Sample records for solar system observations

  1. Solar System Observations with JWST

    NASA Technical Reports Server (NTRS)

    Norwood, James; Hammel, Heidi; Milam, Stefanie; Stansberry, John; Lunine, Jonathan; Chanover, Nancy; Hines, Dean; Sonneborn, George; Tiscareno, Matthew; Brown, Michael; hide

    2014-01-01

    The James Webb Space Telescope will enable a wealth of new scientific investigations in the near- and mid- infrared, with sensitivity and spatial-spectral resolution greatly surpassing its predecessors. In this paper, we focus upon Solar System science facilitated by JWST, discussing the most current information available concerning JWST instrument properties and observing techniques relevant to planetary science. We also present numerous example observing scenarios for a wide variety of Solar System targets to illustrate the potential of JWST science to the Solar System community. This paper updates and supersedes the Solar System white paper published by the JWST Project in 2010 (Lunine et al., 2010). It is based both on that paper and on a workshop held at the annual meeting of the Division for Planetary Sciences in Reno, NV in 2012.

  2. Chandra Observations of the Solar System

    NASA Astrophysics Data System (ADS)

    Lisse, Carey

    2014-11-01

    Many solar system objects are now known to emit X-rays due to charge-exchange between highly charged solar wind (SW) minor ions and neutrals in their extended atmospheres, including Earth, Venus, Mars, Jupiter, and the heliosphere, with total power outputs on the MW - GW scale. (Currently only upper limits exist for Saturn and Pluto.) Chandra observations of their morphology, spectra, and time dependence provide important information about the neutral atmosphere structure and the SW flux and charge state. Chandra observations of solar x-ray scattering from Earth, Venus, Mars, Jupiter, Saturn, and the Moon have also provided important clues for the scattering material and the solar radiation field at the body. We present here a 15 year summary of Chandra's solar system observations.

  3. Solar System Observations with the James Webb Space Telescope

    NASA Technical Reports Server (NTRS)

    Norwood, James; Hammel, Heidi; Milam, Stefanie; Stansberry, John; Lunine, Jonathan; Chanover, Nancy; Hines, Dean; Sonneborn, George; Tiscareno, Matthew; Brown, Michael; hide

    2016-01-01

    The James Webb Space Telescope (JWST) will enable a wealth of new scientific investigations in the near- and mid-infrared, with sensitivity and spatial/spectral resolution greatly surpassing its predecessors. In this paper, we focus upon Solar System science facilitated by JWST, discussing the most current information available concerning JWST instrument properties and observing techniques relevant to planetary science. We also present numerous example observing scenarios for a wide variety of Solar System targets to illustrate the potential of JWST science to the Solar System community. This paper updates and supersedes the Solar System white paper published by the JWST Project in 2010. It is based both on that paper and on a workshop held at the annual meeting of the Division for Planetary Sciences in Reno, NV, in 2012.

  4. Continued Analysis of EUVE Solar System Observations

    NASA Technical Reports Server (NTRS)

    Gladstone, G. Randall

    2001-01-01

    This is the final report for this project. We proposed to continue our work on extracting important results from the EUVE (Extreme UltraViolet Explorer) archive of lunar and jovian system observations. In particular, we planned to: (1) produce several monochromatic images of the Moon at the wavelengths of the brightest solar EUV emission lines; (2) search for evidence of soft X-ray emissions from the Moon and/or X-ray fluorescence at specific EUV wavelengths; (3) search for localized EUV and soft X-ray emissions associated with each of the Galilean satellites; (4) search for correlations between localized Io Plasma Torus (IPT) brightness and volcanic activity on Io; (5) search for soft X-ray emissions from Jupiter; and (6) determine the long term variability of He 58.4 nm emissions from Jupiter, and relate these to solar variability. However, the ADP review panel suggested that the work concentrate on the Jupiter/IPT observations, and provided half the requested funding. Thus we have performed no work on the first two tasks, and instead concentrated on the last three. In addition we used funds from this project to support reduction and analysis of EUVE observations of Venus. While this was not part of the original statement of work, it is entirely in keeping with extracting important results from EUVE solar system observations.

  5. OBSERVATIONS OF HIERARCHICAL SOLAR-TYPE MULTIPLE STAR SYSTEMS

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

    Roberts, Lewis C. Jr.; Tokovinin, Andrei; Mason, Brian D.

    2015-10-15

    Twenty multiple stellar systems with solar-type primaries were observed at high angular resolution using the PALM-3000 adaptive optics system at the 5 m Hale telescope. The goal was to complement the knowledge of hierarchical multiplicity in the solar neighborhood by confirming recent discoveries by the visible Robo-AO system with new near-infrared observations with PALM-3000. The physical status of most, but not all, of the new pairs is confirmed by photometry in the Ks band and new positional measurements. In addition, we resolved for the first time five close sub-systems: the known astrometric binary in HIP 17129AB, companions to the primariesmore » of HIP 33555, and HIP 118213, and the companions to the secondaries in HIP 25300 and HIP 101430. We place the components on a color–magnitude diagram and discuss each multiple system individually.« less

  6. JWST Planetary Observations Within the Solar System

    NASA Technical Reports Server (NTRS)

    Lunine, Jonathan; Hammel, Heidi; Schaller, Emily; Sonneborn, George; Orton, Glenn; Rieke, George; Rieke, Marcia

    2010-01-01

    JWST provides capabilities unmatched by other telescopic facilities in the near to mid infrared part of the electromagnetic spectrum. Its combination of broad wavelength range, high sensitivity and near diffraction-limited imaging around two microns wavelength make it a high value facility for a variety of Solar System targets. Beyond Neptune, a class of cold, large bodies that include Pluto, Triton and Eris exhibits surface deposits of nitrogen, methane, and other molecules that are poorly observed from the ground, but for which JWST might provide spectral mapping at high sensitivity and spatial resolution difficult to match with the current generation of ground-based observatories. The observatory will also provide unique sensitivity in a variety of near and mid infrared windows for observing relatively deep into the atmospheres of Uranus and Neptune, searching there for minor species. It will examine the Jovian aurora in a wavelength regime where the background atmosphere is dark. Special provision of a subarray observing strategy may allow observation of Jupiter and Saturn over a larger wavelength range despite their large surface brightnesses, allowing for detailed observation of transient phenomena including large scale storms and impact-generation disturbances. JWST's observations of Saturn's moon Titan will overlap with and go beyond the 2017 end-of-mission for Cassini, providing an important extension to the time-series of meteorological studies for much of northern hemisphere summer. It will overlap with a number of other planetary missions to targets for which JWST can make unique types of observations. JWST provides a platform for linking solar system and extrasolar planet studies through its unique observational capabilities in both arenas.

  7. What Do Millimeter Continuum and Spectral Line Observations Tell Us about Solar System Bodies?

    NASA Technical Reports Server (NTRS)

    Milam, Stefanie N.

    2013-01-01

    Solar system objects are generally cold and radiate at low frequencies and tend to have strong molecular rotational transitions. Millimeter continuum and spectral line observations provide detailed information for nearly all solar system bodies. At these wavelengths, details of the bulk physical composition of icy surfaces, the size and albedo of small objects, the composition of planetary atmospheres can be measured as well as monitoring of time variable phenomena for extended periods (not restricted to nighttime observations), etc. Major issues in solar system science can be addressed by observations in the millimeter/sub-millimeter regime such as the origin of the solar system (isotope ratios, composition) and the evolution of solar system objects (dynamics, atmospheric constituents, etc). ALMA s exceptional sensitivity, large spectral bandwidth, high spectral resolution, and angular resolution (down to 10 milliarcsec) will enable researchers for the first time to better resolve the smallest bodies in the solar system and provide detailed maps of the larger objects. Additionally, measurements with nearly 8 GHz of instantaneous bandwidth to fully characterize solar system object s spectrum and detect trace species. The spatial information and line profiles can be obtained over 800 GHz of bandwidth in 8 receiver bands to not only assist in the identification of spectral lines and emission components for a given species but also to help elucidate the chemistry of the extraterrestrial bodies closest to us.

  8. Solar system plasma Turbulence: Observations, inteRmittency and Multifractals

    NASA Astrophysics Data System (ADS)

    Echim, Marius M.

    2016-04-01

    The FP7 project STORM is funded by the European Commission to "add value to existing data bases through a more comprehensive interpretation". STORM targets plasma and magnetic field databases collected in the solar wind (Ulysses and also some planetary missions), planetary magnetospheres (Venus Express, Cluster, a few orbits from Cassini), cometary magnetosheaths (e.g. Haley from Giotto observations). The project applies the same package of analysis methods on geomagnetic field observations from ground and on derived indices (e.g. AE, AL, AU, SYM-H). The analysis strategy adopted in STORM is built on the principle of increasing complexity, from lower (like, e.g., the Power Spectral Density - PSD) to higher order analyses (the Probability Distribution Functions - PDFs, Structure Functions - SFs, Fractals and Multifractals - MFs). Therefore STORM targets not only the spectral behavior of turbulent fluctuations but also their topology and scale behavior inferred from advanced mathematical algorithms and geometrical-like analogs. STORM started in January 2013 and ended in December 2015. We will report on a selection of scientific and technical achievements and will highlight: (1) the radial evolution of solar wind turbulence and intermittency based on Ulysses data with some contributions from Venus Express and Cluster; (2) comparative study of fast and slow wind turbulence and intermittency at solar minimum; (3) comparative study of the planetary response (Venus and Earth magnetosheaths) to turbulent solar wind; (4) the critical behavior of geomagnetic fluctuations and indices; (5) an integrated library for non-linear analysis of time series that includes all the approaches adopted in STORM to investigate solar system plasma turbulence. STORM delivers an unprecedented volume of analysed data for turbulence. The project made indeed a systematic survey, orbit by orbit, of data available from ESA repositories and Principal Investigators and provides results ordered as a

  9. Solar System Observing with the Space Infrared Telescope Facility (SIRTF)

    NASA Technical Reports Server (NTRS)

    Cleve, J. Van; Meadows, V. S.; Stansberry, J.

    2003-01-01

    SIRTF is NASA's Space Infrared Telescope Facility. Currently planned for launch on 15 Apr 2003, it is the final element in NASA's Great Observatories Program. SIRTF has an 85 cm diameter f/12 lightweight beryllium telescope, cooled to lekss than 5.5K. It is diffraction-limited at 6.5 microns, and has wavelengthcoverage from 3-180 microns. Its estimated lifetime (limited by cryogen) is 2.5 years at minimum, with a goal of 5+ years. SIRTF has three instruments, IRAC, IRS, and MIPS. IRAC (InfraRed Array Camera) provides simultaneous images at wavelengths of 3.6, 4.5, 5.8, and 8.0 microns. IRS (InfraRed Spectrograph) has 4 modules providing low-resolution (R=60-120) spectra from 5.3 to 40 microns, high-resolution (R=600) spectra from 10 to 37 microns, and an autonomous target acquisition system (PeakUp) which includes small-field imaging at 15 microns. MIPS (Multiband Imaging Photometer for SIRTF)} does imaging photometry at 24, 70, and 160 m and low-resolution (R=15-25) spectroscopy (SED) between 55 and 96 microns. The SIRTF Guaranteed Time Observers (GTOs) are planning to observe Outer Solar System satellites and planets, extinct comets and low-albedo asteroids, Centaurs and Kuiper Belt Objects, cometary dust trails, and a few active short-period comets. The GTO programs are listed in detail in the SIRTF Reserved Observations Catalog (ROC). We would like to emphasize that there remain many interesting subjects for the General Observers (GO). Proposal success for the planetary observer community in the first SIRTF GO proposal cycle (GO-1) determines expectations for future GO calls and Solar System use of SIRTF, so we would like promote a strong set of planetary GO-1 proposals. Towards that end, we present this poster, and we will convene a Solar System GO workshop 3.5 months after launch.

  10. Terahertz photometers to observe solar flares from space (SOLAR-T project)

    NASA Astrophysics Data System (ADS)

    Kaufmann, Pierre; Raulin, Jean-Pierre

    The space experiment SOLAR-T designed to observe solar flares at THz frequencies was completed. We present the concept, fabrication and performance of a double THz photometers system. An innovative optical setup allows observations of the full solar disk and the detection of small burst transients at the same time. It is the first detecting system conceived to observe solar flare THz emissions on board of stratospheric balloons. The system has been integrated to data acquisition and telemetry modules for this application. SOLAR-T uses two Golay cell detectors preceded by low-pass filters made of rough surface primary mirrors and membranes, 3 and 7 THz band-pass filters, and choppers. Its photometers can detect small solar bursts (tens of solar flux units) with sub second time resolution. One artificial Sun setup was developed to simulate actual observations. Tests comprised the whole system performance, on ambient and low pressure and temperature conditions. It is intended to provide data on the still unrevealed spectral shape of the mysterious THz solar flares emissions. The experiment is planned to be on board of two long-duration stratospheric balloon flights over Antarctica and Russia in 2014-2016. The SOLAR-T development, fabrication and tests has been accomplished by engineering and research teams from Mackenzie, Unicamp and Bernard Lyot Solar Observatory; Propertech Ltda.; Neuron Ltda.; and Samsung, Brazil; Tydex LCC, Russia; CONICET, Argentina; the stratospheric balloon missions will be carried in cooperation with teams from University of California, Berkeley, USA (flight over Antarctica), and Lebedev Physical Institute, Moscow, Russia (flight over Russia).

  11. Local tests of gravitation with Gaia observations of Solar System Objects

    NASA Astrophysics Data System (ADS)

    Hees, Aurélien; Le Poncin-Lafitte, Christophe; Hestroffer, Daniel; David, Pedro

    2018-04-01

    In this proceeding, we show how observations of Solar System Objects with Gaia can be used to test General Relativity and to constrain modified gravitational theories. The high number of Solar System objects observed and the variety of their orbital parameters associated with the impressive astrometric accuracy will allow us to perform local tests of General Relativity. In this communication, we present a preliminary sensitivity study of the Gaia observations on dynamical parameters such as the Sun quadrupolar moment and on various extensions to general relativity such as the parametrized post-Newtonian parameters, the fifth force formalism and a violation of Lorentz symmetry parametrized by the Standard-Model extension framework. We take into account the time sequences and the geometry of the observations that are particular to Gaia for its nominal mission (5 years) and for an extended mission (10 years).

  12. The Trojan-Hilda-KBO connection: An observational test of solar system evolution models

    NASA Astrophysics Data System (ADS)

    Wong, Ian; Brown, Michael

    2017-10-01

    Over the past few decades, many theories have been devised to explain the observed solar system architecture. The current paradigm posits that a significant reorganization of the outer Solar System occurred after the end of planet formation. Specifically, it is hypothesized that Jupiter and Saturn crossed a mutual mean motion resonance, leading to a chaotic expansion of the ice giants’ orbits that disrupted the large population of planetesimals situated further out. While the majority of these bodies were ejected from the Solar System, a fraction of them were retained as the present-day Kuiper Belt, while others were scattered inward and captured into resonances with Jupiter to become the Trojans and Hildas. Dynamical instability models invariably predict that Trojans, Hildas, and Kuiper Belt objects (KBOs) were sourced from the same primordial body of outer solar system planetesimals. Therefore, comparison of these minor body populations serves as one of the few available observational tests of our present understanding of solar system evolution.We present the results of a series of studies aimed at synthesizing a detailed picture of Trojans and related asteroid populations. By combining analyses of archival data with new photometric surveys, we have derived the first debiased color distributions of Trojans and KBOs and extended/refined our knowledge of their respective size distributions. In addition, we have explored the peculiar color bimodality attested in the Trojans, Hildas, and KBOs, which indicates the presence of two sub-populations. As part of our continuing efforts to characterize the surface composition of these bodies, we have also obtained new near-infrared spectra of Hildas for comparison with previously published spectra of Trojans covering the same wavelength region. We have utilized the full body of observations to formulate hypotheses regarding the formation, composition, and dynamical/chemical evolution of the primordial outer solar system

  13. The Trojan-Hilda-KBO connection: An observational test of solar system evolution models

    NASA Astrophysics Data System (ADS)

    Wong, I.; Brown, M. E.

    2017-12-01

    Over the past few decades, many theories have been devised to explain the observed solar system architecture. The current paradigm posits that a significant reorganization of the outer Solar System occurred after the end of planet formation. Specifically, it is hypothesized that Jupiter and Saturn crossed a mutual mean motion resonance, leading to a chaotic expansion of the ice giants' orbits that disrupted the large population of planetesimals situated further out. While the majority of these bodies were ejected from the Solar System, a fraction of them were retained as the present-day Kuiper Belt, while others were scattered inward and captured into resonances with Jupiter to become the Trojans and Hildas. Dynamical instability models invariably predict that Trojans, Hildas, and Kuiper Belt objects (KBOs) were sourced from the same primordial body of outer solar system planetesimals. Therefore, comparison of these minor body populations serves as one of the few available observational tests of our present understanding of solar system evolution. We present the results of a series of studies aimed at synthesizing a detailed picture of Trojans and related asteroid populations. By combining analyses of archival data with new photometric surveys, we have derived the first debiased color distributions of Trojans and KBOs and extended/refined our knowledge of their respective size distributions. In addition, we have explored the peculiar color bimodality attested in the Trojans, Hildas, and KBOs, which indicates the presence of two sub-populations. As part of our continuing efforts to characterize the surface composition of these bodies, we have also obtained new near-infrared spectra of Hildas for comparison with previously published spectra of Trojans covering the same wavelength region. We have utilized the full body of observations to formulate hypotheses regarding the formation, composition, and dynamical/chemical evolution of the primordial outer solar system

  14. Exploring our outer solar system - The Giant Planet System Observers

    NASA Astrophysics Data System (ADS)

    Cooper, J. F.; Sittler, E. C., Jr.; Sturner, S. J.; Pitman, J. T.

    As space-faring peoples now work together to plan and implement future missions that robotically prepare for landing humans to explore the Moon, and later Mars, the time is right to develop evolutionary approaches for extending this next generation of exploration beyond Earth's terrestrial planet neighbors to the realm of the giant planets. And while initial fly-by missions have been hugely successful in providing exploratory surveys of what lies beyond Mars, we need to consider now what robotic precursor mission capabilities we need to emplace that prepare us properly, and comprehensively, for long-term robotic exploration, and eventual human habitation, beyond Mars to the outer reaches of our solar system. To develop practical strategies that can establish prioritized capabilities, and then develop a means for achieving those capabilities within realistic budget and technology considerations, and in reasonable timeframes, is our challenge. We suggest one component of such an approach to future outer planets exploration is a series of Giant Planets System Observer (GPSO) missions that provide for long- duration observations, monitoring, and relay functions to help advance our understanding of the outer planets and thereby enable a sound basis for planning their eventual exploration by humans. We envision these missions as being comparable to taking Hubble-class remote-sensing facilities, along with the space physics capabilities of long-lived geospace and heliospheric missions, to the giant planet systems and dedicating long observing lifetimes (HST, 16 yr.; Voyagers, 29 yr.) to the exhaustive study and characterization of those systems. GPSO missions could feature 20-yr+ extended mission lifetimes, direct inject trajectories to maximize useful lifetime on target, placement strategies that take advantage of natural environment shielding (e.g., Ganymede magnetic field) where possible, orbit designs having favorable planetary system viewing geometries, comprehensive

  15. Suzaku Observations of Charge Exchange Emission from Solar System Objects

    NASA Technical Reports Server (NTRS)

    Ezoe, Y.; Fujimoto, R.; Yamasaki, N. Y.; Mitsuda, K.; Ohashi, T.; Ishikawa, K.; Oishi, S.; Miyoshi, Y; Terada, N.; Futaana, Y.; hide

    2012-01-01

    Recent results of charge exchange emission from solar system objects observed with the Japanese Suzaku satellite are reviewed. Suzaku is of great importance to investigate diffuse X-ray emission like the charge exchange from planetary exospheres and comets. The Suzaku studies of Earth's exosphere, Martian exosphere, Jupiter's aurorae, and comets are overviewed.

  16. Observed ices in the Solar System

    USGS Publications Warehouse

    Clark, Roger N.; Grundy, Will; Carlson, Robert R.; Noll, Keith; Gudipati, Murthy; Castillo-Rogez, Julie C.

    2013-01-01

    Ices have been detected and mapped on the Earth and all planets and/or their satellites further from the sun. Water ice is the most common frozen volatile observed and is also unambiguously detected or inferred in every planet and/or their moon(s) except Venus. Carbon dioxide is also extensively found in all systems beyond the Earth except Pluto although it sometimes appears to be trapped rather than as an ice on some objects. The largest deposits of carbon dioxide ice is on Mars. Sulfur dioxide ice is found in the Jupiter system. Nitrogen and methane ices are common beyond the Uranian system. Saturn’s moon Titan probably has the most complex active chemistry involving ices, with benzene (C6H6) and many tentative or inferred compounds including ices of Cyanoacetylene (HC3N), Toluene (C7H8), Cyanogen (C2N2), Acetonitrile (CH3CN), H2O, CO2, and NH3. Confirming compounds on Titan is hampered by its thick smoggy atmosphere. Ammonia was predicted on many icy moons but is notably absent among the definitively detected ices with the possible exception of Enceladus. Comets, storehouses of many compounds that could exist as ices in their nuclei, have only had small amounts of water ice definitively detected on their surfaces. Only one asteroid has had a direct detection of surface water ice, although its presence can be inferred in others. This chapter reviews some of the properties of ices that lead to their detection, and surveys the ices that have been observed on solid surfaces throughout the Solar System.

  17. Interstellar Explorer Observations of the Solar System's Debris Disks

    NASA Astrophysics Data System (ADS)

    Lisse, C. M.; McNutt, R. L., Jr.; Brandt, P. C.

    2017-12-01

    Planetesimal belts and debris disks full of dust are known as the "signposts of planet formation" in exosystems. The overall brightness of a disk provides information on the amount of sourcing planetesimal material, while asymmetries in the shape of the disk can be used to search for perturbing planets. The solar system is known to house two such belts, the Asteroid belt and the Kuiper Belt; and at least one debris cloud, the Zodiacal Cloud, sourced by planetisimal collisions and Kuiper Belt comet evaporative sublimation. However these are poorly understood in toto because we live inside of them. E.g., while we know of the two planetesimal belt systems, it is not clear how much, if any, dust is produced from the Kuiper belt since the near-Sun comet contributions dominate near-Earth space. Understanding how much dust is produced in the Kuiper belt would give us a much better idea of the total number of bodies in the belt, especially the smallest ones, and their dynamical collisional state. Even for the close in Zodiacal cloud, questions remain concerning its overall shape and orientation with respect to the ecliptic and invariable planes of the solar system - they aren't explainable from the perturbations caused by the known planets alone. In this paper we explore the possibilities of using an Interstellar Explorer telescope placed at 200 AU from the sun to observe the brightness, shape, and extent of the solar system's debris disk(s). We should be able to measure the entire extent of the inner, near-earth zodiacal cloud; whether it connects smoothly into an outer cloud, or if there is a second outer cloud sourced by the Kuiper belt and isolated by the outer planets, as predicted by Stark & Kuchner (2009, 2010) and Poppe et al. (2012, 2016; Figure 1). VISNIR imagery will inform about the dust cloud's density, while MIR cameras will provide thermal imaging photometry related to the cloud's dust particle size and composition. Observing at high phase angle by looking

  18. Polarimetry of Solar System Objects: Observations vs. Models

    NASA Astrophysics Data System (ADS)

    Yanamandra-Fisher, P. A.

    2014-04-01

    The overarching goals for the remote sensing and robotic exploration of planetary systems are: (1) understanding the formation of planetary systems and their diversity; and (2) search for habitability. Since all objects have unique polarimetric signatures inclusion of spectrophotopolarimetry as a complementary approach to standard techniques of imaging and spectroscopy, provides insight into the scattering properties of the planetary media. Specifically, linear and circular polarimetric signatures of the object arise from different physical processes and their study proves essential to the characterization of the object. Linear polarization of reflected light by various solar system objects provides insight into the scattering characteristics of atmospheric aerosols and hazes? and surficial properties of atmosphereless bodies. Many optically active materials are anisotropic and so their scattering properties differ with the object's principal axes (such as dichroic or birefringent materials) and are crystalline in structure instead of amorphous, (eg., the presence of olivines and silicates in cometary dust and circumstellar disks? Titan, etc.). Ices (water and other species) are abundant in the system indicated in their near - infrared spectra. Gas giants form outside the frost line (where ices condense), and their satellites and ring systems exhibit signature of water ice? clathrates, nonices (Si, C, Fe) in their NIR spectra and spectral dependence of linear polarization. Additionally, spectral dependence of polarization is important to separate the macroscopic (bulk) properties of the scattering medium from the microscopic (particulate) properties of the scattering medium. Circular polarization, on the other hand, is indicative of magnetic fields and biologically active molecules, necessary for habitability. These applications suffer from lack of detailed observations, instrumentation, dedicated missions and numericalretrieval methods. With recent discoveries and

  19. Recent Variability Observations of Solar System Giant Planets: Fresh Context for Understanding Exoplanet and Brown Dwarf Weather

    NASA Astrophysics Data System (ADS)

    Marley, Mark S.; Kepler Giant Planet Variability Team, Spitzer Ice Giant Variability Team

    2016-10-01

    Over the past several years a number of of high cadence photometric observations of solar system giant planets have been acquired by various platforms. Such observations are of interest as they provide points of comparison to the already expansive set of brown dwarf variability observations and the small, but growing, set of exoplanet variability observations. By measuring how rapidly the integrated light from solar system giant planets can evolve, variability observations of substellar objects that are unlikely to ever be resolved can be placed in a fuller context. Examples of brown dwarf variability observations include extensive work from the ground (e.g., Radigan et al. 2014), Spitzer (e.g., Metchev et al. 2015), Kepler (Gizis et al. 2015), and HST (Yang et al. 2015). Variability has been measured on the planetary mass companion to the brown dwarf 2MASS 1207b (Zhou et al. 2016) and further searches are planned in thermal emission for the known directly imaged planets with ground based telescopes (Apai et al. 2016) and in reflected light with future space based telescopes. Recent solar system variability observations include Kepler monitoring of Neptune (Simon et al. 2016) and Uranus, Spitzer observations of Neptune (Stauffer et al. 2016), and Cassini observations of Jupiter (West et al. in prep). The Cassini observations are of particular interest as they measured the variability of Jupiter at a phase angle of ˜60○, comparable to the viewing geometry expected for space based direct imaging of cool extrasolar Jupiters in reflected light. These solar system analog observations capture many of the characteristics seen in brown dwarf variability, including large amplitudes and rapid light curve evolution on timescales as short as a few rotation periods. Simon et al. (2016) attribute such variations at Neptune to a combination of large scale, stable cloud structures along with smaller, more rapidly varying, cloud patches. The observed brown dwarf and exoplanet

  20. Recent Variability Observations of Solar System Giant Planets: Fresh Context for Understanding Exoplanet and Brown Dwarf Weather

    NASA Technical Reports Server (NTRS)

    Marley, Mark Scott

    2016-01-01

    Over the past several years a number of high cadence photometric observations of solar system giant planets have been acquired by various platforms. Such observations are of interest as they provide points of comparison to the already expansive set of brown dwarf variability observations and the small, but growing, set of exoplanet variability observations. By measuring how rapidly the integrated light from solar system giant planets can evolve, variability observations of substellar objects that are unlikely to ever be resolved can be placed in a fuller context. Examples of brown dwarf variability observations include extensive work from the ground (e.g., Radigen et al. 2014), Spitzer (e.g., Metchev et al. 2015), Kepler (Gizis et al. 2015), and HST (Yang et al. 2015).Variability has been measured on the planetary mass companion to the brown dwarf 2MASS 1207b (Zhou et al. 2016) and further searches are planned in thermal emission for the known directly imaged planets with ground based telescopes (Apai et al. 2016) and in reflected light with future space based telescopes. Recent solar system variability observations include Kepler monitoring of Neptune (Simon et al. 2016) and Uranus, Spitzer observations of Neptune (Stauffer et al. 2016), and Cassini observations of Jupiter (West et al. in prep). The Cassini observations are of particular interest as they measured the variability of Jupiter at a phase angle of approximately 60 deg, comparable to the viewing geometry expected for space based direct imaging of cool extrasolar Jupiters in reflected light. These solar system analog observations capture many of the characteristics seen in brown dwarf variability, including large amplitudes and rapid light curve evolution on timescales as short as a few rotation periods. Simon et al. (2016) attribute such variations at Neptune to a combination of large scale, stable cloud structures along with smaller, more rapidly varying, cloud patches. The observed brown dwarf and

  1. An Airborne Infrared Spectrometer for Solar Eclipse Observations

    NASA Astrophysics Data System (ADS)

    Samra, Jenna; DeLuca, Edward E.; Golub, Leon; Cheimets, Peter; Philip, Judge

    2016-05-01

    The airborne infrared spectrometer (AIR-Spec) is an innovative solar spectrometer that will observe the 2017 solar eclipse from the NSF/NCAR High-Performance Instrumented Airborne Platform for Environmental Research (HIAPER). AIR-Spec will image five infrared coronal emission lines to determine whether they may be useful probes of coronal magnetism.The solar magnetic field provides the free energy that controls coronal heating, structure, and dynamics. Energy stored in coronal magnetic fields is released in flares and coronal mass ejections and ultimately drives space weather. Therefore, direct coronal field measurements have significant potential to enhance understanding of coronal dynamics and improve solar forecasting models. Of particular interest are observations of field lines in the transitional region between closed and open flux systems, providing important information on the origin of the slow solar wind.While current instruments routinely observe only the photospheric and chromospheric magnetic fields, AIR-Spec will take a step toward the direct observation of coronal fields by measuring plasma emission in the infrared at high spatial and spectral resolution. During the total solar eclipse of 2017, AIR-Spec will observe five magnetically sensitive coronal emission lines between 1.4 and 4 µm from the HIAPER Gulfstream V at an altitude above 14.9 km. The instrument will measure emission line intensity, width, and Doppler shift, map the spatial distribution of infrared emitting plasma, and search for waves in the emission line velocities.AIR-Spec consists of an optical system (feed telescope, grating spectrometer, and infrared detector) and an image stabilization system, which uses a fast steering mirror to correct the line-of-sight for platform perturbations. To ensure that the instrument meets its research goals, both systems are undergoing extensive performance modeling and testing. These results are shown with reference to the science requirements.

  2. K2 & Solar System Science

    NASA Technical Reports Server (NTRS)

    Lissauer, Jack

    2015-01-01

    All of the fields that K2 observes are near the ecliptic plane in order to minimize the spin-up of the spacecraft in response to the effects of solar irradiation. The fields observed by K2 are thus rich in Solar System objects including planets, asteroids and trans-Neptunian objects (TNOs). K2 has already performed observations of Neptune and its large moon Triton, 68 Trojan and Hilda asteroids, 5 TNOs (including Pluto) and Comet C/2013 A1 (Siding Springs). About 10,000 main-belt asteroids that fell into the pixel masks of stars have been serendipitously observed. Observations of small bodies are especially useful for determining rotation periods. Uranus will be observed in a future campaign (C8), as will many more small Solar System bodies. The status of various K2 Solar System studies will be reviewed and placed within the context of our current knowledge of the objects being observed.

  3. GAP: yet another image processing system for solar observations.

    NASA Astrophysics Data System (ADS)

    Keller, C. U.

    GAP is a versatile, interactive image processing system for analyzing solar observations, in particular extended time sequences, and for preparing publication quality figures. It consists of an interpreter that is based on a language with a control flow similar to PASCAL and C. The interpreter may be accessed from a command line editor and from user-supplied functions, procedures, and command scripts. GAP is easily expandable via external FORTRAN programs that are linked to the GAP interface routines. The current version of GAP runs on VAX, DECstation, Sun, and Apollo computers. Versions for MS-DOS and OS/2 are in preparation.

  4. Solar Observations with ALMA

    NASA Astrophysics Data System (ADS)

    Wedemeyer, Sven

    2018-04-01

    The continuum intensity at millimeter wavelengths can serve as an essentially linear thermometer of the plasma in a thin layer in the atmosphere of the Sun, whereas the polarisation of the received radiation is a measure for the longitudinal magnetic field component in the same layer. The enormous leap in terms of spatial resolution with the Atacama Large Millimeter/submillimeter Array (ALMA) now makes it possible to observe the intricate fine-structure of the solar atmosphere at sufficiently high spatial, temporal, and spectral resolution, thus enabling studies of a wide range of scientific topics in solar physics that had been inaccessible at millimeter wavelengths before. The radiation observed by ALMA originates mostly from the chromosphere - a complex and dynamic layer between the photosphere and corona, which plays a crucial role in the transport of energy and matter and, ultimately, the heating of the outer solar atmosphere. ALMA observations of the solar chromosphere, which are offered as a regular capability since 2016, therefore have the potential to make important contributions towards the solution of fundamental questions in solar physics with implications for our understanding of stars in general. In this presentation, I will give a short description of ALMA's solar observing mode, it challenges and opportunities, and selected science cases in combination with numerical simulations and coordinated observations at other wavelengths. ALMA's scientific potential for studying the dynamic small-scale pattern of the solar chromosphere is illustrated with first results from Cycle 4.

  5. Long-term solar-terrestrial observations

    NASA Technical Reports Server (NTRS)

    1988-01-01

    The results of an 18-month study of the requirements for long-term monitoring and archiving of solar-terrestrial data is presented. The value of long-term solar-terrestrial observations is discussed together with parameters, associated measurements, and observational problem areas in each of the solar-terrestrial links (the sun, the interplanetary medium, the magnetosphere, and the thermosphere-ionosphere). Some recommendations are offered for coordinated planning for long-term solar-terrestrial observations.

  6. Our Solar System, from the Outside

    NASA Image and Video Library

    2011-04-28

    This graphic, based on data from NASA Voyager spacecraft, shows a model of what our solar system looks like to an observer outside in interstellar space, watching our solar system fly towards the observer.

  7. Development of the prototype data management system of the solar H-alpha full disk observation

    NASA Astrophysics Data System (ADS)

    Wei, Ka-Ning; Zhao, Shi-Qing; Li, Qiong-Ying; Chen, Dong

    2004-06-01

    The Solar Chromospheric Telescope in Yunnan Observatory generates about 2G bytes fits format data per day. Huge amounts of data will bring inconvenience for people to use. Hence, data searching and sharing are important at present. Data searching, on-line browsing, remote accesses and download are developed with a prototype data management system of the solar H-alpha full disk observation, and improved by the working flow technology. Based on Windows XP operating system and MySQL data management system, a prototype system of browse/server model is developed by JAVA and JSP. Data compression, searching, browsing, deletion need authority and download in real-time have been achieved.

  8. Ion Acceleration in Solar Flares Determined by Solar Neutron Observations

    NASA Astrophysics Data System (ADS)

    Watanabe, K.; Solar Neutron Observation Group

    2013-05-01

    Large amounts of particles can be accelerated to relativistic energy in association with solar flares and/or accompanying phenomena (e.g., CME-driven shocks), and they sometimes reach very near the Earth and penetrate the Earth's atmosphere. These particles are observed by ground-based detectors (e.g., neutron monitors) as Ground Level Enhancements (GLEs). Some of the GLEs originate from high energy solar neutrons which are produced in association with solar flares. These neutrons are also observed by ground-based neutron monitors and solar neutron telescopes. Recently, some of the solar neutron detectors have also been operating in space. By observing these solar neutrons, we can obtain information about ion acceleration in solar flares. Such neutrons were observed in association with some X-class flares in solar cycle 23, and sometimes they were observed by two different types of detectors. For example, on 2005 September 7, large solar neutron signals were observed by the neutron monitor at Mt. Chacaltaya in Bolivia and Mexico City, and by the solar neutron telescopes at Chacaltaya and Mt. Sierra Negra in Mexico in association with an X17.0 flare. The neutron signal continued for more than 20 minutes with high statistical significance. Intense gamma-ray emission was also registered by INTEGRAL, and by RHESSI during the decay phase. We analyzed these data using the solar-flare magnetic-loop transport and interaction model of Hua et al. (2002), and found that the model could successfully fit the data with intermediate values of loop magnetic convergence and pitch angle scattering parameters. These results indicate that solar neutrons were produced at the same time as the gamma-ray line emission and that ions were continuously accelerated at the emission site. In this paper, we introduce some of the solar neutron observations in solar cycle 23, and discuss the tendencies of the physical parameters of solar neutron GLEs, and the energy spectrum and population of the

  9. Description and primary results of Total Solar Irradiance Monitor, a solar-pointing instrument on an Earth observing satellite

    NASA Astrophysics Data System (ADS)

    Wang, Hongrui; Fang, Wei; Li, Huiduan

    2015-04-01

    Solar driving mechanism for Earth climate has been a controversial problem for centuries. Long-time data of solar activity is required by the investigations of the solar driving mechanism, such as Total Solar Irradiance (TSI) record. Three Total Solar Irradiance Monitors (TSIM) have been developed by Changchun Institute of Optics, Fine Mechanics and Physics for China Meteorological Administration to maintain continuities of TSI data series which lasted for nearly 4 decades.The newest TSIM has recorded TSI daily with accurate solar pointing on the FY-3C meteorological satellite since Oct 2013. TSIM/FY-3C has a pointing system for automatic solar tracking, onboard the satellite designed mainly for Earth observing. Most payloads of FY-3C are developed for observation of land, ocean and atmosphere. Consequently, the FY-3C satellite is a nadir-pointing spacecraft with its z axis to be pointed at the center of the Earth. Previous TSIMs onboard the FY-3A and FY-3B satellites had no pointing system, solar observations were only performed when the sun swept through field-of-view of the instruments. And TSI measurements are influenced inevitably by the solar pointing errors. Corrections of the solar pointing errors were complex. The problem is now removed by TSIM/FY-3C.TSIM/FY-3C follows the sun accurately by itself using its pointing system based on scheme of visual servo control. The pointing system is consisted of a radiometer package, two motors for solar tracking, a sun sensor and etc. TSIM/FY-3C has made daily observations of TSI for more than one year, with nearly zero solar pointing errors. Short time-scale variations in TSI detected by TSIM/FY-3C are nearly the same with VIRGO/SOHO and TIM/SORCE.Instrument details, primary results of solar pointing control, solar observations and etc will be given in the presentation.

  10. Coherent Backscattering and Opposition Effects Observed in Some Atmosphereless Bodies of the Solar System

    NASA Technical Reports Server (NTRS)

    Dlugach, Zh. M.; Mishchenko, M. I.

    2013-01-01

    The results of photometric and polarimetric observations carried out for some bright atmosphere-less bodies of the Solar system near the zero phase angle reveal the simultaneous existence of two spectacular optical phenomena, the so-called brightness and polarization opposition effects. In a number of studies, these phenomena were explained by the influence of coherent backscattering. However, in general, the interference concept of coherent backscattering can be used only in the case where the particles are in the far-field zones of each other, i.e., when the scattering medium is rather rarefied. Because of this, it is important to prove rigorously and to demonstrate that the coherent backscattering effect may also exist in densely packed scattering media like regolith surface layers of celestial bodies. From the results of the computer modeling performed with the use of numerically exact solutions of the macroscopic Maxwell equations for discrete random media with different packing densities of particles, we studied the origin and evolution of all the opposition phenomena predicted by the coherent backscattering theory for low-packing-density media. It has been shown that the predictions of this theory remain valid for rather high-packing densities of particles that are typical, in particular, of regolith surfaces of the Solar system bodies. The results allow us to conclude that both opposition effects observed simultaneously in some high-albedo atmosphereless bodies of the Solar system are caused precisely by coherent backscattering of solar light in the regolith layers composed of microscopic particles.

  11. Investigating Extra-solar Planetary System Qatar-1 through Transit Observations

    NASA Astrophysics Data System (ADS)

    Thakur, Parijat; Mannaday, Vineet Kumar; Jiang, Ing-Guey; Sahu, Devendra Kumar; Chand, Swadesh

    2018-04-01

    We report the results of the transit timing variation (TTV) analysis of the extra-solar planet Qatar-1b using thirty eight light curves. Our analysis combines thirty five previously available transit light curves with three new transits observed by us between June 2016 and September 2016 using the 2-m Himalayan Chandra Telescope (HCT) at the Indian Astronomical Observatory (Hanle, India). From these transit data, the physical and orbital parameters of the Qatar-1 system are determined. In addition to this, the ephemeris for the orbital period and mid-transit time are refined to investigate the possible TTV. We find that the null-TTV model provides the better fit to the (O-C) data. This indicates that there is no evidence for TTVs to confirm the presence of additional planets in the Qatar-1 system. The use of the 3.6-m Devasthal Optical Telescope (DOT) operated by the Aryabhatta Research Institute of Observational Sciences (ARIES, Nainital, India) could improve the photometric precision to examine the signature of TTVs in this system with a greater accuracy than in the present work.

  12. High resolution solar observations from first principles to applications

    NASA Astrophysics Data System (ADS)

    Verdoni, Angelo P.

    2009-10-01

    The expression "high-resolution observations" in Solar Physics refers to the spatial, temporal and spectral domains in their entirety. High-resolution observations of solar fine structure are a necessity to answer many of the intriguing questions related to solar activity. However, a researcher building instruments for high-resolution observations has to cope with the fact that these three domains often have diametrically opposed boundary conditions. Many factors have to be considered in the design of a successful instrument. Modern post-focus instruments are more closely linked with the solar telescopes that they serve than in past. In principle, the quest for high-resolution observations already starts with the selection of the observatory site. The site survey of the Advanced Technology Solar Telescope (ATST) under the stewardship of the National Solar Observatory (NSO) has identified Big Bear Solar Observatory (BBSO) as one of the best sites for solar observations. In a first step, the seeing characteristics at BBSO based on the data collected for the ATST site survey are described. The analysis will aid in the scheduling of high-resolution observations at BBSO as well as provide useful information concerning the design and implementation of a thermal control system for the New Solar Telescope (NST). NST is an off-axis open-structure Gregorian-style telescope with a 1.6 m aperture. NST will be housed in a newly constructed 5/8-sphere ventilated dome. With optics exposed to the surrounding air, NST's open-structure design makes it particularly vulnerable to the effects of enclosure-related seeing. In an effort to mitigate these effects, the initial design of a thermal control system for the NST dome is presented. The goal is to remediate thermal related seeing effects present within the dome interior. The THermal Control System (THCS) is an essential component for the open-telescope design of NST to work. Following these tasks, a calibration routine for the

  13. Solar System Observations with Spitzer Space Telescope: Preliminary Results

    NASA Technical Reports Server (NTRS)

    Cruikshank, Dale P.

    2005-01-01

    The programs of observations of Solar System bodies conducted in the first year of the operation of the Spitzer Space Telescope as part of the Guaranteed Observing Time allocations are described. Initial results include the determination of the albedos of a number of Kuiper Belt objects and Centaurs from observations of their flux densities at 24 and 70 microns, and the detection of emission bands in the spectra of several distant asteroids (Trojans) around 10 and 25 microns. The 10 Kuiper Belt objects observed to date have albedos in the range 0.08 - 0.15, significantly higher than the earlier estimated 0.04. An additional KBO [(55565) 2002 AW(sub l97)] has an albedo of 0.17 plus or minus 0.03. The emission bands in the asteroid spectra are indicative of silicates, but specific minerals have not yet been identified. The Centaur/comet 29P/Schwassmann-Wachmann 1 has a nucleus surface albedo of 0.025 plus or minus 0.01, and its dust production rate was calculated from the properties of the coma. Several other investigations are in progress as the incoming data are processed and analyzed.

  14. Variations of Solar Radius Observed with RHESSI

    NASA Astrophysics Data System (ADS)

    Fivian, M. D.; Hudson, H. S.; Lin, R. P.

    2003-12-01

    The Solar Aspect System (SAS) of the rotating (at 15 rpm) RHESSI spacecraft has three subsystems. Each of these measures the position of the limb by sampling the full solar chord profile with a linear CCD using a narrow bandwidth filter at 670 nm. With a resolution of each CCD of 1.7 arcsec/pixel, the accuracy of each of the 6 limb positions is theoretically better than 50 mas using 4 pixels at each limb. Since the launch of RHESSI early 2002, solar limbs are sampled with at least 100 Hz. That provides a database of currently 4 x 109 single radius measurements. The main function of SAS is to determine the RHESSI pointing relative to Sun center. The observed precision of this determination has a typical instantaneous (16 Hz) value of about 200 mas (rms). We show and discuss first results of variations of solar radius observed with RHESSI.

  15. XMM-Newton Observations of Solar Wind Charge Exchange Emission

    NASA Technical Reports Server (NTRS)

    Snowden, S. L.; Collier, M. R.; Kuntz, K. D.

    2004-01-01

    We present an XMM-Newton spectrum of diffuse X-ray emission from within the solar system. The spectrum is dominated by O VII and O VIII lines at 0.57 keV and 0.65 keV, O VIII (and possibly Fe XVII) lines at approximately 0.8 keV, Ne IX lines at approximately 0.92 keV, and Mg XI lines at approximately 1.35 keV. This spectrum is consistent with what is expected from charge exchange emission between the highly ionized solar wind and either interstellar neutrals in the heliosphere or material from Earth's exosphere. The emission is clearly seen as a low-energy ( E less than 1.5 keV) spectral enhancement in one of a series of observations of the Hubble Deep Field North. The X-ray enhancement is concurrent with an enhancement in the solar wind measured by the ACE satellite. The solar wind enhancement reaches a flux level an order of magnitude more intense than typical fluxes at 1 AU, and has ion ratios with significantly enhanced higher ionization states. Whereas observations of the solar wind plasma made at a single point reflect only local conditions which may only be representative of solar wind properties with spatial scales ranging from less than half of an Earth radii (approximately 10 s) to 100 Earth radii, X-ray observations of solar wind charge exchange are remote sensing measurements which may provide observations which are significantly more global in character. Besides being of interest in its own right for studies of the solar system, this emission can have significant consequences for observations of more cosmological objects. It can provide emission lines at zero redshift which are of particular interest (e.g., O VII and O VIII) in studies of diffuse thermal emission, and which can therefore act as contamination in objects which cover the entire detector field of view. We propose the use of solar wind monitoring data, such as from the ACE and Wind spacecraft, as a diagnostic to screen for such possibilities.

  16. Origins of Inner Solar Systems

    NASA Astrophysics Data System (ADS)

    Dawson, Rebekah Ilene

    2017-06-01

    Over the past couple decades, thousands of extra-solar planetshave been discovered orbiting other stars. The exoplanets discovered to date exhibit a wide variety of orbital and compositional properties; most are dramatically different from the planets in our own Solar System. Our classical theories for the origins of planetary systems were crafted to account for the Solar System and fail to account for the diversity of planets now known. We are working to establish a new blueprint for the origin of planetary systems and identify the key parameters of planet formation and evolution that establish the distribution of planetary properties observed today. The new blueprint must account for the properties of planets in inner solar systems, regions of planetary systems closer to their star than Earth’s separation from the Sun and home to most exoplanets detected to data. I present work combining simulations and theory with data analysis and statistics of observed planets to test theories of the origins of inner solars, including hot Jupiters, warm Jupiters, and tightly-packed systems of super-Earths. Ultimately a comprehensive blueprint for planetary systems will allow us to better situate discovered planets in the context of their system’s formation and evolution, important factors in whether the planets may harbor life.

  17. COMPTEL solar flare observations

    NASA Technical Reports Server (NTRS)

    Ryan, J. M.; Aarts, H.; Bennett, K.; Debrunner, H.; Devries, C.; Denherder, J. W.; Eymann, G.; Forrest, D. J.; Diehl, R.; Hermsen, W.

    1992-01-01

    COMPTEL as part of a solar target of opportunity campaign observed the sun during the period of high solar activity from 7-15 Jun. 1991. Major flares were observed on 9 and 11 Jun. Although both flares were large GOES events (greater than or = X10), they were not extraordinary in terms of gamma-ray emission. Only the decay phase of the 15 Jun. flare was observed by COMPTEL. We report the preliminary analysis of data from these flares, including the first spectroscopic measurement of solar flare neutrons. The deuterium formation line at 2.223 MeV was present in both events and for at least the 9 Jun. event, was comparable to the flux in the nuclear line region of 4-8 MeV, consistent with Solar-Maximum Mission (SSM) Observations. A clear neutron signal was present in the flare of 9 Jun. with the spectrum extending up to 80 MeV and consistent in time with the emission of gamma-rays, confirming the utility of COMPTEL in measuring the solar neutron flux at low energies. The neutron flux below 100 MeV appears to be lower than that of the 3 Jun. 1982 flare by more than an order of magnitude. The neutron signal of the 11 Jun. event is under study. Severe dead time effects resulting from the intense thermal x-rays require significant corrections to the measured flux which increase the magnitude of the associated systematic uncertainties.

  18. Solar Eclipses Observed from Antarctica

    NASA Astrophysics Data System (ADS)

    Pasachoff, Jay M.

    2013-01-01

    Aspects of the solar corona are still best observed during totality of solar eclipses, and other high-resolution observations of coronal active regions can be observed with radio telescopes by differentiation of occultation observations, as we did with the Jansky Very Large Array for the annular solar eclipse of 2012 May 20 in the US. Totality crossing Antarctica included the eclipse of 2003 November 23, and will next occur on 2021 December 4; annularity crossing Antarctica included the eclipse of 2008 February 7, and will next occur on 2014 April 29. Partial phases as high as 87% coverage were visible and were imaged in Antarctica on 2011 November 25, and in addition to partial phases of the total and annular eclipses listed above, partial phases were visible in Antarctica on 2001 July 2011, 2002 December 4, 2004 April 19, 2006 September 22, 2007 September 11, and 2009 January 26, and will be visible on 2015 September 13, 2016 September 1, 2017 February 26, 2018 February 15, and 2020 December 14. On behalf of the Working Group on Solar Eclipses of the IAU, the poster showed the solar eclipses visible from Antarctica and this article shows a subset (see www.eclipses.info for the full set). A variety of investigations of the Sun and of the response of the terrestrial atmosphere and ionosphere to the abrupt solar cutoff can be carried out at the future eclipses, making the Antarctic observations scientifically useful.

  19. Fast Imaging Solar Spectrograph System in New Solar Telescope

    NASA Astrophysics Data System (ADS)

    Park, Y.-D.; Kim, Y. H.; Chae, J.; Goode, P. R.; Cho, K. S.; Park, H. M.; Nah, J. K.; Jang, B. H.

    2010-12-01

    In 2004, Big Bear Solar Observatory in California, USA launched a project for construction of the world's largest aperture solar telescope (D = 1.6m) called New Solar Telescope(NST). University of Hawaii (UH) and Korea Astronomy and Space Science Institute(KASI) partly collaborate on the project. NST is a designed off-axis parabolic Gregorian reflector with very high spatial resolution(0.07 arcsec at 5000A) and is equipped with several scientific instruments such as Visible Imaging Magnetograph (VIM), InfraRed Imaging Magnetograph IRIM), and so on. Since these scientific instruments are focused on studies of the solar photosphere, we need a post-focus instrument for the NST to study the fine structures and dynamic patterns of the solar chromosphere and low Transition Region (TR) layer, including filaments/prominences, spicules, jets, micro flares, etc. For this reason, we developed and installed a fast imaging solar spectrograph(FISS) system on the NST withadvantages of achieving compact design with high spectral resolution and small aberration as well as recording many solar spectral lines in a single and/or dual band mode. FISS was installed in May, 2010 and now we carry out a test observation. In this talk, we introduce the FISS system and the results of the test observation after FISS installation.

  20. Integrated Access to Solar Observations With EGSO

    NASA Astrophysics Data System (ADS)

    Csillaghy, A.

    2003-12-01

    {\\b Co-Authors}: J.Aboudarham (2), E.Antonucci (3), R.D.Bentely (4), L.Ciminiera (5), A.Finkelstein (4), J.B.Gurman(6), F.Hill (7), D.Pike (8), I.Scholl (9), V.Zharkova and the EGSO development team {\\b Institutions}: (2) Observatoire de Paris-Meudon (France); (3) INAF - Istituto Nazionale di Astrofisica (Italy); (4) University College London (U.K.); (5) Politecnico di Torino (Italy), (6) NASA Goddard Space Flight Center (USA); (7) National Solar Observatory (USA); (8) Rutherford Appleton Lab. (U.K.); (9) Institut d'Astrophysique Spatial, Universite de Paris-Sud (France) ; (10) University of Bradford (U.K) {\\b Abstract}: The European Grid of Solar Observations is the European contribution to the deployment of a virtual solar observatory. The project is funded under the Information Society Technologies (IST) thematic programme of the European Commission's Fifth Framework. EGSO started in March 2002 and will last until March 2005. The project is categorized as a computer science effort. Evidently, a fair amount of issues it addresses are general to grid projects. Nevertheless, EGSO is also of benefit to the application domains, including solar physics, space weather, climate physics and astrophysics. With EGSO, researchers as well as the general public can access and combine solar data from distributed archives in an integrated virtual solar resource. Users express queries based on various search parameters. The search possibilities of EGSO extend the search possibilities of traditional data access systems. For instance, users can formulate a query to search for simultaneous observations of a specific solar event in a given number of wavelengths. In other words, users can search for observations on the basis of events and phenomena, rather than just time and location. The software architecture consists of three collaborating components: a consumer, a broker and a provider. The first component, the consumer, organizes the end user interaction and controls requests

  1. The solar wind-magnetosphere-ionosphere system

    PubMed

    Lyon

    2000-06-16

    The solar wind, magnetosphere, and ionosphere form a single system driven by the transfer of energy and momentum from the solar wind to the magnetosphere and ionosphere. Variations in the solar wind can lead to disruptions of space- and ground-based systems caused by enhanced currents flowing into the ionosphere and increased radiation in the near-Earth environment. The coupling between the solar wind and the magnetosphere is mediated and controlled by the magnetic field in the solar wind through the process of magnetic reconnection. Understanding of the global behavior of this system has improved markedly in the recent past from coordinated observations with a constellation of satellite and ground instruments.

  2. Baby Solar System

    NASA Technical Reports Server (NTRS)

    Currie, Thayne; Grady, Carol

    2012-01-01

    What did our solar system look like in its infancy,...... when the planets were forming? We cannot travel back in time to take an image of the early solar system, but in principle we can have the next best thing: images of infant planetary systems around Sun-like stars with ages of 1 to 5 million years, the time we think it took for the giant planets to form. Infant exoplanetary systems are critically important because they can help us understand how our solar system fits within the context of planet formation in general. More than 80% of stars are born with gas- and dust-rich disks, and thus have the potential to form planets. Through many methods we have identified more than 760 planetary systems around middle-aged stars like the Sun, but many of these have architectures that look nothing like our solar system. Young planetary systems are important missing links between various endpoints and may help us understand how and when these differences emerge. Well-known star-forming regions in Taurus, Scorpius. and Orion contain stars that could have infant planetary systems. But these stars are much more distant than our nearest neighbors such as Alpha Centauri or Sirius, making it extremely challenging to produce clear images of systems that can reveal signs of recent planet formation, let alone reveal the planets themselves. Recently, a star with the unassuming name LkCa 15 may have given us our first detailed "baby picture" of a young planetary system similar to our solar system. Located about 450 light-years away in the Taurus starforming region. LkCa 15 has a mass comparable to the Sun (0.97 solar mass) and an age of l to 5 million years, comparable to the time at which Saturn and perhaps Jupiter formed. The star is surrounded by a gas-rich disk similar in structure to the one in our solar system from which the planets formed. With new technologies and observing strategies, we have confirmed suspicions that LkCa 15's disk harbors a young planetary system.

  3. Origin of Outer Solar System

    NASA Technical Reports Server (NTRS)

    Holman, Matthew J.; Lindstrom, David (Technical Monitor)

    2005-01-01

    Our ongoing research program combines extensive deep and wide-field observations using a variety of observational platforms with numerical studies of the dynamics of small bodies in the outer solar system in order to advance the main scientific goals of the community studying the Kuiper belt and the outer solar system. These include: (1) determining the relative populations of the known classes of KBOs as well as other possible classes; ( 2 ) determining the size distributions or luminosity function of the individual populations or the Kuiper belt as a whole; (3) determining the inclinations distributions of these populations; (4) establishing the radial extent of the Kuiper belt; ( 5 ) measuring and relating the physical properties of different types of KBOs to those of other solar system bodies; and, (6) completing our systematic inventory of the satellites of the outer planets.

  4. Where the Solar system meets the solar neighbourhood: patterns in the distribution of radiants of observed hyperbolic minor bodies

    NASA Astrophysics Data System (ADS)

    de la Fuente Marcos, Carlos; de la Fuente Marcos, Raúl; Aarseth, Sverre J.

    2018-05-01

    Observed hyperbolic minor bodies might have an interstellar origin, but they can be natives of the Solar system as well. Fly-bys with the known planets or the Sun may result in the hyperbolic ejection of an originally bound minor body; in addition, members of the Oort cloud could be forced to follow inbound hyperbolic paths as a result of secular perturbations induced by the Galactic disc or, less frequently, due to impulsive interactions with passing stars. These four processes must leave distinctive signatures in the distribution of radiants of observed hyperbolic objects, both in terms of coordinates and velocity. Here, we perform a systematic numerical exploration of the past orbital evolution of known hyperbolic minor bodies using a full N-body approach and statistical analyses to study their radiants. Our results confirm the theoretical expectations that strong anisotropies are present in the data. We also identify a statistically significant overdensity of high-speed radiants towards the constellation of Gemini that could be due to the closest and most recent known fly-by of a star to the Solar system, that of the so-called Scholz's star. In addition to and besides 1I/2017 U1 (`Oumuamua), we single out eight candidate interstellar comets based on their radiants' velocities.

  5. Preparation for the solar system observations with Herschel: Simulation of Jupiter observations with PACS

    NASA Astrophysics Data System (ADS)

    Sagawa, Hideo; Hartogh, Paul; Rengel, Miriam; de Lange, Arno; Cavalié, Thibault

    2010-11-01

    Observations of the water inventory as well as other chemically important species on Jupiter will be performed in the frame of the guaranteed time key project of the Herschel Space Observatory entitled "Water and related chemistry in the Solar system". Among other onboard instruments, PACS (Photodetector Array Camera and Spectrometer) will provide new data of the spectral atlas in a wide region covering the far-infrared and submillimetre domains, with an improved spectral resolution and a higher sensitivity compared to previous observations carried out by Cassini/CIRS (Composite InfraRed Spectrometer) and by ISO (Infrared Space Observatory). In order to optimise the observational plan and to prepare for the data analysis, we have simulated the expected spectra of PACS Jupiter observations. Our simulation shows that PACS will promisingly detect several H 2O emission lines. As PACS is capable of spatially resolving the Jovian disk, we will be able to discern the external oxygen sources in the giant planets by exploring the horizontal distribution of water. In addition to H 2O lines, some absorption lines due to tropospheric CH 4, HD, PH 3 and NH 3 lines will be observed with PACS. Furthermore, owing to the high sensitivity of the instrument, the current upper limit on the abundance of hydrogen halides such as HCl will be also improved.

  6. On the Performance of Multi-Instrument Solar Flare Observations During Solar Cycle 24

    NASA Astrophysics Data System (ADS)

    Milligan, Ryan O.; Ireland, Jack

    2018-02-01

    The current fleet of space-based solar observatories offers us a wealth of opportunities to study solar flares over a range of wavelengths. Significant advances in our understanding of flare physics often come from coordinated observations between multiple instruments. Consequently, considerable efforts have been, and continue to be, made to coordinate observations among instruments ( e.g. through the Max Millennium Program of Solar Flare Research). However, there has been no study to date that quantifies how many flares have been observed by combinations of various instruments. Here we describe a technique that retrospectively searches archival databases for flares jointly observed by the Ramaty High Energy Solar Spectroscopic Imager (RHESSI), Solar Dynamics Observatory (SDO)/ EUV Variability Experiment (EVE - Multiple EUV Grating Spectrograph (MEGS)-A and -B, Hinode/( EUV Imaging Spectrometer, Solar Optical Telescope, and X-Ray Telescope), and Interface Region Imaging Spectrograph (IRIS). Out of the 6953 flares of GOES magnitude C1 or greater that we consider over the 6.5 years after the launch of SDO, 40 have been observed by 6 or more instruments simultaneously. Using each instrument's individual rate of success in observing flares, we show that the numbers of flares co-observed by 3 or more instruments are higher than the number expected under the assumption that the instruments operated independently of one another. In particular, the number of flares observed by larger numbers of instruments is much higher than expected. Our study illustrates that these missions often acted in cooperation, or at least had aligned goals. We also provide details on an interactive widget ( Solar Flare Finder), now available in SSWIDL, which allows a user to search for flaring events that have been observed by a chosen set of instruments. This provides access to a broader range of events in order to answer specific science questions. The difficulty in scheduling coordinated

  7. Observations of an Eruptive Solar Flare in the Extended EUV Solar Corona

    NASA Astrophysics Data System (ADS)

    Seaton, Daniel B.; Darnel, Jonathan M.

    2018-01-01

    We present observations of a powerful solar eruption, accompanied by an X8.2 solar flare, from NOAA Active Region 12673 on 2017 September 10 by the Solar Ultraviolet Imager (SUVI) on the GOES-16 spacecraft. SUVI is noteworthy for its relatively large field of view, which allows it to image solar phenomena to heights approaching 2 solar radii. These observations include the detection of an apparent current sheet associated with magnetic reconnection in the wake of the eruption, and evidence of an extreme-ultraviolet wave at some of the largest heights ever reported. We discuss the acceleration of the nascent coronal mass ejection to approximately 2000 km s‑1 at about 1.5 solar radii. We compare these observations with models of eruptions and eruption-related phenomena. We also describe the SUVI data and discuss how the scientific community can access SUVI observations of the event.

  8. The formation of the solar system

    NASA Astrophysics Data System (ADS)

    Pfalzner, S.; Davies, M. B.; Gounelle, M.; Johansen, A.; Münker, C.; Lacerda, P.; Portegies Zwart, S.; Testi, L.; Trieloff, M.; Veras, D.

    2015-06-01

    The solar system started to form about 4.56 Gyr ago and despite the long intervening time span, there still exist several clues about its formation. The three major sources for this information are meteorites, the present solar system structure and the planet-forming systems around young stars. In this introduction we give an overview of the current understanding of the solar system formation from all these different research fields. This includes the question of the lifetime of the solar protoplanetary disc, the different stages of planet formation, their duration, and their relative importance. We consider whether meteorite evidence and observations of protoplanetary discs point in the same direction. This will tell us whether our solar system had a typical formation history or an exceptional one. There are also many indications that the solar system formed as part of a star cluster. Here we examine the types of cluster the Sun could have formed in, especially whether its stellar density was at any stage high enough to influence the properties of today’s solar system. The likelihood of identifying siblings of the Sun is discussed. Finally, the possible dynamical evolution of the solar system since its formation and its future are considered.

  9. Data on photovoltaic system using different perturb and observe methods under fast multi-changing solar irradiances.

    PubMed

    Peng, Lele; Zheng, Shubin; Xu, Wei; Xin, Li

    2018-04-01

    This article presents the data on photovoltaic (PV) system used different perturb and observe (P&O) methods under fast multi-changing solar irradiances. The mathematical modeling of the PV system and tangent error P&O method was discussed in our previous study entitled "A novel tangent error maximum power point tracking algorithm for photovoltaic system under fast multi-changing solar irradiances" by Peng et al. (2018) [1]. The data provided in this paper can be used directly without having to spend weeks to simulate the output performance. In addition, it is easy to apply the results for comparison with other algorithms (Kollimalla et al., 2014; Belkaid et al., 2016; Chenchen et al., 2015; Jubaer and Zainal, 2015) [2,3,4,5], and develop a new method for practical application.

  10. The Hadean, Through a Glass Telescopically: Observations of Young Solar Analogs

    NASA Technical Reports Server (NTRS)

    Gaidos, E. J.

    1998-01-01

    Investigations into the Earth's surface environment during the Hadean eon (prior to 3.8 Ga) are hampered by the paucity of the geological and geochemical record and the relative inaccessibility of better-preserved surfaces with possibly similar early histories (i.e., Mars). One approach is to observe nearby, young solar-mass stars as analogs to the Hadean Sun and its environment. A catalog of 38 G and early K stars within 25 pc was constructed based on main-sequence status, bolometric luminosity, lack of known stellar companions within 800 AU, and coronal X-ray luminosities commensurate with the higher activity of solar-mass stars <0.8 b.y. old. Spectroscopic data support the assignment of ages of 0.2 - 0.8 Ga for most of these stars. Observations of these objects will provide insight into external forces that influenced Hadean atmosphere, ocean, and surface evolution (and potential ecosystems), including solar luminosity evolution, the flux and spectrum of solar ultraviolet radiation, the intensity of the solar wind, and the intensity and duration of a late period of heavy bombardment. The standard model of solar evolution predicts a luminosity of 0.75 solar luminosity at the end of the Hadean, implying a terrestrial surface temperature inconsistent with the presence of liquid water and motivating atmospheric greenhouse models. An alternative model fo solar evolution that invokes mass loss, constructed to explain solar Li depletion, attenuates or reverses this luminosity evolution of the atmospheres of Earth and the other terrestrial planets. This model can be tested by Li abundance measurements. The continuum emission from stellar wind plasma during significant mass loss may be detectable at millimeter and radio wavelengths. The Earth (and Moon) experienced a period of intense bombardment prior to 3.8 Ga, long after accretion was completed in the inner solar system and possibly associated with the clearing of residual planetesimals in the outer solar system. Such

  11. Observational Evidence of Magnetic Waves in the Solar Atmosphere

    NASA Astrophysics Data System (ADS)

    McIntosh, Scott W.

    2012-03-01

    The observational evidence in supporting the presence of magnetic waves in the outer solar atmosphere is growing rapidly - we will discuss recent observations and place them in context with salient observations made in the past. While the clear delineation of these magnetic wave "modes" is unclear, much can be learned about the environment in which they originated and possibly how they are removed from the system from the observations. Their diagnostic power is, as yet, untapped and their energy content (both as a mechanical source for the heating of coronal material and acceleration of the solar wind) remains in question, but can be probed observationally - raising challenges for modeling efforts. We look forward to the IRIS mission by proposing some sample observing sequences to help resolve some of the zoological issues present in the literature.

  12. Distribution and solar wind control of compressional solar wind-magnetic anomaly interactions observed at the Moon by ARTEMIS

    NASA Astrophysics Data System (ADS)

    Halekas, J. S.; Poppe, A. R.; Lue, C.; Farrell, W. M.; McFadden, J. P.

