Sample records for geomagnetic secular variations

  1. Geomagnetic field models incorporating physical constraints on the secular variation

    NASA Technical Reports Server (NTRS)

    Constable, Catherine; Parker, Robert L.

    1993-01-01

    This proposal has been concerned with methods for constructing geomagnetic field models that incorporate physical constraints on the secular variation. The principle goal that has been accomplished is the development of flexible algorithms designed to test whether the frozen flux approximation is adequate to describe the available geomagnetic data and their secular variation throughout this century. These have been applied to geomagnetic data from both the early and middle part of this century and convincingly demonstrate that there is no need to invoke violations of the frozen flux hypothesis in order to satisfy the available geomagnetic data.

  2. The 1995 revision of the joint US/UK geomagnetic field models - I. Secular variation

    USGS Publications Warehouse

    Macmillan, S.; Barraclough, D.R.; Quinn, J.M.; Coleman, R.J.

    1997-01-01

    We present the methods used to derive mathematical models of global secular variation of the main geomagnetic field for the period 1985 to 2000. These secular-variation models are used in the construction of the candidate US/UK models for the Definitive Geomagnetic Reference Field at 1990, the International Geomagnetic Reference Field for 1995 to 2000, and the World Magnetic Model for 1995 to 2000 (see paper II, Quinn et al., 1997). The main sources of data for the secular-variation models are geomagnetic observatories and repeat stations. Over the areas devoid of these data secular-variation information is extracted from aeromagnetic and satellite data. We describe how secular variation is predicted up to the year 2000 at the observatories and repeat stations, how the aeromagnetic and satellite data are used, and how all the data are combined to produce the required models.

  3. Localized sudden changes in the geomagnetic secular variation.

    USGS Publications Warehouse

    Alldredge, L.R.

    1987-01-01

    There is much debate as to whether there was a worldwide geomagnetic jerk in 1969 or 1970. It is agreed that there was an unusual sharp change in the secular variation in the east component, Y, in Europe at that time. This note points out how a localized sudden change in the secular variation pattern of one component in Europe can occur without having any large worldwide effects in any of the components. The accompanying changes in the spherical harmonic coefficients for such a localized change are also discussed. -after Author

  4. Analysis of geomagnetic secular variation during 1980-1985 and 1985- 1990, and geomagnetic models proposed for the 1991 revision of the International Geomagnetic Reference Field

    USGS Publications Warehouse

    Peddie, N.W.

    1992-01-01

    The secular variation of the main geomagnetic field during the periods 1980-1985 and 1985-1990 was analyzed in terms of spherical harmonics up to the eighth degree and order. Data from worldwide magnetic observatories and the Navy's Project MAGNET aerial surveys were used. The resulting pair of secular-variation models was used to update the Definitive Geomagnetic Reference Field (DGRF) model for 1980, resulting in new mainfield models for 1985.0 and 1990.0. These, along with the secular-variation model for 1985-1990, were proposed for the 1991 revision of the International Geomagnetic Reference Field (IGRF). -Author

  5. Geomagnetic Secular Variation Prediction with Thermal Heterogeneous Boundary Conditions

    NASA Astrophysics Data System (ADS)

    Kuang, W.; Tangborn, A.; Jiang, W.

    2011-12-01

    It has long been conjectured that thermal heterogeneity at the core-mantle boundary (CMB) affects the geodynamo substantially. The observed two pairs of steady and strong magnetic flux lobes near the Polar Regions and the low secular variation in the Pacific over the past 400 years (and perhaps longer) are likely the consequences of this CMB thermal heterogeneity. There are several studies on the impact of the thermal heterogeneity with numerical geodynamo simulations. However, direct correlation between the numerical results and the observations is found very difficult, except qualitative comparisons of certain features in the radial component of the magnetic field at the CMB. This makes it difficult to assess accurately the impact of thermal heterogeneity on the geodynamo and the geomagnetic secular variation. We revisit this problem with our MoSST_DAS system in which geomagnetic data are assimilated with our geodynamo model to predict geomagnetic secular variations. In this study, we implement a heterogeneous heat flux across the CMB that is chosen based on the seismic tomography of the lowermost mantle. The amplitude of the heat flux (relative to the mean heat flux across the CMB) varies in the simulation. With these assimilation studies, we will examine the influences of the heterogeneity on the forecast accuracies, e.g. the accuracies as functions of the heterogeneity amplitude. With these, we could be able to assess the model errors to the true core state, and thus the thermal heterogeneity in geodynamo modeling.

  6. Accounting for magnetic diffusion in core flow inversions from geomagnetic secular variation

    NASA Astrophysics Data System (ADS)

    Amit, Hagay; Christensen, Ulrich R.

    2008-12-01

    We use numerical dynamos to investigate the possible role of magnetic diffusion at the top of the core. We find that the contribution of radial magnetic diffusion to the secular variation is correlated with that of tangential magnetic diffusion for a wide range of control parameters. The correlation between the two diffusive terms is interpreted in terms of the variation in the strength of poloidal flow along a columnar flow tube. The amplitude ratio of the two diffusive terms is used to estimate the probable contribution of radial magnetic diffusion to the secular variation at Earth-like conditions. We then apply a model where radial magnetic diffusion is proportional to tangential diffusion to core flow inversions of geomagnetic secular variation data. We find that including magnetic diffusion does not change dramatically the global flow but some significant local variations appear. In the non frozen-flux core flow models (termed `diffusive'), the hemispherical dichotomy between the active Atlantic and quiet Pacific is weaker, a cyclonic vortex below North America emerges and the vortex below Asia is stronger. Our results have several important geophysical implications. First, our diffusive flow models contain some flow activity at low latitudes in the Pacific, suggesting a local balance between magnetic field advection and diffusion in that region. Second, the cyclone below North America in our diffusive flows reconciles the difference between mantle-driven thermal wind predictions and frozen-flux core flow models, and is consistent with the prominent intense magnetic flux patch below North America in geomagnetic field models. Finally, we hypothesize that magnetic diffusion near the core surface plays a larger role in the geomagnetic secular variation than usually assumed.

  7. Gravitational dynamos and the low-frequency geomagnetic secular variation.

    PubMed

    Olson, P

    2007-12-18

    Self-sustaining numerical dynamos are used to infer the sources of low-frequency secular variation of the geomagnetic field. Gravitational dynamo models powered by compositional convection in an electrically conducting, rotating fluid shell exhibit several regimes of magnetic field behavior with an increasing Rayleigh number of the convection, including nearly steady dipoles, chaotic nonreversing dipoles, and chaotic reversing dipoles. The time average dipole strength and dipolarity of the magnetic field decrease, whereas the dipole variability, average dipole tilt angle, and frequency of polarity reversals increase with Rayleigh number. Chaotic gravitational dynamos have large-amplitude dipole secular variation with maximum power at frequencies corresponding to a few cycles per million years on Earth. Their external magnetic field structure, dipole statistics, low-frequency power spectra, and polarity reversal frequency are comparable to the geomagnetic field. The magnetic variability is driven by the Lorentz force and is characterized by an inverse correlation between dynamo magnetic and kinetic energy fluctuations. A constant energy dissipation theory accounts for this inverse energy correlation, which is shown to produce conditions favorable for dipole drift, polarity reversals, and excursions.

  8. Gravitational dynamos and the low-frequency geomagnetic secular variation

    PubMed Central

    Olson, P.

