements</span> of mineral content that sparsely sample aerosols from the major dust sources. The importance of climate processes dependent upon aerosol mineral composition shows the need for global and routine mineral <span class="hlt">measurements</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...853..107R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...853..107R"><span>A <span class="hlt">Model</span> of Titan-like Chemistry to Connect Experiments and Cassini <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raymond, Alexander W.; Sciamma-O’Brien, Ella; Salama, Farid; Mazur, Eric</p> <p>2018-02-01</p> <p>A numerical <span class="hlt">model</span> is presented for interpreting the chemical pathways that lead to the experimental mass spectra acquired in the Titan Haze Simulation (THS) laboratory experiments and for comparing the electron density and temperature of the THS plasma to <span class="hlt">observations</span> made at Titan by the Cassini spacecraft. The THS plasma is a pulsed glow-discharge experiment designed to simulate the reaction of N2/CH4-dominated gas in Titan's upper atmosphere. The transient, one-dimensional <span class="hlt">model</span> of THS chemistry tracks the evolution of more than 120 species in the direction of the plasma flow. As the minor species C2H2 and C2H4 are added to the N2/CH4-based mixture, the <span class="hlt">model</span> correctly predicts the emergence of reaction products with up to five carbon atoms in relative abundances that agree well with <span class="hlt">measured</span> mass spectra. Chemical growth in Titan's upper atmosphere transpires through ion–neutral and neutral–neutral chemistry, and the main reactions involving a series of known atmospheric species are retrieved from the calculation. The <span class="hlt">model</span> indicates that the electron density and chemistry are steady during more than 99% of the 300 μs long discharge pulse. The <span class="hlt">model</span> also suggests that the THS ionization fraction and electron temperature are comparable to those <span class="hlt">measured</span> in Titan's upper atmosphere. These findings reaffirm that the THS plasma is a controlled analog environment for studying the first and intermediate steps of chemistry in Titan's upper atmosphere.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMEP51C0571B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMEP51C0571B"><span>Method to Rapidly Collect Thousands of Velocity <span class="hlt">Observations</span> to Validate Million-Element 2D Hydrodynamic <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barker, J. R.; Pasternack, G. B.; Bratovich, P.; Massa, D.; Reedy, G.; Johnson, T.</p> <p>2010-12-01</p> <p>Two-dimensional (depth-averaged) hydrodynamic <span class="hlt">models</span> have existed for decades and are used to study a variety of hydrogeomorphic processes as well as to design river rehabilitation projects. Rapid computer and coding advances are revolutionizing the size and detail of 2D <span class="hlt">models</span>. Meanwhile, advances in topo mapping and environmental informatics are providing the data inputs to drive large, detailed simulations. Million-element computational meshes are in hand. With simulations of this size and detail, the primary challenge has shifted to finding rapid and inexpensive means for testing <span class="hlt">model</span> predictions against <span class="hlt">observations</span>. Standard methods for collecting velocity data include boat-mounted ADCP and point-based sensors on boats or wading rods. These methods are labor intensive and often limited to a narrow flow range. Also, they generate small datasets at a few cross-sections, which is inadequate to characterize the statistical structure of the relation between predictions and <span class="hlt">observations</span>. Drawing on the long-standing oceanographic method of using drogues to track water currents, previous studies have demonstrated the potential of small dGPS units to obtain surface velocity in rivers. However, dGPS is too inaccurate to test 2D <span class="hlt">models</span>. Also, there is financial risk in losing drogues in rough currents. In this study, an RTK GPS unit was mounted onto a manned whitewater kayak. The boater positioned himself into the current and used floating debris to maintain a speed and heading consistent with the ambient surface flow field. RTK GPS <span class="hlt">measurements</span> were taken ever 5 sec. From these positions, a 2D velocity vector was obtained. The method was tested over ~20 km of the lower Yuba River in California in flows ranging from 500-5000 cfs, yielding 5816 <span class="hlt">observations</span>. To compare velocity magnitude against the 2D <span class="hlt">model</span>-predicted depth-averaged value, kayak-based surface values were scaled down by an optimized constant (0.72), which had no negative effect on regression analysis</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.A31A0851P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.A31A0851P"><span>Assimilating Satellite SST <span class="hlt">Observations</span> into a Diurnal Cycle <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pimentel, S.; Haines, K.; Nichols, N. K.