    2017-06-01

    A statistical investigation of 5 years of observations from the two-probe Acceleration, Reconnection, Turbulence, and Electrodynamics of Moon's Interaction with the Sun (ARTEMIS) mission reveals that strong compressional interactions occur infrequently at high altitudes near the ecliptic but can form in a wide range of solar wind conditions and can occur up to two lunar radii downstream from the lunar limb. The compressional events, some of which may represent small-scale collisionless shocks ("limb shocks"), occur in both steady and variable interplanetary magnetic field (IMF) conditions, with those forming in steady IMF well organized by the location of lunar remanent crustal magnetization. The events observed by ARTEMIS have similarities to ion foreshock phenomena, and those observed in variable IMF conditions may result from either local lunar interactions or distant terrestrial foreshock interactions. Observed velocity deflections associated with compressional events are always outward from the lunar wake, regardless of location and solar wind conditions. However, events for which the observed velocity deflection is parallel to the upstream motional electric field form in distinctly different solar wind conditions and locations than events with antiparallel deflections. Consideration of the momentum transfer between incoming and reflected solar wind populations helps explain the observed characteristics of the different groups of events.Plain Language SummaryWe survey the environment around the Moon to determine when and where strong amplifications in the charged particle density and magnetic field strength occur. These structures may be some of the smallest shock waves in the <span class="hlt">solar</span> <span class="hlt">system</span>, and learning about their formation informs us about the interaction of charged particles with small-scale magnetic fields throughout the <span class="hlt">solar</span> <span class="hlt">system</span> and beyond. We find that these compressions occur in an extended region</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930069132&hterms=soup&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsoup','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930069132&hterms=soup&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsoup"><span>Asteroseismology - The impact of <span class="hlt">solar</span> space <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>Hudson, H. S.</p> <p>1993-01-01</p> <p><span class="hlt">Observations</span> from space relevant to <span class="hlt">solar</span> global properties (oscillations, magnetic activity, etc.) are helpful both scientifically and technically in preparing for stellar <span class="hlt">observations</span>. This paper summarizes the results from the main previous experiments (ACRIM, SOUP, and IPHIR), and also gives an initial technical report from the SXT instrument on board Yohkoh, launched in August 1991. The <span class="hlt">solar</span> <span class="hlt">observations</span> to date demonstrate the existence of several mechanisms for low-level variability: spots, faculae, the photospheric network, granulation, and p-mode oscillations. The <span class="hlt">observations</span> of oscillations have been particularly helpful in setting limits on <span class="hlt">solar</span> interior rotation. In addition to the <span class="hlt">solar</span> processes, stars of other types may have different mechanisms of variability. These may include the analogs of coronal holes or <span class="hlt">solar</span> flares, modes of oscillation not detected in the sun, collisions with small bodies, duplicity, and probably mechanisms not invented yet but related in interesting ways to stellar convection and magnetism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070019764','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070019764"><span><span class="hlt">Solar</span> <span class="hlt">Systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1979-01-01</p> <p>The <span class="hlt">solar</span> collectors shown are elements of domestic <span class="hlt">solar</span> hot water <span class="hlt">systems</span> produced by <span class="hlt">Solar</span> One Ltd., Virginia Beach, Virginia. Design of these <span class="hlt">systems</span> benefited from technical expertise provided <span class="hlt">Solar</span> One by NASA's Langley Research Center. The company obtained a NASA technical support package describing the d e sign and operation of <span class="hlt">solar</span> heating equipment in NASA's Tech House, a demonstration project in which aerospace and commercial building technology are combined in an energy- efficient home. <span class="hlt">Solar</span> One received further assistance through personal contact with Langley <span class="hlt">solar</span> experts. The company reports that the technical information provided by NASA influenced <span class="hlt">Solar</span> One's panel design, its selection of a long-life panel coating which increases <span class="hlt">solar</span> collection efficiency, and the method adopted for protecting <span class="hlt">solar</span> collectors from freezing conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.473..345W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.473..345W"><span>Transit visibility zones of the <span class="hlt">Solar</span> <span class="hlt">system</span> planets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wells, R.; Poppenhaeger, K.; Watson, C. A.; Heller, R.</p> <p>2018-01-01</p> <p>The detection of thousands of extrasolar planets by the transit method naturally raises the question of whether potential extrasolar <span class="hlt">observers</span> could detect the transits of the <span class="hlt">Solar</span> <span class="hlt">system</span> planets. We present a comprehensive analysis of the regions in the sky from where transit events of the <span class="hlt">Solar</span> <span class="hlt">system</span> planets can be detected. We specify how many different <span class="hlt">Solar</span> <span class="hlt">system</span> planets can be <span class="hlt">observed</span> from any given point in the sky, and find the maximum number to be three. We report the probabilities of a randomly positioned external <span class="hlt">observer</span> to be able to <span class="hlt">observe</span> single and multiple <span class="hlt">Solar</span> <span class="hlt">system</span> planet transits; specifically, we find a probability of 2.518 per cent to be able to <span class="hlt">observe</span> at least one transiting planet, 0.229 per cent for at least two transiting planets, and 0.027 per cent for three transiting planets. We identify 68 known exoplanets that have a favourable geometric perspective to allow transit detections in the <span class="hlt">Solar</span> <span class="hlt">system</span> and we show how the ongoing K2 mission will extend this list. We use occurrence rates of exoplanets to estimate that there are 3.2 ± 1.2 and 6.6^{+1.3}_{-0.8} temperate Earth-sized planets orbiting GK and M dwarf stars brighter than V = 13 and 16, respectively, that are located in the Earth's transit zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950015389&hterms=imprint&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dimprint','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950015389&hterms=imprint&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dimprint"><span><span class="hlt">Solar</span> <span class="hlt">system</span> formation and the distribution of volatile species</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lunine, Jonathan I.</p> <p>1994-01-01</p> <p>To understand how the <span class="hlt">solar</span> <span class="hlt">system</span> formed we must understand the compositional distribution of the current <span class="hlt">system</span>. Volatile species are particularly important in that their stability as condensed phases is limited in temperature-pressure space, and hence variations in their distribution at present potentially contain an imprint of processes by which temperature and pressure varied in the <span class="hlt">solar</span> nebula. In this talk we restrict ourselves to species more volatile than water ice, and address issues related to processes in the outer <span class="hlt">solar</span> <span class="hlt">system</span> and the formation of bodies there; others in this conference will cover volatile species relevant to inner <span class="hlt">solar</span> <span class="hlt">system</span> processes. Study of the outer <span class="hlt">solar</span> <span class="hlt">system</span> is relevant both to understanding the interface between the <span class="hlt">solar</span> nebula and the progenitor giant molecular cloud (since the chemical links to present-day <span class="hlt">observables</span> in molecular clouds are species like methane, carbon monoxide, etc.), as well as the origin of terrestrial planet atmospheres and oceans (the latter to be covered by Owen). The wealth of compositional information on outer <span class="hlt">solar</span> <span class="hlt">system</span> bodies which has become available from spacecraft and ground-based <span class="hlt">observations</span> challenges traditional simplistic views of the composition and hence dynamics of the <span class="hlt">solar</span> nebula. The basic assumption of thermochemical equilibrium, promulgated in the 1950's, in which methane and ammonia dominate nitrogen- and carbon-bearing species, is demonstrably incorrect on both <span class="hlt">observational</span> and theoretical grounds. However, the kinetic inhibition model which replaced it, in which carbon monoxide and molecular nitrogen dominate a nebula which is fully mixed and hence cycles outer <span class="hlt">solar</span> <span class="hlt">system</span> gases through a hot, chemically active zone near the disk center, is not supported either by <span class="hlt">observations</span>. Instead, a picture of the outer <span class="hlt">solar</span> <span class="hlt">system</span> emerges in which the gas and grains are a mixture of relatively unaltered, or modestly altered, molecular cloud material, along with a fraction</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999nssy.book.....B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999nssy.book.....B"><span>The New <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Beatty, J. Kelly; Collins Petersen, Carolyn; Chaikin, Andrew</p> <p>1999-01-01</p> <p>As the definitive guide for the armchair astronomer, The New <span class="hlt">Solar</span> <span class="hlt">System</span> has established itself as the leading book on planetary science and <span class="hlt">solar</span> <span class="hlt">system</span> studies. Incorporating the latest knowledge of the <span class="hlt">solar</span> <span class="hlt">system</span>, a distinguished team of researchers, many of them Principal Investigators on NASA missions, explain the <span class="hlt">solar</span> <span class="hlt">system</span> with expert ease. The completely-revised text includes the most recent findings on asteroids, comets, the Sun, and our neighboring planets. The book examines the latest research and thinking about the <span class="hlt">solar</span> <span class="hlt">system</span>; looks at how the Sun and planets formed; and discusses our search for other planetary <span class="hlt">systems</span> and the search for life in the <span class="hlt">solar</span> <span class="hlt">system</span>. In full-color and heavily-illustrated, the book contains more than 500 photographs, portrayals, and diagrams. An extensive set of tables with the latest characteristics of the planets, their moon and ring <span class="hlt">systems</span>, comets, asteroids, meteorites, and interplanetary space missions complete the text. New to this edition are descriptions of collisions in the <span class="hlt">solar</span> <span class="hlt">system</span>, full scientific results from Galileo's mission to Jupiter and its moons, and the Mars Pathfinder mission. For the curious <span class="hlt">observer</span> as well as the student of planetary science, this book will be an important library acquisition. J. Kelly Beatty is the senior editor of Sky & Telescope, where for more than twenty years he has reported the latest in planetary science. A renowned science writer, he was among the first journalists to gain access to the Soviet space program. Asteroid 2925 Beatty was named on the occasion of his marriage in 1983. Carolyn Collins Petersen is an award-winning science writer and co-author of Hubble Vision (Cambridge 1995). She has also written planetarium programs seen at hundreds of facilities around the world. Andrew L. Chaikin is a Boston-based science writer. He served as a research geologist at the Smithsonian Institution's Center for Earth and Planetary Studies. He is a contributing editor to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015TESS....131009F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015TESS....131009F"><span><span class="hlt">Solar</span> and Galactic Cosmic Rays <span class="hlt">Observed</span> by SOHO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fleck, Bernhard; Curdt, Werner; Olive, Jean-Philippe; van Overbeek, Ton</p> <p>2015-04-01</p> <p>Both the Cosmic Ray Flux (CRF) and <span class="hlt">Solar</span> Energetic Particles (SEPs) have left an imprint on SOHO technical <span class="hlt">systems</span>. While the <span class="hlt">solar</span> array efficiency degraded irreversibly down to 75% of its original level over 1 ½ <span class="hlt">solar</span> cycles, Single Event Upsets (SEUs) in the solid state recorder (SSR) have been reversed by the memory protection mechanism. We compare the daily CRF <span class="hlt">observed</span> by the Oulu station with the daily SOHO SEU rate and with the degradation curve of the <span class="hlt">solar</span> arrays. The Oulu CRF and the SOHO SSR SEU rate are both modulated by the <span class="hlt">solar</span> cycle and are highly correlated, except for sharp spikes in the SEU rate, caused by isolated SEP events, which also show up as discontinuities in the otherwise slowly decreasing <span class="hlt">solar</span> ray efficiency. This allows to discriminate between effects with <span class="hlt">solar</span> and non-<span class="hlt">solar</span> origin and to compare the relative strength of both. We find that the total number of SSR SEUs with <span class="hlt">solar</span> origin over the 17 ½ years from January 1996 through June 2013 is of the same order as those generated by cosmic ray hits. 49% of the total <span class="hlt">solar</span> array degradation during that time can be attributed to proton events, i.e. the effect of a series of short-lived, violent events (SEPs) is comparable to the cycle-integrated damage by cosmic rays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23124202J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23124202J"><span><span class="hlt">Observations</span> of Fe XIV Line Intensity Variations in the <span class="hlt">Solar</span> Corona During the 21 August 2017 <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Johnson, Payton; Ladd, Edwin</p> <p>2018-01-01</p> <p>We present time- and spatially-resolved <span class="hlt">observations</span> of the inner <span class="hlt">solar</span> corona in the 5303 Å line of Fe XIV, taken during the 21 August 2017 <span class="hlt">solar</span> eclipse from a field <span class="hlt">observing</span> site in Crossville, TN. These <span class="hlt">observations</span> are used to characterize the intensity variations in this coronal emission line, and to compare with oscillation predictions from models for heating the corona by magnetic wave dissipation.The <span class="hlt">observations</span> were taken with two Explore Scientific ED 102CF 102 mm aperture triplet apochromatic refractors. One <span class="hlt">system</span> used a DayStar custom-built 5 Å FWHM filter centered on the Fe XIV coronal spectral line and an Atik Titan camera for image collection. The setup produced images with a pixel size of 2.15 arcseconds (~1.5 Mm at the distance to the Sun), and a field of view of 1420 x 1060 arcseconds, covering approximately 20% of the entire <span class="hlt">solar</span> limb centered near the emerging sunspot complex AR 2672. We obtained images with an exposure time of 0.22 seconds and a frame rate of 2.36 Hz, for a total of 361 images during totality.An identical, co-aligned telescope/camera <span class="hlt">system</span> <span class="hlt">observed</span> the same portion of the <span class="hlt">solar</span> corona, but with a 100 Å FWHM Baader Planetarium <span class="hlt">solar</span> continuum filter centered on a wavelength of 5400 Å. Images with an exposure time of 0.01 seconds were obtained with a frame rate of 4.05 Hz. These simultaneous <span class="hlt">observations</span> are used as a control to monitor brightness variations not related to coronal line oscillations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170000779','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170000779"><span>Search for Primitive Matter in the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Libourel, G.; Michel, P.; Delbo, M.; Ganino, C.; Recio-Blanco, A.; de Laverny, P.; Zolensky, M. E.; Krot, A. N.</p> <p>2017-01-01</p> <p>Recent astronomical <span class="hlt">observations</span> and theoretical modeling led to a consensus regarding the global scenario of the formation of young stellar objects (YSO) from a cold molecular cloud of interstellar dust (organics and minerals) and gas that, in some cases, leads to the formation of a planetary <span class="hlt">system</span>. In the case of our <span class="hlt">Solar</span> <span class="hlt">System</span>, which has already evolved for approximately 4567 Ma, the quest is to access, through the investigation of planets, moons, cometary and asteroidal bodies, meteorites, micrometeorites, and interplanetary dust particles, the primitive material that contains the key information about the early <span class="hlt">Solar</span> <span class="hlt">System</span> processes and its evolution. However, laboratory analyses of extraterrestrial samples, astronomical <span class="hlt">observations</span> and dynamical models of the <span class="hlt">Solar</span> <span class="hlt">System</span> evolution have not brought yet any conclusive evidence on the nature and location of primitive matter in the <span class="hlt">Solar</span> <span class="hlt">System</span>, preventing a clear understanding of its early stages.</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_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_3 --> <div id="page_4" 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_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</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="61"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860015159','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860015159"><span>High-spectral resolution <span class="hlt">solar</span> microwave <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>Hurford, G. J.</p> <p>1986-01-01</p> <p>The application of high-spectral resolution microwave <span class="hlt">observations</span> to the study of <span class="hlt">solar</span> activity is discussed with particular emphasis on the frequency dependence of microwave emission from <span class="hlt">solar</span> active regions. A shell model of gyroresonance emission from active regions is described which suggest that high-spectral resolution, spatially-resolved <span class="hlt">observations</span> can provide quantitative information about the magnetic field distribution at the base of the corona. Corresponding <span class="hlt">observations</span> of a single sunspot with the Owens Valley frequency-agile interferometer at 56 frequencies between 1.2 and 14 Ghs are presented. The overall form of the <span class="hlt">observed</span> size and brightness temperature spectra was consistent with expectations based on the shell model, although there were differences of potential physical significance. The merits and weaknesses of microwave spectroscopy as a technique for measuring magnetic fields in the <span class="hlt">solar</span> corona are briefly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900063357&hterms=background+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dbackground%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900063357&hterms=background+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dbackground%2Bwind"><span><span class="hlt">Solar</span> minimum Lyman alpha sky background <span class="hlt">observations</span> from Pioneer Venus orbiter ultraviolet spectrometer - <span class="hlt">Solar</span> wind latitude variation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ajello, J. M.</p> <p>1990-01-01</p> <p>Measurements of interplanetary H I Lyman alpha over a large portion of the celestial sphere were made at the recent <span class="hlt">solar</span> minimum by the Pioneer Venus orbiter ultraviolet spectrometer. These measurements were performed during a series of spacecraft maneuvers conducted to <span class="hlt">observe</span> Halley's comet in early 1986. Analysis of these data using a model of the passage of interstellar wind hydrogen through the <span class="hlt">solar</span> <span class="hlt">system</span> shows that the rate of charge exchange with <span class="hlt">solar</span> wind protons is 30 percent less over the <span class="hlt">solar</span> poles than in the ecliptic. This result is in agreement with a similar experiment performed with Mariner 10 at the previous <span class="hlt">solar</span> minimum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006Ippa....2a..17T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006Ippa....2a..17T"><span>The chaotic "sculpting" of the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsiganis, K.</p> <p>2006-01-01</p> <p>The orbits of the large celestial bodies in our <span class="hlt">Solar</span> <span class="hlt">System</span> are stable for very long times, as can be shown by numerical simulation. This gives the erroneous impression of perpetual stability of the <span class="hlt">system</span>. It is only when we study the orbital distribution of the numerous minor bodies in the <span class="hlt">Solar</span> <span class="hlt">System</span> that we discover the rich variety of complex dynamical processes that have in fact shaped our <span class="hlt">system</span>. During the last decade, enormous progress has been made, in understanding the evolution of the <span class="hlt">system</span> over the last ~3.9 Gy. However, it also became clear that, in order to unveil its behaviour during the first ~700 million years of its lifetime, we have to find convincing explanations for <span class="hlt">observations</span> that appear as details of its dynamical architecture. In the following we are going to show how the two best known - and up to now unexplained - <span class="hlt">observations</span> in the <span class="hlt">Solar</span> <span class="hlt">System</span>, namely (i) the heavily cratered surface of the Moon and (ii) the elliptic (and not circular) motion of the planets, lead us to the discovery of the chaotic sculpting of the <span class="hlt">Solar</span> <span class="hlt">System</span> [1]-[3].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPSC...11..898B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPSC...11..898B"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Science with the Twinkle Space Mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bowles, N.; Lindsay, S.; Tessenyi, M.; Tinetti, G.; Savini, G.; Tennyson, J.; Pascale, E.; Jason, S.; Vora, A.</p> <p>2017-09-01</p> <p>Twinkle is a space-based telescope mission designed for the spectroscopic <span class="hlt">observation</span> (0.4 to 4.5 μm) of exoplanet atmospheres and <span class="hlt">Solar</span> <span class="hlt">System</span> objects. The <span class="hlt">system</span> design and mission implementation are based on existing, well studied concepts pioneered by Surrey Satellite Technology Ltd for low-Earth orbit Earth <span class="hlt">Observation</span> satellites, supported by a novel international access model to allow facility access to researchers worldwide. Whilst Twinkle's primary science goal is the <span class="hlt">observation</span> of exoplanet atmospheres its wide spectroscopic range and photometric stability also make it a unique platform for the <span class="hlt">observation</span> of <span class="hlt">Solar</span> <span class="hlt">system</span> objects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSA13B3990G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSA13B3990G"><span>The South Pole, Antarctica, <span class="hlt">Solar</span> Radio Telescope (SPASRT) <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gerrard, A. J.; Weatherwax, A. T.; Gary, D. E.; Kujawski, J. T.; Nita, G. M.; Melville, R.; Stillinger, A.; Jeffer, G.</p> <p>2014-12-01</p> <p>The study of the sun in the radio portion of the electromagnetic spectrum furthers our understanding of fundamental <span class="hlt">solar</span> processes <span class="hlt">observed</span> in the X-ray, UV, and visible regions of the spectrum. For example, the study of <span class="hlt">solar</span> radio bursts, which have been shown to cause serious disruptions of technologies at Earth, are essential for advancing our knowledge and understanding of <span class="hlt">solar</span> flares and their relationship to coronal mass ejections and <span class="hlt">solar</span> energetic particles, as well as the underlying particle acceleration mechanisms associated with these processes. In addition, radio coverage of the <span class="hlt">solar</span> atmosphere could yield completely new insights into the variations of output <span class="hlt">solar</span> energy, including Alfven wave propagation through the <span class="hlt">solar</span> atmosphere and into the <span class="hlt">solar</span> wind, which can potentially modulate and disturb the <span class="hlt">solar</span> wind and Earth's geospace environment. In this presentation we discuss the development, construction, and testing of the South Pole, Antarctica, <span class="hlt">Solar</span> Radio Telescope that is planned for installation at South Pole. The <span class="hlt">system</span> will allow for 24-hour continuous, long-term <span class="hlt">observations</span> of the sun across the 1-18 GHz frequency band and allow for truly continuous <span class="hlt">solar</span> <span class="hlt">observations</span>. We show that this <span class="hlt">system</span> will enable unique scientific investigations of the <span class="hlt">solar</span> atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...611A...1M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...611A...1M"><span><span class="hlt">SOLAR</span>-ISS: A new reference spectrum based on <span class="hlt">SOLAR</span>/SOLSPEC <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>Meftah, M.; Damé, L.; Bolsée, D.; Hauchecorne, A.; Pereira, N.; Sluse, D.; Cessateur, G.; Irbah, A.; Bureau, J.; Weber, M.; Bramstedt, K.; Hilbig, T.; Thiéblemont, R.; Marchand, M.; Lefèvre, F.; Sarkissian, A.; Bekki, S.</p> <p>2018-03-01</p> <p>Context. Since April 5, 2008 and up to February 15, 2017, the <span class="hlt">SOLar</span> SPECtrometer (SOLSPEC) instrument of the <span class="hlt">SOLAR</span> payload on board the International Space Station (ISS) has performed accurate measurements of <span class="hlt">solar</span> spectral irradiance (SSI) from the middle ultraviolet to the infrared (165 to 3088 nm). These measurements are of primary importance for a better understanding of <span class="hlt">solar</span> physics and the impact of <span class="hlt">solar</span> variability on climate. In particular, a new reference <span class="hlt">solar</span> spectrum (<span class="hlt">SOLAR</span>-ISS) is established in April 2008 during the <span class="hlt">solar</span> minima of cycles 23-24 thanks to revised engineering corrections, improved calibrations, and advanced procedures to account for thermal and aging corrections of the <span class="hlt">SOLAR</span>/SOLSPEC instrument. Aims: The main objective of this article is to present a new high-resolution <span class="hlt">solar</span> spectrum with a mean absolute uncertainty of 1.26% at 1σ from 165 to 3000 nm. This <span class="hlt">solar</span> spectrum is based on <span class="hlt">solar</span> <span class="hlt">observations</span> of the <span class="hlt">SOLAR</span>/SOLSPEC space-based instrument. Methods: The <span class="hlt">SOLAR</span>/SOLSPEC instrument consists of three separate double monochromators that use concave holographic gratings to cover the middle ultraviolet (UV), visible (VIS), and infrared (IR) domains. Our best ultraviolet, visible, and infrared spectra are merged into a single absolute <span class="hlt">solar</span> spectrum covering the 165-3000 nm domain. The resulting <span class="hlt">solar</span> spectrum has a spectral resolution varying between 0.6 and 9.5 nm in the 165-3000 nm wavelength range. We build a new <span class="hlt">solar</span> reference spectrum (<span class="hlt">SOLAR</span>-ISS) by constraining existing high-resolution spectra to <span class="hlt">SOLAR</span>/SOLSPEC <span class="hlt">observed</span> spectrum. For that purpose, we account for the difference of resolution between the two spectra using the <span class="hlt">SOLAR</span>/SOLSPEC instrumental slit functions. Results: Using <span class="hlt">SOLAR</span>/SOLSPEC data, a new <span class="hlt">solar</span> spectrum covering the 165-3000 nm wavelength range is built and is representative of the 2008 <span class="hlt">solar</span> minimum. It has a resolution better than 0.1 nm below 1000 nm and 1 nm in the 1000-3000 nm wavelength range. The new</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050181977','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050181977"><span><span class="hlt">Solar-System</span> Tests of Gravitational Theories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shapiro, Irwin I.</p> <p>2005-01-01</p> <p>This research is aimed at testing gravitational theory, primarily on an interplanetary scale and using mainly <span class="hlt">observations</span> of objects in the <span class="hlt">solar</span> <span class="hlt">system</span>. Our goal is either to detect departures from the standard model (general relativity) - if any exist within the level of sensitivity of our data - or to support this model by placing tighter bounds on any departure from it. For this project, we have analyzed a combination of <span class="hlt">observational</span> data with our model of the <span class="hlt">solar</span> <span class="hlt">system</span>, including planetary radar ranging, lunar laser ranging, and spacecraft tracking, as well as pulsar timing and pulsar VLBI measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SoPh..292...49T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SoPh..292...49T"><span>Imaging Spectropolarimeter for the Multi-Application <span class="hlt">Solar</span> Telescope at Udaipur <span class="hlt">Solar</span> Observatory: Characterization of Polarimeter and Preliminary <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>Tiwary, Alok Ranjan; Mathew, Shibu K.; Bayanna, A. Raja; Venkatakrishnan, P.; Yadav, Rahul</p> <p>2017-04-01</p> <p>The Multi-Application <span class="hlt">Solar</span> Telescope (MAST) is a 50 cm off-axis Gregorian telescope that has recently become operational at the Udaipur <span class="hlt">Solar</span> Observatory (USO). An imaging spectropolarimeter is being developed as one of the back-end instruments of MAST to gain a better understanding of the evolution and dynamics of <span class="hlt">solar</span> magnetic and velocity fields. This <span class="hlt">system</span> consists of a narrow-band filter and a polarimeter. The polarimeter includes a linear polarizer and two sets of liquid crystal variable retarders (LCVRs). The instrument is intended for simultaneous <span class="hlt">observations</span> in the spectral lines 6173 Å and 8542 Å, which are formed in the photosphere and chromosphere, respectively. In this article, we present results from the characterization of the LCVRs for the spectral lines of interest and the response matrix of the polarimeter. We also present preliminary <span class="hlt">observations</span> of an active region obtained using the spectropolarimeter. For verification purposes, we compare the Stokes <span class="hlt">observations</span> of the active region obtained from the Helioseismic Magnetic Imager (HMI) onboard the <span class="hlt">Solar</span> Dynamics Observatory (SDO) with that of MAST <span class="hlt">observations</span> in the spectral line 6173 Å. We find good agreement between the two <span class="hlt">observations</span>, considering the fact that MAST <span class="hlt">observations</span> are limited by seeing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AAS...22412361S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AAS...22412361S"><span>Flight Performance of the HEROES <span class="hlt">Solar</span> Aspect <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shih, Albert Y.; Christe, Steven; Rodriguez, Marcello; Gregory, Kyle; Cramer, Alexander; Edgerton, Melissa; Gaskin, Jessica; O'Connor, Brian; Sobey, Alexander</p> <p>2014-06-01</p> <p>Hard X-ray (HXR) <span class="hlt">observations</span> of <span class="hlt">solar</span> flares reveal the signatures of energetic electrons, and HXR images with high dynamic range and high sensitivity can distinguish between where electrons are accelerated and where they stop. Furthermore, high-sensitivity HXR measurements may be able to detect the presence of electron acceleration in the non-flaring corona. The High Energy Replicated Optics to Explore the Sun (HEROES) balloon mission added the capability of <span class="hlt">solar</span> <span class="hlt">observations</span> to an existing astrophysics balloon payload, HERO, which used grazing-incidence optics for direct HXR imaging. The HEROES <span class="hlt">Solar</span> Aspect <span class="hlt">System</span> (SAS) was developed and built to provide pointing knowledge during <span class="hlt">solar</span> <span class="hlt">observations</span> to better than the ~20 arcsec FWHM angular resolution of the HXR instrument. The SAS consists of two separate <span class="hlt">systems</span>: the Pitch-Yaw aspect <span class="hlt">System</span> (PYAS) and the Roll Aspect <span class="hlt">System</span> (RAS). The PYAS compares the position of an optical image of the Sun relative to precise fiducials to determine the pitch and yaw pointing offsets from the desired <span class="hlt">solar</span> target. The RAS images the Earth's horizon in opposite directions simultaneously to determine the roll of the gondola. HEROES launched in September 2013 from Fort Sumner, New Mexico, and had a successful one-day flight. We present the detailed analysis of the performance of the SAS for that flight.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000070717','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000070717"><span>Distant Comets in the Early <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Meech, Karen J.</p> <p>2000-01-01</p> <p>The main goal of this project is to physically characterize the small outer <span class="hlt">solar</span> <span class="hlt">system</span> bodies. An understanding of the dynamics and physical properties of the outer <span class="hlt">solar</span> <span class="hlt">system</span> small bodies is currently one of planetary science's highest priorities. The measurement of the size distributions of these bodies will help constrain the early mass of the outer <span class="hlt">solar</span> <span class="hlt">system</span> as well as lead to an understanding of the collisional and accretional processes. A study of the physical properties of the small outer <span class="hlt">solar</span> <span class="hlt">system</span> bodies in comparison with comets in the inner <span class="hlt">solar</span> <span class="hlt">system</span> and in the Kuiper Belt will give us information about the nebular volatile distribution and small body surface processing. We will increase the database of comet nucleus sizes making it statistically meaningful (for both Short-Period and Centaur comets) to compare with those of the Trans-Neptunian Objects. In addition, we are proposing to do active ground-based <span class="hlt">observations</span> in preparation for several upcoming space missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900003151','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900003151"><span>Capabilities of GRO/OSSE for <span class="hlt">observing</span> <span class="hlt">solar</span> flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kurfess, J. D.; Johnson, W. N.; Share, G. H.; Hulburt, E. O.; Matz, S. M.; Murphy, R. J.</p> <p>1989-01-01</p> <p>The launch of the Gamma Ray Observatory (GRO) near <span class="hlt">solar</span> maximum makes <span class="hlt">solar</span> flare studies early in the mission particularly advantageous. The Oriented Scintillation Spectrometer Experiment (OSSE) on GRO, covering the energy range 0.05 to 150 MeV, has some significant advantages over the previous generation of satellite-borne gamma-ray detectors for <span class="hlt">solar</span> <span class="hlt">observations</span>. The OSSE detectors will have about 10 times the effective area of the Gamma-Ray Spectrometer (GRS) on <span class="hlt">Solar</span> Maximum Mission (SMM) for both photons and high-energy neutrons. The OSSE also has the added capability of distinguishing between high-energy neutrons and photons directly. The OSSE spectral accumulation time (approx. 4s) is four times faster than that of the SMM/GRS; much better time resolution is available in selected energy ranges. These characteristics will allow the investigation of particle acceleration in flares based on the evolution of the continuum and nuclear line components of flare spectra, nuclear emission in small flares, the anisotropy of continuum emission in small flares, and the relative intensities of different nuclear lines. The OSSE <span class="hlt">observational</span> program will be devoted primarily to non-<span class="hlt">solar</span> sources. Therefore, <span class="hlt">solar</span> <span class="hlt">observations</span> require planning and special configurations. The instrumental and operational characteristics of OSSE are discussed in the context of undertaking <span class="hlt">solar</span> <span class="hlt">observations</span>. The opportunities for guest investigators to participate in <span class="hlt">solar</span> flare studies with OSSE is also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890016992','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890016992"><span>Chemical evolution: A <span class="hlt">solar</span> <span class="hlt">system</span> perspective</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oro, J.</p> <p>1989-01-01</p> <p>During the last three decades major advances were made in the understanding of the formation of carbon compounds in the universe and of the occurrence of processes of chemical evolution in the <span class="hlt">solar</span> <span class="hlt">system</span> and beyond. This was made possible by the development of new astronomical techniques and by the exploration of the <span class="hlt">solar</span> <span class="hlt">system</span> by means of properly instrumented spacecraft. Some of the major findings made as a result of these <span class="hlt">observations</span> are summarized.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...614A..54V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...614A..54V"><span>LOFAR <span class="hlt">observations</span> of the quiet <span class="hlt">solar</span> corona</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vocks, C.; Mann, G.; Breitling, F.; Bisi, M. M.; Dąbrowski, B.; Fallows, R.; Gallagher, P. T.; Krankowski, A.; Magdalenić, J.; Marqué, C.; Morosan, D.; Rucker, H.</p> <p>2018-06-01</p> <p>Context. The quiet <span class="hlt">solar</span> corona emits meter-wave thermal bremsstrahlung. Coronal radio emission can only propagate above that radius, Rω, where the local plasma frequency equals the <span class="hlt">observing</span> frequency. The radio interferometer LOw Frequency ARray (LOFAR) <span class="hlt">observes</span> in its low band (10-90 MHz) <span class="hlt">solar</span> radio emission originating from the middle and upper corona. Aims: We present the first <span class="hlt">solar</span> aperture synthesis imaging <span class="hlt">observations</span> in the low band of LOFAR in 12 frequencies each separated by 5 MHz. From each of these radio maps we infer Rω, and a scale height temperature, T. These results can be combined into coronal density and temperature profiles. Methods: We derived radial intensity profiles from the radio images. We focus on polar directions with simpler, radial magnetic field structure. Intensity profiles were modeled by ray-tracing simulations, following wave paths through the refractive <span class="hlt">solar</span> corona, and including free-free emission and absorption. We fitted model profiles to <span class="hlt">observations</span> with Rω and T as fitting parameters. Results: In the low corona, Rω < 1.5 <span class="hlt">solar</span> radii, we find high scale height temperatures up to 2.2 × 106 K, much more than the brightness temperatures usually found there. But if all Rω values are combined into a density profile, this profile can be fitted by a hydrostatic model with the same temperature, thereby confirming this with two independent methods. The density profile deviates from the hydrostatic model above 1.5 <span class="hlt">solar</span> radii, indicating the transition into the <span class="hlt">solar</span> wind. Conclusions: These results demonstrate what information can be gleaned from <span class="hlt">solar</span> low-frequency radio images. The scale height temperatures we find are not only higher than brightness temperatures, but also than temperatures derived from coronograph or extreme ultraviolet (EUV) data. Future <span class="hlt">observations</span> will provide continuous frequency coverage. This continuous coverage eliminates the need for local hydrostatic density models in the data analysis and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998etns.conf......','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998etns.conf......"><span>Exploring the Trans-Neptunian <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p>1998-01-01</p> <p>A profound question for scientists, philosophers and, indeed, all humans concerns how the <span class="hlt">solar</span> <span class="hlt">system</span> originated and subsequently evolved. To understand the <span class="hlt">solar</span> <span class="hlt">system</span>'s formation, it is necessary to document fully the chemical and physical makeup of its components today, particularly those parts thought to retain clues about primordial conditions and processes.] In the past decade, our knowledge of the outermost, or trans-neptunian, region of the <span class="hlt">solar</span> <span class="hlt">system</span> has been transformed as a result of Earth-based <span class="hlt">observations</span> of the Pluto-Charon <span class="hlt">system</span>, Voyager 2's encounter with Neptune and its satellite Triton, and recent discoveries of dozens of bodies near to or beyond the orbit of Neptune. As a class, these newly detected objects, along with Pluto, Charon, and Triton, occupy the inner region of a hitherto unexplored component of the <span class="hlt">solar</span> <span class="hlt">system</span>, the Kuiper Belt. The Kuiper Belt is believed to be a reservoir of primordial objects of the type that formed in the <span class="hlt">solar</span> nebula and eventually accreted to form the major planets. The Kuiper Belt is also thought to be the source of short-period comets and a population of icy bodies, the Centaurs, with orbits among the giant planets. Additional components of the distant outer <span class="hlt">solar</span> <span class="hlt">system</span>, such as dust and the Oort comet cloud, as well as the planet Neptune itself, are not discussed in this report. Our increasing knowledge of the trans-neptunian <span class="hlt">solar</span> <span class="hlt">system</span> has been matched by a corresponding increase in our capabilities for remote and in situ <span class="hlt">observation</span> of these distant regions. Over the next 10 to 15 years, a new generation of ground- and space-based instruments, including the Keck and Gemini telescopes and the Space Infrared Telescope Facility, will greatly expand our ability to search for and conduct physical and chemical studies on these distant bodies. Over the same time span, a new generation of lightweight spacecraft should become available and enable the first missions designed specifically to explore the icy</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050041678','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050041678"><span><span class="hlt">Solar-System</span> Tests of Gravitational Theories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shapiro, Irwin I.</p> <p>2005-01-01</p> <p>We are engaged in testing gravitational theory, mainly using <span class="hlt">observations</span> of objects in the <span class="hlt">solar</span> <span class="hlt">system</span> and mainly on the interplanetary scale. Our goal is either to detect departures from the standard model (general relativity) - if any exist within the level of sensitivity of our data - or to support this model by placing tighter bounds on any departure from it. For this project, we have analyzed a combination of <span class="hlt">observational</span> data with our model of the <span class="hlt">solar</span> <span class="hlt">system</span>, including planetary radar ranging, lunar laser ranging, and spacecraft tracking, as well as pulsar timing and pulsar VLBI measurements. In the past year, we have added to our data, primarily lunar laser ranging measurements, but also supplementary data concerning the physical properties of <span class="hlt">solar-system</span> objects, such as the <span class="hlt">solar</span> quadrupole moment, planetary masses, and asteroid radii. Because the <span class="hlt">solar</span> quadrupole moment contributes to the classical precession of planetary perihelia, but with a dependence on distance from the Sun that differs from that of the relativistic precession, it is possible to estimate effects simultaneously. However, our interest is mainly in the relativistic effect, and we find that imposing a constraint on the quadrupole moment from helioseismology studies, gives us a dramatic (about ten-fold) decrease in the standard error of our estimate of the relativistic component of the perihelion advance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900018847','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900018847"><span><span class="hlt">Observed</span> <span class="hlt">solar</span> near UV variability: A contribution to variations of the <span class="hlt">solar</span> constant</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>London, Julius; Pap, Judit; Rottman, Gary J.</p> <p>1989-01-01</p> <p>Continuous Measurements of the <span class="hlt">Solar</span> UV have been made by an instrument on the <span class="hlt">Solar</span> Mesosphere Explorer (SME) since October 1981. The results for the wavelength interval 200 to 300 nm show an irradiance decrease to a minimum in early 1987 and a subsequent increase to mid-April 1989. The <span class="hlt">observed</span> UV changes during part of <span class="hlt">solar</span> cycles 21 to 22 represent approx. 35 percent (during the decreasing phase) and 25 percent (during the increasing phase) of the <span class="hlt">observed</span> variations of the <span class="hlt">solar</span> constant for the same time period as the SME measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA282037','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA282037"><span><span class="hlt">Solar</span> <span class="hlt">Observations</span> on Magneto-Convection</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1989-05-31</p> <p>Technical Library National <span class="hlt">Solar</span> Observatory Sunspot, NM 88349 Karl - Schwarzschild -Strasse 1 8046 Garching bei Mundhen <span class="hlt">Solar</span> <span class="hlt">Observations</span> On Magneto...Schmidt, Hermann-Ulrich Schmidt, Hans-Christoph Thomas (eds.) Max-Planck-Institut fir Physik und Astrophysik Institut fiur Astrophysik Karl ... Schwarzschild -St-. 1 D-8046 Garching, FklG 14TIS CRiA.&l DTIC TA. U~Jar,iou8:ed B ......... ... Distribution I -- Availability COcý----- Avail and or Dist special</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730002079','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730002079"><span>Spacecraft <span class="hlt">observations</span> of the <span class="hlt">solar</span> wind composition</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bame, S. J.</p> <p>1972-01-01</p> <p><span class="hlt">Solar</span> wind composition studies by means of plasma analyzers carried on various spacecraft are reviewed. The average ratio of helium to hydrogen over the <span class="hlt">solar</span> cycle is close to 0.045; values as low as 0.0025 and as high as 0.25 have been <span class="hlt">observed</span>. High values have been <span class="hlt">observed</span> following <span class="hlt">solar</span> flares and interplanetary shock waves when the flare gas driving the shock arrives at the spacecraft. Ions of He-3(+2), O-16(+6), and O-16(+7) have been <span class="hlt">observed</span> with Vela 3 electrostatic analyzers. Further measurements with Vela 5 analyzers have shown the presence of N-14(+6), Si-28(+7) to Si-28(+9) and Fe-56(+7) to Fe-56(+12) ions. The relative abundance of oxygen, silicon, and iron in the <span class="hlt">solar</span> wind of July 6, 1969, was 1.00, 0.21, and 0.17, which is very similar to reported values for the corona. The ratio of helium to oxygen is variable; the average value of He/O is close to 100, but values between 30 and 400 have been <span class="hlt">observed</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720014178','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720014178"><span>Direct <span class="hlt">observations</span> of low-energy <span class="hlt">solar</span> electrons associated with a type 3 <span class="hlt">solar</span> radio burst</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Frank, L. A.; Gurnett, D. A.</p> <p>1972-01-01</p> <p>On 6 April 1971 a <span class="hlt">solar</span> X-ray flare and a type 3 <span class="hlt">solar</span> radio noise burst were <span class="hlt">observed</span> with instrumentation on the eccentric-orbiting satellite IMP 6. The type 3 <span class="hlt">solar</span> radio noise burst was detected down to a frequency of 31 kHz. A highly anisotropic packet of low-energy <span class="hlt">solar</span> electron intensities arrived at the satellite approximately 6000 seconds after the onset of the <span class="hlt">solar</span> flare. This packet of <span class="hlt">solar</span> electron intensities was <span class="hlt">observed</span> for 4200 seconds. Maximum differential intensities of the <span class="hlt">solar</span> electrons were in the energy range of one to several keV. The frequency drift rate of the type 3 radio noise at frequencies below 178 kHz also indicated an average particle speed corresponding to that of a 3-keV electron. The simultaneous <span class="hlt">observations</span> of these <span class="hlt">solar</span> electron intensities and of the type 3 <span class="hlt">solar</span> radio burst are presented, and their interrelationships are explored.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...614A..15Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...614A..15Z"><span>Mutual event <span class="hlt">observations</span> of <span class="hlt">solar</span> <span class="hlt">system</span> objects by SRC on Mars Express. Analysis and release 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>Ziese, R.; Willner, K.</p> <p>2018-06-01</p> <p>Context. Both Martian moons, Phobos and Deimos, have been <span class="hlt">observed</span> during several imaging campaigns by the Super Resolution Channel (SRC) on the Mars Express probe. Several tens of images are obtained during mutual event <span class="hlt">observations</span> - when the Martian moons are both <span class="hlt">observed</span> or together with another <span class="hlt">solar</span> <span class="hlt">system</span> body. These <span class="hlt">observations</span> provide new opportunities to determine the bodies' positions in their orbits. Aims: A method was sought to automate the <span class="hlt">observation</span> of the positions of the imaged bodies. Within one image sequence a similarly accurate localization of the objects in all images should be possible. Methods: Shape models of Phobos and Deimos are applied to simulate the appearance of the bodies in the images. Matching the illuminated simulation against the <span class="hlt">observation</span> provides a reliable determination of the bodies' location within the image. To enhance the matching confidence several corrections need to be applied to the simulation to closely reconstruct the <span class="hlt">observation</span>. Results: A list of 884 relative positions between the different objects is provided through the Centre de Données astronomiques de Strasbourg (CDS). Tables A.1-A.4 are only available at the CDS via anonymous ftp to http://cdsarc.u-strasbg.fr (http://130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/614/A15</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_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_4 --> <div id="page_5" 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_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</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="81"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015nova.pres..313K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015nova.pres..313K"><span>How Normal is Our <span class="hlt">Solar</span> <span class="hlt">System</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kohler, Susanna</p> <p>2015-10-01</p> <p>To date, weve discovered nearly 2000 confirmed exoplanets, as well as thousands of additional candidates. Amidst this vast sea of <span class="hlt">solar</span> <span class="hlt">systems</span>, how special is our own? A new study explores the answer to this question.Analyzing DistributionsKnowing whether our <span class="hlt">solar</span> <span class="hlt">system</span> is unique among exoplanetary <span class="hlt">systems</span> can help us to better understand future <span class="hlt">observations</span> of exoplanets. Furthermore, if our <span class="hlt">solar</span> <span class="hlt">system</span> is typical, this allows us to be optimistic about the possibility of life existing elsewhere in the universe.In a recent study, Rebecca Martin (University of Nevada, Las Vegas) and Mario Livio (Space Telescope Science Institute) examine how normal our <span class="hlt">solar</span> <span class="hlt">system</span> is, by comparing the properties of our planets to the averages obtained from known exoplanets.Comparing PropertiesSo how do we measure up?Densities of planets as a function of their mass. Exoplanets (N=287) are shown in blue, planets in our <span class="hlt">solar</span> <span class="hlt">system</span> are shown in red. [MartinLivio 2015]Planet masses and densitiesThose of the gas giants in our <span class="hlt">solar</span> <span class="hlt">system</span> are pretty typical. The terrestrial planets are on the low side for mass, but thats probably a selection effect: its very difficult to detect low-mass planets.Age of the <span class="hlt">solar</span> <span class="hlt">system</span>Roughly half the stars in the disk of our galaxy are younger than the Sun, and half are older. Were definitely not special in age.Orbital locations of the planetsThis is actually a little strange: our <span class="hlt">solar</span> <span class="hlt">system</span> is lacking close-in planets. All of our planets, in fact, orbit at a distance that is larger than the mean distance <span class="hlt">observed</span> in exoplanetary <span class="hlt">systems</span>. Again, however, this might be a selection effect at work: its easier to detect large planets orbiting very close to their stars.Eccentricities of the planets orbitsOur planets are on very circular orbits and that actually makes us somewhat special too, compared to typical exoplanet <span class="hlt">systems</span>. There is a possible explanation though: eccentricity of orbits tends to decrease with more planets in the <span class="hlt">system</span>. Because</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810064408&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3DDunham','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810064408&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3DDunham"><span>Determination of variations of the <span class="hlt">solar</span> radius from <span class="hlt">solar</span> eclipse <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>Sofia, S.; Dunham, D. W.; Fiala, A. D.</p> <p>1980-01-01</p> <p>This paper describes the method to determine the <span class="hlt">solar</span> radius and its variations from <span class="hlt">observations</span> made during total <span class="hlt">solar</span> eclipses. In particular, the procedure to correct the spherical moon predictions for the effects of lunar mountains and valleys on the width and location of the path of totality is addressed in detail. The errors affecting this technique are addressed, a summary of the results of its application to three <span class="hlt">solar</span> eclipses are presented, and the implications of the results on the constancy of the <span class="hlt">solar</span> constant are described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990hst..prop.2432Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990hst..prop.2432Z"><span>Exceptional <span class="hlt">Solar-System</span> Objects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zellner, Benjamin</p> <p>1990-12-01</p> <p>This is a target-of-opportunity proposal for HST <span class="hlt">observations</span> to be executed if a previously unknown, truly exceptional <span class="hlt">solar-system</span> object or phenomenon is discovered either in the normal course of HST work or by anyone, anywhere. Trails due to unknown moving objects will often appear on HST images made for other purposes. A short trail seen near the opposition point or at high ecliptic latitude could represent a major addition to our knowledge of the <span class="hlt">solar</span> <span class="hlt">system</span>. Thus we further propose that all short trials seen on HST images taken in favorable regions of the sky be given a quick analysis in the <span class="hlt">Observation</span> Support <span class="hlt">System</span> for their possible significance. If an unusual object is found we propose to: (1) Seek from the owner of data rights permission to proceed as may be appropriate; (2) Contact the Minor Planet Center for an evaluation of the significance of the discovery; and (3) For an object that appears to be of great significance where effective groundbased followup appears unlikely, request the HST schedule be replanned for followup images and physical studies using HST.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850023061','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850023061"><span><span class="hlt">Solar</span> dynamic <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dustin, M. O.</p> <p>1985-01-01</p> <p>The development of the <span class="hlt">solar</span> dynamic <span class="hlt">system</span> is discussed. The benefits of the <span class="hlt">solar</span> dynamic <span class="hlt">system</span> over pv <span class="hlt">systems</span> are enumerated. The history of the <span class="hlt">solar</span> dynamic development is recounted. The purpose and approach of the advanced development are outlined. Critical concentrator technology and critical heat recover technology are examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015CEAB...39..109C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015CEAB...39..109C"><span><span class="hlt">Solar</span> and Galactic Cosmic Rays <span class="hlt">Observed</span> by SOHO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Curdt, W.; Fleck, B.</p> <p></p> <p>Both the Cosmic Ray Flux (CRF) and <span class="hlt">Solar</span> Energetic Particles (SEPs) have left an imprint on SOHO technical <span class="hlt">systems</span>. While the <span class="hlt">solar</span> array efficiency degraded irreversibly down to ≈77% of its original level over roughly 1 1/2 <span class="hlt">solar</span> cycles, Single Event Upsets (SEUs) in the solid state recorder (SSR) have been reversed by the memory protection mechanism. We compare the daily CRF <span class="hlt">observed</span> by the Oulu station with the daily SOHO SEU rate and with the degradation curve of the <span class="hlt">solar</span> arrays. The Oulu CRF and the SOHO SSR SEU rate are both modulated by the <span class="hlt">solar</span> cycle and are highly correlated, except for sharp spikes in the SEU rate, caused by isolated SEP events, which also show up as discontinuities in the otherwise slowly decreasing <span class="hlt">solar</span> ray efficiency. This allows to discriminate between effects with <span class="hlt">solar</span> and non-<span class="hlt">solar</span> origin and to compare the relative strength of both. We find that during <span class="hlt">solar</span> cycle 23 (1996 Apr 1 -- 2008 Aug 31) only 6% of the total number of SSR SEUs were caused by SEPs; the remaining 94% were due to galactic cosmic rays. During the maximum period of cycle 23 (2000 Jan 1 -- 2003 Dec 31), the SEP contribution increased to 22%, and during 2001, the year with the highest SEP rate, to 30%. About 40% of the total <span class="hlt">solar</span> array degradation during the 17 years from Jan 1996 through Feb 2013 can be attributed to proton events, i.e. the effect of a series of short-lived, violent SEP events is comparable to the cycle-integrated damage by cosmic rays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930038729&hterms=Prize&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D10%26Ntt%3DPrize','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930038729&hterms=Prize&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D10%26Ntt%3DPrize"><span>1991 Urey Prize Lecture: Physical evolution in the <span class="hlt">solar</span> <span class="hlt">system</span> - Present <span class="hlt">observations</span> as a key to the past</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Binzel, Richard P.</p> <p>1992-01-01</p> <p>The present evaluation of the use of new <span class="hlt">observational</span> methods for exploring <span class="hlt">solar</span> <span class="hlt">system</span> evolutionary processes gives attention to illustrative cases from the constraining of near-earth asteroid sources and the discovery of main-belt asteroid fragments which indicate Vesta to be a source of basaltic achondrite meteorites. The coupling of <span class="hlt">observational</span> constraints with numerical models clarifies cratering and collisional evolution for both main-belt and Trojan asteroids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSH21A4094P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSH21A4094P"><span>Bayesian Analysis Of HMI <span class="hlt">Solar</span> Image <span class="hlt">Observables</span> And Comparison To TSI Variations And MWO Image <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>Parker, D. G.; Ulrich, R. K.; Beck, J.</p> <p>2014-12-01</p> <p>We have previously applied the Bayesian automatic classification <span class="hlt">system</span> AutoClass to <span class="hlt">solar</span> magnetogram and intensity images from the 150 Foot <span class="hlt">Solar</span> Tower at Mount Wilson to identify classes of <span class="hlt">solar</span> surface features associated with variations in total <span class="hlt">solar</span> irradiance (TSI) and, using those identifications, modeled TSI time series with improved accuracy (r > 0.96). (Ulrich, et al, 2010) AutoClass identifies classes by a two-step process in which it: (1) finds, without human supervision, a set of class definitions based on specified attributes of a sample of the image data pixels, such as magnetic field and intensity in the case of MWO images, and (2) applies the class definitions thus found to new data sets to identify automatically in them the classes found in the sample set. HMI high resolution images capture four <span class="hlt">observables</span>-magnetic field, continuum intensity, line depth and line width-in contrast to MWO's two <span class="hlt">observables</span>-magnetic field and intensity. In this study, we apply AutoClass to the HMI <span class="hlt">observables</span> for images from May, 2010 to June, 2014 to identify <span class="hlt">solar</span> surface feature classes. We use contemporaneous TSI measurements to determine whether and how variations in the HMI classes are related to TSI variations and compare the characteristic statistics of the HMI classes to those found from MWO images. We also attempt to derive scale factors between the HMI and MWO magnetic and intensity <span class="hlt">observables</span>. The ability to categorize automatically surface features in the HMI images holds out the promise of consistent, relatively quick and manageable analysis of the large quantity of data available in these images. Given that the classes found in MWO images using AutoClass have been found to improve modeling of TSI, application of AutoClass to the more complex HMI images should enhance understanding of the physical processes at work in <span class="hlt">solar</span> surface features and their implications for the <span class="hlt">solar</span>-terrestrial environment. Ulrich, R.K., Parker, D, Bertello, L. and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800026565&hterms=theories+formation+solar+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtheories%2Bformation%2Bsolar%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800026565&hterms=theories+formation+solar+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtheories%2Bformation%2Bsolar%2Bsystem"><span>New isotopic clues to <span class="hlt">solar</span> <span class="hlt">system</span> formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, T.</p> <p>1979-01-01</p> <p>The presence of two new extinct nuclides Al-26 and Pd-107 with half lives of approximately one million years in the early <span class="hlt">solar</span> <span class="hlt">system</span> implies that there were nucleosynthetic activities involving a great many elements almost at the instant of <span class="hlt">solar</span> <span class="hlt">system</span> formation. Rate gas and oxygen isotopic abundance variations ('anomalies') relative to the 'cosmic' composition were <span class="hlt">observed</span> in a variety of planetary objects, which indicates that isotopic heterogeneities caused by the incomplete mixing of distinct nucleosynthesis components permeate the entire <span class="hlt">solar</span> <span class="hlt">system</span>. These new results have major implications for cosmochronology, nucleosynthesis theory, star formation, planetary heating, and the genetic relationship between different planetary bodies</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1261595','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1261595"><span><span class="hlt">Solar</span> tracking <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Okandan, Murat; Nielson, Gregory N.</p> <p>2016-07-12</p> <p><span class="hlt">Solar</span> tracking <span class="hlt">systems</span>, as well as methods of using such <span class="hlt">solar</span> tracking <span class="hlt">systems</span>, are disclosed. More particularly, embodiments of the <span class="hlt">solar</span> tracking <span class="hlt">systems</span> include lateral supports horizontally positioned between uprights to support photovoltaic modules. The lateral supports may be raised and lowered along the uprights or translated to cause the photovoltaic modules to track the moving sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760044609&hterms=Solar+system+facts&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DSolar%2Bsystem%2Bfacts','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760044609&hterms=Solar+system+facts&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DSolar%2Bsystem%2Bfacts"><span>Structure and evolutionary history of the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Alfven, H.; Arrhenius, G.</p> <p>1975-01-01</p> <p>General principles and <span class="hlt">observational</span> facts concerning the <span class="hlt">solar</span> <span class="hlt">system</span> are examined, taking into account the orbits of planets and satellites, the small bodies, the resonance structure, spin and tides, and postaccretional changes in the <span class="hlt">solar</span> <span class="hlt">system</span>. A description is given of the accretion of celestial bodies and the plasma phase is considered. Aspects of chemical differentiation and the matrix of the groups of bodies are also discussed, giving attention to chemical compositions in the <span class="hlt">solar</span> <span class="hlt">system</span>, meteorites and their precursor states, mass distribution and the critical velocity, and the structure of the groups.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH31B2730P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH31B2730P"><span><span class="hlt">Solar</span> Energetic Particle Composition over Two <span class="hlt">Solar</span> Cycles as <span class="hlt">Observed</span> by the Ulysses/HISCALE and ACE/EPAM Pulse Height Analyzers.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Patterson, J. D.; Madanian, H.; Manweiler, J. W.; Lanzerotti, L. J.</p> <p>2017-12-01</p> <p>We present the compositional variation in the <span class="hlt">Solar</span> Energetic Particle (SEP) population in the inner heliosphere over two <span class="hlt">solar</span> cycles using data from the Ulysses Heliospheric Instrument for Spectra, Composition, and Anisotropy at Low Energies (HISCALE) and Advanced Composition Explorer (ACE) Electron Proton Alpha Monitor (EPAM). The Ulysses mission was active from late 1990 to mid-2009 in a heliopolar orbit inclined by 80° with a perihelion of 1.3 AU and an aphelion of 5.4 AU. The ACE mission has been active since its launch in late 1997 and is in a halo orbit about L1. These two missions provide a total of 27 years of continuous <span class="hlt">observation</span> in the inner heliosphere with twelve years of simultaneous <span class="hlt">observation</span>. HISCALE and EPAM data provide species-resolved differential flux and density of SEP between 0.5-5 MeV/nuc. Several ion species (He, C, O, Ne, Si, Fe) are identified using the Pulse Height Analyzer (PHA) <span class="hlt">system</span> of the Composition Aperture for both instruments. The He density shows a noticeable increase at high <span class="hlt">solar</span> activity followed by a moderate drop at the quiet time of the <span class="hlt">solar</span> minimum between cycles 23 and 24. The density of heavier ions (i.e. O and Fe) change minimally with respect to the F10.7 index variations however, certain energy-specific count rates decrease during <span class="hlt">solar</span> minimum. With Ulysses and ACE <span class="hlt">observing</span> in different regions of the inner heliosphere, there are significant latitudinal differences in how the O/He ratios vary with the <span class="hlt">solar</span> cycle. At <span class="hlt">solar</span> minimum, there is reasonable agreement between the <span class="hlt">observations</span> from both instruments. At <span class="hlt">solar</span> max 23, the differences in composition over the course of the <span class="hlt">solar</span> cycle, and as <span class="hlt">observed</span> at different heliospheric locations can provide insight to the origins of and acceleration processes differentially affecting <span class="hlt">solar</span> energetic ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006cosp...36.1941K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006cosp...36.1941K"><span><span class="hlt">Observational</span> capabilities of <span class="hlt">solar</span> satellite "Coronas-Photon"</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kotov, Yu.</p> <p></p> <p>Coronas-Photon mission is the third satellite of the Russian Coronas program on <span class="hlt">solar</span> activity <span class="hlt">observation</span> The main goal of the Coronas-Photon is the study of <span class="hlt">solar</span> hard electromagnetic radiation in the wide energy range from UV up to high energy gamma-radiation sim 2000MeV Scientific payload for <span class="hlt">solar</span> radiation <span class="hlt">observation</span> consists of three type of instruments 1 monitors Natalya-2M Konus-RF RT-2 Penguin-M BRM Phoka Sphin-X Sokol for spectral and timing measurements of full <span class="hlt">solar</span> disk radiation with timing in flare burst mode up to one msec Instruments Natalya-2M Konus-RF RT-2 will cover the wide energy range of hard X-rays and soft Gamma rays 15keV to 2000MeV and will together constitute the largest area detectors ever used for <span class="hlt">solar</span> <span class="hlt">observations</span> Detectors of gamma-ray monitors are based on structured inorganic scintillators with energy resolution sim 5 for nuclear gamma-line band to 35 for GeV-band PSD analysis is used for gamma neutron separation for <span class="hlt">solar</span> neutron registration T 30MeV Penguin-M has capability to measure linear polarization of hard X-rays using azimuth are measured by Compton scattering asymmetry in case of polarization of an incident flux For X-ray and EUV monitors the scintillation phoswich detectors gas proportional counter CZT assembly and Filter-covered Si-diodes are used 2 Telescope-spectrometer TESIS for imaging <span class="hlt">solar</span> spectroscopy in X-rays with angular resolution up to 1 in three spectral lines and RT-2 CZT assembly of CZT</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.6607M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.6607M"><span>Open Surface <span class="hlt">Solar</span> Irradiance <span class="hlt">Observations</span> - A Challenge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Menard, Lionel; Nüst, Daniel; Jirka, Simon; Maso, Joan; Ranchin, Thierry; Wald, Lucien</p> <p>2015-04-01</p> <p>The newly started project ConnectinGEO funded by the European Commission aims at improving the understanding on which environmental <span class="hlt">observations</span> are currently available in Europe and subsequently providing an informational basis to close gaps in diverse <span class="hlt">observation</span> networks. The project complements supporting actions and networking activities with practical challenges to test and improve the procedures and methods for identifying <span class="hlt">observation</span> data gaps, and to ensure viability in real world scenarios. We present a challenge on future concepts for building a data sharing portal for the <span class="hlt">solar</span> energy industry as well as the state of the art in the domain. Decision makers and project developers of <span class="hlt">solar</span> power plants have identified the Surface <span class="hlt">Solar</span> Irradiance (SSI) and its components as an important factor for their business development. SSI <span class="hlt">observations</span> are crucial in the process of selecting suitable locations for building new plants. Since in-situ pyranometric stations form a sparse network, the search for locations starts with global satellite data and is followed by the deployment of in-situ sensors in selected areas for at least one year. To form a convincing picture, answers must be sought in the conjunction of these EO <span class="hlt">systems</span>, and although companies collecting SSI <span class="hlt">observations</span> are willing to share this information, the means to exchange in-situ measurements across companies and between stakeholders in the market are still missing. We present a solution for interoperable exchange of SSI data comprising in-situ time-series <span class="hlt">observations</span> as well as sensor descriptions based on practical experiences from other domains. More concretely, we will apply concepts and implementations of the Sensor Web Enablement (SWE) framework of the Open Geospatial Consortium (OGC). The work is based on an existing spatial data infrastructure (SDI), which currently comprises metadata, maps and coverage data, but no in-situ <span class="hlt">observations</span> yet. This catalogue is already registered in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=solar+AND+energy+AND+effective&pg=2&id=ED204536','ERIC'); return false;" href="https://eric.ed.gov/?q=solar+AND+energy+AND+effective&pg=2&id=ED204536"><span><span class="hlt">Solar</span> Energy: <span class="hlt">Solar</span> <span class="hlt">System</span> Economics.</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>Knapp, Henry H., III</p> <p></p> <p>This module on <span class="hlt">solar</span> <span class="hlt">system</span> economics is one of six in a series intended for use as supplements to currently available materials on <span class="hlt">solar</span> energy and energy conservation. Together with the recommended texts and references (sources are identified), these modules provide an effective introduction to energy conservation and <span class="hlt">solar</span> energy technologies.…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890027241&hterms=theories+formation+solar+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dtheories%2Bformation%2Bsolar%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890027241&hterms=theories+formation+solar+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dtheories%2Bformation%2Bsolar%2Bsystem"><span>Origin of the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cameron, A. G. W.</p> <p>1988-01-01</p> <p>The current status of the classical model of <span class="hlt">solar-system</span> formation is surveyed, reviewing the results of recent <span class="hlt">observational</span> and theoretical investigations. Topics addressed include interstellar clouds, the collapse of interstellar gas, the primitive <span class="hlt">solar</span> nebula, the formation of the sun, planetesimal accumulation, planetary accumulation, major planetary collisions, the development of planetary atmospheres, and comets. The relative merits of conflicting theories on many key problems are indicated, with reference to more detailed reviews in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SunGe...1a..68S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SunGe...1a..68S"><span>Derivation of Heliophysical Scientific Data from Amateur <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Eclipses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stoev, A. D.; Stoeva, P. V.</p> <p>2006-03-01</p> <p>The basic scientific aims and <span class="hlt">observational</span> experiments included in the complex <span class="hlt">observational</span> program - Total <span class="hlt">Solar</span> Eclipse '99 - are described in the work. Results from teaching and training students of total <span class="hlt">solar</span> eclipse (TSE) <span class="hlt">observation</span> in the Public Astronomical Observatory (PAO) in Stara Zagora and their selection for participation in different <span class="hlt">observational</span> teams are also discussed. During the final stage, a special <span class="hlt">system</span> of methods for investigation of the level of pretensions (the level of ambition as to what he/she feels capable of achieving in the context of problem solving/<span class="hlt">observation</span>) of the students is applied. Results obtained from the <span class="hlt">observational</span> experiments are interpreted mainly in the following themes: Investigation of the structure of the white-light <span class="hlt">solar</span> corona and evolution of separate coronal elements during the total phase of the eclipse; Photometry of the white-light <span class="hlt">solar</span> corona and specific emission lines; Meteorological, actinometrical and optical atmospheric investigations; Astrometry of the Moon during the phase evolution of the eclipse; Biological and behavioral reactions of highly organized colonies (ants and bats) during the eclipse. It is also shown that data processing, <span class="hlt">observational</span> results and their interpretation, presentation and publishing in specialized and amateur editions is a peak in the independent creative activity of students and amateur astronomers. This enables students from the Astronomy schools at Public Astronomical Observatories and Planetariums (PAOP) to develop creative skills, emotional - volitional personal qualities, orientation towards scientific work, <span class="hlt">observations</span> and experiments, and build an effective scientific style of thinking.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150008788&hterms=sail+make&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsail%2Bmake','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150008788&hterms=sail+make&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsail%2Bmake"><span>Hybrids of <span class="hlt">Solar</span> Sail, <span class="hlt">Solar</span> Electric, and <span class="hlt">Solar</span> Thermal Propulsion for <span class="hlt">Solar-System</span> Exploration</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wilcox, Brian H.</p> <p>2012-01-01</p> <p><span class="hlt">Solar</span> sails have long been known to be an attractive method of propulsion in the inner <span class="hlt">solar</span> <span class="hlt">system</span> if the areal density of the overall spacecraft (S/C) could be reduced to approx.10 g/sq m. It has also long been recognized that the figure (precise shape) of useful <span class="hlt">solar</span> sails needs to be reasonably good, so that the reflected light goes mostly in the desired direction. If one could make large reflective surfaces with reasonable figure at an areal density of approx.10 g/sq m, then several other attractive options emerge. One is to use such sails as <span class="hlt">solar</span> concentrators for <span class="hlt">solar</span>-electric propulsion. Current flight <span class="hlt">solar</span> arrays have a specific output of approx. 100W/kg at 1 Astronomical Unit (AU) from the sun, and near-term advances promise to significantly increase this figure. A S/C with an areal density of 10 g/sq m could accelerate up to 29 km/s per year as a <span class="hlt">solar</span> sail at 1 AU. Using the same sail as a concentrator at 30 AU, the same spacecraft could have up to approx. 45 W of electric power per kg of total S/C mass available for electric propulsion (EP). With an EP <span class="hlt">system</span> that is 50% power-efficient, exhausting 10% of the initial S/C mass per year as propellant, the exhaust velocity is approx. 119 km/s and the acceleration is approx. 12 km/s per year. This hybrid thus opens attractive options for missions to the outer <span class="hlt">solar</span> <span class="hlt">system</span>, including sample-return missions. If <span class="hlt">solar</span>-thermal propulsion were perfected, it would offer an attractive intermediate between <span class="hlt">solar</span> sailing in the inner <span class="hlt">solar</span> <span class="hlt">system</span> and <span class="hlt">solar</span> electric propulsion for the outer <span class="hlt">solar</span> <span class="hlt">system</span>. In the example above, both the <span class="hlt">solar</span> sail and <span class="hlt">solar</span> electric <span class="hlt">systems</span> don't have a specific impulse that is near-optimal for the mission. <span class="hlt">Solar</span> thermal propulsion, with an exhaust velocity of the order of 10 km/s, is better matched to many <span class="hlt">solar</span> <span class="hlt">system</span> exploration missions. This paper derives the basic relationships between these three propulsion options and gives examples of missions that might be enabled by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012hell.conf....5M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012hell.conf....5M"><span><span class="hlt">Solar</span> <span class="hlt">observations</span> with a low frequency radio telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Myserlis, I.; Seiradakis, J.; Dogramatzidis, M.</p> <p>2012-01-01</p> <p>We have set up a low frequency radio monitoring station for <span class="hlt">solar</span> bursts at the Observatory of the Aristotle University in Thessaloniki. The station consists of a dual dipole phased array, a radio receiver and a dedicated computer with the necessary software installed. The constructed radio receiver is based on NASA's Radio Jove project. It operates continuously, since July 2010, at 20.1 MHz (close to the long-wavelength ionospheric cut-off of the radio window) with a narrow bandwidth (~5 kHz). The <span class="hlt">system</span> is properly calibrated, so that the recorded data are expressed in antenna temperature. Despite the high interference level of an urban region like Thessaloniki (strong broadcasting shortwave radio stations, periodic experimental signals, CBs, etc), we have detected several low frequency <span class="hlt">solar</span> radio bursts and correlated them with <span class="hlt">solar</span> flares, X-ray events and other low frequency <span class="hlt">solar</span> <span class="hlt">observations</span>. The received signal is monitored in ordinary ASCII format and as audio signal, in order to investigate and exclude man-made radio interference. In order to exclude narrow band interference and calculate the spectral indices of the <span class="hlt">observed</span> events, a second monitoring station, working at 36 MHz, is under construction at the village of Nikiforos near the town of Drama, about 130 km away of Thessaloniki. Finally, we plan to construct a third monitoring station at 58 MHz, in Thessaloniki. This frequency was revealed to be relatively free of interference, after a thorough investigation of the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Ge%26Ae..56.1095T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Ge%26Ae..56.1095T"><span>Forecast of <span class="hlt">solar</span> wind parameters according to STOP magnetograph <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>Tlatov, A. G.; Pashchenko, M. P.; Ponyavin, D. I.; Svidskii, P. M.; Peshcherov, V. S.; Demidov, M. L.</p> <p>2016-12-01</p> <p>The paper discusses the results of the forecast of <span class="hlt">solar</span> wind parameters at a distance of 1 AU made according to <span class="hlt">observations</span> made by the STOP telescope magnetograph during 2014-2015. The Wang-Sheeley-Arge (WSA) empirical model is used to reconstruct the magnetic field topology in the <span class="hlt">solar</span> corona and estimate the <span class="hlt">solar</span> wind speed in the interplanetary medium. The proposed model is adapted to STOP magnetograph <span class="hlt">observations</span>. The results of the calculation of <span class="hlt">solar</span> wind parameters are compared with ACE satellite measurements. It is shown that the use of STOP <span class="hlt">observations</span> provides a significant correlation of predicted <span class="hlt">solar</span> wind speed values with the <span class="hlt">observed</span> ones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140010032','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140010032"><span>Characterizing Cold Giant Planets in Reflected Light: Lessons from 50 Years of Outer <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration and <span class="hlt">Observation</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marley, Mark Scott; Hammel, Heidi</p> <p>2014-01-01</p> <p>A space based coronagraph, whether as part of the WFIRST/AFTA mission or on a dedicated space telescope such as Exo-C or -S, will be able to obtain photometry and spectra of multiple gas giant planets around nearby stars, including many known from radial velocity detections. Such <span class="hlt">observations</span> will constrain the masses, atmospheric compositions, clouds, and photochemistry of these worlds. Giant planet albedo models, such as those of Cahoy et al. (2010) and Lewis et al. (this meeting), will be crucial for mission planning and interpreting the data. However it is equally important that insights gleaned from decades of <span class="hlt">solar</span> <span class="hlt">system</span> imaging and spectroscopy of giant planets be leveraged to optimize both instrument design and data interpretation. To illustrate these points we will draw on examples from <span class="hlt">solar</span> <span class="hlt">system</span> <span class="hlt">observations</span>, by both HST and ground based telescopes, as well as by Voyager, Galileo, and Cassini, to demonstrate the importance clouds, photochemical hazes, and various molecular absorbers play in sculpting the light scattered by <span class="hlt">solar</span> <span class="hlt">system</span> giant planets. We will demonstrate how measurements of the relative depths of multiple methane absorption bands of varying strengths have been key to disentangling the competing effects of gas column abundances, variations in cloud height and opacity, and scattering by high altitude photochemical hazes. We will highlight both the successes, such as the accurate remote determination of the atmospheric methane abundance of Jupiter, and a few failures from these types of <span class="hlt">observations</span>. These lessons provide insights into technical issues facing spacecraft designers, from the selection of the most valuable camera filters to carry to the required capabilities of the flight spectrometer, as well as mission design questions such as choosing the most favorable phase angles for atmospheric characterization.</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_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_5 --> <div id="page_6" 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_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</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="101"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.1460L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.1460L"><span><span class="hlt">Observed</span> Reduction In Surface <span class="hlt">Solar</span> Radiation - Aerosol Forcing Versus Cloud Feedback?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liepert, B.</p> <p></p> <p>The <span class="hlt">solar</span> radiation reaching the ground is a key parameter for the climate <span class="hlt">system</span>. It drives the hydrological cycle and numerous biological processes. Surface <span class="hlt">solar</span> radi- ation revealed an estimated 7W/m2 or 4% decline at sites worldwide from 1961 to 1990. The strongest decline occurred at the United States sites with 19W/m2 or 10%. Increasing air pollution and hence direct and indirect aerosol effect, as we know today can only explain part of the reduction in <span class="hlt">solar</span> radiation. Increasing cloud optical thick- ness - possibly due to global warming - is a more likely explanation for the <span class="hlt">observed</span> reduction in <span class="hlt">solar</span> radiation in the United States. The analysis of surface <span class="hlt">solar</span> radiation data will be shown and compared with GCM results of the direct and indirect aerosol effect. It will be argued that the residual declines in surface <span class="hlt">solar</span> radiation is likely due to cloud feedback.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH12A..04K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH12A..04K"><span>Helioseismology <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Cycles and Dynamo Modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kosovichev, A. G.; Guerrero, G.; Pipin, V.</p> <p>2017-12-01</p> <p>Helioseismology <span class="hlt">observations</span> from the SOHO and SDO, obtained in 1996-2017, provide unique insight into the dynamics of the Sun's deep interior for two <span class="hlt">solar</span> cycles. The data allow us to investigate variations of the <span class="hlt">solar</span> interior structure and dynamics, and compare these variations with dynamo models and simulations. We use results of the local and global helioseismology data processing pipelines at the SDO Joint Science Operations Center (Stanford University) to study <span class="hlt">solar</span>-cycle variations of the differential rotation, meridional circulation, large-scale flows and global asphericity. By comparing the helioseismology results with the evolution of surface magnetic fields we identify characteristic changes associated the initiation and development of <span class="hlt">Solar</span> Cycles 23 and 24. For the physical interpretation of <span class="hlt">observed</span> variations, the results are compared with the current mean-field dynamo models and 3D MHD dynamo simulations. It is shown that the helioseismology inferences provide important constraints on the <span class="hlt">solar</span> dynamo mechanism, may explain the fundamental difference between the two <span class="hlt">solar</span> cycles, and also give information about the next <span class="hlt">solar</span> cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980193221','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980193221"><span>Star Formation and the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bally, John; Boss, Alan; Papanastassiou, Dimitri; Sandford, Scott; Sargent, Anneila</p> <p>1988-01-01</p> <p>We have seen that studies of nearby star-forming regions are beginning to reveal the first signs of protoplanetary disks. Studies of interstellar and interplanetary grains are starting to provide clues about the processing and incorporation of matter into the <span class="hlt">Solar</span> <span class="hlt">System</span>. Studies of meteorites have yielded isotopic anomalies which indicate that some of the grains and inclusions in these bodies are very primitive. Although we have not yet detected a true interstellar grain, some of these materials have not been extensively modified since their removal from the ISM. We are indeed close to seeing our interstellar heritage. The overlap between astronomical and <span class="hlt">Solar</span> <span class="hlt">System</span> studies is in its infancy. What future experiments, <span class="hlt">observations</span>, and missions can be performed in the near future that will greatly enhance our understanding of star formation and the formation of the <span class="hlt">Solar</span> <span class="hlt">System</span>?</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21700869','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21700869"><span>A 15N-poor isotopic composition for the <span class="hlt">solar</span> <span class="hlt">system</span> as shown by Genesis <span class="hlt">solar</span> wind samples.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Marty, B; Chaussidon, M; Wiens, R C; Jurewicz, A J G; Burnett, D S</p> <p>2011-06-24</p> <p>The Genesis mission sampled <span class="hlt">solar</span> wind ions to document the elemental and isotopic compositions of the Sun and, by inference, of the protosolar nebula. Nitrogen was a key target element because the extent and origin of its isotopic variations in <span class="hlt">solar</span> <span class="hlt">system</span> materials remain unknown. Isotopic analysis of a Genesis <span class="hlt">Solar</span> Wind Concentrator target material shows that implanted <span class="hlt">solar</span> wind nitrogen has a (15)N/(14)N ratio of 2.18 ± 0.02 × 10(-3) (that is, ≈40% poorer in (15)N relative to terrestrial atmosphere). The (15)N/(14)N ratio of the protosolar nebula was 2.27 ± 0.03 × 10(-3), which is the lowest (15)N/(14)N ratio known for <span class="hlt">solar</span> <span class="hlt">system</span> objects. This result demonstrates the extreme nitrogen isotopic heterogeneity of the nascent <span class="hlt">solar</span> <span class="hlt">system</span> and accounts for the (15)N-depleted components <span class="hlt">observed</span> in <span class="hlt">solar</span> <span class="hlt">system</span> reservoirs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090004577','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090004577"><span><span class="hlt">Solar</span> Power <span class="hlt">System</span> Design for the <span class="hlt">Solar</span> Probe+ Mission</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Landis, Geoffrey A.; Schmitz, Paul C.; Kinnison, James; Fraeman, Martin; Roufberg, Lew; Vernon, Steve; Wirzburger, Melissa</p> <p>2008-01-01</p> <p><span class="hlt">Solar</span> Probe+ is an ambitious mission proposed to the <span class="hlt">solar</span> corona, designed to make a perihelion approach of 9 <span class="hlt">solar</span> radii from the surface of the sun. The high temperature, high <span class="hlt">solar</span> flux environment makes this mission a significant challenge for power <span class="hlt">system</span> design. This paper summarizes the power <span class="hlt">system</span> conceptual design for the <span class="hlt">solar</span> probe mission. Power supplies considered included nuclear, <span class="hlt">solar</span> thermoelectric generation, <span class="hlt">solar</span> dynamic generation using Stirling engines, and <span class="hlt">solar</span> photovoltaic generation. The <span class="hlt">solar</span> probe mission ranges from a starting distance from the sun of 1 AU, to a minimum distance of about 9.5 <span class="hlt">solar</span> radii, or 0.044 AU, from the center of the sun. During the mission, the <span class="hlt">solar</span> intensity ranges from one to about 510 times AM0. This requires power <span class="hlt">systems</span> that can operate over nearly three orders of magnitude of incident intensity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020087784','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020087784"><span><span class="hlt">Solar</span> Electric <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1987-01-01</p> <p>Heat Pipe Technology, Inc. undertook the development of a PV <span class="hlt">system</span> that could bring <span class="hlt">solar</span> electricity to the individual home at reasonable cost. His <span class="hlt">system</span> employs high efficiency PV modules plus a set of polished reflectors that concentrate the <span class="hlt">solar</span> energy and enhance the output of the modules. Dinh incorporated a sun tracking <span class="hlt">system</span> derived from space tracking technology. It automatically follows the sun throughout the day and turns the modules so that they get maximum exposure to the <span class="hlt">solar</span> radiation, further enhancing the <span class="hlt">system</span> efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770019112','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770019112"><span>Large-Scale periodic <span class="hlt">solar</span> velocities: An <span class="hlt">observational</span> study</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dittmer, P. H.</p> <p>1977-01-01</p> <p><span class="hlt">Observations</span> of large-scale <span class="hlt">solar</span> velocities were made using the mean field telescope and Babcock magnetograph of the Stanford <span class="hlt">Solar</span> Observatory. <span class="hlt">Observations</span> were made in the magnetically insensitive ion line at 5124 A, with light from the center (limb) of the disk right (left) circularly polarized, so that the magnetograph measures the difference in wavelength between center and limb. Computer calculations are made of the wavelength difference produced by global pulsations for spherical harmonics up to second order and of the signal produced by displacing the <span class="hlt">solar</span> image relative to polarizing optics or diffraction grating.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984spin.rept...78.','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984spin.rept...78."><span><span class="hlt">Solar</span> Energy <span class="hlt">Systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p>1984-01-01</p> <p>Calibrated in kilowatt hours per square meter, the <span class="hlt">solar</span> counter produced by Dodge Products, Inc. provides a numerical count of the <span class="hlt">solar</span> energy that has accumulated on a surface. <span class="hlt">Solar</span> energy sensing, measuring and recording devices in corporate <span class="hlt">solar</span> cell technology developed by Lewis Research Center. Customers for their various devices include architects, engineers and others engaged in construction and operation of <span class="hlt">solar</span> energy facilities; manufacturers of <span class="hlt">solar</span> <span class="hlt">systems</span> or <span class="hlt">solar</span> related products, such as glare reducing windows; and <span class="hlt">solar</span> energy planners in federal and state government agencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170002331&hterms=solar+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsolar%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170002331&hterms=solar+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsolar%2Bsystem"><span>James Webb Space Telescope <span class="hlt">Observations</span> of Stellar Occultations by <span class="hlt">Solar</span> <span class="hlt">System</span> Bodies and Rings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Santos-Sanz, P.; French, R. G.; Pinilla-Alonso, N.; Stansberry, J.; Lin, Z-Y.; Zhang, Z-W.; Vilenius, E.; Mueller, Th.; Ortiz, J. L.; Braga-Ribas, F.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170002331'); toggleEditAbsImage('author_20170002331_show'); toggleEditAbsImage('author_20170002331_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170002331_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170002331_hide"></p> <p>2016-01-01</p> <p>In this paper, we investigate the opportunities provided by the James Webb Space Telescope (JWST) for significant scientific advances in the study of <span class="hlt">Solar</span> <span class="hlt">System</span> bodies and rings using stellar occultations. The strengths and weaknesses of the stellar occultation technique are evaluated in light of JWST's unique capabilities. We identify several possible JWST occultation events by minor bodies and rings and evaluate their potential scientific value. These predictions depend critically on accurate a priori knowledge of the orbit of JWST near the Sun–Earth Lagrange point 2 (L2). We also explore the possibility of serendipitous stellar occultations by very small minor bodies as a byproduct of other JWST <span class="hlt">observing</span> programs. Finally, to optimize the potential scientific return of stellar occultation <span class="hlt">observations</span>, we identify several characteristics of JWST's orbit and instrumentation that should be taken into account during JWST's development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011epsc.conf..883R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011epsc.conf..883R"><span>Communicating Herschel Key Programs in <span class="hlt">Solar</span> <span class="hlt">System</span> Studies to the Public</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rengel, M.; Hartogh, P.; Müller, T.</p> <p>2011-10-01</p> <p>The Herschel Space Observatory, one of the cornerstone missions of the European Space Agency (ESA) with participation from NASA, is delivering a wealth of far-infrared and sub-millimeter <span class="hlt">observations</span> of the cold Universe. A considerable part of the <span class="hlt">observing</span> time for the nominal three year mission lifetime has been awarded in the form of Key Programs. Between the 42 key programs (guaranteed and open times), only two key programs are dedicated to study the <span class="hlt">Solar</span> <span class="hlt">System</span>: "Water and Related Chemistry in the <span class="hlt">Solar</span> <span class="hlt">System</span>", also known as Herschel <span class="hlt">Solar</span> <span class="hlt">System</span> <span class="hlt">Observations</span> (HssO) project [1], and "TNOs are Cool: A Survey of the Transneptunian Region" [2]. In the framework of these Programs, a serie of public outreach activities and efforts of its results are being carried out. We present some of the outreach strategies developed (e.g. press releases, web pages, logos, public lectures, exhibitions, interviews, reports, etc.) and some plans in this direction. Our activities introduce people to knowledge and beauty of <span class="hlt">solar</span> <span class="hlt">system</span> research and wider the opportunities for the public to become more involved in topics like <span class="hlt">solar</span> <span class="hlt">system</span> studies, specially in the times of frequent exo-planet discoveries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Ap%26SS.363..118L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Ap%26SS.363..118L"><span>Piecewise mass flows within a <span class="hlt">solar</span> prominence <span class="hlt">observed</span> by the New Vacuum <span class="hlt">Solar</span> Telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Hongbo; Liu, Yu; Tam, Kuan Vai; Zhao, Mingyu; Zhang, Xuefei</p> <p>2018-06-01</p> <p>The material of <span class="hlt">solar</span> prominences is often <span class="hlt">observed</span> in a state of flowing. These mass flows (MF) are important and useful for us to understand the internal structure and dynamics of prominences. In this paper, we present a high resolution Hα <span class="hlt">observation</span> of MFs within a quiescent <span class="hlt">solar</span> prominence. From the <span class="hlt">observation</span>, we find that the plasma primarily has a circular motion and a downward motion separately in the middle section and legs of the prominence, which creates a piecewise mass flow along the <span class="hlt">observed</span> prominence. Moreover, the <span class="hlt">observation</span> also shows a clear displacement of MF's velocity peaks in the middle section of the prominence. All of these provide us with a detailed record of MFs within a <span class="hlt">solar</span> prominence and show a new approach to detecting the physical properties of prominence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED204537.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED204537.pdf"><span><span class="hlt">Solar</span> Energy: <span class="hlt">Solar</span> <span class="hlt">System</span> Design Fundamentals.</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>Knapp, Henry H., III</p> <p></p> <p>This module on <span class="hlt">solar</span> <span class="hlt">system</span> design fundamentals is one of six in a series intended for use as supplements to currently available materials on <span class="hlt">solar</span> energy and energy conservation. Together with the recommended texts and references (sources are identified), these modules provide an effective introduction to energy conservation and <span class="hlt">solar</span> energy…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040074235&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Denergy%2Bsolar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040074235&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Denergy%2Bsolar"><span><span class="hlt">Solar</span> Flares <span class="hlt">Observed</span> with the Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager (RHESSI)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holman, Gordon D.</p> <p>2004-01-01</p> <p><span class="hlt">Solar</span> flares are impressive examples of explosive energy release in unconfined, magnetized plasma. It is generally believed that the flare energy is derived from the coronal magnetic field. However, we have not been able to establish the specific energy release mechanism(s) or the relative partitioning of the released energy between heating, particle acceleration (electrons and ions), and mass motions. NASA's RHESSI Mission was designed to study the acceleration and evolution of electrons and ions in flares by <span class="hlt">observing</span> the X-ray and gamma-ray emissions these energetic particles produce. This is accomplished through the combination of high-resolution spectroscopy and spectroscopic imaging, including the first images of flares in gamma rays. RHESSI has <span class="hlt">observed</span> over 12,000 <span class="hlt">solar</span> flares since its launch on February 5, 2002. I will demonstrate how we use the RHESSI spectra to deduce physical properties of accelerated electrons and hot plasma in flares. Using images to estimate volumes, w e typically find that the total energy in accelerated electrons is comparable to that in the thermal plasma. I will also present flare <span class="hlt">observations</span> that provide strong support for the presence of magnetic reconnection in a large-scale, vertical current sheet in the <span class="hlt">solar</span> corona. RHESSI <span class="hlt">observations</span> such as these are allowing us to probe more deeply into the physics of <span class="hlt">solar</span> flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Ap%26SS.361..159L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Ap%26SS.361..159L"><span>Mass motion in upper <span class="hlt">solar</span> chromosphere detected from <span class="hlt">solar</span> eclipse <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>Li, Zhi; Qu, Zhongquan; Yan, Xiaoli; Dun, Guangtao; Chang, Liang</p> <p>2016-05-01</p> <p>The eclipse-<span class="hlt">observed</span> emission lines formed in the upper <span class="hlt">solar</span> atmosphere can be used to diagnose the atmosphere dynamics which provides an insight to the energy balance of the outer atmosphere. In this paper, we analyze the spectra formed in the upper chromospheric region by a new instrument called Fiber Arrayed <span class="hlt">Solar</span> Optic Telescope (FASOT) around the Gabon total <span class="hlt">solar</span> eclipse on November 3, 2013. The double Gaussian fits of the <span class="hlt">observed</span> profiles are adopted to show enhanced emission in line wings, while red-blue (RB) asymmetry analysis informs that the cool line (about 104 K) profiles can be decomposed into two components and the secondary component is revealed to have a relative velocity of about 16-45 km s^{-1}. The other profiles can be reproduced approximately with single Gaussian fits. From these fittings, it is found that the matter in the upper <span class="hlt">solar</span> chromosphere is highly dynamic. The motion component along the line-of-sight has a pattern asymmetric about the local <span class="hlt">solar</span> radius. Most materials undergo significant red shift motions while a little matter show blue shift. Despite the discrepancy of the motion in different lines, we find that the width and the Doppler shifts both are function of the wavelength. These results may help us to understand the complex mass cycle between chromosphere and corona.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860027605&hterms=RELATIVITY&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DRELATIVITY','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860027605&hterms=RELATIVITY&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DRELATIVITY"><span>Testing relativity with <span class="hlt">solar</span> <span class="hlt">system</span> dynamics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hellings, R. W.</p> <p>1984-01-01</p> <p>A major breakthrough is described in the accuracy of <span class="hlt">Solar</span> <span class="hlt">System</span> dynamical tests of relativistic gravity. The breakthrough was achieved by factoring in ranging data from Viking Landers 1 and 2 from the surface of Mars. Other key data sources included optical transit circle <span class="hlt">observations</span>, lunar laser ranging, planetary radar, and spacecraft (Mariner 9 to Mars and Mariner 10 to Mercury). The <span class="hlt">Solar</span> <span class="hlt">System</span> model which is used to fit the data and the process by which such fits are performed are explained and results are discussed. The results are fully consistent with the predictions of General Relativity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3627923','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3627923"><span>Three-dimensional exploration of the <span class="hlt">solar</span> wind using <span class="hlt">observations</span> of interplanetary scintillation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>TOKUMARU, Munetoshi</p> <p>2013-01-01</p> <p>The <span class="hlt">solar</span> wind, a supersonic plasma flow continuously emanating from the Sun, governs the space environment in a vast region extending to the boundary of the heliosphere (∼100 AU). Precise understanding of the <span class="hlt">solar</span> wind is of importance not only because it will satisfy scientific interest in an enigmatic astrophysical phenomenon, but because it has broad impacts on relevant fields. Interplanetary scintillation (IPS) of compact radio sources at meter to centimeter wavelengths serves as a useful ground-based method for investigating the <span class="hlt">solar</span> wind. IPS measurements of the <span class="hlt">solar</span> wind at a frequency of 327 MHz have been carried out regularly since the 1980s using the multi-station <span class="hlt">system</span> of the <span class="hlt">Solar</span>-Terrestrial Environment Laboratory (STEL) of Nagoya University. This paper reviews new aspects of the <span class="hlt">solar</span> wind revealed from our IPS <span class="hlt">observations</span>. PMID:23391604</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910009603','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910009603"><span>Simultaneous <span class="hlt">Solar</span> Maximum Mission (SMM) and Very Large Array (VLA) <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Willson, Robert F.