    2007-01-01

    Self-sustaining numerical dynamos are used to infer the sources of low-frequency secular variation of the geomagnetic field. Gravitational dynamo models powered by compositional convection in an electrically conducting, rotating fluid shell exhibit several regimes of magnetic field behavior with an increasing Rayleigh number of the convection, including nearly steady dipoles, chaotic nonreversing dipoles, and chaotic reversing dipoles. The time average dipole strength and dipolarity of the magnetic field decrease, whereas the dipole variability, average dipole tilt angle, and frequency of polarity reversals increase with Rayleigh number. Chaotic gravitational dynamos have large-amplitude dipole secular variation with maximum power at frequencies corresponding to a few cycles per million years on Earth. Their external magnetic field structure, dipole statistics, low-frequency power spectra, and polarity reversal frequency are comparable to the geomagnetic field. The magnetic variability is driven by the Lorentz force and is characterized by an inverse correlation between dynamo magnetic and kinetic energy fluctuations. A constant energy dissipation theory accounts for this inverse energy correlation, which is shown to produce conditions favorable for dipole drift, polarity reversals, and excursions. PMID:18048345

  9. On the Possibilities of Predicting Geomagnetic Secular Variation with Geodynamo Modeling

    NASA Technical Reports Server (NTRS)

    Kuang, Wei-Jia; Tangborn, Andrew; Sabaka, Terrance

    2004-01-01

    We use our MoSST core dynamics model and geomagnetic field at the core-mantle boundary (CMB) continued downward from surface observations to investigate possibilities of geomagnetic data assimilation, so that model results and current geomagnetic observations can be used to predict geomagnetic secular variation in future. As the first attempt, we apply data insertion technique to examine evolution of the model solution that is modified by geomagnetic input. Our study demonstrate that, with a single data insertion, large-scale poloidal magnetic field obtained from subsequent numerical simulation evolves similarly to the observed geomagnetic variation, regardless of the initial choice of the model solution (so long it is a well developed numerical solution). The model solution diverges on the time scales on the order of 60 years, similar to the time scales of the torsional oscillations in the Earth's core. Our numerical test shows that geomagnetic data assimilation is promising with our MoSST model.

  10. A model of geomagnetic secular variation for 1980-1983

    USGS Publications Warehouse

    Peddie, N.W.; Zunde, A.K.

    1987-01-01

    We developed an updated model of the secular variation of the main geomagnetic field during 1980 through 1983 based on annual mean values for that interval from 148 worldwide magnetic observatories. The model consists of a series of 80 spherical harmonics, up to and including those of degree and order 8. We used it to form a proposal for the 1985 revision of the International Geomagnetic Reference Field (IGRF). Comparison of the new model, whose mean epoch is approximately 1982.0, with the Provisional Geomagnetic Reference Field for 1975-1980 (PGRF 1975), indicates that the moment of the centered-dipole part of the geomagnetic field is now decreasing faster than it was 5 years ago. The rate (in field units) indicated by PGRF 1975 was about -25 nT a-1, while for the new model it is -28 nT a-1. ?? 1987.

  11. Relative secular variations of the geomagnetic field along the Zgorzelec-Wiżajny profile, Poland

    NASA Astrophysics Data System (ADS)

    Wojas, Anna; Grabowska, Teresa; Mikołajczak, Mateusz

    2018-03-01

    The paper presents results of the study on relative secular variations of total magnetic intensity (TMI) of the geomagnetic field along the 700 km long profile crossing the area of Poland. Surveys were carried out at annual intervals between 1966 and 2016 (50 measurement series), in 31 survey sites (secular points) separated by about 22 km. The studied profile of the SW-NE direction, called Zgorzelec-Wiżajny (Z-W), crosses large parts of the main tectonic units of Europe, namely the Palaeozoic Platform of Central and Western Europe (PLZ) and the East European Craton (EEC), connected by the Teisseyre-Tornquist Zone (TTZ). Using the original methodology of analysis of measured data, reduced to the values of geomagnetic field recorded at the Central Geophysical Observatory in Belsk, the relative secular variations of TMI with the magnetic anomalies (ΔT) and the terrestrial heat flow density (Q) were graphically presented.

  12. On equatorially symmetric and antisymmetric geomagnetic secular variation timescales

    NASA Astrophysics Data System (ADS)

    Amit, Hagay; Coutelier, Maélie; Christensen, Ulrich R.

    2018-03-01

    It has been suggested that the secular variation (SV) timescales of the geomagnetic field vary as 1 / ℓ (where ℓ is the spherical harmonic degree), except for the dipole. Here we propose that the same scaling law applies for SV timescales defined for different symmetry classes of the geomagnetic field and SV. We decompose the field and its SV into symmetric and antisymmetric parts and show in geomagnetic field models and numerical dynamo simulations that the corresponding SV timescales also vary as 1 / ℓ , again except for the dipole. The time-average antisymmetric/symmetric SV timescales are larger/smaller than the total, respectively. The difference in SV timescales between these two symmetry classes is probably due to different degrees of alignment of the core flow with different magnetic field structures at the core-mantle boundary. The symmetric dipole SV timescale in the recent geomagnetic field and in long-term time-averages from numerical dynamos is below the extrapolated 1 / ℓ curve, whereas before ∼ 1965 the geomagnetic dipole tilt was rather steady and the symmetric dipole SV timescale exceeded the extrapolated 1 / ℓ curve. We hypothesize that the period of nearly steady geomagnetic dipole tilt between 1810-1965 was anomalous for the geodynamo. Overall, the deviation of the dipole SV timescales from the 1 / ℓ curves may indicate that magnetic diffusion contributes to the dipole SV more than it does for higher degrees.

  13. Spatial Distribution and Secular Variation of Geomagnetic Filed in China Described by the CHAOS-6 Model and its Error Analysis

    NASA Astrophysics Data System (ADS)

    Wang, Z.; Gu, Z.; Chen, B.; Yuan, J.; Wang, C.

    2016-12-01

    The CHAOS-6 geomagnetic field model, presented in 2016 by the Denmark's national space institute (DTU Space), is a model of the near-Earth magnetic field. According the CHAOS-6 model, seven component data of geomagnetic filed at 30 observatories in China in 2015 and at 3 observatories in China spanning the time interval 2008.0-2016.5 were calculated. Also seven component data of geomagnetic filed from the geomagnetic data of practical observations in China was obtained. Based on the model calculated data and the practical data, we have compared and analyzed the spatial distribution and the secular variation of the geomagnetic field in China. There is obvious difference between the two type data. The CHAOS-6 model cannot describe the spatial distribution and the secular variation of the geomagnetic field in China with comparative precision because of the regional and local magnetic anomalies in China.

  14. The geomagnetic jerk of 2003.5-characterisation with regional observatory secular variation data

    NASA Astrophysics Data System (ADS)

    Feng, Yan; Holme, Richard; Cox, Grace Alexandra; Jiang, Yi

    2018-05-01

    The 2003.5 geomagnetic jerk was identified in geomagnetic records from satellite data, and a matching feature reported in variations in length-of-day (ΔLOD), but detailed study has been hampered by lack of geomagnetic observatory data where it appears strongest. Here we examine secular variation (annual differences of monthly means) based on a new resource of 43 Chinese observatory records for 1998 until the present, focusing on 10 series of particularly high quality and consistency. To obtain a clean series, we calculate the covariance matrix of residuals between measurements and a state-of-the-art field model, CHAOS-6, and use eigenvalue analysis to remove noisy contributions from the uncorrected data. The magnitude of the most significant eigenvector correlates well with Dcx (corrected, extended Dst), suggesting the noise originates from unmodelled external magnetic field. Removal of this noise eliminates much coherent misfit around 2003-2005; nevertheless, the 2003.5 jerk is seen clearly in the first time derivative of the East component in Chinese data, and is also seen in the first time derivative of the vertical component in European data. Estimates of the jerk time are centred on 2003.5, but with some spatial variation; this variation can be eliminated if we allow a discontinuity in the secular variation as well as its temporal gradient. Both regions also provide evidence for a jerk around 2014, although less clearly than 2003.5. We create a new field model based on new data and CHAOS-6 to further examine the regional signals. The new model is close to CHAOS-6, but better fits Chinese data, although modelling also identifies some data features as unphysical.