</p> <p>2006-12-01</p> <p>The wealth of satellite sea surface temperature (SST) data now available opens the possibility of large improvements in SST estimation. However the use of such data is not straight forward; a major difficulty in assimilating satellite <span class="hlt">observations</span> is that they represent a near surface temperature, whereas in ocean <span class="hlt">models</span> the top level represents the temperature at a greater depth. During the day, under favourable conditions of clear skies and calm winds, the near surface temperature is often seen to have a diurnal cycle that is picked up in satellite <span class="hlt">observations</span>. Current ocean <span class="hlt">models</span> do not have the vertical or temporal resolution to adequately represent this daytime warming. The usual approach is to discard daytime <span class="hlt">observations</span> as they are considered diurnally `corrupted'. A new assimilation technique is developed here that assimilates <span class="hlt">observations</span> into a diurnal cycle <span class="hlt">model</span>. The diurnal cycle of SSTs are <span class="hlt">modelled</span> using a 1-D mixed layer <span class="hlt">model</span> with fine near surface resolution and 6 hourly forcing from NWP analyses. The accuracy of the SST estimates are hampered by uncertainties in the forcing data. The extent of diurnal SST warming at a particular location and time is predominately governed by a non-linear response to cloud cover and sea surface wind speeds which greatly affect the air-sea fluxes. The method proposed here combines infrared and microwave SST satellite <span class="hlt">observations</span> in order to derive corrections to the cloud cover and wind speed values over the day. By adjusting the forcing, SST estimation and air-sea fluxes should be improved and are at least more consistent with each other. This new technique for assimilating SST data can be considered a tool for producing more accurate diurnal warming estimates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24560551','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24560551"><span><span class="hlt">Observed</span> changes in radiographic <span class="hlt">measurements</span> of the first ray after frontal plane rotation of the first metatarsal in a cadaveric foot <span class="hlt">model</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dayton, Paul; Feilmeier, Mindi; Hirschi, Jordan; Kauwe, Merrell; Kauwe, John S K</p> <p>2014-01-01</p> <p>We <span class="hlt">observed</span> the changes in the angular <span class="hlt">measurements</span> commonly used in the evaluation of the first metatarsal and first metatarsophalangeal joint in cadaveric specimens before and after frontal plane rotation of the first metatarsal. <span class="hlt">Measurements</span> of the first and second intermetatarsal angle (IMA), hallux abductus angle, proximal articular set angle, and tibial sesamoid position (TSP) were taken after varying degrees of varus and valgus rotation of the first metatarsal. Standard dorsoplantar radiographs were taken at 0°, 10°, 20°, and 30° of valgus rotation of the first metatarsal and repeated at 10°, 20°, and 30° varus rotation of the first metatarsal. The data were analyzed using a mixed linear <span class="hlt">model</span> to compare the change in each angle <span class="hlt">measurement</span> over the range of valgus and varus rotation. The change in the TSP was significant in both valgus and varus rotations (p = .0004 and p = .028, respectively), an increase in valgus rotation causing an increase in the TSP and an increase in varus rotation causing a decrease in TSP. The change in the IMA was significant compared with valgus rotation (p = .028), showing that as the valgus rotation increased, the IMA also increased. However, compared with the varus rotation, the correlation was not significant (p = .18). The proximal articular set angle and hallux abductus angle <span class="hlt">measurements</span>, compared with metatarsal rotation, showed positive trends but were not statistically significant. From our results and a review of the published data, we have hypothesized that frontal plane rotation of the first metatarsal is an integral component of hallux abducto valgus pathologic features, specifically in relation to the TSP and IMA. Copyright © 2014 American College of Foot and Ankle Surgeons. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..APRU12004S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..APRU12004S"><span>Telescope Array UHECR composition <span class="hlt">measurement</span> via stereoscopic fluorescence <span class="hlt">observation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stroman, Thomas; Bergman, Douglas; Telescope Array Collaboration</p> <p>2016-03-01</p> <p>When entering Earth's atmosphere at ultra-high energies, cosmic rays (UHECRs) produce extensive air showers whose longitudinal development is influenced by the incident primary particle's mass. Each longitudinal shower profile reaches its maximum particle count at an atmospheric slant depth Xmax, and the distributions of <span class="hlt">observed</span> Xmax values can be compared to those predicted by detailed simulations of the air-shower physics and the detector; accurately simulated compositions that most closely resemble that found in nature will produce the best agreement between predicted and <span class="hlt">observed</span> Xmax distributions. This is the basis of composition <span class="hlt">measurement</span> at the Telescope Array experiment, the largest and most sensitive UHECR detector in the northern hemisphere. At the perimeter of a large surface-detector array are three fluorescence telescope stations, whose overlapping apertures enable high-precision reconstruction of Xmax from stereoscopic <span class="hlt">observation</span> of air-shower longitudinal profiles. We present the distribution of Xmax <span class="hlt">observed</span> during eight years of operation, and from comparisons with several simulated combinations of composition and high-energy hadronic physics, we show that a low primary mass is favored at E >10 18 . 2 eV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B43A0554S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B43A0554S"><span>Developing a <span class="hlt">Model</span> to Estimate Freshwater Gross Primary Production Using MODIS Surface Temperature <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saberi, S. J.; Weathers, K. C.; Norouzi, H.; Prakash, S.; Solomon, C.; Boucher, J. M.