</p> <p>1991-01-01</p> <p>Very Large Array <span class="hlt">observations</span> at 20 cm wavelength can detect the hot coronal plasma previously <span class="hlt">observed</span> at soft x ray wavelengths. Thermal cyclotron line emission was detected at the apex of coronal loops where the magnetic field strength is relatively constant. Detailed comparison of simultaneous <span class="hlt">Solar</span> Maximum Mission (SMM) Satellite and VLA data indicate that physical parameters such as electron temperature, electron density, and magnetic field strength can be obtained, but that some coronal loops remain invisible in either spectral domain. The unprecedent spatial resolution of the VLA at 20 cm wavelength showed that the precursor, impulsive, and post-flare components of <span class="hlt">solar</span> bursts originate in nearby, but separate loops or <span class="hlt">systems</span> of loops.. In some cases preburst heating and magnetic changes are <span class="hlt">observed</span> from loops tens of minutes prior to the impulsive phase. Comparisons with soft x ray images and spectra and with hard x ray data specify the magnetic field strength and emission mechanism of flaring coronal loops. At the longer 91 cm wavelength, the VLA detected extensive emission interpreted as a hot 10(exp 5) K interface between cool, dense H alpha filaments and the surrounding hotter, rarefield corona. <span class="hlt">Observations</span> at 91 cm also provide evidence for time-correlated bursts in active regions on opposite sides of the <span class="hlt">solar</span> equator; they are attributed to flare triggering by relativistic particles that move along large-scale, otherwise-invisible, magnetic conduits that link active regions in opposite hemispheres of the Sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018nova.pres.3196H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018nova.pres.3196H"><span>Probing the Structure of Our <span class="hlt">Solar</span> <span class="hlt">System</span>'s Edge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hensley, Kerry</p> <p>2018-02-01</p> <p>The boundary between the <span class="hlt">solar</span> wind and the interstellar medium (ISM) at the distant edge of our <span class="hlt">solar</span> <span class="hlt">system</span> has been probed remotely and directly by spacecraft, but questions about its properties persist. What can models tell us about the structure of this region?The Heliopause: A Dynamic BoundarySchematic illustrating different boundaries of our <span class="hlt">solar</span> <span class="hlt">system</span> and the locations of the Voyager spacecraft. [Walt Feimer/NASA GSFCs Conceptual Image Lab]As our <span class="hlt">solar</span> <span class="hlt">system</span> travels through interstellar space, the magnetized <span class="hlt">solar</span> wind flows outward and pushes back on the oncoming ISM, forming a bubble called the heliosphere. The clash of plasmas generates a boundary region called the heliopause, the shape of which depends strongly on the properties of the <span class="hlt">solar</span> wind and the local ISM.Much of our understanding of the outer heliosphere and the local ISM comes from <span class="hlt">observations</span> made by the International Boundary Explorer (IBEX) and the Voyager 1 and Voyager 2 spacecraft. IBEX makes global maps of the flux of neutral atoms, while Voyagers 1 and 2 record the plasma density and magnetic field parameters along their trajectories as they exit the <span class="hlt">solar</span> <span class="hlt">system</span>. In order to interpret the IBEX and Voyager <span class="hlt">observations</span>, astronomers rely on complex models that must capture both global and local effects.Simulations of the plasma density in the meridional plane of the heliosphere due to the interaction of the <span class="hlt">solar</span> wind with the ISM for the case of a relatively dense ISM with a weak magnetic field. [Adapted from Pogorelov et al. 2017]Modeling the Edge of the <span class="hlt">Solar</span> <span class="hlt">System</span>In this study, Nikolai Pogorelov (University of Alabama in Huntsville) and collaborators use a hybrid magneto-hydrodynamical (MHD) and kinetic simulation to capture fully the physical processes happening in the outer heliosphere.MHD models have been used to understand many aspects of plasma flow in the heliosphere. However, they struggle to capture processes that are better described kinetically, like charge exchange</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JAVSO..41R.149H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JAVSO..41R.149H"><span>AAVSO <span class="hlt">Solar</span> <span class="hlt">Observers</span> Worldwide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Howe, R.</p> <p>2013-06-01</p> <p>(Abstract only) For visual <span class="hlt">solar</span> <span class="hlt">observers</span> there has been no biological change in the "detector" (human eye) - at century scales (eye + visual cortex) does not change much over time. Our capacity to "integrate" seeing distortions is not just simple averaging! The visual cortex plays an essential role, and until recently only the SDO-HMI (<span class="hlt">Solar</span> Dynamics Observatory, Helioseismic and Magnetic Imager) has had the capacity to detect the smallest sunspots, called pores. Prior to this the eye was superior to photography and CCD. Imaged data are not directly comparable or substitutable to counts by eye, as the effects of sensor/optical resolution and seeing will have a different influence on the resulting sunspot counts for images when compared to the human eye. Also contributing to the complex task of counting sunspots is differentiating between a sunspot (which is usually defined as having a darker center (umbra) and lighter outer ring (penumbra)) and a pore, made even more complex by the conflicting definitions of the word "pore" in the <span class="hlt">solar</span> context: "pore" can mean a small spot without penumbra or "pore" can mean a random intergranular blemish that is not a true sunspot. The overall agreement is that the smallest spot size is near 2,000 km or ~3 arc sec, (Loughhead, R. E. and Bray, R. J. 1961, Australian J. Phys., 14, 347). Sunspot size is dictated by granulation dynamics rather than spot size (cancellation of convective motion), and by the lifetime of the pore, which averages from 10 to 30 minutes. There is no specific aperture required for AAVSO <span class="hlt">observers</span> contributing sunspot <span class="hlt">observations</span>. However, the detection of the smallest spots is influenced by the resolution of the telescope. Two factors to consider are the theoretical optical resolution (unobstructed aperture), Rayleigh criterion: theta = 138 / D(mm), and Dawes criterion: theta = 116 / D(mm) (http://www.telescope-optics.net/telescope_resolution.htm). However, seeing is variable with time; daytime range will</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000934.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000934.html"><span>NASA's SDO <span class="hlt">Observes</span> an X-class <span class="hlt">Solar</span> Flare</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2017-12-08</p> <p>The sun emitted a significant <span class="hlt">solar</span> flare, peaking at 1:01 a.m. EDT on Oct. 19, 2014. NASA's <span class="hlt">Solar</span> Dynamics Observatory, which is always <span class="hlt">observing</span> the sun, captured an image of the event. <span class="hlt">Solar</span> flares are powerful bursts of radiation. Harmful radiation from a flare cannot pass through Earth's atmosphere to physically affect humans on the ground, however -- when intense enough -- they can disturb the atmosphere in the layer where GPS and communications signals travel. To see how this event may affect Earth, please visit NOAA's Space Weather Prediction Center at spaceweather.gov, the U.S. government's official source for space weather forecasts, alerts, watches and warnings. This flare is classified as an X1.1-class flare. X-class denotes the most intense flares, while the number provides more information about its strength. An X2 is twice as intense as an X1, an X3 is three times as intense, etc. Credit: NASA/SDO NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</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_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" 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_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</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="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170002362&hterms=PLAN&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DPLAN','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170002362&hterms=PLAN&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DPLAN"><span>The James Webb Space Telescope's Plan for Operations and Instrument Capabilities for <span class="hlt">Observations</span> in the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Milam, Stefanie N.; Stansberry, John A.; Sonneborn, George; Thomas, Cristina</p> <p>2016-01-01</p> <p>The James Webb Space Telescope (JWST) is optimized for <span class="hlt">observations</span> in the near- and mid-infrared and will provide essential <span class="hlt">observations</span> for targets that cannot be conducted from the ground or other missions during its lifetime. The state-of-the-art science instruments, along with the telescope's moving target tracking, will enable the infrared study, with unprecedented detail, for nearly every object (Mars and beyond) in the <span class="hlt">Solar</span> <span class="hlt">System</span>. The goals of this special issue are to stimulate discussion and encourage participation in JWST planning among members of the planetary science community. Key science goals for various targets, <span class="hlt">observing</span> capabilities for JWST, and highlights for the complementary nature with other missions/observatories are described in this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999spro.proc...41G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999spro.proc...41G"><span>Physics of the <span class="hlt">Solar</span> Active Regions from 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>Gelfreikh, G. B.</p> <p>1999-12-01</p> <p>Localized increase of the magnetic field <span class="hlt">observed</span> by routine methods on the photosphere result in the growth of a number of active processes in the <span class="hlt">solar</span> atmosphere and the heliosphere. These localized regions of increased magnetic field are called active regions (AR). The main processes of transfer, accumulation and release of energy in an AR is, however, out of scope of photospheric <span class="hlt">observations</span> being essentially a 3D-process and happening either under photosphere or up in the corona. So, to investigate these plasma structures and processes we are bound to use either extrapolation of optical <span class="hlt">observational</span> methods or <span class="hlt">observations</span> in EUV, X-rays and radio. In this review, we stress and illustrate the input to the problem gained from radio astronomical methods and discuss possible future development of their applicatications. Historically speaking each new step in developing radio technique of <span class="hlt">observations</span> resulted in detecting some new physics of ARs. The most significant progress in the last few years in radio diagnostics of the plasma structures of magnetospheres of the <span class="hlt">solar</span> ARs is connected with the developing of the 2D full disk analysis on regular basis made at Nobeyama and detailed multichannel spectral-polarization (but one-dimensional and one per day) <span class="hlt">solar</span> <span class="hlt">observations</span> at the RATAN-600. In this report the bulk of attention is paid to the new approach to the study of <span class="hlt">solar</span> activity gained with the Nobeyama radioheliograph and analyzing the ways for future progress. The most important new features of the multicomponent radio sources of the ARs studied using Nobeyama radioheliograph are as follow: 1. The analysis of magnetic field structures in <span class="hlt">solar</span> corona above sunspot with 2000 G. Their temporal evolution and fluctuations with the periods around 3 and 5 minutes, due to MHD-waves in sunspot magnetic tubes and surrounding plasma. These investigations are certainly based on an analysis of thermal cyclotron emission of lower corona and CCTR above sunspot</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900007302','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900007302"><span>Non-equilibrium chemistry in the <span class="hlt">solar</span> nebula and early <span class="hlt">solar</span> <span class="hlt">system</span>: Implications for the chemistry of comets</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fegley, Bruce, Jr.</p> <p>1989-01-01</p> <p>Theoretical models of <span class="hlt">solar</span> nebula and early <span class="hlt">solar</span> <span class="hlt">system</span> chemistry which take into account the interplay between chemical, physical, and dynamical processes have great utility for deciphering the origin and evolution of the abundant chemically reactive volatiles (H, O, C, N, S) <span class="hlt">observed</span> in comets. In particular, such models are essential for attempting to distinguish between presolar and <span class="hlt">solar</span> nebula products and for quantifying the nature and duration of nebular and early <span class="hlt">solar</span> <span class="hlt">system</span> processing to which the volatile constituents of comets have been subjected. The diverse processes and energy sources responsible for chemical processing in the <span class="hlt">solar</span> nebula and early <span class="hlt">solar</span> <span class="hlt">system</span> are discussed. The processes considered include homogeneous and heterogeneous thermochemical and photochemical reactions, and disequilibration resulting from fluid transport, condensation, and cooling whenever they occur on timescales shorter than those for chemical reactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9914E..21C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9914E..21C"><span>Strategies on <span class="hlt">solar</span> <span class="hlt">observation</span> of Atacama Large Millimeter/submillimeter Array (ALMA) band-1 receiver</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chiong, Chau-Ching; Chiang, Po-Han; Hwang, Yuh-Jing; Huang, Yau-De</p> <p>2016-07-01</p> <p>ALMA covering 35-950 GHz is the largest existing telescope array in the world. Among the 10 receiver bands, Band-1, which covers 35-50 GHz, is the lowest. Due to its small dimension and its time-variant frequency-dependent gain characteristics, current <span class="hlt">solar</span> filter located above the cryostat cannot be applied to Band-1 for <span class="hlt">solar</span> <span class="hlt">observation</span>. Here we thus adopt new strategies to fulfill the goals. Thanks to the flexible dc biasing scheme of the HEMT-based amplifier in Band-1 front-end, bias adjustment of the cryogenic low noise amplifier is investigated to accomplish <span class="hlt">solar</span> <span class="hlt">observation</span> without using <span class="hlt">solar</span> filter. Large power handling range can be achieved by the de-tuning bias technique with little degradation in <span class="hlt">system</span> performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4840508H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4840508H"><span>Astrometry of <span class="hlt">Solar</span> <span class="hlt">System</span> Objects with Gaia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hestroffer, Daniel J.; Arenou, Frederic; Desmars, Josselin; Robert, Vincent; Thuillot, William; Arlot, Jean-Eudes; Carry, Benoit; David, Pedro; Eggl, Siegfried; Fabricius, Claus; Kudryashova, Maria; Lainey, Valery; Spoto, Federica; Tanga, Paolo; Gaia DPAC</p> <p>2016-10-01</p> <p>The Gaia ESA space mission will provide astrometric <span class="hlt">observations</span> of a large number of celestial bodies, with unprecedented accuracy, and in an homogenous reference frame (to become the optical ICRF). The Gaia satellite is monitoring regularly the whole celestial sphere, with one complete scan in about 6month, down to approximately magnitude V≤20.7. It will provide after its nominal lifetime, (5 years, 2014-2019) about 70 astrometric points for several hundred thousands of <span class="hlt">solar</span> <span class="hlt">system</span> objects, asteroids from the Near-Earth region to Centaurs and bright TNOs, as well as planetary satellites and comets. The highly precise astrometric and photometric data is bound to lead to huge advances in the science of small Small <span class="hlt">Solar</span> <span class="hlt">System</span> Bodies (e.g. Tanga et al. 2016 P\\&SS, Hestroffer et al. 2014 COSPAR #40 ; Mignard et al. 2007 EMP).The first Gaia data release (GDR#1) is foreseen for Q3-2016 and will provide highly precise positions of selected stars down to mag V≈20. While <span class="hlt">solar</span> <span class="hlt">system</span> objets data is foreseen for the next data release (in 2017), science of <span class="hlt">Solar</span> <span class="hlt">System</span> will also highly benefit from the Gaia stellar catalogue. We will present the status of the satellite and Gaia mission, and details on the stellar data that will be published in this GDR#1. We discuss the catalogue content, number of stars, parameters and precisions, and the process of cross-matching and validation. We also touch upon the construction of combined Tycho-Gaia TGAS catalogue.A Gaia data daily processing is devoted to the identification of <span class="hlt">Solar</span> <span class="hlt">System</span> Objects. During this process the detection of new (or critical) objects arises and leads to the triggering of scientific alerts to be found on the web gaiafunsso.imcce.fr. We have also set up an international follow-up network called Gaia-FUN-SSO to validate the detection in space. For this goal, in case of detection the <span class="hlt">observational</span> data must be sent to the MPC by the <span class="hlt">observers</span>. Besides, Gaia should benefit for the classical astrometric</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950022709','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950022709"><span><span class="hlt">Solar</span> <span class="hlt">system</span> plasma waves</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gurnett, Donald A.</p> <p>1995-01-01</p> <p>An overview is given of spacecraft <span class="hlt">observations</span> of plasma waves in the <span class="hlt">solar</span> <span class="hlt">system</span>. In situ measurements of plasma phenomena have now been obtained at all of the planets except Mercury and Pluto, and in the interplanetary medium at heliocentric radial distances ranging from 0.29 to 58 AU. To illustrate the range of phenomena involved, we discuss plasma waves in three regions of physical interest: (1) planetary radiation belts, (2) planetary auroral acceleration regions and (3) the <span class="hlt">solar</span> wind. In each region we describe examples of plasma waves that are of some importance, either due to the role they play in determining the physical properties of the plasma, or to the unique mechanism involved in their generation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28983209','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28983209"><span>Modeling <span class="hlt">observations</span> of <span class="hlt">solar</span> coronal mass ejections with heliospheric imagers verified with the Heliophysics <span class="hlt">System</span> Observatory.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Möstl, C; Isavnin, A; Boakes, P D; Kilpua, E K J; Davies, J A; Harrison, R A; Barnes, D; Krupar, V; Eastwood, J P; Good, S W; Forsyth, R J; Bothmer, V; Reiss, M A; Amerstorfer, T; Winslow, R M; Anderson, B J; Philpott, L C; Rodriguez, L; Rouillard, A P; Gallagher, P; Nieves-Chinchilla, T; Zhang, T L</p> <p>2017-07-01</p> <p>We present an advance toward accurately predicting the arrivals of coronal mass ejections (CMEs) at the terrestrial planets, including Earth. For the first time, we are able to assess a CME prediction model using data over two thirds of a <span class="hlt">solar</span> cycle of <span class="hlt">observations</span> with the Heliophysics <span class="hlt">System</span> Observatory. We validate modeling results of 1337 CMEs <span class="hlt">observed</span> with the <span class="hlt">Solar</span> Terrestrial Relations Observatory (STEREO) heliospheric imagers (HI) (science data) from 8 years of <span class="hlt">observations</span> by five in situ <span class="hlt">observing</span> spacecraft. We use the self-similar expansion model for CME fronts assuming 60° longitudinal width, constant speed, and constant propagation direction. With these assumptions we find that 23%-35% of all CMEs that were predicted to hit a certain spacecraft lead to clear in situ signatures, so that for one correct prediction, two to three false alarms would have been issued. In addition, we find that the prediction accuracy does not degrade with the HI longitudinal separation from Earth. Predicted arrival times are on average within 2.6 ± 16.6 h difference of the in situ arrival time, similar to analytical and numerical modeling, and a true skill statistic of 0.21. We also discuss various factors that may improve the accuracy of space weather forecasting using wide-angle heliospheric imager <span class="hlt">observations</span>. These results form a first-order approximated baseline of the prediction accuracy that is possible with HI and other methods used for data by an operational space weather mission at the Sun-Earth L5 point.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5601179','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5601179"><span>Modeling <span class="hlt">observations</span> of <span class="hlt">solar</span> coronal mass ejections with heliospheric imagers verified with the Heliophysics <span class="hlt">System</span> Observatory</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Isavnin, A.; Boakes, P. D.; Kilpua, E. K. J.; Davies, J. A.; Harrison, R. A.; Barnes, D.; Krupar, V.; Eastwood, J. P.; Good, S. W.; Forsyth, R. J.; Bothmer, V.; Reiss, M. A.; Amerstorfer, T.; Winslow, R. M.; Anderson, B. J.; Philpott, L. C.; Rodriguez, L.; Rouillard, A. P.; Gallagher, P.; Nieves‐Chinchilla, T.; Zhang, T. L.</p> <p>2017-01-01</p> <p>Abstract We present an advance toward accurately predicting the arrivals of coronal mass ejections (CMEs) at the terrestrial planets, including Earth. For the first time, we are able to assess a CME prediction model using data over two thirds of a <span class="hlt">solar</span> cycle of <span class="hlt">observations</span> with the Heliophysics <span class="hlt">System</span> Observatory. We validate modeling results of 1337 CMEs <span class="hlt">observed</span> with the <span class="hlt">Solar</span> Terrestrial Relations Observatory (STEREO) heliospheric imagers (HI) (science data) from 8 years of <span class="hlt">observations</span> by five in situ <span class="hlt">observing</span> spacecraft. We use the self‐similar expansion model for CME fronts assuming 60° longitudinal width, constant speed, and constant propagation direction. With these assumptions we find that 23%–35% of all CMEs that were predicted to hit a certain spacecraft lead to clear in situ signatures, so that for one correct prediction, two to three false alarms would have been issued. In addition, we find that the prediction accuracy does not degrade with the HI longitudinal separation from Earth. Predicted arrival times are on average within 2.6 ± 16.6 h difference of the in situ arrival time, similar to analytical and numerical modeling, and a true skill statistic of 0.21. We also discuss various factors that may improve the accuracy of space weather forecasting using wide‐angle heliospheric imager <span class="hlt">observations</span>. These results form a first‐order approximated baseline of the prediction accuracy that is possible with HI and other methods used for data by an operational space weather mission at the Sun‐Earth L5 point. PMID:28983209</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017xru..conf....9D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017xru..conf....9D"><span>X-rays from the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dennerl, K.</p> <p>2017-10-01</p> <p>While the beginning of X-ray astronomy was motivated by <span class="hlt">solar</span> <span class="hlt">system</span> studies (Sun and Moon), the main research interest soon shifted outwards to much more distant and exotic objects. However, the ROSAT discovery of X-rays from comets in 1996 and the insight that this `new' kind of X-ray emission, charge exchange, was underestimated for a long time, has demonstrated that <span class="hlt">solar</span> <span class="hlt">system</span> studies are still important for X-ray astrophysics in general. While comets provide the best case for studying the physics of charge exchange, the X-ray signatures of this process have now also been detected at Venus, Mars, and Jupiter, thanks to Chandra and XMM-Newton. An analysis of the X-ray data of <span class="hlt">solar</span> <span class="hlt">system</span> objects, however, is challenging in many respects. This is particularly true for comets, which appear as moving, extended X-ray sources, emitting a line-rich spectrum at low energies. Especially for XMM-Newton, which has the unparalleled capability to <span class="hlt">observe</span> with five highly sensitive X-ray instruments plus an optical monitor simultaneously, it is a long way towards photometrically and spectroscopically calibrated results, which are consistent between all its instruments. I will show this in my talk, where I will also summarize the current state of <span class="hlt">solar</span> <span class="hlt">system</span> X-ray research.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH23D2703P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH23D2703P"><span>The <span class="hlt">Solar</span> Wind from Pseudostreamers and their Environs: Opportunities for <span class="hlt">Observations</span> with Parker <span class="hlt">Solar</span> Probe and <span class="hlt">Solar</span> Orbiter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Panasenco, O.; Velli, M.; Panasenco, A.; Lionello, R.</p> <p>2017-12-01</p> <p>The <span class="hlt">solar</span> dynamo and photospheric convection lead to three main types of structures extending from the <span class="hlt">solar</span> surface into the corona - active regions, <span class="hlt">solar</span> filaments (prominences when <span class="hlt">observed</span> at the limb) and coronal holes. These structures exist over a wide range of scales, and are interlinked with each other in evolution and dynamics. Active regions can form clusters of magnetic activity and the strongest overlie sunspots. In the decay of active regions, the boundaries separating opposite magnetic polarities (neutral lines) develop specific structures called filament channels above which filaments form. In the presence of flux imbalance decaying active regions can also give birth to lower latitude coronal holes. The accumulation of magnetic flux at coronal hole boundaries also creates conditions for filament formation: polar crown filaments are permanently present at the boundaries of the polar coronal holes. Mid-latitude and equatorial coronal holes - the result of active region evolution - can create pseudostreamers if other coronal holes of the same polarity are present. While helmet streamers form between open fields of opposite polarities, the pseudostreamer, characterized by a smaller coronal imprint, typically shows a more prominent straight ray or stalk extending from the corona. The pseudostreamer base at photospheric heights is multipolar; often one <span class="hlt">observes</span> tripolar magnetic configurations with two neutral lines - where filaments can form - separating the coronal holes. Here we discuss the specific role of filament channels on pseudostreamer topology and on <span class="hlt">solar</span> wind properties. 1D numerical analysis of pseudostreamers shows that the properties of the <span class="hlt">solar</span> wind from around PSs depend on the presence/absence of filament channels, number of channels and chirality at thepseudostreamer base low in the corona. We review and model possible coronal magnetic configurations and <span class="hlt">solar</span> wind plasma properties at different distances from the <span class="hlt">solar</span> surface that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110005625','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110005625"><span><span class="hlt">Solar</span> Flare Impulsive Phase <span class="hlt">Observations</span> from SDO and Other Observatories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chamberlin, Phillip C.; Woods, Thomas N.; Schrijver, Karel; Warren, Harry; Milligan, Ryan; Christe, Steven; Brosius, Jeffrey W.</p> <p>2010-01-01</p> <p>With the start of normal operations of the <span class="hlt">Solar</span> Dynamics Observatory in May 2010, the Extreme ultraviolet Variability Experiment (EVE) and the Atmospheric Imaging Assembly (AIA) have been returning the most accurate <span class="hlt">solar</span> XUV and EUV measurements every 10 and 12 seconds, respectively, at almost 100% duty cycle. The focus of the presentation will be the <span class="hlt">solar</span> flare impulsive phase <span class="hlt">observations</span> provided by EVE and AIA and what these <span class="hlt">observations</span> can tell us about the evolution of the initial phase of <span class="hlt">solar</span> flares. Also emphasized throughout is how simultaneous <span class="hlt">observations</span> with other instruments, such as RHESSI, SOHO-CDS, and HINODE-EIS, will help provide a more complete characterization of the <span class="hlt">solar</span> flares and the evolution and energetics during the impulsive phase. These co-temporal <span class="hlt">observations</span> from the other <span class="hlt">solar</span> instruments can provide information such as extending the high temperature range spectra and images beyond that provided by the EUV and XUV wavelengths, provide electron density input into the lower atmosphere at the footpoints, and provide plasma flows of chromospheric evaporation, among other characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120016043','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120016043"><span>ROSAT <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Wind Charge Exchange with the Lunar Exosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Collier, Michael R.; Snowden, S. L.; Benna, M.; Carter, J. A.; Cravens, T. E.; Hills, H. Kent; Hodges, R. R.; Kuntz, K. D.; Porter, F. Scott; Read, A.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20120016043'); toggleEditAbsImage('author_20120016043_show'); toggleEditAbsImage('author_20120016043_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20120016043_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20120016043_hide"></p> <p>2012-01-01</p> <p>We analyze the ROSAT PSPC soft X-ray image of the Moon taken on 29 June 1990 by examining the radial profile of the count rate in three wedges, two wedges (one north and one south) 13-32 degrees off (19 degrees wide) the terminator towards the dark side and one wedge 38 degrees wide centered on the anti-<span class="hlt">solar</span> direction. The radial profiles of both the north and the south wedges show substantial limb brightening that is absent in the 38 degree wide antisolar wedge. An analysis of the count rate increase associated with the limb brightening shows that its magnitude is consistent with that expected due to <span class="hlt">solar</span> wind charge exchange (SWCX) with the tenuous lunar atmosphere. Along with Mars, Venus, and Earth, the Moon represents another <span class="hlt">solar</span> <span class="hlt">system</span> body at which <span class="hlt">solar</span> wind charge exchange has been <span class="hlt">observed</span>. This technique can be used to explore the <span class="hlt">solar</span> wind-lunar interaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030004996','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030004996"><span>Homemade <span class="hlt">Solar</span> <span class="hlt">Systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1981-01-01</p> <p>Through the use of NASA Tech Briefs, Peter Kask, was able to build a <span class="hlt">solarized</span> domestic hot water <span class="hlt">system</span>. Also by applying NASA's <span class="hlt">solar</span> energy design information, he was able to build a swimming pool heating <span class="hlt">system</span> with minimal outlay for materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JSWSC...6A..40M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JSWSC...6A..40M"><span><span class="hlt">Solar</span> spectral irradiance variability in cycle 24: <span class="hlt">observations</span> and models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marchenko, Sergey V.; DeLand, Matthew T.; Lean, Judith L.</p> <p>2016-12-01</p> <p>Utilizing the excellent stability of the Ozone Monitoring Instrument (OMI), we characterize both short-term (<span class="hlt">solar</span> rotation) and long-term (<span class="hlt">solar</span> cycle) changes of the <span class="hlt">solar</span> spectral irradiance (SSI) between 265 and 500 nm during the ongoing cycle 24. We supplement the OMI data with concurrent <span class="hlt">observations</span> from the Global Ozone Monitoring Experiment-2 (GOME-2) and <span class="hlt">Solar</span> Radiation and Climate Experiment (SORCE) instruments and find fair-to-excellent, depending on wavelength, agreement among the <span class="hlt">observations</span>, and predictions of the Naval Research Laboratory <span class="hlt">Solar</span> Spectral Irradiance (NRLSSI2) and Spectral And Total Irradiance REconstruction for the Satellite era (SATIRE-S) models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780019580&hterms=solar+photovoltaic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsolar%2Bphotovoltaic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780019580&hterms=solar+photovoltaic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsolar%2Bphotovoltaic"><span><span class="hlt">Solar</span> photovoltaic <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Forney, R. G.</p> <p>1978-01-01</p> <p>The Department of Energy's photovoltaic program is outlined. The main objective of the program is the development of low cost reliable terrestrial photovoltaic <span class="hlt">systems</span>. A second objective is to foster widespread use of the <span class="hlt">system</span> in residential, industrial and commercial application. The <span class="hlt">system</span> is reviewed by examining each component; silicon <span class="hlt">solar</span> cell, silicon <span class="hlt">solar</span> cell modules, advanced development modules and power <span class="hlt">systems</span>. Cost and applications of the <span class="hlt">system</span> are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AmJPh..85..485P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AmJPh..85..485P"><span>Resource Letter OSE-1: <span class="hlt">Observing</span> <span class="hlt">Solar</span> Eclipses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, Jay M.; Fraknoi, Andrew</p> <p>2017-07-01</p> <p>This Resource Letter provides a guide to the available literature, listing selected books, articles, and online resources about scientific, cultural, and practical issues related to <span class="hlt">observing</span> <span class="hlt">solar</span> eclipses. It is timely, given that a total <span class="hlt">solar</span> eclipse will cross the continental United States on August 21, 2017. The next total <span class="hlt">solar</span> eclipse path crossing the U.S. and Canada will be on April 8, 2024. In 2023, the path of annularity of an annular eclipse will cross Mexico, the United States, and Canada, with partial phases visible throughout those countries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950033056&hterms=physical+activity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dphysical%2Bactivity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950033056&hterms=physical+activity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dphysical%2Bactivity"><span><span class="hlt">Observations</span> of hysteresis in <span class="hlt">solar</span> cycle variations among seven <span class="hlt">solar</span> activity indicators</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bachmann, Kurt T.; White, Oran R.</p> <p>1994-01-01</p> <p>We show that smoothed time series of 7 indices of <span class="hlt">solar</span> activity exhibit significant <span class="hlt">solar</span> cycle dependent differences in their relative variations during the past 20 years. In some cases these <span class="hlt">observed</span> hysteresis patterns start to repeat over more than one <span class="hlt">solar</span> cycle, giving evidence that this is a normal feature of <span class="hlt">solar</span> variability. Among the indices we study, we find that the hysteresis effects are approximately simple phase shifts, and we quantify these phase shifts in terms of lag times behind the leading index, the International Sunspot Number. Our measured lag times range from less than one month to greater than four months and can be much larger than lag times estimated from short-term variations of these same activity indices during the emergence and decay of major active regions. We argue that hysteresis represents a real delay in the onset and decline of <span class="hlt">solar</span> activity and is an important clue in the search for physical processes responsible for changing <span class="hlt">solar</span> emission at various wavelengths.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060047740&hterms=Solar+still&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DSolar%2Bstill','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060047740&hterms=Solar+still&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DSolar%2Bstill"><span>Initiation of <span class="hlt">Solar</span> Eruptions: Recent <span class="hlt">Observations</span> and Implications for Theories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, A. C.</p> <p>2006-01-01</p> <p><span class="hlt">Solar</span> eruptions involve the violent disruption of a <span class="hlt">system</span> of magnetic field. Just how the field is destabilized and explodes to produce flares and coronal mass ejections (CMEs) is still being debated in the <span class="hlt">solar</span> community. Here I discuss recent <span class="hlt">observational</span> work into these questions by ourselves (me and my colleagues) and others. Our work has concentrated mainly on eruptions that include filaments. We use the filament motion early in the event as a tracer of the motion of the general erupting coronal field in and around the filament, since that field itself is hard to distinguish otherwise. Our main data sources are EUV images from SOHO/EIT and TRACE, soft Xray images from Yohkoh, and magnetograms from SOHO/MDI, supplemented with coronagraph images from SOHO/LASCO, hard X-ray data, and ground-based <span class="hlt">observations</span>. We consider the <span class="hlt">observational</span> findings in terms of three proposed eruption-initiation mechanisms: (i) runaway internal tether-cutting reconnection, (ii) slow external tether-cutting reconnection ("breakout"), and (iii) ideal MHD instability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030025688','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030025688"><span>Wind <span class="hlt">Observations</span> of Anomalous Cosmic Rays from <span class="hlt">Solar</span> Minimum to Maximum</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reames, D. V.; McDonald, F. B.</p> <p>2003-01-01</p> <p>We report the first <span class="hlt">observation</span> near Earth of the time behavior of anomalous cosmic-ray N, O, and Ne ions through the period surrounding the maximum of the <span class="hlt">solar</span> cycle. These <span class="hlt">observations</span> were made by the Wind spacecraft during the 1995-2002 period spanning times from <span class="hlt">solar</span> minimum through <span class="hlt">solar</span> maximum. Comparison of anomalous and galactic cosmic rays provides a powerful tool for the study of the physics of <span class="hlt">solar</span> modulation throughout the <span class="hlt">solar</span> cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P11D..08D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P11D..08D"><span>Effects of <span class="hlt">Solar</span> Irradiance on Ion Fluxes at Mars. MARS EXPRESS and 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>Dubinin, E.; Fraenz, M.; McFadden, J. P.; Eparvier, F. G.; Brain, D. A.; Jakosky, B. M.; Andrews, D. J.; Barbash, S.</p> <p>2016-12-01</p> <p>Recent <span class="hlt">observations</span> by Mars Express and MAVEN spacecraft have shown that the Martian atmosphere/ionosphere is exposed to the impact of <span class="hlt">solar</span> wind which results in losses of volatiles from Mars. This erosion is an important factor for the evolution of the Martian atmosphere and its water inventory. To estimate the escape forced by the <span class="hlt">solar</span> wind during the early <span class="hlt">Solar</span> <span class="hlt">system</span> conditions we need to know how the ionosphere of Mars and escape fluxes depend on variations in the strength of the external drivers, in particularly, of <span class="hlt">solar</span> wind and <span class="hlt">solar</span> EUV flux. We present multi-instrument <span class="hlt">observations</span> of the influence of the <span class="hlt">solar</span> irradiance on the Martian ionosphere and escape fluxes. We use data obtained by the ASPERA-3 and MARSIS experiments on Mars Express and by the STATIC instrument and EUV monitor on MAVEN. <span class="hlt">Observations</span> by Mars Express supplemented by the EUV monitoring at Earth orbit and translated to Mars orbit provide us information about this dependence over more than 10 years whereas the measurements made by MAVEN provide us for the first time the opportunity to study these processes with simultaneous monitoring of the ionospheric variations, planetary ion fluxes and <span class="hlt">solar</span> irradiance. We can show that fluxes of planetary ions through different escape channels (trans-terminator fluxes, ion plume, plasma sheet) respond differently on the EUV variations. The most significant effect on the ion scavenging with increase of the <span class="hlt">solar</span> irradiance is <span class="hlt">observed</span> for low energy ions extracted from the ionosphere while the ion fluxes in the plume are almost insensitive to the EUV variations.</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_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" 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_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</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="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984EOSTr..65R..97R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984EOSTr..65R..97R"><span>New <span class="hlt">solar</span> <span class="hlt">systems</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reichhardt, Tony</p> <p></p> <p>A team of astronomers from UCLA, Cornell University, and the University of Hawaii have discovered what may be two new planetary <span class="hlt">systems</span> aborning around young stars in the constellations Taurus and Monoceros. The team's ground-based infrared <span class="hlt">observations</span> of HL Tau and R Mon reveal features similar to those seen around Vega and Fomalhaut last year by NASA's Infrared Astronomical Satellite (IRAS)—disks of very fine dust particles extending outward from a central star. If current theories about <span class="hlt">solar</span> <span class="hlt">system</span> formation are correct, then those disks most likely represent an early evolutionary step in the formation of planets.Using the technique of speckle interferometry to counter the effects of atmospheric distortion, Steven Beckwith of Cornell, Benjamin Zuckerman of UCLA, Melvin Dyck of the University of Hawaii, and Cornell graduate student Michael Skrutskie were able to make the <span class="hlt">observations</span> using telescopes on Mauna Kea in Hawaii and Kitt Peak in Arizona. What they saw in both cases was short-wavelength infrared starlight being scattered by dust particles surrounding the star. In the case of HL Tau, the dusty “cloud” appears to extend out about 160 Astronomical Units from the star (4 times as wide as our <span class="hlt">solar</span> <span class="hlt">system</span>) in the east-west direction, but only half that far in the north-south direction. The explanation, according to Beckwith, is that “we're looking at a tilted disk rather than an oblate spheroid.” The cloud, in other words, is neither exactly edge-on nor face-on as seen from earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFMSH23C..01T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFMSH23C..01T"><span>A hybrid <span class="hlt">system</span> for <span class="hlt">solar</span> irradiance specification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tobiska, W.; Bouwer, S.</p> <p>2006-12-01</p> <p>Space environment research and space weather operations require <span class="hlt">solar</span> irradiances in a variety of time scales and spectral formats. We describe the development of <span class="hlt">solar</span> irradiance characterization using four models and <span class="hlt">systems</span> that are also used for space weather operations. The four models/<span class="hlt">systems</span> include <span class="hlt">SOLAR</span>2000 (S2K), SOLARFLARE (SFLR), APEX, and IDAR, which are used by Space Environment Technologies (SET) to provide <span class="hlt">solar</span> irradiances from the soft X-rays through the visible spectrum. SFLR uses the GOES 0.1 0.8 nm X-rays in combination with a Mewe model subroutine to provide 0.1 30.0 nm irradiances at 0.1 nm spectral resolution, at 1 minute time resolution, and in a 6-hour XUV EUV spectral <span class="hlt">solar</span> flare evolution forecast with a 7 minute latency and a 2 minute cadence. These irradiances have been calibrated with the SORCE XPS <span class="hlt">observations</span> and we report on the inclusion of these irradiances into the S2K model. The APEX <span class="hlt">system</span> is a real-time data retrieval <span class="hlt">system</span> developed in conjunction with the University of Southern California Space Sciences Center (SSC) to provide SOHO SEM data processing and distribution. SSC provides the updated SEM data to the research community and SET provides the operational data to the space operations community. We describe how the SOHO SEM data, and especially the new S10.7 index, is being integrated directly into the S2K model for space weather operations. The IDAR <span class="hlt">system</span> has been developed by SET to extract coronal hole boundaries, streamers, coronal loops, active regions, plage, network, and background (internetwork) features from <span class="hlt">solar</span> images for comparison with <span class="hlt">solar</span> magnetic features. S2K, SFLR, APEX, and IDAR outputs are integrated through the S2K <span class="hlt">solar</span> irradiance platform that has become a hybrid <span class="hlt">system</span>, i.e., a <span class="hlt">system</span> that is able to produce irradiances using different processes, including empirical and physics-based models combined with real-time data integration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003779&hterms=hodge&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhodge','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003779&hterms=hodge&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhodge"><span>The HEXITEC Hard X-Ray Pixelated CdTe Imager for Fast <span class="hlt">Solar</span> <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>Baumgartner, Wayne H.; Christe, Steven D.; Ryan, Daniel; Inglis, Andrew R.; Shih, Albert Y.; Gregory, Kyle; Wilson, Matt; Seller, Paul; Gaskin, Jessica; Wilson-Hodge, Colleen</p> <p>2016-01-01</p> <p>There is an increasing demand in <span class="hlt">solar</span> and astrophysics for high resolution X-ray spectroscopic imaging. Such <span class="hlt">observations</span> would present ground breaking opportunities to study the poorly understood high energy processes in our <span class="hlt">solar</span> <span class="hlt">system</span> and beyond, such as <span class="hlt">solar</span> flares, X-ray binaries, and active galactic nuclei. However, such <span class="hlt">observations</span> require a new breed of solid state detectors sensitive to high energy X-rays with fine independent pixels to sub-sample the point spread function (PSF) of the X-ray optics. For <span class="hlt">solar</span> <span class="hlt">observations</span> in particular, they must also be capable of handling very high count rates as photon fluxes from <span class="hlt">solar</span> flares often cause pile up and saturation in present generation detectors. The Rutherford Appleton Laboratory (RAL) has recently developed a new cadmium telluride (CdTe) detector <span class="hlt">system</span>, called HEXITEC (High Energy X-ray Imaging Technology). It is an 80 x 80 array of 250 micron independent pixels sensitive in the 2-200 keV band and capable of a high full frame read out rate of 10 kHz. HEXITEC provides the smallest independently read out CdTe pixels currently available, and are well matched to the few arcsecond PSF produced by current and next generation hard X-ray focusing optics. NASA's Goddard and Marshall Space Flight Centers are collaborating with RAL to develop these detectors for use on future space borne hard X-ray focusing telescopes. We show the latest results on HEXITEC's imaging capability, energy resolution, high read out rate, and reveal it to be ideal for such future instruments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770038231&hterms=fossils&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dfossils','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770038231&hterms=fossils&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dfossils"><span>Aluminum-26 in the early <span class="hlt">solar</span> <span class="hlt">system</span> - Fossil or fuel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, T.; Papanastassiou, D. A.; Wasserburg, G. J.</p> <p>1977-01-01</p> <p>The isotopic composition of Mg was measured in different phases of a Ca-Al-rich inclusion in the Allende meteorite. Large excesses of Mg-26 of up to 10% were found. These excesses correlate strictly with the Al-27/Mg-24 ratio for four coexisting phases with distinctive chemical compositions. Models of in situ decay of Al-26 within the <span class="hlt">solar</span> <span class="hlt">system</span> and of mixing of interstellar dust grains containing fossil Al-26 with normal <span class="hlt">solar</span> <span class="hlt">system</span> material are presented. The <span class="hlt">observed</span> correlation provides definitive evidence for the presence of Al-26 in the early <span class="hlt">solar</span> <span class="hlt">system</span>. This requires either injection of freshly synthesized nucleosynthetic material into the <span class="hlt">solar</span> <span class="hlt">system</span> immediately before condensation and planet formation, or local production within the <span class="hlt">solar</span> <span class="hlt">system</span> by intense activity of the early sun. Planets promptly produced from material with the inferred Al-26/Al-27 would melt within about 300,000 years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AIPC..679...43A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AIPC..679...43A"><span>LASCO <span class="hlt">Observations</span> Of The K-Corona From <span class="hlt">Solar</span> Minimum To <span class="hlt">Solar</span> Maximum And Beyond</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrews, Michael D.; Howard, Russell A.</p> <p>2003-09-01</p> <p>The LASCO C2 and C3 coronagraphs on SOHO have been recording a regular series of images of the corona since May 1996. This sequence of data covers the period of <span class="hlt">solar</span> minimum, the increase to <span class="hlt">solar</span> maximum, and the beginning of the decline toward the next <span class="hlt">solar</span> minimum. The images have been analyzed to determine the brightness of the K-corona (<span class="hlt">solar</span> photons Thomson scattered from free electrons). The total brightness of the K-corona is approximately constant from May 1996 through May 1997. The brightness is then seen to increase steadily until early in the year 2000. The structure of the K-corona changes dramatically with <span class="hlt">solar</span> cycle. The shape as seen in C2 becomes almost circular at <span class="hlt">solar</span> maximum while the C3 images continue to show equatorial streamers. The magnitude of the <span class="hlt">solar</span> cycle variation decreases as the height increases. We present data animations (movies) to show the large-scale structure. We have inverted 28-day averages of the white light images to determine radial profiles of electron density. We present these electron profiles, show how they vary as a function of both latitude and time, and compare our <span class="hlt">observed</span> profiles with other models and <span class="hlt">observations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..122.2768L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.2768L"><span>MAVEN <span class="hlt">observations</span> of the <span class="hlt">solar</span> cycle 24 space weather conditions at Mars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, C. O.; Hara, T.; Halekas, J. S.; Thiemann, E.; Chamberlin, P.; Eparvier, F.; Lillis, R. J.; Larson, D. E.; Dunn, P. A.; Espley, J. R.; Gruesbeck, J.; Curry, S. M.; Luhmann, J. G.; Jakosky, B. M.</p> <p>2017-03-01</p> <p>The Mars Atmosphere and Volatile EvolutioN (MAVEN) spacecraft has been continuously <span class="hlt">observing</span> the variability of <span class="hlt">solar</span> soft X-rays and EUV irradiance, monitoring the upstream <span class="hlt">solar</span> wind and interplanetary magnetic field conditions and measuring the fluxes of <span class="hlt">solar</span> energetic ions and electrons since its arrival to Mars. In this paper, we provide a comprehensive overview of the space weather events <span class="hlt">observed</span> during the first ˜1.9 years of the science mission, which includes the description of the <span class="hlt">solar</span> and heliospheric sources of the space weather activity. To illustrate the variety of upstream conditions <span class="hlt">observed</span>, we characterize a subset of the event periods by describing the Sun-to-Mars details using <span class="hlt">observations</span> from the MAVEN <span class="hlt">solar</span> Extreme Ultraviolet Monitor, <span class="hlt">solar</span> energetic particle (SEP) instrument, <span class="hlt">Solar</span> Wind Ion Analyzer, and Magnetometer together with <span class="hlt">solar</span> <span class="hlt">observations</span> using near-Earth assets and numerical <span class="hlt">solar</span> wind simulation results from the Wang-Sheeley-Arge-Enlil model for some global context of the event periods. The subset of events includes an extensive period of intense SEP electron particle fluxes triggered by a series of <span class="hlt">solar</span> flares and coronal mass ejection (CME) activity in December 2014, the impact by a succession of interplanetary CMEs and their associated SEPs in March 2015, and the passage of a strong corotating interaction region (CIR) and arrival of the CIR shock-accelerated energetic particles in June 2015. However, in the context of the weaker heliospheric conditions <span class="hlt">observed</span> throughout <span class="hlt">solar</span> cycle 24, these events were moderate in comparison to the stronger storms <span class="hlt">observed</span> previously at Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060036438&hterms=mcd&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmcd','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060036438&hterms=mcd&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmcd"><span>Cascade Helps JPL Explore the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Burke, G. R.</p> <p>1996-01-01</p> <p>At Jet Propulsion Laboratory (JPL), we are involved with the unmanned exploration of the <span class="hlt">solar</span> <span class="hlt">system</span>. Unmanned probes <span class="hlt">observe</span> the planet surfaces using radar and optical cameras to take a variety of measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679606-bayes-theorem-early-solar-short-lived-radionuclides-case-unexceptional-origin-solar-system','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679606-bayes-theorem-early-solar-short-lived-radionuclides-case-unexceptional-origin-solar-system"><span>BAYES’ THEOREM AND EARLY <span class="hlt">SOLAR</span> SHORT-LIVED RADIONUCLIDES: THE CASE FOR AN UNEXCEPTIONAL ORIGIN FOR THE <span class="hlt">SOLAR</span> <span class="hlt">SYSTEM</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>Young, Edward D., E-mail: eyoung@epss.ucla.edu</p> <p>2016-08-01</p> <p>The presence of excesses of short-lived radionuclides in the early <span class="hlt">solar</span> <span class="hlt">system</span> evidenced in meteorites has been taken as testament to close encounters with exotic nucleosynthetic sources, including supernovae or AGB stars. An analysis of the likelihoods associated with different sources of these extinct nuclides in the early <span class="hlt">solar</span> <span class="hlt">system</span> indicates that, rather than being exotic, their abundances were typical of star-forming regions like those <span class="hlt">observed</span> today in the Galaxy. The radiochemistry of the early <span class="hlt">solar</span> <span class="hlt">system</span> is therefore unexceptional, being the consequence of extensive averaging of solids from molecular clouds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790022944','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790022944"><span>The shape and location of the sector boundary surface in the inner <span class="hlt">solar</span> <span class="hlt">system</span>. [Helios <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>Villante, U.; Bruno, R.; Mariani, F.; Burlaga, L. F.; Ness, N. F.</p> <p>1979-01-01</p> <p>Simultaneous <span class="hlt">observations</span> by Helios-1 and Helios-2 over four <span class="hlt">solar</span> rotations were used to determine the latitudinal dependence of the polarity of the interplanetary magnetic field within plus or minus 7.23 deg of the <span class="hlt">solar</span> equator and within 1 AU. The longitudinal and latitudinal positions of the sector boundary crossing are consistent with a warped sector boundary which extended from the sun to 1 AU and was inclined approximately 10 deg with respect to the heliographic equator. This is consistent with simultaneous Pioneer 11 <span class="hlt">observations</span>, which showed unipolar fields at latitude approximately 16 deg at heliocentric distances greater than 3.5 AU. Two sectors were <span class="hlt">observed</span> at southern latitudes; however, four sectors were <span class="hlt">observed</span> at northern latitudes on two rotations, indicating a distortion from planarity of the sectory boundary surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DDA....4820001H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DDA....4820001H"><span>Astrometry and dynamics of <span class="hlt">Solar</span> <span class="hlt">System</span> Objects with Gaia GDR <span class="hlt">observations</span> and catalogues</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hestroffer, Daniel J. G. J.; Tanga, Paolo</p> <p>2017-06-01</p> <p>The Gaia ESA space mission has started to provide its harvest with the first Gaia data release DR1, published in September 2016. Gaia DR1 provides positions for about 1 billion stars and proper motion for the Tycho-Gaia TGAS of 2 million stars with unprecedented accuracy. The second data release DR2 will be the major step in the Gaia mission, providing all astrometric parameters (including parallax and proper motion) for a billion stars, in an absolute reference frame - to become the optical ICRF. Gaia DR2 will also provide epoch astrometry for about 13000 asteroids from its direct <span class="hlt">observations</span>, down to magnitude V≈20.7. We will discuss the improvement brought by Gaia over 5 years of nominal mission, starting with DR1, and focusing especially on the dynamics of asteroids and other <span class="hlt">Solar</span> <span class="hlt">System</span> Objects. This includes use of the catalogue for calibrating future and past photometric and astrometric <span class="hlt">observations</span> (in particular new reduction of ancient photographic plates digitalised by the NAROO programme), new perspectives for orbit determination and stellar occultations, detection of small acceleration or perturbations for the asteroids. Also we illustrate the ground-based activity coordinated by the Gaia-FUN-SSO network for follow-up <span class="hlt">observations</span> of newly discovered Near Earth Object.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004PhDT.........1Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004PhDT.........1Y"><span>High resolution <span class="hlt">solar</span> <span class="hlt">observations</span> in the context of space weather prediction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Guo</p> <p></p> <p>Space weather has a great impact on the Earth and human life. It is important to study and monitor active regions on the <span class="hlt">solar</span> surface and ultimately to predict space weather based on the Sun's activity. In this study, a <span class="hlt">system</span> that uses the full power of speckle masking imaging by parallel processing to obtain high-spatial resolution images of the <span class="hlt">solar</span> surface in near real-time has been developed and built. The application of this <span class="hlt">system</span> greatly improves the ability to monitor the evolution of <span class="hlt">solar</span> active regions and to predict the adverse effects of space weather. The data obtained by this <span class="hlt">system</span> have also been used to study fine structures on the <span class="hlt">solar</span> surface and their effects on the upper <span class="hlt">solar</span> atmosphere. A <span class="hlt">solar</span> active region has been studied using high resolution data obtained by speckle masking imaging. Evolution of a pore in an active region presented. Formation of a rudimentary penumbra is studied. The effects of the change of the magnetic fields on the upper level atmosphere is discussed. Coronal Mass Ejections (CMEs) have a great impact on space weather. To study the relationship between CMEs and filament disappearance, a list of 431 filament and prominence disappearance events has been compiled. Comparison of this list with CME data obtained by satellite has shown that most filament disappearances seem to have no corresponding CME events. Even for the limb events, only thirty percent of filament disappearances are associated with CMEs. A CME event that was <span class="hlt">observed</span> on March 20, 2000 has been studied in detail. This event did not show the three-parts structure of typical CMEs. The kinematical and morphological properties of this event were examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AdSpR..42.1806S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AdSpR..42.1806S"><span>Amateur <span class="hlt">observations</span> of <span class="hlt">solar</span> eclipses and derivation of scientific data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stoev, A. D.; Stoeva, P. V.</p> <p>2008-12-01</p> <p>This work presents the educational approach of using total <span class="hlt">solar</span> eclipse occurrences as a scientific process learning aid. The work reviews the basic scientific aims and experiments included in the <span class="hlt">observational</span> programs "Total <span class="hlt">solar</span> eclipse 1999 and 2006" (Stoev, A., Kiskinova, N., Muglova, P. et al. Complex <span class="hlt">observational</span> programme of the Yuri Gagarin Public Astronomical Observatory and STIL, BAS, Stara Zagora Department for the August 11, 1999 total <span class="hlt">solar</span> eclipse, in: Total <span class="hlt">Solar</span> Eclipse 1999 - <span class="hlt">Observational</span> Programmes and Coordination, Proceedings, Recol, Haskovo, pp. 133-137, 1999a (in Bulgarian); Stoeva, P.V., Stoev, A.D., Kostadinov, I.N. et al. <span class="hlt">Solar</span> Corona and Atmospheric Effects during the March 29, 2006 Total <span class="hlt">Solar</span> Eclipse, in: 11th International Science Conference <span class="hlt">SOLAR</span>-Terrestrial Influences, Sofia, November 24-25, pp. 69-72, 2005). Results from teaching and training the students in the procedures, methods and equipment necessary for the <span class="hlt">observation</span> of a total <span class="hlt">solar</span> eclipse (TSE) at the Yuri Gagarin Public Astronomical Observatory (PAO) in Stara Zagora, Bulgaria, as well as the selection process used in determining participation in the different <span class="hlt">observational</span> teams are discussed. The final stages reveal the special methodology used to investigate the level of "pretensions", the levels of ambition displayed by the students in achieving each independent goal, and the setting of goals in context with their problem solving capabilities and information gathering abilities in the scientific <span class="hlt">observation</span> process. Results obtained from the <span class="hlt">observational</span> experiments are interpreted mainly in the following themes: Investigation of the structure of the white-light <span class="hlt">solar</span> corona and evolution of separate coronal elements during the total phase of the eclipse; Photometry of the white-light <span class="hlt">solar</span> corona and specific emission lines; Meteorological, actinometrical and optical atmospheric investigations; Astrometry of the Moon during the phase evolution of the eclipse and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADD004267','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADD004267"><span><span class="hlt">Solar</span> Collector Control <span class="hlt">System</span>.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p></p> <p>A <span class="hlt">system</span> for controlling the movement in azimuth and elevation of a large number of sun following solor energy collectors from a single controller...The <span class="hlt">system</span> utilizes servo signal generators, a modulator and a demodulator for transmitting the servo signals, and stepping motors for controlling...remotely located <span class="hlt">solar</span> collectors. The <span class="hlt">system</span> allows precise tracking of the sun by a series of <span class="hlt">solar</span> collectors without the necessity or expense of individualized <span class="hlt">solar</span> trackers. (Author)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000025315','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000025315"><span>Adaptive Optics Imaging of <span class="hlt">Solar</span> <span class="hlt">System</span> Objects</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Roddier, Francois; Owen, Toby</p> <p>1999-01-01</p> <p>Most <span class="hlt">solar</span> <span class="hlt">system</span> objects have never been <span class="hlt">observed</span> at wavelengths longer than the R band with an angular resolution better than 1". The Hubble Space Telescope itself has only recently been equipped to <span class="hlt">observe</span> in the infrared. However, because of its small diameter, the angular resolution is lower than that one can now achieved from the ground with adaptive optics, and time allocated to planetary science is limited. We have successfully used adaptive optics on a 4-m class telescope to obtain 0.1" resolution images of <span class="hlt">solar</span> <span class="hlt">system</span> objects in the far red and near infrared (0.7-2.5 microns), aE wavelengths which best discl"lmlnate their spectral signatures. Our efforts have been put into areas of research for which high angular resolution is essential.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Solar+AND+system&pg=3&id=EJ892047','ERIC'); return false;" href="https://eric.ed.gov/?q=Solar+AND+system&pg=3&id=EJ892047"><span>Precipitation in the <span class="hlt">Solar</span> <span class="hlt">System</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>McIntosh, Gordon</p> <p>2007-01-01</p> <p>As an astronomy instructor, I am always looking for commonly <span class="hlt">observed</span> Earthly experiences to help my students and me understand and appreciate similar occurrences elsewhere in the <span class="hlt">solar</span> <span class="hlt">system</span>. Recently I wrote a short TPT article on frost. This paper is on the related phenomena of precipitation. Precipitation, so common on most of the Earth's…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.P21B0531S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.P21B0531S"><span>The Jupiter <span class="hlt">System</span> <span class="hlt">Observer</span>: Probing the Foundations of Planetary <span class="hlt">Systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Senske, D.; Prockter, L.; Collins, G.; Cooper, J.; Hendrix, A.; Hibbitts, K.; Kivelson, M.; Orton, G.; Schubert, G.; Showman, A.; Turtle, E.; Williams, D.; Kwok, J.; Spilker, T.; Tan-Wang, G.</p> <p>2007-12-01</p> <p>Galileo's <span class="hlt">observations</span> in the 1600's of the dynamic <span class="hlt">system</span> of Jupiter and its moons launched a revolution in understanding the way planetary <span class="hlt">systems</span> operate. Now, some 400 years later, the discovery of extra <span class="hlt">solar</span> planetary <span class="hlt">systems</span> with Jupiter-sized bodies has led to a similar revolution in thought regarding how these <span class="hlt">systems</span> form and evolve. From the time of Galileo, the Jovian <span class="hlt">system</span> has been viewed as a <span class="hlt">solar</span> <span class="hlt">system</span> in miniature, providing a laboratory to study, diverse and dynamic processes in a single place. The icy Galilean satellites provide a window into <span class="hlt">solar</span> <span class="hlt">system</span> history by preserving in their cratering records a chronology dating back nearly 4.5 By and extending to the present. The continuously erupting volcanoes of Io may provide insight into the era when magma oceans were common. The discovery of an internally generated magnetic field at Ganymede, one of only three terrestrial bodies to possess such a field, is a place to gain insight as to how dynamos work. The confirmation and characterization of icy satellite subsurface oceans impacts the way habitability is considered. Understanding the composition and volatile inventory of Jupiter can shed light into how planets accrete from the <span class="hlt">solar</span> nebulae. Finally, like our sun, Jupiter influences its <span class="hlt">system</span> through its extensive magnetic field. In early 2007, NASA's Science Mission Directorate formed four Science Definition Teams (SDTs) to formulate science goals and objectives in anticipation of the initiation of a flagship-class mission to the outer <span class="hlt">solar</span> <span class="hlt">system</span> (Europa, Jupiter <span class="hlt">system</span>, Titan and Enceladus). The Jupiter <span class="hlt">System</span> <span class="hlt">Observer</span> (JSO) mission concept emphasizes overall Jupiter <span class="hlt">system</span> science: 1) Jupiter and its atmosphere, 2) the geology and geophysics of the Galilean satellites (Io, Europa, Ganymede and Callisto), 3) the magnetosphere environment - both Jupiter's and Ganymede's&pand 4) interactions within the <span class="hlt">system</span>. Focusing on the unique geology, presence of an internal magnetic field and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5480931-observations-statistical-simulations-proposed-solar-cycle-qbo-weather-relationship','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5480931-observations-statistical-simulations-proposed-solar-cycle-qbo-weather-relationship"><span><span class="hlt">Observations</span> and statistical simulations of a proposed <span class="hlt">solar</span> cycle/QBO/weather relationship</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>Baldwin, M.P.; Dunkerton, T.J.</p> <p>1989-08-01</p> <p>The 10.7 cm <span class="hlt">solar</span> flux is <span class="hlt">observed</span> to be highly correlated with north pole stratospheric temperatures when partitioned according to the phase of the equatorial stratospheric winds (the quasi-biennial oscillation, or QBO). The authors supplement <span class="hlt">observations</span> with calculations showing that temperatures over most of the northern hemisphere are highly correlated or anticorrelated with north pole temperatures. The <span class="hlt">observed</span> spatial pattern of <span class="hlt">solar</span> cycle correlations at high latitudes is shown to be not unique to the <span class="hlt">solar</span> cycle. The authors present results, similar to the <span class="hlt">observed</span> <span class="hlt">solar</span> cycle correlations, with simulated harmonics of various periods replacing the <span class="hlt">solar</span> cycle. These calculationsmore » demonstrate the correlations at least as high as those for the <span class="hlt">solar</span> cycle results may be obtained using simulated harmonics.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED160429.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED160429.pdf"><span><span class="hlt">Solar</span> Program Assessment: Environmental Factors - <span class="hlt">Solar</span> Total Energy <span class="hlt">Systems</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>Energy Research and Development Administration, Washington, DC. Div. of Solar Energy.</p> <p></p> <p>The purpose of this report is to present and prioritize the major environmental, safety, and social/institutional issues associated with the further development of <span class="hlt">Solar</span> Total Energy <span class="hlt">Systems</span> (STES). <span class="hlt">Solar</span> total energy <span class="hlt">systems</span> represent a specific application of the Federally-funded <span class="hlt">solar</span> technologies. To provide a background for this analysis, the…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020012425&hterms=relativity+theory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Drelativity%2Btheory','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020012425&hterms=relativity+theory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Drelativity%2Btheory"><span><span class="hlt">Solar-System</span> Tests of Gravitational Theories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shapiro, Irwin I.</p> <p>2001-01-01</p> <p>We are engaged in testing gravitational theory, primarily using <span class="hlt">observations</span> of objects in the <span class="hlt">solar</span> <span class="hlt">system</span> and primarily on that scale. Our goal is either to detect departures from the standard model (general relativity) - if any exist within the level of sensitivity of our data - or to place tighter bounds on such departures. For this project, we have analyzed a combination of <span class="hlt">observational</span> data with our model of the <span class="hlt">solar</span> <span class="hlt">system</span>, including mostly planetary radar ranging, lunar laser ranging, and spacecraft tracking, but also including both pulsar timing and pulsar very long base interferometry (VLBI) measurements. This year, we have extended our model of Earth nutation with adjustable correction terms at the principal frequencies. We also refined our model of tidal drag on the Moon's orbit. We believe these changes will make no substantial changes in the results, but we are now repeating the analysis of the whole set of data to verify that belief. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017sko..rept....5M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017sko..rept....5M"><span><span class="hlt">Observational</span> methods for <span class="hlt">solar</span> origin diagnostics of energetic protons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miteva, Rositsa</p> <p>2017-12-01</p> <p>The aim of the present report is to outline the <span class="hlt">observational</span> methods used to determine the <span class="hlt">solar</span> origin - in terms of flares and coronal mass ejections (CMEs) - of the in situ <span class="hlt">observed</span> <span class="hlt">solar</span> energetic protons. Several widely used guidelines are given and different sources of uncertainties are summarized and discussed. In the present study, a new quality factor is proposed as a certainty check on the so-identified flare-CME pairs. In addition, the correlations between the proton peak intensity and the properties of their <span class="hlt">solar</span> origin are evaluated as a function of the quality factor.</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_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" 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_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> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013IAUS..294..571M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013IAUS..294..571M"><span><span class="hlt">Solar</span> flares <span class="hlt">observed</span> simultaneously with SphinX, GOES and RHESSI</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mrozek, Tomasz; Gburek, Szymon; Siarkowski, Marek; Sylwester, Barbara; Sylwester, Janusz; Kępa, Anna; Gryciuk, Magdalena</p> <p>2013-07-01</p> <p>In February 2009, during recent deepest <span class="hlt">solar</span> minimum, Polish <span class="hlt">Solar</span> Photometer in X-rays (SphinX) begun <span class="hlt">observations</span> of the Sun in the energy range of 1.2-15 keV. SphinX was almost 100 times more sensitive than GOES X-ray Sensors. The silicon PIN diode detectors used in the experiment were carefully calibrated on the ground using Synchrotron Radiation Source BESSY II. The SphinX energy range overlaps with the Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager (RHESSI) energy range. The instrument provided us with <span class="hlt">observations</span> of hundreds of very small flares and X-ray brightenings. We have chosen a group of <span class="hlt">solar</span> flares <span class="hlt">observed</span> simultaneously with GOES, SphinX and RHESSI and performed spectroscopic analysis of <span class="hlt">observations</span> wherever possible. The analysis of thermal part of the spectra showed that SphinX is a very sensitive complementary observatory for RHESSI and GOES.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654348-stereoscopic-observation-slipping-reconnection-double-candle-flame-shaped-solar-flare','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654348-stereoscopic-observation-slipping-reconnection-double-candle-flame-shaped-solar-flare"><span>STEREOSCOPIC <span class="hlt">OBSERVATION</span> OF SLIPPING RECONNECTION IN A DOUBLE CANDLE-FLAME-SHAPED <span class="hlt">SOLAR</span> FLARE</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>Gou, Tingyu; Liu, Rui; Wang, Yuming</p> <p>2016-04-20</p> <p>The 2011 January 28 M1.4 flare exhibits two side-by-side candle-flame-shaped flare loop <span class="hlt">systems</span> underneath a larger cusp-shaped structure during the decay phase, as <span class="hlt">observed</span> at the northwestern <span class="hlt">solar</span> limb by the <span class="hlt">Solar</span> Dynamics Observatory . The northern loop <span class="hlt">system</span> brightens following the initiation of the flare within the southern loop <span class="hlt">system</span>, but all three cusp-shaped structures are characterized by ∼10 MK temperatures, hotter than the arch-shaped loops underneath. The “Ahead” satellite of the <span class="hlt">Solar</span> Terrestrial Relations Observatory provides a top view, in which the post-flare loops brighten sequentially, with one end fixed while the other apparently slipping eastward. By performingmore » stereoscopic reconstruction of the post-flare loops in EUV and mapping out magnetic connectivities, we found that the footpoints of the post-flare loops are slipping along the footprint of a hyperbolic flux tube (HFT) separating the two loop <span class="hlt">systems</span> and that the reconstructed loops share similarity with the magnetic field lines that are traced starting from the same HFT footprint, where the field lines are relatively flexible. These results argue strongly in favor of slipping magnetic reconnection at the HFT. The slipping reconnection was likely triggered by the flare and manifested as propagative dimmings before the loop slippage is <span class="hlt">observed</span>. It may contribute to the late-phase peak in Fe xvi 33.5 nm, which is even higher than its main-phase counterpart, and may also play a role in the density and temperature asymmetry <span class="hlt">observed</span> in the northern loop <span class="hlt">system</span> through heat conduction.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030002364','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030002364"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Dynamics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wisdom, Jack</p> <p>2002-01-01</p> <p>In these 18 years, the research has touched every major dynamical problem in the <span class="hlt">solar</span> <span class="hlt">system</span>, including: the effect of chaotic zones on the distribution of asteroids, the delivery of meteorites along chaotic pathways, the chaotic motion of Pluto, the chaotic motion of the outer planets and that of the whole <span class="hlt">solar</span> <span class="hlt">system</span>, the delivery of short period comets from the Kuiper belt, the tidal evolution of the Uranian arid Galilean satellites, the chaotic tumbling of Hyperion and other irregular satellites, the large chaotic variations of the obliquity of Mars, the evolution of the Earth-Moon <span class="hlt">system</span>, and the resonant core- mantle dynamics of Earth and Venus. It has introduced new analytical and numerical tools that are in widespread use. Today, nearly every long-term integration of our <span class="hlt">solar</span> <span class="hlt">system</span>, its subsystems, and other <span class="hlt">solar</span> <span class="hlt">systems</span> uses algorithms that was invented. This research has all been primarily Supported by this sequence of PGG NASA grants. During this period published major investigations of tidal evolution of the Earth-Moon <span class="hlt">system</span> and of the passage of the Earth and Venus through non-linear core-mantle resonances were completed. It has published a major innovation in symplectic algorithms: the symplectic corrector. A paper was completed on non-perturbative hydrostatic equilibrium.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25512527','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25512527"><span>Exoplanet orbital eccentricity: multiplicity relation and the <span class="hlt">Solar</span> <span class="hlt">System</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Limbach, Mary Anne; Turner, Edwin L</p> <p>2015-01-06</p> <p>The known population of exoplanets exhibits a much wider range of orbital eccentricities than <span class="hlt">Solar</span> <span class="hlt">System</span> planets and has a much higher average eccentricity. These facts have been widely interpreted to indicate that the <span class="hlt">Solar</span> <span class="hlt">System</span> is an atypical member of the overall population of planetary <span class="hlt">systems</span>. We report here on a strong anticorrelation of orbital eccentricity with multiplicity (number of planets in the <span class="hlt">system</span>) among cataloged radial velocity (RV) <span class="hlt">systems</span>. The mean, median, and rough distribution of eccentricities of <span class="hlt">Solar</span> <span class="hlt">System</span> planets fits an extrapolation of this anticorrelation to the eight-planet case rather precisely despite the fact that no more than two <span class="hlt">Solar</span> <span class="hlt">System</span> planets would be detectable with RV data comparable to that in the exoplanet sample. Moreover, even if regarded as a single or double planetary <span class="hlt">system</span>, the <span class="hlt">Solar</span> <span class="hlt">System</span> lies in a reasonably heavily populated region of eccentricity-multiplicity space. Thus, the <span class="hlt">Solar</span> <span class="hlt">System</span> is not anomalous among known exoplanetary <span class="hlt">systems</span> with respect to eccentricities when its multiplicity is taken into account. Specifically, as the multiplicity of a <span class="hlt">system</span> increases, the eccentricity decreases roughly as a power law of index -1.20. A simple and plausible but ad hoc and model-dependent interpretation of this relationship implies that ∼ 80% of the one-planet and 25% of the two-planet <span class="hlt">systems</span> in our sample have additional, as yet undiscovered, members but that <span class="hlt">systems</span> of higher <span class="hlt">observed</span> multiplicity are largely complete (i.e., relatively rarely contain additional undiscovered planets). If low eccentricities indeed favor high multiplicities, habitability may be more common in <span class="hlt">systems</span> with a larger number of planets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990115921&hterms=spectroscopy+infrared+hydrocarbons+waters&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dspectroscopy%2Binfrared%2Bhydrocarbons%2Bwaters','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990115921&hterms=spectroscopy+infrared+hydrocarbons+waters&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dspectroscopy%2Binfrared%2Bhydrocarbons%2Bwaters"><span>Remote Thermal IR Spectroscopy of our <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kostiuk, Theodor; Hewagama, Tilak; Goldstein, Jeffrey; Livengood, Timothy; Fast, Kelly</p> <p>1999-01-01</p> <p>Indirect methods to detect extrasolar planets have been successful in identifying a number of stars with companion planets. No direct detection of an extrasolar planet has yet been reported. Spectroscopy in the thermal infrared region provides a potentially powerful approach to detection and characterization of planets and planetary <span class="hlt">systems</span>. We can use knowledge of our own <span class="hlt">solar</span> <span class="hlt">system</span>, its planets and their atmospheres to model spectral characteristics of planets around other stars. Spectra derived from modeling our own <span class="hlt">solar</span> <span class="hlt">system</span> seen from an extrasolar perspective can be used to constrain detection strategies, identification of planetary class (terrestrial vs. gaseous) and retrieval of chemical, thermal and dynamical information. Emission from planets in our <span class="hlt">solar</span> <span class="hlt">system</span> peaks in the thermal infrared region, approximately 10 - 30 microns, substantially displaced from the maximum of the much brighter <span class="hlt">solar</span> emission in the visible near 0.5 microns. This fact provides a relatively good contrast ratio to discriminate between stellar (<span class="hlt">solar</span>) and planetary emission and optimize the delectability of planetary spectra. Important molecular constituents in planetary atmospheres have rotational-vibrational spectra in the thermal infrared region. Spectra from these molecules have been well characterized in the laboratory and studied in the atmospheres of <span class="hlt">solar</span> <span class="hlt">system</span> planets from ground-based and space platforms. The best example of such measurements are the studies with Fourier transform spectrometers, the Infrared Interferometer Spectrometers (IRIS), from spacecraft: Earth <span class="hlt">observed</span> from NIMBUS 8, Mars <span class="hlt">observed</span> from Mariner 9, and the outer planets <span class="hlt">observed</span> from Voyager spacecraft. An Earth-like planet is characterized by atmospheric spectra of ozone, carbon dioxide, and water. Terrestrial planets have oxidizing atmospheres which are easily distinguished from reducing atmospheres of gaseous giant planets which lack oxygen-bearing species and are characterized by spectra</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920003600','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920003600"><span>Studies of relationships among outer <span class="hlt">solar</span> <span class="hlt">system</span> small bodies and related objects</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hartmann, William K.</p> <p>1991-01-01</p> <p>This program involves telescopic <span class="hlt">observations</span> of colorimetry, spectroscopy, and photometry of small bodies of the <span class="hlt">solar</span> <span class="hlt">system</span>, emphasizing possible relationships among outer <span class="hlt">solar</span> <span class="hlt">system</span> asteroids, comets, and certain satellites. Earth approacher targets of opportunity and lab spectroscopic studies are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760087394&hterms=microclimate&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmicroclimate','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760087394&hterms=microclimate&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmicroclimate"><span><span class="hlt">Solar</span> energy microclimate as determined from satellite <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>Vonder Haar, T. H.; Ellis, J. S.</p> <p>1975-01-01</p> <p>A method is presented for determining <span class="hlt">solar</span> insolation at the earth's surface using satellite broadband visible radiance and cloud imagery data, along with conventional in situ measurements. Conventional measurements are used to both tune satellite measurements and to develop empirical relationships between satellite <span class="hlt">observations</span> and surface <span class="hlt">solar</span> insolation. Cloudiness is the primary modulator of sunshine. The satellite measurements as applied in this method consider cloudiness both explicitly and implicitly in determining surface <span class="hlt">solar</span> insolation at space scales smaller than the conventional pyranometer network.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012CEAB...36...71M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012CEAB...36...71M"><span>Common SphinX and RHESSI <span class="hlt">observations</span> of <span class="hlt">solar</span> flares</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mrozek, T.; Gburek, S.; Siarkowski, M.; Sylwester, B.; Sylwester, J.; Gryciuk, M.</p> <p></p> <p>The Polish X-ray spectrofotometer SphinX has <span class="hlt">observed</span> a great number of <span class="hlt">solar</span> flares in the year 2009 - during the most quiet <span class="hlt">solar</span> minimum almost over the last 100 years. Hundreds of flares have been recorded due to excellent sensitivity of SphinX's detectors. The Si-PIN diodes are about 100 times more sensitive to X-rays than GOES X-ray Monitors. SphinX detectors were absolutely calibrated on Earth with a use of the BESSY synchrotron. In space <span class="hlt">observations</span> were made in the range 1.2-15~keV with 480~eV energy resolution. SphinX data overlap with the low-energy end of the Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager (RHESSI) data. RHESSI detectors are quite old (7 years in 2009), but still sensitive enough to provide us with <span class="hlt">observations</span> of extremely weak <span class="hlt">solar</span> flares such as those which occurred in 2009. We have selected a group of flares simultaneously <span class="hlt">observed</span> by RHESSI and SphinX and performed a spectroscopic analysis of the data. Moreover, we compared the physical parameters of these flares plasma. Preliminary results of the comparison show very good agreement between both instruments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040061993&hterms=mips&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmips','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040061993&hterms=mips&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmips"><span>First <span class="hlt">Solar</span> <span class="hlt">System</span> Results of the Spitzer Space Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>VanCleve, J.; Cruikshank, D. P.; Stansberry, J. A.; Burgdorf, M. J.; Devost, D.; Emery, J. P.; Fazio, G.; Fernandez, Y. R.; Glaccum, W.; Grillmair, C.</p> <p>2004-01-01</p> <p>The Spitzer Space Telescope, formerly known as SIRTF, is now operational and delivers unprecedented sensitivity for the <span class="hlt">observation</span> of <span class="hlt">Solar</span> <span class="hlt">System</span> targets. Spitzer's capabilities and first general results were presented at the January 2004 AAS meeting. In this poster, we focus on Spitzer's performance for moving targets, and the first <span class="hlt">Solar</span> <span class="hlt">System</span> results. Spitzer has three instruments, IRAC, IRS, and MIPS. IRAC (InfraRed Array Camera) provides simultaneous images at wavelengths of 3.6, 4.5, 5.8, and 8.0 microns. IRS (InfraRed Spectrograph) has 4 modules providing low-resolution (R=60-120) spectra from 5.3 to 40 microns, high-resolution (R=600) spectra from 10 to 37 m, and an autonomous target acquisition <span class="hlt">system</span> (PeakUp) which includes small-field imaging at 15 m. MIPS (Multiband Imaging Photometer for SIRTF) does imaging photometry at 24, 70, and 160 m and low-resolution (R=15-25) spectroscopy (SED) between 55 and 96 microns. Guaranteed Time <span class="hlt">Observer</span> (GTO) programs include the moons of the outer <span class="hlt">Solar</span> <span class="hlt">System</span>, Pluto, Centaurs, Kuiper Belt Objects, and comets</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740044469&hterms=Systems+Reward&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSystems%2BReward','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740044469&hterms=Systems+Reward&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSystems%2BReward"><span>Exploration of the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Henderson, A., Jr. (Editor); Grey, J.</p> <p>1974-01-01</p> <p>The potential achievements of <span class="hlt">solar</span> <span class="hlt">system</span> exploration are outlined, and a course of action is suggested which will maximize the rewards. Also provided is a sourcebook of information on the <span class="hlt">solar</span> <span class="hlt">system</span> and the technology being brought to bear for its exploration. The document explores the degree to which three practical questions can be answered: why it is necessary to explore the <span class="hlt">solar</span> <span class="hlt">system</span>, why understanding of the <span class="hlt">solar</span> <span class="hlt">system</span> is important to us, and why we cannot wait until all terrestrial problems are solved before an attempt is made to solve problems in space.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AdSpR..47.1538K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AdSpR..47.1538K"><span>Results of <span class="hlt">solar</span> <span class="hlt">observations</span> by the CORONAS-F payload</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuznetsov, V. D.; Sobelman, I. I.; Zhitnik, I. A.; Kuzin, S. V.; Kotov, Yu. D.; Charikov, Yu. E.; Kuznetsov, S. N.; Mazets, E. P.; Nusinov, A. A.; Pankov, A. M.; Sylwester, J.</p> <p>2011-05-01</p> <p>The CORONAS-F mission experiments and results have been reviewed. The <span class="hlt">observations</span> with the DIFOS multi-channel photometer in a broad spectral range from 350 to 1500 nm have revealed the dependence of the relative amplitudes of p-modes of the global <span class="hlt">solar</span> oscillations on the wavelength that agrees perfectly well with the earlier data obtained in a narrower spectral ranges. The SPIRIT EUV <span class="hlt">observations</span> have enabled the study of various manifestations of <span class="hlt">solar</span> activity and high-temperature events on the Sun. The data from the X-ray spectrometer RESIK, gamma spectrometer HELICON, flare spectrometer IRIS, amplitude-temporal spectrometer AVS-F, and X-ray spectrometer RPS-1 have been used to analyze the X- and gamma-ray emission from <span class="hlt">solar</span> flares and for diagnostics of the flaring plasma. The absolute and relative content of various elements (such as potassium, argon, and sulfur) of <span class="hlt">solar</span> plasma in flares has been determined for the first time with the X-ray spectrometer RESIK. The <span class="hlt">Solar</span> Cosmic Ray Complex monitored the <span class="hlt">solar</span> flare effects in the Earth's environment. The UV emission variations recorded during <span class="hlt">solar</span> flares in the vicinity of the 120-nm wavelength have been analyzed and the amplitude of relative variations has been determined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140010418','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140010418"><span>Elemental GCR <span class="hlt">Observations</span> during the 2009-2010 <span class="hlt">Solar</span> Minimum Period</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lave, K. A.; Israel, M. H.; Binns, W. R.; Christian, E. R.; Cummings, A. C.; Davis, A. J.; deNolfo, G. A.; Leske, R. A.; Mewaldt, R. A.; Stone, E. C.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20140010418'); toggleEditAbsImage('author_20140010418_show'); toggleEditAbsImage('author_20140010418_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20140010418_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20140010418_hide"></p> <p>2013-01-01</p> <p>Using <span class="hlt">observations</span> from the Cosmic Ray Isotope Spectrometer (CRIS) onboard the Advanced Composition Explorer (ACE), we present new measurements of the galactic cosmic ray (GCR) elemental composition and energy spectra for the species B through Ni in the energy range approx. 50-550 MeV/nucleon during the record setting 2009-2010 <span class="hlt">solar</span> minimum period. These data are compared with our <span class="hlt">observations</span> from the 1997-1998 <span class="hlt">solar</span> minimum period, when <span class="hlt">solar</span> modulation in the heliosphere was somewhat higher. For these species, we find that the intensities during the 2009-2010 <span class="hlt">solar</span> minimum were approx. 20% higher than those in the previous <span class="hlt">solar</span> minimum, and in fact were the highest GCR intensities recorded during the space age. Relative abundances for these species during the two <span class="hlt">solar</span> minimum periods differed by small but statistically significant amounts, which are attributed to the combination of spectral shape differences between primary and secondary GCRs in the interstellar medium and differences between the levels of <span class="hlt">solar</span> modulation in the two <span class="hlt">solar</span> minima. We also present the secondary-to-primary ratios B/C and (Sc+Ti+V)/Fe for both <span class="hlt">solar</span> minimum periods, and demonstrate that these ratios are reasonably well fit by a simple "leaky-box" galactic transport model that is combined with a spherically symmetric <span class="hlt">solar</span> modulation model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH33A2036C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH33A2036C"><span>New <span class="hlt">Observations</span> of Soft X-ray (0.5-5 keV) <span class="hlt">Solar</span> Spectra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caspi, A.; Woods, T. N.; Mason, J. P.; Jones, A. R.; Warren, H. P.</p> <p>2013-12-01</p> <p>The <span class="hlt">solar</span> corona is the brightest source of X-rays in the <span class="hlt">solar</span> <span class="hlt">system</span>, and the X-ray emission is highly variable on many time scales. However, the actual <span class="hlt">solar</span> soft X-ray (SXR) (0.5-5 keV) spectrum is not well known, particularly during <span class="hlt">solar</span> quiet periods, as, with few exceptions, this energy range has not been systematically studied in many years. Previous <span class="hlt">observations</span> include high-resolution but very narrow-band spectra from crystal spectrometers (e.g., Yohkoh/BCS), or integrated broadband irradiances from photometers (e.g., GOES/XRS, TIMED/XPS, etc.) that lack detailed spectral information. In recent years, broadband measurements with moderate energy resolution (~0.5-0.7 keV FWHM) were made by SphinX on CORONAS-Photon and SAX on MESSENGER, although they did not extend to energies below ~1 keV. We present <span class="hlt">observations</span> of <span class="hlt">solar</span> SXR emission obtained using new instrumentation flown on recent SDO/EVE calibration rocket underflights. The photon-counting spectrometer, a commercial Amptek X123 with a silicon drift detector and an 8 μm Be window, measures the <span class="hlt">solar</span> disk-integrated SXR emission from ~0.5 to >10 keV with ~0.15 keV FWHM resolution and 1 s cadence. A novel imager, a pinhole X-ray camera using a cooled frame-transfer CCD (15 μm pixel pitch), Ti/Al/C filter, and 5000 line/mm Au transmission grating, images the full Sun in multiple spectral orders from ~0.1 to ~5 nm with ~10 arcsec/pixel and ~0.01 nm/pixel spatial and spectral detector scales, respectively, and 10 s cadence. These instruments are prototypes for future CubeSat missions currently being developed. We present new results of <span class="hlt">solar</span> <span class="hlt">observations</span> on 04 October 2013 (NASA sounding rocket 36.290). We compare with previous results from 23 June 2012 (NASA sounding rocket 36.286), during which <span class="hlt">solar</span> activity was low and no signal was <span class="hlt">observed</span> above ~4 keV. We compare our spectral and imaging measurements with spectra and broadband irradiances from other instruments, including SDO/EVE, GOES/XRS, TIMED</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMIN43C0092B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMIN43C0092B"><span>Survey of localized <span class="hlt">solar</span> flare signatures in the ionosphere with GNSS, VLF, and GOES <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>Blevins, S. M.; Hayes, L.; Collado-Vega, Y. M.; Michael, B. P.; Noll, C. E.</p> <p>2017-12-01</p> <p>Global navigation satellite <span class="hlt">system</span> (GNSS) phase measurements of the total electron content (TEC) and ionospheric delay are sensitive to sudden increases in electron density in the layers of the Earth's ionosphere. These sudden ionospheric disruptions, or SIDs, are due to enhanced X-ray and extreme ultraviolet radiation from a <span class="hlt">solar</span> flare that drastically increases the electron density in localized regions. SIDs are <span class="hlt">solar</span> flare signatures in the Earth's ionosphere and can be <span class="hlt">observed</span> with very low frequency (VLF 3-30 kHz) monitors and dual-frequency GNSS (L1 = 1575.42 MHz, L2 = 1227.60 MHz) receivers that probe lower (D-region) to upper (F-region) ionospheric layers, respectively. Data from over 500 <span class="hlt">solar</span> flare events, spanning April 2010 to July 2017, including GOES C-, M-, and X-class <span class="hlt">solar</span> flares at various intensities, were collected from the Space Weather Database Of Notifications, Knowledge, Information (DONKI) developed at the NASA Goddard Space Flight Center (GSFC) Community Coordinated Modeling Center (CCMC). Historical GOES satellite (NOAA) X-ray flux (NASA GSFC CCMC integrated Space Weather Analysis <span class="hlt">system</span> (iSWA)), and VLF SID (Stanford University <span class="hlt">Solar</span> SID Space Weather Monitor program) time series data are available for all <span class="hlt">solar</span> flare events of the sample set. We use GNSS data archived at the NASA GSFC Crustal Dynamics Data Information <span class="hlt">System</span> (CDDIS) to characterize the F-region reactions to the increased ionization, complementing the ground-based D-region (VLF), and space-based X-ray <span class="hlt">observations</span> (GOES). CDDIS provides GNSS data with 24-hour coverage at a temporal resolution of 30 seconds from over 500 stations. In our study we choose 63 stations, spanning 23 countries at a variety of geographic locations to provide continuous coverage for all <span class="hlt">solar</span> flare events in the sample. This geographic distribution enables us to explore the effects of different <span class="hlt">solar</span> flare intensities at localized regions in the Earths ionosphere around the globe. The GNSS</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1052226','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1052226"><span><span class="hlt">Solar</span> Resource & Meteorological Assessment Project (SOLRMAP): <span class="hlt">Observed</span> Atmospheric and <span class="hlt">Solar</span> Information <span class="hlt">System</span> (OASIS); Tucson, Arizona (Data)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Wilcox, S.; Andreas, A.</p> <p>2010-11-03</p> <p>The U.S. Department of Energy's National Renewable Energy Laboratory collaborates with the <span class="hlt">solar</span> industry to establish high quality <span class="hlt">solar</span> and meteorological measurements. This <span class="hlt">Solar</span> Resource and Meteorological Assessment Project (SOLRMAP) provides high quality measurements to support deployment of power projects in the United States. The no-funds-exchanged collaboration brings NREL <span class="hlt">solar</span> resource assessment expertise together with industry needs for measurements. The end result is high quality data sets to support the financing, design, and monitoring of large scale <span class="hlt">solar</span> power projects for industry in addition to research-quality data for NREL model development. NREL provides consultation for instrumentation and station deployment, along with instrument calibrations, data acquisition, quality assessment, data distribution, and summary reports. Industry participants provide equipment, infrastructure, and station maintenance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...611A..90B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...611A..90B"><span>Constraints on <span class="hlt">observing</span> brightness asymmetries in protoplanetary disks at <span class="hlt">solar</span> <span class="hlt">system</span> scale</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brunngräber, Robert; Wolf, Sebastian</p> <p>2018-04-01</p> <p>We have quantified the potential capabilities of detecting local brightness asymmetries in circumstellar disks with the Very Large Telescope Interferometer (VLTI) in the mid-infrared wavelength range. The study is motivated by the need to evaluate theoretical models of planet formation by direct <span class="hlt">observations</span> of protoplanets at early evolutionary stages, when they are still embedded in their host disk. Up to now, only a few embedded candidate protoplanets have been detected with semi-major axes of 20-50 au. Due to the small angular separation from their central star, only long-baseline interferometry provides the angular resolving power to detect disk asymmetries associated to protoplanets at <span class="hlt">solar</span> <span class="hlt">system</span> scales in nearby star-forming regions. In particular, infrared <span class="hlt">observations</span> are crucial to <span class="hlt">observe</span> scattered stellar radiation and thermal re-emission in the vicinity of embedded companions directly. For this purpose we performed radiative transfer simulations to calculate the thermal re-emission and scattered stellar flux from a protoplanetary disk hosting an embedded companion. Based on that, visibilities and closure phases are calculated to simulate <span class="hlt">observations</span> with the future beam combiner MATISSE, operating at the L, M and N bands at the VLTI. We find that the flux ratio of the embedded source to the central star can be as low as 0.5 to 0.6% for a detection at a feasible significance level due to the heated dust in the vicinity of the embedded source. Furthermore, we find that the likelihood for detection is highest for sources at intermediate distances r ≈ 2-5 au and disk masses not higher than ≈10-4 M⊙.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRA..120.6055Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRA..120.6055Y"><span>UV <span class="hlt">solar</span> irradiance in <span class="hlt">observations</span> and the NRLSSI and SATIRE-S models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yeo, K. L.; Ball, W. T.; Krivova, N. A.; Solanki, S. K.; Unruh, Y. C.; Morrill, J.</p> <p>2015-08-01</p> <p>Total <span class="hlt">solar</span> irradiance and UV spectral <span class="hlt">solar</span> irradiance has been monitored since 1978 through a succession of space missions. This is accompanied by the development of models aimed at replicating <span class="hlt">solar</span> irradiance by relating the variability to <span class="hlt">solar</span> magnetic activity. The Naval Research Laboratory <span class="hlt">Solar</span> 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 <span class="hlt">solar</span> irradiance over the period of satellite <span class="hlt">observation</span> currently available. There is persistent controversy between the various measurements and models in terms of the wavelength dependence of the variation over the <span class="hlt">solar</span> cycle, with repercussions on our understanding of the influence of UV <span class="hlt">solar</span> irradiance variability on the stratosphere. We review the measurement and modeling of UV <span class="hlt">solar</span> irradiance variability over the period of satellite <span class="hlt">observation</span>. The SATIRE-S reconstruction is consistent with spectral <span class="hlt">solar</span> irradiance <span class="hlt">observations</span> where they are reliable. It is also supported by an independent, empirical reconstruction of UV spectral <span class="hlt">solar</span> irradiance based on Upper Atmosphere Research Satellite/<span class="hlt">Solar</span> Ultraviolet Spectral Irradiance Monitor measurements from an earlier study. The weaker <span class="hlt">solar</span> 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 <span class="hlt">solar</span> cycle variability is detrimentally affected by the uncertainty in the SSI <span class="hlt">observations</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030111914&hterms=relativity+theory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Drelativity%2Btheory','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030111914&hterms=relativity+theory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Drelativity%2Btheory"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Test of Gravitational Theories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shapiro, Irwin I.</p> <p>2003-01-01</p> <p>We are engaged in testing gravitational theory, mainly using <span class="hlt">observations</span> of objects in the <span class="hlt">solar</span> <span class="hlt">system</span> and mainly on the interplanetary scale. Our goal is either to detect departures from the standard model (general relativity) - if any exist within the level of sensitivity of our data - or to place tighter bounds on such departures. For this project, we have analyzed a combination of <span class="hlt">observational</span> data with our model of the <span class="hlt">solar</span> <span class="hlt">system</span>, including primarily planetary radar ranging, lunar laser ranging, and spacecraft tracking, but also including both pulsar timing and pulsar VLBI measurements. In the past year, we have included new data in the analysis, primarily tracking data from the Mars Pathfinder mission. Although these data are relatively few in number, they extend the time span of high-precision tracking on the surface of Mars from six years to over 20. As a result, the statistical standard deviation of our estimate of Mars precession rate has nearly halved, and the rest of the parameters in our <span class="hlt">solar-system</span> model have experienced a corresponding, albeit smaller, improvement (about 20% for t,he relevant asteroid masses, 10% for the semimajor axis of Mars orbit, and smaller amounts for most other parameters). In the coming year, we plan to continue adding data to our set, as available. Ne 2 expect to use these data and improved models to obtain estimates of the gravitational- theory parameters and to publish these results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUSMSA32A..02D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUSMSA32A..02D"><span><span class="hlt">Solar</span> Control of Earth's Ionosphere: <span class="hlt">Observations</span> from <span class="hlt">Solar</span> Cycle 23</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Doe, R. A.; Thayer, J. P.; Solomon, S. C.