  15. New evidence of a fast secular variation of the geomagnetic field 1000 BCE: archaeomagnetic study of Bavarian potteries

    NASA Astrophysics Data System (ADS)

    Hervé, G.; Gilder, S.; Fassbinder, J.; Metzler-Nebelsick, C.; Schnepp, E.; Geisweid, L.; Putz, A.; Reuss, S.; Riedel, G.; Westhausen, I.; Wittenborn, F.

    2016-12-01

    This study presents new archaeointensity results obtained on 350 pottery sherds from 45 graves and pits from 12 sites around Munich (Germany). The features are dated between 1400 and 400 BCE by ceramic and metallic artifacts, radiocarbon and dendrochronology. We collected only red- or partly red-colored sherds in order to minimize mineralogical alteration during laboratory experiments. Rock magnetism analyses show that the remanent magnetization is mainly carried by titanomagnetite. Archaeointensities were determined using the Thellier-Thellier protocol with corrections of TRM anisotropy and cooling rate on one to three specimens per sherd. The experiments were completed using Triaxe and multispecimen (MSP-DSC) methods. Around 60 per cent of the sherds provide reliable results, allowing the computation of 35 mean archaeointensity values. This quadruples the number of previously published data in Western Europe. The secular variation of the geomagnetic field strength is low from 1400 to 1200 BCE with intensities close to 50 µT then the intensity increased to 70 µT around 1000-900 BCE. After a minimum 50 µT near 750 BCE, the intensity increased again to 90 µT at 650 BCE. This high secular variation rate (0.4 µT/year) is especially apparent in the sherds from a fountain dated between 750 and 650 BCE. Next, the intensity remained high until 400 BCE before rapidly decreasing to 200 BCE. As the sharp change in geomagnetic direction around 800 BCE is not contemporaneous with an intensity high, this period is probably not characterized by an archaeomagnetic jerk. The trend of secular variation with two intensity maxima is similar to the one observed in the Near East. The Virtual Axial Dipole Moments of the two regions are approximately the same after 700 BCE, but before they are systematically 1-2 × 1022 Am2 higher in the Near East. This difference may be a further proof of a geomagnetic field anomaly in this area 1000 BCE, yet there is no evidence for a geomagnetic

  16. Time-causal decomposition of geomagnetic time series into secular variation, solar quiet, and disturbance signals

    USGS Publications Warehouse

    Rigler, E. Joshua

    2017-04-26

    A theoretical basis and prototype numerical algorithm are provided that decompose regular time series of geomagnetic observations into three components: secular variation; solar quiet, and disturbance. Respectively, these three components correspond roughly to slow changes in the Earth’s internal magnetic field, periodic daily variations caused by quasi-stationary (with respect to the sun) electrical current systems in the Earth’s magnetosphere, and episodic perturbations to the geomagnetic baseline that are typically driven by fluctuations in a solar wind that interacts electromagnetically with the Earth’s magnetosphere. In contrast to similar algorithms applied to geomagnetic data in the past, this one addresses the issue of real time data acquisition directly by applying a time-causal, exponential smoother with “seasonal corrections” to the data as soon as they become available.

  17. Simultaneous stochastic inversion for geomagnetic main field and secular variation. II - 1820-1980

    NASA Technical Reports Server (NTRS)

    Bloxham, Jeremy; Jackson, Andrew

    1989-01-01

    With the aim of producing readable time-dependent maps of the geomagnetic field at the core-mantle boundary, the method of simultaneous stochastic inversion for the geomagnetic main field and secular variation, described by Bloxham (1987), was applied to survey data from the period 1820-1980 to yield two time-dependent geomagnetic-field models, one for the period 1900-1980 and the other for 1820-1900. Particular consideration was given to the effect of crustal fields on observations. It was found that the existing methods of accounting for these fields as sources of random noise are inadequate in two circumstances: (1) when sequences of measurements are made at one particular site, and (2) for measurements made at satellite altitude. The present model shows many of the features in the earth's magnetic field at the core-mantle boundary described by Bloxham and Gubbins (1985) and supports many of their earlier conclusions.

  18. Modeling of geomagnetic field secular variations observed in the Balkan area for purposes of regional topographic mapping

    NASA Astrophysics Data System (ADS)

    Metodiev, Metodi; Trifonova, Petya; Buchvarov, Ivan

    2014-05-01

    The most significant of the Earth's magnetic field elements is the geomagnetic declination, which is widely used in geodesy, cartography and their associated navigational systems. The geomagnetic declination is incorporated in the naval navigation maps and is used in the navigation process. It is also a very important factor for aviation where declination data have major importance for every airport (civil or military). As the geomagnetic field changes with time but maps of the geomagnetic declination are not published annually and are reduced to an epoch in the past, it is necessary to define two additional parameters in the maps, needed to determine the value of the geomagnetic declination for a particular moment in the future: 1) estimated value of the annual declination variation and 2) a table with the average diurnal variation of the declination for a given month and hour. The goal of our research is to analyze the annual mean values of geomagnetic declination on the territory of the Balkan Peninsula for obtaining of a best fitting model of that parameter which can be used for prediction of the declination value for the next 10 years. The same study was performed in 1990 for the purposes of Bulgarian declination map's preparation. As a result, a linear model of the declination annual variation was obtained for the neighboring observatories and repeat stations data, and a map of the obtained values for the Bulgarian territory was drawn. We use the latest version of the GFZ Reference Internal Magnetic Model (GRIMM-3.0) to compare the magnetic field evolution predicted by that model between 2001 and 2010 to the data collected in five independent geomagnetic observatories in the Balkan region (PAG, SUA, PEG, IZN, GCK) over the same time interval. We conclude that the geomagnetic core field secular variation in this area is well described by the global model. The observed small-scale differences might indicate induced lithospheric anomalies but it is still an open

  19. Statistics of the geomagnetic secular variation for the past 5Ma

    NASA Technical Reports Server (NTRS)

    Constable, C. G.; Parker, R. L.

    1986-01-01

    A new statistical model is proposed for the geomagnetic secular variation over the past 5Ma. Unlike previous models, the model makes use of statistical characteristics of the present day geomagnetic field. The spatial power spectrum of the non-dipole field is consistent with a white source near the core-mantle boundary with Gaussian distribution. After a suitable scaling, the spherical harmonic coefficients may be regarded as statistical samples from a single giant Gaussian process; this is the model of the non-dipole field. The model can be combined with an arbitrary statistical description of the dipole and probability density functions and cumulative distribution functions can be computed for declination and inclination that would be observed at any site on Earth's surface. Global paleomagnetic data spanning the past 5Ma are used to constrain the statistics of the dipole part of the field. A simple model is found to be consistent with the available data. An advantage of specifying the model in terms of the spherical harmonic coefficients is that it is a complete statistical description of the geomagnetic field, enabling us to test specific properties for a general description. Both intensity and directional data distributions may be tested to see if they satisfy the expected model distributions.