</p> <p>2016-12-01</p> <p>Lakes contribute to local and regional climate conditions, cycle nutrients, and are viable indicators of climate change due to their sensitivity to disturbances in their water and airsheds. Utilizing spaceborne remote sensing (RS) techniques has considerable potential in studying lake dynamics because it allows for coherent and consistent spatial and temporal <span class="hlt">observations</span> as well as estimates of lake functions without in situ <span class="hlt">measurements</span>. However, in order for RS products to be useful, algorithms that relate in situ <span class="hlt">measurements</span> to RS data must be developed. Estimates of lake metabolic rates are of particular scientific interest since they are indicative of lakes' roles in carbon cycling and ecological function. Currently, there are few existing algorithms relating remote sensing products to in-lake estimates of metabolic rates and more in-depth studies are still required. Here we use satellite surface temperature <span class="hlt">observations</span> from Moderate Resolution Imaging Spectroradiometer (MODIS) product (MYD11A2) and published in-lake gross primary production (GPP) estimates for eleven globally distributed lakes during a one-year period to produce a univariate quadratic equation <span class="hlt">model</span>. The general <span class="hlt">model</span> was validated using other lakes during an equivalent one-year time period (R2=0.76). The statistical analyses reveal significant positive relationships between MODIS temperature data and the previously <span class="hlt">modeled</span> in-lake GPP. Lake-specific <span class="hlt">models</span> for Lake Mendota (USA), Rotorua (New Zealand), and Taihu (China) showed stronger relationships than the general combined <span class="hlt">model</span>, pointing to local influences such as watershed characteristics on in-lake GPP in some cases. These validation data suggest that the developed algorithm has a potential to predict lake GPP on a global scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22289012','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22289012"><span>Foundation <span class="hlt">observation</span> of teaching project--a developmental <span class="hlt">model</span> of peer <span class="hlt">observation</span> of teaching.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pattison, Andrew Timothy; Sherwood, Morgan; Lumsden, Colin James; Gale, Alison; Markides, Maria</p> <p>2012-01-01</p> <p>Peer <span class="hlt">observation</span> of teaching is important in the development of educators. The foundation curriculum specifies teaching competencies that must be attained. We created a developmental <span class="hlt">model</span> of peer <span class="hlt">observation</span> of teaching to help our foundation doctors achieve these competencies and develop as educators. A process for peer <span class="hlt">observation</span> was created based on key features of faculty development. The project consisted of a pre-<span class="hlt">observation</span> meeting, the <span class="hlt">observation</span>, a post-<span class="hlt">observation</span> debrief, writing of reflective reports and group feedback sessions. The project was evaluated by completion of questionnaires and focus groups held with both foundation doctors and the students they taught to achieve triangulation. Twenty-one foundation doctors took part. All completed reflective reports on their teaching. Participants described the process as useful in their development as educators, citing specific examples of changes to their teaching practice. Medical students rated the sessions as better or much better quality as their usual teaching. The study highlights the benefits of the project to individual foundation doctors, undergraduate medical students and faculty. It acknowledges potential anxieties involved in having teaching <span class="hlt">observed</span>. A structured programme of <span class="hlt">observation</span> of teaching can deliver specific teaching competencies required by foundation doctors and provides additional benefits.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AdWR...50..120K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AdWR...50..120K"><span>Evaluating the two-source energy balance <span class="hlt">model</span> using local thermal and surface flux <span class="hlt">observations</span> in a strongly advective irrigated agricultural area</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kustas, William P.; Alfieri, Joseph G.; Anderson, Martha C.; Colaizzi, Paul D.; Prueger, John H.; Evett, Steven R.; Neale, Christopher M. U.; French, Andrew N.; Hipps, Lawrence E.; Chávez, José L.; Copeland, Karen S.; Howell, Terry A.</p> <p>2012-12-01</p> <p>Application and validation of many thermal remote sensing-based energy balance <span class="hlt">models</span> involve the use of local meteorological inputs of incoming solar radiation, wind speed and air temperature as well as accurate land surface temperature (LST), vegetation cover and surface flux <span class="hlt">measurements</span>. For operational applications at large scales, such local information is not routinely available. In addition, the uncertainty in LST estimates can be several degrees due to sensor calibration issues, atmospheric effects and spatial variations in surface emissivity. Time differencing techniques using multi-temporal thermal remote sensing <span class="hlt">observations</span> have been developed to reduce errors associated with deriving the surface-air temperature gradient, particularly in complex landscapes. The Dual-Temperature-Difference (DTD) method addresses these issues by utilizing the Two-Source Energy Balance (TSEB) <span class="hlt">model</span> of Norman et al. (1995) [1], and is a relatively simple scheme requiring meteorological input from standard synoptic weather station networks