</p> <p>2005-05-01</p> <p>A nine year database of sunlit E-region electron density altitude profiles (Ne(z)) measured by the Sondrestrom ISR has been partitioned over a 30-bin parameter space of averaged 10.7 cm <span class="hlt">solar</span> radio flux (F10.7) and <span class="hlt">solar</span> zenith angle (χ) to investigate long-term <span class="hlt">solar</span> and thermospheric variability, and to validate contemporary EUV photoionization models. A two stage filter, based on rejection of Ne(z) profiles with large Hall to Pedersen ratio, is used to minimize auroral contamination. Resultant filtered mean Ne(z) compares favorably with subauroral Ne measured for the same F10.7 and χ conditions at the Millstone Hill ISR. Mean Ne, as expected, increases with <span class="hlt">solar</span> activity and decreases with large χ, and the variance around mean Ne is shown to be greatest at low F10.7 (<span class="hlt">solar</span> minimum). ISR-derived mean Ne is compared with two EUV models: (1) a simple model without photoelectrons and based on the 5 -- 105 nm EUVAC model <span class="hlt">solar</span> flux [Richards et al., 1994] and (2) the GLOW model [Solomon et al., 1988; Solomon and Abreu, 1989] suitably modified for inclusion of XUV spectral components and photoelectron flux. Across parameter space and for all altitudes, Model 2 provides a closer match to ISR mean Ne and suggests that the photoelectron and XUV enhancements are essential to replicate measured plasma densities below 150 km. Simulated Ne variance envelopes, given by perturbing the Model 2 neutral atmosphere input by the measured extremum in Ap, F10.7, and Te, are much narrower than ISR-derived geophysical variance envelopes. We thus conclude that long-term variability of the EUV spectra dominates over thermospheric variability and that EUV spectral variability is greatest at <span class="hlt">solar</span> minimum. ISR -- model comparison also provides evidence for the emergence of an H (Lyman β) Ne feature at <span class="hlt">solar</span> maximum. Richards, P. G., J. A. Fennelly, and D. G. Torr, EUVAC: A <span class="hlt">solar</span> EUV flux model for aeronomic calculations, J. Geophys. Res., 99, 8981, 1994. Solomon, S. C., P. B. Hays</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006ihy..workE.100S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006ihy..workE.100S"><span><span class="hlt">Solar</span> <span class="hlt">Observations</span> as Educational Tools (P8)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shylaja, B. S.</p> <p>2006-11-01</p> <p>taralaya89@yahoo.co.in <span class="hlt">Solar</span> <span class="hlt">observations</span> are very handy tools to expose the students to the joy of research. In this presentation I briefly discuss the various experiments already done here with a small 6" Coude refractor. These include simple experiments like eclipse <span class="hlt">observations</span>, rotation measurements, variation in the angular size of the sun through the year as well as sun spot size variations, Doppler measurements, identification of elements from <span class="hlt">solar</span> spectrum (from published high resolution spectrum), limb darkening measurements, deriving the curve of growth (from published data). I also describe the theoretical implications of the experiments and future plans to develop this as a platform for motivating students towards a career in basic science 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_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/1999dss..book.....J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999dss..book.....J"><span>Discovering the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jones, Barrie W.</p> <p>1999-04-01</p> <p>Discovering the <span class="hlt">Solar</span> <span class="hlt">System</span> Barrie W. Jones The Open University, Milton Keynes, UK Discovering the <span class="hlt">Solar</span> <span class="hlt">System</span> is a comprehensive, up-to-date account of the <span class="hlt">Solar</span> <span class="hlt">System</span> and of the ways in which the various bodies have been investigated and modelled. The approach is thematic, with sequences of chapters on the interiors of planetary bodies, on their surfaces, and on their atmospheres. Within each sequence there is a chapter on general principles and processes followed by one or two chapters on specific bodies. There is also an introductory chapter, a chapter on the origin of the <span class="hlt">Solar</span> <span class="hlt">System</span>, and a chapter on asteroids, comets and meteorites. Liberally illustrated with diagrams, black and white photographs and colour plates, Discovering the <span class="hlt">Solar</span> <span class="hlt">System</span> also features: * tables of essential data * question and answers within the text * end of section review questions with answers and comments Discovering the <span class="hlt">Solar</span> <span class="hlt">System</span> is essential reading for all undergraduate students for whom astronomy or planetary science are components of their degrees, and for those at a more advanced level approaching the subject for the first time. It will also be of great interest to non-specialists with a keen interest in astronomy. A small amount of scientific knowledge is assumed plus familiarity with basic algebra and graphs. There is no calculus. Praise for this book includes: ".certainly qualifies as an authoritative text. The author clearly has an encyclopedic knowledge of the subject." Meteorics and Planetary Science ".liberally doused with relevant graphs, tables, and black and white figures of good quality." EOS, Transactions of the American Geophysical Union ".one of the best books on the <span class="hlt">Solar</span> <span class="hlt">System</span> I have seen. The general accuracy and quality of the content is excellent." Journal of the British Astronomical Association</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018oeps.book....2M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018oeps.book....2M"><span>The Formation and Evolution of the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marov, Mikhail</p> <p>2018-05-01</p> <p>The formation and evolution of our <span class="hlt">solar</span> <span class="hlt">system</span> (and planetary <span class="hlt">systems</span> around other stars) are among the most challenging and intriguing fields of modern science. As the product of a long history of cosmic matter evolution, this important branch of astrophysics is referred to as stellar-planetary cosmogony. Interdisciplinary by way of its content, it is based on fundamental theoretical concepts and available <span class="hlt">observational</span> data on the processes of star formation. Modern <span class="hlt">observational</span> data on stellar evolution, disc formation, and the discovery of extrasolar planets, as well as mechanical and cosmochemical properties of the <span class="hlt">solar</span> <span class="hlt">system</span>, place important constraints on the different scenarios developed, each supporting the basic cosmogony concept (as rooted in the Kant-Laplace hypothesis). Basically, the sequence of events includes fragmentation of an original interstellar molecular cloud, emergence of a primordial nebula, and accretion of a protoplanetary gas-dust disk around a parent star, followed by disk instability and break-up into primary solid bodies (planetesimals) and their collisional interactions, eventually forming a planet. Recent decades have seen major advances in the field, due to in-depth theoretical and experimental studies. Such advances have clarified a new scenario, which largely supports simultaneous stellar-planetary formation. Here, the collapse of a protosolar nebula's inner core gives rise to fusion ignition and star birth with an accretion disc left behind: its continuing evolution resulting ultimately in protoplanets and planetary formation. Astronomical <span class="hlt">observations</span> have allowed us to resolve in great detail the turbulent structure of gas-dust disks and their dynamics in regard to <span class="hlt">solar</span> <span class="hlt">system</span> origin. Indeed radio isotope dating of chondrite meteorite samples has charted the age and the chronology of key processes in the formation of the <span class="hlt">solar</span> <span class="hlt">system</span>. Significant progress also has been made in the theoretical study and computer modeling</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011CoSka..41...85Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011CoSka..41...85Z"><span><span class="hlt">Solar</span> <span class="hlt">observations</span> carried out at the INAF - Catania Astrophysical Observatory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zuccarello, F.; Contarino, L.; Romano, P.</p> <p>2011-10-01</p> <p><span class="hlt">Solar</span> <span class="hlt">observations</span> at the INAF - Catania Astrophysical Observatory are carried out by means of an equatorial spar, which includes: a Cook refractor, used to make daily drawings of sunspot groups from visual <span class="hlt">observations</span>; a 150-mm refractor with an Hα Lyot filter for chromospheric <span class="hlt">observations</span>; a 150-mm refractor feeding an Hα Halle filter for limb <span class="hlt">observations</span> of the chromosphere. The photospheric and chromospheric data are daily distributed to several international <span class="hlt">Solar</span> Data Centers. Recently, a program of Flare Warning has been implemented, with the aim of determining the probability that an active region yields a flare on the basis of its characteristics deduced from optical <span class="hlt">observations</span>. Some science results obtained by means of <span class="hlt">solar</span> data acquired at the INAF - Catania Astrophysical Observatory, as well as by space-instruments data, are briefly described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004DPS....36.1311K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004DPS....36.1311K"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Educators Program</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Knudsen, R.</p> <p>2004-11-01</p> <p>The <span class="hlt">Solar</span> <span class="hlt">System</span> Educators Program is a nationwide network of highly motivated teachers who lead workshops that show other teachers in their local communities how to successfully incorporate NASA materials and research into their classes. Currently there are 57 <span class="hlt">Solar</span> <span class="hlt">System</span> Educators in 37 states whose workshops are designed to assist their fellow teachers in understanding and including standards-based NASA materials into their classroom activities. <span class="hlt">Solar</span> <span class="hlt">System</span> Educators attend a training institute during their first year in the program and have the option of attending subsequent annual institutes. The volunteers in this program receive additional web-based mission-specific telecon trainings in conjunction with the <span class="hlt">Solar</span> <span class="hlt">System</span> Ambassadors. Resource and handout materials in the form of DVDs, posters, pamphlets, fact sheets, postcards and bookmarks are also provided. Scientists can get involved with this program by partnering with the <span class="hlt">Solar</span> <span class="hlt">System</span> Educators in their regions, presenting at their workshops and mentoring these outstanding volunteers. This formal education program helps optimize project funding set aside for education through the efforts of these volunteer master teachers. At the same time, teachers become familiar with NASA's educational materials with which to inspire students into pursuing careers in science, technology, engineering and math.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6030685','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6030685"><span><span class="hlt">Solar</span> <span class="hlt">system</span> fault detection</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Farrington, R.B.; Pruett, J.C. Jr.</p> <p>1984-05-14</p> <p>A fault detecting apparatus and method are provided for use with an active <span class="hlt">solar</span> <span class="hlt">system</span>. The apparatus provides an indication as to whether one or more predetermined faults have occurred in the <span class="hlt">solar</span> <span class="hlt">system</span>. The apparatus includes a plurality of sensors, each sensor being used in determining whether a predetermined condition is present. The outputs of the sensors are combined in a pre-established manner in accordance with the kind of predetermined faults to be detected. Indicators communicate with the outputs generated by combining the sensor outputs to give the user of the <span class="hlt">solar</span> <span class="hlt">system</span> and the apparatus an indication as to whether a predetermined fault has occurred. Upon detection and indication of any predetermined fault, the user can take appropriate corrective action so that the overall reliability and efficiency of the active <span class="hlt">solar</span> <span class="hlt">system</span> are increased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/866073','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/866073"><span><span class="hlt">Solar</span> <span class="hlt">system</span> fault detection</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Farrington, Robert B.; Pruett, Jr., James C.</p> <p>1986-01-01</p> <p>A fault detecting apparatus and method are provided for use with an active <span class="hlt">solar</span> <span class="hlt">system</span>. The apparatus provides an indication as to whether one or more predetermined faults have occurred in the <span class="hlt">solar</span> <span class="hlt">system</span>. The apparatus includes a plurality of sensors, each sensor being used in determining whether a predetermined condition is present. The outputs of the sensors are combined in a pre-established manner in accordance with the kind of predetermined faults to be detected. Indicators communicate with the outputs generated by combining the sensor outputs to give the user of the <span class="hlt">solar</span> <span class="hlt">system</span> and the apparatus an indication as to whether a predetermined fault has occurred. Upon detection and indication of any predetermined fault, the user can take appropriate corrective action so that the overall reliability and efficiency of the active <span class="hlt">solar</span> <span class="hlt">system</span> are increased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4291657','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4291657"><span>Exoplanet orbital eccentricity: Multiplicity relation and the <span class="hlt">Solar</span> <span class="hlt">System</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>Limbach, Mary Anne; Turner, Edwin L.</p> <p>2015-01-01</p> <p>The known population of exoplanets exhibits a much wider range of orbital eccentricities than <span class="hlt">Solar</span> <span class="hlt">System</span> planets and has a much higher average eccentricity. These facts have been widely interpreted to indicate that the <span class="hlt">Solar</span> <span class="hlt">System</span> is an atypical member of the overall population of planetary <span class="hlt">systems</span>. We report here on a strong anticorrelation of orbital eccentricity with multiplicity (number of planets in the <span class="hlt">system</span>) among cataloged radial velocity (RV) <span class="hlt">systems</span>. The mean, median, and rough distribution of eccentricities of <span class="hlt">Solar</span> <span class="hlt">System</span> planets fits an extrapolation of this anticorrelation to the eight-planet case rather precisely despite the fact that no more than two <span class="hlt">Solar</span> <span class="hlt">System</span> planets would be detectable with RV data comparable to that in the exoplanet sample. Moreover, even if regarded as a single or double planetary <span class="hlt">system</span>, the <span class="hlt">Solar</span> <span class="hlt">System</span> lies in a reasonably heavily populated region of eccentricity−multiplicity space. Thus, the <span class="hlt">Solar</span> <span class="hlt">System</span> is not anomalous among known exoplanetary <span class="hlt">systems</span> with respect to eccentricities when its multiplicity is taken into account. Specifically, as the multiplicity of a <span class="hlt">system</span> increases, the eccentricity decreases roughly as a power law of index –1.20. A simple and plausible but ad hoc and model-dependent interpretation of this relationship implies that ∼80% of the one-planet and 25% of the two-planet <span class="hlt">systems</span> in our sample have additional, as yet undiscovered, members but that <span class="hlt">systems</span> of higher <span class="hlt">observed</span> multiplicity are largely complete (i.e., relatively rarely contain additional undiscovered planets). If low eccentricities indeed favor high multiplicities, habitability may be more common in <span class="hlt">systems</span> with a larger number of planets. PMID:25512527</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900003175','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900003175"><span>A high-speed digital camera <span class="hlt">system</span> for the <span class="hlt">observation</span> of rapid H-alpha fluctuations in <span class="hlt">solar</span> flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kiplinger, Alan L.; Dennis, Brian R.; Orwig, Larry E.</p> <p>1989-01-01</p> <p>Researchers developed a prototype digital camera <span class="hlt">system</span> for obtaining H-alpha images of <span class="hlt">solar</span> flares with 0.1 s time resolution. They intend to operate this <span class="hlt">system</span> in conjunction with SMM's Hard X Ray Burst Spectrometer, with x ray instruments which will be available on the Gamma Ray Observatory and eventually with the Gamma Ray Imaging Device (GRID), and with the High Resolution Gamma-Ray and Hard X Ray Spectrometer (HIREGS) which are being developed for the Max '91 program. The digital camera has recently proven to be successful as a one camera <span class="hlt">system</span> operating in the blue wing of H-alpha during the first Max '91 campaign. Construction and procurement of a second and possibly a third camera for simultaneous <span class="hlt">observations</span> at other wavelengths are underway as are analyses of the campaign data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PRP.....2....1S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PRP.....2....1S"><span>The complex planetary synchronization structure of the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scafetta, N.</p> <p>2014-01-01</p> <p>The complex planetary synchronization structure of the <span class="hlt">solar</span> <span class="hlt">system</span>, which since Pythagoras of Samos (ca. 570-495 BC) is known as the music of the spheres, is briefly reviewed from the Renaissance up to contemporary research. Copernicus' heliocentric model from 1543 suggested that the planets of our <span class="hlt">solar</span> <span class="hlt">system</span> form a kind of mutually ordered and quasi-synchronized <span class="hlt">system</span>. From 1596 to 1619 Kepler formulated preliminary mathematical relations of approximate commensurabilities among the planets, which were later reformulated in the Titius-Bode rule (1766-1772), which successfully predicted the orbital position of Ceres and Uranus. Following the discovery of the ~ 11 yr sunspot cycle, in 1859 Wolf suggested that the <span class="hlt">observed</span> <span class="hlt">solar</span> variability could be approximately synchronized with the orbital movements of Venus, Earth, Jupiter and Saturn. Modern research has further confirmed that (1) the planetary orbital periods can be approximately deduced from a simple <span class="hlt">system</span> of resonant frequencies; (2) the <span class="hlt">solar</span> <span class="hlt">system</span> oscillates with a specific set of gravitational frequencies, and many of them (e.g., within the range between 3 yr and 100 yr) can be approximately constructed as harmonics of a base period of ~ 178.38 yr; and (3) <span class="hlt">solar</span> and climate records are also characterized by planetary harmonics from the monthly to the millennial timescales. This short review concludes with an emphasis on the contribution of the author's research on the empirical evidences and physical modeling of both <span class="hlt">solar</span> and climate variability based on astronomical harmonics. The general conclusion is that the <span class="hlt">solar</span> <span class="hlt">system</span> works as a resonator characterized by a specific harmonic planetary structure that also synchronizes the Sun's activity and the Earth's climate. The special issue Pattern in <span class="hlt">solar</span> variability, their planetary origin and terrestrial impacts (Mörner et al., 2013) further develops the ideas about the planetary-<span class="hlt">solar</span>-terrestrial interaction with the personal contribution of 10</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020044830','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020044830"><span><span class="hlt">Solar-System</span> Tests of Gravitational Theories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shapiro, Irwin I.</p> <p>2002-01-01</p> <p>We are engaged in testing gravitational theory by means of <span class="hlt">observations</span> of objects in the <span class="hlt">solar</span> <span class="hlt">system</span>. This work tests the equivalence principle (EP), the Shapiro time delay, the advances of planetary perihelion, the possibility of a secular variation G(dot) in the 'gravitational constant' G, and the rate of the de Sitter (geodetic) precession of the Earth-Moon <span class="hlt">system</span>. We describe here the results under this contract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900027756&hterms=nonimaging&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dnonimaging','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900027756&hterms=nonimaging&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dnonimaging"><span>Simultaneous multi-frequency imaging <span class="hlt">observations</span> of <span class="hlt">solar</span> microwave bursts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kundu, M. R.; White, S. M.; Schmahl, E. J.</p> <p>1989-01-01</p> <p>The results of simultaneous two-frequency imaging <span class="hlt">observations</span> of <span class="hlt">solar</span> microwave bursts with the Very Large Array are reviewed. Simultaneous 2 and 6 cm <span class="hlt">observations</span> have been made of bursts which are optically thin at both frequencies, or optically thick at the lower frequency. In the latter case, the source structure may differ at the two frequencies, but the two sources usually seem to be related. However, this is not always true of simultaneous 6 and 20 cm <span class="hlt">observations</span>. The results have implications for the analysis of nonimaging radio data of <span class="hlt">solar</span> and stellar flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984bahi.rept.....N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984bahi.rept.....N"><span><span class="hlt">Solar</span>-gas <span class="hlt">systems</span> impact analysis study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Neill, C. P.; Hahn, E. F.; Loose, J. C.; Poe, T. E.; Hirshberg, A. S.; Haas, S.; Preble, B.; Halpin, J.</p> <p>1984-07-01</p> <p>The impacts of <span class="hlt">solar</span>/gas technologies on gas consumers and on gas utilities were measured separately and compared against the impacts of competing gas and electric <span class="hlt">systems</span> in four climatic regions of the U.S. A methodology was developed for measuring the benefits or penalties of <span class="hlt">solar</span>/gas <span class="hlt">systems</span> on a combined basis for consumers sand distribution companies. It is shown that the combined benefits associated with <span class="hlt">solar</span>/gas <span class="hlt">systems</span> are generally greatest when the <span class="hlt">systems</span> are purchased by customers who would have otherwise chosen high-efficiency electric <span class="hlt">systems</span> (were <span class="hlt">solar</span>/gas <span class="hlt">systems</span> not available in the market place). The role of gas utilities in encouraging consumer acceptance of <span class="hlt">solar</span>/gas <span class="hlt">systems</span> was also examined ion a qualitative fashion. A decision framework for analyzing the type and level of utility involvement in <span class="hlt">solar</span>/gas technologies was developed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28554978','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28554978"><span>Asteroid-comet continuum objects in the <span class="hlt">solar</span> <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hsieh, Henry H</p> <p>2017-07-13</p> <p>In this review presented at the Royal Society meeting, 'Cometary science after Rosetta', I present an overview of studies of small <span class="hlt">solar</span> <span class="hlt">system</span> objects that exhibit properties of both asteroids and comets (with a focus on so-called active asteroids). Sometimes referred to as 'transition objects', these bodies are perhaps more appropriately described as 'continuum objects', to reflect the notion that rather than necessarily representing actual transitional evolutionary states between asteroids and comets, they simply belong to the general population of small <span class="hlt">solar</span> <span class="hlt">system</span> bodies that happen to exhibit a continuous range of <span class="hlt">observational</span>, physical and dynamical properties. Continuum objects are intriguing because they possess many of the properties that make classical comets interesting to study (e.g. relatively primitive compositions, ejection of surface and subsurface material into space where it can be more easily studied, and orbital properties that allow us to sample material from distant parts of the <span class="hlt">solar</span> <span class="hlt">system</span> that would otherwise be inaccessible), while allowing us to study regions of the <span class="hlt">solar</span> <span class="hlt">system</span> that are not sampled by classical comets.This article is part of the themed issue 'Cometary science after Rosetta'. © 2017 The Author(s).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6348968-galaxy-solar-system','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6348968-galaxy-solar-system"><span>Galaxy and the <span class="hlt">solar</span> <span class="hlt">system</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>Smoluchowski, R.; Bahcall, J.M.; Matthews, M.S.</p> <p>1986-01-01</p> <p>The <span class="hlt">solar</span>-Galactic neighborhood, massive interstellar clouds and other Galactic features, the Oort cloud, perturbations of the <span class="hlt">solar</span> <span class="hlt">system</span>, and the existence and stability of a <span class="hlt">solar</span> companion star are examined in chapters based on contributions to a conference held in Tucson, AZ during January 1985. The individual topics addressed include: the Galactic environment of the <span class="hlt">solar</span> <span class="hlt">system</span>; stars within 25 pc of the sun; the path of the sun in 100 million years; the local velocity field in the last billion years; interstellar clouds near the sun; and evidence for a local recent supernova. Also considered are: dynamic influence ofmore » Galactic tides and molecular clouds on the Oort cloud; cometary evidence for a <span class="hlt">solar</span> companion; dynamical interactions between the Oort cloud and the Galaxy; geological periodicities and the Galaxy; giant comets and the Galaxy; dynamical evidence for Planet X; evolution of the <span class="hlt">solar</span> <span class="hlt">system</span> in the presence of a <span class="hlt">solar</span> companion star; mass extinctions, crater ages, and comet showers; evidence for Nemesis, a <span class="hlt">solar</span> companion star.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPSC...11..102P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPSC...11..102P"><span>Transits in our <span class="hlt">Solar</span> <span class="hlt">System</span> for educational activities: Mercury Transit 2016 and Total <span class="hlt">Solar</span> Eclipse 2017</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pérez-Ayúcar, M.; Breitfelner, M.</p> <p>2017-09-01</p> <p><span class="hlt">Solar</span> transits are rare astronomical event of profound historical importance and with an enormous potential to engage nowadays students and general public into Planetary Sciences and Space. Mercury transits occur only about every 13-14 times per century. Total <span class="hlt">solar</span> eclipses occur around 18 months apart somewhere on Earth, but they recur only every 3-4 centuries on the same location. Although its historic scientific importance (examples, to measure the distances in the <span class="hlt">solar</span> <span class="hlt">system</span>, to <span class="hlt">observe</span> the <span class="hlt">solar</span> corona) has diminished since humanity roams our <span class="hlt">solar</span> <span class="hlt">system</span> with robotic spacecrafts, transits remain a spectacular astronomical event that is used very effectively to engage general public and students to Science and Space in general. The educational project CESAR (Cooperation through Education in Science and Astronomy Research) has been covering since 2012 such events (Venus transit 2012, live Sun transmissions, <span class="hlt">solar</span> eclipses, ISS transits ...). We report the outstanding outcome of the two public educational and outreach events since last year: the May 2016 Mercury Transit, and the recent August 2017 Total Eclipse. And the follow up activities expected for future transits.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.P21A1202S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.P21A1202S"><span>Modeling the <span class="hlt">Solar</span> Probe Plus Dust Environment: Comparison with MESSENGER <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>Strong, S. B.; Strikwerda, T.</p> <p>2009-12-01</p> <p>NASA’s <span class="hlt">Solar</span> Probe Plus mission will be the first to approach the Sun as close as 9 <span class="hlt">solar</span> radii from the surface. This mission will provide the only in-situ <span class="hlt">observations</span> of the Sun’s corona. In the absence of <span class="hlt">observational</span> data (e.g. Helios, Pioneer), specifically at distances less than 0.4 AU, the precise ambient dust distributions at these distances remain unknown and limited to extrapolative models for distances < 1 AU (e.g. Mann et al. 2004). For the <span class="hlt">Solar</span> Probe Plus mission, it has become critical to characterize the inner <span class="hlt">solar</span> <span class="hlt">system</span> dust environment in order to examine potential impacts on spacecraft health and attitude. We have implemented the Mann et al. (2004) and Grün et al. (1985) dust distribution theory along with Mie scattering effects to determine the magnitude of <span class="hlt">solar</span> irradiance scattered towards an optical sensor such as a star tracker as a function of ecliptic latitude and longitude for distances 0.05 to 1 AU. Background irradiance data from NASA’s MESSENGER mission (down to 0.3 AU) reveal trends consistent with our model predictions, potentially validating Mann et al. (2004) and Grün et al. (1985) theory, but perhaps suggesting an enhancement of dust density short ward of 0.3 AU. This paper will present the scattering model and analysis of MESSENGER data gathered to date, during the phasing orbits, and includes star tracker background irradiance, irradiance distribution over the sky, and effects on star magnitude sensitivity and position accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH51C2513A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH51C2513A"><span>Periodicities <span class="hlt">observed</span> on <span class="hlt">solar</span> flux index (F10.7) during geomagnetic disturbances</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Adhikari, B.; Narayan, C.; Chhatkuli, D. N.</p> <p>2017-12-01</p> <p><span class="hlt">Solar</span> activities change within the period of 11 years. Sometimes the greatest event occurs in the period of <span class="hlt">solar</span> maxima and the lowest activity occurs in the period of <span class="hlt">solar</span> minimum. During the time period of <span class="hlt">solar</span> activity sunspots number will vary. A 10.7 cm <span class="hlt">solar</span> flux measurement is a determination of the strength of <span class="hlt">solar</span> radio emission. The <span class="hlt">solar</span> flux index is more often used for the prediction and monitoring of the <span class="hlt">solar</span> activity. This study mainly focused on the variation on <span class="hlt">solar</span> flux index and amount of electromagnetic wave in the atmosphere. Both seasonal and yearly variation on <span class="hlt">solar</span> F10.7 index. We also analyzed the dataset obatained from riometer.Both instruments show seasonal and yearly variations. We also <span class="hlt">observed</span> the <span class="hlt">solar</span> cycle dependence on <span class="hlt">solar</span> flux index and found a strong dependence on <span class="hlt">solar</span> activity. Results also show that <span class="hlt">solar</span> intensities higher during the rising phase of <span class="hlt">solar</span> cycle. We also <span class="hlt">observed</span> periodicities on <span class="hlt">solar</span> flux index using wavelet analysis. Through this analysis, it was found that the power intensities of <span class="hlt">solar</span> flux index show a high spectral variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.6369D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.6369D"><span>Forbush Decrease Prediction Based on Remote <span class="hlt">Solar</span> <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>Dumbovic, Mateja; Vrsnak, Bojan; Calogovic, Jasa</p> <p>2016-04-01</p> <p>We study the relation between remote <span class="hlt">observations</span> of coronal mass ejections (CMEs), their associated <span class="hlt">solar</span> flares and short-term depressions in the galactic cosmic-ray flux (so called Forbush decreases). Statistical relations between Forbush decrease magnitude and several CME/flare parameters are examined. In general we find that Forbush decrease magnitude is larger for faster CMEs with larger apparent width, which is associated with stronger flares that originate close to the center of the <span class="hlt">solar</span> disk and are (possibly) involved in a CME-CME interaction. The statistical relations are quantified and employed to forecast expected Forbush decrease magnitude range based on the selected remote <span class="hlt">solar</span> <span class="hlt">observations</span> of the CME and associated <span class="hlt">solar</span> flare. Several verification measures are used to evaluate the forecast method. We find that the forecast is most reliable in predicting whether or not a CME will produce a Forbush decrease with a magnitude >3 %. The main advantage of the method is that it provides an early prediction, 1-4 days in advance. Based on the presented research, an online forecast tool was developed (Forbush Decrease Forecast Tool, FDFT) available at Hvar Observatory web page: http://oh.geof.unizg.hr/FDFT/fdft.php. We acknowledge the support of Croatian Science Foundation under the project 6212 "<span class="hlt">Solar</span> and Stellar Variability" and of European social fond under the project "PoKRet".</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AcASn..55..447S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AcASn..55..447S"><span>Multi-wavelength and High-resolution <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Eruptive Activities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Y. D.</p> <p>2014-09-01</p> <p>In recent years, various <span class="hlt">solar</span> eruptive activities have been <span class="hlt">observed</span> in the <span class="hlt">solar</span> atmosphere, such as <span class="hlt">solar</span> flares, filament eruptions, jets, coronal mass ejections (CMEs), and magnetohydrodynamics (MHD) waves. Previous <span class="hlt">observations</span> have indicated that <span class="hlt">solar</span> magnetic field plays a dominant role in the processes of all kinds of <span class="hlt">solar</span> activities. Since many large-scale <span class="hlt">solar</span> eruptive activities can cause significant effects on the space environment of the Earth as well as the human life, studying and forecasting the <span class="hlt">solar</span> activities are urgent tasks for us. In addition, the Sun is the nearest star to the Earth, so that people can directly <span class="hlt">observe</span> and study it in detail. Hence, studying the Sun can also provide a reference to study other stars in the universe. This thesis focuses on the multi-wavelength and high-resolution <span class="hlt">observations</span> of three types of <span class="hlt">solar</span> eruptive activities: filament eruptions, coronal jets, and coronal MHD waves. By analyzing various <span class="hlt">observations</span> taken by ground-based and space-borne instruments, we try to understand the inherent physical mechanisms, and construct models to interpret different kinds of <span class="hlt">solar</span> eruptive activities. The triggering mechanism and the cause of a failed filament eruption are studied in Chapter 3, which indicates that the energy released in the flare is a key factor to the fate of the filament. Two successive filament eruptions are studied in Chapter 4, which indicates that the magnetic implosion could be the physical linkage between them, and the structures of coronal magnetic fields are important for producing sympathetic eruptions. A magnetic unwinding jet and a blowout jet are studied in Chapters 5 and 6, respectively. The former exhibits obvious radial expansion, which undergoes three distinct phases: the slow expansion phase, the fast expansion phase, and the steady phase. In addition, calculation indicates that the non-potential magnetic field in the jet can supply sufficient energy for producing the unwinding</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003791&hterms=THz&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DTHz','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003791&hterms=THz&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DTHz"><span>THz <span class="hlt">Solar</span> <span class="hlt">Observations</span> on Board of a Trans-Antarctic Stratospheric Balloon Flight</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kaufmann, P.; Abrantes, A.; Bortolucci, E. C.; Caspi, A.; Fernandes, L. O. T.; Kropotov, G.; Kudaka, A. S.; Laurent, G.; Machado, N.; Marcon, R.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003791'); toggleEditAbsImage('author_20170003791_show'); toggleEditAbsImage('author_20170003791_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003791_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003791_hide"></p> <p>2016-01-01</p> <p>A new <span class="hlt">system</span> of two photometers was built to <span class="hlt">observe</span> the Sun at 3 and 7 THz from space, named SOLART. It has been flown coupled to U.C. Berkeley GRIPS experiment on a NASA stratospheric balloon flight over Antarctica, 19-30 January 2016. The mission was successfully accomplished. We describe the <span class="hlt">system</span> performance, <span class="hlt">solar</span> brightness determination and the first THz impulsive burst detected.</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('http://adsabs.harvard.edu/abs/2000AIPC..510..551E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000AIPC..510..551E"><span>High-energy <span class="hlt">solar</span> flare <span class="hlt">observations</span> at the Y2K maximum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emslie, A. Gordon</p> <p>2000-04-01</p> <p><span class="hlt">Solar</span> flares afford an opportunity to <span class="hlt">observe</span> processes associated with the acceleration and propagation of high-energy particles at a level of detail not accessible in any other astrophysical source. I will review some key results from previous high-energy <span class="hlt">solar</span> flare <span class="hlt">observations</span>, including those from the Compton Gamma-Ray Observatory, and the problems that they pose for our understanding of energy release and particle acceleration processes in the astrophysical environment. I will then discuss a program of high-energy <span class="hlt">observations</span> to be carried out during the upcoming 2000-2001 <span class="hlt">solar</span> maximum that is aimed at addressing and resolving these issues. A key element in this <span class="hlt">observational</span> program is the High Energy <span class="hlt">Solar</span> Spectroscopic Imager (HESSI) spacecraft, which will provide imaging spectroscopic <span class="hlt">observations</span> with spatial, temporal, and energy resolutions commensurate with the physical processes believed to be operating, and will in addition provide the first true gamma-ray spectroscopy of an astrophysical source. .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSM23D..01M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSM23D..01M"><span>Magnetopause Boundary Processes Throughout the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Masters, A.</p> <p>2014-12-01</p> <p>Earth is not the only planet in the <span class="hlt">Solar</span> <span class="hlt">System</span> with a natural magnetic shield. Mercury, Jupiter, Saturn, Uranus, and Neptune are similarly protected from the <span class="hlt">solar</span> wind and cosmic rays. However, like our planet, the magnetic shielding of each of these magnetized planets can break down, driving energy flow through each planetary magnetosphere. Although studies of the magnetopause boundary of Earth's magnetosphere have shed considerable light on the processes that lead to this breakdown, the extent to which we can apply this understanding to the diverse space plasma environments surrounding other planets remains unclear. Here we review what we have learnt so far about the operation of magnetopause boundary processes at all the magnetized planets in the <span class="hlt">Solar</span> <span class="hlt">System</span>, and outline some of the relevant outstanding questions. We start by consolidating present understanding of terrestrial magnetopause processes, which is our reference when considering other boundaries. We focus on selected processes (magnetic reconnection, Kelvin-Helmholtz instability), compare how we expect them to operate at each planetary magnetopause, and assess whether or not this is consistent with in situ spacecraft <span class="hlt">observations</span>. For each planetary magnetosphere we then discuss the nature of the total interaction with the <span class="hlt">solar</span> wind, and whether this is expected to be dominant over internal drivers of magnetospheric dynamics. A combination of further spacecraft exploration and dedicated numerical modeling is required in order to address the many outstanding questions concerning this topic. Progress in this direction would have broad implications for other space plasma <span class="hlt">systems</span>, in our <span class="hlt">solar</span> <span class="hlt">system</span> and beyond.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990080908&hterms=theory+building&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtheory%2Bbuilding','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990080908&hterms=theory+building&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtheory%2Bbuilding"><span>Update of the ISTP <span class="hlt">Solar</span> Maximum Mission: ISTP Project Scientist for Theory and Ground-Based <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>Curtis, Steve</p> <p>1999-01-01</p> <p>Building upon the numerous successes of the pre-<span class="hlt">solar</span> maximum International <span class="hlt">Solar</span> Terrestrial Physics (ISTP) mission, the ISTP <span class="hlt">Solar</span> Maximum Mission is expected to produce new insights into global flow of energy, momentum, and mass, from the Sun, through the heliosphere, into the magnetosphere and to their final deposition in the terrestrial upper atmosphere/ionosphere <span class="hlt">system</span>. Of particular interest is the determination of the geo-effectiveness of <span class="hlt">solar</span> events, principally Coronal Mass Ejections (CMEs). Given the expected increased frequency and strength of CMEs during the <span class="hlt">Solar</span> Maximum period, a major advance in our understanding of nature of the coupling of CMEs to the magnetosphere-ionosphere-atmosphere <span class="hlt">system</span> is expected. The roles during this time of the various ISTP assets will be discussed. These assets will include the SOHO, Wind, Polar, and Geotail spacecraft, the ground-based <span class="hlt">observing</span> networks and the theory tools.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960009416','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960009416"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Exploration, 1995-2000</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Squyres, S.; Varsi, G.; Veverka, J.; Soderblom, L.; Black, D.; Stern, A.; Stetson, D.; Brown, R. A.; Niehoff, J.; Squibb, G.</p> <p>1994-01-01</p> <p>Goals for planetary exploration during the next decade include: (1) determine how our <span class="hlt">solar</span> <span class="hlt">system</span> formed, and understand whether planetary <span class="hlt">systems</span> are a common phenomenon through out the cosmos; (2) explore the diverse changes that planets have undergone throughout their history and that take place at present, including those that distinguish Earth as a planet; (3) understand how life might have formed on Earth, whether life began anywhere else in the <span class="hlt">solar</span> <span class="hlt">system</span>, and whether life (including intelligent beings) might be a common cosmic phenomenon; (4) discover and investigate natural phenomena that occur under conditions not realizable in laboratories; (5) discover and inventory resources in the <span class="hlt">solar</span> <span class="hlt">system</span> that could be used by human civilizations in the future; and (6) make the <span class="hlt">solar</span> <span class="hlt">system</span> a part of the human experience in the same way that Earth is, and hence lay the groundwork for human expansion into the <span class="hlt">solar</span> <span class="hlt">system</span> in the coming century. The plan for <span class="hlt">solar</span> <span class="hlt">system</span> exploration is motivated by these goals as well as the following principle: The <span class="hlt">solar</span> <span class="hlt">system</span> exploration program will conduct flight programs and supporting data analysis and scientific research commensurate with United States leadership in space exploration. These programs and research must be of the highest scientific merit, they must be responsive to public excitement regarding planetary exploration, and they must contribute to larger national goals in technology and education. The result will be new information, which is accessible to the public, creates new knowledge, and stimulates programs of education to increase the base of scientific knowledge in the general public.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhTea..55..240L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhTea..55..240L"><span>Studying the <span class="hlt">Solar</span> <span class="hlt">System</span> Can Be More Than Just "Stamp Collecting"</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>LoPresto, Michael C.</p> <p>2017-04-01</p> <p>While teaching his first-ever introductory college astronomy course, I heard a graduate student make the comment that compared to other areas of astronomy, studying the <span class="hlt">solar</span> <span class="hlt">system</span> is just "stamp collecting." Coverage of the <span class="hlt">solar</span> <span class="hlt">system</span> in an introductory college astronomy course certainly could consist mostly of showing images and reporting facts, but by using <span class="hlt">observations</span> that can be made from images and also data and other known facts about the objects, instruction on <span class="hlt">solar</span> <span class="hlt">system</span> topics can be more conceptual, involving just as much inquiry and discovery as any area of astronomy or physics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7739E..2OC','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7739E..2OC"><span>Secondary mirror <span class="hlt">system</span> for the European <span class="hlt">Solar</span> Telescope (EST)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cavaller, L.; Siegel, B.; Prieto, G.; Hernandez, E.; Casalta, J. M.; Mercader, J.; Barriga, J.</p> <p>2010-07-01</p> <p>The European <span class="hlt">Solar</span> Telescope (EST) is a European collaborative project to build a 4m class <span class="hlt">solar</span> telescope in the Canary Islands, which is now in its design study phase. The telescope will provide diffraction limited performance for several instruments <span class="hlt">observing</span> simultaneously at the Coudé focus at different wavelengths. A multi-conjugated adaptive optics <span class="hlt">system</span> composed of a tip-tilt mirror and several deformable mirrors will be integrated in the telescope optical path. The secondary mirror <span class="hlt">system</span> is composed of the mirror itself (Ø800mm), the alignment drives and the cooling <span class="hlt">system</span> needed to remove the <span class="hlt">solar</span> heat load from the mirror. During the design study the feasibility to provide fast tip-tilt capabilities at the secondary mirror to work as the adaptive optics tip-tilt mirror is also being evaluated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840057982&hterms=radiation+Solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dradiation%2BSolar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840057982&hterms=radiation+Solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dradiation%2BSolar"><span><span class="hlt">Observed</span> ozone response to variations in <span class="hlt">solar</span> ultraviolet radiation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gille, J. C.; Smythe, C. M.; Heath, D. F.</p> <p>1984-01-01</p> <p>During the winter of 1979, the <span class="hlt">solar</span> ultraviolet irradiance varied with a period of 13.5 days and an amplitude of 1 percent. The zonal mean ozone values in the tropics varied with the <span class="hlt">solar</span> irradiance, with an amplitude of 0.25 to 0.60 percent. This <span class="hlt">observation</span> agrees with earlier calculations, although the response may be overestimated. These results imply changes in ozone at an altitude of 48 kilometers of up to 12 percent over an 11-year <span class="hlt">solar</span> cycle. Interpretation of ozone changes in the upper stratosphere will require measurements of <span class="hlt">solar</span> ultraviolet radiation at wavelengths near 200 nanometers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150008280','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150008280"><span>Approaching <span class="hlt">Solar</span> Maximum 24 with Stereo-Multipoint <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Energetic Particle Events</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dresing, N.; Cohen, C. M. S.; Gomez-Herrero, R.; Heber, B.; Klassen, A.; Leske, R. A.; Mason, G. M.; Mewaldt, R. A.; von Rosenvinge, T. T.</p> <p>2014-01-01</p> <p>Since the beginning of the <span class="hlt">Solar</span> Terrestrial Relations Observatory (STEREO) mission at the end of 2006, the two spacecraft have now separated by more than 130? degrees from the Earth. A 360-degree view of the Sun has been possible since February 2011, providing multipoint in situ and remote sensing <span class="hlt">observations</span> of unprecedented quality. Combining STEREO <span class="hlt">observations</span> with near-Earth measurements allows the study of <span class="hlt">solar</span> energetic particle (SEP) events over a wide longitudinal range with minimal radial gradient effects. This contribution provides an overview of recent results obtained by the STEREO/IMPACT team in combination with <span class="hlt">observations</span> by the ACE and SOHO spacecraft. We focus especially on multi-spacecraft investigations of SEP events. The large longitudinal spread of electron and 3He-rich events as well as unusual anisotropies will be presented and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://nineplanets.org','SCIGOVWS'); return false;" href="http://nineplanets.org"><span>The Nine Planets <span class="hlt">Solar</span> <span class="hlt">System</span> Tour</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p><em>Astronomy</em> news section which gives news, notes and general <span class="hlt">observations</span>, we also have an interactive tour of ; Notes <em>Astronomy</em> picture of the day. For a full list of contents please see here. cna classes online Professional <em>Astronomy</em> research paper writing help can be found at AdvancedWriters.com. <span class="hlt">Solar</span> <span class="hlt">system</span> tour</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004A%26A...427..717A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004A%26A...427..717A"><span>Comparison of CCD astrolabe multi-site <span class="hlt">solar</span> diameter <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>Andrei, A. H.; Boscardin, S. C.; Chollet, F.; Delmas, C.; Golbasi, O.; Jilinski, E. G.; Kiliç, H.; Laclare, F.; Morand, F.; Penna, J. L.; Reis Neto, E.</p> <p>2004-11-01</p> <p>Results are presented of measured variations of the photospheric <span class="hlt">solar</span> diameter, as concurrently <span class="hlt">observed</span> at three sites of the R2S3 (Réseau de Suivi au Sol du Rayon Solaire) consortium in 2001. Important <span class="hlt">solar</span> flux variations appeared in that year, just after the maximum of <span class="hlt">solar</span> activity cycle 23, make that time stretch particularly promising for a comparison of the multi-site results. The sites are those in Turkey, France and Brasil. All <span class="hlt">observations</span> are made with similar CCD <span class="hlt">solar</span> astrolabes, and at nearby effective wavelengths. The data reductions share algorithms, that are alike, the outcomes of which are here treated after applying a normalization correction using the Fried parameter. Since the sites are geographically quite far, atmospheric conditions are dismissed as possible causes of the large common trend found. Owing to particularities of each site, the common continuous <span class="hlt">observational</span> period extends from April to September. The standard deviation for the daily averages is close to 0.47 arcsec for the three sites. Accordingly, the three series are smoothed by a low-pass-band Fourier filter of 150 <span class="hlt">observations</span> (typically one month). The main common features found are a declining linear trend, of the order of 0.7 mas/day, and a relative maximum, around MJD 2120, of the order of 100 mas. Standard statistical tests endorse the correlation of the three series.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E2170E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E2170E"><span>Can The Periods of Some Extra-<span class="hlt">Solar</span> Planetary <span class="hlt">Systems</span> be Quantized?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El Fady Morcos, Abd</p> <p></p> <p>A simple formula was derived before by Morcos (2013 ), to relate the quantum numbers of planetary <span class="hlt">systems</span> and their periods. This formula is applicable perfectly for the <span class="hlt">solar</span> <span class="hlt">system</span> planets, and some extra-<span class="hlt">solar</span> planets , of stars of approximately the same masses like the Sun. This formula has been used to estimate the periods of some extra-<span class="hlt">solar</span> planet of known quantum numbers. The used quantum numbers were calculated previously by other authors. A comparison between the <span class="hlt">observed</span> and estimated periods, from the given formula has been done. The differences between the <span class="hlt">observed</span> and calculated periods for the extra-<span class="hlt">solar</span> <span class="hlt">systems</span> have been calculated and tabulated. It is found that there is an error of the range of 10% The same formula has been also used to find the quantum numbers, of some known periods, exo-planet. Keywords: Quantization; Periods; Extra-Planetary; Extra-<span class="hlt">Solar</span> Planet REFERENCES [1] Agnese, A. G. and Festa, R. “Discretization on the Cosmic Scale Inspirred from the Old Quantum Mechanics,” 1998. http://arxiv.org/abs/astro-ph/9807186 [2] Agnese, A. G. and Festa, R. “Discretizing ups-Andro- medae Planetary <span class="hlt">System</span>,” 1999. http://arxiv.org/abs/astro-ph/9910534. [3] Barnothy, J. M. “The Stability of the <span class="hlt">Solar</span> Systemand of Small Stellar <span class="hlt">Systems</span>,” Proceedings of the IAU Sympo-sium 62, Warsaw, 5-8 September 1973, pp. 23-31. [4] Morcos, A.B. , “Confrontation between Quantized Periods of Some Extra-<span class="hlt">Solar</span> Planetary <span class="hlt">Systems</span> and Observations”, International Journal of Astronomy and Astrophysics, 2013, 3, 28-32. [5] Nottale, L. “Fractal Space-Time and Microphysics, To-wards a Theory of Scale Relativity,” World Scientific, London, 1994. [6] Nottale , L., “Scale-Relativity and Quantization of Extra- <span class="hlt">Solar</span> Planetary <span class="hlt">Systems</span>,” Astronomy & Astrophysics, Vol. 315, 1996, pp. L9-L12 [7] Nottale, L., Schumacher, G. and Gay, J. “Scale-Relativity and Quantization of the <span class="hlt">Solar</span> <span class="hlt">Systems</span>,” Astronomy & Astrophysics letters, Vol. 322, 1997, pp. 1018-10 [8</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22106251','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22106251"><span>Cosmochemical evidence for astrophysical processes during the formation of our <span class="hlt">solar</span> <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>MacPherson, Glenn J; Boss, Alan</p> <p>2011-11-29</p> <p>Through the laboratory study of ancient <span class="hlt">solar</span> <span class="hlt">system</span> materials such as meteorites and comet dust, we can recognize evidence for the same star-formation processes in our own <span class="hlt">solar</span> <span class="hlt">system</span> as those that we can <span class="hlt">observe</span> now through telescopes in nearby star-forming regions. High temperature grains formed in the innermost region of the <span class="hlt">solar</span> <span class="hlt">system</span> ended up much farther out in the <span class="hlt">solar</span> <span class="hlt">system</span>, not only the asteroid belt but even in the comet accretion region, suggesting a huge and efficient process of mass transport. Bi-polar outflows, turbulent diffusion, and marginal gravitational instability are the likely mechanisms for this transport. The presence of short-lived radionuclides in the early <span class="hlt">solar</span> <span class="hlt">system</span>, especially (60)Fe, (26)Al, and (41)Ca, requires a nearby supernova shortly before our <span class="hlt">solar</span> <span class="hlt">system</span> was formed, suggesting that the Sun was formed in a massive star-forming region similar to Orion or Carina. <span class="hlt">Solar</span> <span class="hlt">system</span> formation may have been "triggered" by ionizing radiation originating from massive O and B stars at the center of an expanding HII bubble, one of which may have later provided the supernova source for the short-lived radionuclides. Alternatively, a supernova shock wave may have simultaneously triggered the collapse and injected the short-lived radionuclides. Because the Sun formed in a region where many other stars were forming more or less contemporaneously, the bi-polar outflows from all such stars enriched the local region in interstellar silicate and oxide dust. This may explain several <span class="hlt">observed</span> anomalies in the meteorite record: a near absence of detectable (no extreme isotopic properties) presolar silicate grains and a dichotomy in the isotope record between (26)Al and nucleosynthetic (nonradiogenic) anomalies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA41B2371S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA41B2371S"><span>Radiation Environments for Future Human Exploration Throughout the <span class="hlt">Solar</span> <span class="hlt">System</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schwadron, N.; Gorby, M.; Linker, J.; Riley, P.; Torok, T.; Downs, C.; Spence, H. E.; Desai, M. I.; Mikic, Z.; Joyce, C. J.; Kozarev, K. A.; Townsend, L. W.; Wimmer-Schweingruber, R. F.</p> <p>2016-12-01</p> <p>Acute space radiation hazards pose one of the most serious risks to future human and robotic exploration. The ability to predict when and where large events will occur is necessary in order to mitigate their hazards. The largest events are usually associated with complex sunspot groups (also known as active regions) that harbor strong, stressed magnetic fields. Highly energetic protons accelerated very low in the corona by the passage of coronal mass ejection (CME)-driven compressions or shocks and from flares travel near the speed of light, arriving at Earth minutes after the eruptive event. Whether these particles actually reach Earth, the Moon, Mars (or any other point) depends on their transport in the interplanetary magnetic field and their magnetic connection to the shock. Recent contemporaneous <span class="hlt">observations</span> during the largest events in almost a decade show the unique longitudinal distributions of this ionizing radiation broadly distributed from sources near the Sun and yet highly isolated during the passage of CME shocks. Over the last decade, we have <span class="hlt">observed</span> space weather events as the <span class="hlt">solar</span> wind exhibits extremely low densities and magnetic field strengths, representing states that have never been <span class="hlt">observed</span> during the space age. The highly abnormal <span class="hlt">solar</span> activity during cycles 23 and 24 has caused the longest <span class="hlt">solar</span> minimum in over 80 years and continues into the unusually small <span class="hlt">solar</span> maximum of cycle 24. As a result of the remarkably weak <span class="hlt">solar</span> activity, we have also <span class="hlt">observed</span> the highest fluxes of galactic cosmic rays in the space age and relatively small particle radiation events. We have used <span class="hlt">observations</span> from LRO/CRaTER to examine the implications of these highly unusual <span class="hlt">solar</span> conditions for human space exploration throughout the inner <span class="hlt">solar</span> <span class="hlt">system</span>. While these conditions are not a show-stopper for long-duration missions (e.g., to the Moon, an asteroid, or Mars), galactic cosmic ray radiation remains a significant and worsening factor that limits</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20180000549&hterms=Solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DSolar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20180000549&hterms=Solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DSolar"><span>Finding the Needles in the Haystacks: High-Fidelity Models of the Modern and Archean <span class="hlt">Solar</span> <span class="hlt">System</span> for Simulating Exoplanet <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>Roberge, Aki; Rizzo, Maxime J.; Lincowski, Andrew P.; Arney, Giada N.; Stark, Christopher C.; Robinson, Tyler D.; Snyder, Gregory F.; Pueyo, Laurent; Zimmerman, Neil T.; Jansen, Tiffany; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20180000549'); toggleEditAbsImage('author_20180000549_show'); toggleEditAbsImage('author_20180000549_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20180000549_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20180000549_hide"></p> <p>2017-01-01</p> <p>We present two state-of-the-art models of the <span class="hlt">solar</span> <span class="hlt">system</span>, one corresponding to the present day and one to the Archean Eon 3.5 billion years ago. Each model contains spatial and spectral information for the star, the planets, and the interplanetary dust, extending to 50 au from the Sun and covering the wavelength range 0.3-2.5 micron. In addition, we created a spectral image cube representative of the astronomical backgrounds that will be seen behind deep <span class="hlt">observations</span> of extrasolar planetary <span class="hlt">systems</span>, including galaxies and Milky Way stars. These models are intended as inputs to high-fidelity simulations of direct <span class="hlt">observations</span> of exoplanetary <span class="hlt">systems</span> using telescopes equipped with high-contrast capability. They will help improve the realism of <span class="hlt">observation</span> and instrument parameters that are required inputs to statistical observatory yield calculations, as well as guide development of post-processing algorithms for telescopes capable of directly imaging Earth-like planets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008cosp...37..458C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008cosp...37..458C"><span>The MEXART ips <span class="hlt">observations</span> in route to the next <span class="hlt">solar</span> maximum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carrillo-Vargas, Armando; Gonzalez-Esparza, Americo; Andrade, Ernesto; Perez-Enriquez, Roman; Aguilar-Rodriguez, Ernesto; Casillas-Perez, Gilberto; Jeyakumar, Solai; Kurtz, Stanley; Sierra, Pablo; Vazquez, Samuel</p> <p></p> <p>We report the status of the Mexican Array Radio Telescope (MEXART) in preparation for the next <span class="hlt">solar</span> maximum. During this epoch, the MEXART will be one of the four dedicated radio telescopes (with the ORT in India; STEL in Japan; and MWA in Australia) to track large-scale structures in the <span class="hlt">solar</span> wind using the interplanetary scintillation (IPS) technique. This network of IPS observatories would produce, for the first time four g maps of the sky showing the size and shape of disturbances between the Sun and the Earth. We describe the operation and current <span class="hlt">observations</span> of the first IPS radio sources at 140 MHz detected by the MEXART. These <span class="hlt">observations</span> use a plane dipole array of 1024 elements (16 lines with 64 dipoles each one), feeding a Butler matrix of 16x16 ports. This <span class="hlt">system</span> generates a 16 lobes at fixed declinations covering 120 degrees (from 40 degrees South to 80 degrees North). The beam fan uses the Earth's rotation to cover the whole sky. The <span class="hlt">observations</span> that will be made with the network of observatories of interplanetary flashing will complement the <span class="hlt">observations</span> of other observatories, instruments in situ, space probes, satellite, among others.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170008030','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170008030"><span><span class="hlt">Solar</span> Spectral Irradiance Variability in Cycle 24: Model Predictions and OMI <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>Marchenko, S.; DeLand, M.; Lean, J.</p> <p>2016-01-01</p> <p>Utilizing the excellent stability of the Ozone Monitoring Instrument (OMI), we characterize both short-term (<span class="hlt">solar</span> rotation) and long-term (<span class="hlt">solar</span> cycle) changes of the <span class="hlt">solar</span> spectral irradiance (SSI) between 265-500 nanometers during the ongoing Cycle 24. We supplement the OMI data with concurrent <span class="hlt">observations</span> from the GOME-2 (Global Ozone Monitoring Experiment - 2) and SORCE (<span class="hlt">Solar</span> Radiation and Climate Experiment) instruments and find fair-to-excellent agreement between the <span class="hlt">observations</span> and predictions of the NRLSSI2 (Naval Research Laboratory <span class="hlt">Solar</span> Spectral Irradiance - post SORCE) and SATIRE-S (the Naval Research Laboratory's Spectral And Total Irradiance REconstruction for the Satellite era) models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27194964','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27194964"><span><span class="hlt">Solar</span> Adaptive Optics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rimmele, Thomas R; Marino, Jose</p> <p></p> <p>Adaptive optics (AO) has become an indispensable tool at ground-based <span class="hlt">solar</span> telescopes. AO enables the ground-based <span class="hlt">observer</span> to overcome the adverse effects of atmospheric seeing and obtain diffraction limited <span class="hlt">observations</span>. Over the last decade adaptive optics <span class="hlt">systems</span> have been deployed at major ground-based <span class="hlt">solar</span> telescopes and revitalized ground-based <span class="hlt">solar</span> astronomy. The relatively small aperture of <span class="hlt">solar</span> telescopes and the bright source make <span class="hlt">solar</span> AO possible for visible wavelengths where the majority of <span class="hlt">solar</span> <span class="hlt">observations</span> are still performed. <span class="hlt">Solar</span> AO <span class="hlt">systems</span> enable diffraction limited <span class="hlt">observations</span> of the Sun for a significant fraction of the available <span class="hlt">observing</span> time at ground-based <span class="hlt">solar</span> telescopes, which often have a larger aperture than equivalent space based observatories, such as HINODE. New ground breaking scientific results have been achieved with <span class="hlt">solar</span> adaptive optics and this trend continues. New large aperture telescopes are currently being deployed or are under construction. With the aid of <span class="hlt">solar</span> AO these telescopes will obtain <span class="hlt">observations</span> of the highly structured and dynamic <span class="hlt">solar</span> atmosphere with unprecedented resolution. This paper reviews <span class="hlt">solar</span> adaptive optics techniques and summarizes the recent progress in the field of <span class="hlt">solar</span> adaptive optics. An outlook to future <span class="hlt">solar</span> AO developments, including a discussion of Multi-Conjugate AO (MCAO) and Ground-Layer AO (GLAO) will be given. Supplementary material is available for this article at 10.12942/lrsp-2011-2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996DPS....28.2504G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996DPS....28.2504G"><span>JPL's On-Line <span class="hlt">Solar</span> <span class="hlt">System</span> Data Service</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Giorgini, J. D.; Yeomans, D. K.; Chamberlin, A. B.; Chodas, P. W.; Jacobson, R. A.; Keesey, M. S.; Lieske, J. H.; Ostro, S. J.; Standish, E. M.; Wimberly, R. N.</p> <p>1996-09-01</p> <p>Numerous data products from the JPL ephemeris team are being made available via an interactive telnet computer service and separate web page. For over 15,000 comets and asteroids, 60 natural satellites, and 9 planets, users with an Internet connection can easily create and download information 24 hours a day, 7 days a week. These data include customized, high precision ephemerides, orbital and physical characteristics, and search-lists of comets and asteroids that match combinations of up to 39 different parameters. For each body, the user can request computation of more than 70 orbital and physical quantities. Ephemerides output can be generated in ICRF/J2000.0 and FK4/1950.0 reference frames with TDB, TT, or UTC timescales, as appropriate, at user specified intervals. Computed tables are derived from the same ephemerides used at JPL for radar astronomy and spacecraft navigation. The dynamics and computed <span class="hlt">observables</span> include relativistic effects. Available ephemeris time spans currently range from A.D. 1599-2200 for the planets to a few decades for the satellites, comets and asteroids. Information on the interference from sunlight and moonlight is available. As an example of a few of the features available, we note that a user could easily generate information on satellite and planetary magnitudes, illuminated fractions, and the planetographic longitudes and latitudes of their centers and sub-<span class="hlt">solar</span> points as seen from a particular observatory location on Earth. Satellite transits, occultations and eclipses are available as well. The resulting ASCII tables can be transferred to the user's host computer via e-mail, ftp, or kermit protocols. For those who have WWW access, the telnet <span class="hlt">solar</span> <span class="hlt">system</span> ephemeris service will be one feature of the JPL <span class="hlt">solar</span> <span class="hlt">system</span> web page. This page will provide up-to-date physical and orbital characteristics as well as current and predicted <span class="hlt">observing</span> opportunities for all <span class="hlt">solar</span> <span class="hlt">system</span> bodies. Close Earth approaches and radar <span class="hlt">observations</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED219649.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED219649.pdf"><span>Residential <span class="hlt">Solar</span> <span class="hlt">Systems</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>Fulkerson, Dan</p> <p></p> <p>This publication contains student and teacher instructional materials for a course in residential <span class="hlt">solar</span> <span class="hlt">systems</span>. The text is designed either as a basic <span class="hlt">solar</span> course or as a supplement to extend student skills in areas such as architectural drafting, air conditioning and refrigeration, and plumbing. The materials are presented in four units…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AdSpR..60.1585S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AdSpR..60.1585S"><span>Ionospheric winter anomaly and annual anomaly <span class="hlt">observed</span> from Formosat-3/COSMIC Radio Occultation <span class="hlt">observations</span> during the ascending phase of <span class="hlt">solar</span> cycle 24</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sai Gowtam, V.; Tulasi Ram, S.</p> <p>2017-10-01</p> <p>Ionospheric winter and annual anomalies have been investigated during the ascending phase of <span class="hlt">solar</span> cycle 24 using high-resolution global 3D - data of the FORMOSAT - 3/COSMIC (Formosa satellite - 3/Constellation <span class="hlt">Observing</span> <span class="hlt">System</span> for Meterology, Ionosphere and Climate) radio occultation <span class="hlt">observations</span>. Our detailed analysis shows that the occurrence of winter anomaly at low-latitudes is confined only to the early morning to afternoon hours, whereas, the winter anomaly at mid-latitudes is almost absent at all local times during the ascending phase of <span class="hlt">solar</span> cycle 24. Further, in the topside ionosphere (altitudes of 400 km and above), the winter anomaly is completely absent at all local times. In contrast, the ionospheric annual anomaly is consistently <span class="hlt">observed</span> at all local times and altitudes during this ascending phase of <span class="hlt">solar</span> cycle 24. The annual anomaly exhibits strong enhancements over southern EIA crest latitudes during day time and around Weddle Sea Anomaly (WSA) region during night times. The global mean annual asymmetry index is also computed to understand the altitudinal variation. The global mean AI maximizes around 300-500 km altitudes during the low <span class="hlt">solar</span> active periods (2008-10), whereas it extends up to 600 km during moderate to high (2011) <span class="hlt">solar</span> activity period. These findings from our study provide new insights to the current understanding of the annual anomaly.</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('http://hdl.handle.net/2060/20070014672','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070014672"><span>NASA's <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Program</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Robinson, James</p> <p>2005-01-01</p> <p>A viewgraph presentation describing NASA's <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Program is shown. The topics include: 1) <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration with Highlights and Status of Programs; 2) Technology Drivers and Plans; and 3) Summary</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170010276','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170010276"><span>Organics and Ices in the Outer <span class="hlt">Solar</span> <span class="hlt">System</span>: Connections to the Interstellar Medium</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pendleton, Y. J.; Cruikshank, D. P.</p> <p>2017-01-01</p> <p>The <span class="hlt">solar</span> nebula, that aggregate of gas and dust that formed the birthplace of the Sun, planets and plethora of small bodies comprising the <span class="hlt">Solar</span> <span class="hlt">System</span>, originated in a molecular cloud that is thought to have spawned numerous additional stars, some with their own planets and attendant small bodies. The question of the chemical and physical reprocessing of the original interstellar materials in the <span class="hlt">solar</span> nebula has challenged both theory and <span class="hlt">observations</span>. The acquisition and analysis of samples of comet and asteroid solids, and a growing suite of in-situ and close-up analyses of relatively unaltered small <span class="hlt">Solar</span> <span class="hlt">System</span> bodies now adds critical new dimensions to the study of the origin and evolution of the early <span class="hlt">solar</span> nebula. Better understanding the original composition of the material from which our <span class="hlt">solar</span> nebula formed, and the processing that material experienced, will aid in formulations of chemistry that might occur in other <span class="hlt">solar</span> <span class="hlt">systems</span>. While we seek to understand the compositional history of planetary bodies in our own <span class="hlt">Solar</span> <span class="hlt">System</span>, we will inevitably learn more about the materials that comprise exoplanets and their surrounding <span class="hlt">systems</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH14B..03M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH14B..03M"><span>Do In Situ <span class="hlt">Observations</span> Contain Signatures of Intermittent Fast <span class="hlt">Solar</span> Wind Acceleration?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matteini, L.; Horbury, T. S.; Stansby, D.</p> <p>2017-12-01</p> <p>Disentangling local plasma properties and <span class="hlt">Solar</span> origin structures in in situ data is a crucial aspect for the understanding of <span class="hlt">solar</span> wind acceleration and evolution. This is particularly challenging at 1 AU and beyond, where structures of various origin have had time to interact and merge, smoothing out their main characteristics. <span class="hlt">Observations</span> of more pristine plasma closer to the Sun are therefore needed. In preparation of the forthcoming <span class="hlt">Solar</span> Orbiter and Parker <span class="hlt">Solar</span> Probe missions, Helios <span class="hlt">observations</span> as close as to 0.3 AU - although old, not yet fully exploited - can be used to test our expectations and make new predictions. Recent <span class="hlt">observations</span> (Matteini et al. 2014, 2015) have outlined the presence of intense (up to 1000km/s) and short-living velocity peaks that ubiquitously characterize the typical profile of the fast <span class="hlt">solar</span> wind at 0.3 AU, suggesting that these features could be remnants of processes occurring in the <span class="hlt">Solar</span> atmosphere and a signature of intermittent <span class="hlt">solar</span> wind acceleration from coronal holes. We discuss results about statistics of these events, characterizing their physical properties and trying to link them with typical <span class="hlt">Solar</span> temporal and spatial scales. Finally we also discuss how these velocity peaks will likely affect the future in situ exploration of the inner heliosphere by <span class="hlt">Solar</span> Orbiter and the Parker <span class="hlt">Solar</span> Probe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1174434','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1174434"><span>Adaptive, full-spectrum <span class="hlt">solar</span> energy <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Muhs, Jeffrey D.; Earl, Dennis D.</p> <p>2003-08-05</p> <p>An adaptive full spectrum <span class="hlt">solar</span> energy <span class="hlt">system</span> having at least one hybrid <span class="hlt">solar</span> concentrator, at least one hybrid luminaire, at least one hybrid photobioreactor, and a light distribution <span class="hlt">system</span> operably connected to each hybrid <span class="hlt">solar</span> concentrator, each hybrid luminaire, and each hybrid photobioreactor. A lighting control <span class="hlt">system</span> operates each component.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013MS%26E...53a2005A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013MS%26E...53a2005A"><span>Development of <span class="hlt">Solar</span> Powered Irrigation <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abdelkerim, A. I.; Sami Eusuf, M. M. R.; Salami, M. J. E.; Aibinu, A.; Eusuf, M. A.</p> <p>2013-12-01</p> <p>Development of a <span class="hlt">solar</span> powered irrigation <span class="hlt">system</span> has been discussed in this paper. This <span class="hlt">system</span> would be SCADA-based and quite useful in areas where there is plenty of sunshine but insufficient water to carry out farming activities, such as rubber plantation, strawberry plantation, or any plantation, that requires frequent watering. The <span class="hlt">system</span> is powered by <span class="hlt">solar</span> <span class="hlt">system</span> as a renewable energy which uses <span class="hlt">solar</span> panel module to convert Sunlight into electricity. The development and implementation of an automated SCADA controlled <span class="hlt">system</span> that uses PLC as a controller is significant to agricultural, oil and gas monitoring and control purpose purposes. In addition, the <span class="hlt">system</span> is powered by an intelligent <span class="hlt">solar</span> <span class="hlt">system</span> in which <span class="hlt">solar</span> panel targets the radiation from the Sun. Other than that, the <span class="hlt">solar</span> <span class="hlt">system</span> has reduced energy cost as well as pollution. The <span class="hlt">system</span> is equipped with four input sensors; two soil moisture sensors, two level detection sensors. Soil moisture sensor measures the humidity of the soil, whereas the level detection sensors detect the level of water in the tank. The output sides consist of two solenoid valves, which are controlled respectively by two moistures sensors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27386512','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27386512"><span>Inner <span class="hlt">solar</span> <span class="hlt">system</span> material discovered in the Oort cloud.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Meech, Karen J; Yang, Bin; Kleyna, Jan; Hainaut, Olivier R; Berdyugina, Svetlana; Keane, Jacqueline V; Micheli, Marco; Morbidelli, Alessandro; Wainscoat, Richard J</p> <p>2016-04-01</p> <p>We have <span class="hlt">observed</span> C/2014 S3 (PANSTARRS), a recently discovered object on a cometary orbit coming from the Oort cloud that is physically similar to an inner main belt rocky S-type asteroid. Recent dynamical models successfully reproduce the key characteristics of our current <span class="hlt">solar</span> <span class="hlt">system</span>; some of these models require significant migration of the giant planets, whereas others do not. These models provide different predictions on the presence of rocky material expelled from the inner <span class="hlt">solar</span> <span class="hlt">system</span> in the Oort cloud. C/2014 S3 could be the key to verifying these predictions of the migration-based dynamical models. Furthermore, this object displays a very faint, weak level of comet-like activity, five to six orders of magnitude less than that of typical ice-rich comets on similar Orbits coming from the Oort cloud. For the nearly tailless appearance, we are calling C/2014 S3 a Manx object. Various arguments convince us that this activity is produced by sublimation of volatile ice, that is, normal cometary activity. The activity implies that C/2014 S3 has retained a tiny fraction of the water that is expected to be present at its formation distance in the inner <span class="hlt">solar</span> <span class="hlt">system</span>. We may be looking at fresh inner <span class="hlt">solar</span> <span class="hlt">system</span> Earth-forming material that was ejected from the inner <span class="hlt">solar</span> <span class="hlt">system</span> and preserved for billions of years in the Oort cloud.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000053505','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000053505"><span>Mission to the <span class="hlt">Solar</span> <span class="hlt">System</span>: Exploration and Discovery. A Mission and Technology Roadmap</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gulkis, S. (Editor); Stetson, D. S. (Editor); Stofan, E. R. (Editor)</p> <p>1998-01-01</p> <p><span class="hlt">Solar</span> <span class="hlt">System</span> exploration addresses some of humanity's most fundamental questions: How and when did life form on Earth? Does life exist elsewhere in the <span class="hlt">Solar</span> <span class="hlt">System</span> or in the Universe? - How did the <span class="hlt">Solar</span> <span class="hlt">System</span> form and evolve in time? - What can the other planets teach us about the Earth? This document describes a Mission and Technology Roadmap for addressing these and other fundamental <span class="hlt">Solar</span> <span class="hlt">System</span> Questions. A Roadmap Development Team of scientists, engineers, educators, and technologists worked to define the next evolutionary steps in in situ exploration, sample return, and completion of the overall <span class="hlt">Solar</span> <span class="hlt">System</span> survey. Guidelines were to "develop aa visionary, but affordable, mission and technology development Roadmap for the exploration of the <span class="hlt">Solar</span> <span class="hlt">System</span> in the 2000 to 2012 timeframe." The Roadmap provides a catalog of potential flight missions. (Supporting research and technology, ground-based <span class="hlt">observations</span>, and laboratory research, which are no less important than flight missions, are not included in this Roadmap.)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850025584','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850025584"><span>Simultaneous <span class="hlt">Solar</span> Maximum Mission and Very Large Array (VLA) <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lang, K. R.</p> <p>1985-01-01</p> <p>Simultaneous <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions with the <span class="hlt">Solar</span> Maximum Mission (SMM) Satellite and the Very Large Array (VLA) have been obtained and analyzed. Combined results enhance the scientific return for beyond that expeted from using either SMM or VLA alone. A total of two weeks of simultaneous SMM/VLA data were obtained. The multiple wavelength VLA <span class="hlt">observations</span> were used to determine the temperature and magnetic structure at different heights within coronal loops. These data are compared with simultaneous SMM <span class="hlt">observations</span>. Several papers on the subject are in progress. They include VLA <span class="hlt">observations</span> of compact, transient sources in the transition region; simultaneous SMM/VLA <span class="hlt">observations</span> of the coronal loops in one active region and the evolution of another one; and sampling of the coronal plasma using thermal cyclotron lines (magnetic field - VLA) and soft X ray spectral lines (electron density and electron temperaure-SMM).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930009356','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930009356"><span>Exobiology in <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Carle, Glenn C. (Editor); Schwartz, Deborah E. (Editor); Huntington, Judith L. (Editor)</p> <p>1992-01-01</p> <p>A symposium, 'Exobiology in <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration,' was held on 24-26 Aug. 1988. The symposium provided an in-depth investigation of the role of Exobiology in <span class="hlt">solar</span> <span class="hlt">system</span> exploration. It is expected that the symposium will provide direction for future participation of the Exobiology community in <span class="hlt">solar</span> <span class="hlt">system</span> exploration and alert the Planetary community to the continued importance of an Exobiology Flight Program. Although the focus of the symposium was primarily on Exobiology in <span class="hlt">solar</span> <span class="hlt">system</span> exploration missions, several ground based and Earth-orbital projects such as the Search for Extraterrestrial Intelligence, Gas Grain Facility, and Cosmic Dust Collection Facility represent upcoming research opportunities planned to accommodate the goals and objectives of the Exobiology community as well. This report contains papers for all but one of the presentations given at the symposium.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870003089','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870003089"><span>Simultaneous <span class="hlt">Solar</span> Maximum Mission (SMM) and very large array <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lang, K. R.</p> <p>1986-01-01</p> <p>The research deals mainly with Very Large Array and <span class="hlt">Solar</span> Maximum Mission <span class="hlt">observations</span> of the ubiquitous coronal loops that dominate the structure of the low corona. As illustrated, the <span class="hlt">observations</span> of thermal cyclotron lines at microwave wavelengths provide a powerful new method of accurately specifying the coronal magnetic field strength. Processes are delineated that trigger <span class="hlt">solar</span> eruptions from coronal loops, including preburst heating and the magnetic interaction of coronal loops. Evidence for coherent burst mechanisms is provided for both the Sun and nearby stars, while other <span class="hlt">observations</span> suggest the presence of currents that may amplify the coronal magnetic field to unexpectedly high levels. The existence is reported of a new class of compact, variable moving sources in regions of apparently weak photospheric field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110008004','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110008004"><span>The <span class="hlt">Solar</span> Dynamics Observatory, Studying the Sun and Its Influence on Other Bodies in the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chamberlin, P. C.</p> <p>2011-01-01</p> <p>The <span class="hlt">solar</span> photon output, which was once thought to be constant, varies over all time scales from seconds during <span class="hlt">solar</span> flares to years due to the <span class="hlt">solar</span> cycle. These <span class="hlt">solar</span> variations cause significant deviations in the Earth and space environments on similar time scales, such as affecting the atmospheric densities and composition of particular atoms, molecules, and ions in the atmospheres of the Earth and other planets. Presented and discussed will be examples of unprecedented <span class="hlt">observations</span> from NASA's new <span class="hlt">solar</span> observatory, the <span class="hlt">Solar</span> Dynamics Observatory (SDO). Using three specialized instruments, SDO measures the origins of <span class="hlt">solar</span> activity from inside the Sun, though its atmosphere, then accurately measuring the Sun's radiative output in X-ray and EUV wavelengths (0.1-121 nm). Along with the visually appealing <span class="hlt">observations</span> will be discussions of what these measurements can tell us about how the plasma motions in all layers of the Sun modifies and strengthens the weak <span class="hlt">solar</span> dipole magnetic field to drive large energy releases in <span class="hlt">solar</span> eruptions. Also presented will be examples of how the release of the Sun's energy, in the form of photons and high energy particles, physically influence other bodies in the <span class="hlt">solar</span> <span class="hlt">system</span> such as Earth, Mars, and the Moon, and how these changes drive changes in the technology that we are becoming dependent upon. The presentation will continuously emphasize how SDO, the first satellite in NASA's Living with a Star program, improving our understanding of the variable Sun and its Heliospheric influence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020069138&hterms=firenze&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dfirenze','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020069138&hterms=firenze&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dfirenze"><span><span class="hlt">Solar</span> Wind Characteristics from SOHO-Sun-Ulysses Quadrature <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>Poletto, Giannina; Suess, Steve T.; Six, N. Frank (Technical Monitor)</p> <p>2002-01-01</p> <p>Over the past few years, we have been running SOHO (<span class="hlt">Solar</span> and Heliospheric Observatory)-Sun-Ulysses quadrature campaigns, aimed at comparing the plasma properties at coronal altitudes with plasma properties at interplanetary distances. Coronal plasma has been <span class="hlt">observed</span> by SOHO experiments: mainly, we used LASCO (Large Angle and Spectrometric Coronagraph Experiment) data to understand the overall coronal configuration at the time of quadratures and analyzed SUMER (<span class="hlt">Solar</span> Ultraviolet Measurements of Emitted Radiation), CDS (Coronal Diagnostic Spectrometer) and UVCS (Ultraviolet Coronagraph Spectrometer) data to derive its physical characteristics. At interplanetary distances, SWICS (<span class="hlt">Solar</span> Wind Ion Composition Spectrometer) and SWOOPS (<span class="hlt">Solar</span> Wind <span class="hlt">Observation</span> over the Poles of the Sun) aboard Ulysses provided us with interplanetary plasma data. Here we report on results from some of the campaigns. We notice that, depending on the geometry of the quadrature, i.e. on whether the radial to Ulysses traverses the corona at high or low latitudes, we are able to study different kinds of <span class="hlt">solar</span> wind. In particular, a comparison between low-latitude and high-latitude wind, allowed us to provide evidence for differences in the acceleration of polar, fast plasma and equatorial, slow plasma: the latter occurring at higher levels and through a more extended region than fast wind. These properties are shared by both the proton and heavy ions outflows. Quadrature <span class="hlt">observations</span> may provide useful information also on coronal vs. in situ elemental composition. To this end, we analyzed spectra taken in the corona, at altitudes ranging between approx. 1.02 and 2.2 <span class="hlt">solar</span> radii, and derived the abundances of a number of ions, including oxygen and iron. Values of the O/Fe ratio, at coronal levels, have been compared with measurements of this ratio made by SWICS at interplanetary distances. Our results are compared with previous findings and predictions from modeling efforts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ASPC..463..439S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ASPC..463..439S"><span>Instrument Design of the Large Aperture <span class="hlt">Solar</span> UV Visible and IR <span class="hlt">Observing</span> Telescope (SUVIT) for the <span class="hlt">SOLAR</span>-C Mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suematsu, Y.; Katsukawa, Y.; Shimizu, T.; Ichimoto, K.; Takeyama, N.</p> <p>2012-12-01</p> <p>We present an instrumental design of one major <span class="hlt">solar</span> <span class="hlt">observation</span> payload planned for the <span class="hlt">SOLAR</span>-C mission: the <span class="hlt">Solar</span> Ultra-violet Visible and near IR <span class="hlt">observing</span> Telescope (SUVIT). The SUVIT is designed to provide high-angular-resolution investigation of the lower <span class="hlt">solar</span> atmosphere, from the photosphere to the uppermost chromosphere, with enhanced spectroscopic and spectro-polarimetric capability in wide wavelength regions from 280 nm (Mg II h&k lines) to 1100 nm (He I 1083 nm line) with 1.5 m class aperture and filtergraphic and spectrographic instruments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ASPC..504..331M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ASPC..504..331M"><span><span class="hlt">Solar</span> Radio <span class="hlt">Observation</span> using Callisto Spectrometer at Sumedang West Java Indonesia: Current Status and Future Development Plan in Indonesia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Manik, T.; Sitompul, P.; Batubara, M.; Harjana, T.; Yatini, C. Y.; Monstein, C.</p> <p>2016-04-01</p> <p>Sumedang Observatory (6.91°S, 107,84°E) was established in 1975 and is one of the <span class="hlt">solar</span> <span class="hlt">observation</span> facilities of the Space Science Center of Indonesian National Institute of Aeronautics and Space (LAPAN), located around 40 km, east part of Bandung City, West Java, Indonesia. Several instrumentations for <span class="hlt">solar</span> and space <span class="hlt">observation</span> such as optical telescopes, radio <span class="hlt">solar</span> spectrograph, flux gate magnetometer, etc. are operated there, together with an ionosphere sounding <span class="hlt">system</span> (ionosonde) that was set up later. In July 2014, a standard Callisto (Compound Astronomical Low-cost Low-frequency Instrument for Spectroscopy and Transportable Observatory) spectrometer was installed at Sumedang Observatory for <span class="hlt">solar</span> radio activity monitoring. Callisto has been developed in the framework of IHY2007 and ISWI, supported by UN and NASA. Callisto spectrometer has <span class="hlt">observation</span> capability in the frequency range of 45-870 MHz. The Callisto spectrometer receives signal by using a set of 21 elements log-periodic antenna, model CLP5130-1N, pointed to the Sun and equipped with a low noise pre-amplifier. With respect to the Radio Frequency Interferences (RFI) measurements, the Callisto spectrometer is operated individually in frequency ranges of 45-80 MHz and 180-450 MHz. <span class="hlt">Observation</span> status and data flow are monitored in on-line from center office located in Bandung. The data was transferred to central database at FHNW (Fachhochschule Nordwestschweiz) server every 15 minutes to appear on e-Callisto network subsequently. A real time data transfer and data processing based on Python software also has been developed successfully to be used as an input for Space Weather Information and Forecasting Services (SWIFtS) provided by LAPAN. On 5th November 2014, Callisto spectrometer at Sumedang <span class="hlt">observed</span> the first clear <span class="hlt">solar</span> radio event, a <span class="hlt">solar</span> radio burst type II corresponding to a coronal mass ejection (CME), indicated by a strong X-ray event of M7.9 that was informed on by Space Weather</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013cctp.book..539H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013cctp.book..539H"><span><span class="hlt">Solar</span> Irradiance Variability and Its Impacts on the Earth Climate <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harder, J. W.; Woods, T. N.</p> <p></p> <p>The Sun plays a vital role in the evolution of the climates of terrestrial planets. <span class="hlt">Observations</span> of the <span class="hlt">solar</span> spectrum are now routinely made that span the wavelength range from the X-ray portion of the spectrum (5 nm) into the infrared to about 2400 nm. Over this very broad wavelength range, accounting for about 97% of the total <span class="hlt">solar</span> irradiance, the intensity varies by more than 6 orders of magnitude, requiring a suite of very different and innovative instruments to determine both the spectral irradiance and its variability. The origins of <span class="hlt">solar</span> variability are strongly linked to surface magnetic field changes, and analysis of <span class="hlt">solar</span> images and magnetograms show that the intensity of emitted radiation from <span class="hlt">solar</span> surface features in active regions has a very strong wavelength and magnetic field strength dependence. These magnetic fields produce <span class="hlt">observable</span> <span class="hlt">solar</span> surface features such as sunspots, faculae, and network structures that contribute in different ways to the radiated output. Semi-empirical models of <span class="hlt">solar</span> spectral irradiance are able to capture much of the Sun's output, but this topic remains an active area of research. Studies of <span class="hlt">solar</span> structures in both high spectral and spatial resolution are refining this understanding. Advances in Earth <span class="hlt">observation</span> <span class="hlt">systems</span> and high-quality three-dimensional chemical climate models provide a sound methodology to study the mechanisms of the interaction between Earth's atmosphere and the incoming <span class="hlt">solar</span> radiation. Energetic photons have a profound effect on the chemistry and dynamics of the thermosphere and ionosphere, and these processes are now well represented in upper atmospheric models. In the middle and lower atmosphere the effects of <span class="hlt">solar</span> variability enter the climate <span class="hlt">system</span> through two nonexclusive pathways referred to as the top-down and bottom-up mechanisms. The top-down mechanism proceeds through the alteration of the photochemical rates that establish the middle atmospheric temperature structure and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AstHe..95..179T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AstHe..95..179T"><span><span class="hlt">Observation</span> of the total <span class="hlt">solar</span> eclipse on 21 June 2001 in Zambia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takahashi, Noritsugu; Yumoto, Kiyohumi; Ichimoto, Kiyoshi</p> <p>2002-04-01</p> <p>On 21 June 2001, path of totality in Angola, Zambia, Zimbabwe, Mozambique, and Madagascar in Africa. The Japan Scientific <span class="hlt">Observation</span> Team, consisting primarily of the members of the <span class="hlt">Solar</span> Eclipse Subcommittee of the Committee for International Collaboration in Astronomy of the Science Council of JAPAN, visited Lusaka in Zambia to <span class="hlt">observe</span> the total <span class="hlt">solar</span> eclipse. Blessed with fine weather, the <span class="hlt">observation</span> was successful. The outline of the influence of <span class="hlt">solar</span> eclipse on the terrestrial magnetism, polarization of the flash spectrum, and other <span class="hlt">observation</span> data, as well as the way educational activities were carried out, are reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3228481','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3228481"><span>Cosmochemical evidence for astrophysical processes during the formation of our <span class="hlt">solar</span> <span class="hlt">system</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>MacPherson, Glenn J.; Boss, Alan</p> <p>2011-01-01</p> <p>Through the laboratory study of ancient <span class="hlt">solar</span> <span class="hlt">system</span> materials such as meteorites and comet dust, we can recognize evidence for the same star-formation processes in our own <span class="hlt">solar</span> <span class="hlt">system</span> as those that we can <span class="hlt">observe</span> now through telescopes in nearby star-forming regions. High temperature grains formed in the innermost region of the <span class="hlt">solar</span> <span class="hlt">system</span> ended up much farther out in the <span class="hlt">solar</span> <span class="hlt">system</span>, not only the asteroid belt but even in the comet accretion region, suggesting a huge and efficient process of mass transport. Bi-polar outflows, turbulent diffusion, and marginal gravitational instability are the likely mechanisms for this transport. The presence of short-lived radionuclides in the early <span class="hlt">solar</span> <span class="hlt">system</span>, especially 60Fe, 26Al, and 41Ca, requires a nearby supernova shortly before our <span class="hlt">solar</span> <span class="hlt">system</span> was formed, suggesting that the Sun was formed in a massive star-forming region similar to Orion or Carina. <span class="hlt">Solar</span> <span class="hlt">system</span> formation may have been “triggered” by ionizing radiation originating from massive O and B stars at the center of an expanding HII bubble, one of which may have later provided the supernova source for the short-lived radionuclides. Alternatively, a supernova shock wave may have simultaneously triggered the collapse and injected the short-lived radionuclides. Because the Sun formed in a region where many other stars were forming more or less contemporaneously, the bi-polar outflows from all such stars enriched the local region in interstellar silicate and oxide dust. This may explain several <span class="hlt">observed</span> anomalies in the meteorite record: a near absence of detectable (no extreme isotopic properties) presolar silicate grains and a dichotomy in the isotope record between 26Al and nucleosynthetic (nonradiogenic) anomalies. PMID:22106251</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890006492','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890006492"><span>Millimeter wavelength <span class="hlt">observations</span> of <span class="hlt">solar</span> flares for Max 1991</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kundu, M. R.; Gopalswamy, N.; Nitta, N.; Schmahl, E. J.; White, S. M.; Welch, W. J.</p> <p>1988-01-01</p> <p>The Hat Creek millimeter-wave interferometer (to be known as the Berkeley-Illinois-Maryland Array, BIMA) is being upgraded. The improved array will become available during the coming <span class="hlt">solar</span> maximum, and will have guaranteed time for <span class="hlt">solar</span> <span class="hlt">observing</span>. The Hat Creek millimeter-wave interferometer is described along with the improvements. The scientific objectives are briefly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH13B2477B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH13B2477B"><span>Polarization <span class="hlt">Observations</span> of the Total <span class="hlt">Solar</span> Eclipse of August 21, 2017</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burkepile, J.; Boll, A.; Casini, R.; de Toma, G.; Elmore, D. F.; Gibson, K. L.; Judge, P. G.; Mitchell, A. M.; Penn, M.; Sewell, S. D.; Tomczyk, S.; Yanamandra-Fisher, P. A.</p> <p>2017-12-01</p> <p>A total <span class="hlt">solar</span> eclipse offers ideal sky conditions for viewing the <span class="hlt">solar</span> corona. Light from the corona is composed of three components: the E-corona, made up of spectral emission lines produced by ionized elements in the corona; the K-corona, produced by photospheric light that is Thomson scattered by coronal electrons; and the F-corona, produced by sunlight scattered from dust particles in the near Sun environment and in interplanetary space. Polarized white light <span class="hlt">observations</span> of the corona provide a way of isolating the K-corona to determine its structure, brightness, and density. This work focuses on broadband white light polarization <span class="hlt">observations</span> of the corona during the upcoming <span class="hlt">solar</span> eclipse from three different instruments. We compare coronal polarization brightness <span class="hlt">observations</span> of the August 21, 2017 total <span class="hlt">solar</span> eclipse from the NCAR/High Altitude Observatory (HAO) Rosetta Stone experiment using the 4-D Technology PolarCam camera with the two Citizen PACA_CATE17Pol telescopes that will acquire linear polarization <span class="hlt">observations</span> of the eclipse and the NCAR/HAO K-Cor white light coronagraph <span class="hlt">observations</span> from the Mauna Loa <span class="hlt">Solar</span> Observatory in Hawaii. This comparison includes a discussion of the cross-calibration of the different instruments and reports the results of the coronal polarization brightness and electron density of the corona. These <span class="hlt">observations</span> will be compared with results from previous coronal measurements taken at different phases of the <span class="hlt">solar</span> cycle. In addition, we report on the performance of the three different polarimeters. The 4-D PolarCam uses a linear polarizer array, PACA_CATE17Pol uses a nematic liquid crystal retarder in a single beam configuration and K-Cor uses a pair of ferroelectric liquid crystal retarders in a dual-beam configuration. The use of the 4-D PolarCam camera in the Rosetta Stone experiment is to demonstrate the technology for acquiring high cadence polarization measurements. The Rosetta Stone experiment is funded through</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1982pvsp.conf.1172M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1982pvsp.conf.1172M"><span>Grid-connected distributed <span class="hlt">solar</span> power <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moyle, R.; Chernoff, H.; Schweizer, T.</p> <p></p> <p>This paper discusses some important, though often ignored, technical and economic issues of distributed <span class="hlt">solar</span> power <span class="hlt">systems</span>: protection of the utility <span class="hlt">system</span> and nonsolar customers requires suitable interfaced equipment. Purchase criteria must mirror reality; most analyses use life-cycle costing with low discount rates - most buyers use short payback periods. Distributing, installing, and marketing small, distributed <span class="hlt">solar</span> <span class="hlt">systems</span> is more costly than most analyses estimate. Results show that certain local conditions and uncommon purchase considerations can combine to make small, distributed <span class="hlt">solar</span> power attractive, but lower interconnect costs (per kW), lower marketing and product distribution costs, and more favorable purchase criteria make large, centralized <span class="hlt">solar</span> energy more attractive. Specifically, the value of dispersed <span class="hlt">solar</span> <span class="hlt">systems</span> to investors and utilities can be higher than $2000/kw. However, typical residential owners place a value of well under $1000 on the installed <span class="hlt">system</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_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('https://www.osti.gov/biblio/21452817-measuring-mass-solar-system-planets-using-pulsar-timing','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21452817-measuring-mass-solar-system-planets-using-pulsar-timing"><span>MEASURING THE MASS OF <span class="hlt">SOLAR</span> <span class="hlt">SYSTEM</span> PLANETS USING PULSAR TIMING</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>Champion, D. J.; Hobbs, G. B.; Manchester, R. N.</p> <p></p> <p>High-precision pulsar timing relies on a <span class="hlt">solar</span> <span class="hlt">system</span> ephemeris in order to convert times of arrival (TOAs) of pulses measured at an observatory to the <span class="hlt">solar</span> <span class="hlt">system</span> barycenter. Any error in the conversion to the barycentric TOAs leads to a systematic variation in the <span class="hlt">observed</span> timing residuals; specifically, an incorrect planetary mass leads to a predominantly sinusoidal variation having a period and phase associated with the planet's orbital motion about the Sun. By using an array of pulsars (PSRs J0437-4715, J1744-1134, J1857+0943, J1909-3744), the masses of the planetary <span class="hlt">systems</span> from Mercury to Saturn have been determined. These masses are consistentmore » with the best-known masses determined by spacecraft <span class="hlt">observations</span>, with the mass of the Jovian <span class="hlt">system</span>, 9.547921(2) x10{sup -4} M {sub sun}, being significantly more accurate than the mass determined from the Pioneer and Voyager spacecraft, and consistent with but less accurate than the value from the Galileo spacecraft. While spacecraft are likely to produce the most accurate measurements for individual <span class="hlt">solar</span> <span class="hlt">system</span> bodies, the pulsar technique is sensitive to planetary <span class="hlt">system</span> masses and has the potential to provide the most accurate values of these masses for some planets.