  20. A study of alternative schemes for extrapolation of secular variation at observatories

    USGS Publications Warehouse

    Alldredge, L.R.

    1976-01-01

    The geomagnetic secular variation is not well known. This limits the useful life of geomagnetic models. The secular variation is usually assumed to be linear with time. It is found that attenative schemes that employ quasiperiodic variations from internal and external sources can improve the extrapolation of secular variation at high-quality observatories. Although the schemes discussed are not yet fully applicable in worldwide model making, they do suggest some basic ideas that may be developed into useful tools in future model work. ?? 1976.

  1. Importance of selecting archaeomagnetic data for geomagnetic modelling: example of the new Western Europe directional and intensity secular variation curves from 1500 BC to 200 AD

    NASA Astrophysics Data System (ADS)

    Herve, Gwenael; Chauvin, Annick; Lanos, Philippe

    2014-05-01

    At the regional scale, the dispersion between archaeomagnetic data and especially archaeointensities suggests that some of them may be biased. As a consequence, it appears necessary to perform a selection of available data before to compute mean regional secular variation curves or geomagnetic models. However the definition of suitable selection criteria is not obvious and we need to know how to manage "old" data acquired during the 60-70s. The Western Europe directional and intensity data set from 1500 BC to 200 AD allows to discuss these issues. It has recently been enhanced by 39 new archaeodirections and 23 new archaeointensities (Hervé et al., 2013a and 2013b data sets and 5 unpublished data). First, the whole Western Europe data set was selected but the strong dispersion restricted the accuracy and the reliability of the new Western Europe secular variation curves at Paris. The causes of the dispersion appear different between archaeodirections and archaeointensities. In the directional data set, the main problem comes from some age errors in the oldest published data. Since their publication their archaeological dating may have changed of 50 years or more. For intensity data that were acquired much more recently, the dispersion mainly results from the use of unreliable archaeointensity protocols. We propose a weighting approach based on the number of specimens and the use of pTRM-checks, anisotropy and cooling rate corrections. Only 63% of available archaeodirections and 32% of archaeointensities were used to build the new Western Europe secular variation curves from 1500 BC to 200 AD. These curves reveal that selecting the reference data avoids wrong estimations of the shape of the secular variation curves, the secular variation rate, the dating of archaeomagnetic jerks... Finally, it is worth pointing out that current geomagnetic global models take into account almost all the data that we decided to reject. It could partly explain why their predictions at

  2. Statistics of the geomagnetic secular variation for the past 5 m.y

    NASA Technical Reports Server (NTRS)

    Constable, C. G.; Parker, R. L.

    1988-01-01

    A new statistical model is proposed for the geomagnetic secular variation over the past 5Ma. Unlike previous models, the model makes use of statistical characteristics of the present day geomagnetic field. The spatial power spectrum of the non-dipole field is consistent with a white source near the core-mantle boundary with Gaussian distribution. After a suitable scaling, the spherical harmonic coefficients may be regarded as statistical samples from a single giant Gaussian process; this is the model of the non-dipole field. The model can be combined with an arbitrary statistical description of the dipole and probability density functions and cumulative distribution functions can be computed for declination and inclination that would be observed at any site on Earth's surface. Global paleomagnetic data spanning the past 5Ma are used to constrain the statistics of the dipole part of the field. A simple model is found to be consistent with the available data. An advantage of specifying the model in terms of the spherical harmonic coefficients is that it is a complete statistical description of the geomagnetic field, enabling us to test specific properties for a general description. Both intensity and directional data distributions may be tested to see if they satisfy the expected model distributions.

  3. Geomagnetic field secular variation in Pacific Ocean: A Bayesian reference curve based on Holocene Hawaiian lava flows

    NASA Astrophysics Data System (ADS)

    Tema, E.; Herrero-Bervera, E.; Lanos, Ph.

    2017-11-01

    Hawaii is an ideal place for reconstructing the past variations of the Earth's magnetic field in the Pacific Ocean thanks to the almost continuous volcanic activity during the last 10 000 yrs. We present here an updated compilation of palaeomagnetic data from historic and radiocarbon dated Hawaiian lava flows available for the last ten millennia. A total of 278 directional and 66 intensity reference data have been used for the calculation of the first full geomagnetic field reference secular variation (SV) curves for central Pacific covering the last ten millennia. The obtained SV curves are calculated following recent advances on curve building based on the Bayesian statistics and are well constrained for the last five millennia while for older periods their error envelopes are wide due to the scarce number of reference data. The new Bayesian SV curves show three clear intensity maxima during the last 3000 yrs that are accompanied by sharp directional changes. Such short-term variations of the geomagnetic field could be interpreted as archaeomagnetic jerks and could be an interesting feature of the geomagnetic field variation in the Pacific Ocean that should be further explored by new data.

  4. Dynamic Responses of the Earth's Outer Core to Assimilation of Observed Geomagnetic Secular Variation

    NASA Technical Reports Server (NTRS)

    Kuang, Weijia; Tangborn, Andrew

    2014-01-01

    Assimilation of surface geomagnetic observations and geodynamo models has advanced very quickly in recent years. However, compared to advanced data assimilation systems in meteorology, geomagnetic data assimilation (GDAS) is still in an early stage. Among many challenges ranging from data to models is the disparity between the short observation records and the long time scales of the core dynamics. To better utilize available observational information, we have made an effort in this study to directly assimilate the Gauss coefficients of both the core field and its secular variation (SV) obtained via global geomagnetic field modeling, aiming at understanding the dynamical responses of the core fluid to these additional observational constraints. Our studies show that the SV assimilation helps significantly to shorten the dynamo model spin-up process. The flow beneath the core-mantle boundary (CMB) responds significantly to the observed field and its SV. The strongest responses occur in the relatively small scale flow (of the degrees L is approx. 30 in spherical harmonic expansions). This part of the flow includes the axisymmetric toroidal flow (of order m = 0) and non-axisymmetric poloidal flow with m (is) greater than 5. These responses can be used to better understand the core flow and, in particular, to improve accuracies of predicting geomagnetic variability in future.

  5. Constraints on geomagnetic secular variation modeling from electromagnetism and fluid dynamics of the Earth's core

    NASA Technical Reports Server (NTRS)

    Benton, E. R.

    1986-01-01

    A spherical harmonic representation of the geomagnetic field and its secular variation for epoch 1980, designated GSFC(9/84), is derived and evaluated. At three epochs (1977.5, 1980.0, 1982.5) this model incorporates conservation of magnetic flux through five selected patches of area on the core/mantle boundary bounded by the zero contours of vertical magnetic field. These fifteen nonlinear constraints are included like data in an iterative least squares parameter estimation procedure that starts with the recently derived unconstrained field model GSFC (12/83). Convergence is approached within three iterations. The constrained model is evaluated by comparing its predictive capability outside the time span of its data, in terms of residuals at magnetic observatories, with that for the unconstrained model.

  6. Archaeomagnetic results from southern Italy and their bearing on geomagnetic secular variation

    NASA Astrophysics Data System (ADS)

    Evans, M. E.; Hoye, G. S.