or mesoscale <span class="hlt">modeling</span>. A comparison of the TSEB and DTD schemes is performed using LST and flux <span class="hlt">observations</span> from eddy covariance (EC) flux towers and large weighing lysimeters (LYs) in irrigated cotton fields collected during BEAREX08, a large-scale field experiment conducted in the semi-arid climate of the Texas High Plains as described by Evett et al. (2012) [2]. <span class="hlt">Model</span> output of the energy fluxes (i.e., net radiation, soil heat flux, sensible and latent heat flux) generated with DTD and TSEB using local and remote meteorological <span class="hlt">observations</span> are compared with EC and LY <span class="hlt">observations</span>. The DTD method is found to be significantly more robust in flux estimation compared to the TSEB using the remote meteorological <span class="hlt">observations</span>. However, discrepancies between <span class="hlt">model</span> and <span class="hlt">measured</span> fluxes are also found to be significantly affected by the local inputs of LST and vegetation cover and the representativeness of the remote sensing <span class="hlt">observations</span> with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.1263D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.1263D"><span>Helicopter-borne <span class="hlt">observations</span> of the continental background aerosol in combination with remote sensing and ground-based <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Düsing, Sebastian; Wehner, Birgit; Seifert, Patric; Ansmann, Albert; Baars, Holger; Ditas, Florian; Henning, Silvia; Ma, Nan; Poulain, Laurent; Siebert, Holger; Wiedensohler, Alfred; Macke, Andreas</p> <p>2018-01-01</p> <p> different altitudes were determined using the airborne in situ <span class="hlt">measurements</span> and were compared with the lidar <span class="hlt">measurements</span>. The investigation of the optical properties shows that on average the airborne-based particle light backscatter coefficient is 50.1 % smaller for 1064 nm, 27.4 % smaller for 532 nm, and 29.5 % smaller for 355 nm than the <span class="hlt">measurements</span> of the lidar system. These results are quite promising, since in situ <span class="hlt">measurement</span>-based Mie calculations of the particle light backscattering are scarce and the <span class="hlt">modeling</span> is quite challenging. In contrast, for the particle light extinction coefficient we found a good agreement. The airborne-based particle light extinction coefficient was just 8.2 % larger for 532 nm and 3 % smaller for 355 nm, for an assumed LR of 55 sr. The particle light extinction coefficient for 1064 nm was derived with a LR of 30 sr. For this wavelength, the airborne-based particle light extinction coefficient is 5.2 % smaller than the lidar <span class="hlt">measurements</span>. For the first time, the lidar ratio of 30 sr for 1064 nm was determined on the basis of in situ <span class="hlt">measurements</span> and the LR of 55 sr for 355 and 532 nm wavelength was reproduced for European continental aerosol on the basis of this comparison. Lidar <span class="hlt">observations</span> and the in situ based aerosol optical properties agree within the uncertainties. However, our <span class="hlt">observations</span> indicate that a determination of the PNSD for a large size range is important for a reliable <span class="hlt">modeling</span> of aerosol particle backscattering.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1917007S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1917007S"><span>Quantitative assessments of mantle flow <span class="hlt">models</span> against seismic <span class="hlt">observations</span>: Influence of uncertainties in mineralogical parameters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schuberth, Bernhard S. A.</p> <p>2017-04-01</p> <p> synthetic traveltime data can then be compared - on statistical grounds - to the traveltime variations <span class="hlt">observed</span> on Earth. Here, we now investigate the influence of uncertainties in the various input parameters that enter our <span class="hlt">modelling</span>. This is especially important for the material properties at high pressure and high temperature entering the mineralogical <span class="hlt">models</span>. In particular, this concerns uncertainties that arise from relating <span class="hlt">measurements</span> in the laboratory to Earth properties on a global scale. As one example, we will address the question on the influence of anelasticity on the variance of global synthetic traveltime residuals. Owing to the differences in seismic frequency content between laboratory <span class="hlt">measurements</span> (MHz to GHz) and the Earth (mHz to Hz), the seismic velocities given in the mineralogical <span class="hlt">models</span> need to be adjusted; that is, corrected for dispersion due to anelastic effects. This correction will increase the sensitivity of the seismic velocities to temperature variations. The magnitude of this increase depends on absolute temperature, frequency, the frequency dependence of attenuation and the activation enthalpy of the dissipative process. Especially the latter two are poorly known for mantle minerals and our results indicate that variations in activation enthalpy potentially produce the largest differences in temperature sensitivity with respect to the purely elastic case. We will present new wave propagation simulations and corresponding statistical analyses of traveltime <span class="hlt">measurements</span> for different synthetic seismic <span class="hlt">models</span> spanning the possible range of anelastic velocity conversions (while being based on the same mantle circulation <span class="hlt">model</span>).