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860022990&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DSMM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860022990&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DSMM"><span><span class="hlt">Observations</span> of Halley's Comet by the <span class="hlt">Solar</span> Maximum Mission (SMM)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Niedner, M. B.</p> <p>1986-01-01</p> <p><span class="hlt">Solar</span> Maximum Mission coronagraph/polarimeter <span class="hlt">observations</span> of large scale phenomena in Halley's Comet are discussed. <span class="hlt">Observations</span> of the hydrogen coma with the UV spectrometer are considered. It is concluded that coronograph/polarimeter <span class="hlt">observations</span> of the disconnection event, in which the entire plasma tail uproots itself from the head of the comet, is convected away in the <span class="hlt">solar</span> wind at speeds in the 50 to 100 km/sec range (relative to the head), and is replaced by a plasma tail constructed from folding ion-tail rays, are the most interesting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998DPS....30.2601E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998DPS....30.2601E"><span><span class="hlt">Observation</span> of <span class="hlt">solar-system</span> objects with the ISO satellite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Encrenaz, Therese</p> <p>1998-09-01</p> <p>The ISO (Infrared Space Observatory) mission was an ESA earth-orbiting satellite devoted to the infrared <span class="hlt">observation</span> of astronomical sources. The 60-cm helium-cooled telescope was launched in November 1995 and ended its life in May 1998. The satellite was equipped with 4 focal-plane instruments: a camera (CAM, 2.5-17 microns), a photometer (PHT, 2-200 microns) and two spectrometers, SWS (2.3-45 microns) and LWS (45-180 microns). A description of the ISO mission can be found in Kessler et al.(A&A 315 L27, 1996). <span class="hlt">Observations</span> with ISO have been performed on all classes of <span class="hlt">solar-system</span> objects. Several important discoveries have been obtained from the ISO data, in particular with the SWS instrument. A few of them are listed below: (1) a new determination of D/H on the four giant planets; (2) the discovery of an external source of water in the stratospheres of the giant planets and Titan; (3) the detection of CO_2 in the stratospheres of Jupiter, Saturn and Neptune; (4) the detection of new hydrocarbons (CH_3C_2H, C_4H_2, C_6H_6, CH_3) in Saturn's stratosphere; (5) the detection of tropospheric water in Saturn; (6) the detection of CO_2 in comet Hale-Bopp at far heliocentric distances (4.6 AU); (7) the first detection of forsterite (Mg_2SiO_4) in the dust of comet Hale-Bopp; (7) the determination of the formation temperature of comets Hale-Bopp and Hartley 2 (27 K and 35 K respectively) from the measurement of the ortho-para ratio in their H_2O nu _3 emission lines. In addition, ISO spectra of Titan, Io and the other galilean satellites, and asteroids were also recorded; IR photometry was achieved on Pluto, distant comets and zodiacal light. Preliminary results can be found in Crovisier et al. (A&A 315 L385, 1996; Science 275 1904, 1996), Encrenaz et al. (A&A 315 L397, 1996; A&A 333 L43, 1998), de Graauw et al. (A&A 321 L13, 1997), Feuchtgruber et al. (Nature 389 159, 1997), Griffin et al. (A&A 315 L389, 1996), Davis et al. (A&A 315 L393, 1996), Reach et al. (A&A 315 L</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/909656','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/909656"><span>Hybrid <span class="hlt">solar</span> lighting <span class="hlt">systems</span> and components</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Muhs, Jeffrey D [Lenoir City, TN; Earl, Dennis D [Knoxville, TN; Beshears, David L [Knoxville, TN; Maxey, Lonnie C [Powell, TN; Jordan, John K [Oak Ridge, TN; Lind, Randall F [Lenoir City, TN</p> <p>2007-06-12</p> <p>A hybrid <span class="hlt">solar</span> lighting <span class="hlt">system</span> and components having at least one hybrid <span class="hlt">solar</span> concentrator, at least one fiber receiver, at least one hybrid luminaire, and a light distribution <span class="hlt">system</span> operably connected to each hybrid <span class="hlt">solar</span> concentrator and each hybrid luminaire. A controller operates each component.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010119917&hterms=hydrate&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dhydrate','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010119917&hterms=hydrate&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dhydrate"><span>Physical State of Ices in the Outer <span class="hlt">Solar</span> <span class="hlt">System</span>. Revised</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Roush, Ted L.; DeVincenzi, Donald (Technical Monitor)</p> <p>2001-01-01</p> <p>Comparison of the identity and abundances of ices <span class="hlt">observed</span> around protostars and those associated with comets clearly suggests that comets preserve the heritage of the interstellar materials that aggregated to form them. However, the ability to identify these same species on icy satellites in the outer <span class="hlt">solar</span> <span class="hlt">system</span> is a complex function of the composition of the original ices, their subsequent thermal histories, and their exposure to various radiation environments. Our ability to identify the ices currently present on objects in the outer <span class="hlt">solar</span> <span class="hlt">system</span> relies upon <span class="hlt">observational</span> and laboratory, and theoretical efforts. To date there is ample <span class="hlt">observational</span> evidence for crystalline water ice throughout the outer <span class="hlt">solar</span> <span class="hlt">system</span>. In addition, there is growing evidence that amorphous ice may be present on some bodies. More volatile ices, e.g. N2, CH4. CO, and other species, e.g. ammonia hydrate, are identified on objects lying at and beyond Uranus. Both photolysis and radiolysis play important roles in altering the original surfaces due to chemical reactions and erosion of the surface. Ultraviolet photolysis appears to dominate alteration of the upper few hundred Angstroms, although sputtering the surface can sometimes be a significantly competitative process; dominating on icy surfaces embedded in a strong planetary magnetospheric field. There is growing <span class="hlt">observational</span> evidence that the by-products of photolysis and radiolysis, suggested on a theoretical basis, are present on icy surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPSC...11..178G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPSC...11..178G"><span>Testing space weather connections in the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grison, B.; Souček, J.; Krupař, V.; Píša, D.; Santolík, O.; Taubenschuss, U.; Němec, F.</p> <p>2017-09-01</p> <p>This study aims at testing and validating tools for prediction of the impact of <span class="hlt">solar</span> events in the vicinity of inner and outer <span class="hlt">solar</span> <span class="hlt">system</span> planets using in-situ spacecraft data (primarily MESSENGER, STEREO and ACE, but also VEX and Cassini), remote Jovian <span class="hlt">observations</span> (Hubble telescope, Nançay decametric array), existing catalogues (HELCATS and Tao et al. (2005)) and the tested propagating models (the ICME radial propagation tool of the CDPP and the 1-D MHD code propagation model presented in Tao et al. (2005)).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001cxo..pres...17.','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001cxo..pres...17."><span>Young Stars in Orion May Solve Mystery of Our <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p>2001-09-01</p> <p>Scientists may have to give the Sun a little more credit. Exotic isotopes present in the early <span class="hlt">Solar</span> <span class="hlt">System</span>--which scientists have long-assumed were sprinkled there by a powerful, nearby star explosion--may have instead been forged locally by our Sun during the colossal <span class="hlt">solar</span>-flare tantrums of its baby years. The isotopes--special forms of atomic nuclei, such as aluminum-26, calcium-41, and beryllium-10--can form in the X-ray <span class="hlt">solar</span> flares of young stars in the Orion Nebula, which behave just like our Sun would have at such an early age. The finding, based on <span class="hlt">observations</span> by the Chandra X-ray Observatory, has broad implications for the formation of our own <span class="hlt">Solar</span> <span class="hlt">System</span>. Eric Feigelson, professor of astronomy and astrophysics at Penn State, led a team of scientists on this Chandra <span class="hlt">observation</span> and presents these results in Washington, D.C., today at a conference entitled "Two Years of Science with Chandra". "The Chandra study of Orion gives us the first chance to study the flaring properties of stars resembling the Sun when our <span class="hlt">solar</span> <span class="hlt">system</span> was forming," said Feigelson. "We found a much higher rate of flares than expected, sufficient to explain the production of many unusual isotopes locked away in ancient meteorites. If the young stars in Orion can do it, then our Sun should have been able to do it too." Scientists who study how our <span class="hlt">Solar</span> <span class="hlt">System</span> formed from a collapsed cloud of dust and gas have been hard pressed to explain the presence of these extremely unusual chemical isotopes. The isotopes are short-lived and had to have been formed no earlier than the creation of the <span class="hlt">Solar</span> <span class="hlt">System</span>, some five billion years ago. Yet these elements cannot be produced by a star as massive as our Sun under normal circumstances. (Other elements, such as silver and gold, were created long before the creation of the <span class="hlt">solar</span> <span class="hlt">system</span>.) The perplexing presence of these isotopic anomalies, found in ancient meteoroids orbiting the Earth, led to the theory that a supernova explosion occurred</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005aabb.book..305C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005aabb.book..305C"><span>Our <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coates, Andrew</p> <p>2005-10-01</p> <p>Up until the dark ages, humankind knew of six planets including our own. The invention of the telescope, and the beginnings of scientific thought on orbits and planetary motion, were in the seventeenth century. The next three centuries added Uranus, Neptune and Pluto to the known list as well as the many moons, asteroids and comets that we know today. It is only in the latter part of the 20th century that we have been privileged to carry out in-situ exploration of the planets, comets and the <span class="hlt">solar</span> wind's realm and to begin to understand the special conditions on Earth which meant that life started here. This is leading to a detailed view of the processes which have shaped our <span class="hlt">solar</span> <span class="hlt">system</span>. Here, we briefly review our current knowledge of the <span class="hlt">solar</span> <span class="hlt">system</span> we inhabit. We discuss the current picture of how the <span class="hlt">solar</span> <span class="hlt">system</span> began. Important processes at work, such as collisions and volcanism, and atmospheric evolution, are discussed. The planets, comets and asteroids are all discussed in general terms, together with the important discoveries from space missions which have led to our current views. For each of the bodies we present the current understanding of the physical properties and interrelationships and present questions for further study. The significance of recent results, such as proof that there were one standing bodies of water on Mars, and the discovery of what appears to be an Oort cloud comet, are put into context. What is in store for planetary exploration and discoveries in the future? Already a sequence of Mars exploration missions, a landing on a comet, further exploration of Saturn and the Jovian <span class="hlt">system</span> and the first flyby of Pluto are planned. We examine the major scientific questions to be answered. We also discuss the prospects for finding other Earth-like planets elsewhere, and for finding extraterrestrial life both within and beyond our own <span class="hlt">solar</span> <span class="hlt">system</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770025638','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770025638"><span><span class="hlt">Solar</span> energy collection <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Selcuk, M. K. (Inventor)</p> <p>1977-01-01</p> <p>An improved <span class="hlt">solar</span> energy collection <span class="hlt">system</span>, having enhanced energy collection and conversion capabilities, is delineated. The <span class="hlt">system</span> is characterized by a plurality of receivers suspended above a heliostat field comprising a multiplicity of reflector surfaces, each being adapted to direct a concentrated beam of <span class="hlt">solar</span> energy to illuminate a target surface for a given receiver. A magnitude of efficiency, suitable for effectively competing with <span class="hlt">systems</span> employed in collecting and converting energy extracted from fossil fuels, is indicated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E.521E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E.521E"><span>The Search for Life in the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ehrenfreund, Pascale</p> <p>2016-07-01</p> <p>To unravel the origins of life on Earth and possibly elsewhere remains one of mankind's most important discoveries. Basic building blocks of life are widespread in planetary <span class="hlt">systems</span> in our Milky Way and other galaxies. Extraterrestrial material delivered to young terrestrial planetary surfaces in the early history of our <span class="hlt">solar</span> <span class="hlt">system</span> through asteroids, comets and meteorites may have provided significant raw material for the emergence of life on Earth. Since August 2014 the comet rendezvous mission Rosetta has monitored the evolution of comet 67P/Churyumov-Gerasimenko during its approach to the Sun and <span class="hlt">observed</span> numerous volatiles and complex organic compounds on the comet surface. Several asteroid sample return missions as well as the improved analyses of key meteorites increase our knowledge about the organic inventory that seeded the young planets. Prokaryotic, anaerobic bacteria, which are approximately 3.5 billion years old, represent the first evidence for life on Earth. Since then, life has evolved to high complexity and adapted to nearly every explored environment on our planet. Extreme life on Earth has expanded the list of potentially habitable <span class="hlt">solar</span> <span class="hlt">system</span> environments. However, our neighbor planet Mars is the most promising target to search for life within our <span class="hlt">solar</span> <span class="hlt">system</span>. Data from the Curiosity rover show regions that were habitable in the past, traces of organic carbon and active CH_4 in the Martian atmosphere at present. Recent discoveries such as the plumes from the southern polar region of Enceladus and plume activity on Europa strengthen the long-standing hypothesis that moons in our <span class="hlt">solar</span> <span class="hlt">system</span> contain substantial bodies of water and are probably habitable. Since decades, a fleet of robotic space missions target planets, moons and small bodies to reveal clues on the origin of our <span class="hlt">solar</span> <span class="hlt">system</span> and life beyond Earth. This lecture will review and discuss past, current and future space missions investigating habitability and biosignatures in our</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9909E..7CM','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9909E..7CM"><span>Simulation of DKIST <span class="hlt">solar</span> adaptive optics <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marino, Jose; Carlisle, Elizabeth; Schmidt, Dirk</p> <p>2016-07-01</p> <p><span class="hlt">Solar</span> adaptive optics (AO) simulations are a valuable tool to guide the design and optimization process of current and future <span class="hlt">solar</span> AO and multi-conjugate AO (MCAO) <span class="hlt">systems</span>. <span class="hlt">Solar</span> AO and MCAO <span class="hlt">systems</span> rely on extended object cross-correlating Shack-Hartmann wavefront sensors to measure the wavefront. Accurate <span class="hlt">solar</span> AO simulations require computationally intensive operations, which have until recently presented a prohibitive computational cost. We present an update on the status of a <span class="hlt">solar</span> AO and MCAO simulation tool being developed at the National <span class="hlt">Solar</span> Observatory. The simulation tool is a multi-threaded application written in the C++ language that takes advantage of current large multi-core CPU computer <span class="hlt">systems</span> and fast ethernet connections to provide accurate full simulation of <span class="hlt">solar</span> AO and MCAO <span class="hlt">systems</span>. It interfaces with KAOS, a state of the art <span class="hlt">solar</span> AO control software developed by the Kiepenheuer-Institut fuer Sonnenphysik, that provides reliable AO control. We report on the latest results produced by the <span class="hlt">solar</span> AO simulation tool.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750013235','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750013235"><span>Exploration of the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Henderson, A., Jr.; Grey, J.</p> <p>1974-01-01</p> <p>A sourcebook of information on the <span class="hlt">solar</span> <span class="hlt">system</span> and the technology used for its exploration is presented. An outline of the potential achievements of <span class="hlt">solar</span> <span class="hlt">system</span> exploration is given along with a course of action which maximizes the rewards to mankind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..228a2012F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..228a2012F"><span>Liquid metals for <span class="hlt">solar</span> power <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Flesch, J.; Niedermeier, K.; Fritsch, A.; Musaeva, D.; Marocco, L.; Uhlig, R.; Baake, E.; Buck, R.; Wetzel, T.</p> <p>2017-07-01</p> <p>The use of liquid metals in <span class="hlt">solar</span> power <span class="hlt">systems</span> is not new. The receiver tests with liquid sodium in the 1980s at the Plataforma <span class="hlt">Solar</span> de Almería (PSA) already proved the feasibility of liquid metals as heat transfer fluid. Despite the high efficiency achieved with that receiver, further investigation of liquid metals in <span class="hlt">solar</span> power <span class="hlt">systems</span> was stopped due to a sodium spray fire. Recently, the topic has become interesting again and the gained experience during the last 30 years of liquid metals handling is applied to the concentrated <span class="hlt">solar</span> power community. In this paper, recent activities of the Helmholtz Alliance LIMTECH concerning liquid metals for <span class="hlt">solar</span> power <span class="hlt">systems</span> are presented. In addition to the components and <span class="hlt">system</span> simulations also the experimental setup and results are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030111407&hterms=public+relations&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dpublic%2Brelations','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030111407&hterms=public+relations&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dpublic%2Brelations"><span>Reuniting the <span class="hlt">Solar</span> <span class="hlt">System</span>: Integrated Education and Public Outreach Projects for <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Missions and Programs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lowes, Leslie; Lindstrom, Marilyn; Stockman, Stephanie; Scalice, Daniela; Klug, Sheri</p> <p>2003-01-01</p> <p>The <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Education Forum has worked for five years to foster Education and Public Outreach (E/PO) cooperation among missions and programs in order to leverage resources and better meet the needs of educators and the public. These efforts are coming together in a number of programs and products and in '2004 - The Year of the <span class="hlt">Solar</span> <span class="hlt">System</span>.' NASA's practice of having independent E/PO programs for each mission and its public affairs emphasis on uniqueness has led to a public perception of a fragmented <span class="hlt">solar</span> <span class="hlt">system</span> exploration program. By working to integrate <span class="hlt">solar</span> <span class="hlt">system</span> E/PO, the breadth and depth of the <span class="hlt">solar</span> <span class="hlt">system</span> exploration program is revealed. When emphasis is put on what missions have in common, as well as their differences, each mission is seen in the context of the whole program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH51D..02L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH51D..02L"><span><span class="hlt">Solar</span> Polar Imager: <span class="hlt">Observing</span> Coronal Transients from a New Perspective (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liewer, P. C.</p> <p>2013-12-01</p> <p>The heliophysics community has long recognized the need for a mission to <span class="hlt">observe</span> the Sun and corona from a polar perspective. One mission concept, the <span class="hlt">Solar</span> Polar Imager (SPI), has been studied extensively (Liewer et al in NASA Space Science Vision Missions, 2008). In this concept, a <span class="hlt">solar</span> sail is used to place a spacecraft in a circular 0.48-AU heliocentric orbit with an inclination of ~75 degrees. This orbit enables crucial <span class="hlt">observations</span> not possible from lower latitude perspectives. Magnetograph and Doppler <span class="hlt">observations</span> from a polar vantage point would revolutionize our understanding of the mechanism of <span class="hlt">solar</span> activity cycles, polar magnetic field reversals, the internal structure and dynamics of the Sun and its atmosphere. The rapid 4-month polar orbit combined with both in situ and remote sensing instrumentation further enables unprecedented studies of the physical connection between the Sun, the <span class="hlt">solar</span> wind, and <span class="hlt">solar</span> energetic particles. From the polar perspective, white light imagers could be used to track CMEs and predict their arrival at Earth (as demonstrated by STEREO). SPI is also well suited to study the relative roles of CME-driven shock versus flare-associated processes in <span class="hlt">solar</span> energetic particle acceleration. With the circular 0.48 AU orbit, <span class="hlt">solar</span> energetic particles could be more easily traced to their sources and their variation with latitude can be studied at a constant radius. This talk will discuss the science objectives, instrumentation and mission design for the SPI mission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012IAUSS...6E.401U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012IAUSS...6E.401U"><span><span class="hlt">Observing</span> strategies for future <span class="hlt">solar</span> facilities: the ATST test case</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uitenbroek, H.; Tritschler, A.</p> <p>2012-12-01</p> <p>Traditionally <span class="hlt">solar</span> <span class="hlt">observations</span> have been scheduled and performed very differently from night time efforts, in particular because we have been <span class="hlt">observing</span> the Sun for a long time, requiring new combinations of <span class="hlt">observables</span> to make progress, and because <span class="hlt">solar</span> physics <span class="hlt">observations</span> are often event driven on time scales of hours to days. With the proposal pressure that is expected for new large-aperture facilities, we can no longer afford the time spent on custom setups, and will have to rethink our scheduling and operations. We will discuss our efforts at Sac Peak in preparing for this new era, and outline the planned scheduling and operations planning for the ATST in particular.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4928888','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4928888"><span>Inner <span class="hlt">solar</span> <span class="hlt">system</span> material discovered in the Oort cloud</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Meech, Karen J.; Yang, Bin; Kleyna, Jan; Hainaut, Olivier R.; Berdyugina, Svetlana; Keane, Jacqueline V.; Micheli, Marco; Morbidelli, Alessandro; Wainscoat, Richard J.</p> <p>2016-01-01</p> <p>We have <span class="hlt">observed</span> C/2014 S3 (PANSTARRS), a recently discovered object on a cometary orbit coming from the Oort cloud that is physically similar to an inner main belt rocky S-type asteroid. Recent dynamical models successfully reproduce the key characteristics of our current <span class="hlt">solar</span> <span class="hlt">system</span>; some of these models require significant migration of the giant planets, whereas others do not. These models provide different predictions on the presence of rocky material expelled from the inner <span class="hlt">solar</span> <span class="hlt">system</span> in the Oort cloud. C/2014 S3 could be the key to verifying these predictions of the migration-based dynamical models. Furthermore, this object displays a very faint, weak level of comet-like activity, five to six orders of magnitude less than that of typical ice-rich comets on similar Orbits coming from the Oort cloud. For the nearly tailless appearance, we are calling C/2014 S3 a Manx object. Various arguments convince us that this activity is produced by sublimation of volatile ice, that is, normal cometary activity. The activity implies that C/2014 S3 has retained a tiny fraction of the water that is expected to be present at its formation distance in the inner <span class="hlt">solar</span> <span class="hlt">system</span>. We may be looking at fresh inner <span class="hlt">solar</span> <span class="hlt">system</span> Earth-forming material that was ejected from the inner <span class="hlt">solar</span> <span class="hlt">system</span> and preserved for billions of years in the Oort cloud. PMID:27386512</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810000157&hterms=economics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D30%26Ntt%3Deconomics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810000157&hterms=economics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D30%26Ntt%3Deconomics"><span>Dormitory <span class="hlt">Solar-Energy-System</span> Economics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1982-01-01</p> <p>102-page report analyzes long-term economic performance of a prepackaged <span class="hlt">solar</span> energy assembly <span class="hlt">system</span> at a dormitory installation and extrapolates to four additional sites about the U.S. Method of evaluation is f-chart procedure for <span class="hlt">solar</span>-heating and domestic hotwater <span class="hlt">systems</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1982ATJSE.104..158M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1982ATJSE.104..158M"><span>A regional comparison of <span class="hlt">solar</span>, heat pump, and <span class="hlt">solar</span>-heat pump <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Manton, B. E.; Mitchell, J. W.</p> <p>1982-08-01</p> <p>A comparative study of the thermal and economic performance of the parallel and series <span class="hlt">solar</span> heat pump <span class="hlt">systems</span>, stand alone <span class="hlt">solar</span> and stand alone heat pump <span class="hlt">systems</span> for residential space and domestic hot water heating for the U.S. using FCHART 4.0 is presented. Results show that the parallel <span class="hlt">solar</span> heat pump <span class="hlt">system</span> yields the greatest energy savings in the south. Very low cost collectors (50-150 dollars/sq m) are required for a series <span class="hlt">solar</span> heat pump <span class="hlt">system</span> in order for it to compete economically with the better of the parallel or <span class="hlt">solar</span> <span class="hlt">systems</span>. Conventional oil or gas furnaces need to have a seasonal efficiency of at least 70-85% in order to save as much primary energy as the best primary <span class="hlt">system</span> in the northeast. In addition, the implications of these results for current or proposed federal tax credit measures are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890062593&hterms=Qbo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DQbo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890062593&hterms=Qbo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DQbo"><span><span class="hlt">Observations</span> and statistical simulations of a proposed <span class="hlt">solar</span> cycle/QBO/weather relationship</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Baldwin, Mark P.; Dunkerton, Timothy J.</p> <p>1989-01-01</p> <p>The 10.7-cm <span class="hlt">solar</span> flux is <span class="hlt">observed</span> to be highly correlated with North Pole stratospheric temperatures when partitioned according to the phase of the equatorial stratospheric winds (the quasi-biennial oscillation, or QBO). Calculations show that temperatures over most of the Northern Hemisphere are highly correlated or anticorrelated with North Pole temperatures. The <span class="hlt">observed</span> spatial pattern of <span class="hlt">solar</span>-cycle correlations at high latitudes is shown to be not unique to the <span class="hlt">solar</span> cycle.</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/2001RaSc...36..773C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001RaSc...36..773C"><span>Total <span class="hlt">solar</span> eclipse effects on VLF signals: <span class="hlt">Observations</span> and modeling</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.; Rodger, Craig J.; Thomson, Neil R.; Lichtenberger, János; Steinbach, Péter; Cannon, Paul; Angling, Matthew J.</p> <p></p> <p>During the total <span class="hlt">solar</span> eclipse <span class="hlt">observed</span> 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 <span class="hlt">observed</span> throughout the whole eclipse period on path lengths <2000 km, while negative amplitude changes were <span class="hlt">observed</span> on paths >10,000 km. Negative phase changes were <span class="hlt">observed</span> on most paths, independent of path length. Although there was significant variation from path to path, the typical changes <span class="hlt">observed</span> were ~3 dB and ~50°. The changes <span class="hlt">observed</span> 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 <span class="hlt">observations</span>. 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 <span class="hlt">observations</span> made during the <span class="hlt">solar</span> 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 <span class="hlt">solar</span> radiation levels. The calculated electron concentration values at 77 km altitude throughout the period of the <span class="hlt">solar</span> eclipse show good agreement with the values determined from <span class="hlt">observations</span> at all times, which suggests that a linear variation in electron production rate with <span class="hlt">solar</span> ionizing radiation is reasonable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH51D2610K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH51D2610K"><span>Identifying and Characterizing Kinetic Instabilities using <span class="hlt">Solar</span> Wind <span class="hlt">Observations</span> of Non-Maxwellian Plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klein, K. G.</p> <p>2016-12-01</p> <p>Weakly collisional plasmas, of the type typically <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind, are commonly in a state other than local thermodynamic equilibrium. This deviation from a Maxwellian velocity distribution can be characterized by pressure anisotropies, disjoint beams streaming at differing speeds, leptokurtic distributions at large energies, and other non-thermal features. As these features may be artifacts of dynamic processes, including the the acceleration and expansion of the <span class="hlt">solar</span> wind, and as the free energy contained in these features can drive kinetic micro-instabilities, accurate measurement and modeling of these features is essential for characterizing the <span class="hlt">solar</span> wind. After a review of these features, a technique is presented for the efficient calculation of kinetic instabilities associated with a general, non-Maxwellian plasma. As a proof of principle, this technique is applied to bi-Maxwellian <span class="hlt">systems</span> for which kinetic instability thresholds are known, focusing on parameter scans including beams and drifting heavy minor ions. The application of this technique to fits of velocity distribution functions from current, forthcoming, and proposed missions including WIND, DSCOVR, <span class="hlt">Solar</span> Probe Plus, and THOR, as well as the underlying measured distribution functions, is discussed. Particular attention is paid to the effects of instrument pointing and integration time, as well as potential deviation between instabilities associated with the Maxwellian fits and those associated with the <span class="hlt">observed</span>, potentially non-Maxwellian, velocity distribution. Such application may further illuminate the role instabilities play in the evolution of the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016nova.pres..637K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016nova.pres..637K"><span>A Ninth Planet in Our <span class="hlt">Solar</span> <span class="hlt">System</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kohler, Susanna</p> <p>2016-01-01</p> <p>The recent discovery that the orbits of some Kuiper belt objects (KBOs) share properties has proved puzzling. A pair of scientists have now proposed a bold explanation: there may be a planet-sized object yet undetected in our <span class="hlt">solar</span> <span class="hlt">system</span>.Mysterious ClusteringKBOs, the population of mainly small objects beyond Neptune, have proven an especially interesting subject of study in the last decade as many small, distant bodies (such as Eris, the object that led to the demotion of Pluto to dwarf planet) have been discovered.Previous studies have recently discovered that some especially distant KBOs those that orbit with semimajor axes of a 150 AU, nearly four times that of Pluto all cross the ecliptic at a similar phase in their elliptical trajectories. This is unexpected, since gravitational tugs from the giant planets should have randomized this parameter over our <span class="hlt">solar</span> <span class="hlt">systems</span> multi-billion-year lifespan.Physical alignment of the orbits of Kuiper belt objects with a 250 AU (and two objects with a 150 AU that are dynamically stable). [Batygin Brown 2016]Two scientists at California Institute of Technology, Konstantin Batygin and Michael Brown (you might recognize Brown as the man who killed Pluto) have now increased the mystery. In a recently published a study, they demonstrate that for KBOs that have orbits with a 250 AU, the orbits are actually physically aligned.To explain this unexpected alignment which Batygin and Brown calculate has only a 0.007% probability of having occurred by chance the authors ask an exciting question: could this be caused by the presence of an unseen, large, perturbing body further out in the <span class="hlt">solar</span> <span class="hlt">system</span>?Simulating a Ninth PlanetThe authors test this hypothesis by carrying out both analytical calculations and numerical N-body simulations designed to determine if the gravitational influence of a distant, planetary-mass companion can explain the behavior we <span class="hlt">observe</span> from the large-orbit KBOs.Simulation of the effect of a distant planet (M = 10</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016MS%26E..162a2002S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016MS%26E..162a2002S"><span><span class="hlt">Solar</span> powered desalination <span class="hlt">system</span> using Fresnel lens</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sales, M. T. B. F.</p> <p>2016-11-01</p> <p>The Philippines is surrounded by coastal areas and these areas can be a potential source for potable water. This study aims to design and construct a <span class="hlt">solar</span> powered desalination <span class="hlt">system</span> using Fresnel lens. The experimental study was conducted using polluted salt water for the sample and desalination was carried out using the designed <span class="hlt">system</span>. The desalination <span class="hlt">system</span> was composed of the <span class="hlt">solar</span> concentrator, <span class="hlt">solar</span> still and the condenser <span class="hlt">system</span>. The Fresnel lens was made of acrylic plastic and was an effective <span class="hlt">solar</span> concentrator. <span class="hlt">Solar</span> stills made of dark colored glass bottles were effective in absorbing the <span class="hlt">solar</span> energy. The condenser <span class="hlt">system</span> made of polybutylene and polystyrene were effective in condensing the vapor at ambient temperature. The shortest time of vaporization of the salt water was at 293 sec and the optimum angle of position of the lens was 36.42°. The amount of condensate collected was directly proportional to the amount of salt water in the <span class="hlt">solar</span> still. The highest mean efficiency of the designed set-up was 34.82%. The water produced by the <span class="hlt">solar</span> powered desalination <span class="hlt">system</span> using Fresnel lens passed the standards set by WHO (World Health Organization) for drinking water.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22342126-serendipitous-all-sky-survey-bright-objects-outer-solar-system','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22342126-serendipitous-all-sky-survey-bright-objects-outer-solar-system"><span>A serendipitous all sky survey for bright objects in the outer <span class="hlt">solar</span> <span class="hlt">system</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>Brown, M. E.; Drake, A. J.; Djorgovski, S. G.</p> <p>2015-02-01</p> <p>We use seven year's worth of <span class="hlt">observations</span> from the Catalina Sky Survey and the Siding Spring Survey covering most of the northern and southern hemisphere at galactic latitudes higher than 20° to search for serendipitously imaged moving objects in the outer <span class="hlt">solar</span> <span class="hlt">system</span>. These slowly moving objects would appear as stationary transients in these fast cadence asteroids surveys, so we develop methods to discover objects in the outer <span class="hlt">solar</span> <span class="hlt">system</span> using individual <span class="hlt">observations</span> spaced by months, rather than spaced by hours, as is typically done. While we independently discover eight known bright objects in the outer <span class="hlt">solar</span> <span class="hlt">system</span>, the faintestmore » having V=19.8±0.1, no new objects are discovered. We find that the survey is nearly 100% efficient at detecting objects beyond 25 AU for V≲19.1 (V≲18.6 in the southern hemisphere) and that the probability that there is one or more remaining outer <span class="hlt">solar</span> <span class="hlt">system</span> object of this brightness left to be discovered in the unsurveyed regions of the galactic plane is approximately 32%.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1362154-building-sun4cast-system-improvements-solar-power-forecasting','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1362154-building-sun4cast-system-improvements-solar-power-forecasting"><span>Building the Sun4Cast <span class="hlt">System</span>: Improvements in <span class="hlt">Solar</span> Power Forecasting</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Haupt, Sue Ellen; Kosovic, Branko; Jensen, Tara; ...</p> <p>2017-06-16</p> <p>The Sun4Cast <span class="hlt">System</span> results from a research-to-operations project built on a value chain approach, and benefiting electric utilities’ customers, society, and the environment by improving state-of-the-science <span class="hlt">solar</span> power forecasting capabilities. As integration of <span class="hlt">solar</span> power into the national electric grid rapidly increases, it becomes imperative to improve forecasting of this highly variable renewable resource. Thus, a team of researchers from public, private, and academic sectors partnered to develop and assess a new <span class="hlt">solar</span> power forecasting <span class="hlt">system</span>, Sun4Cast. The partnership focused on improving decision-making for utilities and independent <span class="hlt">system</span> operators, ultimately resulting in improved grid stability and cost savings for consumers.more » The project followed a value chain approach to determine key research and technology needs to reach desired results. Sun4Cast integrates various forecasting technologies across a spectrum of temporal and spatial scales to predict surface <span class="hlt">solar</span> irradiance. Anchoring the <span class="hlt">system</span> is WRF-<span class="hlt">Solar</span>, a version of the Weather Research and Forecasting (WRF) numerical weather prediction (NWP) model optimized for <span class="hlt">solar</span> irradiance prediction. Forecasts from multiple NWP models are blended via the Dynamic Integrated Forecast (DICast) <span class="hlt">System</span>, the basis of the <span class="hlt">system</span> beyond about 6 h. For short-range (0-6 h) forecasts, Sun4Cast leverages several <span class="hlt">observation</span>-based nowcasting technologies. These technologies are blended via the Nowcasting Expert <span class="hlt">System</span> Integrator (NESI). The NESI and DICast <span class="hlt">systems</span> are subsequently blended to produce short to mid-term irradiance forecasts for <span class="hlt">solar</span> array locations. The irradiance forecasts are translated into power with uncertainties quantified using an analog ensemble approach, and are provided to the industry partners for real-time decision-making. The Sun4Cast <span class="hlt">system</span> ran operationally throughout 2015 and results were assessed. As a result, this paper analyzes the collaborative design process, discusses the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1362154','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1362154"><span>Building the Sun4Cast <span class="hlt">System</span>: Improvements in <span class="hlt">Solar</span> Power Forecasting</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>Haupt, Sue Ellen; Kosovic, Branko; Jensen, Tara</p> <p></p> <p>The Sun4Cast <span class="hlt">System</span> results from a research-to-operations project built on a value chain approach, and benefiting electric utilities’ customers, society, and the environment by improving state-of-the-science <span class="hlt">solar</span> power forecasting capabilities. As integration of <span class="hlt">solar</span> power into the national electric grid rapidly increases, it becomes imperative to improve forecasting of this highly variable renewable resource. Thus, a team of researchers from public, private, and academic sectors partnered to develop and assess a new <span class="hlt">solar</span> power forecasting <span class="hlt">system</span>, Sun4Cast. The partnership focused on improving decision-making for utilities and independent <span class="hlt">system</span> operators, ultimately resulting in improved grid stability and cost savings for consumers.more » The project followed a value chain approach to determine key research and technology needs to reach desired results. Sun4Cast integrates various forecasting technologies across a spectrum of temporal and spatial scales to predict surface <span class="hlt">solar</span> irradiance. Anchoring the <span class="hlt">system</span> is WRF-<span class="hlt">Solar</span>, a version of the Weather Research and Forecasting (WRF) numerical weather prediction (NWP) model optimized for <span class="hlt">solar</span> irradiance prediction. Forecasts from multiple NWP models are blended via the Dynamic Integrated Forecast (DICast) <span class="hlt">System</span>, the basis of the <span class="hlt">system</span> beyond about 6 h. For short-range (0-6 h) forecasts, Sun4Cast leverages several <span class="hlt">observation</span>-based nowcasting technologies. These technologies are blended via the Nowcasting Expert <span class="hlt">System</span> Integrator (NESI). The NESI and DICast <span class="hlt">systems</span> are subsequently blended to produce short to mid-term irradiance forecasts for <span class="hlt">solar</span> array locations. The irradiance forecasts are translated into power with uncertainties quantified using an analog ensemble approach, and are provided to the industry partners for real-time decision-making. The Sun4Cast <span class="hlt">system</span> ran operationally throughout 2015 and results were assessed. As a result, this paper analyzes the collaborative design process, discusses the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002sssy.book.....G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002sssy.book.....G"><span>The Story of the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garlick, Mark A.</p> <p>2002-03-01</p> <p>The bodies of our <span class="hlt">Solar</span> <span class="hlt">System</span> have orbited continously around the Sun since their formation, but they have not always been there, and conditions have not always been as they are today. The Story of the <span class="hlt">Solar</span> <span class="hlt">System</span> explains how our <span class="hlt">Solar</span> <span class="hlt">System</span> came into existence, how it has evolved and how it might end billions of years from now. After a brief historical introduction, Mark Garlick describes the birth of the Sun and the steps that built up the bodies of the <span class="hlt">Solar</span> <span class="hlt">System</span>. Vivid illustrations of planets, moons, asteroids and comets complement the detailed descriptions. A comparison of these objects, and an analysis of how they have changed and evolved since birth is followed by a look towards the end of the <span class="hlt">Solar</span> <span class="hlt">System</span>'s existence. Mark A. Garlick obtained his PhD in astrophysics from the Mullard Space Science Laboratory in Surrey, England. He is a member of the International Association of Astronomical Artists, and currently works as a freelance science writer and astronomical illustrator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006JGRA..11112S01N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JGRA..11112S01N"><span>Magnetic helicity and flux tube dynamics in the <span class="hlt">solar</span> convection zone: Comparisons between <span class="hlt">observation</span> and theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nandy, Dibyendu</p> <p>2006-12-01</p> <p>Magnetic helicity, a conserved topological parameter in ideal MHD <span class="hlt">systems</span>, conditions close to which are realized in the <span class="hlt">solar</span> plasma, is intimately connected to the creation and subsequent dynamics of magnetic flux tubes in the <span class="hlt">solar</span> interior. It can therefore be used as a tool to probe such dynamics. In this paper we show how photospheric <span class="hlt">observations</span> of magnetic helicity of isolated magnetic flux tubes, manifested as the twist and writhe of <span class="hlt">solar</span> active regions, can constrain the creation and dynamics of flux tubes in the <span class="hlt">solar</span> convection zone and the nature of convective turbulence itself. We analyze the <span class="hlt">observed</span> latitudinal distribution of twists in photospheric active regions, derived from <span class="hlt">solar</span> vector magnetograms, in the largest such sample studied till-date. We confirm and put additional constraints on the hemispheric twist helicity trend and find that the dispersion in the active region twist distribution is latitude-independent, implying that the amplitude of turbulent fluctuations does not vary with latitude in the convection zone. Our data set also shows that the amplitude and dispersion of twist decreases with increasing magnetic size of active regions, supporting the conclusion that larger flux tubes are less affected by turbulence. Among the various theoretical models that have been proposed till-date to explain the origin of twist, our <span class="hlt">observations</span> best match the Σ effect model, which invokes helical turbulent buffeting of rising flux tubes as the mechanism for twist creation. Finally, we complement our analysis of twists with past <span class="hlt">observations</span> of tilts in <span class="hlt">solar</span> active regions and tie them in with theoretical modeling studies, to build up a comprehensive picture of the dynamics of twisted magnetic flux tubes throughout the <span class="hlt">solar</span> convection zone. This general framework, binding together theory and <span class="hlt">observations</span>, suggests that flux tubes have a wide range of twists in the <span class="hlt">solar</span> convection zone, with some as high as to make them susceptible to the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040073528&hterms=chaos&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dchaos','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040073528&hterms=chaos&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dchaos"><span>Chaos in the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lecar, Myron; Franklin, Fred A.; Holman, Matthew J.; Murray, Norman J.</p> <p>2001-01-01</p> <p>The physical basis of chaos in the <span class="hlt">solar</span> <span class="hlt">system</span> is now better understood: In all cases investigated so far, chaotic orbits result from overlapping resonances. Perhaps the clearest examples are found in the asteroid belt. Overlapping resonances account for its kirkwood gaps and were used to predict and find evidence for very narrow gaps in the outer belt. Further afield, about one new "short-peroid" comet is discovered each year. They are believed to come from the "Kuiper Belt" (at 40 AU or more) via chaotic orbits produced by mean-motion and secular resonances with Neptune. Finally, the planetary <span class="hlt">system</span> itself is not immune from chaos. In the inner <span class="hlt">solar</span> <span class="hlt">system</span>, overlapping secular resonances have been identified as the possible source of chaos. For example, Mercury in 1012 years, may suffer a close encounter with Venus or plunge into the Sun. In the outer <span class="hlt">solar</span> <span class="hlt">system</span>, three-body resonances have been identified as a source of chaos, but on an even longer time scale of 109 times the age of the <span class="hlt">solar</span> <span class="hlt">system</span>. On the human time scale, the planets do follow their orbits in a stately procession, and we can predict their trajectories for hundreds of thousands of years. That is because the mavericks, with shorter instability times, have long since been ejected. The <span class="hlt">solar</span> <span class="hlt">system</span> is not stable; it is just old!</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780021634','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780021634"><span>Storage <span class="hlt">systems</span> for <span class="hlt">solar</span> thermal power</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Calogeras, J. E.; Gordon, L. H.</p> <p>1978-01-01</p> <p>The development status is reviewed of some thermal energy storage technologies specifically oriented towards providing diurnal heat storage for <span class="hlt">solar</span> central power <span class="hlt">systems</span> and <span class="hlt">solar</span> total energy <span class="hlt">systems</span>. These technologies include sensible heat storage in caverns and latent heat storage using both active and passive heat exchange processes. In addition, selected thermal storage concepts which appear promising to a variety of advanced <span class="hlt">solar</span> thermal <span class="hlt">system</span> applications are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH42A..06D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH42A..06D"><span><span class="hlt">Observational</span> evidence for Alfven waves in the <span class="hlt">solar</span> atmosphere (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>De Pontieu, B.</p> <p>2013-12-01</p> <p>Alfven waves have long been suspected of playing an important role in both heating the corona and accelerating the <span class="hlt">solar</span> wind. Recently, more and more <span class="hlt">observational</span> evidence for the presence of such waves has been reported in both the corona and the lower <span class="hlt">solar</span> atmosphere. I will review <span class="hlt">observations</span> of the properties and presence of Alfven waves from CoMP, Hinode, AIA and ground-based telescopes in both coronal lines and the lower <span class="hlt">solar</span> atmosphere. I will discuss our current understanding of the importance of these waves for the energy balance of the corona. I will also present initial results of the Interface Region Imaging Spectrograph (IRIS) which was launched in June 2013 and obtains images and spectra in both the far and near ultraviolet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018DDA....4930201K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018DDA....4930201K"><span>Using Real and Simulated TNOs to Constrain the Outer <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaib, Nathan</p> <p>2018-04-01</p> <p>Over the past 2-3 decades our understanding of the outer <span class="hlt">solar</span> system’s history and current state has evolved dramatically. An explosion in the number of detected trans-Neptunian objects (TNOs) coupled with simultaneous advances in numerical models of orbital dynamics has driven this rapid evolution. However, successfully constraining the orbital architecture and evolution of the outer <span class="hlt">solar</span> <span class="hlt">system</span> requires accurately comparing simulation results with <span class="hlt">observational</span> datasets. This process is challenging because <span class="hlt">observed</span> datasets are influenced by orbital discovery biases as well as TNO size and albedo distributions. Meanwhile, such influences are generally absent from numerical results. Here I will review recent work I and others have undertaken using numerical simulations in concert with catalogs of <span class="hlt">observed</span> TNOs to constrain the outer <span class="hlt">solar</span> system’s current orbital architecture and past evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...852...79Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...852...79Y"><span>Two <span class="hlt">Solar</span> Tornadoes <span class="hlt">Observed</span> with the Interface Region Imaging Spectrograph</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Zihao; Tian, Hui; Peter, Hardi; Su, Yang; Samanta, Tanmoy; Zhang, Jingwen; Chen, Yajie</p> <p>2018-01-01</p> <p>The barbs or legs of some prominences show an apparent motion of rotation, which are often termed <span class="hlt">solar</span> tornadoes. It is under debate whether the apparent motion is a real rotating motion, or caused by oscillations or counter-streaming flows. We present analysis results from spectroscopic <span class="hlt">observations</span> of two tornadoes by the Interface Region Imaging Spectrograph. Each tornado was <span class="hlt">observed</span> for more than 2.5 hr. Doppler velocities are derived through a single Gaussian fit to the Mg II k 2796 Å and Si IV 1393 Å line profiles. We find coherent and stable redshifts and blueshifts adjacent to each other across the tornado axes, which appears to favor the interpretation of these tornadoes as rotating cool plasmas with temperatures of 104 K–105 K. This interpretation is further supported by simultaneous <span class="hlt">observations</span> of the Atmospheric Imaging Assembly on board the <span class="hlt">Solar</span> Dynamics Observatory, which reveal periodic motions of dark structures in the tornadoes. Our results demonstrate that spectroscopic <span class="hlt">observations</span> can provide key information to disentangle different physical processes in <span class="hlt">solar</span> prominences.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23383910','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23383910"><span>Ion kinetic scale in the <span class="hlt">solar</span> wind <span class="hlt">observed</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Śafránková, Jana; Němeček, Zdeněk; Přech, Lubomír; Zastenker, Georgy N</p> <p>2013-01-11</p> <p>This Letter shows the first results from the <span class="hlt">solar</span> wind monitor onboard the Spektr-R spacecraft which measures plasma moments with a time resolution of 31 ms. This high-time resolution allows us to make direct <span class="hlt">observations</span> of <span class="hlt">solar</span> wind turbulence below ion kinetic length scales. We present examples of the frequency spectra of the density, velocity, and thermal velocity. Our study reveals that although these parameters exhibit the same behavior at the magnetohydrodynamic scale, their spectra are remarkably different at the kinetic scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740018557','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740018557"><span><span class="hlt">Solar</span> radio <span class="hlt">observations</span> in support of Skylab A</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gotwols, B. L.</p> <p>1974-01-01</p> <p>The <span class="hlt">solar</span> radio spectra were recorded in real time, both on film and magnetic tape, during the period from November 1972 to February 1974. A catalogue of the <span class="hlt">observations</span> is given for the frequency range 565-1000 MHz and includes descriptions of the bursts, intensity scales, and pertinent remarks. Some theoretical considerations resulting from the research are given. Equipment modified for the experiment is described and the text of the final report which summarizes the research on type IV <span class="hlt">solar</span> radio bursts is included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663151-high-resolution-multi-wavelength-simultaneous-imaging-system-solar-adaptive-optics','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663151-high-resolution-multi-wavelength-simultaneous-imaging-system-solar-adaptive-optics"><span>A High-resolution Multi-wavelength Simultaneous Imaging <span class="hlt">System</span> with <span class="hlt">Solar</span> Adaptive Optics</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>Rao, Changhui; Zhu, Lei; Gu, Naiting</p> <p></p> <p>A high-resolution multi-wavelength simultaneous imaging <span class="hlt">system</span> from visible to near-infrared bands with a <span class="hlt">solar</span> adaptive optics <span class="hlt">system</span>, in which seven imaging channels, including the G band (430.5 nm), the Na i line (589 nm), the H α line (656.3 nm), the TiO band (705.7 nm), the Ca ii IR line (854.2 nm), the He i line (1083 nm), and the Fe i line (1565.3 nm), are chosen, is developed to image the <span class="hlt">solar</span> atmosphere from the photosphere layer to the chromosphere layer. To our knowledge, this is the <span class="hlt">solar</span> high-resolution imaging <span class="hlt">system</span> with the widest spectral coverage. This <span class="hlt">system</span> wasmore » demonstrated at the 1 m New Vaccum <span class="hlt">Solar</span> Telescope and the on-sky high-resolution <span class="hlt">observational</span> results were acquired. In this paper, we will illustrate the design and performance of the imaging <span class="hlt">system</span>. The calibration and the data reduction of the <span class="hlt">system</span> are also presented.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/10116814','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/10116814"><span>Views of the <span class="hlt">solar</span> <span class="hlt">system</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>Hamilton, C.</p> <p>1995-02-01</p> <p>Views of the <span class="hlt">Solar</span> <span class="hlt">System</span> has been created as an educational tour of the <span class="hlt">solar</span> <span class="hlt">system</span>. It contains images and information about the Sun, planets, moons, asteroids and comets found within the <span class="hlt">solar</span> <span class="hlt">system</span>. The image processing for many of the images was done by the author. This tour uses hypertext to allow space travel by simply clicking on a desired planet. This causes information and images about the planet to appear on screen. While on a planet page, hyperlinks travel to pages about the moons and other relevant available resources. Unusual terms are linked to and defined in themore » Glossary page. Statistical information of the planets and satellites can be browsed through lists sorted by name, radius and distance. History of Space Exploration contains information about rocket history, early astronauts, space missions, spacecraft and detailed chronology tables of space exploration. The Table of Contents page has links to all of the various pages within Views Of the <span class="hlt">Solar</span> <span class="hlt">System</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRD..120.6500W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRD..120.6500W"><span>Decadal variability of surface incident <span class="hlt">solar</span> radiation over China: <span class="hlt">Observations</span>, satellite retrievals, and reanalyses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Kaicun; Ma, Qian; Li, Zhijun; Wang, Jiankai</p> <p>2015-07-01</p> <p>Existing studies have shown that <span class="hlt">observed</span> surface incident <span class="hlt">solar</span> radiation (Rs) over China may have important inhomogeneity issues. This study provides metadata and reference data to homogenize <span class="hlt">observed</span> Rs, from which the decadal variability of Rs over China can be accurately derived. From 1958 to 1990, diffuse <span class="hlt">solar</span> radiation (Rsdif) and direct <span class="hlt">solar</span> radiation (Rsdir) were measured separately, and Rs was calculated as their sum. The pyranometers used to measure Rsdif had a strong sensitivity drift problem, which introduced a spurious decreasing trend into the <span class="hlt">observed</span> Rsdif and Rs data, whereas the <span class="hlt">observed</span> Rsdir did not suffer from this sensitivity drift problem. From 1990 to 1993, instruments and measurement methods were replaced and measuring stations were restructured in China, which introduced an abrupt increase in the <span class="hlt">observed</span> Rs. Intercomparisons between <span class="hlt">observation</span>-based and model-based Rs performed in this research show that sunshine duration (SunDu)-derived Rs is of high quality and can be used as reference data to homogenize <span class="hlt">observed</span> Rs data. The homogenized and adjusted data of <span class="hlt">observed</span> Rs combines the advantages of <span class="hlt">observed</span> Rs in quantifying hourly to monthly variability and SunDu-derived Rs in depicting decadal variability and trend. Rs averaged over 105 stations in China decreased at -2.9 W m-2 per decade from 1961 to 1990 and remained stable afterward. This decadal variability is confirmed by the <span class="hlt">observed</span> Rsdir and diurnal temperature ranges, and can be reproduced by high-quality Earth <span class="hlt">System</span> Models. However, neither satellite retrievals nor reanalyses can accurately reproduce such decadal variability over China.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P23F..07H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P23F..07H"><span>UV Signatures of Ices: Moons in the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hendrix, A. R.; Hansen, C. J.; Retherford, K. D.; Vilas, F.</p> <p>2017-12-01</p> <p>Using Earth-orbiting telescopes such as the International Ultraviolet Explorer and the Hubble Space Telescope, significant advances have been made in the area of ultraviolet <span class="hlt">observations</span> of <span class="hlt">solar</span> <span class="hlt">system</span> objects. More in-depth studies have been made using interplanetary probes such as Galileo, Cassini and Lunar Reconnaissance Orbiter (LRO). While the UV spectral range has traditionally been used to study atmospheric and auroral processes, there is much to be learned by examining solid surfaces in the UV, including surface composition, weathering processes and effects, and the generation of thin atmospheres. Here we focus on moons in the <span class="hlt">solar</span> <span class="hlt">system</span>, including Earth's moon and the Saturnian satellites. The diagnostic UV signature of H2O is used to study ice in the lunar polar regions as well as hydration at lower latitudes, in <span class="hlt">observations</span> from LRO LAMP. The water ice signature is nearly ubiquitous in the Saturn <span class="hlt">system</span>; Cassini UVIS datasets are used to study grain sizes, exogenic processes/effects and non-ice species.</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://hdl.handle.net/2060/19800022964','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800022964"><span><span class="hlt">Solar</span> rocket <span class="hlt">system</span> concept analysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Boddy, J. A.</p> <p>1980-01-01</p> <p>The use of <span class="hlt">solar</span> energy to heat propellant for application to Earth orbital/planetary propulsion <span class="hlt">systems</span> is of interest because of its performance capabilities. The achievable specific impulse values are approximately double those delivered by a chemical rocket <span class="hlt">system</span>, and the thrust is at least an order of magnitude greater than that produced by a mercury bombardment ion propulsion thruster. The primary advantage the <span class="hlt">solar</span> heater thruster has over a mercury ion bombardment <span class="hlt">system</span> is that its significantly higher thrust permits a marked reduction in mission trip time. The development of the space transportation <span class="hlt">system</span>, offers the opportunity to utilize the full performance potential of the <span class="hlt">solar</span> rocket. The requirements for transfer from low Earth orbit (LEO) to geosynchronous equatorial orbit (GEO) was examined as the return trip, GEO to LEO, both with and without payload. Payload weights considered ranged from 2000 to 100,000 pounds. The performance of the <span class="hlt">solar</span> rocket was compared with that provided by LO2-LH2, N2O4-MMH, and mercury ion bombardment <span class="hlt">systems</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.771a2038M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.771a2038M"><span>Stellar background <span class="hlt">observation</span> during Total <span class="hlt">Solar</span> Eclipse March 9th 2016</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mumtahana, Farahhati; Timur Jaelani, Anton; Muhamad, Johan; Sutastio, Heri</p> <p>2016-11-01</p> <p>We report <span class="hlt">observation</span> and an early analysis of stellar background from total <span class="hlt">solar</span> eclipse in Ternate, Indonesia. The eclipse phenomena which occurred on March, 9th 2016 was <span class="hlt">observed</span> with certain portable instruments in order to obtain the stars behind the Sun in particular field of view and resolution. From our <span class="hlt">observation</span> site in Ternate city, <span class="hlt">solar</span> eclipse occurred in the late morning when the weather was unfortunately cloudy. However, during the darkness of totality, we obtained several point source objects between the gaps of the moving clouds and we suspected them as very faint stars due to their appearance in several frames. Those so called stars have been identified and measured with respect to their positions toward the center of the Sun. The main purpose of this research is to revisit strong lensing calculation of the Sun during total <span class="hlt">solar</span> eclipse by measuring the deflection angle of the background stars as it had been calculated by Einstein and proved by Eddington at a total <span class="hlt">solar</span> eclipse in 1919. To accomplish this aim, we need to conduct another <span class="hlt">observation</span> to measure position of the same stars in the next period when those stars appear in the night sky.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4811705P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4811705P"><span>The 2016 Transit of Mercury <span class="hlt">Observed</span> from Major <span class="hlt">Solar</span> Telescopes and Satellites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, Jay M.; Schneider, Glenn; Gary, Dale; Chen, Bin; Sterling, Alphonse C.; Reardon, Kevin P.; Dantowitz, Ronald; Kopp, Greg A.</p> <p>2016-10-01</p> <p>We report <span class="hlt">observations</span> from the ground and space of the 9 May 2016 transit of Mercury. We build on our explanation of the black-drop effect in transits of Venus based on spacecraft <span class="hlt">observations</span> of the 1999 transit of Mercury (Schneider, Pasachoff, and Golub, Icarus 168, 249, 2004). In 2016, we used the 1.6-m New <span class="hlt">Solar</span> Telescope at the Big Bear <span class="hlt">Solar</span> Observatory with active optics to <span class="hlt">observe</span> Mercury's transit at high spatial resolution. We again saw a small black-drop effect as 3rd contact neared, confirming the data that led to our earlier explanation as a confluence of the point-spread function and the extreme <span class="hlt">solar</span> limb darkening (Pasachoff, Schneider, and Golub, in IAU Colloq. 196, 2004). We again used IBIS on the Dunn <span class="hlt">Solar</span> Telescope of the Sacramento Peak Observatory, as A. Potter continued his <span class="hlt">observations</span>, previously made at the 2006 transit of Mercury, at both telescopes of the sodium exosphere of Mercury (Potter, Killen, Reardon, and Bida, Icarus 226, 172, 2013). We imaged the transit with IBIS as well as with two RED Epic IMAX-quality cameras alongside it, one with a narrow passband. We show animations of our high-resolution ground-based <span class="hlt">observations</span> along with <span class="hlt">observations</span> from XRT on JAXA's Hinode and from NASA's <span class="hlt">Solar</span> Dynamics Observatory. Further, we report on the limit of the transit change in the Total <span class="hlt">Solar</span> Irradiance, continuing our interest from the transit of Venus TSI (Schneider, Pasachoff, and Willson, ApJ 641, 565, 2006; Pasachoff, Schneider, and Willson, AAS 2005), using NASA's SORCE/TIM and the Air Force's TCTE/TIM. See http://transitofvenus.info and http://nicmosis.as.arizona.edu.Acknowledgments: We were glad for the collaboration at Big Bear of Claude Plymate and his colleagues of the staff of the Big Bear <span class="hlt">Solar</span> Observatory. We also appreciate the collaboration on the transit studies of Robert Lucas (Sydney, Australia) and Evan Zucker (San Diego, California). JMP appreciates the sabbatical hospitality of the Division of Geosciences and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011SPD....42.1501S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011SPD....42.1501S"><span><span class="hlt">Solar</span> Hard X-ray <span class="hlt">Observations</span> with NuSTAR</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, David M.; Krucker, S.; Hudson, H. S.; Hurford, G. J.; White, S. M.; Mewaldt, R. A.; Stern, D.; Grefenstette, B. W.; Harrison, F. A.</p> <p>2011-05-01</p> <p>High-sensitivity imaging of coronal hard X-rays allows detection of freshly accelerated nonthermal electrons at the acceleration site. A few such <span class="hlt">observations</span> have been made with Yohkoh and RHESSI, but a leap in sensitivity could help pin down the time, place, and manner of reconnection. In 2012, the Nuclear Spectroscopic Telescope Array (NuSTAR), a NASA Small Explorer for high energy astrophysics that uses grazing-incidence optics to focus X-rays up to 80 keV, will be launched. NuSTAR is capable of <span class="hlt">solar</span> pointing, and three weeks will be dedicated to <span class="hlt">solar</span> <span class="hlt">observing</span> during the baseline two-year mission. NuSTAR will be 200 times more sensitive than RHESSI in the hard X-ray band. This will allow the following new <span class="hlt">observations</span>, among others: 1) Extrapolation of the micro/nanoflare distribution by two orders of magnitude down in flux 2) Search for hard X-rays from network nanoflares (soft X-ray bright points) and evaluation of their role in coronal heating 3) Discovery of hard X-ray bremsstrahlung from the electron beams driving type III radio bursts, and measurement of their electron spectrum 4) Hard X-ray studies of polar soft X-ray jets and impulsive <span class="hlt">solar</span> energetic particle events at the edge of coronal holes, and comparison of these events with <span class="hlt">observations</span> of 3He and other particles in interplanetary space 5) Study of coronal bremsstrahlung from particles accelerated by coronal mass ejections as they are first launched 6) Study of particles at the coronal reconnection site when flare footpoints are occulted; and 7) Search for hypothetical axion particles created in the <span class="hlt">solar</span> core via the hard X-ray signal from their conversion to X-rays in the coronal magnetic field. NuSTAR will also serve as a pathfinder for a future dedicated space mission with enhanced capabilities, such as a satellite version of the FOXSI sounding rocket.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050180713&hterms=comparative&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dcomparative','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050180713&hterms=comparative&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dcomparative"><span>A Comparative View of X-rays from the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bhardwaj, Anil; Elsner, Ron; Gladstone, Randy; Cravens, Tom; Waite, Hunter; Branduardi-Raymont, Graziella; Ostgaard, Nikolai; Dennerl, Konrad; Lisse, Carey; Kharchenko, Vasili</p> <p>2005-01-01</p> <p>With the advent of sophisticated X-ray observatories, viz., Chandra and XMM-Newton, the field of planetary X-ray astronomy is advancing at a faster pace. Several new <span class="hlt">solar</span> <span class="hlt">system</span> objects are now know to shine in X-rays at energies generally below 2 keV. Jupiter, Saturn, and Earth, all three magnetized planets, have been <span class="hlt">observed</span> by Chandra and XMM-Newton. At Jupiter, both auroral and non-auroral disk X-ray emissions have been <span class="hlt">observed</span>. The first soft X-ray <span class="hlt">observation</span> of Earth's aurora by Chandra shows that it is highly variable. X-rays have been detected from Saturn's disk, but no convincing evidence of X-ray aurora has been seen. Several comets have been <span class="hlt">observed</span> in X-rays by Chandra and XMM-Newton. Cometary X-rays are produced due to change exchange of <span class="hlt">solar</span> wind ions with cold cometary neutrals. Soft X-rays have also been <span class="hlt">observed</span> from Venus, Mars, Moon, Io, Europa, Io plasma torus, and heliosphere. The non-auroral X-ray emissions from Jupiter, Saturn, and Earth, and those from sunlit disk of Mars, Venus, and Moon are produced due to scattering of <span class="hlt">solar</span> X-rays. The spectral characteristics of X-ray emission from comets, heliosphere, darkside of Moon, and Martian halo are quite similar, but they appear to be quite different from those of Jovian auroral X-rays. The X- ray aurora on Earth is generated by electron bremsstrahlung and on Jupiter by precipitation of highly-ionized energetic heavy ions. In this paper we will present a comparative overview of X-ray emission from different <span class="hlt">solar</span> <span class="hlt">system</span> objects and make an attempt to synthesize a coherent picture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013CoSka..43...81M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013CoSka..43...81M"><span><span class="hlt">Solar</span> radio <span class="hlt">observations</span> and radio interference monitoring in Roztoky</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Monstein, C.; Baluďanský, D.</p> <p>2013-10-01</p> <p>This paper is part of a planned measurement campaign in which spectrum measurements were carried out at different locations worldwide within potential locations of the e-Callisto network. The results of measurements at the Callisto <span class="hlt">observing</span> station in Roztoky, which took place at the beginning of May 2013, are presented. Measurements were made out with a special low cost broadband logarithmic periodic antenna connected to a Callisto spectrometer designed and built at ETH Zurich (Benz, 2004). This study provides the technical basis to decide whether it is possible to make <span class="hlt">solar</span> spectroscopic measurements below 1 GHz (λ>30 cm) at the <span class="hlt">observing</span> station. In terms of electromagnetic interference, Roztoky is not perfect for broadband spectroscopic <span class="hlt">solar</span> radio astronomy <span class="hlt">observations</span> due to non negligible radio interference level from the nearby FM-transmitters. Nevertheless, low frequency <span class="hlt">observations</span> below 80 MHz, as well as <span class="hlt">observations</span> in some small bands above 116 MHz can be done.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790054881&hterms=TES+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DTES%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790054881&hterms=TES+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DTES%2Bsystem"><span><span class="hlt">Solar</span> Stirling <span class="hlt">system</span> development</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stearns, J. W., Jr.; Won, Y. S.; Poon, P. T.; Das, R.; Chow, E. Y.</p> <p>1979-01-01</p> <p>A low-cost, high-efficiency dish-Stirling <span class="hlt">solar</span> thermal-electric power <span class="hlt">system</span> is being developed for test in 1981. <span class="hlt">System</span> components are the <span class="hlt">solar</span> concentrator, receiver, fossil fuel combustor, thermal energy storage (TES), engine-generator, and power processing. <span class="hlt">System</span> conceptualization is completed and design is in progress. Two receiver alternatives are being evaluated, a direct-coupled receiver-engine configuration with no TES and a heat pipe receiver with TES. <span class="hlt">System</span> cost projections are being made. Goals for the <span class="hlt">system</span> development task are (1) to develop an advanced dish-Stirling technology, utilizing a team of industrial contractors, (2) to demonstrate that technology at the <span class="hlt">system</span> level, and (3) to determine how to achieve low production cost.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730008067','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730008067"><span>Space <span class="hlt">observations</span> of the variability of <span class="hlt">solar</span> irradiance in the near and far ultraviolet</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heath, D. F.</p> <p>1972-01-01</p> <p>Satellite <span class="hlt">observations</span> of the ultraviolet <span class="hlt">solar</span> irradiance in selected wavelength bands between 1200 and 3000 a were made continuously by photometers consisting of broad-band sensors operated on Numbus 3 and 4 which were launched in April 1969 and 1970. In addition, spectrophotometer measurements of the <span class="hlt">solar</span> irradiance were made with a dispersive instrument at 12 selected wavelengths from 2550 to 3400 a with a 10 a bandpass on Nimbus 4. Variations of the <span class="hlt">solar</span> irradiance associated with the <span class="hlt">solar</span> rotational period were <span class="hlt">observed</span> since the launch of Nimbus 3. These variations are apparently associated with two source regions separated by about 180 deg in <span class="hlt">solar</span> longitude. The change in irradiance with <span class="hlt">solar</span> rotation was found to increase with decreasing wavelengths. Different types of the <span class="hlt">observed</span> variations in uv <span class="hlt">solar</span> irradiance can be classified in accordance with characteristics times, e.g. in the order of increasing periods as follows: (1)flare associated enhancements (2) 27-day variations due to <span class="hlt">solar</span> rotation; (3) a possible biennial effect; and (4) long term variations associated with the 11-year <span class="hlt">solar</span> cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920038086&hterms=text+historical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dtext%2Bhistorical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920038086&hterms=text+historical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dtext%2Bhistorical"><span>Sir William Herschel's notebooks - Abstracts of <span class="hlt">solar</span> <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>Hoyt, Douglas V.; Schatten, Kenneth H.</p> <p>1992-01-01</p> <p>An introduction to the background of Sir William Herschel's notebooks and the historical context within which his <span class="hlt">observations</span> were made are provided. The <span class="hlt">observations</span> have relevance in reconstructing <span class="hlt">solar</span> behavior, as discussed in a separate analysis paper by Hoyt and Schatten (1992), and in understanding active features on the sun such as faculae. The text of Herschel's notebooks with modern terms used throughout forms the body of this paper. The complete text has not previously been published and is not easily accessible to scholars. Herschel used different words for <span class="hlt">solar</span> features than are used today, and thus, for clarity, his terminology is changed on two occasions. A glossary explains the terminology changed. In the text of the notebooks, several contemporaries are mentioned; a brief description of Herschel's colleagues is provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22126712-hemispheric-asymmetries-polar-solar-wind-observed-ulysses-near-minima-solar-cycles','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22126712-hemispheric-asymmetries-polar-solar-wind-observed-ulysses-near-minima-solar-cycles"><span>HEMISPHERIC ASYMMETRIES IN THE POLAR <span class="hlt">SOLAR</span> WIND <span class="hlt">OBSERVED</span> BY ULYSSES NEAR THE MINIMA OF <span class="hlt">SOLAR</span> CYCLES 22 AND 23</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>Ebert, R. W.; Dayeh, M. A.; Desai, M. I.</p> <p>2013-05-10</p> <p>We examined <span class="hlt">solar</span> wind plasma and interplanetary magnetic field (IMF) <span class="hlt">observations</span> from Ulysses' first and third orbits to study hemispheric differences in the properties of the <span class="hlt">solar</span> wind and IMF originating from the Sun's large polar coronal holes (PCHs) during the declining and minimum phase of <span class="hlt">solar</span> cycles 22 and 23. We identified hemispheric asymmetries in several parameters, most notably {approx}15%-30% south-to-north differences in averages for the <span class="hlt">solar</span> wind density, mass flux, dynamic pressure, and energy flux and the radial and total IMF magnitudes. These differences were driven by relatively larger, more variable <span class="hlt">solar</span> wind density and radial IMF betweenmore » {approx}36 Degree-Sign S-60 Degree-Sign S during the declining phase of <span class="hlt">solar</span> cycles 22 and 23. These <span class="hlt">observations</span> indicate either a hemispheric asymmetry in the PCH output during the declining and minimum phase of <span class="hlt">solar</span> cycles 22 and 23 with the southern hemisphere being more active than its northern counterpart, or a <span class="hlt">solar</span> cycle effect where the PCH output in both hemispheres is enhanced during periods of higher <span class="hlt">solar</span> activity. We also report a strong linear correlation between these <span class="hlt">solar</span> wind and IMF parameters, including the periods of enhanced PCH output, that highlight the connection between the <span class="hlt">solar</span> wind mass and energy output and the Sun's magnetic field. That these enhancements were not matched by similar sized variations in <span class="hlt">solar</span> wind speed points to the mass and energy responsible for these increases being added to the <span class="hlt">solar</span> wind while its flow was subsonic.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001079.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001079.html"><span>A First for NASA's IRIS: <span class="hlt">Observing</span> a Gigantic Eruption of <span class="hlt">Solar</span> Material</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2014-05-30</p> <p>Watch a video from this event here: www.flickr.com/photos/gsfc/14118958800/ A coronal mass ejection, or CME, surged off the side of the sun on May 9, 2014, and NASA's newest <span class="hlt">solar</span> observatory caught it in extraordinary detail. This was the first CME <span class="hlt">observed</span> by the Interface Region Imaging Spectrograph, or IRIS, which launched in June 2013 to peer into the lowest levels of the sun's atmosphere with better resolution than ever before. Watch the movie to see how a curtain of <span class="hlt">solar</span> material erupts outward at speeds of 1.5 million miles per hour. Read more: 1.usa.gov/1kp7O4F NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=installing+AND+solar&id=ED215189','ERIC'); return false;" href="https://eric.ed.gov/?q=installing+AND+solar&id=ED215189"><span><span class="hlt">Solar</span> Heating <span class="hlt">Systems</span>: Student Manual.</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>Green, Joanne; And Others</p> <p></p> <p>This Student Manual for a <span class="hlt">Solar</span> Heating <span class="hlt">System</span> curriculum contains 22 units of instructional materials for students to use in a course or courses on <span class="hlt">solar</span> heating <span class="hlt">systems</span> (see note). For each unit (task), objectives, assignment sheets, laboratory assignments, information sheets, checkpoints (tests), and job sheets are provided. Materials are set…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19970031744&hterms=solar+intensity+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsolar%2Bintensity%2Bmeasurement','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19970031744&hterms=solar+intensity+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsolar%2Bintensity%2Bmeasurement"><span>Spacecraft Radio Scintillation and <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Woo, Richard</p> <p>1993-01-01</p> <p>When a wave propagates through a turbulent medium, scattering by the random refractive index inhomogeneities can lead to a wide variety of phenomena that have been the subject of extensive study. The <span class="hlt">observed</span> scattering effects include amplitude or intensity scintillation, phase scintillation, angular broadening, and spectral broadening, among others. In this paper, I will refer to these scattering effects collectively as scintillation. Although the most familiar example is probably the twinkling of stars (light wave intensity scintillation by turbulence in the Earth's atmosphere), scintillation has been encountered and investigated in such diverse fields as ionospheric physics, oceanography, radio astronomy, and radio and optical communications. Ever since planetary spacecraft began exploring the <span class="hlt">solar</span> <span class="hlt">system</span>, scintillation has appeared during the propagation of spacecraft radio signals through planetary atmospheres, planetary ionospheres, and the <span class="hlt">solar</span> wind. Early studies of these phenomena were motivated by the potential adverse effects on communications and navigation, and on experiments that use the radio link to conduct scientific investigations. Examples of the latter are radio occultation measurements (described below) of planetary atmospheres to deduce temperature profiles, and the search for gravitational waves. However,these concerns soon gave way to the emergence of spacecraft radio scintillation as a new scientific tool for exploring small-scale dynamics in planetary atmospheres and structure in the <span class="hlt">solar</span> wind, complementing in situ and other remote sensing spacecraft measurements, as well as scintillation measurements using natural (celestial) radio sources. The purpose of this paper is to briefly describe and review the <span class="hlt">solar</span> <span class="hlt">system</span> spacecraft radio scintillation <span class="hlt">observations</span>, to summarize the salient features of wave propagation analyses employed in interpreting them, to underscore the unique remote sensing capabilities and scientific relevance of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15791734','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15791734"><span><span class="hlt">Solar</span> particle events <span class="hlt">observed</span> at Mars: dosimetry measurements and model calculations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cleghorn, Timothy F; Saganti, Premkumar B; Zeitlin, Cary J; Cucinotta, Francis A</p> <p>2004-01-01</p> <p>During the period from March 13, 2002 to mid-September, 2002, six <span class="hlt">solar</span> particle events (SPE) were <span class="hlt">observed</span> by the MARIE instrument onboard the Odyssey Spacecraft in Martian Orbit. These events were <span class="hlt">observed</span> also by the GOES 8 satellite in Earth orbit, and thus represent the first time that the same SPE have been <span class="hlt">observed</span> at these separate locations. The characteristics of these SPE are examined, given that the active regions of the <span class="hlt">solar</span> disc from which the event originated can usually be identified. The dose rates at Martian orbit are calculated, both for the galactic and <span class="hlt">solar</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050164094&hterms=caries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dcaries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050164094&hterms=caries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dcaries"><span><span class="hlt">Solar</span> particle events <span class="hlt">observed</span> at Mars: dosimetry measurements and model calculations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cleghorn, Timothy F.; Saganti, Premkumar B.; Zeitlin, Cary J.; Cucinotta, Francis A.</p> <p>2004-01-01</p> <p>During the period from March 13, 2002 to mid-September, 2002, six <span class="hlt">solar</span> particle events (SPE) were <span class="hlt">observed</span> by the MARIE instrument onboard the Odyssey Spacecraft in Martian Orbit. These events were <span class="hlt">observed</span> also by the GOES 8 satellite in Earth orbit, and thus represent the first time that the same SPE have been <span class="hlt">observed</span> at these separate locations. The characteristics of these SPE are examined, given that the active regions of the <span class="hlt">solar</span> disc from which the event originated can usually be identified. The dose rates at Martian orbit are calculated, both for the galactic and <span class="hlt">solar</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ASPC..500...43P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ASPC..500...43P"><span>Preparing for and <span class="hlt">Observing</span> the 2017 Total <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, J.</p> <p>2015-11-01</p> <p>I discuss ongoing plans and discussions for EPO and scientific <span class="hlt">observing</span> of the 21 August 2017 total <span class="hlt">solar</span> eclipse. I discuss aspects of EPO based on my experiences at the 60 <span class="hlt">solar</span> eclipses I have seen. I share cloud statistics along the eclipse path compiled by Jay Anderson, the foremost eclipse meteorologist. I show some sample <span class="hlt">observations</span> of composite imagery, of spectra, and of terrestrial temperature changes based on <span class="hlt">observations</span> of recent eclipses, including 2012 from Australia and 2013 from Gabon. Links to various mapping sites of totality, partial phases, and other eclipse-related information, including that provided by Michael Zeiler, Fred Espenak (retired from NASA) and Xavier Jubier can be found on the website I run for the International Astronomical Union's Working Group on Eclipses at http://www.eclipses.info.</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 <span class="hlt">Solar</span> Radiation by Clouds: <span class="hlt">Observations</span> Versus Models</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 <span class="hlt">solar</span> radiation by clouds. Collocated satellite and surface measurements of <span class="hlt">solar</span> radiation at five geographically diverse locations showed significant <span class="hlt">solar</span> absorption by clouds, resulting in about 25 watts per square meter more global-mean absorption by the cloudy atmosphere than predicted by theoretical models. 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('http://hdl.handle.net/2060/19720005143','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720005143"><span><span class="hlt">Solar</span> electric propulsion <span class="hlt">system</span> technology</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Masek, T. D.; Macie, T. W.</p> <p>1971-01-01</p> <p>Achievements in the <span class="hlt">solar</span> electric propulsion <span class="hlt">system</span> technology program (SEPST 3) are reported and certain propulsion <span class="hlt">system</span>-spacecraft interaction problems are discussed. The basic <span class="hlt">solar</span> electric propulsion <span class="hlt">system</span> concept and elements are reviewed. Hardware is discussed only briefly, relying on detailed fabrication or assembly descriptions reported elsewhere. Emphasis is placed on recent performance data, which are presented to show the relationship between spacecraft requirements and present technology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMSH33A2035S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMSH33A2035S"><span>Radio Imaging <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Activity Cycle and Its Anomaly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shibasaki, K.</p> <p>2011-12-01</p> <p>The 24th <span class="hlt">solar</span> activity cycle has started and relative sunspot numbers are increasing. However, their rate of increase is rather slow compared to previous cycles. Active region sizes are small, lifetime is short, and big (X-class) flares are rare so far. We study this anomalous situation using data from Nobeyama Radioheliograph (NoRH). Radio imaging <span class="hlt">observations</span> have been done by NoRH since 1992. Nearly 20 years of daily radio images of the Sun at 17 GHz are used to synthesize a radio butterfly diagram. Due to stable operation of the instrument and a robust calibration method, uniform datasets are available covering the whole period of <span class="hlt">observation</span>. The radio butterfly diagram shows bright features corresponding to active region belts and their migration toward low latitude as the <span class="hlt">solar</span> cycle progresses. In the present <span class="hlt">solar</span> activity cycle (24), increase of radio brightness is delayed and slow. There are also bright features around both poles (polar brightening). Their brightness show <span class="hlt">solar</span> cycle dependence but peaks around <span class="hlt">solar</span> minimum. Comparison between the last minimum and the previous one shows decrease of its brightness. This corresponds to weakening of polar magnetic field activity between them. In the northern pole, polar brightening is already weakened in 2011, which means it is close to <span class="hlt">solar</span> maximum in the northern hemisphere. Southern pole does not show such feature yet. Slow rise of activity in active region belt, weakening of polar activity during the minimum, and large north-south asymmetry in polar activity imply that global <span class="hlt">solar</span> activity and its synchronization are weakening.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title24-vol2/pdf/CFR-2013-title24-vol2-sec203-18a.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title24-vol2/pdf/CFR-2013-title24-vol2-sec203-18a.pdf"><span>24 CFR 203.18a - <span class="hlt">Solar</span> energy <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-04-01</p> <p>... 24 Housing and Urban Development 2 2013-04-01 2013-04-01 false <span class="hlt">Solar</span> energy <span class="hlt">system</span>. 203.18a... § 203.18a <span class="hlt">Solar</span> energy <span class="hlt">system</span>. (a) The dollar limitation provided in § 203.18(a) may be increased by up... to the installation of a <span class="hlt">solar</span> energy <span class="hlt">system</span>. (b) <span class="hlt">Solar</span> energy <span class="hlt">system</span> is defined as any addition...</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('https://www.gpo.gov/fdsys/pkg/CFR-2014-title24-vol2/pdf/CFR-2014-title24-vol2-sec203-18a.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title24-vol2/pdf/CFR-2014-title24-vol2-sec203-18a.pdf"><span>24 CFR 203.18a - <span class="hlt">Solar</span> energy <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-04-01</p> <p>... 24 Housing and Urban Development 2 2014-04-01 2014-04-01 false <span class="hlt">Solar</span> energy <span class="hlt">system</span>. 203.18a... § 203.18a <span class="hlt">Solar</span> energy <span class="hlt">system</span>. (a) The dollar limitation provided in § 203.18(a) may be increased by up... to the installation of a <span class="hlt">solar</span> energy <span class="hlt">system</span>. (b) <span class="hlt">Solar</span> energy <span class="hlt">system</span> is defined as any addition...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title24-vol2/pdf/CFR-2012-title24-vol2-sec203-18a.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title24-vol2/pdf/CFR-2012-title24-vol2-sec203-18a.pdf"><span>24 CFR 203.18a - <span class="hlt">Solar</span> energy <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-04-01</p> <p>... 24 Housing and Urban Development 2 2012-04-01 2012-04-01 false <span class="hlt">Solar</span> energy <span class="hlt">system</span>. 203.18a... § 203.18a <span class="hlt">Solar</span> energy <span class="hlt">system</span>. (a) The dollar limitation provided in § 203.18(a) may be increased by up... to the installation of a <span class="hlt">solar</span> energy <span class="hlt">system</span>. (b) <span class="hlt">Solar</span> energy <span class="hlt">system</span> is defined as any addition...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title24-vol2/pdf/CFR-2010-title24-vol2-sec203-18a.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title24-vol2/pdf/CFR-2010-title24-vol2-sec203-18a.pdf"><span>24 CFR 203.18a - <span class="hlt">Solar</span> energy <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-04-01</p> <p>... 24 Housing and Urban Development 2 2010-04-01 2010-04-01 false <span class="hlt">Solar</span> energy <span class="hlt">system</span>. 203.18a... § 203.18a <span class="hlt">Solar</span> energy <span class="hlt">system</span>. (a) The dollar limitation provided in § 203.18(a) may be increased by up... to the installation of a <span class="hlt">solar</span> energy <span class="hlt">system</span>. (b) <span class="hlt">Solar</span> energy <span class="hlt">system</span> is defined as any addition...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title24-vol2/pdf/CFR-2011-title24-vol2-sec203-18a.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title24-vol2/pdf/CFR-2011-title24-vol2-sec203-18a.pdf"><span>24 CFR 203.18a - <span class="hlt">Solar</span> energy <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-04-01</p> <p>... 24 Housing and Urban Development 2 2011-04-01 2011-04-01 false <span class="hlt">Solar</span> energy <span class="hlt">system</span>. 203.18a... § 203.18a <span class="hlt">Solar</span> energy <span class="hlt">system</span>. (a) The dollar limitation provided in § 203.18(a) may be increased by up... to the installation of a <span class="hlt">solar</span> energy <span class="hlt">system</span>. (b) <span class="hlt">Solar</span> energy <span class="hlt">system</span> is defined as any addition...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011SPD....42.1903C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011SPD....42.1903C"><span>Tiny Pores <span class="hlt">Observed</span> by New <span class="hlt">Solar</span> Telescope and Hinode</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cho, KyungSuk; Bong, S.; Chae, J.; Kim, Y.; Park, Y.; Ahn, K.; Katsukawa, Y.</p> <p>2011-05-01</p> <p>Seoul National University and Korea Astronomy and Space Science Institute installed Fast Imaging <span class="hlt">Solar</span> Spectrograph (FISS) in the Cude room of the 1.6 m New <span class="hlt">Solar</span> Telescope (NST) at Big Bear <span class="hlt">Solar</span> Observatory on May 14, 2010. FISS is a unique <span class="hlt">system</span> that can do imaging of H-alpha and Ca II 8542 band simultaneously, which is quite suitable for studying of dynamics of chromosphere. To investigate the relationship between the photospheric and low-chromospheric motions at the pore region, we took a coordinate <span class="hlt">observation</span> with NST/FISS and Hinode/SOT for new emerging active region (AR11117) on October 26, 2010. In the <span class="hlt">observed</span> region, we could find two tiny pores and two small magnetic concentrations (SMCs), which have similar magnetic flux with the pores but do not look dark. Magnetic flux density and Doppler velocities at the photosphere are estimated by applying the center-of-gravity (COG) method to the HINODE/spectropolarimeter (SP) data. The line-of-sight motions above the photosphere are determined by adopting the bisector method to the wing spectra of Ha and CaII 8542 lines. As results, we found the followings. (1)There are upflow motion on the pores and downflow motion on the SMCs. (2)Towards the CaII 8542 line center, upflow motion decrease and turn to downward motion in pores, while the speed of down flow motion increases in the SMCs. (3)There is oscillating motion above pores and the SMCs, and this motion keep its pattern along the height. (4) As height increase, there is a general tendency of the speed shift to downward on pores and the SMCs. In this poster, we will present preliminary understanding of the coupling of pore dynamics between the photosphere and the low-chromosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P13A1901L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P13A1901L"><span><span class="hlt">Solar</span> Wind Interaction and Crustal Field Influences on Mars' Upper Ionosphere: MAVEN <span class="hlt">Observations</span> Compared to Model Results</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luhmann, J. G.; Alvarez, K.; Curry, S.; Dong, C.; Ma, Y.; Bougher, S. W.; Benna, M.; Elrod, M. K.; Mahaffy, P. R.; Withers, P.; Girazian, Z.; Connerney, J. E. P.; Brain, D.; Jakosky, B. M.</p> <p>2016-12-01</p> <p>Since the two Viking Landers, progress on improving our global knowledge of the Martian ionosphere's characteristics has been limited by the available instrumentation and sampling geometries. In particular, while remote sensing and the lower energy plasma spectrometer <span class="hlt">observations</span> on missions including MGS and MEX provided insights on the effects of the crustal magnetic fields of Mars and the <span class="hlt">solar</span> wind interaction, these measurements did not allow the broader thermal ion surveys necessary to test our current understanding of the region between the exobase at 200 km altitude and the <span class="hlt">solar</span> wind interaction boundary. In this study we use the MAVEN NGIMS thermal ion mass spectrometer <span class="hlt">observations</span> from the prime mission year 2015 to construct some statistical pictures of the increasingly collisionless region of the ionosphere between 200 and 500 km where crustal field and <span class="hlt">solar</span> wind interaction effects should begin to dominate its behavior. Comparisons with models of the <span class="hlt">solar</span> wind interaction with Mars provide important global context for these <span class="hlt">observations</span>, including the roles of <span class="hlt">system</span> diversity associated with changing crustal field and interplanetary field orientations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5766751-solar-converter-system-thermal-overload-protection','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5766751-solar-converter-system-thermal-overload-protection"><span><span class="hlt">Solar</span> converter <span class="hlt">system</span> with thermal overload protection</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>Popovich, J.M.; Thornbury, T.R.</p> <p>1979-10-02</p> <p>A <span class="hlt">solar</span> energy conversion <span class="hlt">system</span> comprises: (a) a <span class="hlt">solar</span> converter in which liquid absorbs <span class="hlt">solar</span> radiation, the liquid being <span class="hlt">solar</span> energy absorptive; (b) first means to circulate said liquid for flow through the converter; and (c) means to effect removal of liquid from the converter in response to an undesirable operation condition in said <span class="hlt">system</span>. 12 claims.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970034981','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970034981"><span>Fragmentary <span class="hlt">Solar</span> <span class="hlt">System</span> History</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marti, Kurt</p> <p>1997-01-01</p> <p>The objective of this research is an improved understanding of the early <span class="hlt">solar</span> <span class="hlt">system</span> environment and of the processes involved in the nebula and in the evolution of solid bodies. We present results of our studies on the isotopic signatures in selected primitive <span class="hlt">solar</span> <span class="hlt">system</span> objects and on the evaluation of the cosmic ray records and of inferred collisional events. Furthermore, we report data of trapped martian atmospheric gases in meteorites and the inferred early evolution of Mars' atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007DPS....39.2805S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007DPS....39.2805S"><span>Scientific Investigation of the Jovian <span class="hlt">System</span>: the Jupiter <span class="hlt">System</span> <span class="hlt">Observer</span> Mission Concept</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Spilker, Thomas R.; Senske, D. A.; Prockter, L.; Kwok, J. H.; Tan-Wang, G. H.; SDT, JSO</p> <p>2007-10-01</p> <p>NASA's Science Mission Directorate (SMD), in efforts to start an outer <span class="hlt">solar</span> <span class="hlt">system</span> flagship mission in the near future, commissioned studies of mission concepts for four high-priority outer <span class="hlt">solar</span> <span class="hlt">system</span> destinations: Europa, the Jovian <span class="hlt">system</span>, Titan, and Enceladus. Our team has identified and evaluated science and mission architectures to investigate major elements of the Jovian <span class="hlt">system</span>: Jupiter, the Galilean moons, rings, and magnetosphere, and their interactions. SMD dubbed the mission concept the "Jupiter <span class="hlt">System</span> <span class="hlt">Observer</span> (JSO)." At abstract submission this JPL-led study is nearly complete, with final report submission in August 2007. SMD intends to select a subset of these four concepts for additional detailed study, leading to a potential flagship mission new start. A rich set of science objectives that JSO can address quite well have been identified. The highly capable science payload (including 50-cm optic), an extensive tour with multiple close flybys of Io, Europa, Ganymede and Callisto, and a significant time in orbit at Ganymede, addresses a large set of <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Decadal Survey (2003) and NASA <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Roadmap (2006) high-priority objectives. With the engineering team, the Science Definition Team evaluated a suite of mission architectures and the science they enable to arrive at two architectures that provide the best science for their estimated mission costs. This paper discusses the science objectives and operational capabilities and considerations for these mission concepts. This work was performed at JPL, APL, and other institutions under contract to NASA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22519953-new-horizons-solar-wind-around-pluto-swap-observations-solar-wind-from-au','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22519953-new-horizons-solar-wind-around-pluto-swap-observations-solar-wind-from-au"><span>THE NEW HORIZONS <span class="hlt">SOLAR</span> WIND AROUND PLUTO (SWAP) <span class="hlt">OBSERVATIONS</span> OF THE <span class="hlt">SOLAR</span> WIND FROM 11–33 au</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>Elliott, H. A.; McComas, D. J.; Valek, P.</p> <p></p> <p>The <span class="hlt">Solar</span> Wind Around Pluto (SWAP) instrument on National Aeronautics and Space Administration's New Horizons Pluto mission has collected <span class="hlt">solar</span> wind <span class="hlt">observations</span> en route from Earth to Pluto, and these <span class="hlt">observations</span> continue beyond Pluto. Few missions have explored the <span class="hlt">solar</span> wind in the outer heliosphere making this dataset a critical addition to the field. We created a forward model of SWAP count rates, which includes a comprehensive instrument response function based on laboratory and flight calibrations. By fitting the count rates with this model, the proton density (n), speed (V), and temperature (T) parameters are determined. Comparisons between SWAP parametersmore » and both propagated 1 au <span class="hlt">observations</span> and prior Voyager 2 <span class="hlt">observations</span> indicate consistency in both the range and mean wind values. These comparisons as well as our additional findings confirm that small and midsized <span class="hlt">solar</span> wind structures are worn down with increasing distance due to dynamic interaction of parcels of wind with different speed. For instance, the T–V relationship steepens, as the range in V is limited more than the range in T with distance. At times the T–V correlation clearly breaks down beyond 20 au, which may indicate wind currently expanding and cooling may have an elevated T reflecting prior heating and compression in the inner heliosphere. The power of wind parameters at shorter periodicities decreases with distance as the longer periodicities strengthen. The <span class="hlt">solar</span> rotation periodicity is present in temperature beyond 20 au indicating the <span class="hlt">observed</span> parcel temperature may reflect not only current heating or cooling, but also heating occurring closer to the Sun.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010018997','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010018997"><span>Spacewatch Survey of the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McMillan, Robert S.