    2005-07-01

    Archaeodirectional results from kilns and other baked structures in southern Italy are presented. They are generally compatible with the much larger data sets from France and Bulgaria. In particular, a summary of all the results associated with the well-known eruption of Vesuvius that destroyed Pompeii ( n = 9, D = 355°, I = 58°, α95 = 1.5°) provides a reliable archaeomagnetic anchor point supporting the French and Bulgarian master curves. It is extremely well-constrained in time and it comprises independent studies carried out in four different countries. Furthermore, it is derived from a diverse set of features agreement amongst which argues strongly against significant perturbations due to magnetic refraction, structural disturbance, or depositional shallowing. In terms of geomagnetic secular variation, we interpret the western European archaeomagnetic data summarized here in terms of an open loop caused by westward drift, followed by an inclination low spanning the first few centuries CE representing the signal of a static flux pulse that reaches a maximum magnetic moment of a few percent of the earth's main central dipole.

  7. Main field and secular variation modeling with Defense Meteorological Satellite Program magnetic measurements

    NASA Astrophysics Data System (ADS)

    Alken, P.; Olsen, N.; Finlay, C. C.; Chulliat, A.

    2017-12-01

    In order to investigate the spatial structure and development of rapid (sub-decadal) changes in the geomagnetic core field, including its secular variation and acceleration, global magnetic measurements from space play a crucial role. With the end of the CHAMP mission in September 2010, there has been a gap in high-quality satellite magnetic field measurements until the Swarm mission was launched in November 2013. Geomagnetic main field models during this period have relied on the global ground observatory network which, due to its sparse spatial configuration, has difficulty in resolving secular variation and acceleration at higher spherical harmonic degrees. In this presentation we will show new results in building main field models during this "gap period", based on vector magnetic measurements from four Defense Meteorological Satellite Program (DMSP) satellites. While the fluxgate instruments onboard DMSP were not designed for high-quality core field modeling, we find that the DMSP dataset can provide valuable information on secular variation and acceleration during the gap period.

  8. Evaluation of a new paleosecular variation activity index as a diagnostic tool for geomagnetic field variations

    NASA Astrophysics Data System (ADS)

    Panovska, Sanja; Constable, Catherine

    2015-04-01

    Geomagnetic indices like Dst, K and A, have been used since the early twentieth century to characterize activity in the external part of the modern geomagnetic field and as a diagnostic for space weather. These indices reflect regional and global activity and serve as a proxy for associated physical processes. However, no such tools are yet available for the internal geomagnetic field driven by the geodynamo in Earth's liquid outer core. To some extent this reflects limited spatial and temporal sampling for longer timescales associated with paleomagnetic secular variation, but recent efforts in both paleomagnetic data gathering and modeling activity suggest that longer term characterization of the internal geomagnetic weather/climate and its variability would be useful. Specifically, we propose an index for activity in paleosecular variation, useful as both a local and global measure of field stability during so-called normal secular variation and as a means of identifying more extreme behavior associated with geomagnetic excursions and reversals. To date, geomagnetic excursions have been identified by virtual geomagnetic poles (VGPs) deviating more than some conventional limit from the geographic pole (often 45 degrees), and/or by periods of significant intensity drops below some critical value, for example 50% of the present-day field. We seek to establish a quantitative definition of excursions in paleomagnetic records by searching for synchronous directional deviations and lows in relative paleointensity. We combine paleointensity variations with deviations from the expected geocentric axial dipole (GAD) inclination in a single parameter, which we call the paleosecular variation (PSV) activity index. This new diagnostic can be used on any geomagnetic time series (individual data records, model predictions, spherical harmonic coefficients, etc.) to characterize the level of paleosecular variation activity, find excursions, or even study incipient reversals

  9. Paleomagnetic directions and thermoluminescence dating from a bread oven-floor sequence in Lübeck (Germany): A record of 450 years of geomagnetic secular variation

    NASA Astrophysics Data System (ADS)

    Schnepp, Elisabeth; Pucher, Rudolf; Goedicke, Christian; Manzano, Ana; Müller, Uwe; Lanos, Philippe

    2003-02-01

    A record of about 450 years of geomagnetic secular variation is presented from a single archaeological site in Lübeck (Germany) where a sequence of 25 bread oven floors has been preserved in a bakery from medieval times until today. The age dating of the oven-floor sequence is based on historical documents, 14C-dating and thermoluminescence dating. It confines the time interval from about 1300 to 1800 A.D. Paleomagnetic directions have been determined from each oven floor by means of 198 oriented hand samples. After alternating field as well as thermal demagnetization experiments, the characteristic remanent magnetization direction was obtained using principal component analysis. The mean directions of 24 oven floors are characterized by high Fisherian precision parameters (>146) and small α95 confidence limits (1.2°-4.6°). For obtaining a smooth curve of geomagnetic secular variation for Lübeck, a spherical spline function was fitted to the data using a Bayesian approach, which considers not only the obtained ages, but also stratigraphic order. Correlation with historical magnetic records suggests that the age estimation for the upper 10 layers was too young and must date from the end of the sixteenth to the mid of the eighteenth century. For the lowermost 14 layers, dating is reliable and provides a secular variation curve for Germany. The inclination shows a minimum in the fourteenth century and then increases by more than 10°. Declination shows a local minimum around 1400 A.D. followed by a maximum in the seventeenth century. This is followed by the movement of declination about 30° to western directions.

  10. Magnetic Navigation in Sea Turtles: Insights from Secular Variation

    NASA Astrophysics Data System (ADS)

    Putman, N. F.; Lohmann, K.

    2011-12-01

    Sea turtles are iconic migrants that posses a sensitive magnetic-sense that guides their long-distance movements in a variety of contexts. In the first few hours after hatching turtles use the magnetic field to maintain an offshore compass heading to reach deeper water, out of the reach of nearshore predators. Young turtles engage in directed swimming in response to regional magnetic fields that exist along their transoceanic migratory path. Older turtles also use magnetic information to relocate foraging sites and islands used for nesting after displacement. Numerous hypotheses have been put forth to explain how magnetic information functions in these movements, however, there is little consensus among animal navigation researchers. A particular vexing issue is how magnetic navigation can function under the constraints of the constant, gradual shifting of the earth's magnetic field (secular variation). Here, I present a framework based on models of recent geomagnetic secular variation to explore several navigational mechanisms proposed for sea turtles. I show that while examination of secular variation likely falsifies some hypothetical navigational strategies, it provides key insights into the selective pressures that could maintain other navigational mechanisms. Moreover, examination of secular variation's influence on the navigational precision in reproductive migrations of sea turtles offers compelling explanations for the population structure along sea turtle nesting beaches as well as spatiotemporal variation in nesting turtle abundance.

  11. Secular trends in storm-level geomagnetic activity

    USGS Publications Warehouse

    Love, J.J.

    2011-01-01

    Analysis is made of K-index data from groups of ground-based geomagnetic observatories in Germany, Britain, and Australia, 1868.0-2009.0, solar cycles 11-23. Methods include nonparametric measures of trends and statistical significance used by the hydrological and climatological research communities. Among the three observatory groups, German K data systematically record the highest disturbance levels, followed by the British and, then, the Australian data. Signals consistently seen in K data from all three observatory groups can be reasonably interpreted as physically meaninginful: (1) geomagnetic activity has generally increased over the past 141 years. However, the detailed secular evolution of geomagnetic activity is not well characterized by either a linear trend nor, even, a monotonic trend. Therefore, simple, phenomenological extrapolations of past trends in solar and geomagnetic activity levels are unlikely to be useful for making quantitative predictions of future trends lasting longer than a solar cycle or so. (2) The well-known tendency for magnetic storms to occur during the declining phase of a sunspot-solar cycles is clearly seen for cycles 14-23; it is not, however, clearly seen for cycles 11-13. Therefore, in addition to an increase in geomagnetic activity, the nature of solar-terrestrial interaction has also apparently changed over the past 141 years. ?? Author(s) 2011.