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DPPGI2006K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DPPGI2006K"><span>MHD <span class="hlt">modeling</span> of DIII-D QH-mode discharges and comparison to <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>King, Jacob</p> <p>2016-10-01</p> <p>MHD <span class="hlt">modeling</span> of DIII-D QH-mode discharges and comparison to <span class="hlt">observations</span> Nonlinear NIMROD simulations, initialized from a reconstruction of a DIII-D QH-mode discharge with broadband MHD, saturate into a turbulent state, but do not saturate when flow is not included. This is consistent with the experimental results of the quiescent regime <span class="hlt">observed</span> on DIII-D with broadband MHD activity [Garofalo et al., PoP (2015) and refs. within]. These ELM-free discharges have the normalized pedestal-plasma confinement necessary for burning-plasma operation on ITER. Relative to QH-mode operation with more coherent MHD activity, operation with broadband MHD tends to occur at higher densities and lower rotation and thus may be more relevant to ITER. The nonlinear NIMROD simulations require highly accurate equilibrium reconstructions. Our equilibrium reconstructions include the scrape-off-layer profiles and the <span class="hlt">measured</span> toroidal and poloidal rotation profiles. The simulation develops into a saturated turbulent state and the n=1 and 2 modes become dominant through an inverse cascade. Each toroidal mode in the range of n=1-5 is dominant at a different time. The perturbations are advected and sheared apart in the counter-clockwise direction consistent with the direction of the poloidal flow inside the LCFS. Work towards validation through comparison to magnetic coil and Doppler reflectometry <span class="hlt">measurements</span> is presented. Consistent with experimental <span class="hlt">observations</span> during QH-mode, the simulated state leads to large particle transport relative to the thermal transport. Analysis shows that the phase of the density and temperature perturbations differ resulting in greater convective particle transport relative to the convective thermal transport. This work supported by the U.S. Department of Energy Office of Science and the SciDAC Center for Extended MHD <span class="hlt">Modeling</span> under Contract Numbers DE-FC02-06ER54875, DE-FC02-08ER54972 and DE-FC02-04ER54698.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880024294&hterms=Lte&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DLte','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880024294&hterms=Lte&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DLte"><span>LTE <span class="hlt">modeling</span> of inhomogeneous chromospheric structure using high-resolution limb <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lindsey, C.</p> <p>1987-01-01</p> <p>The paper discusses considerations relevant to LTE <span class="hlt">modeling</span> of rough atmospheres. Particular attention is given to the application of recent high-resolution <span class="hlt">observations</span> of the solar limb in the far-infrared and radio continuum to the <span class="hlt">modeling</span> of chromospheric spicules. It is explained how the continuum limb <span class="hlt">observations</span> can be combined with morphological knowledge of spicule structure to <span class="hlt">model</span> the physical conditions in chromospheric spicules. This discussion forms the basis for a chromospheric <span class="hlt">model</span> presented in a parallel publication based on <span class="hlt">observations</span> ranging from 100 microns to 2.6 mm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10136E..13K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10136E..13K"><span>Visual-search <span class="hlt">model</span> <span class="hlt">observer</span> for assessing mass detection in CT</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Karbaschi, Zohreh; Gifford, Howard C.</p> <p>2017-03-01</p> <p>Our aim is to devise <span class="hlt">model</span> <span class="hlt">observers</span> (MOs) to evaluate acquisition protocols in medical imaging. To optimize protocols for human <span class="hlt">observers</span>, an MO must reliably interpret images containing quantum and anatomical noise under aliasing conditions. In this study of sampling parameters for simulated lung CT, the lesion-detection performance of human <span class="hlt">observers</span> was compared with that of visual-search (VS) <span class="hlt">observers</span>, a channelized nonprewhitening (CNPW) <span class="hlt">observer</span>, and a channelized Hoteling (CH) <span class="hlt">observer</span>. Scans of a mathematical torso phantom <span class="hlt">modeled</span> single-slice parallel-hole CT with varying numbers of detector pixels and angular projections. Circular lung lesions had a fixed radius. Twodimensional FBP reconstructions were performed. A localization ROC study was conducted with the VS, CNPW and human <span class="hlt">observers</span>, while the CH <span class="hlt">observer</span> was applied in a location-known ROC study. Changing the sampling parameters had negligible effect on the CNPW and CH <span class="hlt">observers</span>, whereas several VS <span class="hlt">observers</span> demonstrated a sensitivity to sampling artifacts that was in agreement with how the humans performed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20120013526&hterms=mass+communication&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmass%2Bcommunication','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20120013526&hterms=mass+communication&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmass%2Bcommunication"><span>Optimal Asteroid Mass Determination from Planetary Range <span class="hlt">Observations</span>: A Study of a Simplified Test <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuchynka, P.; Laskar, J.; Fienga, A.