</p> <p>2000-01-01</p> <p>The purpose of the Spacewatch project is to explore the various populations of small objects throughout the <span class="hlt">solar</span> <span class="hlt">system</span>. Statistics on all classes of small bodies are needed to infer their physical and dynamical evolution. More Earth Approachers need to be found to assess the impact hazard. (We have adopted the term "Earth Approacher", EA, to include all those asteroids, nuclei of extinct short period comets, and short period comets that can approach close to Earth. The adjective "near" carries potential confusion, as we have found in communicating with the media, that the objects are always near Earth, following it like a cloud.) Persistent and voluminous accumulation of astrometry of incidentally <span class="hlt">observed</span> main belt asteroids MBAs will eventually permit the Minor Planet Center (MPQ to determine the orbits of large numbers (tens of thousands) of asteroids. Such a large body of information will ultimately allow better resolution of orbit classes and the determinations of luminosity functions of the various classes, Comet and asteroid recoveries are essential services to planetary astronomy. Statistics of objects in the outer <span class="hlt">solar</span> <span class="hlt">system</span> (Centaurs, scattered-disk objects, and Trans-Neptunian Objects; TNOs) ultimately will tell part of the story of <span class="hlt">solar</span> <span class="hlt">system</span> evolution. Spacewatch led the development of sky surveying by electronic means and has acted as a responsible interface to the media and general public on this discipline and on the issue of the hazard from impacts by asteroids and comets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8448E..0AK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8448E..0AK"><span>Optimisation of <span class="hlt">solar</span> synoptic <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>Klvaña, Miroslav; Sobotka, Michal; Švanda, Michal</p> <p>2012-09-01</p> <p>The development of instrumental and computer technologies is connected with steadily increasing needs for archiving of large data volumes. The current trend to meet this requirement includes the data compression and growth of storage capacities. This approach, however, has technical and practical limits. A further reduction of the archived data volume can be achieved by means of an optimisation of the archiving that consists in data selection without losing the useful information. We describe a method of optimised archiving of <span class="hlt">solar</span> images, based on the selection of images that contain a new information. The new information content is evaluated by means of the analysis of changes detected in the images. We present characteristics of different kinds of image changes and divide them into fictitious changes with a disturbing effect and real changes that provide a new information. In block diagrams describing the selection and archiving, we demonstrate the influence of clouds, the recording of images during an active event on the Sun, including a period before the event onset, and the archiving of long-term history of <span class="hlt">solar</span> activity. The described optimisation technique is not suitable for helioseismology, because it does not conserve the uniform time step in the archived sequence and removes the information about <span class="hlt">solar</span> oscillations. In case of long-term synoptic <span class="hlt">observations</span>, the optimised archiving can save a large amount of storage capacities. The actual capacity saving will depend on the setting of the change-detection sensitivity and on the capability to exclude the fictitious changes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH24A..02H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH24A..02H"><span>The Unique Scientific Assets of Multi-Wavelength Total <span class="hlt">Solar</span> Eclipse <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>Habbal, S. R.; Druckmuller, M.; Ding, A.</p> <p>2017-12-01</p> <p>Total <span class="hlt">solar</span> eclipses continue to yield new discoveries regarding the dynamics and thermodynamics of the corona, due to the radial span of the field of view available during totality, starting from the <span class="hlt">solar</span> surface out to several <span class="hlt">solar</span> radii, and due to the diagnostic potential provided by coronal emission lines. Scientific highlights from past eclipse <span class="hlt">observations</span> as well as from the 21 August 2017 eclipse, now spanning a <span class="hlt">solar</span> cycle, will be presented. These include white light and spectral line imaging as well as imaging spectrometry. Emphasis will be placed on the unique insights into the origin of dynamic structures captured in eclipse images, and the temperature distribution in the corona derived from these eclipse <span class="hlt">observations</span>. Implications of these results for the general problem of coronal heating, as well as for the next generation of space instrumentation will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840005044','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840005044"><span>Iron charge states <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ipavich, F. M.; Galvin, A. B.; Gloeckler, G.; Hovestadt, D.; Klecker, B.; Scholer, M.</p> <p>1983-01-01</p> <p><span class="hlt">Solar</span> wind measurements from the ULECA sensor of the Max-Planck-Institut/University of Maryland experiment on ISEE-3 are reported. The low energy section of approx the ULECA sensor selects particles by their energy per charge (over the range 3.6 keV/Q to 30 keV/Q) and simultaneously measures their total energy with two low-noise solid state detectors. <span class="hlt">Solar</span> wind Fe charge state measurements from three time periods of high speed <span class="hlt">solar</span> wind occurring during a post-shock flow and a coronal hole-associated high speed stream are presented. Analysis of the post-shock flow <span class="hlt">solar</span> wind indicates the charge state distributions for Fe were peaked at approx +16, indicative of an unusually high coronal temperature (3,000,000 K). In contrast, the Fe charge state distribution <span class="hlt">observed</span> in a coronal hole-associated high speed stream peaks at approx -9, indicating a much lower coronal temperature (1,400,000 K). This constitutes the first reported measurements of iron charge states in a coronal hole-associated high speed stream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19750044107&hterms=effect+global+warming&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Deffect%2Bglobal%2Bwarming','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19750044107&hterms=effect+global+warming&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Deffect%2Bglobal%2Bwarming"><span>Recent advances in satellite <span class="hlt">observations</span> of <span class="hlt">solar</span> variability and global atmospheric ozone</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heath, D. F.</p> <p>1974-01-01</p> <p>A description is given of the temporal behavior of the sun as an ultraviolet variable star in relation to daily zonal means of atmospheric ozone from the total amount to that above the 10-mb and 4-mb pressure levels. A significant correlation has been <span class="hlt">observed</span> between enhancements in the ultraviolet <span class="hlt">solar</span> irradiances and terrestrial passages of the <span class="hlt">solar</span> magnetic field sector boundary structure. However, it has not yet been possible to separate <span class="hlt">solar</span> from the dynamical effects on the variability in the zonal means of ozone. Attention is given to global changes in ozone which have been derived from the satellite <span class="hlt">observations</span> in terms of season, <span class="hlt">solar</span> variability, and major stratospheric disturbances such as stratospheric warmings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Solar+AND+system&id=EJ876099','ERIC'); return false;" href="https://eric.ed.gov/?q=Solar+AND+system&id=EJ876099"><span>Wind in the <span class="hlt">Solar</span> <span class="hlt">System</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>McIntosh, Gordon</p> <p>2010-01-01</p> <p>As an astronomy instructor I am always looking for commonly experienced Earthly phenomena to help my students and me understand and appreciate similar occurrences elsewhere in the <span class="hlt">solar</span> <span class="hlt">system</span>. Recently I wrote short "TPT" articles on frost and precipitation. The present article is on winds in the <span class="hlt">solar</span> <span class="hlt">system</span>. A windy day or storm might…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=solar+AND+two&pg=5&id=ED215187','ERIC'); return false;" href="https://eric.ed.gov/?q=solar+AND+two&pg=5&id=ED215187"><span><span class="hlt">Solar</span> Heating <span class="hlt">Systems</span>: Instructor's Guide.</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>Green, Joanne; And Others</p> <p></p> <p>This Instructor's Guide for a <span class="hlt">Solar</span> Heating <span class="hlt">System</span> Curriculum is designed to accompany the Student Manual and the Progress Checks and Test Manual for the course (see note), in order to facilitate the instruction of classes on <span class="hlt">solar</span> heating <span class="hlt">systems</span>. The Instructor's Guide contains a variety of materials used in teaching the courses, including…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030011518&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsolar%2Bradiation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030011518&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsolar%2Bradiation"><span>Comparison of ScaRaB, GOES 8, Aircraft, and Surface <span class="hlt">Observations</span> of the Absorption of <span class="hlt">Solar</span> Radiation by Clouds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pope, Shelly K.; Valero, Francisco P. J.; Collins, William D.; Minnis, Patrick</p> <p>2002-01-01</p> <p>Data obtained by the Scanner for Radiation Budget (ScaRaB) instrument on the Meteor 3 satellite have been analyzed and compared to satellite (GOES 8), aircraft (Radiation Measurement <span class="hlt">System</span>, RAMS), and surface (Baseline <span class="hlt">Solar</span> Radiation Network (BSRN), <span class="hlt">Solar</span> and Infrared <span class="hlt">Observations</span> <span class="hlt">System</span> (SIROS), and RAMS) measurements of irradiance obtained during the Atmospheric Radiation Measurements Enhanced Shortwave Experiment (ARESE). It is found that the ScaRaB data covering the period from March 1994 to February 1995 (the instrument's operational lifetime) indicate excess absorption of <span class="hlt">solar</span> radiation by the cloudy atmosphere in agreement with previous aircraft, surface, and GOES 8 results. The full ScaRaB data set combined with BSRN and SIROS surface <span class="hlt">observations</span> gives an average all-sky absorptance of 0.28. The GOES 8 data set combined with RAMS surface <span class="hlt">observations</span> gives an average all-sky absorptance of 0.26. The aircraft data set (RAMS) gives a mean all-sky absorptance of 0.24 (for the column between 0.5 and 13 km).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1980dspe.rept.....K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1980dspe.rept.....K"><span>Decentralized <span class="hlt">solar</span> photovoltaic energy <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krupka, M. C.</p> <p>1980-09-01</p> <p>Emphasis was placed upon the selection and use of a model residential photovoltaic <span class="hlt">system</span> to develop and quantify the necessary data. The model consists of a reference home located in Phoenix, AZ utilizing a unique <span class="hlt">solar</span> cell array roof shingle combination. Silicon <span class="hlt">solar</span> cells, rated at 13.5 percent efficiency at 28 C and 100 mW/sq cm insolation are used to generate 10 kW (peak). An all electric home is considered with lead acid battery storage, DC AC inversion and utility backup. The reference home is compared to others in regions of different insolation. It is suggested that <span class="hlt">solar</span> cell materials production and fabrication may have the major environmental impact when comparing all facets of photovoltaic <span class="hlt">system</span> usage. Fabrication of the various types of <span class="hlt">solar</span> cell <span class="hlt">systems</span> involves the need, handling, and transportation of many toxic and hazardous chemicals with attendant health and safety impacts. Increases in production of such materials as lead, antimony, sulfuric acid, copper, plastics, cadmium and gallium will be required should large scale usage of photovoltaic <span class="hlt">systems</span> be implemented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AcAau..95..210S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AcAau..95..210S"><span>An innovative deployable <span class="hlt">solar</span> panel <span class="hlt">system</span> for Cubesats</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Santoni, Fabio; Piergentili, Fabrizio; Donati, Serena; Perelli, Massimo; Negri, Andrea; Marino, Michele</p> <p>2014-02-01</p> <p>One of the main Cubesat bus limitations is the available on-board power. The maximum power obtained using body mounted <span class="hlt">solar</span> panels and advanced triple junction <span class="hlt">solar</span> cells on a triple unit Cubesat is typically less than 10 W. The Cubesat performance and the mission scenario opened to these small satellite <span class="hlt">systems</span> could be greatly enhanced by an increase of the available power. This paper describes the design and realization of a modular deployable <span class="hlt">solar</span> panel <span class="hlt">system</span> for Cubesats, consisting of a modular hinge and spring <span class="hlt">system</span> that can be potentially used on-board single (1U), double(2U), triple (3U) and six units (6U) Cubesats. The size of each <span class="hlt">solar</span> panels is the size of a lateral Cubesat surface. The <span class="hlt">system</span> developed is the basis for a SADA (<span class="hlt">Solar</span> Array Drive Assembly), in which a maneuvering capability is added to the deployed <span class="hlt">solar</span> array in order to follow the apparent motion of the sun. The <span class="hlt">system</span> design trade-off is discussed, comparing different deployment concepts and architectures, leading to the final selection for the modular design. A prototype of the <span class="hlt">system</span> has been realized for a 3U Cubesat, consisting of two deployable <span class="hlt">solar</span> panel <span class="hlt">systems</span>, made of three <span class="hlt">solar</span> panels each, for a total of six deployed <span class="hlt">solar</span> panels. The deployment <span class="hlt">system</span> is based on a plastic fiber wire and thermal cutters, guaranteeing a suitable level of reliability. A test-bed for the <span class="hlt">solar</span> panel deployment testing has been developed, supporting the <span class="hlt">solar</span> array during deployment reproducing the dynamical situation in orbit. The results of the deployment <span class="hlt">system</span> testing are discussed, including the design and realization of the test-bed, the mechanical stress given to the <span class="hlt">solar</span> cells by the deployment accelerations and the overall <span class="hlt">system</span> performance. The maximum power delivered by the <span class="hlt">system</span> is about 50.4 W BOL, greatly enhancing the present Cubesat <span class="hlt">solar</span> array performance.</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('http://hdl.handle.net/2060/19750016559','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750016559"><span>Jupiter: Giant of the <span class="hlt">solar</span> <span class="hlt">system</span>. [its <span class="hlt">solar</span> orbits</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1975-01-01</p> <p>Jupiter, its relationship to the other planets in the <span class="hlt">solar</span> <span class="hlt">system</span>, its twelve natural satellites, <span class="hlt">solar</span> orbit and the appearance of Jupiter in the sky, and the sightings and motions of Jupiter in 1973 are discussed. Educational study projects for students are also included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23230304W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23230304W"><span>Modeling Jovian Magnetospheres Beyond the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Williams, Peter K. G.</p> <p>2018-06-01</p> <p>Low-frequency radio <span class="hlt">observations</span> are believed to represent one of the few means of directly probing the magnetic fields of extrasolar planets. However, a half-century of low-frequency planetary <span class="hlt">observations</span> within the <span class="hlt">Solar</span> <span class="hlt">System</span> demonstrate that detailed, physically-motivated magnetospheric models are needed to properly interpret the radio data. I will present recent work in this area focusing on the current state of the art: relatively high-frequency <span class="hlt">observations</span> of relatively massive objects, which are now understood to have magnetospheres that are largely planetary in nature. I will highlight the key challenges that will arise in future space-based <span class="hlt">observations</span> of lower-mass objects at lower frequencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005MSAIS...6...34F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005MSAIS...6...34F"><span>Alenia Spazio: Space Programs for <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration .</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferri, A.</p> <p></p> <p>Alenia Spazio is the major Italian space industry and one of the largest in Europe, with 2,400 highly skilled employees and 16,000 square meters of clean rooms and laboratories for advanced technological research that are among the most modern and well-equipped in Europe. The company has wide experience in the design, development, assembly, integration, verification and testing of complete space <span class="hlt">systems</span>: satellites for telecommunications and navigation, remote sensing, meteorology and scientific applications; manned <span class="hlt">systems</span> and space infrastructures; launch, transport and re-entry <span class="hlt">systems</span>, and control centres. Alenia Spazio has contributed to the construction of over 200 satellites and taken part in the most important national and international space programmes, from the International Space Station to the new European global navigation <span class="hlt">system</span> Galileo. Focusing on <span class="hlt">Solar</span> <span class="hlt">System</span> exploration, in the last 10 years the Company took part, with different roles, to the major European and also NASA missions in the field: Rosetta, Mars Express, Cassini; will soon take part in Venus Express, and is planning the future with Bepi Colombo, <span class="hlt">Solar</span> Orbiter, GAIA and Exomars. In this paper, as in the presentation, a very important Earth <span class="hlt">Observation</span> mission is also presented: GOCE. All in all, the Earth is by all means part of the <span class="hlt">Solar</span> <span class="hlt">system</span> as well and we like to see it as a planet to be explored.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P54C..05K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P54C..05K"><span>Correlating <span class="hlt">Solar</span> Wind Modulation with Ionospheric Variability at Mars from MEX and 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>Kopf, A. J.; Morgan, D. D.; Halekas, J. S.; Ruhunusiri, S.; Gurnett, D. A.; Connerney, J. E. P.</p> <p>2017-12-01</p> <p>The synthesis of <span class="hlt">observations</span> by the Mars Express and Mars Atmosphere and Volatiles Evolution (MAVEN) spacecraft allows for a unique opportunity to study variability in the Martian ionosphere from multiple perspectives. One major source for this variability is the <span class="hlt">solar</span> wind. Due to its elliptical orbit which precesses over time, MAVEN periodically spends part of its orbit outside the Martian bow shock, allowing for direct measurements of the <span class="hlt">solar</span> wind impacting the Martian plasma environment. When the Mars Advanced Radar for Subsurface and Ionosphere Sounding (MARSIS) instrument aboard Mars Express is simultaneously sounding the ionosphere, the influence from changes in the <span class="hlt">solar</span> wind can be <span class="hlt">observed</span>. Previous studies have suggested a positive correlation, connecting ionospheric density to the <span class="hlt">solar</span> wind proton flux, but depended on Earth-based measurements for <span class="hlt">solar</span> wind conditions. More recently, research has indicated that <span class="hlt">observations</span> of ionospheric variability from these two spacecraft can be connected in special cases, such as shock wave impacts or specific <span class="hlt">solar</span> wind magnetic field orientations. Here we extend this to more general <span class="hlt">solar</span> wind conditions and examine how changes in the <span class="hlt">solar</span> wind properties measured by MAVEN instruments correlate with ionospheric structure and dynamics <span class="hlt">observed</span> simultaneously in MARSIS remote and local measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001171.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001171.html"><span><span class="hlt">Solar</span> <span class="hlt">System</span>, in Perspective</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2014-03-24</p> <p>This artist's concept puts <span class="hlt">solar</span> <span class="hlt">system</span> distances in perspective. The scale bar is in astronomical units, with each set distance beyond 1 AU representing 10 times the previous distance. One AU is the distance from the sun to the Earth, which is about 93 million miles or 150 million kilometers. Neptune, the most distant planet from the sun, is about 30 AU. Informally, the term "<span class="hlt">solar</span> <span class="hlt">system</span>" is often used to mean the space out to the last planet. Scientific consensus, however, says the <span class="hlt">solar</span> <span class="hlt">system</span> goes out to the Oort Cloud, the source of the comets that swing by our sun on long time scales. Beyond the outer edge of the Oort Cloud, the gravity of other stars begins to dominate that of the sun. The inner edge of the main part of the Oort Cloud could be as close as 1,000 AU from our sun. The outer edge is estimated to be around 100,000 AU. NASA's Voyager 1, humankind's most distant spacecraft, is around 125 AU. Scientists believe it entered interstellar space, or the space between stars, on Aug. 25, 2012. Much of interstellar space is actually inside our <span class="hlt">solar</span> <span class="hlt">system</span>. It will take about 300 years for Voyager 1 to reach the inner edge of the Oort Cloud and possibly about 30,000 years to fly beyond it. Alpha Centauri is currently the closest star to our <span class="hlt">solar</span> <span class="hlt">system</span>. But, in 40,000 years, Voyager 1 will be closer to the star AC +79 3888 than to our own sun. AC +79 3888 is actually traveling faster toward Voyager 1 than the spacecraft is traveling toward it. The Voyager spacecraft were built and continue to be operated by NASA's Jet Propulsion Laboratory, in Pasadena, Calif. Caltech manages JPL for NASA. The Voyager missions are a part of NASA's Heliophysics <span class="hlt">System</span> Observatory, sponsored by the Heliophysics Division of the Science Mission Directorate at NASA Headquarters in Washington. For more information about Voyager, visit: www.nasa.gov/voyager and voyager.jpl.nasa.gov . Image credit: NASA/JPL-Caltech NASA image use policy. NASA Goddard Space Flight Center enables</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22521848-observing-cascades-solar-bullets-high-resolution-ii','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22521848-observing-cascades-solar-bullets-high-resolution-ii"><span><span class="hlt">OBSERVING</span> CASCADES OF <span class="hlt">SOLAR</span> BULLETS AT HIGH RESOLUTION. II</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>Scullion, E.; Engvold, O.; Lin, Y.</p> <p></p> <p>High resolution <span class="hlt">observations</span> from the Swedish 1-m <span class="hlt">Solar</span> Telescope revealed bright, discrete, blob-like structures (which we refer to as <span class="hlt">solar</span> bullets) in the Hα 656.28 nm line core that appear to propagate laterally across the <span class="hlt">solar</span> atmosphere as clusters in active regions (ARs). These small-scale structures appear to be field aligned and many bullets become triggered simultaneously and traverse collectively as a cluster. Here, we conduct a follow-up study on these rapidly evolving structures with coincident <span class="hlt">observations</span> from the <span class="hlt">Solar</span> Dynamics Observatory/Atmospheric Imaging Assembly. With the co-aligned data sets, we reveal (a) an evolving multithermal structure in the bullet clustermore » ranging from chromospheric to at least transition region temperatures, (b) evidence for cascade-like behavior and corresponding bidirectional motions in bullets within the cluster, which indicate that there is a common source of the initial instability leading to bullet formation, and (c) a direct relationship between co-incident bullet velocities <span class="hlt">observed</span> in Hα and He ii 30.4 nm and an inverse relationship with respect to bullet intensity in these channels. We find evidence supporting that bullets are typically composed of a cooler, higher density core detectable in Hα with a less dense, hotter, and fainter co-moving outer sheath. Bullets unequivocally demonstrate the finely structured nature of the AR corona. We have no clear evidence for bullets being associated with locally heated (or cooled), fast flowing plasma. Fast MHD pulses (such as solitons) could best describe the dynamic properties of bullets whereas the presence of a multithermal structure is new.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..798A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..798A"><span>Results of Spectral Corona <span class="hlt">Observations</span> in <span class="hlt">Solar</span> Activity Cycles 17-24</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aliev, A. Kh.; Guseva, S. A.; Tlatov, A. G.</p> <p>2017-12-01</p> <p>The results of the work of the global <span class="hlt">observation</span> network are considered, and a comparative analysis of the data of various coronal observatories is performed. The coronal activity index has been reconstructed for the period 1939-2016 based on the data of various observatories in Kislovodsk <span class="hlt">system</span>. For this purpose, the corona daily intensity maps from the Sacramento Peak and Lomnický Štít observatories according to the <span class="hlt">Solar</span>-Geophysical Data journal have been digitized; they supplement the data of other observatories. The homogeneity and continuity of the corona <span class="hlt">observations</span> at the Kislovodsk station, including activity cycle 24, is confirmed. Unfortunately, the only observatory at present that continues <span class="hlt">observation</span> of the spectral corona in Fe XIV 5303 Å and Fe XIV 6374 Å lines is the Kislovodsk astronomical station Mountain Astronomical Station (MAS) of the Central Astronomical Observatory, Russian Academy of Sciences (Pulkovo). The data on the combined corona in 5303 Å line are analyzed. It is shown that there is a high correlation of the intensity index of green corona with <span class="hlt">solar</span> radiation measurements in the vacuum UV region. Data on the beginning of the new 25th activity cycle in the corona at high latitudes are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70175395','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70175395"><span>Evaluating the effectiveness of wildlife detection and <span class="hlt">observation</span> technologies at a <span class="hlt">solar</span> power tower facility</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Diehl, Robert H.; Valdez, Ernest W.; Preston, Todd M.; Wellik, Mike J.; Cryan, Paul</p> <p>2016-01-01</p> <p><span class="hlt">Solar</span> power towers produce electrical energy from sunlight at an industrial scale. Little is known about the effects of this technology on flying animals and few methods exist for automatically detecting or <span class="hlt">observing</span> wildlife at <span class="hlt">solar</span> towers and other tall anthropogenic structures. Smoking objects are sometimes <span class="hlt">observed</span> co-occurring with reflected, concentrated light (“<span class="hlt">solar</span> flux”) in the airspace around <span class="hlt">solar</span> towers, but the identity and origins of such objects can be difficult to determine. In this <span class="hlt">observational</span> pilot study at the world’s largest <span class="hlt">solar</span> tower facility, we assessed the efficacy of using radar, surveillance video, and insect trapping to detect and <span class="hlt">observe</span> animals flying near the towers. During site visits in May and September 2014, we monitored the airspace surrounding towers and <span class="hlt">observed</span> insects, birds, and bats under a variety of environmental and operational conditions. We detected and broadly differentiated animals or objects moving through the airspace generally using radar and near <span class="hlt">solar</span> towers using several video imaging methods. Video revealed what appeared to be mostly small insects burning in the <span class="hlt">solar</span> flux. Also, we occasionally detected birds flying in the <span class="hlt">solar</span> flux but could not accurately identify birds to species or the types of insects and small objects composing the vast majority of smoking targets. Insect trapping on the ground was somewhat effective at sampling smaller insects around the tower, and presence and abundance of insects in the traps generally trended with radar and video <span class="hlt">observations</span>. Traps did not tend to sample the larger insects we sometimes <span class="hlt">observed</span> flying in the <span class="hlt">solar</span> flux or found dead on the ground beneath the towers. Some of the methods we tested (e.g., video surveillance) could be further assessed and potentially used to automatically detect and <span class="hlt">observe</span> flying animals in the vicinity of <span class="hlt">solar</span> towers to advance understanding about their effects on wildlife.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27462989','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27462989"><span>Evaluating the Effectiveness of Wildlife Detection and <span class="hlt">Observation</span> Technologies at a <span class="hlt">Solar</span> Power Tower Facility.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Diehl, Robert H; Valdez, Ernest W; Preston, Todd M; Wellik, Michael J; Cryan, Paul M</p> <p>2016-01-01</p> <p><span class="hlt">Solar</span> power towers produce electrical energy from sunlight at an industrial scale. Little is known about the effects of this technology on flying animals and few methods exist for automatically detecting or <span class="hlt">observing</span> wildlife at <span class="hlt">solar</span> towers and other tall anthropogenic structures. Smoking objects are sometimes <span class="hlt">observed</span> co-occurring with reflected, concentrated light ("<span class="hlt">solar</span> flux") in the airspace around <span class="hlt">solar</span> towers, but the identity and origins of such objects can be difficult to determine. In this <span class="hlt">observational</span> pilot study at the world's largest <span class="hlt">solar</span> tower facility, we assessed the efficacy of using radar, surveillance video, and insect trapping to detect and <span class="hlt">observe</span> animals flying near the towers. During site visits in May and September 2014, we monitored the airspace surrounding towers and <span class="hlt">observed</span> insects, birds, and bats under a variety of environmental and operational conditions. We detected and broadly differentiated animals or objects moving through the airspace generally using radar and near <span class="hlt">solar</span> towers using several video imaging methods. Video revealed what appeared to be mostly small insects burning in the <span class="hlt">solar</span> flux. Also, we occasionally detected birds flying in the <span class="hlt">solar</span> flux but could not accurately identify birds to species or the types of insects and small objects composing the vast majority of smoking targets. Insect trapping on the ground was somewhat effective at sampling smaller insects around the tower, and presence and abundance of insects in the traps generally trended with radar and video <span class="hlt">observations</span>. Traps did not tend to sample the larger insects we sometimes <span class="hlt">observed</span> flying in the <span class="hlt">solar</span> flux or found dead on the ground beneath the towers. Some of the methods we tested (e.g., video surveillance) could be further assessed and potentially used to automatically detect and <span class="hlt">observe</span> flying animals in the vicinity of <span class="hlt">solar</span> towers to advance understanding about their effects on wildlife.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4963080','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4963080"><span>Evaluating the Effectiveness of Wildlife Detection and <span class="hlt">Observation</span> Technologies at a <span class="hlt">Solar</span> Power Tower Facility</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Diehl, Robert H.; Valdez, Ernest W.; Preston, Todd M.; Wellik, Michael J.; Cryan, Paul M.</p> <p>2016-01-01</p> <p><span class="hlt">Solar</span> power towers produce electrical energy from sunlight at an industrial scale. Little is known about the effects of this technology on flying animals and few methods exist for automatically detecting or <span class="hlt">observing</span> wildlife at <span class="hlt">solar</span> towers and other tall anthropogenic structures. Smoking objects are sometimes <span class="hlt">observed</span> co-occurring with reflected, concentrated light (“<span class="hlt">solar</span> flux”) in the airspace around <span class="hlt">solar</span> towers, but the identity and origins of such objects can be difficult to determine. In this <span class="hlt">observational</span> pilot study at the world’s largest <span class="hlt">solar</span> tower facility, we assessed the efficacy of using radar, surveillance video, and insect trapping to detect and <span class="hlt">observe</span> animals flying near the towers. During site visits in May and September 2014, we monitored the airspace surrounding towers and <span class="hlt">observed</span> insects, birds, and bats under a variety of environmental and operational conditions. We detected and broadly differentiated animals or objects moving through the airspace generally using radar and near <span class="hlt">solar</span> towers using several video imaging methods. Video revealed what appeared to be mostly small insects burning in the <span class="hlt">solar</span> flux. Also, we occasionally detected birds flying in the <span class="hlt">solar</span> flux but could not accurately identify birds to species or the types of insects and small objects composing the vast majority of smoking targets. Insect trapping on the ground was somewhat effective at sampling smaller insects around the tower, and presence and abundance of insects in the traps generally trended with radar and video <span class="hlt">observations</span>. Traps did not tend to sample the larger insects we sometimes <span class="hlt">observed</span> flying in the <span class="hlt">solar</span> flux or found dead on the ground beneath the towers. Some of the methods we tested (e.g., video surveillance) could be further assessed and potentially used to automatically detect and <span class="hlt">observe</span> flying animals in the vicinity of <span class="hlt">solar</span> towers to advance understanding about their effects on wildlife. PMID:27462989</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720003183','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720003183"><span>Dynamics of the <span class="hlt">solar</span> wind and its interaction with bodies in the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Spreiter, J. R.</p> <p>1971-01-01</p> <p>A discussion of the <span class="hlt">solar</span> wind and its interaction with bodies of the <span class="hlt">solar</span> <span class="hlt">system</span> is presented. An overall unified account of the role of shock waves in the heating of the <span class="hlt">solar</span> corona, the transmission of <span class="hlt">solar</span> disturbances to the <span class="hlt">solar</span> <span class="hlt">system</span>, the flow fields of planets and natural satellites, and biological effects are provided. An analysis of magnetometer data from Explorer 33 and Vela 3A satellites to identify characteristics of <span class="hlt">solar</span> wind shock waves is included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790016262','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790016262"><span><span class="hlt">Solar</span> energy collection <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miller, C. G.; Stephens, J. B. (Inventor)</p> <p>1979-01-01</p> <p>A fixed, linear, ground-based primary reflector having an extended curved sawtooth-contoured surface covered with a metalized polymeric reflecting material, reflects <span class="hlt">solar</span> energy to a movably supported collector that is kept at the concentrated line focus reflector primary. The primary reflector may be constructed by a process utilizing well known freeway paving machinery. The <span class="hlt">solar</span> energy absorber is preferably a fluid transporting pipe. Efficient utilization leading to high temperatures from the reflected <span class="hlt">solar</span> energy is obtained by cylindrical shaped secondary reflectors that direct off-angle energy to the absorber pipe. A seriatim arrangement of cylindrical secondary reflector stages and spot-forming reflector stages produces a high temperature <span class="hlt">solar</span> energy collection <span class="hlt">system</span> of greater efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Solar+AND+system&pg=4&id=ED495218','ERIC'); return false;" href="https://eric.ed.gov/?q=Solar+AND+system&pg=4&id=ED495218"><span>Our <span class="hlt">Solar</span> <span class="hlt">System</span>. Our <span class="hlt">Solar</span> <span class="hlt">System</span> Topic Set</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>Phelan, Glen</p> <p>2006-01-01</p> <p>This book examines the planets and other objects in space that make up the <span class="hlt">solar</span> <span class="hlt">system</span>. It also shows how technology helps students learn about our neighbors in space. The suggested age range for this book is 3-8 with a guided reading level of Q-R. The Fry level is 3.2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..122.9815K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.9815K"><span>Applying Nyquist's method for stability determination to <span class="hlt">solar</span> wind <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>Klein, Kristopher G.; Kasper, Justin C.; Korreck, K. E.; Stevens, Michael L.</p> <p>2017-10-01</p> <p>The role instabilities play in governing the evolution of <span class="hlt">solar</span> and astrophysical plasmas is a matter of considerable scientific interest. The large number of sources of free energy accessible to such nearly collisionless plasmas makes general modeling of unstable behavior, accounting for the temperatures, densities, anisotropies, and relative drifts of a large number of populations, analytically difficult. We therefore seek a general method of stability determination that may be automated for future analysis of <span class="hlt">solar</span> wind <span class="hlt">observations</span>. This work describes an efficient application of the Nyquist instability method to the Vlasov dispersion relation appropriate for hot, collisionless, magnetized plasmas, including the <span class="hlt">solar</span> wind. The algorithm recovers the familiar proton temperature anisotropy instabilities, as well as instabilities that had been previously identified using fits extracted from in situ <span class="hlt">observations</span> in Gary et al. (2016). Future proposed applications of this method are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070020281&hterms=exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dexchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070020281&hterms=exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dexchange"><span>Chandra <span class="hlt">Observations</span> of Comet 2P/Encke 2003: First Detection of a Collisionally Thin, Fast <span class="hlt">Solar</span> Wind Charge Exchange <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lisse, C. M.; Christian, D. J.; Deneri, K.; Wolk, S. J.; Bodewits, D.; Hoekstra, R.; Combi, M. R.; Makinen, T.; Dryer, M.; Fry, C. D.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20070020281'); toggleEditAbsImage('author_20070020281_show'); toggleEditAbsImage('author_20070020281_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20070020281_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20070020281_hide"></p> <p>2005-01-01</p> <p>We report the results of 15 hr of Chandra <span class="hlt">observations</span> of comet 2P/Encke 2003 on November 24. X-ray emission from comet Encke was resolved on scales of 500-40,000 km, with unusual morphology due to the presence of a low-density, collisionally thin (to charge exchange) coma. A light curve with peak-to-peak amplitude of 20% consistent with a nucleus rotational period of 11.1 hr was found, further evidence for a collisionally thin coma. We confirm emission lines due to oxygen and neon in the 800-1000 eV range but find very unusual oxygen and carbon line ratios in the 200-700 eV range, evidence for low-density, high effective temperature <span class="hlt">solar</span> wind composition. We compare the X-ray spectral <span class="hlt">observation</span> results to contemporaneous measurements of the coma and <span class="hlt">solar</span> wind made by other means and find good evidence for the dominance of a postshock bubble of expanding <span class="hlt">solar</span> wind plasma, moving at 600 km/s with charge state composition between that of the "fast" and "slow" <span class="hlt">solar</span> winds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820008601','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820008601"><span><span class="hlt">Solar</span> heated fluidized bed gasification <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Qader, S. A. (Inventor)</p> <p>1981-01-01</p> <p>A <span class="hlt">solar</span>-powered fluidized bed gasification <span class="hlt">system</span> for gasifying carbonaceous material is presented. The <span class="hlt">system</span> includes a <span class="hlt">solar</span> gasifier which is heated by fluidizing gas and steam. Energy to heat the gas and steam is supplied by a high heat capacity refractory honeycomb which surrounds the fluid bed reactor zone. The high heat capacity refractory honeycomb is heated by <span class="hlt">solar</span> energy focused on the honeycomb by <span class="hlt">solar</span> concentrator through <span class="hlt">solar</span> window. The fluid bed reaction zone is also heated directly and uniformly by thermal contact of the high heat capacity ceramic honeycomb with the walls of the fluidized bed reactor. Provisions are also made for recovering and recycling catalysts used in the gasification process. Back-up furnace is provided for start-up procedures and for supplying heat to the fluid bed reaction zone when adequate supplies of <span class="hlt">solar</span> energy are not available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985Gelio...2...28S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985Gelio...2...28S"><span>Control of <span class="hlt">solar</span> energy <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sizov, Iu. M.; Zakhidov, R. A.; Baranov, V. G.</p> <p></p> <p>Two approaches to the control of large <span class="hlt">solar</span> energy <span class="hlt">systems</span>, i.e., programmed control and control <span class="hlt">systems</span> relying on the use of orientation transducers and feedback, are briefly reviewed, with particular attention given to problems associated with these control <span class="hlt">systems</span>. A new control <span class="hlt">system</span> for large <span class="hlt">solar</span> power plants is then proposed which is based on a combination of these approaches. The general design of the control <span class="hlt">system</span> is shown and its principle of operation described. The efficiency and cost effectiveness of the approach proposed here are demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990110718&hterms=Memory+attitude&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DMemory%2Battitude','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990110718&hterms=Memory+attitude&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DMemory%2Battitude"><span><span class="hlt">Solar</span> Particle Induced Upsets in the TDRS-1 Attitude Control <span class="hlt">System</span> RAM During the October 1989 <span class="hlt">Solar</span> Particle Events</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Croley, D. R.; Garrett, H. B.; Murphy, G. B.; Garrard,T. L.</p> <p>1995-01-01</p> <p>The three large <span class="hlt">solar</span> particle events, beginning on October 19, 1989 and lasting approximately six days, were characterized by high fluences of <span class="hlt">solar</span> protons and heavy ions at 1 AU. During these events, an abnormally large number of upsets (243) were <span class="hlt">observed</span> in the random access memory of the attitude control <span class="hlt">system</span> (ACS) control processing electronics (CPE) on-board the geosynchronous TDRS-1 (Telemetry and Data Relay Satellite). The RAM unit affected was composed of eight Fairchild 93L422 memory chips. The Galileo spacecraft, launched on October 18, 1989 (one day prior to the <span class="hlt">solar</span> particle events) <span class="hlt">observed</span> the fluxes of heavy ions experienced by TDRS-1. Two solid-state detector telescopes on-board Galileo, designed to measure heavy ion species and energy, were turned on during time periods within each of the three separate events. The heavy ion data have been modeled and the time history of the events reconstructed to estimate heavy ion fluences. These fluences were converted to effective LET spectra after transport through the estimated shielding distribution around the TDRS-1 ACS <span class="hlt">system</span>. The number of single event upsets (SEU) expected was calculated by integrating the measured cross section for the Fairchild 93L422 memory chip with average effective LET spectrum. The expected number of heavy ion induced SEU's calculated was 176. GOES-7 proton data, <span class="hlt">observed</span> during the <span class="hlt">solar</span> particle events, were used to estimate the number of proton-induced SEU's by integrating the proton fluence spectrum incident on the memory chips, with the two-parameter Bendel cross section for proton SEU'S. The proton fluence spectrum at the device level was gotten by transporting the protons through the estimated shielding distribution. The number of calculated proton-induced SEU's was 72, yielding a total of 248 predicted SEU'S, very dose to the 243 <span class="hlt">observed</span> SEU'S. These calculations uniquely demonstrate the roles that <span class="hlt">solar</span> heavy ions and protons played in the production of SEU</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770066439&hterms=application+Fourier&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dapplication%2BFourier','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770066439&hterms=application+Fourier&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dapplication%2BFourier"><span>The application of Fourier transform spectroscopy to the remote identification of solids in the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Larson, H. P.; Fink, U.</p> <p>1977-01-01</p> <p>The techniques of Fourier transform spectroscopy combined with large aperture telescopes and advances in detector technology now permit infrared (at a wavelength greater than 1 micron) <span class="hlt">observations</span> of the surfaces of small <span class="hlt">solar</span> <span class="hlt">system</span> objects such as asteroids and satellites. The results demonstrate that this activity can produce important new compositional information related to the origin and evolution of the <span class="hlt">solar</span> <span class="hlt">system</span>. The detection of water ice in Saturn's rings and on some of the satellites of Jupiter and Saturn confirm expectations that ices are important mineralogical components in the chemistry of the outer <span class="hlt">solar</span> <span class="hlt">system</span>. More recent studies of the mineralogical composition of the surfaces of asteroids provide a new <span class="hlt">observational</span> link to the origin of meteorites and the early thermal history of the <span class="hlt">solar</span> <span class="hlt">system</span>. These results have been dependent upon supporting laboratory studies of the spectral behavior of ices and minerals to define the potential, and limitations, of the method. Since many of the astronomical <span class="hlt">observations</span> have been exploratory in nature, prospects are good that continued refinement of the techniques will lead to additional insights.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1019563','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1019563"><span>Hybrid <span class="hlt">solar</span> lighting distribution <span class="hlt">systems</span> and components</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Muhs, Jeffrey D [Lenoir City, TN; Earl, Dennis D [Knoxville, TN; Beshears, David L [Knoxville, TN; Maxey, Lonnie C [Powell, TN; Jordan, John K [Oak Ridge, TN; Lind, Randall F [Lenoir City, TN</p> <p>2011-07-05</p> <p>A hybrid <span class="hlt">solar</span> lighting distribution <span class="hlt">system</span> and components having at least one hybrid <span class="hlt">solar</span> concentrator, at least one fiber receiver, at least one hybrid luminaire, and a light distribution <span class="hlt">system</span> operably connected to each hybrid <span class="hlt">solar</span> concentrator and each hybrid luminaire. A controller operates all components.</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://ntrs.nasa.gov/search.jsp?R=19870000022&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsolar%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870000022&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsolar%2Benergy"><span>Evaluating Performances of <span class="hlt">Solar</span>-Energy <span class="hlt">Systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jaffe, L. D.</p> <p>1987-01-01</p> <p>CONC11 computer program calculates performances of dish-type <span class="hlt">solar</span> thermal collectors and power <span class="hlt">systems</span>. <span class="hlt">Solar</span> thermal power <span class="hlt">system</span> consists of one or more collectors, power-conversion subsystems, and powerprocessing subsystems. CONC11 intended to aid <span class="hlt">system</span> designer in comparing performance of various design alternatives. Written in Athena FORTRAN and Assembler.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040086783&hterms=Solar+still&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSolar%2Bstill','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040086783&hterms=Solar+still&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSolar%2Bstill"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Studies in the Infrared with the Spitzer Space Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cruikshank, D. P.; Stansberry, J. A.; Cleve, J. Van; Burgdorf, M. J.; Fernandez, Y. R.; Meadows, V. S.; Reach, W. T.</p> <p>2004-01-01</p> <p>The Spitzer Space Telescope, formerly known as SIRTF, is a cryogenic telescope (85 cm diameter) operating in a heliocentric orbit trailing the Earth. Its three instruments provide capabilities for spectroscopy, wide-field and small-field imaging at many wavelengths in the range 3.5-160 microns. <span class="hlt">Observations</span> to be executed in the first two years in programs defined by the Guaranteed Time <span class="hlt">Observer</span> (GTO) group (the authors of this presentation) consist of photometry, spectroscopy, and radiometry of many <span class="hlt">Solar</span> <span class="hlt">System</span> objects, including Titan and other satellites of the outer planets, Pluto, Centaurs, trans-Neptunian objects, comers, asteroids, Uranus, and Neptune. At the time of the preparation of this abstract, some preliminary <span class="hlt">observations</span> have been made, but the final calibration and reduction of the data are still in progress. The latest results of the <span class="hlt">Solar</span> <span class="hlt">System</span> investigations will be presented here.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050202052&hterms=theories+formation+solar+system&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtheories%2Bformation%2Bsolar%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050202052&hterms=theories+formation+solar+system&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtheories%2Bformation%2Bsolar%2Bsystem"><span>Constraints on the Detection of the <span class="hlt">Solar</span> Nebula's Oxidation State Through Asteroid <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>Abell, P. A.; Gaffey, M. J.; Hardersen, P. S.</p> <p>2005-01-01</p> <p>Introduction: Asteroids represent the only in situ surviving population of planetesimals from the formation of the inner <span class="hlt">solar</span> <span class="hlt">system</span> and therefore include materials from the very earliest stages of <span class="hlt">solar</span> <span class="hlt">system</span> formation. Hence, these bodies can provide constraints on the processes and conditions that were present during this epoch and can be used to test current models and theories describing the late <span class="hlt">solar</span> nebula, the early <span class="hlt">solar</span> <span class="hlt">system</span> and subsequent planetary accretion. From detailed knowledge of asteroid mineralogic compositions the probable starting materials, thermal histories, and oxidation states of asteroid parent bodies can be inferred. If such data can be obtained from specific mainbelt source regions, then this information can be used to map out the formation conditions of the late <span class="hlt">solar</span> nebula within the inner <span class="hlt">solar</span> <span class="hlt">system</span> and possibly distinguish any trends in oxidation state that may be present.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1215666-solar-thermophotovoltaic-system-using-nanostructures','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1215666-solar-thermophotovoltaic-system-using-nanostructures"><span><span class="hlt">Solar</span> thermophotovoltaic <span class="hlt">system</span> using nanostructures</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ungaro, Craig; Gray, Stephen K.; Gupta, Mool C.</p> <p>2015-08-20</p> <p>This paper presents results on a highly efficient experimental <span class="hlt">solar</span> thermophotovoltaic (STPV) <span class="hlt">system</span> using simulated <span class="hlt">solar</span> energy. An overall power conversion efficiency of 6.2% was recorded under <span class="hlt">solar</span> simulation. This was matched with a thermodynamic model, and the losses within the <span class="hlt">system</span>, as well as a path forward to mitigate these losses, have been investigated. The <span class="hlt">system</span> consists of a planar, tungsten absorbing/emitting structure with an anti-reflection layer coated laser-microtextured absorbing surface and single-layer dielectric coated emitting surface. A GaSb PV cell was used to capture the emitted radiation and convert it into electrical energy. This simple structure is bothmore » easy to fabricate and temperature stable, and contains no moving parts or heat exchange fluids.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26406745','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26406745"><span><span class="hlt">Solar</span> thermophotovoltaic <span class="hlt">system</span> using nanostructures.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ungaro, Craig; Gray, Stephen K; Gupta, Mool C</p> <p>2015-09-21</p> <p>This paper presents results on a highly efficient experimental <span class="hlt">solar</span> thermophotovoltaic (STPV) <span class="hlt">system</span> using simulated <span class="hlt">solar</span> energy. An overall power conversion efficiency of 6.2% was recorded under <span class="hlt">solar</span> simulation. This was matched with a thermodynamic model, and the losses within the <span class="hlt">system</span>, as well as a path forward to mitigate these losses, have been investigated. The <span class="hlt">system</span> consists of a planar, tungsten absorbing/emitting structure with an anti-reflection layer coated laser-microtextured absorbing surface and single-layer dielectric coated emitting surface. A GaSb PV cell was used to capture the emitted radiation and convert it into electrical energy. This simple structure is both easy to fabricate and temperature stable, and contains no moving parts or heat exchange fluids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021396&hterms=dropout&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddropout','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021396&hterms=dropout&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddropout"><span>Suprathermal electron loss cone distributions in the <span class="hlt">solar</span> wind: Ulysses <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>Phillips, J. L.; Feldman, W. C.; Gosling, J. T.; Hammond, C. M.; Forsyth, R. J.</p> <p>1995-01-01</p> <p><span class="hlt">Solar</span> wind suprathermal electron distributions in the <span class="hlt">solar</span> wind generally carry a field-aligned antisunward heat flux. Within coronal mass ejections and upstream of strong shocks driven by corotating interaction regions (CIRs), counterstreaming electron beams are <span class="hlt">observed</span>. We present <span class="hlt">observations</span> by the Ulysses <span class="hlt">solar</span> wind plasma experiment of a new class of suprathermal electron signatures. At low <span class="hlt">solar</span> latitudes and heliocentric distances beyond 3.5 AU Ulysses encountered several intervals, ranging in duration from 1 hour to 22 hours, in which the suprathermal distributions included an antisunward field-aligned beam and a return population with a flux dropout typically spanning +/- 60 deg from the sunward field-aligned direction. All events occurred within CIRs, downstream of the forward and reverse shocks or waves bounding the interaction regions. We evaluate the hypothesis that the sunward-moving electrons result from reflection of the antisunward beams at magnetic field compressions downstream from the <span class="hlt">observations</span>, with wide loss cones caused by the relatively weak compression ratio. This hypothesis requires that field magnitude within the CIRs actually increase with increasing field-aligned distance from the Sun. Details of the electron distributions and ramifications for CIR and shock geometry will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SpWea..16..245H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SpWea..16..245H"><span>Onsets of <span class="hlt">Solar</span> Proton Events in Satellite and Ground Level <span class="hlt">Observations</span>: A Comparison</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Jing; Rodriguez, Juan V.</p> <p>2018-03-01</p> <p>The early detection of <span class="hlt">solar</span> proton event onsets is essential for protecting humans and electronics in space, as well as passengers and crew at aviation altitudes. Two commonly compared methods for <span class="hlt">observing</span> <span class="hlt">solar</span> proton events that are sufficiently large and energetic to be detected on the ground through the creation of secondary radiation—known as ground level enhancements (GLEs)—are (1) a network of ground-based neutron monitors (NMs) and (2) satellite-based particle detectors. Until recently, owing to the different time resolution of the two data sets, it has not been feasible to compare these two types of <span class="hlt">observations</span> using the same detection algorithm. This paper presents a comparison between the two <span class="hlt">observational</span> platforms using newly processed >100 MeV 1 min count rates and fluxes from National Oceanic and Atmospheric Administration's Geostationary Operational Environmental Satellite (GOES) 8-12 satellites, and 1 min count rates from the Neutron Monitor Database. We applied the same detection algorithm to each data set (tuned to the different background noise levels of the instrument types). Seventeen SPEs with GLEs were studied: GLEs 55-70 from <span class="hlt">Solar</span> Cycle 23 and GLE 71 from <span class="hlt">Solar</span> Cycle 24. The median difference in the event detection times by GOES and NM data is 0 min, indicating no innate benefit in time of either <span class="hlt">system</span>. The 10th, 25th, 75th, and 90th percentiles of the onset time differences (GOES minus NMs) are -7.2 min, -1.5 min, 2.5 min, and 4.2 min, respectively. This is in contrast to previous studies in which NM detections led GOES by 8 to 52 min without accounting for different alert protocols.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=materials+AND+storage+AND+thermal&id=EJ136819','ERIC'); return false;" href="https://eric.ed.gov/?q=materials+AND+storage+AND+thermal&id=EJ136819"><span>Advances in <span class="hlt">Solar</span> Heating and Cooling <span class="hlt">Systems</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>Ward, Dan S.</p> <p>1976-01-01</p> <p>Reports on technological advancements in the fields of <span class="hlt">solar</span> collectors, thermal storage <span class="hlt">systems</span>, and <span class="hlt">solar</span> heating and cooling <span class="hlt">systems</span>. Diagrams aid in the understanding of the thermodynamics of the <span class="hlt">systems</span>. (CP)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61...74P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61...74P"><span>Improving magnetosphere in situ <span class="hlt">observations</span> using <span class="hlt">solar</span> sails</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Parsay, Khashayar; Schaub, Hanspeter; Schiff, Conrad; Williams, Trevor</p> <p>2018-01-01</p> <p>Past and current magnetosphere missions employ conventional spacecraft formations for in situ <span class="hlt">observations</span> of the geomagnetic tail. Conventional spacecraft flying in inertially fixed Keplerian orbits are only aligned with the geomagnetic tail once per year, since the geomagnetic tail is always aligned with the Earth-Sun line, and therefore, rotates annually. <span class="hlt">Solar</span> sails are able to artificially create sun-synchronous orbits such that the orbit apse line remains aligned with the geomagnetic tail line throughout the entire year. This continuous presence in the geomagnetic tail can significantly increase the science phase for magnetosphere missions. In this paper, the problem of <span class="hlt">solar</span> sail formation design is explored using nonlinear programming to design optimal two-craft, triangle, and tetrahedron <span class="hlt">solar</span> sail formations, in terms of formation quality and formation stability. The designed formations are directly compared to the formations used in NASA's Magnetospheric Multi-Scale mission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.P21B0532S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.P21B0532S"><span>The Jupiter <span class="hlt">System</span> <span class="hlt">Observer</span> Mission Concept: Scientific Investigation of the Jovian <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Spilker, T. R.; Senske, D. A.; Prockter, L.; Kwok, J. H.; Tan-Wang, G. H.; Sdt, J.</p> <p>2007-12-01</p> <p>NASA's Science Mission Directorate (SMD), in efforts to start an outer <span class="hlt">solar</span> <span class="hlt">system</span> flagship mission in the near future, commissioned studies of mission concepts for four high-priority outer <span class="hlt">solar</span> <span class="hlt">system</span> destinations: Europa, the Jovian <span class="hlt">system</span>, Titan, and Enceladus. Our team has identified and evaluated science and mission architectures to investigate major elements of the Jovian <span class="hlt">system</span>: Jupiter, the Galilean moons, rings, and magnetosphere, and their interactions. SMD dubbed the mission concept the "Jupiter <span class="hlt">System</span> <span class="hlt">Observer</span> (JSO)." This JPL-led study's final report is now complete and was submitted in August 2007. SMD intends to select a subset of these four concepts for additional detailed study, leading to a potential flagship mission new start. The study's NASA-appointed, multi-institutional Science Definition Team (SDT) identified a rich set of science objectives that JSO can address quite well. The highly capable science payload (including ~50-cm optics), an extensive tour with multiple close flybys of Io, Europa, Ganymede and Callisto, and a significant time in orbit at Ganymede, addresses a large set of <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Decadal Survey (2003) and NASA <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration Roadmap (2006) high-priority objectives. With the engineering team, the SDT evaluated a suite of mission architectures and the science they enable to arrive at two architectures that provide the best science for their estimated mission costs. This paper discusses the science objectives and operational capabilities and considerations for these mission concepts, and some options available for emphasizing specific science objectives. This work was performed at JPL, APL, and other institutions under contract to NASA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1980STIN...8113516B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1980STIN...8113516B"><span><span class="hlt">Systems</span> analysis techniques for annual cycle thermal energy storage <span class="hlt">solar</span> <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baylin, F.</p> <p>1980-07-01</p> <p>Community-scale annual cycle thermal energy storage <span class="hlt">solar</span> <span class="hlt">systems</span> are options for building heat and cooling. A variety of approaches are feasible in modeling ACTES <span class="hlt">solar</span> <span class="hlt">systems</span>. The key parameter in such efforts, average collector efficiency, is examined, followed by several approaches for simple and effective modeling. Methods are also examined for modeling building loads for structures based on both conventional and passive architectural designs. Two simulation models for sizing <span class="hlt">solar</span> heating <span class="hlt">systems</span> with annual storage are presented. Validation is presented by comparison with the results of a study of seasonal storage <span class="hlt">systems</span> based on SOLANSIM, an hour-by-hour simulation. These models are presently used to examine the economic trade-off between collector field area and storage capacity. Programs directed toward developing other <span class="hlt">system</span> components such as improved tanks and <span class="hlt">solar</span> ponds or design tools for ACTES <span class="hlt">solar</span> <span class="hlt">systems</span> are examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SoPh..293...90K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SoPh..293...90K"><span>Combined Radio and Space-Based <span class="hlt">Solar</span> <span class="hlt">Observations</span>: From Techniques to New Results - Preface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kontar, Eduard P.; Nindos, Alexander</p> <p>2018-06-01</p> <p>The phenomena <span class="hlt">observed</span> at the Sun have a variety of unique radio signatures that can be used to diagnose the processes in the <span class="hlt">solar</span> atmosphere. The insights provided by radio <span class="hlt">observations</span> are further enhanced when they are combined with <span class="hlt">observations</span> from space-based telescopes. This Topical collection demonstrates the power of combination methodology at work and provides new results on i) type I <span class="hlt">solar</span> radio bursts and thermal emission to study active regions; ii) type II and IV bursts to better understand the structure of coronal mass ejections; and iii) non-thermal gyro-synchrotron and/or type III bursts to improve the characterisation of particle acceleration in <span class="hlt">solar</span> flares. The ongoing improvements in time, frequency, and spatial resolutions of ground-based telescopes reveal new levels in the complexity of <span class="hlt">solar</span> phenomena and pose new questions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20110007245&hterms=Butterfly&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DButterfly','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20110007245&hterms=Butterfly&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DButterfly"><span><span class="hlt">Solar</span> Sources and Geospace Consequences of Interplanetary Magnetic Clouds <span class="hlt">Observed</span> During <span class="hlt">Solar</span> Cycle 23</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gopalswamy, N.; Akiyama, S.; Yashiro, S.; Michalek, G.; Lepping, R. P.</p> <p>2007-01-01</p> <p>We present results of a statistical investigation of 99 magnetic clouds (MCs) <span class="hlt">observed</span> during 1995-2005. The MC-associated coronal mass ejections (CMEs) are faster and wider on the average and originate within +/-30deg from the <span class="hlt">solar</span> disk center. The <span class="hlt">solar</span> sources of MCs also followed the butterfly diagram. The correlation between the magnetic field strength and speed of MCs was found to be valid over a much wider range of speeds. The number of south-north (SN) MCs was dominant and decreased with <span class="hlt">solar</span> cycle, while the number of north-south (NS) MCs increased confirming the odd-cycle behavior. Two-thirds of MCs were geoeffective; the Dst index was highly correlated with speed and magnetic field in MCs as well as their product. Many (55%) fully northward (FN) MCs were geoeffective solely due to their sheaths. The non-geoeffective MCs were slower (average speed approx. 382 km/s), had a weaker southward magnetic field (average approx. -5.2nT), and occurred mostly during the rise phase of the <span class="hlt">solar</span> activity cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740029492&hterms=Solar+power+filters&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSolar%2Bpower%2Bfilters','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740029492&hterms=Solar+power+filters&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSolar%2Bpower%2Bfilters"><span>High voltage <span class="hlt">solar</span> cell power generating <span class="hlt">system</span> for regulated <span class="hlt">solar</span> array development</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levy, E., Jr.; Hoffman, A. C.</p> <p>1973-01-01</p> <p>A laboratory <span class="hlt">solar</span> power <span class="hlt">system</span> regulated by on-panel switches has been delivered for operating high power (3 kw), high voltage (15,000 volt) loads (communication tubes, ion thrusters). The modular <span class="hlt">system</span> consists of 26 <span class="hlt">solar</span> arrays, each with an integral light source and cooling <span class="hlt">system</span>. A typical array contains 2560 series-connected cells. Each light source consists of twenty 500 watt tungsten iodide lamps providing plus or minus 5 per cent uniformity at one <span class="hlt">solar</span> constant. An array temperature of less than 40 C is achieved using an infrared filter, a water cooled plate, a vacuum hold-down <span class="hlt">system</span>, and air flushing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AAS...22012701P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AAS...22012701P"><span>Transits of Venus and Mercury: Exoplanet Analogs in Our <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, Jay M.</p> <p>2012-05-01</p> <p>Since Johannes Kepler's predictions of transits of Mercury and Venus in 1631, and <span class="hlt">observations</span> by Jeremiah Horrocks and William Crabtree of the 1639 transit of Venus, only 5 other transits of Venus have been <span class="hlt">observed</span>: in 1761 and 1769, 1874 and 1882, and 2004. Expeditions were sent all over the world for the 18th and 19th century transits to follow the methods of Halley and others to determine the Astronomical Unit, giving the size and scale of the <span class="hlt">solar</span> <span class="hlt">system</span>, arguably the most important problem in astronomy for centuries. I will discuss how the infamous black-drop effect bedeviled astronomers in that quest for an accurate A.U., and how Glenn Schneider and I explained the effect through satellite <span class="hlt">observations</span> of transits of Mercury, showing that it was not simply caused by the Cytherean atmosphere. During the 2004 transit, we worked with Richard Willson of ACRIMsat to detect the 0.1% drop in the Total <span class="hlt">Solar</span> Irradiance, showing the effect of <span class="hlt">solar</span> limb darkening, positioning such <span class="hlt">observations</span> of transits of Venus and of Mercury as analogs to exoplanet transits. Our <span class="hlt">observations</span> of the atmosphere of Venus with NASA's Transition Region and Coronal Explorer in 2004 led us to plan extensive <span class="hlt">observations</span> of Venus's atmosphere and other phenomena during the June 5, 2012, transit of Venus, the last to be visible from Earth until 2117. We will have used NASA's <span class="hlt">Solar</span> Dynamics Observatory, Hinode, ACRIMsat, and other spacecraft, and ground-based <span class="hlt">solar</span> telescopes at Sacramento Peak, Kitt Peak, Big Bear, and Haleakala to <span class="hlt">observe</span> the transit; I hope to give preliminary reports on these <span class="hlt">observations</span> during this talk. Further, I will discuss the plans of Ehrenreich and colleagues for Hubble <span class="hlt">observations</span> of this transit and our hopes of detecting transits of Venus and Earth as seen from Jupiter and Saturn over the next few years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663867-continued-kinematic-photometric-investigations-hierarchical-solar-type-multiple-star-systems','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663867-continued-kinematic-photometric-investigations-hierarchical-solar-type-multiple-star-systems"><span>Continued Kinematic and Photometric Investigations of Hierarchical <span class="hlt">Solar</span>-type Multiple Star <span class="hlt">Systems</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>Roberts, Lewis C. Jr.; Marinan, Anne D.; Tokovinin, Andrei</p> <p>2017-03-01</p> <p>We <span class="hlt">observed</span> 15 of the <span class="hlt">solar</span>-type binaries within 67 pc of the Sun previously <span class="hlt">observed</span> by the Robo-AO <span class="hlt">system</span> in the visible, with the PHARO near-infrared camera and the PALM-3000 adaptive optics <span class="hlt">system</span> on the 5 m Hale telescope. The physical status of the binaries is confirmed through common proper motion and detection of orbital motion. In the process, we detected a new candidate companion to HIP 95309. We also resolved the primary of HIP 110626 into a close binary, making that <span class="hlt">system</span> a triple. These detections increase the completeness of the multiplicity survey of the <span class="hlt">solar</span>-type stars within 67more » pc of the Sun. Combining our <span class="hlt">observations</span> of HIP 103455 with archival astrometric measurements and RV measurements, we are able to compute the first orbit of HIP 103455, showing that the binary has a 68 year period. We place the components on a color–magnitude diagram and discuss each multiple <span class="hlt">system</span> individually.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IJMPD..2430015I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IJMPD..2430015I"><span>Gravitational anomalies in the <span class="hlt">solar</span> <span class="hlt">system</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Iorio, Lorenzo</p> <p>2015-02-01</p> <p>Mindful of the anomalous perihelion precession of Mercury discovered by Le Verrier in the second half of the nineteenth century and its successful explanation by Einstein with his General Theory of Relativity in the early years of the twentieth century, discrepancies among <span class="hlt">observed</span> effects in our <span class="hlt">Solar</span> <span class="hlt">system</span> and their theoretical predictions on the basis of the currently accepted laws of gravitation applied to known matter-energy distributions have the potential of paving the way for remarkable advances in fundamental physics. This is particularly important now more than ever, given that most of the universe seems to be made of unknown substances dubbed Dark Matter and Dark Energy. Should this not be directly the case, <span class="hlt">Solar</span> <span class="hlt">system</span>'s anomalies could anyhow lead to advancements in either cumulative science, as shown to us by the discovery of Neptune in the first half of the nineteenth century, and technology itself. Moreover, investigations in one of such directions can serendipitously enrich the other one as well. The current status of some alleged gravitational anomalies in the <span class="hlt">Solar</span> <span class="hlt">system</span> is critically reviewed. They are: (a) Possible anomalous advances of planetary perihelia. (b) Unexplained orbital residuals of a recently discovered moon of Uranus (Mab). (c) The lingering unexplained secular increase of the eccentricity of the orbit of the Moon. (d) The so-called Faint Young Sun Paradox. (e) The secular decrease of the mass parameter of the Sun. (f) The Flyby Anomaly. (g) The Pioneer Anomaly. (h) The anomalous secular increase of the astronomical unit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090038667&hterms=chemistry+laboratory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dchemistry%2Blaboratory','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090038667&hterms=chemistry+laboratory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dchemistry%2Blaboratory"><span>Laboratory Studies of Ethane Ice Relevant to Outer <span class="hlt">Solar</span> <span class="hlt">System</span> Surfaces</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moore, Marla H.; Hudson, Reggie; Raines, Lily</p> <p>2009-01-01</p> <p>Oort Cloud comets, as well as TNOs Makemake (2045 FYg), Quaoar, and Pluto, are known to contain ethane. However, even though this molecule is found on several outer <span class="hlt">Solar</span> <span class="hlt">System</span> objects relatively little information is available about its amorphous and crystalline phases. In new experiments, we have prepared ethane ices at temperatures applicable to the outer <span class="hlt">Solar</span> <span class="hlt">System</span>, and have heated and ion-irradiated these ices to study phase changes and ethane's radiation chemistry using mid-IR spectroscopy (2.2 - 16.6 microns). Included in our work is the meta-stable phase that exists at 35 - 55 K. These results, including newly obtained optical constants, are relevant to ground-based <span class="hlt">observational</span> campaigns, the New Horizons mission, and supporting laboratory work. An improved understanding of solid-phase ethane may contribute to future searches for this and other hydrocarbons in the outer <span class="hlt">Solar</span> <span class="hlt">System</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH53A2546J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH53A2546J"><span>Lessons Learned from 10 Years of STEREO <span class="hlt">Solar</span> Wind <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>Jian, L. K.; Russell, C. T.; Luhmann, J. G.; Galvin, A. B.</p> <p>2017-12-01</p> <p>We have conducted long-term <span class="hlt">observations</span> of large-scale <span class="hlt">solar</span> wind structures since the launch of STEREO spacecraft, specifically interplanetary CMEs (ICMEs), slow-to-fast stream interaction regions (SIRs), and interplanetary shocks. In combination with our previous <span class="hlt">observations</span> of the same <span class="hlt">solar</span> wind structures in 1995-2009 using Wind/ACE data and the same identification criteria, we have first studied the <span class="hlt">solar</span> cycle variations of these structures, especially for the same phases of <span class="hlt">solar</span> cycles 23 and 24. Attributing the shocks to the interplanetary drivers, we have statistically compared the shocks driven by ICMEs and SIRs, and explained the shocks without a clear local driver. In addition, using the longitudinal and latitudinal separations between the twin spacecraft, we have investigated the recurrence and variability of ICMEs and SIRs, and gained the critical implications for the proposed L5 mission. At last, we have associated the heliospheric current sheet (HCS) crossings with the ICMEs and SIRs, and compared the properties of SIRs with and without HCS crossings, which correspond to the helmet streamers and pseudostreamers, respectively. The findings are important constraints on the theories of slow wind origin.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE10002E..05S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE10002E..05S"><span>Characterization of optical turbulence at the GREGOR <span class="hlt">solar</span> telescope: temporal and local behavior and its influence on the <span class="hlt">solar</span> <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>Sprung, D.; Sucher, E.; Stein, K.; von der Lühe, O.; Berkefeld, Th.</p> <p>2016-10-01</p> <p>Local atmospheric turbulence at the telescope level is regarded as a major reason for affecting the performance of the adaptive optics <span class="hlt">systems</span> using wavelengths in the visible and infrared for <span class="hlt">solar</span> <span class="hlt">observations</span>. During the day the air masses around the telescope dome are influenced by flow distortions. Additionally heating of the infrastructure close to telescope causes thermal turbulence. Thereby optical turbulence is produced and leads to quality changes in the local seeing throughout the day. Image degradation will be yielded affecting the performance of adaptive optical <span class="hlt">systems</span>. The spatial resolution of the <span class="hlt">solar</span> <span class="hlt">observations</span> will be reduced. For this study measurements of the optical turbulence, represented by the structure function parameter of the refractive index Cn2 were performed on several locations at the GREGOR telescope at the Teide observatory at Tenerife at the Canary Islands / Spain. Since September 2012 measurements of Cn2 were carried out between the towers of the Vacuum Tower Telescope (VTT) and of GREGOR with a laser-scintillometer. The horizontal distance of the measurement path was about 75 m. Additional from May 2015 up to March 2016 the optical turbulence was determined at three additional locations close to the <span class="hlt">solar</span> telescope GREGOR. The optical turbulence is derived from sonic anemometer measurements. Time series of the sonic temperature are analyzed and compared to the direct measurements of the laser scintillometer. Meteorological conditions are investigated, especially the influence of the wind direction. Turbulence of upper atmospheric layers is not regarded. The measured local turbulence is compared to the <span class="hlt">system</span> performance of the GREGOR telescopes. It appears that the mountain ridge effects on turbulence are more relevant than any local causes of seeing close to the telescope. Results of these analyses and comparison of nearly one year of measurements are presented and discussed.</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('https://ntrs.nasa.gov/search.jsp?R=20000084345&hterms=earth+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dearth%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000084345&hterms=earth+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dearth%2Bsystem"><span>The Earth <span class="hlt">Observing</span> <span class="hlt">System</span> Terra Mission</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kaufman, Yoram J.</p> <p>2000-01-01</p> <p>Langley's remarkable <span class="hlt">solar</span> and lunar spectra collected from Mt. Whitney inspired Arrhenius to develop the first quantitative climate model in 1896. After the launch in Dec. 16 1999, NASA's Earth <span class="hlt">Observing</span> AM Satellite (EOS-Terra) will repeat Langley's experiment, but for the entire planet, thus pioneering a wide array of calibrated spectral <span class="hlt">observations</span> from space of the Earth <span class="hlt">System</span>. Conceived in response to real environmental problems, EOS-Terra, in conjunction with other international satellite efforts, will fill a major gap in current efforts by providing quantitative global data sets with a resolution smaller than 1 km on the physical, chemical and biological elements of the earth <span class="hlt">system</span>. Thus, like Langley's data, EOS-Terra can revolutionize climate research by inspiring a new generation of climate <span class="hlt">system</span> models and enable us to assess the human impact on the environment. In the talk I shall review the historical perspective of the Terra mission and the key new elements of the mission. We expect to have some first images that demonstrate the most innovative capability from EOS Terra: MODIS - 1.37 microns cirrus channel; 250 m daily cover for clouds and vegetation change; 7 <span class="hlt">solar</span> channels for land and aerosol; new fire channels; Chlorophyll fluorescence; MISR - 9 multi angle views of clouds and vegetation; MOPITT - Global CO maps and CH4 maps; ASTER - Thermal channels for geological studies with 15-90 m resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJPv...9....7K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJPv...9....7K"><span>Monitoring a photovoltaic <span class="hlt">system</span> during the partial <span class="hlt">solar</span> eclipse of August 2017</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kurinec, Santosh K.; Kucer, Michal; Schlein, Bill</p> <p>2018-05-01</p> <p>The power output of a 4.85 kW residential photovoltaic (PV) <span class="hlt">system</span> located in Rochester, NY is monitored during the partial <span class="hlt">solar</span> eclipse of August 21, 2017. The data is compared with the data on a day before and on the same day, a year ago. The area of exposed <span class="hlt">solar</span> disk is measured using astrophotography every 16 s of the eclipse. Global <span class="hlt">solar</span> irradiance is estimated using the eclipse shading, time of the day, location coordinates, atmospheric conditions and panel orientation. A sharp decline, as expected in the energy produced is <span class="hlt">observed</span> at the time of the peak of the eclipse. The <span class="hlt">observed</span> data of the PV energy produced is related with the model calculations taking into account <span class="hlt">solar</span> eclipse coverage and cloudiness conditions. The paper provides a cohesive approach of irradiance calculations and obtaining anticipated PV performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820047282&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D80%26Ntt%3Dlazarus','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820047282&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D80%26Ntt%3Dlazarus"><span>Voyager <span class="hlt">observations</span> of <span class="hlt">solar</span> wind proton temperature - 1-10 AU</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gazis, P. R.; Lazarus, A. J.</p> <p>1982-01-01</p> <p>Simultaneous measurements are made of the <span class="hlt">solar</span> wind proton temperatures by the Voyager 1 and 2 spacecraft, far from earth, and the IMP 8 spacecraft in earth orbit. This technique permits a separation of radial and temporal variations of <span class="hlt">solar</span> wind parameters. The average value of the proton temperature between 1 and 9 AU is <span class="hlt">observed</span> to decrease as r (the heliocentric radius) to the -(0.7 + or - 0.2). This is slower than would be expected for adiabatic expansion. A detailed examination of the <span class="hlt">solar</span> wind stream structure shows that considerable heating occurs at the interface between high and low speed streams.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140002866','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140002866"><span>Dust in the <span class="hlt">Solar</span> <span class="hlt">System</span> - Properties and Origins</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Messenger, Scott; Keller, Lindsay; Nakamura-Messenger, Keiko</p> <p>2013-01-01</p> <p> include both amorphous and crystalline silicates. The organic matter in these samples also exhibits highly anomalous H, C, and N isotopic compositions that are consistent with formation in low temperature environments at the outermost regions of the <span class="hlt">solar</span> nebula or presolar cold molecular cloud. The scientific frontiers for these samples include working toward a better understanding of the origins of the <span class="hlt">solar</span> <span class="hlt">system</span> amorphous and crystalline grains in IDPs and the very challenging task of determining the chemical composition of sub-micron organic grains. Laboratory studies of ancient and present-day dust in the <span class="hlt">Solar</span> <span class="hlt">System</span> thus reveal in exquisite detail the chemistry, mineralogy and isotopic properties of materials that derive from a range of astrophysical environments. These studies are an important complement to astronomical <span class="hlt">observations</span> that help to place the laboratory <span class="hlt">observations</span> into broader context.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DPS....4910103P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DPS....4910103P"><span><span class="hlt">Solar-system</span> Education for the 2017 Total <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, Jay M.</p> <p>2017-10-01</p> <p>I describe an extensive outreach program about the Sun, the silhouette of the Moon, and the circumstances both celestial and terrestrial of the August 21, 2017, total <span class="hlt">solar</span> eclipse. Publications included a summary of the last decade of <span class="hlt">solar</span>-eclipse research for Nature Astronomy, a Resource Letter on <span class="hlt">Observing</span> <span class="hlt">Solar</span> Eclipses for the American Journal of Physics, and book reviews for Nature and for Phi Beta Kappa's Key Reporter. Symposia arranged include sessions at AAS, APS, AGU, and AAAS. Lectures include all ages from pre-school through elementary school to high school to senior-citizen residences. The work, including the scientific research about the <span class="hlt">solar</span> corona that is not part of this abstract, was supported by grants from the <span class="hlt">Solar</span> Terrestrial Program of the Atmospheric and Geospace Sciences Division of NSF and from the Committee for Research and Exploration of the National Geographic Society. Additional student support was received from NSF, NASA's Massachusetts Space Grant Consortium, the Honorary Research Society Sigma Xi, the Clare Booth Luce Foundation, and funds at Williams College.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...856L..10M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...856L..10M"><span>Heliosphere Responds to a Large <span class="hlt">Solar</span> Wind Intensification: Decisive <span class="hlt">Observations</span> from IBEX</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McComas, D. J.; Dayeh, M. A.; Funsten, H. O.; Heerikhuisen, J.; Janzen, P. H.; Reisenfeld, D. B.; Schwadron, N. A.; Szalay, J. R.; Zirnstein, E. J.</p> <p>2018-03-01</p> <p>Our heliosphere—the bubble in the local interstellar medium produced by the Sun’s outflowing <span class="hlt">solar</span> wind—has finally responded to a large increase in <span class="hlt">solar</span> wind output and pressure in the second half of 2014. NASA’s Interstellar Boundary Explorer (IBEX) mission remotely monitors the outer heliosphere by <span class="hlt">observing</span> energetic neutral atoms (ENAs) returning from the heliosheath, the region between the termination shock and heliopause. IBEX <span class="hlt">observed</span> a significant enhancement in higher energy ENAs starting in late 2016. While IBEX <span class="hlt">observations</span> over the previous decade reflected a general reduction of ENA intensities, indicative of a deflating heliosphere, new <span class="hlt">observations</span> show that the large (∼50%), persistent increase in the <span class="hlt">solar</span> wind dynamic pressure has modified the heliosheath, producing enhanced ENA emissions. The combination of these new <span class="hlt">observations</span> with simulation results indicate that this pressure is re-expanding our heliosphere, with the termination shock and heliopause already driven outward in the locations closest to the Sun. The timing between the IBEX <span class="hlt">observations</span>, a large transient pressure enhancement seen by Voyager 2, and the simulations indicates that the pressure increase propagated through the heliosheath, reflected off the heliopause, and the enhanced density of the <span class="hlt">solar</span> wind filled the heliosheath behind it before generating significantly enhanced ENA emissions. The coming years should see significant changes in anomalous cosmic rays, galactic cosmic radiation, and the filtration of interstellar neutral atoms into the inner heliosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MNRAS.472.2686X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MNRAS.472.2686X"><span>Perihelion precession caused by <span class="hlt">solar</span> oblateness variation in equatorial and ecliptic coordinate <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Yan; Shen, Yunzhong; Xu, Guochang; Shan, Xinjian; Rozelot, Jean-Pierre</p> <p>2017-12-01</p> <p>Analytic solutions of planetary orbits disturbed by <span class="hlt">solar</span> gravitational oblateness have been derived and given in the <span class="hlt">solar</span> equatorial coordinate <span class="hlt">system</span>, although the results usually have to be represented in the ecliptic coordinate <span class="hlt">system</span>. The perihelion precession of interest in the <span class="hlt">solar</span> equatorial and ecliptic coordinate <span class="hlt">systems</span> is partly periodical and not negligible. The result shows that the difference in Mercury's perihelion precession between the <span class="hlt">solar</span> equatorial plane and the ecliptic plane can reach a magnitude of 126708J2, which is even bigger than the perihelion precession itself (101516J2). Due to the temporal variability of the oblateness, the periodic variation of the J2 term, instead of simply a constant, is taken into account and solutions are derived. In the case of Mercury, the periodic J2 has an effect of nearly 0.8 per cent of the secular perihelion precession of Mercury. This indicates that a better understanding of the <span class="hlt">solar</span> oblateness is required, which could be done through <span class="hlt">observation</span> in the <span class="hlt">solar</span> orbits instead of on Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhDT........15K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhDT........15K"><span>First <span class="hlt">observation</span> of beryllium-7 <span class="hlt">solar</span> neutrinos with KamLAND</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Keefer, Gregory J.</p> <p>2009-09-01</p> <p>The international KamLAND collaboration operates a 1 kton liquid scintillation detector in the Kamioka mine in Gifu, Japan. KamLAND's main scientific results are the precision measurement of the <span class="hlt">solar</span> Dm 2 12 = 7.58[Special characters omitted.] (stat) [Special characters omitted.] (syst) and tan 2 [straight theta] 12 = 0.56[Special characters omitted.] (stat) [Special characters omitted.] (syst) utilizing reactor n e and first evidence for the <span class="hlt">observation</span> of geologically produced anti-neutrinos. In an effort to extend KamLAND's scientific reach, extensive research has been performed on preparing a spectroscopic measurement of 7 Be <span class="hlt">solar</span> n e s. This work provides the first inclusive analysis of KamLAND's backgrounds below 1 MeV. 85 Kr and 210 Pb, dissolved in KamLAND liquid scintillator, were found to be the dominant source of low energy backgrounds. The concentration of these ultra-trace contaminants were determined to be 10 -20 g/g. This is more than 6 orders of magnitude lower than commercially available ultra-pure liquids. To attain a signal-to-background ratio suitable for the detection of 7 Be <span class="hlt">solar</span> n e s, the concentration of these contaminants had to be reduced by 5 orders of magnitude. A comprehensive study of 210 Pb removal was undertaken over the course of this thesis. This work further covers techniques for the removal of 220 Rn, 222 Rn and their daughter nuclei from liquid scintillator at concentrations of 10^-18 g/g. Purification techniques studied in this work include water extraction, isotope exchange, adsorption, and distillation. These laboratory studies guided the design and implementation of a large scale purification <span class="hlt">system</span> in the Kamioka mine. The purification <span class="hlt">system</span>'s design and operation is discussed in detail as well as specific experiments devised to control scintillator quality and radio-purity. The purification <span class="hlt">system</span>'s effectiveness in removing radioactive trace impurities is analyzed in detail. The total scintillator purified over two</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002cosp...34E2215C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002cosp...34E2215C"><span><span class="hlt">Solar</span> particle events <span class="hlt">observed</span> at Mars: dosimetry measurements and model calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cleghorn, T.; Saganti, P.; Zeitlin, C.; Cucinotta, F.</p> <p></p> <p>The first <span class="hlt">solar</span> particle events from a Martian orbit are <span class="hlt">observed</span> 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 <span class="hlt">solar</span> particle events <span class="hlt">observed</span> 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 <span class="hlt">observed</span> on March 16t h through 20t h and on April 22n d corresponding to <span class="hlt">solar</span> particle events that were <span class="hlt">observed</span> 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 <span class="hlt">observed</span> by the MARIE instrument are within 10% of the model calculations. Dosimetry measurements and model calculation will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApJ...824L..23B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApJ...824L..23B"><span><span class="hlt">Observational</span> Constraints on the Orbit and Location of Planet Nine in the Outer <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brown, Michael E.; Batygin, Konstantin</p> <p>2016-06-01</p> <p>We use an extensive suite of numerical simulations to constrain the mass and orbit of Planet Nine, the recently proposed perturber in a distant eccentric orbit in the outer <span class="hlt">solar</span> <span class="hlt">system</span>. We compare our simulations to the <span class="hlt">observed</span> population of aligned eccentric high semimajor axis Kuiper belt objects (KBOs) and determine which simulation parameters are statistically compatible with the <span class="hlt">observations</span>. We find that only a narrow range of orbital elements can reproduce the <span class="hlt">observations</span>. In particular, the combination of semimajor axis, eccentricity, and mass of Planet Nine strongly dictates the semimajor axis range of the orbital confinement of the distant eccentric KBOs. Allowed orbits, which confine KBOs with semimajor axis beyond 380 au, have perihelia roughly between 150 and 350 au, semimajor axes between 380 and 980 au, and masses between 5 and 20 Earth masses. Orbitally confined objects also generally have orbital planes similar to that of the planet, suggesting that the planet is inclined approximately 30°to the ecliptic. We compare the allowed orbital positions and estimated brightness of Planet Nine to previous and ongoing surveys which would be sensitive to the planet’s detection and use these surveys to rule out approximately two-thirds of the planet’s orbit. Planet Nine is likely near aphelion with an approximate brightness of 22< V< 25. At opposition, its motion, mainly due to parallax, can easily be detected within 24 hours.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E.787H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E.787H"><span><span class="hlt">Observations</span> of a <span class="hlt">solar</span> storm from the stratosphere: The BARREL Mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Halford, Alexa</p> <p>2016-07-01</p> <p>During the Balloon Array for Radiation belt Relativistic Electron Losses (BARREL) second campaign, BARREL <span class="hlt">observed</span> with a single primary instrument, a 3"x3" NaI spectrometer measuring 20 keV - 10 MeV X-rays [Woodger et al 2015 JGR], portions of an entire <span class="hlt">solar</span> storm. This very small event, in terms of geomagnetic activity, or one of the largest of the current <span class="hlt">solar</span> cycle, in terms of <span class="hlt">solar</span> energetic particle events, has given us a very clear set of <span class="hlt">observations</span> of the response of the day side magnetosphere to the arrival of an interplanetary coronal mass ejection shock. The BARREL mission of opportunity working in tandem with the Van Allen Probes was designed to study the loss of radiation belt electrons to the ionosphere and upper atmosphere. However BARREL is able to see X-rays from a multitude of sources. During the second campaign, the Sun produced, and BARREL <span class="hlt">observed</span>, an X-class flare [McGregor et al in prep.]. This was followed by BARREL <span class="hlt">observations</span> of X-rays, gamma-rays, and directly injected protons from the <span class="hlt">solar</span> energetic particle (SEP) event associated with the eruption from the Sun while simultaneously the Van Allen Probes <span class="hlt">observed</span> the SEP protons in the inner magnetosphere [Halford et al 2016 submitted JGR]. Two days later the shock generated by the interplanetary coronal mass ejection (ICME-shock) hit the Earth while BARREL was in conjunction with the Van Allen Probes and GOES [Halford et al 2015 JGR]. Although this was a Mars directed CME and the Earth only received a glancing blow [Möstl et al 2015 Nat. Commun., Mays et al 2015 ApJ], the modest compression led to the formation of ultra low frequency (ULF) waves, electromagnetic ion cyclotron (EMIC) waves, and very low frequency (VLF) whistler mode waves [Halford and Mann 2016 submitted to JGR]. The combination of these waves and the enhancement of the local particle population led to precipitation of electrons remotely <span class="hlt">observed</span> by BARREL. This was not a Halloween, Bastille Day, or one of the now</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=solar+AND+radiation&pg=5&id=ED166008','ERIC'); return false;" href="https://eric.ed.gov/?q=solar+AND+radiation&pg=5&id=ED166008"><span>Basics of <span class="hlt">Solar</span> Heating & Hot Water <span class="hlt">Systems</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>American Inst. of Architects, Washington, DC.</p> <p></p> <p>In presenting the basics of <span class="hlt">solar</span> heating and hot water <span class="hlt">systems</span>, this publication is organized from the general to the specific. It begins by presenting functional and operational descriptions of <span class="hlt">solar</span> heating and domestic hot water <span class="hlt">systems</span>, outlining the basic concepts and terminology. This is followed by a description of <span class="hlt">solar</span> energy utilization…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010cosp...38.4039M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38.4039M"><span>Electron Radiation Belts of the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mauk, Barry; Fox, Nicola</p> <p></p> <p>To address the question of what factors dictate similarities and differences between radiation belts, we present comparisons between the electron radiation belt spectra of all five strongly magnetized planets within the <span class="hlt">solar</span> <span class="hlt">system</span>: Earth, Jupiter, Saturn, Uranus, and Neptune. We choose the highest intensity <span class="hlt">observed</span> electron spectrum within each <span class="hlt">system</span> (highest specifically near 1 MeV) and compare them against expectations based on the so-called Kennel-Petschek limit (KP; 1966) for each <span class="hlt">system</span>. For evaluating the KP limit, we begin with the new relativis-tically correct formulation of Summers et al. (2009) but then add several refinements of our own. Specifically, we: 1) utilized a much more flexible analytic spectral shape that allows us to accurately fit <span class="hlt">observed</span> radiation belt spectra; 2) adopt the point of view that the anisotropy parameter is not a free parameter but must take on a minimal value, as originally proposed by Kennel and Petschek (1966); and 3) examine the differential characteristics of the KP limit along the lines of what Schulz and Davidson (1988) performed for the non-relativistic formula-tion. We find that three factors limit the highest electron radiation belt intensities within <span class="hlt">solar</span> <span class="hlt">system</span> planetary magnetospheres: a) whistler mode interactions that limit spectral intensities to a differential Kennel-Petschek limit (3 planets); b) the absence of robust acceleration pro-cesses associated with injection dynamics (1 planet); and c) material interactions between the radiation particles and clouds of gas and dust (1 planet).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EOSTr..83R.322S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EOSTr..83R.322S"><span>Panel proposes <span class="hlt">solar</span> <span class="hlt">system</span> missions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Showstack, Randy</p> <p></p> <p>A proposed probe to the Kuiper Belt and Pluto and another to Europa are among the priority <span class="hlt">Solar</span> <span class="hlt">System</span> exploration missions that should be pursued by NASA over the next decade, according to an 11 July report by a steering group of the Space Studies Board of the U.S. National Research Council (NRC).The report, "New Frontiers in the <span class="hlt">Solar</span> <span class="hlt">System</span>: An Integrated Exploration Strategy," was requested by NASA, and proposes a set of new missions and facilities to respond to key questions in four cross-cutting themes. The themes, which the report indicates form the basis for an integrated space exploration strategy are: the first billion years of <span class="hlt">Solar</span> <span class="hlt">System</span> history; volatiles and organics: the stuff of life; the origin and evolution of habitable worlds; and processes: how planets work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10565E..0RS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10565E..0RS"><span>Optical and thermal design of 1.5-m aperture <span class="hlt">solar</span> UV visible and IR <span class="hlt">observing</span> telescope for <span class="hlt">Solar</span>-C mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suematsu, Y.; Katsukawa, Y.; Shimizu, T.; Ichimoto, K.; Horiuchi, T.; Matsumoto, Y.; Takeyama, N.</p> <p>2017-11-01</p> <p>The next Japanese <span class="hlt">solar</span> mission, <span class="hlt">SOLAR</span>-C, which has been envisaged after successful science operation of Hinode (<span class="hlt">SOLAR</span>-B) mission, is perusing two plans: plan-A and plan-B, and under extensive study from science objectives as well as engineering point of view. The plan-A aims at performing out-of-ecliptic <span class="hlt">observations</span> for investigating, with helioseismic approach, internal structure and dynamo mechanisms of the Sun. It also explores polar regions where fast <span class="hlt">solar</span> wind is believed to originate. A baseline orbit for plan-A is a circular orbit of 1 AU distance from the Sun with its inclination at around or greater than 40 degrees. The plan-B aims to study small-scale plasma processes and structures in the <span class="hlt">solar</span> atmosphere which attract researchers' growing interest, followed by many Hinode discoveries [1], for understanding fully dynamism and magnetic nature of the atmosphere. With plan-B, high-angular-resolution investigation of the entire <span class="hlt">solar</span> atmosphere (from the photosphere to the corona, including their interface layers, i.e., chromosphere and transition region) is to be performed with enhanced spectroscopic and spectro-polarimetric capability as compared with Hinode, together with enhanced sensitivity towards ultra-violet wavelengths. The orbit of plan-B is either a <span class="hlt">solar</span> synchronous polar orbit of altitude around 600 km or a geosynchronous orbit to ensure continuous <span class="hlt">solar</span> <span class="hlt">observations</span>. After the decision of any one of the two plans, the <span class="hlt">SOLAR</span>-C will be proposed for launch in mid-2010s. In this paper, we will present a basic design of one of major planned instrumental payload for the plan-B: the <span class="hlt">Solar</span> Ultra-violet Visible and near IR <span class="hlt">observing</span> Telescope (hereafter referred to as SUVIT). The basic concept in designing the SUVIT is to utilize as much as possible a heritage of successful telescope of the <span class="hlt">Solar</span> Optical Telescope (SOT) aboard Hinode [2]. Major differences of SUVIT from SOT are the three times larger aperture of 1.5 m, which enables to collect one</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..APR.L1002C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..APR.L1002C"><span><span class="hlt">Observation</span> of freakish-asteroid-discovered-resembles support my idea that many dark comets were arrested and lurked in the <span class="hlt">solar</span> <span class="hlt">system</span> after every impaction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cao, Dayong</p> <p>2014-03-01</p> <p>New <span class="hlt">observations</span> show that some asteroids are looked like comets. http://www.astrowatch.net/2013/11/freakish-asteroid-discovered-resembles.html, http://www.astrowatch.net/2013/11/astronomers-puzzle-over-newfound.html. It supports my idea that ``many dark comets with very special tilted orbits were arrested and lurked in the <span class="hlt">solar</span> <span class="hlt">system</span>'' - ``Sun's companion-dark hole seasonal took its dark comets belt and much dark matter to impact near our earth. And some of them probability hit on our earth. So this model kept and triggered periodic mass extinctions on our earth every 25 to 27 million years. After every impaction, many dark comets with very special tilted orbits were arrested and lurked in the <span class="hlt">solar</span> <span class="hlt">system</span>. Because some of them picked up many <span class="hlt">solar</span> matter, so it looked like the asteroids. When the dark hole-Tyche goes near the <span class="hlt">solar</span> <span class="hlt">system</span> again, they will impact near planets.'' The idea maybe explains why do the asteroid looks like the comet? Where are the asteroids come from? What relationship do they have with the impactions and extinctions? http://meetings.aps.org/link/BAPS.2011.CAL.C1.7, http://meetings.aps.org/Meeting/CAL12/Event/181168, http://meetings.aps.org/link/BAPS.2013.MAR.H1.267. During 2009 to 2010, I had presented there are many dark comets like dark Asteroids near the orbit of Jupiter in ASP Meetings. In 2010, NASA's WISE found them. http://meetings.aps.org/link/BAPS.2011.APR.K1.17, http://www.nasa.gov/mission_pages/WISE/news/wise20100122.html Avoid Earth Extinction Associ.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22356468-solar-wind-neon-abundance-observed-ace-swics-ulysses-swics','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22356468-solar-wind-neon-abundance-observed-ace-swics-ulysses-swics"><span>The <span class="hlt">solar</span> wind neon abundance <span class="hlt">observed</span> with ACE/SWICS and ULYSSES/SWICS</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>Shearer, Paul; Raines, Jim M.; Lepri, Susan T.