  12. Main field and recent secular variation.

    USGS Publications Warehouse

    Alldredge, L.R.

    1983-01-01

    As Cain (1979) indicated might happen in the last IUGG quadrennial report, added resources were made available during the past few years and a real impulse was added to the geomagnetic work in the US by the launching of the MAGSAT Satellite. This new effort paid off in terms of new charts, additional long wavelength studies, and external source studies. As before, however, the future funding for new starts in geomagnetism does not look bright at the present time. A single MAGSAT in orbit a little more than seven months did wonders for main field (M.F.) charting, but did little or nothing for secular variation (S.V.) charting. It would take a number of repeated MAGSATS to help the S.V. picture. Meanwhile, the world magnetic observatory net and surface repeat stations remain as the main source of S.V. data. -from Author

  13. Are secular correlations between sunspots, geomagnetic activity, and global temperature significant?

    USGS Publications Warehouse

    Love, J.J.; Mursula, K.; Tsai, V.C.; Perkins, D.M.

    2011-01-01

    Recent studies have led to speculation that solar-terrestrial interaction, measured by sunspot number and geomagnetic activity, has played an important role in global temperature change over the past century or so. We treat this possibility as an hypothesis for testing. We examine the statistical significance of cross-correlations between sunspot number, geomagnetic activity, and global surface temperature for the years 1868-2008, solar cycles 11-23. The data contain substantial autocorrelation and nonstationarity, properties that are incompatible with standard measures of cross-correlational significance, but which can be largely removed by averaging over solar cycles and first-difference detrending. Treated data show an expected statistically- significant correlation between sunspot number and geomagnetic activity, Pearson p < 10-4, but correlations between global temperature and sunspot number (geomagnetic activity) are not significant, p = 0.9954, (p = 0.8171). In other words, straightforward analysis does not support widely-cited suggestions that these data record a prominent role for solar-terrestrial interaction in global climate change. With respect to the sunspot-number, geomagnetic-activity, and global-temperature data, three alternative hypotheses remain difficult to reject: (1) the role of solar-terrestrial interaction in recent climate change is contained wholly in long-term trends and not in any shorter-term secular variation, or, (2) an anthropogenic signal is hiding correlation between solar-terrestrial variables and global temperature, or, (3) the null hypothesis, recent climate change has not been influenced by solar-terrestrial interaction. ?? 2011 by the American Geophysical Union.

  14. Are secular correlations between sunspots, geomagnetic activity, and global temperature significant?

    NASA Astrophysics Data System (ADS)

    Love, Jeffrey J.; Mursula, Kalevi; Tsai, Victor C.; Perkins, David M.

    2011-11-01

    Recent studies have led to speculation that solar-terrestrial interaction, measured by sunspot number and geomagnetic activity, has played an important role in global temperature change over the past century or so. We treat this possibility as an hypothesis for testing. We examine the statistical significance of cross-correlations between sunspot number, geomagnetic activity, and global surface temperature for the years 1868-2008, solar cycles 11-23. The data contain substantial autocorrelation and nonstationarity, properties that are incompatible with standard measures of cross-correlational significance, but which can be largely removed by averaging over solar cycles and first-difference detrending. Treated data show an expected statistically-significant correlation between sunspot number and geomagnetic activity, Pearson p < 10-4, but correlations between global temperature and sunspot number (geomagnetic activity) are not significant, p = 0.9954, (p = 0.8171). In other words, straightforward analysis does not support widely-cited suggestions that these data record a prominent role for solar-terrestrial interaction in global climate change. With respect to the sunspot-number, geomagnetic-activity, and global-temperature data, three alternative hypotheses remain difficult to reject: (1) the role of solar-terrestrial interaction in recent climate change is contained wholly in long-term trends and not in any shorter-term secular variation, or, (2) an anthropogenic signal is hiding correlation between solar-terrestrial variables and global temperature, or, (3) the null hypothesis, recent climate change has not been influenced by solar-terrestrial interaction.

  15. A Statistical Model of the Fluctuations in the Geomagnetic Field from Paleosecular Variation to Reversal

    PubMed

    Camps; Prevot

    1996-08-09

    The statistical characteristics of the local magnetic field of Earth during paleosecular variation, excursions, and reversals are described on the basis of a database that gathers the cleaned mean direction and average remanent intensity of 2741 lava flows that have erupted over the last 20 million years. A model consisting of a normally distributed axial dipole component plus an independent isotropic set of vectors with a Maxwellian distribution that simulates secular variation fits the range of geomagnetic fluctuations, in terms of both direction and intensity. This result suggests that the magnitude of secular variation vectors is independent of the magnitude of Earth's axial dipole moment and that the amplitude of secular variation is unchanged during reversals.

  16. An activity index for geomagnetic paleosecular variation, excursions, and reversals

    NASA Astrophysics Data System (ADS)

    Panovska, S.; Constable, C. G.

    2017-04-01

    Magnetic indices provide quantitative measures of space weather phenomena that are widely used by researchers in geomagnetism. We introduce an index focused on the internally generated field that can be used to evaluate long term variations or climatology of modern and paleomagnetic secular variation, including geomagnetic excursions, polarity reversals, and changes in reversal rate. The paleosecular variation index, Pi, represents instantaneous or average deviation from a geocentric axial dipole field using normalized ratios of virtual geomagnetic pole colatitude and virtual dipole moment. The activity level of the index, σPi, provides a measure of field stability through the temporal standard deviation of Pi. Pi can be calculated on a global grid from geomagnetic field models to reveal large scale geographic variations in field structure. It can be determined for individual time series, or averaged at local, regional, and global scales to detect long term changes in geomagnetic activity, identify excursions, and transitional field behavior. For recent field models, Pi ranges from less than 0.05 to 0.30. Conventional definitions for geomagnetic excursions are characterized by Pi exceeding 0.5. Strong field intensities are associated with low Pi unless they are accompanied by large deviations from axial dipole field directions. σPi provides a measure of geomagnetic stability that is modulated by the level of PSV or frequency of excursional activity and reversal rate. We demonstrate uses of Pi for paleomagnetic observations and field models and show how it could be used to assess whether numerical simulations of the geodynamo exhibit Earth-like properties.

  17. Steady induction effects in geomagnetism. Part 1A: Steady motional induction of geomagnetic chaos

    NASA Technical Reports Server (NTRS)

    Voorhies, Coerte V.

    1992-01-01

    Geomagnetic effects of magnetic induction by hypothetically steady fluid motion and steady magnetic flux diffusion near the top of Earth's core are investigated using electromagnetic theory, simple magnetic earth models, and numerical experiments with geomagnetic field models. The problem of estimating a steady fluid velocity field near the top of Earth's core which induces the secular variation indicated by broad-scale models of the observed geomagnetic field is examined and solved. In Part 1, the steady surficial core flow estimation problem is solved in the context of the source-free mantle/frozen-flux core model. In the first paper (IA), the theory underlying such estimates is reviewed and some consequences of various kinematic and dynamic flow hypotheses are derived. For a frozen-flux core, fluid downwelling is required to change the mean square normal magnetic flux density averaged over the core-mantle boundary. For surficially geostrophic flow, downwelling implies poleward flow. The solution of the forward steady motional induction problem at the surface of a frozen-flux core is derived and found to be a fine, easily visualized example of deterministic chaos. Geomagnetic effects of statistically steady core surface flow may well dominate secular variation over several decades. Indeed, effects of persistent, if not steady, surficially geostrophic core flow are described which may help explain certain features of the present broad-scale geomagnetic field and perhaps paleomagnetic secular variation.