</p> <p>2011-01-01</p> <p>Mars ranging <span class="hlt">observations</span> are available over the past 10 years with an accuracy of a few meters. Such precise <span class="hlt">measurements</span> of the Earth-Mars distance provide valuable constraints on the masses of the asteroids perturbing both planets. Today more than 30 asteroid masses have thus been estimated from planetary ranging data (see [1] and [2]). Obtaining unbiased mass estimations is nevertheless difficult. Various systematic errors can be introduced by imperfect reduction of spacecraft tracking <span class="hlt">observations</span> to planetary ranging data. The large number of asteroids and the limited a priori knowledge of their masses is also an obstacle for parameter selection. Fitting in a <span class="hlt">model</span> a mass of a negligible perturber, or on the contrary omitting a significant perturber, will induce important bias in determined asteroid masses. In this communication, we investigate a simplified version of the mass determination problem. Instead of planetary ranging <span class="hlt">observations</span> from spacecraft or radar data, we consider synthetic ranging <span class="hlt">observations</span> generated with the INPOP [2] ephemeris for a test <span class="hlt">model</span> containing 25000 asteroids. We then suggest a method for optimal parameter selection and estimation in this simplified framework.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930015969','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930015969"><span>The atmospheric effects of stratospheric aircraft. Report of the 1992 <span class="hlt">Models</span> and <span class="hlt">Measurements</span> Workshop. Volume 2: Comparisons with global atmospheric <span class="hlt">measurements</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Prather, Michael J. (Editor); Remsberg, Ellis E. (Editor)</p> <p>1993-01-01</p> <p>This Workshop on Stratospheric <span class="hlt">Models</span> and <span class="hlt">Measurements</span> (M&M) marks a significant expansion in the history of <span class="hlt">model</span> intercomparisons. It provides a foundation for establishing the credibility of stratospheric <span class="hlt">models</span> used in environmental assessments of chlorofluorocarbons, aircraft emissions, and climate-chemistry interactions. The core of the M&M comparisons involves the selection of <span class="hlt">observations</span> of the current stratosphere (i.e., within the last 15 years): these data are believed to be accurate and representative of certain aspects of stratospheric chemistry and dynamics that the <span class="hlt">models</span> should be able to simulate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSEC14C1009M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSEC14C1009M"><span>Wave Dissipation over Nearshore Beach Morphology: Insights from High-Resolution LIDAR <span class="hlt">Observations</span> and the SWASH Wave <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mulligan, R. P.; Gomes, E.; McNinch, J.; Brodie, K. L.</p> <p>2016-02-01</p> <p>Numerical <span class="hlt">modelling</span> of the nearshore zone can be computationally intensive due to the complexity of wave breaking, and the need for high temporal and spatial resolution. In this study we apply the SWASH non-hydrostatic wave-flow <span class="hlt">model</span> that phase-resolves the free surface and fluid motions in the water column at high resolution. The <span class="hlt">model</span> is forced using <span class="hlt">observed</span> directional energy spectra, and results are compared to wave <span class="hlt">observations</span> during moderate storm events. <span class="hlt">Observations</span> are collected outside the surf zone using acoustic wave and currents sensors, and inside the surf zone over a 100 m transect using high-resolution LIDAR <span class="hlt">measurements</span> of the sea surface from a sensor mounted on a tower on the beach dune at the Field Research Facility in Duck, NC. The <span class="hlt">model</span> is applied to four cases with different wave conditions and bathymetry, and used to predict the spatial variability in wave breaking, and correlation between energy dissipation and morphologic features. <span class="hlt">Model</span> results compare well with <span class="hlt">observations</span> of spectral evolution outside the surf zone, and with the remotely sensed <span class="hlt">observations</span> of wave transformation inside the surf zone. The results indicate the importance of nearshore bars, rip-channels, and larger features (major scour depression under the pier following large waves from Hurricane Irene) on the location of wave breaking and alongshore variability in wave energy dissipation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A31G2268V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A31G2268V"><span><span class="hlt">Measurement</span> needs guided by synthetic radar scans in high-resolution <span class="hlt">model</span> output</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Varble, A.; Nesbitt, S. W.; Borque, P.