</p> <p></p> <p>Using in situ ion spectrometry data from ACE/SWICS, we determine the <span class="hlt">solar</span> wind Ne/O elemental abundance ratio and examine its dependence on wind speed and evolution with the <span class="hlt">solar</span> cycle. We find that Ne/O is inversely correlated with wind speed, is nearly constant in the fast wind, and correlates strongly with <span class="hlt">solar</span> activity in the slow wind. In fast wind streams with speeds above 600 km s{sup –1}, we find Ne/O = 0.10 ± 0.02, in good agreement with the extensive polar <span class="hlt">observations</span> by Ulysses/SWICS. In slow wind streams with speeds below 400 km s{sup –1}, Ne/O ranges from amore » low of 0.12 ± 0.02 at <span class="hlt">solar</span> maximum to a high of 0.17 ± 0.03 at <span class="hlt">solar</span> minimum. These measurements place new and significant empirical constraints on the fractionation mechanisms governing <span class="hlt">solar</span> wind composition and have implications for the coronal and photospheric abundances of neon and oxygen. The results are made possible by a new data analysis method that robustly identifies rare elements in the measured ion spectra. The method is also applied to Ulysses/SWICS data, which confirms the ACE <span class="hlt">observations</span> and extends our view of <span class="hlt">solar</span> wind neon into the three-dimensional heliosphere.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH41A2749N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH41A2749N"><span>Statistical and <span class="hlt">observational</span> research of <span class="hlt">solar</span> flare for total spectra and geometrical features</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nishimoto, S.; Watanabe, K.; Imada, S.; Kawate, T.; Lee, K. S.</p> <p>2017-12-01</p> <p>Impulsive energy release phenomena such as <span class="hlt">solar</span> flares, sometimes affect to the <span class="hlt">solar</span>-terrestrial environment. Usually, we use soft X-ray flux (GOES class) as the index of flare scale. However, the magnitude of effect to the <span class="hlt">solar</span>-terrestrial environment is not proportional to that scale. To identify the relationship between <span class="hlt">solar</span> flare phenomena and influence to the <span class="hlt">solar</span>-terrestrial environment, we need to understand the full spectrum of <span class="hlt">solar</span> flares. There is the <span class="hlt">solar</span> flare irradiance model named the Flare Irradiance Spectral Model (FISM) (Chamberlin et al., 2006, 2007, 2008). The FISM can estimate <span class="hlt">solar</span> flare spectra with high wavelength resolution. However, this model can not express the time evolution of emitted plasma during the <span class="hlt">solar</span> flare, and has low accuracy on short wavelength that strongly effects and/or controls the total flare spectra. For the purpose of obtaining the time evolution of total <span class="hlt">solar</span> flare spectra, we are performing statistical analysis of the electromagnetic data of <span class="hlt">solar</span> flares. In this study, we select <span class="hlt">solar</span> flare events larger than M-class from the Hinode flare catalogue (Watanabe et al., 2012). First, we focus on the EUV emission <span class="hlt">observed</span> by the SDO/EVE. We examined the intensities and time evolutions of five EUV lines of 55 flare events. As a result, we found positive correlation between the "soft X-ray flux" and the "EUV peak flux" for all EVU lines. Moreover, we found that hot lines peaked earlier than cool lines of the EUV light curves. We also examined the hard X-ray data obtained by RHESSI. When we analyzed 163 events, we found good correlation between the "hard X-ray intensity" and the "soft X-ray flux". Because it seems that the geometrical features of <span class="hlt">solar</span> flares effect to those time evolutions, we also looked into flare ribbons <span class="hlt">observed</span> by SDO/AIA. We examined 21 flare events, and found positive correlation between the "GOES duration" and the "ribbon length". We also found positive correlation between the "ribbon</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030055661&hterms=Solar+system+facts&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSolar%2Bsystem%2Bfacts','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030055661&hterms=Solar+system+facts&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSolar%2Bsystem%2Bfacts"><span><span class="hlt">Observational</span> Investigation of <span class="hlt">Solar</span> Interior and Atmosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuhn, Jeffrey R.</p> <p>2003-01-01</p> <p>The Imaging Vector Magnetograph (IVM) has been modified to make it easier to <span class="hlt">observe</span> at more than one spectral line. The cell holding the blocking filter has been replaced by a four-position filter wheel, so that changing to a different line is a matter of a few minutes rather than the several hours it used to take to disassemble the cell and install a new filter. Three new filters have been obtained, for Na 1589.6 nm, Fe 1630.25 nm, and H 1656.3 nm. The new filters have better bandpass profiles than the ones they replaced: somewhat wider, with flatter tops and steeper wings. This results in a reduction of parasitic light coming from adjacent Fabry-Perot orders, from seven percent to about two percent, and flattens the apparent continuum. The Mees CCD Imaging Spectrograph (MCCD) was upgraded under this grant, with a new control computer and data <span class="hlt">system</span>. The camera was replaced with a faster, larger-format frame-transfer camera. Final integration of the upgrades is not yet complete, but tests indicate that the <span class="hlt">system</span> cadence will be improved by a factor of five to ten, while increasing the spatial coverage by a factor of two (depending on <span class="hlt">observation</span> options). Synoptic <span class="hlt">observations</span> with the IVM and MCCD continue to be conducted daily, to the extent permitted by the fact that we have a single <span class="hlt">observer</span> responsible for the <span class="hlt">observations</span>. The older Haleakala Stokes Polarimeter is also used to make a daily vector magnetogram, normally of the region selected by the Reuven Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager (RHESSI) duty scientists. This instrument, however, is showing its age to the extent that its maintenance is becoming something of a challenge. We also run a white light full-disk imager and a video H alpha prominence camera, continuously during times of <span class="hlt">observations</span>. Of particular interest, we obtained rapid-cadence <span class="hlt">observations</span> of the 2003 July 15 white light flare with both the IVM and MCCD. The vector magnetograms show no obvious difference between the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740054880&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DExciter','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740054880&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DExciter"><span>Satellite <span class="hlt">observations</span> of type III <span class="hlt">solar</span> radio bursts at low frequencies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fainberg, J.; Stone, R. G.</p> <p>1974-01-01</p> <p>Type III <span class="hlt">solar</span> radio bursts have been <span class="hlt">observed</span> from 10 MHz to 10 kHz by satellite experiments above the terrestrial plasmasphere. <span class="hlt">Solar</span> radio emission in this frequency range results from excitation of the interplanetary plasma by energetic particles propagating outward along open field lines over distances from 5 earth radii to at least 1 AU from the sun. This review summarizes the morphology, characteristics, and analysis of individual as well as storms of bursts. Substantial evidence is available to show that the radio emission is <span class="hlt">observed</span> at the second harmonic instead of the fundamental of the plasma frequency. This brings the density scale derived by radio <span class="hlt">observations</span> into better agreement with direct <span class="hlt">solar</span> wind density measurements at 1 AU and relaxes the requirement for type III propagation along large density-enhanced regions. This density scale with the measured direction of arrival of the radio burst allows the trajectory of the exciter path to be determined from 10 earth radii to 1 AU.</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/1999AAS...194.8003A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999AAS...194.8003A"><span>YOHKOH <span class="hlt">Observations</span> at the Y2K <span class="hlt">Solar</span> Maximum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aschwanden, M. J.</p> <p>1999-05-01</p> <p>Yohkoh will provide simultaneous co-aligned soft X-ray and hard X-ray <span class="hlt">observations</span> of <span class="hlt">solar</span> flares at the coming <span class="hlt">solar</span> maximum. The Yohkoh Soft X-ray Telescope (SXT) covers the approximate temperature range of 2-20 MK with a pixel size of 2.46\\arcsec, and thus complements ideally the EUV imagers sensitive in the 1-2 MK plasma, such as SoHO/EIT and TRACE. The Yohkoh Hard X-ray Telescope (HXT) offers hard X-ray imaging at 20-100 keV at a time resolution of down to 0.5 sec for major events. In this paper we review the major SXT and HXT results from Yohkoh <span class="hlt">solar</span> flare <span class="hlt">observations</span>, and anticipate some of the key questions that can be addressed through joint <span class="hlt">observations</span> with other ground and space-based observatories. This encompasses the dynamics of flare triggers (e.g. emerging flux, photospheric shear, interaction of flare loops in quadrupolar geometries, large-scale magnetic reconfigurations, eruption of twisted sigmoid structures, coronal mass ejections), the physics of particle dynamics during flares (acceleration processes, particle propagation, trapping, and precipitation), and flare plasma heating processes (chromospheric evaporation, coronal energy loss by nonthermal particles). In particular we will emphasize on how Yohkoh data analysis is progressing from a qualitative to a more quantitative science, employing 3-dimensional modeling and numerical simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.6000S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.6000S"><span>Interaction between <span class="hlt">Solar</span> Wind and Lunar Magnetic Anomalies <span class="hlt">observed</span> by Kaguya MAP-PACE</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saito, Yoshifumi; Yokota, Shoichiro; Tanaka, Takaaki; Asamura, Kazushi; Nishino, Masaki; Yamamoto, Tadateru; Uemura, Kota; Tsunakawa, Hideo</p> <p>2010-05-01</p> <p>It is known that Moon has neither global intrinsic magnetic field nor thick atmosphere. Different from the Earth's case where the intrinsic global magnetic field prevents the <span class="hlt">solar</span> wind from penetrating into the magnetosphere, <span class="hlt">solar</span> wind directly impacts the lunar surface. Since the discovery of the lunar crustal magnetic field in 1960s, several papers have been published concerning the interaction between the <span class="hlt">solar</span> wind and the lunar magnetic anomalies. MAG/ER on Lunar Prospector found heating of the <span class="hlt">solar</span> wind electrons presumably due to the interaction between the <span class="hlt">solar</span> wind and the lunar magnetic anomalies and the existence of the mini-magnetosphere was suggested. However, the detailed mechanism of the interaction has been unclear mainly due to the lack of the in-situ <span class="hlt">observed</span> data of low energy ions. MAgnetic field and Plasma experiment - Plasma energy Angle and Composition Experiment (MAP-PACE) on Kaguya (SELENE) completed its ˜1.5-year <span class="hlt">observation</span> of the low energy charged particles around the Moon on 10 June, 2009. Kaguya was launched on 14 September 2007 by H2A launch vehicle from Tanegashima Space Center in Japan. Kaguya was inserted into a circular lunar polar orbit of 100km altitude and continued <span class="hlt">observation</span> for nearly 1.5 years till it impacted the Moon on 10 June 2009. During the last 5 months, the orbit was lowered to ˜50km-altitude between January 2009 and April 2009, and some orbits had further lower perilune altitude of ˜10km after April 2009. MAP-PACE consisted of 4 sensors: ESA (Electron Spectrum Analyzer)-S1, ESA-S2, IMA (Ion Mass Analyzer), and IEA (Ion Energy Analyzer). All the sensors performed quite well as expected from the laboratory experiment carried out before launch. Since each sensor had hemispherical field of view, two electron sensors and two ion sensors that were installed on the spacecraft panels opposite to each other could cover full 3-dimensional phase space of low energy electrons and ions. One of the ion sensors IMA was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JGRD..118.9552Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JGRD..118.9552Z"><span>Correcting surface <span class="hlt">solar</span> radiation of two data assimilation <span class="hlt">systems</span> against FLUXNET <span class="hlt">observations</span> in North America</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Lei; Lee, Xuhui; Liu, Shoudong</p> <p>2013-09-01</p> <p><span class="hlt">Solar</span> radiation at the Earth's surface is an important driver of meteorological and ecological processes. The objective of this study is to evaluate the accuracy of the reanalysis <span class="hlt">solar</span> radiation produced by NARR (North American Regional Reanalysis) and MERRA (Modern-Era Retrospective Analysis for Research and Applications) against the FLUXNET measurements in North America. We found that both assimilation <span class="hlt">systems</span> systematically overestimated the surface <span class="hlt">solar</span> radiation flux on the monthly and annual scale, with an average bias error of +37.2 Wm-2 for NARR and of +20.2 Wm-2 for MERRA. The bias errors were larger under cloudy skies than under clear skies. A postreanalysis algorithm consisting of empirical relationships between model bias, a clearness index, and site elevation was proposed to correct the model errors. Results show that the algorithm can remove the systematic bias errors for both FLUXNET calibration sites (sites used to establish the algorithm) and independent validation sites. After correction, the average annual mean bias errors were reduced to +1.3 Wm-2 for NARR and +2.7 Wm-2 for MERRA. Applying the correction algorithm to the global domain of MERRA brought the global mean surface incoming shortwave radiation down by 17.3 W m-2 to 175.5 W m-2. Under the constraint of the energy balance, other radiation and energy balance terms at the Earth's surface, estimated from independent global data products, also support the need for a downward adjustment of the MERRA surface <span class="hlt">solar</span> radiation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT........33K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT........33K"><span>Extreme Worlds of the Outer <span class="hlt">Solar</span> <span class="hlt">System</span>: Dynamic Processes on Uranus & Io</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kleer, Katherine Rebecca de</p> <p></p> <p> <span class="hlt">system</span> outliers through studies of Uranus' atmosphere and rings and of Io's thermal activity. I show that Uranus' rings are spectrally flat in the near-infrared, setting them apart from all other ring <span class="hlt">systems</span> in the <span class="hlt">solar</span> <span class="hlt">system</span>. I investigate the vertical profile of species in Uranus' atmosphere, and demonstrate evidence for seasonal trends in the upper atmosphere on decadal timescales. Based on a large high-cadence dataset of Io's volcanism obtained with adaptive optics over 100 nights, I show that the thermal timelines of Io's volcanoes indicate at least two distinct classes of eruption. The asymmetric spatial distribution of Io's volcanic heat flow suggests additional mechanisms at work modulating the effects of tidal heating. I present the detection of one of the most powerful eruptions ever seen on Io, which I use to derive a eruption temperature of >1300 K, consistent with a highly mafic magma composition. Geophysical modeling of the thermal timeline of Loki Patera, a distinctive volcanic feature on Io, indicates low lava thermal conductivities also consistent with a highly-mafic silicate composition. Ultra-high-resolution thermal mapping of this patera reveals a multi-phase volcanic resurfacing process that hints at the plumbing <span class="hlt">system</span> underlying this massive volcanic feature. The results presented here are founded on near-infrared <span class="hlt">observations</span> of unprecedented resolution in the spatial, spectral, and temporal domains. The interpretation of the data utilizes rigorous statistical techniques to draw meaningful conclusions. In addition to the scientific impact of the findings, this work therefore also pioneers specific ground-based telescope capabilities and analysis tools, and demonstrates their utility to <span class="hlt">solar</span> <span class="hlt">system</span> science. Chapter 2 presents the first high-resolution spectra of Uranus' rings. Chapter 3 introduces Markov Chain Monte Carlo simulations into ice giant atmospheric radiative transfer model- ing, permitting a rigorous analysis of parameter</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.4109M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.4109M"><span>Work on a New <span class="hlt">Solar-System</span> Ephemeris: 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>Mai, Enrico; Müller, Jürgen</p> <p>2014-05-01</p> <p>Currently, within a coordinated project in Germany, integrated methods and procedures for a consistent definition and realization of reference <span class="hlt">systems</span> on Earth and in space are being developed. Barycentric ephemerides represent a dynamical realization of the Barycentric Celestial Reference <span class="hlt">System</span> (BCRS), which is fundamental not only for the problem of interplanetary navigation but through its intimate relation to the Geocentric Celestial Reference <span class="hlt">System</span> (GCRS). In accordance with existing renowned ephemerides (INPOP, DE, EPM) we want to lay the foundation for a new <span class="hlt">solar-system</span> ephemeris. We collected available <span class="hlt">observational</span> data for the planets as well as high-precise tracking data to various spacecrafts (interplanetary probes, planetary orbiters and landers). Furthermore, we set up the usual relativistic (post-Newtonian) force model in line with the latest French INPOP ephemeris, with a few exceptions. The focus in modeling is on the lunar librations and asteroid perturbations. Regarding the treatment of the Moon, we draw upon the elaborated modeling within the existing LLR analysis software at IfE and its ongoing improvements. Nowadays, any modern ephemeris, besides perturbations due to general mass inhomogeneities (at least for the Earth and the Moon) and <span class="hlt">solar</span> flattening, respective figure-figure interactions and tidal effects, proper rotations and librations etc., has to account for the significant gravitational effect of the vast number of minor bodies in the <span class="hlt">solar-system</span> (especially within the major asteroid belt between Mars and Jupiter) on the long-term evolution of planetary orbits. Due to limited computational resources, one is able to integrate the equations of motion (EOM) of only a comparatively small selection of asteroids simultaneously with the EOM of the major <span class="hlt">solar-system</span> bodies (i.e., planets, Sun, Moon). On the other hand, one can efficiently account for the remaining asteroids by the introduction of at least one mass ring, the parameters of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11538135','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11538135"><span>The search for extra-<span class="hlt">solar</span> planetary <span class="hlt">systems</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Paresce, F</p> <p>1992-01-01</p> <p>I review the <span class="hlt">observational</span> evidence for planetary <span class="hlt">systems</span> around nearby stars and, using our own <span class="hlt">solar</span> <span class="hlt">system</span> as a guide, assess the stringent requirements that new searches need to meet in order to unambiguously establish the presence of another planetary <span class="hlt">system</span>. Basically, these requirements are: 1 milliarcsecond or better positional accuracy for astrometric techniques, 9 orders of magnitude or better star to planet luminosity ratio discrimination at 0.5 to 1" separation in the optical for direct imaging techniques, 10 meters sec-1 or better radial velocity accuracy for reflex motion techniques and +/-1% or better brightness fluctuation accuracy for planet/star occultation measurements. The astrometric accuracy is in reach of HST, direct imaging will require much larger telescopes and/or a 50 times smoother mirror than HST while the reflex motion and occultation techniques best performed on the ground are just becoming viable and promise exciting new discoveries. On the other band, new indirect evidence on the existence of other planetary <span class="hlt">systems</span> also comes from the <span class="hlt">observation</span> of large dusty disks around nearby main sequence stars not too dissimilar from our sun. In one particular case, that of Beta Pictoris, a flattened disk seen nearly edge-on has been imaged in the optical and near IR down to almost 70 AU of the star. It probably represents a young planetary <span class="hlt">system</span> in its clearing out phase as planetesimals collide, erode and are swept out of the inner <span class="hlt">system</span> by radiation pressure. The hypothesized Kuiper belt around our <span class="hlt">solar</span> <span class="hlt">system</span> may be the analogous structure in a later evolutionary stage. Features of this type have been detected in the far IR and sub-millimeter wavelength regions around 50-100 nearby main sequence and pre-main sequence stars. I discuss a battery of new accurate <span class="hlt">observations</span> planned in the near future of these objects some of which may actually harbour planets or planetesimals that will certainly dramatically improve our knowledge of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110007799','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110007799"><span>Did Cosmology Trigger the Origin of the <span class="hlt">Solar</span> <span class="hlt">System</span>?</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Blome, H.-J.; Wilson, T. L.</p> <p>2011-01-01</p> <p>It is a matter of curious coincidence that the <span class="hlt">Solar</span> <span class="hlt">System</span> formed 4.6 billion years ago around the same epoch that the Friedmann-Lemaitre (FL) universe became -dominated or dark-energy-dominated, where is the cosmological constant. This <span class="hlt">observation</span> was made in the context of known gravitational anomalies that affect spacecraft orbits during planetary flyby's and the Pioneer anomaly, both possibly having connections with cosmology. In addition, it has been known for some time that the Universe is not only expanding but accelerating as well. Hence one must add the onset of cosmological acceleration in the FL universe as having a possible influence on the origin of the <span class="hlt">Solar</span> <span class="hlt">System</span>. These connections will now be examined in greater detail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880002239','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880002239"><span>Large-scale horizontal flows from SOUP <span class="hlt">observations</span> of <span class="hlt">solar</span> granulation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>November, L. J.; Simon, G. W.; Tarbell, T. D.; Title, A. M.; Ferguson, S. H.</p> <p>1987-01-01</p> <p>Using high resolution time sequence photographs of <span class="hlt">solar</span> granulation from the SOUP experiment on Spacelab 2, large scale horizontal flows were <span class="hlt">observed</span> in the <span class="hlt">solar</span> surface. The measurement method is based upon a local spatial cross correlation analysis. The horizontal motions have amplitudes in the range 300 to 1000 m/s. Radial outflow of granulation from a sunspot penumbra into surrounding photosphere is a striking new discovery. Both the supergranulation pattern and cellular structures having the scale of mesogranulation are seen. The vertical flows that are inferred by continuity of mass from these <span class="hlt">observed</span> horizontal flows have larger upflow amplitudes in cell centers than downflow amplitudes at cell boundaries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987NASCP2483..121N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987NASCP2483..121N"><span>Large-scale horizontal flows from SOUP <span class="hlt">observations</span> of <span class="hlt">solar</span> granulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>November, L. J.; Simon, G. W.; Tarbell, T. D.; Title, A. M.; Ferguson, S. H.</p> <p>1987-09-01</p> <p>Using high-resolution time-sequence photographs of <span class="hlt">solar</span> granulation from the SOUP experiment on Spacelab 2 the authors <span class="hlt">observed</span> large-scale horizontal flows in the <span class="hlt">solar</span> surface. The measurement method is based upon a local spatial cross correlation analysis. The horizontal motions have amplitudes in the range 300 to 1000 m/s. Radial outflow of granulation from a sunspot penumbra into the surrounding photosphere is a striking new discovery. Both the supergranulation pattern and cellular structures having the scale of mesogranulation are seen. The vertical flows that are inferred by continuity of mass from these <span class="hlt">observed</span> horizontal flows have larger upflow amplitudes in cell centers than downflow amplitudes at cell boundaries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930004279','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930004279"><span><span class="hlt">Observations</span> of <span class="hlt">solar</span> wind ion charge exchange in the comet Halley coma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fuselier, S. A.; Shelley, E. G.; Goldstein, B. E.; Goldstein, R.; Neugebauer, M.; Ip, W.-H.; Balsiger, H.; Reme, H.</p> <p>1991-01-01</p> <p>Giotto Ion Mass Spectrometer/High Energy Range Spectrometer (IMS/HERS) <span class="hlt">observations</span> of <span class="hlt">solar</span> wind ions show charge exchange effects and <span class="hlt">solar</span> wind compositional changes in the coma of comet Halley. As the comet was approached, the He(++) to proton density ratio increased until about 1 hour before closest approach after which time it decreased. Abrupt increases in this ratio were also <span class="hlt">observed</span> in the beginning and near the end of the so-called Mystery Region (8.6 - 5.5(10)(exp 5) km from the comet along the spacecraft trajectory). These abrupt increases in the density ratio were well correlated with enhanced fluxes of keV electrons as measured by the Giotto plasma electron spectrometer. The general increase and then decrease of the He(++) to proton density ratio is quantitatively consistent with a combination of the addition of protons of cometary origin to the plasma and loss of plasma through charge exchange of protons and He(++). In general agreement with the <span class="hlt">solar</span> wind proton and He(++) <span class="hlt">observations</span>, <span class="hlt">solar</span> wind oxygen and carbon ions were <span class="hlt">observed</span> to charge exchange from higher to lower charge states with decreasing distance to the comet. The more abrupt increases in the He(++) to proton and the He(++) to O(6+) density ratios in the mystery region require a change in the <span class="hlt">solar</span> wind ion composition in this region while the correlation with energetic electrons indicates processes associated with the comet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018IJE...105..694W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IJE...105..694W"><span><span class="hlt">Solar</span> power generation <span class="hlt">system</span> for reducing leakage current</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Jinn-Chang; Jou, Hurng-Liahng; Hung, Chih-Yi</p> <p>2018-04-01</p> <p>This paper proposes a transformer-less multi-level <span class="hlt">solar</span> power generation <span class="hlt">system</span>. This <span class="hlt">solar</span> power generation <span class="hlt">system</span> is composed of a <span class="hlt">solar</span> cell array, a boost power converter, an isolation switch set and a full-bridge inverter. A unipolar pulse-width modulation (PWM) strategy is used in the full-bridge inverter to attenuate the output ripple current. Circuit isolation is accomplished by integrating the isolation switch set between the <span class="hlt">solar</span> cell array and the utility, to suppress the leakage current. The isolation switch set also determines the DC bus voltage for the full-bridge inverter connecting to the <span class="hlt">solar</span> cell array or the output of the boost power converter. Accordingly, the proposed transformer-less multi-level <span class="hlt">solar</span> power generation <span class="hlt">system</span> generates a five-level voltage, and the partial power of the <span class="hlt">solar</span> cell array is also converted to AC power using only the full-bridge inverter, so the power efficiency is increased. A prototype is developed to validate the performance of the proposed transformer-less multi-level <span class="hlt">solar</span> power generation <span class="hlt">system</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-PIA21428.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-PIA21428.html"><span>TRAPPIST-1 Comparison to <span class="hlt">Solar</span> <span class="hlt">System</span> and Jovian Moons</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2017-02-22</p> <p>All seven planets discovered in orbit around the red dwarf star TRAPPIST-1 could easily fit inside the orbit of Mercury, the innermost planet of our <span class="hlt">solar</span> <span class="hlt">system</span>. In fact, they would have room to spare. TRAPPIST-1 also is only a fraction of the size of our sun; it isn't much larger than Jupiter. So the TRAPPIST-1 <span class="hlt">system</span>'s proportions look more like Jupiter and its moons than those of our <span class="hlt">solar</span> <span class="hlt">system</span>. The seven planets of TRAPPIST-1 are all Earth-sized and terrestrial, according to research published in 2017 in the journal Nature. TRAPPIST-1 is an ultra-cool dwarf star in the constellation Aquarius, and its planets orbit very close to it. The <span class="hlt">system</span> has been revealed through <span class="hlt">observations</span> from NASA's Spitzer Space Telescope and the ground-based TRAPPIST (TRAnsiting Planets and PlanetesImals Small Telescope) telescope, as well as other ground-based observatories. The <span class="hlt">system</span> was named for the TRAPPIST telescope. http://photojournal.jpl.nasa.gov/catalog/PIA21428</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61.2531K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61.2531K"><span><span class="hlt">Observation</span> of a 27-day <span class="hlt">solar</span> signature in noctilucent cloud altitude</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Köhnke, Merlin C.; von Savigny, Christian; Robert, Charles E.</p> <p>2018-05-01</p> <p>Previous studies have identified <span class="hlt">solar</span> 27-day signatures in several parameters in the Mesosphere/Lower thermosphere region, including temperature and Noctilucent cloud (NLC) occurrence frequency. In this study we report on a <span class="hlt">solar</span> 27-day signature in NLC altitude with peak-to-peak variations of about 400 m. We use SCIAMACHY limb-scatter <span class="hlt">observations</span> from 2002 to 2012 to detect NLCs. The superposed epoch analysis method is applied to extract <span class="hlt">solar</span> 27-day signatures. A 27-day signature in NLC altitude can be identified in both hemispheres in the SCIAMACHY dataset, but the signature is more pronounced in the northern hemisphere. The <span class="hlt">solar</span> signature in NLC altitude is found to be in phase with <span class="hlt">solar</span> activity and temperature for latitudes ≳ 70 ° N. We provide a qualitative explanation for the positive correlation between <span class="hlt">solar</span> activity and NLC altitude based on published model simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29773922','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29773922"><span>Trilogy, a Planetary Geodesy Mission Concept for Measuring the Expansion of the <span class="hlt">Solar</span> <span class="hlt">System</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Smith, David E; Zuber, Maria T; Mazarico, Erwan; Genova, Antonio; Neumann, Gregory A; Sun, Xiaoli; Torrence, Mark H; Mao, Dan-Dan</p> <p>2018-04-01</p> <p>The scale of the <span class="hlt">solar</span> <span class="hlt">system</span> is slowly changing, likely increasing as a result of <span class="hlt">solar</span> mass loss, with additional change possible if there is a secular variation of the gravitational constant, G . The measurement of the change of scale could provide insight into the past and the future of the <span class="hlt">solar</span> <span class="hlt">system</span>, and in addition a better understanding of planetary motion and fundamental physics. Estimates for the expansion of the scale of the <span class="hlt">solar</span> <span class="hlt">system</span> are of order 1.5 cm year -1 AU -1 , which over several years is an <span class="hlt">observable</span> quantity with present-day laser ranging <span class="hlt">systems</span>. This estimate suggests that laser measurements between planets could provide an accurate estimate of the <span class="hlt">solar</span> <span class="hlt">system</span> expansion rate. We examine distance measurements between three bodies in the inner <span class="hlt">solar</span> <span class="hlt">system</span> -- Earth's Moon, Mars and Venus -- and outline a mission concept for making the measurements. The concept involves placing spacecraft that carry laser ranging transponders in orbit around each body and measuring the distances between the three spacecraft over a period of several years. The analysis of these range measurements would allow the co-estimation of the spacecraft orbit, planetary ephemerides, other geophysical parameters related to the constitution and dynamics of the central bodies, and key geodetic parameters related to the <span class="hlt">solar</span> <span class="hlt">system</span> expansion, the Sun, and theoretical physics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018P%26SS..153..127S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018P%26SS..153..127S"><span>Trilogy, a planetary geodesy mission concept for measuring the expansion of the <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, David E.; Zuber, Maria T.; Mazarico, Erwan; Genova, Antonio; Neumann, Gregory A.; Sun, Xiaoli; Torrence, Mark H.; Mao, Dan-dan</p> <p>2018-04-01</p> <p>The scale of the <span class="hlt">solar</span> <span class="hlt">system</span> is slowly changing, likely increasing as a result of <span class="hlt">solar</span> mass loss, with additional change possible if there is a secular variation of the gravitational constant, G. The measurement of the change of scale could provide insight into the past and the future of the <span class="hlt">solar</span> <span class="hlt">system</span>, and in addition a better understanding of planetary motion and fundamental physics. Estimates for the expansion of the scale of the <span class="hlt">solar</span> <span class="hlt">system</span> are of order 1.5 cm year-1 AU-1, which over several years is an <span class="hlt">observable</span> quantity with present-day laser ranging <span class="hlt">systems</span>. This estimate suggests that laser measurements between planets could provide an accurate estimate of the <span class="hlt">solar</span> <span class="hlt">system</span> expansion rate. We examine distance measurements between three bodies in the inner <span class="hlt">solar</span> <span class="hlt">system</span> - Earth's Moon, Mars and Venus - and outline a mission concept for making the measurements. The concept involves placing spacecraft that carry laser ranging transponders in orbit around each body and measuring the distances between the three spacecraft over a period of several years. The analysis of these range measurements would allow the co-estimation of the spacecraft orbit, planetary ephemerides, other geophysical parameters related to the constitution and dynamics of the central bodies, and key geodetic parameters related to the <span class="hlt">solar</span> <span class="hlt">system</span> expansion, the Sun, and theoretical physics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...859..121K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...859..121K"><span>Motions in Prominence Barbs <span class="hlt">Observed</span> on the <span class="hlt">Solar</span> Limb</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kucera, T. A.; Ofman, L.; Tarbell, T. D.</p> <p>2018-06-01</p> <p>We analyze and discuss an example of prominence barbs <span class="hlt">observed</span> on the limb on 2016 January 7 by the Hinode/<span class="hlt">Solar</span> Optical Telescope in Ca II and Hα, the Interface Region Imaging Spectrograph, with slit jaw images and Mg II spectral data, and the <span class="hlt">Solar</span> Dynamics Observatory’s Atmospheric Imaging Assembly. In the recent literature there has been a debate concerning whether these features, sometimes referred to as “tornadoes,” are rotating. Our data analysis provides no evidence for systematic rotation in the barbs. We do find line-of-sight motions in the barbs that vary with location and time. We also discuss <span class="hlt">observations</span> of features moving along the barbs. These moving features are elongated parallel to the <span class="hlt">solar</span> limb and tend to come in clusters of features moving along the same or similar paths in the plane of the sky during a period of 10 minutes to an hour, moving toward or away from the limb. The motion may have a component along the line of sight as well. The spectral data indicate that the features are Doppler shifted. We discuss possible explanations for these features.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980017007','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980017007"><span>Stellar Occultation Studies of the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Elliot, James L.</p> <p>1998-01-01</p> <p>Earth-based <span class="hlt">observations</span> of stellar occultations provide extremely high spatial resolution for bodies in the outer <span class="hlt">solar</span> <span class="hlt">system</span>, about 10,000 times better than that of traditional imaging <span class="hlt">observations</span>. Stellar occultation data can be used to establish the structure of atmospheres and rings of <span class="hlt">solar</span> <span class="hlt">system</span> bodies at high spatial resolution. Airborne occultation <span class="hlt">observations</span> are particularly effective, since the controlled mobility of the <span class="hlt">observing</span> platform allows the <span class="hlt">observer</span> to fly within the optimum part of the occultation shadow for most events that are visible from Earth. Airborne <span class="hlt">observations</span> are carried out above any clouds and are nearly free of scintillation noise from the Earth's atmosphere. KAO occultation <span class="hlt">observations</span> resulted in the first detection of gravity waves in the Martian atmosphere, discovery of the Uranian rings, the first detection of Pluto's atmosphere, the first Earth-based investigations of Triton's atmosphere, and the discovery of narrow jets from Chiron's nucleus. The first SOFIA occultation opportunity will be an investigation of Pluto's atmospheric structure in November, 2002, and will resolve a problem that has lingered since the KAO discovery <span class="hlt">observation</span> fourteen years earlier. We plan to continue our successful airborne occultation program with the greatly enhanced capability provided by SOFIA. We propose here to replace our KAO occultation photometer with one having twice the throughput, half the noise, a somewhat wider wavelength range, four times the field of view, and ten times the frame rate to optimize its performance and to capitalize on the larger collecting area offered by SOFIA. It will also allow for simultaneous visible and IR occultation <span class="hlt">observations</span>, greatly enriching the results that we can obtain from occultations. We call this new imaging occultation photometer HOPI (High-speed Occultation Photometer and Imager). HOPI will provide a signal-to-noise ratio two to four times that of our present photometer for a given</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810000147&hterms=Solar+Energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DSolar%2BEnergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810000147&hterms=Solar+Energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DSolar%2BEnergy"><span>Heat-Transfer Fluids for <span class="hlt">Solar</span>-Energy <span class="hlt">Systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parker, J. C.</p> <p>1982-01-01</p> <p>43-page report investigates noncorrosive heat-transport fluids compatible with both metallic and nonmetallic <span class="hlt">solar</span> collectors and plumbing <span class="hlt">systems</span>. Report includes tables and figures of X-ray inspections for corrosion and schematics of <span class="hlt">solar</span>-heat transport <span class="hlt">systems</span> and heat rejection <span class="hlt">systems</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1973b0009G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1973b0009G"><span>A parametric investigation on a <span class="hlt">solar</span> dish-Stirling <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gholamalizadeh, Ehsan; Chung, Jae Dong</p> <p>2018-06-01</p> <p>The aim of this study is to analyze the performance of a <span class="hlt">solar</span> dish-Stirling <span class="hlt">system</span>. A mathematical model for the overall thermal efficiency of the <span class="hlt">solar</span>-powered high-temperature-differential dish-Stirling engine is described. This model takes into account pressure losses due to fluid friction which is internal to the engine, mechanical friction between the moving parts, actual heat transfer includes the effects of both internal and external irreversibilities of the cycle and finite regeneration processes time. Validation was done through comparison with the actual power output of the "EuroDish" <span class="hlt">system</span>. Moreover, the effects of dish diameter and working fluid on the performance of the <span class="hlt">system</span> were studied. An increase of about 7.2% was <span class="hlt">observed</span> for the power output using hydrogen as the working fluid rather than helium. Also, the focal distance for any diameter of dish was calculated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvD..96f4040D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvD..96f4040D"><span>Cosmological evolution and <span class="hlt">Solar</span> <span class="hlt">System</span> consistency of massive scalar-tensor gravity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Pirey Saint Alby, Thibaut Arnoulx; Yunes, Nicolás</p> <p>2017-09-01</p> <p>The scalar-tensor theory of Damour and Esposito-Farèse recently gained some renewed interest because of its ability to suppress modifications to general relativity in the weak field, while introducing large corrections in the strong field of compact objects through a process called scalarization. A large sector of this theory that allows for scalarization, however, has been shown to be in conflict with <span class="hlt">Solar</span> <span class="hlt">System</span> <span class="hlt">observations</span> when accounting for the cosmological evolution of the scalar field. We here study an extension of this theory by endowing the scalar field with a mass to determine whether this allows the theory to pass <span class="hlt">Solar</span> <span class="hlt">System</span> constraints upon cosmological evolution for a larger sector of coupling parameter space. We show that the cosmological scalar field goes first through a quiescent phase, similar to the behavior of a massless field, but then it enters an oscillatory phase, with an amplitude (and frequency) that decays (and grows) exponentially. We further show that after the field enters the oscillatory phase, its effective energy density and pressure are approximately those of dust, as expected from previous cosmological studies. Due to these oscillations, we show that the scalar field cannot be treated as static today on astrophysical scales, and so we use time-dependent perturbation theory to compute the scalar-field-induced modifications to <span class="hlt">Solar</span> <span class="hlt">System</span> <span class="hlt">observables</span>. We find that these modifications are suppressed when the mass of the scalar field and the coupling parameter of the theory are in a wide range, allowing the theory to pass <span class="hlt">Solar</span> <span class="hlt">System</span> constraints, while in principle possibly still allowing for scalarization.</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/2015EPSC...10..845B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EPSC...10..845B"><span>RECON - A new <span class="hlt">system</span> for probing the outer <span class="hlt">solar</span> <span class="hlt">system</span> with stellar occultations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buie, M. W.; Keller, J. M.; Wasserman, L. H.</p> <p>2015-10-01</p> <p>The Research and Education Collaborative Occultation Network (RECON) is a new <span class="hlt">system</span> for coordinated occultation <span class="hlt">observations</span> of outer <span class="hlt">solar</span> <span class="hlt">system</span> objects. Occultations by objects in the outer <span class="hlt">solar</span> <span class="hlt">system</span> are more difficult to predict due to their large distance and limited duration of the astrometric data used to determine their orbits and positions. This project brings together the research and educational community into a unique citizen-science partnership to overcome the difficulties of <span class="hlt">observing</span> these distant objects. The goal of the project is to get sizes and shapes for TNOs with diameters larger than 100 km. As a result of the <span class="hlt">system</span> design it will also serve as a probe for binary <span class="hlt">systems</span> with spatial separations too small to be resolved directly. Our <span class="hlt">system</span> takes the new approach of setting up a large number of fixed <span class="hlt">observing</span> stations and letting the shadows come to the network. The nominal spacing of the stations is 50 km. The spread of the network is roughly 2000 km along a roughly north-south line in the western United States. The network contains 56 stations that are committed to the project and we get additional ad hoc support from the International Occultation Timing Association. At our minimum size, two stations will record an event while the other stations will be probing for secondary events. Larger objects will get more chords and will allow determination of shape profiles. The stations are almost exclusively sited and associated with schools, usually at the 9-12 grade level. We have successfully completed our first TNO <span class="hlt">observation</span> which is presented in the compainion paper by G. Rossi et al (this conference).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100040500','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100040500"><span><span class="hlt">Solar</span> Spicules Near and at the Limb, <span class="hlt">Observed</span> from Hinode</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, A. C.; Moore, R. L.</p> <p>2010-01-01</p> <p><span class="hlt">Solar</span> spicules appear as narrow jets emanating from the chromosphere and extending into the corona. They have been <span class="hlt">observed</span> for over a hundred years, mainly in chromospheric spectral lines such as H-alpha. Because they are at the limit of visibility of ground-based instruments, their nature has long been a puzzle. In recent years however, vast progress has been made in understanding them both theoretically and <span class="hlt">observationally</span>, as spicule studies have undergone a revolution because of the superior resolution and time cadence of ground-based and space-based instruments. Even more rapid progress is currently underway, due to the <span class="hlt">Solar</span> Optical Telescope (SOT) instrument on the Hinode spacecraft. Here we present <span class="hlt">observations</span> of spicules from Hinode SOT, as seen near the limb with the Ca II filtergraph.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26003563','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26003563"><span>Physical Limits of <span class="hlt">Solar</span> Energy Conversion in the Earth <span class="hlt">System</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kleidon, Axel; Miller, Lee; Gans, Fabian</p> <p>2016-01-01</p> <p><span class="hlt">Solar</span> energy provides by far the greatest potential for energy generation among all forms of renewable energy. Yet, just as for any form of energy conversion, it is subject to physical limits. Here we review the physical limits that determine how much energy can potentially be generated out of sunlight using a combination of thermodynamics and <span class="hlt">observed</span> climatic variables. We first explain how the first and second law of thermodynamics constrain energy conversions and thereby the generation of renewable energy, and how this applies to the conversions of <span class="hlt">solar</span> radiation within the Earth <span class="hlt">system</span>. These limits are applied to the conversion of direct and diffuse <span class="hlt">solar</span> radiation - which relates to concentrated <span class="hlt">solar</span> power (CSP) and photovoltaic (PV) technologies as well as biomass production or any other photochemical conversion - as well as <span class="hlt">solar</span> radiative heating, which generates atmospheric motion and thus relates to wind power technologies. When these conversion limits are applied to <span class="hlt">observed</span> data sets of <span class="hlt">solar</span> radiation at the land surface, it is estimated that direct concentrated <span class="hlt">solar</span> power has a potential on land of up to 11.6 PW (1 PW=10(15) W), whereas photovoltaic power has a potential of up to 16.3 PW. Both biomass and wind power operate at much lower efficiencies, so their potentials of about 0.3 and 0.1 PW are much lower. These estimates are considerably lower than the incoming flux of <span class="hlt">solar</span> radiation of 175 PW. When compared to a 2012 primary energy demand of 17 TW, the most direct uses of <span class="hlt">solar</span> radiation, e.g., by CSP or PV, have thus by far the greatest potential to yield renewable energy requiring the least space to satisfy the human energy demand. Further conversions into <span class="hlt">solar</span>-based fuels would be reduced by further losses which would lower these potentials. The substantially greater potential of <span class="hlt">solar</span>-based renewable energy compared to other forms of renewable energy simply reflects much fewer and lower unavoidable conversion losses when <span class="hlt">solar</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21378340-direct-solutions-maxwell-equations-explain-opposition-phenomena-observed-high-albedo-solar-system-objects','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21378340-direct-solutions-maxwell-equations-explain-opposition-phenomena-observed-high-albedo-solar-system-objects"><span>DIRECT SOLUTIONS OF THE MAXWELL EQUATIONS EXPLAIN OPPOSITION PHENOMENA <span class="hlt">OBSERVED</span> FOR HIGH-ALBEDO <span class="hlt">SOLAR</span> <span class="hlt">SYSTEM</span> OBJECTS</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>Mishchenko, Michael I.; Liu Li; Dlugach, Janna M.</p> <p>2009-11-10</p> <p>Several spectacular backscattering effects <span class="hlt">observed</span> for particulate planetary surfaces have been interpreted in terms of the effect of weak localization (WL) of electromagnetic waves. However, the interference concept of WL explicitly relies on the notion of phase of an electromagnetic wave and is strictly applicable only when particles forming the surface are widely separated. Therefore, one needs a definitive quantitative proof of the WL nature of specific optical effects <span class="hlt">observed</span> for densely packed particulate media. We use numerically exact computer solutions of the Maxwell equations to simulate electromagnetic scattering by realistic models consisting of large numbers of randomly positioned, denselymore » packed particles. By increasing the particle packing density from zero to approx40%, we track the onset and evolution of the full suite of backscattering optical effects predicted by the low-density theory of WL, including the brightness and polarization opposition effects (BOE and POE). We find that all manifestations of WL, except the circular polarization ratio and POE, are remarkably immune to packing-density effects. Even POE can survive packing densities typical of planetary regolith surfaces. Our numerical data coupled with the results of unique <span class="hlt">observations</span> at near-backscattering geometries demonstrate that the BOE and POE detected simultaneously for high-albedo <span class="hlt">solar</span> <span class="hlt">system</span> objects are caused by the effect of WL.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.477.3646A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.477.3646A"><span>Properties of the single Jovian planet population and the pursuit of <span class="hlt">Solar</span> <span class="hlt">system</span> analogues</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Agnew, Matthew T.; Maddison, Sarah T.; Horner, Jonathan</p> <p>2018-07-01</p> <p>While the number of exoplanets discovered continues to increase at a rapid rate, we are still to discover any <span class="hlt">system</span> that truly resembles the <span class="hlt">Solar</span> <span class="hlt">system</span>. Existing and near future surveys will likely continue this trend of rapid discovery. To see if these <span class="hlt">systems</span> are <span class="hlt">Solar</span> <span class="hlt">system</span> analogues, we will need to efficiently allocate resources to carry out intensive follow-up <span class="hlt">observations</span>. We seek to uncover the properties and trends across <span class="hlt">systems</span> that indicate how much of the habitable zone is stable in each <span class="hlt">system</span> to provide focus for planet hunters. We study the dynamics of all known single Jovian planetary <span class="hlt">systems</span> to assess the dynamical stability of the habitable zone around their host stars. We perform a suite of simulations of all <span class="hlt">systems</span> where the Jovian planet will interact gravitationally with the habitable zone, and broadly classify these <span class="hlt">systems</span>. Besides the <span class="hlt">system</span>'s mass ratio (Mpl/Mstar), the Jovian planet's semimajor axis (apl), and eccentricity (epl), we find that there are no underlying <span class="hlt">system</span> properties which are <span class="hlt">observable</span> that indicate the potential for planets to survive within the <span class="hlt">system</span>'s habitable zone. We use Mpl/Mstar, apl, and epl to generate a parameter space over which the unstable <span class="hlt">systems</span> cluster, thus allowing us to predict which <span class="hlt">systems</span> to exclude from future <span class="hlt">observational</span> or numerical searches for habitable exoplanets. We also provide a candidate list of 20 <span class="hlt">systems</span> that have completely stable habitable zones and Jovian planets orbiting beyond the habitable zone as potential first-order <span class="hlt">Solar</span> <span class="hlt">system</span> analogues.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140003190','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140003190"><span>A Comparison Of A <span class="hlt">Solar</span> Power Satellite Concept To A Concentrating <span class="hlt">Solar</span> Power <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Smitherman, David V.</p> <p>2013-01-01</p> <p>A comparison is made of a <span class="hlt">Solar</span> Power Satellite concept in geostationary Earth orbit to a Concentrating <span class="hlt">Solar</span> Power <span class="hlt">system</span> on the ground to analyze overall efficiencies of each infrastructure from <span class="hlt">solar</span> radiance at 1 AU to conversion and transmission of electrical energy into the power grid on the Earth's surface. Each <span class="hlt">system</span> is sized for a 1-gigawatt output to the power grid and then further analyzed to determine primary collector infrastructure areas. Findings indicate that even though the <span class="hlt">Solar</span> Power Satellite concept has a higher end-to-end efficiency, that the combined space and ground collector infrastructure is still about the same size as a comparable Concentrating <span class="hlt">Solar</span> Power <span class="hlt">system</span> on the ground.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960003654&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D60%26Ntt%3DDunham','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960003654&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D60%26Ntt%3DDunham"><span>Exploring small bodies in the outer <span class="hlt">solar</span> <span class="hlt">system</span> with stellar occultations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Elliot, Jim L.; Dunham, Edward W.; Olkin, C. B.</p> <p>1995-01-01</p> <p>Stellar occultation <span class="hlt">observations</span> probe the atmospheric structure and extinction of outer <span class="hlt">solar</span> <span class="hlt">system</span> bodies with a spatial resolution of a few kilometers, and an airborne platform allows the <span class="hlt">observation</span> of occultations by small bodies that are not visible from fixed telescopes. Results from occultations by Triton, Pluto, and Chiron <span class="hlt">observed</span> with KAO are discussed, and future directions for this program are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830051997&hterms=radioactivity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dradioactivity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830051997&hterms=radioactivity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dradioactivity"><span>Extinct radioactivities - A three-phase mixing model. [for early <span class="hlt">solar</span> <span class="hlt">system</span> abundances</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Clayton, D. D.</p> <p>1983-01-01</p> <p>A new class of models is advanced for interpreting the relationship of radioactive abundances in the early <span class="hlt">solar</span> <span class="hlt">system</span> to their average concentration in the interstellar medium. The model assumes that fresh radioactivities are ejected from supernovae into the hot interstellar medium, and that the time scales for changes of phase into molecular clouds determine how much survives for formation therein of the <span class="hlt">solar</span> <span class="hlt">system</span>. A more realistic and physically motivated understanding of the low <span class="hlt">observed</span> concentrations of I-129, Pu-244, and Pd-107 may result.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998IAUS..185..453N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998IAUS..185..453N"><span>MHD oscillations <span class="hlt">observed</span> in the <span class="hlt">solar</span> photosphere with the Michelson Doppler Imager</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Norton, A.; Ulrich, R. K.; Bogart, R. S.; Bush, R. I.; Hoeksema, J. T.</p> <p></p> <p>Magnetohydrodynamic oscillations are <span class="hlt">observed</span> in the <span class="hlt">solar</span> photosphere with the Michelson Doppler Imager (MDI). Images of <span class="hlt">solar</span> surface velocity and magnetic field strength with 4'' spatial resolution and a 60 second temporal resolution are analyzed. A two dimensional gaussian aperture with a FWHM of 10'' is applied to the data in regions of sunspot, plage and quiet sun and the resulting averaged signal is returned each minute. Significant power is <span class="hlt">observed</span> in the magnetic field oscillations with periods of five minutes. The effect of misregistration between MDI's left circularly polarized (LCP) and right circularly polarized (RCP) images has been investigated and is found not to be the cause of the <span class="hlt">observed</span> magnetic oscillations. It is assumed that the large amplitude acoustic waves with 5 minute periods are the driving mechanism behind the magnetic oscillations. The nature of the magnetohydrodynamic oscillations are characterized by their phase relations with simultaneously <span class="hlt">observed</span> <span class="hlt">solar</span> surface velocity oscillations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10235E..0BV','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10235E..0BV"><span>Joint <span class="hlt">observations</span> of <span class="hlt">solar</span> corona in space projects ARKA and KORTES</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vishnyakov, Eugene A.; Bogachev, Sergey A.; Kirichenko, Alexey S.; Reva, Anton A.; Loboda, Ivan P.; Malyshev, Ilya V.; Ulyanov, Artem S.; Dyatkov, Sergey Yu.; Erkhova, Nataliya F.; Pertsov, Andrei A.; Kuzin, Sergey V.</p> <p>2017-05-01</p> <p>ARKA and KORTES are two upcoming <span class="hlt">solar</span> space missions in extreme ultraviolet and X-ray wavebands. KORTES is a sun-oriented mission designed for the Russian segment of International Space Station. KORTES consists of several imaging and spectroscopic instruments that will <span class="hlt">observe</span> the <span class="hlt">solar</span> corona in a number of wavebands, covering EUV and X-ray ranges. The surveillance strategy of KORTES is to cover a wide range of <span class="hlt">observations</span> including simultaneous imaging, spectroscopic and polarization measurements. ARKA is a small satellite <span class="hlt">solar</span> mission intended to take highresolution images of the Sun at the extreme ultraviolet wavelengths. ARKA will be equipped with two high-resolution EUV telescopes designed to collect images of the Sun with approximately 150 km spatial resolution in the field of view of about 10'×10'. The scientific results of the mission may have a significant impact on the theory of coronal heating and may help to clarify the physics of small-scale <span class="hlt">solar</span> structures and phenomena including oscillations of fine coronal structures and the physics of micro- and nanoflares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1981STIN...8229742F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1981STIN...8229742F"><span>Corrosion and scaling in <span class="hlt">solar</span> heating <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Foresti, R. J., Jr.</p> <p>1981-12-01</p> <p>Corrosion, as experienced in <span class="hlt">solar</span> heating <span class="hlt">systems</span>, is described in simplistic terms to familiarize designers and installers with potential problems and their solutions. The role of a heat transfer fluid in a <span class="hlt">solar</span> <span class="hlt">system</span> is briefly discussed, and the choice of an aqueous solution is justified. The complexities of the multiple chemical and physical reactions are discussed in order that uncertainties of corrosion behavior can be anticipated. Some basic theories of corrosion are described, aggressive environments for some common metals are identified, and the role of corrosion inhibitors is delineated. The similarities of thermal and material characteristics of a solor <span class="hlt">system</span> and an automotive cooling <span class="hlt">system</span> are discussed. Based on the many years of experience with corrosion in automotive <span class="hlt">systems</span>, it is recommended that similar antifreezes and corrosion inhibitors should be used in <span class="hlt">solar</span> <span class="hlt">systems</span>. The importance of good <span class="hlt">solar</span> <span class="hlt">system</span> design and fabrication is stressed and specific characteristics that affect corrosion are identified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160013204','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160013204"><span>Beam-Forming Concentrating <span class="hlt">Solar</span> Thermal Array Power <span class="hlt">Systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoppe, Daniel J. (Inventor); Cwik, Thomas A. (Inventor); Dimotakis, Paul E. (Inventor)</p> <p>2016-01-01</p> <p>The present invention relates to concentrating <span class="hlt">solar</span>-power <span class="hlt">systems</span> and, more particularly, beam-forming concentrating <span class="hlt">solar</span> thermal array power <span class="hlt">systems</span>. A <span class="hlt">solar</span> thermal array power <span class="hlt">system</span> is provided, including a plurality of <span class="hlt">solar</span> concentrators arranged in pods. Each <span class="hlt">solar</span> concentrator includes a <span class="hlt">solar</span> collector, one or more beam-forming elements, and one or more beam-steering elements. The <span class="hlt">solar</span> collector is dimensioned to collect and divert incoming rays of sunlight. The beam-forming elements intercept the diverted rays of sunlight, and are shaped to concentrate the rays of sunlight into a beam. The steering elements are shaped, dimensioned, positioned, and/or oriented to deflect the beam toward a beam output path. The beams from the concentrators are converted to heat at a receiver, and the heat may be temporarily stored or directly used to generate electricity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Solar+AND+still&id=EJ1014064','ERIC'); return false;" href="https://eric.ed.gov/?q=Solar+AND+still&id=EJ1014064"><span>Elementary Students' Mental Models of the <span class="hlt">Solar</span> <span class="hlt">System</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>Calderon-Canales, Elena; Flores-Camacho, Fernando; Gallegos-Cazares, Leticia</p> <p>2013-01-01</p> <p>This research project aimed to identify and analyze Mexican primary school students' ideas about the components of the <span class="hlt">solar</span> <span class="hlt">system</span>. In particular, this study focused on conceptions of the <span class="hlt">solar</span> <span class="hlt">system</span> and representations of the dynamics of the <span class="hlt">solar</span> <span class="hlt">system</span> based on the functional and structural models that students make in school. Using a…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900049938&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSMM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900049938&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSMM"><span><span class="hlt">Solar</span> wind and coronal structure near sunspot minimum - Pioneer and SMM <span class="hlt">observations</span> from 1985-1987</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mihalov, J. D.; Barnes, A.; Hundhausen, A. J.; Smith, E. J.</p> <p>1990-01-01</p> <p>Changes in <span class="hlt">solar</span> wind speed and magnetic polarity <span class="hlt">observed</span> at the Pioneer spacecraft are discussed here in terms of the changing magnetic geometry implied by SMM coronagraph <span class="hlt">observations</span> over the period 1985-1987. The pattern of recurrent <span class="hlt">solar</span> wind streams, the long-term average speed, and the sector polarity of the interplanetary magnetic field all changed in a manner suggesting both a temporal variation, and a changing dependence on heliographic latitude. Coronal <span class="hlt">observations</span> during this epoch show a systematic variation in coronal structure and the magnetic structure imposed on the expanding <span class="hlt">solar</span> wind. These <span class="hlt">observations</span> suggest interpretation of the <span class="hlt">solar</span> wind speed variations in terms of the familiar model where the speed increases with distance from a nearly flat interplanetary current sheet, and where this current sheet becomes aligned with the <span class="hlt">solar</span> equatorial plane as sunspot minimum approaches, but deviates rapidly from that orientation after minimum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM11B2312S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM11B2312S"><span>Vortex, ULF wave and Aurora <span class="hlt">Observation</span> after <span class="hlt">Solar</span> Wind Dynamic Pressure Change</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, Q.</p> <p>2017-12-01</p> <p>Here we will summarize our recent study and show some new results on the Magnetosphere and Ionosphere Response to Dynamic Pressure Change/disturbances in the <span class="hlt">Solar</span> Wind and foreshock regions. We study the step function type <span class="hlt">solar</span> wind dynamic pressure change (increase/decrease) interaction with the magnetosphere using THEMIS satellites at both dayside and nightside in different geocentric distances. Vortices generated by the dynamic pressure change passing along the magnetopause are found and compared with model predictions. ULF waves and vortices are excited in the dayside and nightside plasma sheet when dynamic pressure change hit the magnetotail. The related ionospheric responses, such as aurora and TCVs, are also investigated. We compare Global MHD simulations with the <span class="hlt">observations</span>. We will also show some new results that dayside magnetospheric FLRs might be caused by foreshock structures.Shi, Q. Q. et al. (2013), THEMIS <span class="hlt">observations</span> of ULF wave excitation in the nightside plasma sheet during sudden impulse events, J. Geophys. Res. Space Physics, 118, doi:10.1029/2012JA017984. Shi, Q. Q. et al. (2014), <span class="hlt">Solar</span> wind pressure pulse-driven magnetospheric vortices and their global consequences, J. Geophys. Res. Space Physics, 119, doi:10.1002/2013JA019551. Tian, A.M. et al.(2016), Dayside magnetospheric and ionospheric responses to <span class="hlt">solar</span> wind pressure increase: Multispacecraft and ground <span class="hlt">observations</span>, J. Geophys. Res., 121, doi:10.1002/2016JA022459. Shen, X.C. et al.(2015), Magnetospheric ULF waves with increasing amplitude related to <span class="hlt">solar</span> wind dynamic pressure changes: THEMIS <span class="hlt">observations</span>, J. Geophys. Res., 120, doi:10.1002/2014JA020913Zhao, H. Y. et al. (2016), Magnetospheric vortices and their global effect after a <span class="hlt">solar</span> wind dynamic pressure decrease, J. Geophys. Res. Space Physics, 121, doi:10.1002/2015JA021646. Shen, X. C., et al. (2017), Dayside magnetospheric ULF wave frequency modulated by a <span class="hlt">solar</span> wind dynamic pressure negative impulse, J. Geophys. Res</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1029149','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1029149"><span>Exploring the Outer <span class="hlt">Solar</span> <span class="hlt">System</span> with the ESSENCE Supernova Survey</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>Becker, A.C.; /Washington U., Seattle, Astron. Dept.; Arraki, K.</p> <p></p> <p>We report the discovery and orbital determination of 14 trans-Neptunian objects (TNOs) from the ESSENCE Supernova Survey difference imaging data set. Two additional objects discovered in a similar search of the SDSS-II Supernova Survey database were recovered in this effort. ESSENCE repeatedly <span class="hlt">observed</span> fields far from the <span class="hlt">solar</span> <span class="hlt">system</span> ecliptic (-21{sup o} < {beta} < -5{sup o}), reaching limiting magnitudes per <span class="hlt">observation</span> of I {approx} 23.1 and R {approx} 23.7. We examine several of the newly detected objects in detail, including 2003 UC{sub 414}, which orbits entirely between Uranus and Neptune and lies very close to a dynamical region thatmore » would make it stable for the lifetime of the <span class="hlt">solar</span> <span class="hlt">system</span>. 2003 SS{sub 422} and 2007 TA{sub 418} have high eccentricities and large perihelia, making them candidate members of an outer class of TNOs. We also report a new member of the 'extended' or 'detached' scattered disk, 2004 VN{sub 112}, and verify the stability of its orbit using numerical simulations. This object would have been visible to ESSENCE for only {approx}2% of its orbit, suggesting a vast number of similar objects across the sky. We emphasize that off-ecliptic surveys are optimal for uncovering the diversity of such objects, which in turn will constrain the history of gravitational influences that shaped our early <span class="hlt">solar</span> <span class="hlt">system</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900018277&hterms=organic+carbon+fraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dorganic%2Bcarbon%2Bfraction','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900018277&hterms=organic+carbon+fraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dorganic%2Bcarbon%2Bfraction"><span>Carbon in the outer <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Simonelli, D. P.; Pollack, J. B.; Mckay, C. P.</p> <p>1990-01-01</p> <p>The satellites of Uranus, with densities between 1.3 and 1.7 g cm(-3) (from Voyager 2 <span class="hlt">observations</span>) and the Pluto-Charon <span class="hlt">system</span>, with a mean density of just above 1.8 g cm(-3) (from terrestrial <span class="hlt">observations</span> of mutual eclipse events), are too dense to have a significant amount of methane ice in their interiors. However, the <span class="hlt">observed</span> densities do not preclude contributions from such organic materials as the acid-insoluble residue in carbonaceous chondrites and laboratory-produced tholins, which have densities on the order of approximately 1.5 g cm(-3). These and other considerations have led researchers to investigate the carbon mass budget in the outer <span class="hlt">solar</span> <span class="hlt">system</span>, with an emphasis on understanding the contribution of organic materials. Modeling of the interiors of Pluto and Charon (being carried out by R. Reynolds and A. Summers of NASA/Ames), assuming rock and water ice as the only constituents, suggests a silicate mass fraction for this <span class="hlt">system</span> on the order of 0.65 to 0.70. The present work includes the most recent estimates of the C/H enhancements and high z/low z ratios of the giant planets (Pollack and Bodenheimer, 1987), and involves a more careful estimation of the high z/low z mass ratio expected from <span class="hlt">solar</span> abundances than was used in Pollack et al. (1986), including the influence of the fraction of C in CO on the amount of condensed water ice. These calculations indicate that for a particular fraction of C in CO and a given fraction of C-bearing planetesimals that dissolve in the envelope (most likely in the range 0.50 to 0.75), (1) Jupiter and Saturn require a larger fraction of C in condensed materials than Uranus and Neptune, but (2) the Jupiter and Saturn results are much less strongly constrained by the error bars on the <span class="hlt">observed</span> C/H enhancements and high z/low z ratios than is the case for Uranus and Neptune. The clearest result is that in the region of the <span class="hlt">solar</span> nebula near Uranus and Neptune, the minority of carbon that is not in gaseous CO (1</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1436683','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1436683"><span><span class="hlt">Solar</span> thermochemical processing <span class="hlt">system</span> and method</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>Wegeng, Robert S.; Humble, Paul H.; Krishnan, Shankar</p> <p></p> <p>A <span class="hlt">solar</span> thermochemical processing <span class="hlt">system</span> is disclosed. The <span class="hlt">system</span> includes a first unit operation for receiving concentrated <span class="hlt">solar</span> energy. Heat from the <span class="hlt">solar</span> energy is used to drive the first unit operation. The first unit operation also receives a first set of reactants and produces a first set of products. A second unit operation receives the first set of products from the first unit operation and produces a second set of products. A third unit operation receives heat from the second unit operation to produce a portion of the first set of reactants.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SSRv..212..835G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SSRv..212..835G"><span>Water and Volatiles in the Outer <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grasset, O.; Castillo-Rogez, J.; Guillot, T.; Fletcher, L. N.; Tosi, F.</p> <p>2017-10-01</p> <p>Space exploration and ground-based <span class="hlt">observations</span> have provided outstanding evidence of the diversity and the complexity of the outer <span class="hlt">solar</span> <span class="hlt">system</span>. This work presents our current understanding of the nature and distribution of water and water-rich materials from the water snow line to the Kuiper Belt. This synthesis is timely, since a thorough exploration of at least one object in each region of the outer <span class="hlt">solar</span> <span class="hlt">system</span> has now been achieved. Next steps, starting with the Juno mission now in orbit around Jupiter, will be more focused on understanding the processes at work than on describing the general characteristics of each giant planet <span class="hlt">systems</span>. This review is organized in three parts. First, the nature and the distribution of water and volatiles in giant and intermediary planets are described from their inner core to their outer envelopes. A special focus is given to Jupiter and Saturn, which are much better understood than the two ice giants (Uranus and Neptune) thanks to the Galileo and Cassini missions. Second, the icy moons will be discussed. Space missions and ground-based <span class="hlt">observations</span> have revealed the variety of icy surfaces in the outer <span class="hlt">system</span>. While Europa, Enceladus, and maybe Titan present past or even active tectonic and volcanic activities, many other moons have been dead worlds for more than 3 billion years. Ice compositions found at these bodies are also complex and it is now commonly admitted that icy surfaces are never composed of pure ices. A detailed review of the distribution of non-ice materials on the surfaces and in the tenuous atmospheres of the moons is proposed, followed by a more focused discussion on the nature and the characteristics of the liquid layers trapped below the cold icy crusts that have been suggested in the icy Galilean moons, and in Enceladus, Dione, and Titan at Saturn. Finally, the recent <span class="hlt">observations</span> collected by Dawn at Ceres and New Horizons at Pluto, as well as the state of knowledge of other transneptunian objects</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E2093Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E2093Y"><span>Revealing Exo-Zody and Exo-Planets from <span class="hlt">Solar</span> <span class="hlt">System</span> Dust Measurements: ALADDIN-2 for the <span class="hlt">Solar</span> Power Sail Mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yano, Hajime; Hirai, Takayuki</p> <p>2016-07-01</p> <p>The dust structure of our <span class="hlt">Solar</span> <span class="hlt">System</span> provides a benchmark information of dust disks of other exo-planetary <span class="hlt">systems</span> in general, just like the Sun as the closest main sequence G-star that we can study with the most details. Heliocentric dust distributions and gravitational and orbital interactions with planets such as mean motion resonances (MMRs) of dust flux of our <span class="hlt">Solar</span> <span class="hlt">System</span> are what we can transfer the knowledge of our <span class="hlt">Solar</span> <span class="hlt">System</span> dust apply to infer anisotropic exo-zodiacal brightness, or spatial structures within a exo-planetary dust disks with information about potentially embedded planets inside. In the coming era of disk resolved <span class="hlt">observations</span> by ALMA, TMT and other new telescopes, we will be able to apply what we find in the <span class="hlt">Solar</span> <span class="hlt">System</span> to the rest of planetary <span class="hlt">systems</span>. In 2010-11, the IKAROS <span class="hlt">solar</span> sail spacecraft carried the ALADDIN large area dust detector array to study large meteoroids between the Earth and Venus orbits. Yano et al. directly detected both the Earth's and Venus' MMRs dust structures, being consistent with numerical simulations that predict the existence of such local enhancements of dust distribution around these terrestrial planets, as well as Neptune. JAXA's <span class="hlt">Solar</span> Power Sail mission plans to carry even larger dust detector inherited the technology onboard IKAROS, namely ALADDIN-2 in order to search for such MMRs in the Mars and Jupiter orbits, as predicted by Kuchner et al.(2000), in addition to make a continuous measurement of large dust flux from 1.0 to 5.2 AU crossing the main asteroid belt up to Jupiter Trojan region. It is also noted that recent reanalysis of the Pioneer 10 and 11 photo polarimeter data suggests a small enhancement of the brightness towards the anti-<span class="hlt">solar</span> direction near Jupiter the largest planet of our <span class="hlt">Solar</span> <span class="hlt">System</span>, implying a possible existence of a dust belt related to the planet. The spatial density of dust particles directly measured by the ALADDIN-2 will provide a more conclusive and direct proof due 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_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('http://adsabs.harvard.edu/abs/1995ITNS...42.1489C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995ITNS...42.1489C"><span><span class="hlt">Solar</span> particle induced upsets in the TDRS-1 attitude control <span class="hlt">system</span> RAM during the October 1989 <span class="hlt">solar</span> particle events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Croley, D. R.; Garrett, H. B.; Murphy, G. B.; Garrard, T. L.</p> <p>1995-10-01</p> <p>The three large <span class="hlt">solar</span> particle events, beginning on October 19, 1989 and lasting approximately six days, were characterized by high fluences of <span class="hlt">solar</span> protons and heavy ions at 1 AU. During these events, an abnormally large number of upsets (243) were <span class="hlt">observed</span> in the random access memory of the attitude control <span class="hlt">system</span> (ACS) control processing electronics (CPE) on-board the geosynchronous TDRS-1 (Telemetry and Data Relay Satellite). The RAR I unit affected was composed of eight Fairchild 93L422 memory chips. The Galileo spacecraft, launched on October 18, 1989 (one day prior to the <span class="hlt">solar</span> particle events) <span class="hlt">observed</span> the fluxes of heavy ions experienced by TDRS-1. Two solid-state detector telescopes on-board Galileo designed to measure heavy ion species and energy, were turned on during time periods within each of the three separate events. The heavy ion data have been modeled and the time history of the events reconstructed to estimate heavy ion fluences. These fluences were converted to effective LET spectra after transport through the estimated shielding distribution around the TDRS-1 ACS <span class="hlt">system</span>. The number of single event upsets (SEU) expected was calculated by integrating the measured cross section for the Fairchild 93L422 memory chip with average effective LET spectrum. The expected number of heavy ion induced SEUs calculated was 176. GOES-7 proton data, <span class="hlt">observed</span> during the <span class="hlt">solar</span> particle events, were used to estimate the number of proton-induced SEUs by integrating the proton fluence spectrum incident on the memory chips, with the two-parameter Bendel cross section for proton SEUs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016CeMDA.126..145L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016CeMDA.126..145L"><span>Quantification of tidal parameters from <span class="hlt">Solar</span> <span class="hlt">System</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>Lainey, Valéry</p> <p>2016-11-01</p> <p>Tidal dissipation is the main driver of orbital evolution of natural satellites and a key point to understand the exoplanetary <span class="hlt">system</span> configurations. Despite its importance, its quantification from <span class="hlt">observations</span> still remains difficult for most objects of our own <span class="hlt">Solar</span> <span class="hlt">System</span>. In this work, we overview the method that has been used to determine, directly from <span class="hlt">observations</span>, the tidal parameters, with emphasis on the Love number k_2 and the tidal quality factor Q. Up-to-date values of these tidal parameters are summarized. Last, an assessment on the possible determination of the tidal ratio k_2/Q of Uranus and Neptune is done. This may be particularly relevant for coming astrometric campaigns and future space missions focused on these <span class="hlt">systems</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800000048&hterms=gas+natural&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dgas%2Bnatural','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800000048&hterms=gas+natural&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dgas%2Bnatural"><span>Benefit assessment of <span class="hlt">solar</span>-augmented natural gas <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Davis, E. S.; French, R. L.; Sohn, R. L.</p> <p>1980-01-01</p> <p>Report details how <span class="hlt">solar</span>-energy-augmented <span class="hlt">system</span> can reduce natural gas consumption by 40% to 70%. Applications discussed include: domestic hot water <span class="hlt">system</span>, <span class="hlt">solar</span>-assisted gas heat pumps, direct heating from storage tank. Industrial uses, <span class="hlt">solar</span>-assisted appliances, and economic factors are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26ES...40a2011G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26ES...40a2011G"><span>Classifications of central <span class="hlt">solar</span> domestic hot water <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, J. Y.; Hao, B.; Peng, C.; Wang, S. S.</p> <p>2016-08-01</p> <p>Currently, there are many means by which to classify <span class="hlt">solar</span> domestic hot water <span class="hlt">systems</span>, which are often categorized according to their scope of supply, <span class="hlt">solar</span> collector positions, and type of heat storage tank. However, the lack of systematic and scientific classification as well as the general disregard of the thermal performance of the auxiliary heat source is important to DHW <span class="hlt">systems</span>. Thus, the primary focus of this paper is to determine a classification <span class="hlt">system</span> for <span class="hlt">solar</span> domestic hot water <span class="hlt">systems</span> based on the positions of the <span class="hlt">solar</span> collector and auxiliary heating device, both respectively and in combination. Field-testing data regarding many central <span class="hlt">solar</span> DHW <span class="hlt">systems</span> demonstrates that the position of the auxiliary heat source clearly reflects the operational energy consumption. The consumption of collective auxiliary heating hot water <span class="hlt">system</span> is much higher than individual auxiliary heating hot water <span class="hlt">system</span>. In addition, costs are significantly reduced by the separation of the heat storage tank and the auxiliary heating device.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E1451K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E1451K"><span>Common <span class="hlt">observations</span> of <span class="hlt">solar</span> X-rays from SPHINX/CORONAS-PHOTON and XRS/MESSENGER</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kepa, Anna; Sylwester, Janusz; Sylwester, Barbara; Siarkowski, Marek; Mrozek, Tomasz; Gryciuk, Magdalena; Phillips, Kenneth</p> <p></p> <p>SphinX was a soft X-ray spectrophotometer constructed in the Space Research Centre of Polish Academy of Sciences. The instrument was launched on 30 January 2009 aboard CORONAS-PHOTON satellite as a part of TESIS instrument package. SphinX measured total <span class="hlt">solar</span> X-ray flux in the energy range from 1 to 15 keV during the period of very low <span class="hlt">solar</span> activity from 20 February to 29 November 2009. For these times the <span class="hlt">solar</span> detector (X-ray Spectrometer - XRS) onboard MESSENGER also <span class="hlt">observed</span> the <span class="hlt">solar</span> X-rays from a different vantage point. XRS measured the radiation in similar energy range. We present results of the comparison of <span class="hlt">observations</span> from both instruments and show the preliminary results of physical analysis of spectra for selected flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000096238&hterms=earth+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dearth%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000096238&hterms=earth+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dearth%2Bsystem"><span>The Earth <span class="hlt">Observing</span> <span class="hlt">System</span> Terra Mission</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kaufman, Yoram J.; Einaudi, Franco (Technical Monitor)</p> <p>2000-01-01</p> <p>Langley's remarkable <span class="hlt">solar</span> and lunar spectra collected from Mt. Whitney inspired Arrhenius to develop the first quantitative climate model in 1896. After the launch in Dec. 16 1999, NASA's Earth <span class="hlt">Observing</span> AM Satellite (EOS-Terra) will repeat Langley's experiment, but for the entire planet, thus pioneering a wide array of calibrated spectral <span class="hlt">observations</span> from space of the Earth <span class="hlt">System</span>. Conceived in response to real environmental problems, EOS-Terra, in conjunction with other international satellite efforts, will fill a major gap in current efforts by providing quantitative global data sets with a resolution better than 1 km on the physical, chemical and biological elements of the earth <span class="hlt">system</span>. Thus, like Langley's data, EOS-Terra can revolutionize climate research by inspiring a new generation of climate <span class="hlt">system</span> models and enable us to assess the human impact on the environment. In the talk I shall review the historical perspective of the Terra mission and the key new elements of the mission. We expect to have first images that demonstrate the most innovative capability from EOS Terra 5 instruments: MODIS - 1.37 micron cirrus cloud channel; 250m daily coverage for clouds and vegetation change; 7 <span class="hlt">solar</span> channels for land and aerosol studies; new fire channels; Chlorophyll fluorescence; MISR - first 9 multi angle views of clouds and vegetation; MOPITT - first global CO maps and C114 maps; ASTER - Thermal channels for geological studies with 15-90 m resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1981msfc.reptQ....H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1981msfc.reptQ....H"><span><span class="hlt">Solar</span> cooling <span class="hlt">system</span> performance, Frenchman's Reef Hotel, Virgin Islands</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harber, H.</p> <p>1981-09-01</p> <p>The operational and thermal performance of a variety of <span class="hlt">solar</span> <span class="hlt">systems</span> are described. The <span class="hlt">Solar</span> Cooling <span class="hlt">System</span> was installed in a hotel at St. Thomas, U. S. Virgin Islands. The <span class="hlt">system</span> consists of the evacuated glass tube collectors, two 2500 gallon tanks, pumps, computerized controller, a large <span class="hlt">solar</span> optimized industrial sized lithium bromide absorption chiller, and associated plumbing. <span class="hlt">Solar</span> heated water is pumped through the <span class="hlt">system</span> to the designed public areas such as lobby, lounges, restaurant and hallways. Auxiliary heat is provided by steam and a heat exchanger to supplement the <span class="hlt">solar</span> heat.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810025068','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810025068"><span><span class="hlt">Solar</span> cooling <span class="hlt">system</span> performance, Frenchman's Reef Hotel, Virgin Islands</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harber, H.</p> <p>1981-01-01</p> <p>The operational and thermal performance of a variety of <span class="hlt">solar</span> <span class="hlt">systems</span> are described. The <span class="hlt">Solar</span> Cooling <span class="hlt">System</span> was installed in a hotel at St. Thomas, U. S. Virgin Islands. The <span class="hlt">system</span> consists of the evacuated glass tube collectors, two 2500 gallon tanks, pumps, computerized controller, a large <span class="hlt">solar</span> optimized industrial sized lithium bromide absorption chiller, and associated plumbing. <span class="hlt">Solar</span> heated water is pumped through the <span class="hlt">system</span> to the designed public areas such as lobby, lounges, restaurant and hallways. Auxiliary heat is provided by steam and a heat exchanger to supplement the <span class="hlt">solar</span> heat.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790003300','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790003300"><span>Non-tracking <span class="hlt">solar</span> energy collector <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Selcuk, M. K. (Inventor)</p> <p>1978-01-01</p> <p>A <span class="hlt">solar</span> energy collector <span class="hlt">system</span> is described characterized by an improved concentrator for directing incident rays of <span class="hlt">solar</span> energy on parallel strip-like segments of a flatplate receiver. Individually mounted reflector modules of a common asymmetrical triangular cross-sectional configuration supported for independent orientation are asymmetric included with vee-trough concentrators for deflecting incident <span class="hlt">solar</span> energy toward the receiver.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810000155&hterms=Solar+Energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DSolar%2BEnergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810000155&hterms=Solar+Energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DSolar%2BEnergy"><span>Economic Evaluation of Townhouse <span class="hlt">Solar</span> Energy <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1982-01-01</p> <p><span class="hlt">Solar</span>-energy site in Columbia, South Carolina, is comprised of four townhouse apartments. Report summarizes economic evaluation of <span class="hlt">solar</span>--energy <span class="hlt">system</span> and projected performance of similar <span class="hlt">systems</span> in four other selected cities. <span class="hlt">System</span> is designed to supply 65 percent of heating and 75 percent of hot water.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT.......208L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT.......208L"><span><span class="hlt">Solar</span> Energy <span class="hlt">Systems</span> for Ohioan Residential Homeowners</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luckett, Rickey D.</p> <p></p> <p>Dwindling nonrenewable energy resources and rising energy costs have forced the United States to develop alternative renewable energy sources. The United States' <span class="hlt">solar</span> energy industry has seen an upsurge in recent years, and photovoltaic holds considerable promise as a renewable energy technology. The purpose of this case study was to explore homeowner's awareness of the benefits of <span class="hlt">solar</span> energy. Disruptive-innovation theory was used to explore marketing strategies for conveying information to homeowners about access to new <span class="hlt">solar</span> energy products and services. Twenty residential homeowners were interviewed face-to-face to explore (a) perceived benefits of <span class="hlt">solar</span> energy in their county in Ohio, and (b) perceptions on the rationale behind the marketing strategy of <span class="hlt">solar</span> energy <span class="hlt">systems</span> sold for residential use. The study findings used inductive analyses and coding interpretation to explore the participants' responses that revealed 3 themes: the existence of environmental benefits for using <span class="hlt">solar</span> energy <span class="hlt">systems</span>, the expensive cost of equipment associated with government incentives, and the lack of marketing information that is available for consumer use. The implications for positive social change include the potential to enable corporate leaders, small business owners, and entrepreneurs to develop marketing strategies for renewable energy <span class="hlt">systems</span>. These strategies may promote use of <span class="hlt">solar</span> energy <span class="hlt">systems</span> as a clean, renewable, and affordable alternative electricity energy source for the 21st century.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020042347&hterms=organic+chemistry&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dorganic%2Bchemistry','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020042347&hterms=organic+chemistry&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dorganic%2Bchemistry"><span>Organic Chemistry: From the Interstellar Medium to the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sandford, Scott; Witteborn, Fred C. (Technical Monitor)</p> <p>1997-01-01</p> <p>This talk will review the various types of organic materials <span class="hlt">observed</span> in different environments in the interstellar medium, discuss the processes by which these materials may have formed and been modified, and present the evidence supporting the contention that at least a fraction of this material survived incorporation, substantially unaltered, into our <span class="hlt">Solar</span> <span class="hlt">System</span> during its formation. The nature of this organic material is of direct interest to issues associated with the origin of life, both because this material represents a large fraction of the <span class="hlt">Solar</span> <span class="hlt">System</span> inventory of the biogenically-important elements, and because many of the compounds in this inventory have biogenic implications. Several specific examples of such molecules will be briefly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011MNRAS.417..314M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011MNRAS.417..314M"><span>The diversity of planetary <span class="hlt">system</span> architectures: contrasting theory 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>Miguel, Y.; Guilera, O. M.; Brunini, A.</p> <p>2011-10-01</p> <p>In order to explain the <span class="hlt">observed</span> diversity of planetary <span class="hlt">system</span> architectures and relate this primordial diversity to the initial properties of the discs where they were born, we develop a semi-analytical model for computing planetary <span class="hlt">system</span> formation. The model is based on the core instability model for the gas accretion of the embryos and the oligarchic growth regime for the accretion of the solid cores. Two regimes of planetary migration are also included. With this model, we consider different initial conditions based on recent results of protoplanetary disc <span class="hlt">observations</span> to generate a variety of planetary <span class="hlt">systems</span>. These <span class="hlt">systems</span> are analysed statistically, exploring the importance of several factors that define the planetary <span class="hlt">system</span> birth environment. We explore the relevance of the mass and size of the disc, metallicity, mass of the central star and time-scale of gaseous disc dissipation in defining the architecture of the planetary <span class="hlt">system</span>. We also test different values of some key parameters of our model to find out which factors best reproduce the diverse sample of <span class="hlt">observed</span> planetary <span class="hlt">systems</span>. We assume different migration rates and initial disc profiles, in the context of a surface density profile motivated by similarity solutions. According to this, and based on recent protoplanetary disc <span class="hlt">observational</span> data, we predict which <span class="hlt">systems</span> are the most common in the <span class="hlt">solar</span> neighbourhood. We intend to unveil whether our <span class="hlt">Solar</span> <span class="hlt">system</span> is a rarity or whether more planetary <span class="hlt">systems</span> like our own are expected to be found in the near future. We also analyse which is the more favourable environment for the formation of habitable planets. Our results show that planetary <span class="hlt">systems</span> with only terrestrial planets are the most common, being the only planetary <span class="hlt">systems</span> formed when considering low-metallicity discs, which also represent the best environment for the development of rocky, potentially habitable planets. We also found that planetary <span class="hlt">systems</span> like our own are not rare in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA....13551G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA....13551G"><span><span class="hlt">Solar</span> active region display <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Golightly, M.; Raben, V.; Weyland, M.</p> <p>2003-04-01</p> <p>The <span class="hlt">Solar</span> Active Region Display <span class="hlt">System</span> (SARDS) is a client-server application that automatically collects a wide range of <span class="hlt">solar</span> data and displays it in a format easy for users to assimilate and interpret. Users can rapidly identify active regions of interest or concern from color-coded indicators that visually summarize each region's size, magnetic configuration, recent growth history, and recent flare and CME production. The active region information can be overlaid onto <span class="hlt">solar</span> maps, multiple <span class="hlt">solar</span> images, and <span class="hlt">solar</span> difference images in orthographic, Mercator or cylindrical equidistant projections. Near real-time graphs display the GOES soft and hard x-ray flux, flare events, and daily F10.7 value as a function of time; color-coded indicators show current trends in soft x-ray flux, flare temperature, daily F10.7 flux, and x-ray flare occurrence. Through a separate window up to 4 real-time or static graphs can simultaneously display values of KP, AP, daily F10.7 flux, GOES soft and hard x-ray flux, GOES >10 and >100 MeV proton flux, and Thule neutron monitor count rate. Climatologic displays use color-valued cells to show F10.7 and AP values as a function of Carrington/Bartel's rotation sequences - this format allows users to detect recurrent patterns in <span class="hlt">solar</span> and geomagnetic activity as well as variations in activity levels over multiple <span class="hlt">solar</span> cycles. Users can customize many of the display and graph features; all displays can be printed or copied to the <span class="hlt">system</span>'s clipboard for "pasting" into other applications. The <span class="hlt">system</span> obtains and stores space weather data and images from sources such as the NOAA Space Environment Center, NOAA National Geophysical Data Center, the joint ESA/NASA SOHO spacecraft, and the Kitt Peak National <span class="hlt">Solar</span> Observatory, and can be extended to include other data series and image sources. Data and images retrieved from the <span class="hlt">system</span>'s database are converted to XML and transported from a central server using HTTP and SOAP protocols, allowing</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1982STIN...8233887E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1982STIN...8233887E"><span><span class="hlt">Solar</span>- and wind-powered irrigation <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Enochian, R. V.</p> <p>1982-02-01</p> <p>Five different direct <span class="hlt">solar</span> and wind energy <span class="hlt">systems</span> are technically feasible for powering irrigation pumps. However, with projected rates of fossil fuel costs, only two may produce significant unsubsidied energy for irrigation pumping before the turn of the century. These are photovoltaic <span class="hlt">systems</span> with nonconcentrating collectors (providing that projected costs of manufacturing <span class="hlt">solar</span> cells prove correct); and wind <span class="hlt">systems</span>, especially in remote areas where adequate wind is available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160011197','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160011197"><span>Clasp/SJ <span class="hlt">Observation</span> of Time Variations of Lyman-Alpha Emissions in a <span class="hlt">Solar</span> Active Region</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ishikawa, S.; Kubo, M.; Katsukawa, Y.; Kano, R.; Narukage, N.; Ishikawa, R.; Bando, T.; Winebarger, A.; Kobayashi, K.; Trujillo Bueno, J.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20160011197'); toggleEditAbsImage('author_20160011197_show'); toggleEditAbsImage('author_20160011197_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20160011197_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20160011197_hide"></p> <p>2016-01-01</p> <p>The Chromospheric Lyman-alpha SpectroPolarimeter (CLASP) is a sounding rocket experiment launched on September 3, 2015 to investigate the <span class="hlt">solar</span> chromosphere, and the slit-jaw (SJ) optical <span class="hlt">system</span> took Lya images with the high time cadence of 0.6 s. By the CLASP/SJ <span class="hlt">observation</span>, many time variations in the <span class="hlt">solar</span> chromosphere with the time scale of <1 minute were discovered (see the poster by Kubo et al., Pa-13). We focused on an active region and investigated the short (<30 s) time variations and relation to the coronal structure <span class="hlt">observed</span> by SDO/AIA. We compared the Ly(alpha) time variations at footpoints of coronal magnetic fields <span class="hlt">observed</span> by AIA 211 Å (approx.2 MK) and AIA 171 Å (0.6 MK), and non-loop regions. As the result, we found the <30 s Ly(alpha) time variations had more in the footpoint regions. On the other hand, the <30 s time variations had no dependency on the temperature of the loop.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70168446','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70168446"><span>Cryovolcanism in the outer <span class="hlt">solar</span> <span class="hlt">system</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>Geissler, Paul E.</p> <p>2015-01-01</p> <p>Cryovolcanism is defined as the extrusion of liquids and vapors of materials that would be frozen solid at the planetary surface temperatures of the icy bodies of the outer <span class="hlt">solar</span> <span class="hlt">system</span>. Active cryovolcanism is now known to occur on Saturn's moon Enceladus and on Neptune's moon Triton and is suspected on Jupiter's moon Europa, while evidence for past cryovolcanic activity is widespread throughout the outer <span class="hlt">solar</span> <span class="hlt">system</span>. This chapter examines the mechanisms and manifestations of cryovolcanism, beginning with a review of the materials that make up these unusual ‘‘magmas’’ and the means by which they might erupt and concluding with a volcanologist's tour of the farthest reaches of the <span class="hlt">solar</span> <span class="hlt">system</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790041801&hterms=wind+monitor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dwind%2Bmonitor','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790041801&hterms=wind+monitor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dwind%2Bmonitor"><span>Signatures of <span class="hlt">solar</span> wind latitudinal structure in interplanetary Lyman-alpha emissions - Mariner 10 <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>Kumar, S.; Broadfoot, A. L.</p> <p>1979-01-01</p> <p>A detailed analysis is conducted which shows that signatures in the interplanetary Lyman-alpha emissions <span class="hlt">observed</span> in three different data sets from Mariner 10 (corresponding to different locations of the spacecraft) provide firm evidence that the intensity departures are correlated with a decrease in <span class="hlt">solar</span> wind flux with increasing latitude. It is suggested that <span class="hlt">observations</span> of the interplanetary emission can be used to monitor average <span class="hlt">solar</span> wind activity at high latitudes. The asymmetry in the <span class="hlt">solar</span> radiation field as a source of <span class="hlt">observed</span> departures in L-alpha data is considered and attention is given to the interstellar hydrogen and helium density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22086330-ace-swics-observations-heavy-ion-dropouts-within-solar-wind','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22086330-ace-swics-observations-heavy-ion-dropouts-within-solar-wind"><span>ACE/SWICS <span class="hlt">OBSERVATIONS</span> OF HEAVY ION DROPOUTS WITHIN THE <span class="hlt">SOLAR</span> WIND</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>Weberg, Micah J.; Zurbuchen, Thomas H.; Lepri, Susan T., E-mail: mjweberg@umich.edu, E-mail: thomasz@umich.edu, E-mail: slepri@umich.edu</p> <p>2012-11-20</p> <p>We present the first in situ <span class="hlt">observations</span> of heavy ion dropouts within the slow <span class="hlt">solar</span> wind, <span class="hlt">observed</span> for select elements ranging from helium to iron. For iron, these dropouts manifest themselves as depletions of the Fe/H ratio by factors up to {approx}25. The events often exhibit mass-dependent fractionation and are contained in slow, unsteady wind found within a few days from known stream interfaces. We propose that such dropouts are evidence of gravitational settling within large coronal loops, which later undergo interchange reconnection and become source regions of slow, unsteady wind. Previously, spectroscopic studies by Raymond et al. in 1997more » (and later Feldman et al. in 1999) have yielded strong evidence for gravitational settling within these loops. However, their expected in situ signature plasma with heavy elements fractionated by mass was not <span class="hlt">observed</span> prior to this study. Using data from the SWICS instrument on board the Advanced Composition Explorer (ACE), we investigate the composition of the <span class="hlt">solar</span> wind within these dropouts and explore long term trends over most of a <span class="hlt">solar</span> cycle.