  18. The use of MAGSAT data to determine secular variation.

    USGS Publications Warehouse

    Cain, J.C.; Frayser, J.; Muth, L.; Schmitz, D.

    1983-01-01

    A combined spatial and secular variation model of the geomagnetic field, labeled M061581, is derived from a selection of MAGSAT data. Secular variation (SV) data computed from linear fits to midnight hourly values from 19 magnetic observatories were also included in the analysis but were seen to have little effect on the model. The SV patterns from this new model are compared with those from the 1980 IGRF and with those for 1970 computed by the DGRF and with the 1960 patterns computed using the GSFC(12/66) model. Most of the features of the M061581 are identical in location and level with those of the 1980 IGRF. Together they confirm that the reversals in sign of field change seen over Asia and North America between 1965 and 1975 are reverting to the pre-1965 states. The M061581 model gives -32 nT/yr for the dipole decay rate, larger than the 70% increase already reported since 1965. -Authors

  19. A candidate secular variation model for IGRF-12 based on Swarm data and inverse geodynamo modelling

    NASA Astrophysics Data System (ADS)

    Fournier, Alexandre; Aubert, Julien; Thébault, Erwan

    2015-05-01

    In the context of the 12th release of the international geomagnetic reference field (IGRF), we present the methodology we followed to design a candidate secular variation model for years 2015-2020. An initial geomagnetic field model centered around 2014.3 is first constructed, based on Swarm magnetic measurements, for both the main field and its instantaneous secular variation. This initial model is next fed to an inverse geodynamo modelling framework in order to specify, for epoch 2014.3, the initial condition for the integration of a three-dimensional numerical dynamo model. The initialization phase combines the information contained in the initial model with that coming from the numerical dynamo model, in the form of three-dimensional multivariate statistics built from a numerical dynamo run unconstrained by data. We study the performance of this novel approach over two recent 5-year long intervals, 2005-2010 and 2009-2014. For a forecast horizon of 5 years, shorter than the large-scale secular acceleration time scale (˜10 years), we find that it is safer to neglect the flow acceleration and to assume that the flow determined by the initialization is steady. This steady flow is used to advance the three-dimensional induction equation forward in time, with the benefit of estimating the effects of magnetic diffusion. The result of this deterministic integration between 2015.0 and 2020.0 yields our candidate average secular variation model for that time frame, which is thus centered on 2017.5.

  20. Evaluation of the 1985-1990 IGRF secular variation candidates

    USGS Publications Warehouse

    Cain, J.C.; Kluth, C.

    1987-01-01

    The IGRF secular variation model for 1985-1990 was adopted by the International Association of Geomagnetism and Aeronomy at its Prague meeting in August 1985 as an average of the three candidate models submitted to the committee. We compared the three models at epoch 1985.0 against each other and against a new model based on observatory data available as of July 1, 1985. These comparisons showed that one of the three candidate models disagreed more with the other two and our model, especially in the eastern Pacific. None of the candidate models was seen to respond to a change in the secular variation of the vertical component that appears to have taken place most strongly in the western Pacific area since 1982. The lack of satellite data was seen to be a significant handicap towards prediction of the field change over most of the Earth's surface, especially the southern oceans. Maximum errors of any model are estimated to be of the order of 80 nT a-1. ?? 1987.

  1. Recent geomagnetic secular variation from Swarm and ground observatories as estimated in the CHAOS-6 geomagnetic field model

    NASA Astrophysics Data System (ADS)

    Finlay, Christopher C.; Olsen, Nils; Kotsiaros, Stavros; Gillet, Nicolas; Tøffner-Clausen, Lars

    2016-07-01

    We use more than 2 years of magnetic data from the Swarm mission, and monthly means from 160 ground observatories as available in March 2016, to update the CHAOS time-dependent geomagnetic field model. The new model, CHAOS-6, provides information on time variations of the core-generated part of the Earth's magnetic field between 1999.0 and 2016.5. We present details of the secular variation (SV) and secular acceleration (SA) from CHAOS-6 at Earth's surface and downward continued to the core surface. At Earth's surface, we find evidence for positive acceleration of the field intensity in 2015 over a broad area around longitude 90°E that is also seen at ground observatories such as Novosibirsk. At the core surface, we are able to map the SV up to at least degree 16. The radial field SA at the core surface in 2015 is found to be largest at low latitudes under the India-South-East Asia region, under the region of northern South America, and at high northern latitudes under Alaska and Siberia. Surprisingly, there is also evidence for significant SA in the central Pacific region, for example near Hawaii where radial field SA is observed on either side of a jerk in 2014. On the other hand, little SV or SA has occurred over the past 17 years in the southern polar region. Inverting for a quasi-geostrophic core flow that accounts for this SV, we obtain a prominent planetary-scale, anti-cyclonic, gyre centred on the Atlantic hemisphere. We also find oscillations of non-axisymmetric, azimuthal, jets at low latitudes, for example close to 40°W, that may be responsible for localized SA oscillations. In addition to scalar data from Ørsted, CHAMP, SAC-C and Swarm, and vector data from Ørsted, CHAMP and Swarm, CHAOS-6 benefits from the inclusion of along-track differences of scalar and vector field data from both CHAMP and the three Swarm satellites, as well as east-west differences between the lower pair of Swarm satellites, Alpha and Charlie. Moreover, ground observatory SV

  2. The Egyptian geomagnetic reference field to the Epoch, 2010.0

    NASA Astrophysics Data System (ADS)

    Deebes, H. A.; Abd Elaal, E. M.; Arafa, T.; Lethy, A.; El Emam, A.; Ghamry, E.; Odah, H.

    2017-06-01

    The present work is a compilation of two tasks within the frame of the project ;Geomagnetic Survey & Detailed Geomagnetic Measurements within the Egyptian Territory; funded by the ;Science and Technology Development Fund agency (STDF);. The National Research Institute of Astronomy and Geophysics (NRIAG), has conducted a new extensive land geomagnetic survey that covers the whole Egyptian territory. The field measurements have been done at 3212 points along all the asphalted roads, defined tracks, and ill-defined tracks in Egypt; with total length of 11,586 km. In the present work, the measurements cover for the first time new areas as: the southern eastern borders of Egypt including Halayeb and Shlatin, the Quattara depresion in the western desert, and the new roads between Farafra and Baharia oasis. Also marine geomagnetic survey have been applied for the first time in Naser lake. Misallat and Abu-Simble geomagnetic observatories have been used to reduce the field data to the Epoch 2010. During the field measurements, whenever possible, the old stations occupied by the previous observers have been re-occupied to determine the secular variations at these points. The geomagnetic anomaly maps, the normal geomagnetic field maps with their corresponding secular variation maps, the normal geomagnetic field equations of the geomagnetic elements (EGRF) and their corresponding secular variations equations, are outlined. The anomalous sites, as discovered from the anomaly maps are, only, mentioned. In addition, a correlation between the International Geomagnetic Reference Field (IGRF) 2010.0 and the Egyptian Geomagnetic Reference Field (EGRF) 2010 is indicated.

  3. Development of a Process Based Paleomagnetic Secular Variation Dating Curve for the Northern Hemisphere Through the Radiocarbon Interval

    NASA Astrophysics Data System (ADS)

    Stoner, J. S.; Reilly, B. T.; Walczak, M. H.; Mix, A. C.; Lavoie, N.; Velle, J. H.; St-Onge, G.; Xuan, C.