</p> <p>2017-12-01</p> <p>Microphysical and dynamical process interactions within deep convective clouds are not well understood, partly because <span class="hlt">measurement</span> strategies often focus on statistics of cloud state rather than cloud processes. While processes cannot be directly <span class="hlt">measured</span>, they can be inferred with sufficiently frequent and detailed scanning radar <span class="hlt">measurements</span> focused on the life cycleof individual cloud regions. This is a primary goal of the 2018-19 DOE ARM Cloud, Aerosol, and Complex Terrain Interactions (CACTI) and NSF Remote sensing of Electrification, Lightning, And Mesoscale/microscale Processes with Adaptive Ground <span class="hlt">Observations</span> (RELAMPAGO) field campaigns in central Argentina, where orographic deep convective initiation is frequent with some high-impact systems growing into the tallest and largest in the world. An array of fixed and mobile scanning multi-wavelength dual-polarization radars will be coupled with surface <span class="hlt">observations</span>, sounding systems, multi-wavelength vertical profilers, and aircraft in situ <span class="hlt">measurements</span> to characterize convective cloud life cycles and their relationship with environmental conditions. While detailed cloud processes are an <span class="hlt">observational</span> target, the radar scan patterns that are most ideal for <span class="hlt">observing</span> them are unclear. They depend on the locations and scales of key microphysical and dynamical processes operating within the cloud. High-resolution simulations of clouds, while imperfect, can provide information on these locations and scales that guide radar <span class="hlt">measurement</span> needs. Radar locations are set in the <span class="hlt">model</span> domain based on planned experiment locations, and simulatedorographic deep convective initiation and upscale growth are sampled using a number of different scans involving RHIs or PPIs with predefined elevation and azimuthal angles that approximately conform with radar range and beam width specifications. Each full scan pattern is applied to output atsingle <span class="hlt">model</span> time steps with time step intervals that depend on the length of time</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.5878D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.5878D"><span>Calibration of a distributed hydrologic <span class="hlt">model</span> using <span class="hlt">observed</span> spatial patterns from MODIS data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Demirel, Mehmet C.; González, Gorka M.; Mai, Juliane; Stisen, Simon</p> <p>2016-04-01</p> <p>Distributed hydrologic <span class="hlt">models</span> are typically calibrated against streamflow <span class="hlt">observations</span> at the outlet of the basin. Along with these <span class="hlt">observations</span> from gauging stations, satellite based estimates offer independent evaluation data such as remotely sensed actual evapotranspiration (aET) and land surface temperature. The primary objective of the study is to compare <span class="hlt">model</span> calibrations against traditional downstream discharge <span class="hlt">measurements</span> with calibrations against simulated spatial patterns and combinations of both types of <span class="hlt">observations</span>. While the discharge based <span class="hlt">model</span> calibration typically improves the temporal dynamics of the <span class="hlt">model</span>, it seems to give rise to minimum improvement of the simulated spatial patterns. In contrast, objective functions specifically targeting the spatial pattern performance could potentially increase the spatial <span class="hlt">model</span> performance. However, most <span class="hlt">modeling</span> studies, including the <span class="hlt">model</span> formulations and parameterization, are not designed to actually change the simulated spatial pattern during calibration. This study investigates the potential benefits of incorporating spatial patterns from MODIS data to calibrate the mesoscale hydrologic <span class="hlt">model</span> (mHM). This <span class="hlt">model</span> is selected as it allows for a change in the spatial distribution of key soil parameters through the optimization of pedo-transfer function parameters and includes options for using fully distributed daily Leaf Area Index (LAI) values directly as input. In addition the simulated aET can be estimated at a spatial resolution suitable for comparison to the spatial patterns <span class="hlt">observed</span> with MODIS data. To increase our control on spatial calibration we introduced three additional parameters to the <span class="hlt">model</span>. These new parameters are part of an empirical equation to the calculate crop coefficient (Kc) from daily LAI maps and used to update potential evapotranspiration (PET) as <span class="hlt">model</span> inputs. This is done instead of correcting/updating PET with just a uniform (or aspect driven) factor used in the mHM <span class="hlt">model</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.H42C..04V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.H42C..04V"><span>Balancing <span class="hlt">model</span> complexity and <span class="hlt">measurements</span> in hydrology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Van De Giesen, N.; Schoups, G.; Weijs, S. V.</p> <p>2012-12-01</p> <p>The Data Processing Inequality implies that hydrological <span class="hlt">modeling</span> can only reduce, and never increase, the amount of information available in the original data used to formulate and calibrate hydrological <span class="hlt">models</span>: I(X;Z(Y)) ≤ I(X;Y). Still, hydrologists around the world seem quite content building <span class="hlt">models</span> for "their" watersheds to move our discipline forward. Hydrological <span class="hlt">models</span> tend to have a hybrid character with respect to underlying physics. Most <span class="hlt">models</span> make use of some well established physical principles, such as mass and energy balances. One could argue that such principles are based on many <span class="hlt">observations</span>, and therefore add data. These physical principles, however, are applied to hydrological <span class="hlt">models</span> that often contain concepts that have no direct counterpart in the <span class="hlt">observable</span> physical universe, such as "buckets" or "reservoirs" that fill up and empty out over time. These not-so-physical concepts are more like the Artificial Neural Networks and Support Vector Machines of the Artificial Intelligence (AI) community. Within AI, one quickly came to the realization that by increasing <span class="hlt">model</span> complexity, one