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080025158&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dsolar%2Bradiation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080025158&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dsolar%2Bradiation"><span>Using <span class="hlt">Observations</span> of Deep Convective <span class="hlt">Systems</span> to Constrain Atmospheric Column Absorption of <span class="hlt">Solar</span> Radiation in the Optically Thick Limit</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dong, Xiquan; Wielicki, Bruce A.; Xi, Baike; Hu, Yongxiang; Mace, Gerald G.; Benson, Sally; Rose, Fred; Kato, Seiji; Charlock, Thomas; Minnis, Patrick</p> <p>2008-01-01</p> <p>Atmospheric column absorption of <span class="hlt">solar</span> radiation A(sub col) is a fundamental part of the Earth's energy cycle but is an extremely difficult quantity to measure directly. To investigate A(sub col), we have collocated satellite-surface <span class="hlt">observations</span> for the optically thick Deep Convective <span class="hlt">Systems</span> (DCS) at the Department of Energy Atmosphere Radiation Measurement (ARM) Tropical Western Pacific (TWP) and Southern Great Plains (SGP) sites during the period of March 2000 December 2004. The surface data were averaged over a 2-h interval centered at the time of the satellite overpass, and the satellite data were averaged within a 1 deg X 1 deg area centered on the ARM sites. In the DCS, cloud particle size is important for top-of-atmosphere (TOA) albedo and A(sub col) although the surface absorption is independent of cloud particle size. In this study, we find that the A(sub col) in the tropics is approximately 0.011 more than that in the middle latitudes. This difference, however, disappears, i.e., the A(sub col) values at both regions converge to the same value (approximately 0.27 of the total incoming <span class="hlt">solar</span> radiation) in the optically thick limit (tau greater than 80). Comparing the <span class="hlt">observations</span> with the NASA Langley modified Fu_Liou 2-stream radiative transfer model for optically thick cases, the difference between <span class="hlt">observed</span> and model-calculated surface absorption, on average, is less than 0.01, but the model-calculated TOA albedo and A(sub col) differ by 0.01 to 0.04, depending primarily on the cloud particle size <span class="hlt">observation</span> used. The model versus <span class="hlt">observation</span> discrepancies found are smaller than many previous studies and are just within the estimated error bounds. We did not find evidence for a large cloud absorption anomaly for the optically thick limit of extensive ice cloud layers. A more modest cloud absorption difference of 0.01 to 0.04 cannot yet be ruled out. The remaining uncertainty could be reduced with additional cases, and by reducing the current</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('https://ntrs.nasa.gov/search.jsp?R=19760038407&hterms=Extinction+threshold&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DExtinction%2Bthreshold','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760038407&hterms=Extinction+threshold&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DExtinction%2Bthreshold"><span>The <span class="hlt">solar</span>-flare infrared continuum - <span class="hlt">Observational</span> techniques and upper limits</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hudson, H. S.</p> <p>1975-01-01</p> <p>Exploratory <span class="hlt">observations</span> at 20 microns and 350 microns have determined detection thresholds for <span class="hlt">solar</span> flares in these wavelengths. In the 20-micron range, <span class="hlt">solar</span> atmospheric fluctuations (the 'temperature field') set the basic limits on flare detectability at about 5 K; at 350 microns, extinction in the earth's atmosphere provides the basic limitation of about 30 K. These thresholds are low enough for the successful detection of several infrared-emitting components of large flares. The upper limits obtained for subflares indicate that the thickness of the H-alpha flare region does not exceed approximately 10 km. This result confirms the conclusion of Suemoto and Hiei (1959) regarding the small effective thickness of the H-alpha-emitting regions in <span class="hlt">solar</span> flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654390-observations-reconnection-flows-flare-solar-disk','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654390-observations-reconnection-flows-flare-solar-disk"><span><span class="hlt">Observations</span> of Reconnection Flows in a Flare on the <span class="hlt">Solar</span> Disk</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, Juntao; Simões, P. J. A.; Jeffrey, N. L. S.</p> <p></p> <p>Magnetic reconnection is a well-accepted part of the theory of <span class="hlt">solar</span> eruptive events, though the evidence is still circumstantial. Intrinsic to the reconnection picture of a <span class="hlt">solar</span> eruptive event, particularly in the standard model for two-ribbon flares (CSHKP model), are an advective flow of magnetized plasma into the reconnection region, expansion of field above the reconnection region as a flux rope erupts, retraction of heated post-reconnection loops, and downflows of cooling plasma along those loops. We report on a unique set of <span class="hlt">Solar</span> Dynamics Observatory /Atmospheric Imaging Assembly imaging and Hinode /EUV Imaging Spectrometer spectroscopic <span class="hlt">observations</span> of the disk flaremore » SOL2016-03-23T03:54 in which all four flows are present simultaneously. This includes spectroscopic evidence for a plasma upflow in association with large-scale expanding closed inflow field. The reconnection inflows are symmetric, and consistent with fast reconnection, and the post-reconnection loops show a clear cooling and deceleration as they retract. <span class="hlt">Observations</span> of coronal reconnection flows are still rare, and most events are <span class="hlt">observed</span> at the <span class="hlt">solar</span> limb, obscured by complex foregrounds, making their relationship to the flare ribbons, cusp field, and arcades formed in the lower atmosphere difficult to interpret. The disk location and favorable perspective of this event have removed these ambiguities giving a clear picture of the reconnection dynamics.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Ap%26SS.358...25G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Ap%26SS.358...25G"><span>Improved SOT (Hinode mission) high resolution <span class="hlt">solar</span> imaging <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>Goodarzi, H.; Koutchmy, S.; Adjabshirizadeh, A.</p> <p>2015-08-01</p> <p>We consider the best today available <span class="hlt">observations</span> of the Sun free of turbulent Earth atmospheric effects, taken with the <span class="hlt">Solar</span> Optical Telescope (SOT) onboard the Hinode spacecraft. Both the instrumental smearing and the <span class="hlt">observed</span> stray light are analyzed in order to improve the resolution. The Point Spread Function (PSF) corresponding to the blue continuum Broadband Filter Imager (BFI) near 450 nm is deduced by analyzing (i) the limb of the Sun and (ii) images taken during the transit of the planet Venus in 2012. A combination of Gaussian and Lorentzian functions is selected to construct a PSF in order to remove both smearing due to the instrumental diffraction effects (PSF core) and the large-angle stray light due to the spiders and central obscuration (wings of the PSF) that are responsible for the parasitic stray light. A Max-likelihood deconvolution procedure based on an optimum number of iterations is discussed. It is applied to several <span class="hlt">solar</span> field images, including the granulation near the limb. The normal non-magnetic granulation is compared to the abnormal granulation which we call magnetic. A new feature appearing for the first time at the extreme- limb of the disk (the last 100 km) is discussed in the context of the definition of the <span class="hlt">solar</span> edge and of the <span class="hlt">solar</span> diameter. A single sunspot is considered in order to illustrate how effectively the restoration works on the sunspot core. A set of 125 consecutive deconvolved images is assembled in a 45 min long movie illustrating the complexity of the dynamical behavior inside and around the sunspot.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P51C2600L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P51C2600L"><span>Analysis of <span class="hlt">Solar</span> Wind Precipitation on Mars Using MAVEN/SWIA <span class="hlt">Observations</span> of Spacecraft-Scattered Ions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lue, C.; Halekas, J. S.</p> <p>2017-12-01</p> <p>Particle sensors on the MAVEN spacecraft (SWIA, SWEA, STATIC) <span class="hlt">observe</span> precipitating <span class="hlt">solar</span> wind ions during MAVEN's periapsis passes in the Martian atmosphere (at 120-250 km altitude). The signature is <span class="hlt">observed</span> as positive and negative particles at the <span class="hlt">solar</span> wind energy, traveling away from the Sun. The <span class="hlt">observations</span> can be explained by the <span class="hlt">solar</span> wind penetrating the Martian magnetic barrier in the form of energetic neutral atoms (ENAs) due to charge-exchange with the Martian hydrogen corona, and then being reionized in positive or negative form upon impact with the atmosphere (1). These findings have elucidated <span class="hlt">solar</span> wind precipitation dynamics at Mars, and can also be used to monitor the <span class="hlt">solar</span> wind even when MAVEN is at periapsis (2). In the present study, we focus on a SWIA instrument background signal that has been interpreted as spacecraft/instrument-scattered ions (2). We aim to model and subtract the scattered ion signal from the <span class="hlt">observations</span> including those of reionized <span class="hlt">solar</span> wind. We also aim to use the scattered ion signal to track hydrogen ENAs impacting the spacecraft above the reionization altitude. We characterize the energy spectrum and directional scattering function for <span class="hlt">solar</span> wind scattering off the SWIA aperture structure, the radome and the spacecraft body. We find a broad scattered-ion energy spectrum up to the <span class="hlt">solar</span> wind energy, displaying increased energy loss and reduced flux with increasing scattering angle, allowing correlations with the <span class="hlt">solar</span> wind direction, energy, and flux. We develop models that can be used to predict the scattered signal based on the direct <span class="hlt">solar</span> wind <span class="hlt">observations</span> or to infer the <span class="hlt">solar</span> wind properties based on the <span class="hlt">observed</span> scattered signal. We then investigate deviations to the models when the spacecraft is in the Martian atmosphere and evaluate the plausibility of that these are caused by ENAs. We also perform SIMION modeling of the scattering process and the resulting signal detection by SWIA, to study the results from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017eaa..book..771O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017eaa..book..771O"><span>British <span class="hlt">Observations</span> of the 18 August 1868 Total <span class="hlt">Solar</span> Eclipse from Guntoor, India</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Orchiston, Wayne; Lee, Eun-Hee; Ahn, Young-Sook</p> <p></p> <p>The total <span class="hlt">solar</span> eclipse of 18 August 1868 was <span class="hlt">observed</span> in Aden, India, Siam (present-day Thailand) and the Dutch East Indies (present-day Indonesia). One Indian expedition was sponsored by the Royal Astronomical Society, and led by Major J.F. Tennant. In this chapter we describe the <span class="hlt">observing</span> team and instruments, discuss their <span class="hlt">observations</span>, and conclude with some remarks on the place of the 1868 eclipse in <span class="hlt">solar</span> studies and later nineteenth century European astronomical expeditions to India.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AAS...22052112M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AAS...22052112M"><span><span class="hlt">Solar</span> Hard X-ray <span class="hlt">Observations</span> with NuSTAR</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marsh, Andrew; Smith, D. M.; Krucker, S.; Hudson, H. S.; Hurford, G. J.; White, S. M.; Mewaldt, R. A.; Harrison, F. A.; Grefenstette, B. W.; Stern, D.</p> <p>2012-05-01</p> <p>High-sensitivity imaging of coronal hard X-rays allows detection of freshly accelerated nonthermal electrons at the acceleration site. A few such <span class="hlt">observations</span> have been made with Yohkoh and RHESSI, but a leap in sensitivity could help pin down the time, place, and manner of reconnection. Around the time of this meeting, the Nuclear Spectroscopic Telescope ARray (NuSTAR), a NASA Small Explorer for high energy astrophysics that uses grazing-incidence optics to focus X-rays up to 80 keV, will be launched. Three weeks will be dedicated to <span class="hlt">solar</span> <span class="hlt">observing</span> during the baseline two-year mission. NuSTAR will be 200 times more sensitive than RHESSI in the hard X-ray band. This will allow the following new <span class="hlt">observations</span>, among others: 1) Extrapolation of the micro/nanoflare distribution by two orders of magnitude down in flux; 2) Search for hard X-rays from network nanoflares (soft X-ray bright points) and evaluation of their role in coronal heating; 3) Discovery of hard X-ray bremsstrahlung from the electron beams driving type III radio bursts, and measurement of their electron spectrum; 4) Hard X-ray studies of polar soft X-ray jets and impulsive <span class="hlt">solar</span> energetic particle events at the edge of coronal holes; 5) Study of coronal bremsstrahlung from particles accelerated by coronal mass ejections as they are first launched; 6) Study of particles at the coronal reconnection site when flare footpoints and loops are occulted; 7) Search for weak high-temperature coronal plasmas in active regions that are not flaring; and 8) Search for hypothetical axion particles created in the <span class="hlt">solar</span> core via the hard X-ray signal from their conversion to X-rays in the coronal magnetic field. NuSTAR will also serve as a pathfinder for a future dedicated space mission with enhanced capabilities, such as a satellite version of the FOXSI sounding rocket.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23135425L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23135425L"><span>SPHEREx: Science Opportunities for <span class="hlt">Solar</span> <span class="hlt">System</span> Astronomy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lisse, Carey Michael; SPHEREx Science Team</p> <p>2018-01-01</p> <p>SPHEREx, a mission in NASA's Medium Explorer (MIDEX) program that was selected for Phase A study in August 2017, will perform an all-sky near-infrared spectral survey between 0.75 - 5.0 µm in R = 41 filters, and with R = 135 coverage from 4.2 - 5.0 µm, reaching L ~ 19 (5-sigma).SPHEREx has high potential for <span class="hlt">solar</span> <span class="hlt">system</span> science. The 96-band survey will cover the entire sky 4 times over the course of 2 years, including thousands of foreground <span class="hlt">solar</span> <span class="hlt">system</span> asteroids, comets, Trojans, and KBOs. By canvassing the entire <span class="hlt">solar</span> <span class="hlt">system</span> for 2 years, SPHEREx has the potential not only to achieve a relatively complete sensitivity limited survey of the <span class="hlt">solar</span> <span class="hlt">system</span>'s bodies, but also some capability to search for variation in these bodies over time.For example, the large legacy dataset of SPHEREx will update the WISE catalogue of asteroid sizes and albedos by providing a spectral survey of tens of thousands of bodies. It will provide spectral classification of hundreds of Trojan asteroids, allowing for direct comparison to the asteroid results. It will extend optical surveys of comet composition by dynamical type to hundreds of objects in the NIR, while determining water/dust/CO/CO2 activity vs distance. SPHEREx will also map in great temporal and spatial detail the zodiacal dust debris disk cloud that these bodies produce, providing an unprecedented level of information concerning the sources and sinks of this material.In this paper, we discuss the data release schedule and some example science studies the planetary astronomy community will be able to access using the SPHEREx database. We also outline existing plans within the SPHEREx team to develop software tools to enable easy access to the data and to conduct catalog searches, and ways in which the community can provide input to the SPHEREx Science Team on scientific studies and data/software requirements for those studies, enabling a large number of scientific studies while finding interesting targets for follow</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170003413','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170003413"><span>Deployable Propulsion and Power <span class="hlt">Systems</span> for <span class="hlt">Solar</span> <span class="hlt">System</span> Exploration</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Johnson, Les; Carr, John</p> <p>2017-01-01</p> <p>NASA is developing thin-film based, deployable propulsion, power and communication <span class="hlt">systems</span> for small spacecraft that could provide a revolutionary new capability allowing small spacecraft exploration of the <span class="hlt">solar</span> <span class="hlt">system</span>. The Near Earth Asteroid (NEA) Scout reconnaissance mission will demonstrate <span class="hlt">solar</span> sail propulsion on a 6U CubeSat interplanetary spacecraft and lay the groundwork for their future use in deep space science and exploration missions. <span class="hlt">Solar</span> sails use sunlight to propel vehicles through space by reflecting <span class="hlt">solar</span> photons from a large, mirror-like sail made of a lightweight, highly reflective material. This continuous photon pressure provides propellantless thrust, allowing for very high delta V maneuvers on long-duration, deep space exploration. Since reflected light produces thrust, <span class="hlt">solar</span> sails require no onboard propellant. The Lightweight Integrated <span class="hlt">Solar</span> Array and Transceiver (LISA-T) is a launch stowed, orbit deployed array on which thin-film photovoltaic and antenna elements are embedded. Inherently, small satellites are limited in surface area, volume, and mass allocation; driving competition between power, communications, and GN&C (guidance navigation and control) subsystems. This restricts payload capability and limits the value of these low-cost satellites. LISA-T is addressing this issue, deploying large-area arrays from a reduced volume and mass envelope - greatly enhancing power generation and communications capabilities of small spacecraft. The NEA Scout mission, funded by NASA's Advanced Exploration <span class="hlt">Systems</span> Program and managed by NASA MSFC, will use the <span class="hlt">solar</span> sail as its primary propulsion <span class="hlt">system</span>, allowing it to survey and image one or more NEA's of interest for possible future human exploration. NEA Scout uses a 6U cubesat (to be provided by NASA's Jet Propulsion Laboratory), an 86 sq m <span class="hlt">solar</span> sail and will weigh less than 12 kilograms. NEA Scout will be launched on the first flight of the Space Launch <span class="hlt">System</span> in 2018. Similar in concept</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840013920','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840013920"><span><span class="hlt">Observations</span> of <span class="hlt">solar</span>-cell metallization corrosion</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mon, G. R.</p> <p>1983-01-01</p> <p>The Engineering Sciences Area of the Jet Propulsion Laboratory (JPL) Flat-Plate <span class="hlt">Solar</span> Array Project is performing long term environmental tests on photovoltaic modules at Wyle Laboratories in Huntsville, Alabama. Some modules have been exposed to 85 C/85% RH and 40 C/93% RH for up to 280 days. Other modules undergoing temperature-only exposures ( 3% RH) at 85 C and 100 C have been tested for more than 180 days. At least two modules of each design type are exposed to each environment - one with, and the other without a 100-mA forward bias. Degradation is both visually <span class="hlt">observed</span> and electrically monitored. Visual <span class="hlt">observations</span> of changes in appearance are recorded at each inspection time. Significant visual <span class="hlt">observations</span> relating to metallization corrosion (and/or metallization-induced corrosion) include discoloration (yellowing and browning) of grid lines, migration of grid line material into the encapsulation (blossoming), the appearance of rainbow-like diffraction patterns on the grid lines, and brown spots on collectors and grid lines. All of these <span class="hlt">observations</span> were recorded for electrically biased modules in the 280-day tests with humidity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123..848L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123..848L"><span>The 11 Year <span class="hlt">Solar</span> Cycle Response of the Equatorial Ionization Anomaly <span class="hlt">Observed</span> by GPS Radio Occultation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, King-Fai; Lin, Li-Ching; Bui, Xuan-Hien; Liang, Mao-Chang</p> <p>2018-01-01</p> <p>We have retrieved the latitudinal and vertical structures of the 11 year <span class="hlt">solar</span> cycle modulation on ionospheric electron density using 14 years of satellite-based radio occultation measurements utilizing the Global Positioning <span class="hlt">System</span>. The densities at the crests of the equatorial ionization anomaly (EIA) in the subtropics near 300 km in 2003 and 2014 (high <span class="hlt">solar</span> activity with <span class="hlt">solar</span> 10.7 cm flux, <fi>F</fi>10.7 ≈ 140 <span class="hlt">solar</span> flux unit (sfu)) were 3 times higher than that in 2009 (low <span class="hlt">solar</span> activity <fi>F</fi>10.7 ≈ 70 sfu). The higher density is attributed to the elevated <span class="hlt">solar</span> extreme ultraviolet and geomagnetic activity during high <span class="hlt">solar</span> activity periods. The location of the EIA crests moved 50 km upward and 10° poleward, because of the enhanced E × B force. The EIA in the northern hemisphere was more pronounced than that in the southern hemisphere. This interhemispheric asymmetry is consistent with the effect of enhanced transequatorial neutral wind. The above <span class="hlt">observations</span> were reproduced qualitatively by the two benchmark runs of the Thermosphere-Ionosphere-Electrodynamics General Circulation Model. In addition, we have studied the impact of the 11 year <span class="hlt">solar</span> cycle on the 27 day <span class="hlt">solar</span> cycle response of the ionospheric electron density. Beside the expected modulation on the amplitude of the 27 day <span class="hlt">solar</span> variation due to the 11 year <span class="hlt">solar</span> cycle, we find that the altitude of the maximal 27 day <span class="hlt">solar</span> response is unexpectedly 50 km higher than that of the 11 year <span class="hlt">solar</span> response. This is the first time that a vertical dependence of the <span class="hlt">solar</span> responses on different time scales is reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060029839&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=20060029839&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcorona"><span>Ka-band and X-band <span class="hlt">observations</span> of the <span class="hlt">solar</span> corona acquired during the Cassini 2001 superior conjunction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Morabito, D. D.</p> <p>2002-01-01</p> <p>Simultaneous dual-frequency Ka-band (32 GHz) and X-band (8.4 GHz) carrier signal data have been acquired during the superior conjunction of the Cassini spacecraft June 2001, using the NASA Deep Space Network's facilities located in Goldstone, California. The <span class="hlt">solar</span> elongation angle of the <span class="hlt">observations</span> varied from -4.1 degrees (-16 <span class="hlt">solar</span> radii) to -0.6 degrees (-2.3 <span class="hlt">solar</span> radii). The <span class="hlt">observed</span> coronal and <span class="hlt">solar</span> effects on the signals include spectral broadening, amplitude scintillation, phase scintillation, and increased noise. The measurements were generally consistent with existing <span class="hlt">solar</span> models, except during <span class="hlt">solar</span> transient events when the signatures of the measurements were <span class="hlt">observed</span> to increase significantly above the quiet background levels. This is the second <span class="hlt">solar</span> conjunction of Cassini for which simultaneous X/Ka data were acquired. Both <span class="hlt">solar</span> conjunctions, conducted in May 2000 and June 2001, occurred near the peak of the current 11 year <span class="hlt">solar</span> cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...611A..36V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...611A..36V"><span><span class="hlt">Solar</span>-wind predictions for the Parker <span class="hlt">Solar</span> Probe orbit. Near-Sun extrapolations derived from an empirical <span class="hlt">solar</span>-wind model based on Helios and OMNI <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>Venzmer, M. S.; Bothmer, V.</p> <p>2018-03-01</p> <p>Context. The Parker <span class="hlt">Solar</span> Probe (PSP; formerly <span class="hlt">Solar</span> Probe Plus) mission will be humanitys first in situ exploration of the <span class="hlt">solar</span> corona with closest perihelia at 9.86 <span class="hlt">solar</span> radii (R⊙) distance to the Sun. It will help answer hitherto unresolved questions on the heating of the <span class="hlt">solar</span> corona and the source and acceleration of the <span class="hlt">solar</span> wind and <span class="hlt">solar</span> energetic particles. The scope of this study is to model the <span class="hlt">solar</span>-wind environment for PSPs unprecedented distances in its prime mission phase during the years 2018 to 2025. The study is performed within the Coronagraphic German And US <span class="hlt">Solar</span>ProbePlus Survey (CGAUSS) which is the German contribution to the PSP mission as part of the Wide-field Imager for <span class="hlt">Solar</span> PRobe. Aim. We present an empirical <span class="hlt">solar</span>-wind model for the inner heliosphere which is derived from OMNI and Helios data. The German-US space probes Helios 1 and Helios 2 flew in the 1970s and <span class="hlt">observed</span> <span class="hlt">solar</span> wind in the ecliptic within heliocentric distances of 0.29 au to 0.98 au. The OMNI database consists of multi-spacecraft intercalibrated in situ data obtained near 1 au over more than five <span class="hlt">solar</span> cycles. The international sunspot number (SSN) and its predictions are used to derive dependencies of the major <span class="hlt">solar</span>-wind parameters on <span class="hlt">solar</span> activity and to forecast their properties for the PSP mission. Methods: The frequency distributions for the <span class="hlt">solar</span>-wind key parameters, magnetic field strength, proton velocity, density, and temperature, are represented by lognormal functions. In addition, we consider the velocity distributions bi-componental shape, consisting of a slower and a faster part. Functional relations to <span class="hlt">solar</span> activity are compiled with use of the OMNI data by correlating and fitting the frequency distributions with the SSN. Further, based on the combined data set from both Helios probes, the parameters frequency distributions are fitted with respect to <span class="hlt">solar</span> distance to obtain power law dependencies. Thus an empirical <span class="hlt">solar</span>-wind model for the inner</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820010812','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820010812"><span><span class="hlt">Solar</span> energy control <span class="hlt">system</span>. [temperature measurement</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Currie, J. R. (Inventor)</p> <p>1981-01-01</p> <p>A <span class="hlt">solar</span> energy control <span class="hlt">system</span> for a hot air type <span class="hlt">solar</span> energy heating <span class="hlt">system</span> wherein thermocouples are arranged to sense the temperature of a <span class="hlt">solar</span> collector, a space to be heated, and a top and bottom of a heat storage unit is disclosed. Pertinent thermocouples are differentially connected together, and these are employed to effect the operation of dampers, a fan, and an auxiliary heat source. In accomplishing this, the differential outputs from the thermocouples are amplified by a single amplifier by multiplexing techniques. Additionally, the amplifier is corrected as to offset by including as one multiplex channel a common reference signal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.tmp..843A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.tmp..843A"><span>Properties of the single Jovian planet population and the pursuit of <span class="hlt">Solar</span> <span class="hlt">system</span> analogues</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Agnew, Matthew T.; Maddison, Sarah T.; Horner, Jonathan</p> <p>2018-04-01</p> <p>While the number of exoplanets discovered continues to increase at a rapid rate, we are still to discover any <span class="hlt">system</span> that truly resembles the <span class="hlt">Solar</span> <span class="hlt">system</span>. Existing and near future surveys will likely continue this trend of rapid discovery. To see if these <span class="hlt">systems</span> are <span class="hlt">Solar</span> <span class="hlt">system</span> analogues, we will need to efficiently allocate resources to carry out intensive follow-up <span class="hlt">observations</span>. We seek to uncover the properties and trends across <span class="hlt">systems</span> that indicate how much of the habitable zone is stable in each <span class="hlt">system</span> to provide focus for planet hunters. We study the dynamics of all known single Jovian planetary <span class="hlt">systems</span>, to assess the dynamical stability of the habitable zone around their host stars. We perform a suite of simulations of all <span class="hlt">systems</span> where the Jovian planet will interact gravitationally with the habitable zone, and broadly classify these <span class="hlt">systems</span>. Besides the <span class="hlt">system</span>'s mass ratio (Mpl/Mstar), and the Jovian planet's semi-major axis (apl) and eccentricity (epl), we find that there are no underlying <span class="hlt">system</span> properties which are <span class="hlt">observable</span> that indicate the potential for planets to survive within the <span class="hlt">system</span>'s habitable zone. We use Mpl/Mstar, apl and epl to generate a parameter space over which the unstable <span class="hlt">systems</span> cluster, thus allowing us to predict which <span class="hlt">systems</span> to exclude from future <span class="hlt">observational</span> or numerical searches for habitable exoplanets. We also provide a candidate list of 20 <span class="hlt">systems</span> that have completely stable habitable zones and Jovian planets orbiting beyond the habitable zone as potential first order <span class="hlt">Solar</span> <span class="hlt">system</span> analogues.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22518823-new-observations-solar-kev-soft-ray-spectrum','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22518823-new-observations-solar-kev-soft-ray-spectrum"><span>NEW <span class="hlt">OBSERVATIONS</span> OF THE <span class="hlt">SOLAR</span> 0.5–5 KEV SOFT X-RAY SPECTRUM</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>Caspi, Amir; Woods, Thomas N.; Warren, Harry P.</p> <p>2015-03-20</p> <p>The <span class="hlt">solar</span> corona is orders of magnitude hotter than the underlying photosphere, but how the corona attains such high temperatures is still not understood. Soft X-ray (SXR) emission provides important diagnostics for thermal processes in the high-temperature corona, and is also an important driver of ionospheric dynamics at Earth. There is a crucial <span class="hlt">observational</span> gap between ∼0.2 and ∼4 keV, outside the ranges of existing spectrometers. We present <span class="hlt">observations</span> from a new SXR spectrometer, the Amptek X123-SDD, which measured the spatially integrated <span class="hlt">solar</span> spectral irradiance from ∼0.5 to ∼5 keV, with ∼0.15 keV FWHM resolution, during sounding rocket flights onmore » 2012 June 23 and 2013 October 21. These measurements show that the highly variable SXR emission is orders of magnitude greater than that during the deep minimum of 2009, even with only weak activity. The <span class="hlt">observed</span> spectra show significant high-temperature (5–10 MK) emission and are well fit by simple power-law temperature distributions with indices of ∼6, close to the predictions of nanoflare models of coronal heating. <span class="hlt">Observations</span> during the more active 2013 flight indicate an enrichment of low first-ionization potential elements of only ∼1.6, below the usually <span class="hlt">observed</span> value of ∼4, suggesting that abundance variations may be related to coronal heating processes. The XUV Photometer <span class="hlt">System</span> Level 4 data product, a spectral irradiance model derived from integrated broadband measurements, significantly overestimates the spectra from both flights, suggesting a need for revision of its non-flare reference spectra, with important implications for studies of Earth ionospheric dynamics driven by <span class="hlt">solar</span> SXRs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19970026762&hterms=senior&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsenior','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19970026762&hterms=senior&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsenior"><span>Optical Waveguide <span class="hlt">Solar</span> Energy <span class="hlt">System</span> for Lunar Materials Processing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nakamura, T.; Case, J. A.; Senior, C. L.</p> <p>1997-01-01</p> <p>This paper discusses results of our work on development of the Optical Waveguide (OW) <span class="hlt">Solar</span> Energy <span class="hlt">System</span> for Lunar Materials Processing. In the OW <span class="hlt">system</span> as shown, <span class="hlt">solar</span> radiation is collected by the concentrator which transfers the concentrated <span class="hlt">solar</span> radiation to the OW transmission line consisting of low-loss optical fibers. The OW line transmits the <span class="hlt">solar</span> radiation to the thermal reactor of the lunar materials processing plant. The feature of the OW <span class="hlt">system</span> are: (1) Highly concentrated <span class="hlt">solar</span> radiation (up to 104 suns) can be transmitted via flexible OW lines directly into the thermal reactor for materials processing: (2) <span class="hlt">Solar</span> radiation intensity or spectra can be tailored to specific materials processing steps; (3) Provide <span class="hlt">solar</span> energy to locations or inside of enclosures that would not otherwise have an access to <span class="hlt">solar</span> energy; and (4) The <span class="hlt">system</span> can be modularized and can be easily transported to and deployed at the lunar base.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IAUGA..2236038H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IAUGA..2236038H"><span>42 Years of Continuous <span class="hlt">Observations</span> of the <span class="hlt">Solar</span> Diameter - 1974 to 2015</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Humberto Andrei, Alexandre; Calderari Boscardin, Sergio; Lousada Penna, Jucira; Vani Leister, Nelson</p> <p>2015-08-01</p> <p>We present an analysis of 42 years of continuous measurements of the photospheric <span class="hlt">solar</span> diameter, taken at major national observatories, using the same fundamental method, and similar apparatus. Such a series overlap <span class="hlt">observations</span> from the Calern Observatory/France (<span class="hlt">Solar</span> Astrolabe in 1975-2003 to 253 obs/year lead by F. Laclare and C. Delmas; Doraysol in 2000-2005 to 3,070 obs/year lead by C. Delmas and V. Sinceac), from the IAG/USP/Brazil (<span class="hlt">Solar</span> Astrolabe in 1974-1994 to 95 obs/year lead by N. VaniLeister, P. Benevides and M. Emilio), from the Antalya Observatory/Turkey (CCD Astrolabe in 2000-2007 to 400 obs/year lead by F. Chollet and OI. Golbasi), from the San Fernando Observatory/Spain (<span class="hlt">Solar</span> Astrolabe in 1972-1975 to 133 obs/year lead by J. Muiños), from Observatório Nacional/Brasil (CCD Astrolabe in 1998-2009 to 1,820 obs/year lead by J. Penna, E. Reis Neto and A.H. Andrei; Heliometer 2010-2015 to 8,509 obs/year lead by S.C. Boscardin, J.L. Penna and A.H. Andrei). The Heliometer is fully automatized in its <span class="hlt">observations</span> and continues in regular operation with no plan of stopping; it shares with the former instruments the physical/mathematical definition of the limb, and the instruments aperture and focal length. We perform a reconciliation of all these series, using the common stretches. A modulation with the 11 years cycle of <span class="hlt">solar</span> activity is evident. However when such modulation is removed, both from the <span class="hlt">solar</span> diameter compound series and from the <span class="hlt">solar</span> activity series (given by the sunspots count), a very strong anti-correlation surfaces. This suggests a smaller diameter for the forthcoming cycles, in a behavior similar to that on the Minima of Dalton and Maunder. This study stresses the importance of keeping and make available such long, continuous, and uniform series of <span class="hlt">solar</span> diameter measurements. Maybe even the more by the controversy about its magnitude and origin. This presentation is dedicated to all the teams that developed and sustained the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070014939&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpuzzle','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070014939&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpuzzle"><span>Implications of RHESSI <span class="hlt">Observations</span> for <span class="hlt">Solar</span> Flare Models and Energetics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holman, Gordon D.</p> <p>2006-01-01</p> <p><span class="hlt">Observations</span> of <span class="hlt">solar</span> flares in X-rays and gamma-rays provide the most direct information about the hottest plasma and energetic electrons and ions accelerated in flares. The Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager (RHESSI) has <span class="hlt">observed</span> over 18000 <span class="hlt">solar</span> flares in X-rays and gamma-rays since its launch in February of 2002. RHESSI <span class="hlt">observes</span> the full Sun at photon energies from as low as 3 keV to as high as 17 MeV with a spectral resolution on the order of 1 keV. It also provides images in arbitrary bands within this energy range with spatial resolution as good as 3 seconds of arc. Full images are typically produced every 4 seconds, although higher time resolution is possible. This unprecedented combination of spatial, spectral, and temporal resolution, spectral range and flexibility has led to fundamental advances in our understanding of flares. I will show RHESSI and coordinated <span class="hlt">observations</span> that confirm coronal magnetic reconnection models for eruptive flares and coronal mass ejections, but also present new puzzles for these models. I will demonstrate how the analysis of RHESSI spectra has led to a better determination of the energy flux and total energy in accelerated electrons, and of the energy in the hot, thermal flare plasma. I will discuss how these energies compare with each other and with the energy contained in other flare-related phenomena such as interplanetary particles and coronal mass ejections.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810018607&hterms=gas+pump&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgas%2Bpump','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810018607&hterms=gas+pump&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgas%2Bpump"><span>Assessment of <span class="hlt">solar</span>-assisted gas-fired heat pump <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lansing, F. L.</p> <p>1981-01-01</p> <p>As a possible application for the Goldstone Energy Project, the performance of a 10 ton heat pump unit using a hybrid <span class="hlt">solar</span> gas energy source was evaluated in an effort to optimize the <span class="hlt">solar</span> collector size. The heat pump <span class="hlt">system</span> is designed to provide all the cooling and/or heating requirements of a selected office building. The <span class="hlt">system</span> performance is to be augmented in the heating mode by utilizing the waste heat from the power cycle. A simplified <span class="hlt">system</span> analysis is described to assess and compute interrrelationships of the engine, heat pump, and <span class="hlt">solar</span> and building performance parameters, and to optimize the <span class="hlt">solar</span> concentrator/building area ratio for a minimum total <span class="hlt">system</span> cost. In addition, four alternative heating cooling <span class="hlt">systems</span>, commonly used for building comfort, are described; their costs are compared, and are found to be less competitive with the gas <span class="hlt">solar</span> heat pump <span class="hlt">system</span> at the projected <span class="hlt">solar</span> equipment costs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860027106&hterms=Gravitational+motion+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DGravitational%2Bmotion%2Bsystem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860027106&hterms=Gravitational+motion+system&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DGravitational%2Bmotion%2Bsystem"><span>Terrestrial record of the <span class="hlt">solar</span> <span class="hlt">system</span>'s oscillation about the galactic plane</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stothers, R. B.</p> <p>1985-01-01</p> <p>A new study is presented of the <span class="hlt">observational</span> evidence pertaining to the theory which attributes the episodic component of the earth's impact cratering record over the past 600 Myr to gravitational encounters between the <span class="hlt">solar</span> <span class="hlt">system</span> and interstellar clouds that cause comets to fall into the <span class="hlt">solar</span> <span class="hlt">system</span> and impact the earth. Contrary to a claim by Thaddeus and Chanan (1985), the vertical scale height of the clouds seems to be sufficently small and the sun's vertical trajectory sufficiently large for the modulating effect of the sun's galactovertical motion to be detectable in the terrestrial record of impact cratering with at least a 50 percent a priori probability.</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://ntrs.nasa.gov/search.jsp?R=20060050341&hterms=white+cane&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwhite%2Bcane','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060050341&hterms=white+cane&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwhite%2Bcane"><span>On the Rates of Coronal Mass Ejections: Remote <span class="hlt">Solar</span> and In Situ <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>Riley, Pete; Schatzman, C.; Cane, H. V.; Richardson, I. G.; Gopalswamy, N.</p> <p>2006-01-01</p> <p>We compare the rates of coronal mass ejections (CMEs) as inferred from remote <span class="hlt">solar</span> <span class="hlt">observations</span> and interplanetary CMEs (ICMEs) as inferred from in situ <span class="hlt">observations</span> at both 1 AU and Ulyssses from 1996 through 2004. We also distinguish between those ICMEs that contain a magnetic cloud (MC) and those that do not. While the rates of CMEs and ICMEs track each other well at <span class="hlt">solar</span> minimum, they diverge significantly in early 1998, during the ascending phase of the <span class="hlt">solar</span> cycle, with the remote <span class="hlt">solar</span> <span class="hlt">observations</span> yielding approximately 20 times more events than are seen at 1 AU. This divergence persists through 2004. A similar divergence occurs between MCs and non-MC ICMEs. We argue that these divergences are due to the birth of midlatitude active regions, which are the sites of a distinct population of CMEs, only partially intercepted by Earth, and we present a simple geometric argument showing that the CME and ICME rates are consistent with one another. We also acknowledge contributions from (1) an increased rate of high-latitude CMEs and (2) focusing effects from the global <span class="hlt">solar</span> field. While our analysis, coupled with numerical modeling results, generally supports the interpretation that whether one <span class="hlt">observes</span> a MC within an ICME is sensitive to the trajectory of the spacecraft through the ICME (i.e., an <span class="hlt">observational</span> selection effect), one result directly contradicts it. Specifically, we find no systematic offset between the latitudinal origin of ICMEs that contain MCs at 1 AU in the ecliptic plane and that of those that do not.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021428&hterms=micro+wind&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmicro%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021428&hterms=micro+wind&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmicro%2Bwind"><span><span class="hlt">Observations</span> of micro-turbulence in the <span class="hlt">solar</span> wind near the sun with interplanetary scintillation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yamauchi, Y.; Misawa, H.; Kojima, M.; Mori, H.; Tanaka, T.; Takaba, H.; Kondo, T.; Tokumaru, M.; Manoharan, P. K.</p> <p>1995-01-01</p> <p>Velocity and density turbulence of <span class="hlt">solar</span> wind were inferred from interplanetary scintillation (IPS) <span class="hlt">observations</span> at 2.3 GHz and 8.5 GHz using a single-antenna. The <span class="hlt">observations</span> were made during September and October in 1992 - 1994. They covered the distance range between 5 and 76 <span class="hlt">solar</span> radii (Rs). We applied the spectrum fitting method to obtain a velocity, an axial ratio, an inner scale and a power-law spectrum index. We examined the difference of the turbulence properties near the Sun between low-speed <span class="hlt">solar</span> wind and high-speed <span class="hlt">solar</span> wind. Both of <span class="hlt">solar</span> winds showed acceleration at the distance range of 10 - 30 Rs. The radial dependence of anisotropy and spectrum index did not have significant difference between low-speed and high-speed <span class="hlt">solar</span> winds. Near the sun, the radial dependence of the inner scale showed the separation from the linear relation as reported by previous works. We found that the inner scale of high-speed <span class="hlt">solar</span> wind is larger than that of low-speed wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21313770-solar-cycle-lost-early-sunspot-observations-resolve-old-mystery','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21313770-solar-cycle-lost-early-sunspot-observations-resolve-old-mystery"><span>A <span class="hlt">SOLAR</span> CYCLE LOST IN 1793-1800: EARLY SUNSPOT <span class="hlt">OBSERVATIONS</span> RESOLVE THE OLD MYSTERY</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>Usoskin, Ilya G.; Mursula, Kalevi; Arlt, Rainer</p> <p>2009-08-01</p> <p>Because of the lack of reliable sunspot <span class="hlt">observations</span>, the quality of the sunspot number series is poor in the late 18th century, leading to the abnormally long <span class="hlt">solar</span> cycle (1784-1799) before the Dalton minimum. Using the newly recovered <span class="hlt">solar</span> drawings by the 18-19th century <span class="hlt">observers</span> Staudacher and Hamilton, we construct the <span class="hlt">solar</span> butterfly diagram, i.e., the latitudinal distribution of sunspots in the 1790s. The sudden, systematic occurrence of sunspots at high <span class="hlt">solar</span> latitudes in 1793-1796 unambiguously shows that a new cycle started in 1793, which was lost in the traditional Wolf sunspot series. This finally confirms the existence of themore » lost cycle that has been proposed earlier, thus resolving an old mystery. This Letter brings the attention of the scientific community to the need of revising the sunspot series in the 18th century. The presence of a new short, asymmetric cycle implies changes and constraints to sunspot cycle statistics, <span class="hlt">solar</span> activity predictions, and <span class="hlt">solar</span> dynamo theories, as well as for <span class="hlt">solar</span>-terrestrial relations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021265&hterms=faraday&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfaraday','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021265&hterms=faraday&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfaraday"><span>Faraday rotation fluctutation spectra <span class="hlt">observed</span> during <span class="hlt">solar</span> occultation of the Helios spacecraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Andreev, V.; Efimov, A. I.; Samoznaev, L.; Bird, M. K.</p> <p>1995-01-01</p> <p>Faraday rotation (FR) measurements using linearly polarized radio signals from the two Helios spacecraft were carried out during the period from 1975 to 1984. This paper presents the results of a spectral analysis of the Helios S-band FR fluctuations <span class="hlt">observed</span> at heliocentric distances from 2.6 to 15 <span class="hlt">solar</span> radii during the superior conjunctions 1975-1983. The mean intensity of the FR fluctuations does not exceed the noise level for <span class="hlt">solar</span> offsets greater than ca. 15 <span class="hlt">solar</span> radii. The rms FR fluctuation amplitude increases rapidly as the radio ray path approaches the Sun, varying according to a power law (exponent: 2.85 +/- 0.15) at <span class="hlt">solar</span> distances 4-12 <span class="hlt">solar</span> radii. At distances inside 4 <span class="hlt">solar</span> radii the increase is even steeper (exponent: 5.6 +/- 0.2). The equivalent two-dimensional FR fluctuation spectrum is well modeled by a single power-law over the frequency range from 5 to 50 mHz. For heliocentric distances larger than 4 <span class="hlt">solar</span> radii the spectral index varies between 1.1 and 1.6 with a mean value of 1.4 +/- 0.2, corresponding to a 3-D spectral index p = 2.4. FR fluctuations thus display a somwhat lower spectral index compared with phase and amplitude fluctuations. Surprisingly high values of the spectral index were found for measurements inside 4 <span class="hlt">solar</span> radii (p = 2.9 +/- 0.2). This may arise from the increasingly dominant effect of the magnetic field on radio wave propagation at small <span class="hlt">solar</span> offsets. Finally, a quasiperiodic component, believed to be associated with Alfven waves, was discovered in some (but not all!) fluctuation spectra <span class="hlt">observed</span> simultaneously at two ground stations. Characteristic periods and bulk velocities of this component were 240 +/- 30 sec and 300 +/- 60 km/s, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150010735','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150010735"><span>On Lunar Exospheric Column Densities and <span class="hlt">Solar</span> Wind Access Beyond the Terminator from ROSAT Soft X-Ray <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Wind Charge Exchange</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Collier, Michael R.; Snowden, S. L.; Sarantos, M.; Benna, M.; Carter, J. A.; Cravens, T. E.; Farrell, W. M.; Fatemi, S.; Hills, H. Kent; Hodges, R. R.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20150010735'); toggleEditAbsImage('author_20150010735_show'); toggleEditAbsImage('author_20150010735_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20150010735_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20150010735_hide"></p> <p>2014-01-01</p> <p>We analyze the Rontgen satellite (ROSAT) position sensitive proportional counter soft X-ray image of the Moon taken on 29 June 1990 by examining the radial profile of the surface brightness in three wedges: two 19 deg wedges (one north and one south) 13-32 deg off the terminator toward the dark side and one wedge 38 deg wide centered on the antisolar direction. The radial profiles of both the north and the south wedges show significant limb brightening that is absent in the 38 deg wide antisolar wedge. An analysis of the soft X-ray intensity increase associated with the limb brightening shows that its magnitude is consistent with that expected due to <span class="hlt">solar</span> wind charge exchange (SWCX) with the tenuous lunar atmosphere based on lunar exospheric models and hybrid simulation results of <span class="hlt">solar</span> wind access beyond the terminator. Soft X-ray imaging thus can independently infer the total lunar limb column density including all species, a property that before now has not been measured, and provide a large-scale picture of the <span class="hlt">solar</span> wind-lunar interaction. Because the SWCX signal appears to be dominated by exospheric species arising from <span class="hlt">solar</span> wind implantation, this technique can also determine how the exosphere varies with <span class="hlt">solar</span> wind conditions. Now, along with Mars, Venus, and Earth, the Moon represents another <span class="hlt">solar</span> <span class="hlt">system</span> body at which SWCX has been <span class="hlt">observed</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1981soen.proc...15W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1981soen.proc...15W"><span>Experiences in <span class="hlt">solar</span> cooling <span class="hlt">systems</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ward, D. S.</p> <p></p> <p>The results of performance evaluations for nine <span class="hlt">solar</span> cooling <span class="hlt">systems</span> are presented, and reasons fow low or high net energy balances are discussed. Six of the nine <span class="hlt">systems</span> are noted to have performed unfavorably compared to standard cooling <span class="hlt">systems</span> due to thermal storage losses, excessive <span class="hlt">system</span> electrical demands, inappropriate control strategies, poor <span class="hlt">system</span>-to-load matching, and poor chiller performance. A reduction in heat losses in one residential unit increased the total <span class="hlt">system</span> efficiency by 2.5%, while eliminating heat losses to the building interior increased the efficiency by 3.3%. The best <span class="hlt">system</span> incorporated a lithium bromide absorption chiller and a Rankine cycle compression unit for a commercial application. Improvements in the cooling tower and fan configurations to increase the <span class="hlt">solar</span> cooling <span class="hlt">system</span> efficiency are indicated. Best performances are expected to occur in climates inducing high annual cooling loads.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740051637&hterms=Solar+power+filters&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSolar%2Bpower%2Bfilters','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740051637&hterms=Solar+power+filters&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSolar%2Bpower%2Bfilters"><span>High voltage <span class="hlt">solar</span> cell power generating <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levy, E., Jr.; Opjorden, R. W.; Hoffman, A. C.</p> <p>1974-01-01</p> <p>A laboratory <span class="hlt">solar</span> power <span class="hlt">system</span> regulated by on-panel switches has been delivered for operating high power (3 kW), high voltage (15,000 volt) loads (communication tubes, ion thrusters). The modular <span class="hlt">system</span> consists of 26 <span class="hlt">solar</span> arrays, each with an integral light source and cooling <span class="hlt">system</span>. A typical array contains 2,560 series-connected cells. Each light source consists of twenty 500-watt tungsten iodide lamps providing plus or minus 5 percent uniformity at one <span class="hlt">solar</span> constant. An array temperature of less than 40 C is achieved using an infrared filter, a water-cooled plate, a vacuum hold-down <span class="hlt">system</span>, and air flushing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20100002102&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dpuzzle','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20100002102&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dpuzzle"><span><span class="hlt">Solar</span> Spicules Near and at the Limb, <span class="hlt">Observed</span> from Hinode</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, Alphonse C.; Moore, Ronald</p> <p>2009-01-01</p> <p><span class="hlt">Solar</span> spicules appear as narrow jets emanating from the chromosphere and extending into the corona. They have been <span class="hlt">observed</span> for over a hundred years, mainly in chromospheric spectral lines such as H-alpha. Because they are at the limit of visibility of ground-based instruments, their nature has long been a puzzle (Beckers 1968, 1972; Sterling 2000). In recent years however, vast progress has been made in understanding them both theoretically and <span class="hlt">observationally</span>, as spicule studies have undergone a revolution because of the superior resolution and time cadence of ground-based and space-based instruments (e.g., DePontieu et al. 2004). Even more rapid progress is currently underway, due to the <span class="hlt">Solar</span> Optical Telescope (SOT) instrument on the Hinode spacecraft (e.g., De Pontieu et al. 2007a, 2007b). Here we present <span class="hlt">observations</span> of spicules from Hinode SOT, as seen near the limb with the Ca II filtergraph.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008epsc.conf..835J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008epsc.conf..835J"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Science with LSST</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jones, R. L.; Chesley, S. R.; Connolly, A. J.; Harris, A. W.; Ivezic, Z.; Knezevic, Z.; Kubica, J.; Milani, A.; Trilling, D. E.</p> <p>2008-09-01</p> <p>The Large Synoptic Survey Telescope (LSST) will provide a unique tool to study moving objects throughout the <span class="hlt">solar</span> <span class="hlt">system</span>, creating massive catalogs of Near Earth Objects (NEOs), asteroids, Trojans, TransNeptunian Objects (TNOs), comets and planetary satellites with well-measured orbits and high quality, multi-color photometry accurate to 0.005 magnitudes for the brightest objects. In the baseline LSST <span class="hlt">observing</span> plan, back-to-back 15-second images will reach a limiting magnitude as faint as r=24.7 in each 9.6 square degree image, twice per night; a total of approximately 15,000 square degrees of the sky will be imaged in multiple filters every 3 nights. This time sampling will continue throughout each lunation, creating a huge database of <span class="hlt">observations</span>. Fig. 1 Sky coverage of LSST over 10 years; separate panels for each of the 6 LSST filters. Color bars indicate number of <span class="hlt">observations</span> in filter. The catalogs will include more than 80% of the potentially hazardous asteroids larger than 140m in diameter within the first 10 years of LSST operation, millions of main-belt asteroids and perhaps 20,000 Trans-Neptunian Objects. Objects with diameters as small as 100m in the Main Belt and <100km in the Kuiper Belt can be detected in individual images. Specialized `deep drilling' <span class="hlt">observing</span> sequences will detect KBOs down to 10s of kilometers in diameter. Long period comets will be detected at larger distances than previously possible, constrainting models of the Oort cloud. With the large number of objects expected in the catalogs, it may be possible to <span class="hlt">observe</span> a pristine comet start outgassing on its first journey into the inner <span class="hlt">solar</span> <span class="hlt">system</span>. By <span class="hlt">observing</span> fields over a wide range of ecliptic longitudes and latitudes, including large separations from the ecliptic plane, not only will these catalogs greatly increase the numbers of known objects, the characterization of the inclination distributions of these populations will be much improved. Derivation of proper elements for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AN....337.1064T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AN....337.1064T"><span>Daniel K. Inouye <span class="hlt">Solar</span> Telescope: High-resolution <span class="hlt">observing</span> of the dynamic Sun</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tritschler, A.; Rimmele, T. R.; Berukoff, S.; Casini, R.; Kuhn, J. R.; Lin, H.; Rast, M. P.; McMullin, J. P.; Schmidt, W.; Wöger, F.; DKIST Team</p> <p>2016-11-01</p> <p>The 4-m aperture Daniel K. Inouye <span class="hlt">Solar</span> Telescope (DKIST) formerly known as the Advanced Technology <span class="hlt">Solar</span> Telescope (ATST) is currently under construction on Haleakalā (Maui, Hawai'i) projected to start operations in 2019. At the time of completion, DKIST will be the largest ground-based <span class="hlt">solar</span> telescope providing unprecedented resolution and photon collecting power. The DKIST will be equipped with a set of first-light facility-class instruments offering unique imaging, spectroscopic and spectropolarimetric <span class="hlt">observing</span> opportunities covering the visible to infrared wavelength range. This first-light instrumentation suite will include: a Visible Broadband Imager (VBI) for high-spatial and -temporal resolution imaging of the <span class="hlt">solar</span> atmosphere; a Visible Spectro-Polarimeter (ViSP) for sensitive and accurate multi-line spectropolarimetry; a Fabry-Pérot based Visible Tunable Filter (VTF) for high-spatial resolution spectropolarimetry; a fiber-fed Diffraction-Limited Near Infra-Red Spectro-Polarimeter (DL-NIRSP) for two-dimensional high-spatial resolution spectropolarimetry (simultaneous spatial and spectral information); and a Cryogenic Near Infra-Red Spectro-Polarimeter (Cryo-NIRSP) for coronal magnetic field measurements and on-disk <span class="hlt">observations</span> of, e.g., the CO lines at 4.7 μm. We will provide an overview of the DKIST's unique capabilities with strong focus on the first-light instrumentation suite, highlight some of the additional properties supporting <span class="hlt">observations</span> of transient and dynamic <span class="hlt">solar</span> phenomena, and touch on some operational strategies and the DKIST critical science plan.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850063244&hterms=solar+photovoltaic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsolar%2Bphotovoltaic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850063244&hterms=solar+photovoltaic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsolar%2Bphotovoltaic"><span>Laser and <span class="hlt">solar</span>-photovoltaic space power <span class="hlt">systems</span> comparison. II.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>De Young, R. J.; Stripling, J.; Enderson, T. M.; Humes, D. H.; Davis, W. T.</p> <p>1984-01-01</p> <p>A comparison of total <span class="hlt">system</span> cost is made between <span class="hlt">solar</span> photovoltaic and laser/receiver <span class="hlt">systems</span>. The laser <span class="hlt">systems</span> assume either a <span class="hlt">solar</span>-pumped CO2 blackbody transfer laser with MHD receiver or a <span class="hlt">solar</span> pumped liquid neodymium laser with a photovoltaic receiver. Total <span class="hlt">system</span> costs are less for the laser <span class="hlt">systems</span> below 300 km where drag is significant. <span class="hlt">System</span> costs are highly dependent on altitude.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..186a2031G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..186a2031G"><span>Design and realization of an autonomous <span class="hlt">solar</span> <span class="hlt">system</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gaga, A.; Diouri, O.; Es-sbai, N.; Errahimi, F.</p> <p>2017-03-01</p> <p>The aim of this work is the design and realization of an autonomous <span class="hlt">solar</span> <span class="hlt">system</span>, with MPPT control, a regulator charge/discharge of batteries, an H-bridge multi-level inverter with acquisition <span class="hlt">system</span> and supervising based on a microcontroller. The proposed approach is based on developing a software platform in the LabVIEW environment which gives the <span class="hlt">system</span> a flexible structure for controlling, monitoring and supervising the whole <span class="hlt">system</span> in real time while providing power maximization and best quality of energy conversion from DC to AC power. The reliability of the proposed <span class="hlt">solar</span> <span class="hlt">system</span> is validated by the simulation results on PowerSim and experimental results achieved with a <span class="hlt">solar</span> panel, a Lead acid battery, <span class="hlt">solar</span> regulator and an H-bridge cascaded topology of single-phase inverter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003TrGeo...1..407D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003TrGeo...1..407D"><span>Condensation and Evaporation of <span class="hlt">Solar</span> <span class="hlt">System</span> Materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davis, A. M.; Richter, F. M.</p> <p>2003-12-01</p> <p>It is widely believed that the materials making up the <span class="hlt">solar</span> <span class="hlt">system</span> were derived from a nebular gas and dust cloud that went through an early high-temperature stage during which virtually all of the material was in the gas phase. At one time, it was thought that the entire inner <span class="hlt">solar</span> nebula was hot, but it is now believed that most material was processed through regions where high temperatures were achieved. Certainly some material, such as presolar grains (cf., Mendybaev et al., 2002a), has never been exposed to high temperatures. As the <span class="hlt">system</span> cooled, solids and perhaps liquids began to condense, but at some point the partially condensed materials became isolated from the remaining gas. Various lines of evidence support this view. At the largest scale, there is the <span class="hlt">observation</span> that the Earth, Moon, Mars, and all chondritic meteorites except for the CI chondrites are depleted to varying degrees in the abundances of moderately volatile elements relative to bulk <span class="hlt">solar</span> <span class="hlt">system</span> composition. The CI chondrites reflect the bulk composition of the <span class="hlt">solar</span> <span class="hlt">system</span> for all but hydrogen, carbon, nitrogen, oxygen, and the rare gases, the most volatile elements (see Chapter 1.03; Palme et al., 1988; McDonough and Sun, 1995; Humayun and Cassen, 2000). The depletions in moderately volatile elements are, to a significant degree, correlated with condensation temperature, suggesting progressive removal of gas as condensation proceeded ( Cassen, 1996). Additional <span class="hlt">observations</span> that can be explained by partial condensation are that various particularly primitive components of meteorites (e.g., calcium-, aluminum-rich refractory inclusions, and certain metal grains) have mineralogy and/or details of their chemical composition that are remarkably similar to what is calculated for equilibrium condensates from a <span class="hlt">solar</span> composition gas. For example, the calcium-, aluminum-rich inclusions (CAIs) in chondritic meteorites have compositions very similar to that calculated for the first 5% of total</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016A%26A...596A..42B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016A%26A...596A..42B"><span>Mass-loading of the <span class="hlt">solar</span> wind at 67P/Churyumov-Gerasimenko. <span class="hlt">Observations</span> and modelling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Behar, E.; Lindkvist, J.; Nilsson, H.; Holmström, M.; Stenberg-Wieser, G.; Ramstad, R.; Götz, C.</p> <p>2016-11-01</p> <p>Context. The first long-term in-situ <span class="hlt">observation</span> of the plasma environment in the vicinity of a comet, as provided by the European Rosetta spacecraft. Aims: Here we offer characterisation of the <span class="hlt">solar</span> wind flow near 67P/Churyumov-Gerasimenko (67P) and its long term evolution during low nucleus activity. We also aim to quantify and interpret the deflection and deceleration of the flow expected from ionization of neutral cometary particles within the undisturbed <span class="hlt">solar</span> wind. Methods: We have analysed in situ ion and magnetic field data and combined this with hybrid modeling of the interaction between the <span class="hlt">solar</span> wind and the comet atmosphere. Results: The <span class="hlt">solar</span> wind deflection is increasing with decreasing heliocentric distances, and exhibits very little deceleration. This is seen both in <span class="hlt">observations</span> and in modeled <span class="hlt">solar</span> wind protons. According to our model, energy and momentum are transferred from the <span class="hlt">solar</span> wind to the coma in a single region, centered on the nucleus, with a size in the order of 1000 km. This interaction affects, over larger scales, the downstream modeled <span class="hlt">solar</span> wind flow. The energy gained by the cometary ions is a small fraction of the energy available in the <span class="hlt">solar</span> wind. Conclusions: The deflection of the <span class="hlt">solar</span> wind is the strongest and clearest signature of the mass-loading for a small, low-activity comet, whereas there is little deceleration of the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910020921','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910020921"><span>Significant reduction in arc frequency biased <span class="hlt">solar</span> cells: <span class="hlt">Observations</span>, diagnostics, and mitigation technique(s)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Upschulte, B. L.; Weyl, G. M.; Marinelli, W. J.; Aifer, E.; Hastings, D.; Snyder, D.</p> <p>1991-01-01</p> <p>A variety of experiments were performed which identify key factors contributing to the arcing of negatively biased high voltage <span class="hlt">solar</span> cells. These efforts have led to reduction of greater than a factor of 100 in the arc frequency of a single cell following proper remediation procedures. Experiments naturally lead to and focussed on the adhesive/encapsulant that is used to bond the protective cover slip to the <span class="hlt">solar</span> cell. An image-intensified charge coupled device (CCD) camera <span class="hlt">system</span> recorded UV emission from arc events which occurred exclusively along the interfacial edge between the cover slip and the <span class="hlt">solar</span> cell. Microscopic inspection of this interfacial region showed a bead of encapsulant along this entire edge. Elimination of this encapsulant bead reduced the arc frequency by two orders of magnitude. Water contamination was also identified as a key contributor which enhances arcing of the encapsulant bead along the <span class="hlt">solar</span> cell edge. Spectrally resolved measurements of the <span class="hlt">observable</span> UV light shows a feature assignable to OH(A-X) electronic emission, which is common for water contaminated discharges. Experiments in which the <span class="hlt">solar</span> cell temperature was raised to 85 C showed a reduced arcing frequency, suggesting desorption of H2O. Exposing the <span class="hlt">solar</span> cell to water vapor was shown to increase the arcing frequency. Clean dry gases such as O2, N2, and Ar show no enhancement of the arcing rate. Elimination of the exposed encapsulant eliminates any measurable sensitivity to H2O vapor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040088897&hterms=Paradox+value&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DParadox%2Bvalue','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040088897&hterms=Paradox+value&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DParadox%2Bvalue"><span>The faint young Sun paradox: an <span class="hlt">observational</span> test of an alternative <span class="hlt">solar</span> model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gaidos, E. J.; Gudel, M.; Blake, G. A.</p> <p>2000-01-01</p> <p>We report the results of deep <span class="hlt">observations</span> at radio (3.6 cm) wavelengths of the nearby <span class="hlt">solar</span>-type star pi 01 Ursa Majoris with the Very Large Array (VLA) intended to test an alternative theory of <span class="hlt">solar</span> luminosity evolution. The standard model predicts a <span class="hlt">solar</span> luminosity only 75% of the present value and surface temperatures below freezing on Earth and Mars at 4 Ga, seemingly in conflict with geologic evidence for liquid water on these planets. An alternative model invokes a compensatory mass loss through a declining <span class="hlt">solar</span> wind that results in a more consistent early luminosity. The free-free emission from an enhanced wind around nearby young Sun-like stars should be detectable at microwave frequencies. Our <span class="hlt">observations</span> of pi 01 UMa, a 300 million year-old <span class="hlt">solar</span>-mass star, place an upper limit on the mass loss rate of 4-5 x 10(-11) M(<span class="hlt">solar</span>) yr-1. Total mass loss from such a star over 4 Gyr would be less than 6%. If this star is indeed an analog of the early Sun, it casts doubt on the alternative model as a solution to the faint young Sun paradox, particularly for Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015pthp.confE..57E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015pthp.confE..57E"><span>The exploration of exoplanets: What can we learn from <span class="hlt">solar</span> <span class="hlt">system</span> synergies?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Encrenaz, Therese</p> <p>2015-07-01</p> <p>Most of the discovered exoplanets are "exotic" with regard to the <span class="hlt">Solar</span> <span class="hlt">system</span>, with characteristics that are very different from our own planets. Still, we can use the experience gained in the study of the <span class="hlt">solar</span> <span class="hlt">system</span> planets for trying to understand the physical nature of exoplanets. The properties of their atmospheres are, as in the case of the <span class="hlt">Solar</span> <span class="hlt">system</span>, constrained by a few parameters: their mass and radius, the stellar radiation flux (and thus the star's properties and its distance to the planet), the planet's ellipticity, its inclination, its rotation, the presence or absence of a magnetosphere... Under some simple hypotheses (thermochemical equilibrium and absence of migration), it is possible to make simple predictions about the nature of the exoplanet's atmospheric composition, on the basis of the planet's mass and its equilibrium temperature. The study of <span class="hlt">solar</span> <span class="hlt">system</span> planets also tells us which other mechanisms may lead to a departure from thermochemical equilibrium, in particular photochemistry and transport-induced quenching. The study of planetary spectra is a good starting point to try to understand the spectra of exoplanets that now become available through transit spectroscopy <span class="hlt">observations</span>. From the spectral type of the hosting star and its distance to the exoplanet, one can estimate the spectral ranges where reflected/scattered stellar radiation and thermal emission dominate. In the thermal regime, the <span class="hlt">observation</span> of a given molecule in different bands of different intensities may provide constraints on the vertical thermal profile and the vertical distribution of the molecule.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.nrel.gov/esif/partnerships-caiso-first-solar.html','SCIGOVWS'); return false;" href="https://www.nrel.gov/esif/partnerships-caiso-first-solar.html"><span>NREL, California Independent <span class="hlt">System</span> Operator, and First <span class="hlt">Solar</span> | Energy</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p><em><span class="hlt">Solar</span></em> NREL, California Independent <span class="hlt">System</span> Operator, and First <em><span class="hlt">Solar</span></em> Demonstrate Essential Reliability Services with Utility-Scale <em><span class="hlt">Solar</span></em> NREL, the California Independent <span class="hlt">System</span> Operator (CAISO), and First <em><span class="hlt">Solar</span></em> conducted a demonstration project on a large utility-scale photovoltaic (<em>PV</em>) power plant in California to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810016050','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810016050"><span><span class="hlt">Solar</span> energy <span class="hlt">system</span> economic evaluation: Contemporary Newman, Georgia</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1980-01-01</p> <p>An economic evaluation of performance of the <span class="hlt">solar</span> energy <span class="hlt">system</span> (based on life cycle costs versus energy savings) for five cities considered to be representative of a broad range of environmental and economic conditions in the United States is discussed. The considered life cycle costs are: hardware, installation, maintenance, and operating costs for the <span class="hlt">solar</span> unique components of the total <span class="hlt">system</span>. The total <span class="hlt">system</span> takes into consideration long term average environmental conditions, loads, fuel costs, and other economic factors applicable in each of five cities. Selection criteria are based on availability of long term weather data, heating degree days, cold water supply temperature, <span class="hlt">solar</span> insolation, utility rates, market potential, and type of <span class="hlt">solar</span> <span class="hlt">system</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1980ibm..reptRX....','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1980ibm..reptRX...."><span><span class="hlt">Solar</span> energy <span class="hlt">system</span> economic evaluation: Contemporary Newman, Georgia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p>1980-09-01</p> <p>An economic evaluation of performance of the <span class="hlt">solar</span> energy <span class="hlt">system</span> (based on life cycle costs versus energy savings) for five cities considered to be representative of a broad range of environmental and economic conditions in the United States is discussed. The considered life cycle costs are: hardware, installation, maintenance, and operating costs for the <span class="hlt">solar</span> unique components of the total <span class="hlt">system</span>. The total <span class="hlt">system</span> takes into consideration long term average environmental conditions, loads, fuel costs, and other economic factors applicable in each of five cities. Selection criteria are based on availability of long term weather data, heating degree days, cold water supply temperature, <span class="hlt">solar</span> insolation, utility rates, market potential, and type of <span class="hlt">solar</span> <span class="hlt">system</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><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('https://eric.ed.gov/?q=solar+AND+radiation&pg=7&id=ED222643','ERIC'); return false;" href="https://eric.ed.gov/?q=solar+AND+radiation&pg=7&id=ED222643"><span>Development of a Conceptual Structure for Architectural <span class="hlt">Solar</span> Energy <span class="hlt">Systems</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>Ringel, Robert F.</p> <p></p> <p><span class="hlt">Solar</span> subsystems and components were identified and conceptual structure was developed for architectural <span class="hlt">solar</span> energy heating and cooling <span class="hlt">systems</span>. Recent literature related to <span class="hlt">solar</span> energy <span class="hlt">systems</span> was reviewed and analyzed. <span class="hlt">Solar</span> heating and cooling <span class="hlt">system</span>, subsystem, and component data were compared for agreement and completeness. Significant…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29866837','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29866837"><span>Proterozoic Milankovitch cycles and the history of the <span class="hlt">solar</span> <span class="hlt">system</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Meyers, Stephen R; Malinverno, Alberto</p> <p>2018-06-19</p> <p>The geologic record of Milankovitch climate cycles provides a rich conceptual and temporal framework for evaluating Earth <span class="hlt">system</span> evolution, bestowing a sharp lens through which to view our planet's history. However, the utility of these cycles for constraining the early Earth <span class="hlt">system</span> is hindered by seemingly insurmountable uncertainties in our knowledge of <span class="hlt">solar</span> <span class="hlt">system</span> behavior (including Earth-Moon history), and poor temporal control for validation of cycle periods (e.g., from radioisotopic dates). Here we address these problems using a Bayesian inversion approach to quantitatively link astronomical theory with geologic <span class="hlt">observation</span>, allowing a reconstruction of Proterozoic astronomical cycles, fundamental frequencies of the <span class="hlt">solar</span> <span class="hlt">system</span>, the precession constant, and the underlying geologic timescale, directly from stratigraphic data. Application of the approach to 1.4-billion-year-old rhythmites indicates a precession constant of 85.79 ± 2.72 arcsec/year (2σ), an Earth-Moon distance of 340,900 ± 2,600 km (2σ), and length of day of 18.68 ± 0.25 hours (2σ), with dominant climatic precession cycles of ∼14 ky and eccentricity cycles of ∼131 ky. The results confirm reduced tidal dissipation in the Proterozoic. A complementary analysis of Eocene rhythmites (∼55 Ma) illustrates how the approach offers a means to map out ancient <span class="hlt">solar</span> <span class="hlt">system</span> behavior and Earth-Moon history using the geologic archive. The method also provides robust quantitative uncertainties on the eccentricity and climatic precession periods, and derived astronomical timescales. As a consequence, the temporal resolution of ancient Earth <span class="hlt">system</span> processes is enhanced, and our knowledge of early <span class="hlt">solar</span> <span class="hlt">system</span> dynamics is greatly improved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810030756&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3DDunham','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810030756&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3DDunham"><span><span class="hlt">Observations</span> of a probable change in the <span class="hlt">solar</span> radius between 1715 and 1979</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dunham, D. W.; Sofia, S.; Fiala, A. D.; Muller, P. M.; Herald, D.</p> <p>1980-01-01</p> <p>A decrease in the <span class="hlt">solar</span> radius is determined using the technique of Dunham and Dunham (1973), in which timed <span class="hlt">observations</span> are made just inside the path edges. When the method is applied to the <span class="hlt">solar</span> eclipses of 1715, 1976, and 1979, the <span class="hlt">solar</span> radius for 1715 is 0.34 + or - 0.2 arc second larger than the recent values, with no significant change between 1976 and 1979. The duration of totality is examined as a function of distance from the edges of the path. Corrections to the radius of the sun derived from <span class="hlt">observations</span> of the 1976 and 1979 eclipses by the International Occultation Timing Association are also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011arec.conf..348C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011arec.conf..348C"><span>Design of <span class="hlt">Solar</span> Street Lamp Control <span class="hlt">System</span> Based on MPPT</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cui, Fengying</p> <p></p> <p>This paper proposes a new <span class="hlt">solar</span> street lamp control <span class="hlt">system</span> which is composed of photovoltaic cell, controller, battery and load. In this <span class="hlt">system</span> controller as the key part applies the microchip to achieve many functions. According to the nonlinear output characteristics of <span class="hlt">solar</span> cell and the influence of environment, it uses the perturbation and <span class="hlt">observation</span> (P&O) method to realize the maximum power point tracking (MPPT) and promotes the efficiency. In order to prolong the battery life the pulse width modulation (PWM) charge mode is selected to control the battery capacity and provent the battery from the state of over-charge and over-discharge. Meanwhile the function of temperature compensation, charge and discharge protection are set to improve the running safety and stability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25238324','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25238324"><span>Geology and photometric variation of <span class="hlt">solar</span> <span class="hlt">system</span> bodies with minor atmospheres: implications for solid exoplanets.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fujii, Yuka; Kimura, Jun; Dohm, James; Ohtake, Makiko</p> <p>2014-09-01</p> <p>A reasonable basis for future astronomical investigations of exoplanets lies in our best knowledge of the planets and satellites in the <span class="hlt">Solar</span> <span class="hlt">System</span>. <span class="hlt">Solar</span> <span class="hlt">System</span> bodies exhibit a wide variety of surface environments, even including potential habitable conditions beyond Earth, and it is essential to know how they can be characterized from outside the <span class="hlt">Solar</span> <span class="hlt">System</span>. In this study, we provide an overview of geological features of major <span class="hlt">Solar</span> <span class="hlt">System</span> solid bodies with minor atmospheres (i.e., the terrestrial Moon, Mercury, the Galilean moons, and Mars) that affect surface albedo at local to global scale, and we survey how they influence point-source photometry in the UV/visible/near IR (i.e., the reflection-dominant range). We simulate them based on recent mapping products and also compile <span class="hlt">observed</span> light curves where available. We show a 5-50% peak-to-trough variation amplitude in one spin rotation associated with various geological processes including heterogeneous surface compositions due to igneous activities, interaction with surrounding energetic particles, and distribution of grained materials. Some indications of these processes are provided by the amplitude and wavelength dependence of variation in combinations of the time-averaged spectra. We also estimate the photometric precision needed to detect their spin rotation rates through periodogram analysis. Our survey illustrates realistic possibilities for inferring the detailed properties of solid exoplanets with future direct imaging <span class="hlt">observations</span>. Key Words: Planetary environments-Planetary geology-<span class="hlt">Solar</span> <span class="hlt">System</span>-Extrasolar terrestrial planets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23131505K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23131505K"><span>Helioseismic <span class="hlt">Observations</span> of Two <span class="hlt">Solar</span> Cycles and Constraints on Dynamo Theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kosovichev, Alexander</p> <p>2018-01-01</p> <p>Helioseismology data from the SOHO and SDO, obtained in 1996-2017 for almost two <span class="hlt">solar</span> cycles, provide a unique opportunity to investigate variations of the <span class="hlt">solar</span> interior structure and dynamics, and link these variations to the current dynamo models and simulations. The <span class="hlt">solar</span> oscillation frequencies and frequency splitting of medium-degree p- and f-modes, as well as helioseismic inversions have been used to analyze variations of the differential rotation (“torsional oscillations”) and the global asphericity. By comparing the helioseismology results with the synoptic surface magnetic fields we identify characteristic changes associated the initiation and evolution of the <span class="hlt">solar</span> cycles, 23 and 24. The <span class="hlt">observational</span> results are compared with the current mean-field dynamo models and 3D MHD dynamo simulations. It is shown that the helioseismology inferences provide important constraints on the dynamics of the tachocline and near-surface shear layer, and also may explain the fundamental difference between the two <span class="hlt">solar</span> cycles and detect the onset of the next cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21452700-detection-vortex-tubes-solar-granulation-from-observations-sunrise','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21452700-detection-vortex-tubes-solar-granulation-from-observations-sunrise"><span>DETECTION OF VORTEX TUBES IN <span class="hlt">SOLAR</span> GRANULATION FROM <span class="hlt">OBSERVATIONS</span> WITH SUNRISE</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>Steiner, O.; Franz, M.; Bello Gonzalez, N.</p> <p>2010-11-10</p> <p>We have investigated a time series of continuum intensity maps and corresponding Dopplergrams of granulation in a very quiet <span class="hlt">solar</span> region at the disk center, recorded with the Imaging Magnetograph eXperiment (IMaX) on board the balloon-borne <span class="hlt">solar</span> observatory SUNRISE. We find that granules frequently show substructure in the form of lanes composed of a leading bright rim and a trailing dark edge, which move together from the boundary of a granule into the granule itself. We find strikingly similar events in synthesized intensity maps from an ab initio numerical simulation of <span class="hlt">solar</span> surface convection. From cross sections through the computationalmore » domain of the simulation, we conclude that these granular lanes are the visible signature of (horizontally oriented) vortex tubes. The characteristic optical appearance of vortex tubes at the <span class="hlt">solar</span> surface is explained. We propose that the <span class="hlt">observed</span> vortex tubes may represent only the large-scale end of a hierarchy of vortex tubes existing near the <span class="hlt">solar</span> surface.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110016582','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110016582"><span>Meteoroids: The Smallest <span class="hlt">Solar</span> <span class="hlt">System</span> Bodies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moser, Danielle E. (Compiler); Hardin, B. F. (Compiler); Janches, Diego (Compiler)</p> <p>2011-01-01</p> <p>This volume is a compilation of articles reflecting the current state of knowledge on the physics, chemistry, astronomy, and aeronomy of small bodies in the <span class="hlt">solar</span> <span class="hlt">system</span>. The articles included here represent the most recent results in meteor, meteoroid, and related research fields and were presented May 24-28, 2010, in Breckenridge, Colorado, USA at Meteoroids 2010: An International Conference on Minor Bodies in the <span class="hlt">Solar</span> <span class="hlt">System</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003263&hterms=light&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dlight','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003263&hterms=light&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dlight"><span>Deep HST/STIS Visible-Light Imaging of Debris <span class="hlt">Systems</span> Around <span class="hlt">Solar</span> Analog Hosts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schneider, Glenn; Grady, Carol A.; Stark, Christopher C.; Gaspar, Andras; Carson, Joseph; Debes, John H.; Henning, Thomas; Hines, Dean C.; Jang-Condell, Hannah; Kuchner, Marc J.</p> <p>2016-01-01</p> <p>We present new Hubble Space Telescope <span class="hlt">observations</span> of three a priori known starlight-scattering circumstellar debris <span class="hlt">systems</span> (CDSs) viewed at intermediate inclinations around nearby close-<span class="hlt">solar</span> analog stars: HD 207129, HD202628, and HD 202917. Each of these CDSs possesses ring-like components that are more massive analogs of our <span class="hlt">solar</span> <span class="hlt">systems</span> Edgeworth Kuiper Belt. These <span class="hlt">systems</span> were chosen for follow-up <span class="hlt">observations</span> to provide imaging with higher fidelity and better sensitivity for the sparse sample of <span class="hlt">solar</span>-analog CDSs that range over two decades in <span class="hlt">systemic</span> ages, with HD 202628 and HD 207129 (both approx. 2.3 Gyr) currently the oldest CDSs imaged in visible or near-IR light. These deep (10-14 ks) <span class="hlt">observations</span>, made with six-roll point-spread-function template visible-light coronagraphy using the Space Telescope Imaging Spectrograph, were designed to better reveal their angularly large debris rings of diffuse low surface brightness, and for all targets probe their exo-ring environments for starlight-scattering materials that present <span class="hlt">observational</span> challenges for current ground-based facilities and instruments. Contemporaneously also <span class="hlt">observing</span> with a narrower occulter position, these <span class="hlt">observations</span> additionally probe the CDS endo-ring environments that are seen to be relatively devoid of scatterers. We discuss the morphological, geometrical, and photometric properties of these CDSs also in the context of other CDSs hosted by FGK stars that we have previously imaged as a homogeneously <span class="hlt">observed</span> ensemble. From this combined sample we report a general decay in quiescent-disk F disk /F star optical brightness approx. t( exp.-0.8), similar to what is seen at thermal IR wavelengths, and CDSs with a significant diversity in scattering phase asymmetries, and spatial distributions of their starlight-scattering grains.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770005579','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770005579"><span>The Redox flow <span class="hlt">system</span> for <span class="hlt">solar</span> photovoltaic energy storage</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Odonnell, P.; Gahn, R. F.</p> <p>1976-01-01</p> <p>A new method of storage was applied to a <span class="hlt">solar</span> photovoltaic <span class="hlt">system</span>. The storage method is a redox flow <span class="hlt">system</span> which utilizes the oxidation-reduction capability of two soluble electrochemical redox couples for its storage capacity. The particular variant described separates the charging and discharging function of the <span class="hlt">system</span> such that the electrochemical couples are simultaneously charged and discharged in separate parts of the <span class="hlt">system</span>. The <span class="hlt">solar</span> array had 12 <span class="hlt">solar</span> cells; wired in order to give a range of voltages and currents. The <span class="hlt">system</span> stored the <span class="hlt">solar</span> energy so that a load could be run continually day and night. The main advantages of the redox <span class="hlt">system</span> are that it can accept a charge in the low voltage range and produce a relatively constant output regardless of <span class="hlt">solar</span> activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016MS%26E..147a2070V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016MS%26E..147a2070V"><span>Adaptability of <span class="hlt">solar</span> energy conversion <span class="hlt">systems</span> on ships</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Visa, I.; Cotorcea, A.; Neagoe, M.; Moldovan, M.</p> <p>2016-08-01</p> <p>International trade of goods largely uses maritime/transoceanic ships driven by engines using fossil fuels. This two centuries tradition is technologically mature but significantly adds to the CO2 emissions; therefore, recent trends focus on on-board implementation of <span class="hlt">systems</span> converting the <span class="hlt">solar</span> energy into power (photovoltaic <span class="hlt">systems</span>) or heat (<span class="hlt">solar</span>-thermal <span class="hlt">systems</span>). These <span class="hlt">systems</span> are carbon-emissions free but are still under research and plenty of effort is devoted to fast reach maturity and feasibility. Unlike the <span class="hlt">systems</span> implemented in a specific continental location, the design of <span class="hlt">solar</span> energy conversion <span class="hlt">systems</span> installed on shipboard has to face the problem generated by the <span class="hlt">system</span> base motion along with the ship travelling on routes at different latitudes: the navigation direction and sense and roll-pitch combined motion with reduced amplitude, but with relatively high frequency. These raise highly interesting challenges in the design and development of mechanical <span class="hlt">systems</span> that support the maximal output in terms of electricity or heat. The paper addresses the modelling of the relative position of a <span class="hlt">solar</span> energy conversion surface installed on a ship according to the current position of the sun; the model is based on the navigation trajectory/route, ship motion generated by waves and the relative sun-earth motion. The model describes the incidence angle of the sunray on the conversion surface through five characteristic angles: three used to define the ship orientation and two for the <span class="hlt">solar</span> angles; based on, their influence on the efficiency in <span class="hlt">solar</span> energy collection is analyzed by numerical simulations and appropriate recommendations are formulated for increasing the <span class="hlt">solar</span> energy conversion <span class="hlt">systems</span> adaptability on ships.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090025890','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090025890"><span>STEREO <span class="hlt">Observations</span> of Energetic Neutral Hydrogen Atoms during the 5 December 2006 <span class="hlt">Solar</span> Flare</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mewaldt, R. A.; Leske, R. A.; Stone, E. C.; Barghouty, A. F.; Labrador, A. W.; Cohen, C. M. S.; Cummings, A. C.; Davis, A. J.; vonRosenvinge, T. T.; Wiedenbeck, M. E.</p> <p>2009-01-01</p> <p>We report the discovery of energetic neutral hydrogen atoms emitted during the X9 <span class="hlt">solar</span> event of December 5, 2006. Beginning 1 hour following the onset of this E79 flare, the Low Energy Telescopes (LETs) on both the STEREO A and B spacecraft <span class="hlt">observed</span> a sudden burst of 1.6 to 15 MeV protons beginning hours before the onset of the main <span class="hlt">solar</span> energetic particle (SEP) event at Earth. More than 70% of these particles arrived from a longitude within 10 of the Sun, consistent with the measurement resolution. The derived emission profile at the Sun had onset and peak times remarkably similar to the GOES soft X-ray profile and continued for more than an hour. The <span class="hlt">observed</span> arrival directions and energy spectrum argue strongly that the particle events less than 5 MeV were due to energetic neutral hydrogen atoms (ENAs). To our knowledge, this is the first reported <span class="hlt">observation</span> of ENA emission from a <span class="hlt">solar</span> flare/coronal mass ejection. Possible origins for the production of ENAs in a large <span class="hlt">solar</span> event are considered. We conclude that the <span class="hlt">observed</span> ENAs were most likely produced in the high corona and that charge-transfer reactions between accelerated protons and partially-stripped coronal ions are an important source of ENAs in <span class="hlt">solar</span> events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850039166&hterms=population+characteristic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpopulation%2Bcharacteristic*','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850039166&hterms=population+characteristic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpopulation%2Bcharacteristic*"><span>Characteristics of <span class="hlt">solar</span> and heliospheric ion populations <span class="hlt">observed</span> near earth</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gloeckler, G.</p> <p>1984-01-01</p> <p>The composition and spectra of ions in <span class="hlt">solar</span>-energetic-particle and energetic-storm-particle events, of diffuse ions upstream of the earth bow shock, and of ions in deep-geomagnetic-tail plasmoids are characterized in a summary of in situ <span class="hlt">observations</span>. Data are presented in graphs and tables, and remarkable similarities are noted in the distribution functions of the heliospheric ion populations. The <span class="hlt">solar</span> wind, acting through acceleration mechanisms associated with shocks and turbulence, is identified as the major plasma source of suprathermal and energetic particles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760026534','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760026534"><span>Initial operation of a <span class="hlt">solar</span> heating and cooling <span class="hlt">system</span> in a full-scale <span class="hlt">solar</span> building test facility</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Knoll, R. H.; Miao, D.; Hamlet, I. L.; Jensen, R. N.</p> <p>1976-01-01</p> <p>The <span class="hlt">Solar</span> Building Test Facility (SBTF) was constructed to advance the technology for heating and cooling of office buildings with <span class="hlt">solar</span> energy. Its purposes are to (1) test <span class="hlt">system</span> components which include high-performing collectors, (2) test the performance of a complete <span class="hlt">solar</span> heating and cooling <span class="hlt">system</span>, (3) investigate component interactions, and (4) investigate durability, maintenance and reliability of components. The SBTF consists of a 50,000 square foot office building modified to accept <span class="hlt">solar</span> heated water for operation of an absorption air conditioner and for the baseboard heating <span class="hlt">system</span>. A 12,666 square foot <span class="hlt">solar</span> collector field with a 30,000 gallon storage tank provides the <span class="hlt">solar</span> heated water. A description of the <span class="hlt">system</span> and the collectors selected is printed along with the objectives, test approach, expected <span class="hlt">system</span> performance, and some preliminary results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020023610&hterms=systems+diffuse&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsystems%2Bdiffuse','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020023610&hterms=systems+diffuse&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsystems%2Bdiffuse"><span>Processing Mechanisms for Interstellar Ices: Connections to the <span class="hlt">Solar</span> <span class="hlt">System</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pendleton, Y. J.; Cuzzi, Jeffrey N. (Technical Monitor)</p> <p>1995-01-01</p> <p>The organic component of the interstellar medium, which has revealed itself through the ubiquitous 3.4 micrometers hydrocarbon absorption feature, is widespread throughout the disk of our galaxy and has been attributed to dust grains residing in the diffuse interstellar medium. The absorption band positions near 3.4 micrometers are characteristic of C-H stretching vibrations in the -CH3 and -CH2- groups of saturated aliphatic hydrocarbons associated with perturbing chemical groups. The production of complex molecules is thought to occur within dense molecular clouds when ice-mantled grains are processed by various energetic mechanisms. Studies of the processing of interstellar ices and the subsequent production of organic residues have relevance to studies of ices in the <span class="hlt">solar</span> <span class="hlt">system</span>, because primitive, icy <span class="hlt">solar</span> <span class="hlt">system</span> bodies such as those in the Kuiper belt are likely reservoirs of organic material, either preserved from the interstellar medium or produced in situ. Connections between the interstellar medium and the early <span class="hlt">solar</span> nebula have long been a source of interest. A comparison of the interstellar organics and the Murchison meteorite illustrates the importance of probing the interstellar connection to the <span class="hlt">solar</span> <span class="hlt">system</span>, because although the carbonaceous meteorites are undoubtedly highly processed, they do retain specific interstellar signatures (such as diamonds, SiC grains, graphite and enriched D/H). The organic component, while not proven interstellar, has a remarkable similarity to the interstellar organics <span class="hlt">observed</span> in over a dozen sightlines through our galaxy. This paper compares spectra from laboratory organics produced through the processing of interstellar ice analog materials with the high resolution infrared <span class="hlt">observations</span> of the interstellar medium in order to investigate the mechanisms (such as ion bombardment, plasma processing, and UV photolysis) that may be producing the organics in the ISM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003114&hterms=Wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DWind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003114&hterms=Wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DWind"><span>Slow <span class="hlt">Solar</span> Wind: <span class="hlt">Observations</span> and Modeling</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abbo, L.; Ofman, L.; Antiochos, S. K.; Hansteen, V. H.; Harra, L.; Ko, Y.-K.; Lapenta, G.; Li, B.; Riley, P.; Strachan, L.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003114'); toggleEditAbsImage('author_20170003114_show'); toggleEditAbsImage('author_20170003114_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003114_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003114_hide"></p> <p>2016-01-01</p> <p>While it is certain that the fast <span class="hlt">solar</span> wind originates from coronal holes, where and how the slow <span class="hlt">solar</span> wind (SSW) is formed remains an outstanding question in <span class="hlt">solar</span> physics even in the post-SOHO era. The quest for the SSW origin forms a major objective for the planned future missions such as the <span class="hlt">Solar</span> Orbiter and <span class="hlt">Solar</span> Probe Plus. Nonetheless, results from spacecraft data, combined with theoretical modeling, have helped to investigate many aspects of the SSW. Fundamental physical properties of the coronal plasma have been derived from spectroscopic and imaging remote-sensing data and in situ data, and these results have provided crucial insights for a deeper understanding of the origin and acceleration of the SSW. Advanced models of the SSW in coronal streamers and other structures have been developed using 3D MHD and multi-fluid equations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910008844','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910008844"><span>Megawatt <span class="hlt">solar</span> power <span class="hlt">systems</span> for lunar surface operations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Adams, B.; Alhadeff, S.; Beard, S.; Carlile, D.; Cook, D.; Douglas, C.; Garcia, D.; Gillespie, D.; Golingo, R.; Gonzalez, D.</p> <p>1990-01-01</p> <p>The work presented here shows that a <span class="hlt">solar</span> power <span class="hlt">system</span> can provide power on the order of one megawatt to a lunar base with a fairly high specific power. The main drawback to using <span class="hlt">solar</span> power is still the high mass, and therefore, cost of supplying energy storage through the <span class="hlt">solar</span> night. The use of cryogenic reactant storage in a fuel cell <span class="hlt">system</span>, however, greatly reduces the total <span class="hlt">system</span> mass over conventional energy storage schemes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19750045079&hterms=orbiting+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dorbiting%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19750045079&hterms=orbiting+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dorbiting%2Bwind"><span>Direct <span class="hlt">observations</span> of a flare related coronal and <span class="hlt">solar</span> wind disturbance</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gosling, J. T.; Hildner, E.; Macqueen, R. M.; Munro, R. H.; Poland, A. I.; Ross, C. L.</p> <p>1975-01-01</p> <p>Numerous mass ejections from the sun have been detected with orbiting coronagraphs. Here for the first time we document and discuss the direct association of a coronagraph <span class="hlt">observed</span> mass ejection, which followed a 2B flare, with a large interplanetary shock wave disturbance <span class="hlt">observed</span> at 1 AU. Estimates of the mass and energy content of the coronal disturbance are in reasonably good agreement with estimates of the mass and energy content of the <span class="hlt">solar</span> wind disturbance at 1 AU. The energy estimates as well as the transit time of the disturbance are also in good agreement with numerical models of shock wave propagation in the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23145206T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23145206T"><span><span class="hlt">Solar</span> <span class="hlt">System</span> Evolution through Planetesmial Collisions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Trierweiler, Isabella; Laughlin, Greg</p> <p>2018-01-01</p> <p>Understanding planet formation is crucial to unraveling the history of our <span class="hlt">Solar</span> <span class="hlt">System</span>. Refining our theory of planet formation has become particularly important as the discovery of exoplanet <span class="hlt">systems</span> through missions like Kepler have indicated that our <span class="hlt">system</span> is incredibly unique. Compared to other <span class="hlt">systems</span> around Sun-like stars, we are missing a significant amount of mass in the inner region of our <span class="hlt">solar</span> <span class="hlt">system</span>.A leading explanation for the low mass of the terrestrial planets is Jupiter’s Grand Tack. In this theory, the existence of the rocky planets is thought to be the result of the migration of Jupiter through the inner <span class="hlt">solar</span> <span class="hlt">system</span>. This migration could spark a collisional cascade of planetesimals, allowing planetesimals to drift inwards and shepherd an original set of massive planets into the Sun, thus explaining the absence of massive planets in our current <span class="hlt">system</span>. The remnants of the planetesimals would them become the building blocks for a new generation of smaller, rocky planets.Using the N-body simulator REBOUND, we investigate the dynamics of the Grand Tack. We focus in particular on collisional cascades, which are thought to cause the inward planetesimal drift. We first modify the simulator to account for fragmentation outcomes in planetesimal collisions. Modeling disks of varying initial conditions, we then characterize the disk conditions needed to begin a cascade and shed light on the <span class="hlt">solar</span> system’s dynamics just prior to the formation of the terrestrial planets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930066714&hterms=nu&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnu%253Fl','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930066714&hterms=nu&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnu%253Fl"><span><span class="hlt">Observations</span> of intermediate degree <span class="hlt">solar</span> oscillations - 1989 April-June</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bachmann, Kurt T.; Schou, Jesper; Brown, Timothy M.</p> <p>1993-01-01</p> <p>Frequencies, splittings, and line widths from 85 d of full disk Doppler <span class="hlt">observations</span> of <span class="hlt">solar</span> p-modes taken between April 4 and June 30, 1989 are presented. Comparison of the present mode parameters with published Big Bear <span class="hlt">Solar</span> Observatory (BBSO) results yields good agreement in general and is thus a confirmation of their work using an independent instrument and set of analysis routines. Average differences in p-mode frequencies measured by the two experiments in spring-summer 1989 are explained as a result of differences in the exact periods of data collection during a time of rapidly changing <span class="hlt">solar</span> activity. It is shown that the present a(1) splitting coefficients for p-modes with nu/L less than 45 micro-Hz suffer from a significant systematic error. Evidence is presented to the effect that a detector distortion or alignment problem, not a problem with the power spectra analysis, is the most likely explanation of this a(1) anomaly.</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><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><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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