could basically fit any dataset but that complexity should be controlled in order to be able to predict unseen events. The more data are available to train or calibrate the <span class="hlt">model</span>, the more complex it can be. Many complexity control approaches exist in AI, with Solomonoff inductive inference being one of the first formal approaches, the Akaike Information Criterion the most popular, and Statistical Learning Theory arguably being the most comprehensive practical approach. In hydrology, complexity control has hardly been used so far. There are a number of reasons for that lack of interest, the more valid ones of which will be presented during the presentation. For starters, there are no readily available complexity <span class="hlt">measures</span> for our <span class="hlt">models</span>. Second, some unrealistic simplifications of the underlying complex physics tend to have a smoothing effect on possible <span class="hlt">model</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFMSH42A..06S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFMSH42A..06S"><span><span class="hlt">Modeling</span> Spectral Turnovers in Interplanetary Shocks <span class="hlt">Observed</span> by ULYSSES</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Summerlin, E. J.; Baring, M. G.</p> <p>2009-12-01</p> <p>Interplanetary shocks in the heliosphere provide excellent test cases for the simulation and theory of particle acceleration at shocks thanks to the presence of in-situ <span class="hlt">measurements</span> and a relatively well understood initial particle distribution. The Monte-Carlo test particle simulation employed in this work has been previously used to study injection and acceleration from thermal energies into the high energy power-law tail at co-rotating interaction regions (CIRs) in the heliosphere presuming a steady state planar shock (Summerlin & Baring, 2006, Baring and Summerlin, 2008). These simulated power-spectra compare favorably with in-situ <span class="hlt">measurements</span> from the ULYSSES spacecraft below 60 keV. However, to effectively <span class="hlt">model</span> the high energy exponential cutoff at energies above 60 keV <span class="hlt">observed</span> in these distributions, simulations must apply spatial or temporal constraints to the acceleration process. This work studies the effects of a variety of temporal and spatial co! nstraints (including spatial constraints on the turbulent region around the shock as determined by magnetometer data, spatial constraints related to the scale size of the shock and constraints on the acceleration time based on the known limits for the shock's lifetime) on the high energy cut-off and compares simulated particle spectra to those <span class="hlt">observed</span> by the ULYSSES HI-SCALE instrument in an effort to determine which constraint is creating the cut-off and using that constraining parameter to determine additional information about the shock that can not, normally, be determined by a single data point, such as the spatial extent of the shock or how long the shock has been propagating through the heliosphere before it encounters the spacecraft. Shocks <span class="hlt">observed</span> by multiple spacecraft will be of particular interest as their parameters will be better constrained than shocks <span class="hlt">observed</span> by only one spacecraft. To achieve these goals, the simulation will be modified to include the re! trodictive approach of Jones</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5432377','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5432377"><span><span class="hlt">Model</span> based inference from microvascular <span class="hlt">measurements</span>: Combining experimental <span class="hlt">measurements</span> and <span class="hlt">model</span> predictions using a Bayesian probabilistic approach</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Rasmussen, Peter M.; Smith, Amy F.; Sakadžić, Sava; Boas, David A.; Pries, Axel R.; Secomb, Timothy W.; Østergaard, Leif</p> <p>2017-01-01</p> <p>Objective In vivo imaging of the microcirculation and network-oriented <span class="hlt">modeling</span> have emerged as powerful means of studying microvascular function and understanding its physiological significance. Network-oriented <span class="hlt">modeling</span> may provide the means of summarizing vast amounts of data produced by high-throughput imaging techniques in terms of key, physiological indices. To estimate such indices with sufficient certainty, however, network-oriented analysis must be robust to the inevitable presence of uncertainty due to <span class="hlt">measurement</span> errors as well as <span class="hlt">model</span> errors. Methods We propose the Bayesian probabilistic data analysis framework as a means of integrating experimental <span class="hlt">measurements</span> and network <span class="hlt">model</span> simulations into a combined and statistically coherent analysis. The framework naturally handles noisy <span class="hlt">measurements</span> and provides posterior distributions of <span class="hlt">model</span> parameters as well as physiological indices associated with uncertainty. Results We applied the analysis framework to experimental data from three rat mesentery networks and one mouse brain cortex network. We inferred distributions for more than five hundred unknown pressure and hematocrit boundary conditions. <span class="hlt">Model</span> predictions were consistent with previous analyses, and remained robust when <span class="hlt">measurements</span> were omitted from <span class="hlt">model</span> calibration. Conclusion Our Bayesian probabilistic approach may be suitable for optimizing data acquisition and for analyzing and reporting large datasets acquired as part of microvascular imaging studies. 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