    2017-12-01

    Paleomagnetic secular variation is a well-known centennial to millennial stratigraphic dating tool, but is generally considered to be regionally limited. Recent observations from the Holocene suggest that such spatial limitations may result from our incomplete understanding of field dynamics, rather than actual geomagnetic limitations. Comparisons of independently well-dated, high-resolution paleomagnetic secular variation records from the mid-latitudes of the Northern Hemisphere—including Asia, Northwest Pacific, Northeast Pacific, North America, North Atlantic, and Europe—reveal the existence of a primary (there may be others) coherent millennial scale oscillation of the geomagnetic field. This oscillation is observed using different geomagnetic parameters (e.g., inclination, declination, intensity) and signs depending on the site's location relative to the region of primary geomagnetic flux. This distinct spatial and temporal pattern is consistent with oscillations of geomagnetic flux recurring at just a few locations. The recurring persistence of this pattern, through the Holocene and possibly much longer, implicates lower mantle heterogeneity as a likely driver of field morphology. As with any paleo reconstructions, data coverage is far from perfect and as a result the geomagnetic details are just coming into focus. Yet, the stratigraphic potential is readily apparent and, if iteratively used, could significantly enhance our geomagnetic understanding as well as facilitate chronological control in a variety of settings. Here we explore the nature, uncertainties, and implications; including our initial attempt to extend the oscillation beyond the Holocene and through the radiocarbon interval starting from a Northeast Pacific perspective. Our intent is to develop a type curve with constrained uncertainties that can be used for stratigraphic correlation around the Northern Hemisphere as we move toward a process based dynamic magnetostratigraphic understanding.

  4. A global analysis of the 1991 geomagnetic jerk

    NASA Astrophysics Data System (ADS)

    De Michelis, Paola; Cafarella, Lili; Meloni, Antonio

    2000-12-01

    A recent examination of the geomagnetic annual mean values for the European magnetic observatories has shown the existence of a sudden change in the secular acceleration in about 1991 (Cafarella & Meloni 1995; Macmillan 1996). Using first differences of the Y (east geomagnetic field component) mean values from 74 observatories, the worldwide character of the 1991 impulse has been determined (De Michelis et al. 1998). Using data from 109 observatories widely distributed all over the world, the structure of the secular variation for the X (north) and Z (vertical) magnetic field intensities around 1990 was investigated, and evidence of this most recent jerk was found. External effects were removed from the annual mean data by comparing the long-term variations of the geomagnetic field components at individual observatories with the long-term variations of two geomagnetic indices, aa and Dst, and of a solar index, the Wolf number R. A careful analysis has been carried out on the amplitude of the external disturbance, on its dependence on latitude, and on the weights of the geomagnetic indices in the evaluation of the resulting external field. The secular variation has been evaluated from the corrected annual means. Around 1990, the secular variation can be fitted at many observatories by two straight lines with a sudden and marked change in slope. In this manner the jerk occurrence time and the intensity of the step in the second time derivative (ΔX'', ΔY'' and ΔZ'') were computed. Maps of ΔX'', ΔY'' and ΔZ'' provide information on the worldwide intensity distribution of the examined event. Maps of the jerk occurrence-time distributions are also given. The mean jerk occurrence time is 1990.1+/-0.6. Finally, a spherical harmonic analysis was used to complete the quantitative description of this phenomenon in order to study the trend of the energy density spectrum as a function of the harmonic degree n.

  5. Evaluating secular acceleration in geomagnetic field model GRIMM-3

    NASA Astrophysics Data System (ADS)

    Lesur, V.; Wardinski, I.

    2012-12-01

    Secular acceleration of the magnetic field is the rate of change of its secular variation. One of the main results of studying magnetic data collected by the German survey satellite CHAMP was the mapping of field acceleration and its evolution in time. Questions remain about the accuracy of the modeled acceleration and the effect of the applied regularization processes. We have evaluated to what extent the regularization affects the temporal variability of the Gauss coefficients. We also obtained results of temporal variability of the Gauss coefficients where alternative approaches to the usual smoothing norms have been applied for regularization. Except for the dipole term, the secular acceleration of the Gauss coefficients is fairly well described up to spherical harmonic degree 5 or 6. There is no clear evidence from observatory data that the spectrum of this acceleration is underestimated at the Earth surface. Assuming a resistive mantle, the observed acceleration supports a characteristic time scale for the secular variation of the order of 11 years.

  6. On the geomagnetic jerk of 1969

    NASA Technical Reports Server (NTRS)

    Mcleod, M. G.

    1985-01-01

    Courtillot et al. (1978) have first reported a sudden change in the slope of the first time derivatives of the geomagnetic field components which occurred around 1970. It was found that the change took place in a large part of the northern hemisphere. Malin and Hodder (1982) reported on studies which were conducted to determine whether this 1970 step change in the second time derivative of the geomagnetic field components, which they termed a geomagnetic 'jerk', was of internal or external origin. It was concluded that internal sources can give rise to changes in secular variation on time scales as short as one or two years and that these were the major factor in the geomagnetic jerk which occurred around 1970. The present paper provides new supporting evidence for the existence of a worldwide geomagnetic jerk, its (average) time of occurrence, and its internal nature. New estimates are given of the spherical harmonic coefficients of the jerk and of the pre-1969 and post-1969 secular acceleration.

  7. Variations in the geomagnetic dipole moment during the Holocene and the past 50 kyr

    NASA Astrophysics Data System (ADS)

    Knudsen, Mads Faurschou; Riisager, Peter; Donadini, Fabio; Snowball, Ian; Muscheler, Raimund; Korhonen, Kimmo; Pesonen, Lauri J.

    2008-07-01

    All absolute paleointensity data published in peer-reviewed journals were recently compiled in the GEOMAGIA50 database. Based on the information in GEOMAGIA50, we reconstruct variations in the geomagnetic dipole moment over the past 50 kyr, with a focus on the Holocene period. A running-window approach is used to determine the axial dipole moment that provides the optimal least-squares fit to the paleointensity data, whereas associated error estimates are constrained using a bootstrap procedure. We subsequently compare the reconstruction from this study with previous reconstructions of the geomagnetic dipole moment, including those based on cosmogenic radionuclides ( 10Be and 14C). This comparison generally lends support to the axial dipole moments obtained in this study. Our reconstruction shows that the evolution of the dipole moment was highly dynamic, and the recently observed rates of change (5% per century) do not appear unique. We observe no apparent link between the occurrence of archeomagnetic jerks and changes in the geomagnetic dipole moment, suggesting that archeomagnetic jerks most likely represent drastic changes in the orientation of the geomagnetic dipole axis or periods characterized by large secular variation of the non-dipole field. This study also shows that the Holocene geomagnetic dipole moment was high compared to that of the preceding ˜ 40 kyr, and that ˜ 4 · 10 22 Am 2 appears to represent a critical threshold below which geomagnetic excursions and reversals occur.

  8. Main field and secular variation candidate models for the 12th IGRF generation after 10 months of Swarm measurements

    NASA Astrophysics Data System (ADS)

    Saturnino, Diana; Langlais, Benoit; Civet, François; Thébault, Erwan; Mandea, Mioara

    2015-06-01

    We describe the main field and secular variation candidate models for the 12th generation of the International Geomagnetic Reference Field model. These two models are derived from the same parent model, in which the main field is extrapolated to epoch 2015.0 using its associated secular variation. The parent model is exclusively based on measurements acquired by the European Space Agency Swarm mission between its launch on 11/22/2013 and 09/18/2014. It is computed up to spherical harmonic degree and order 25 for the main field, 13 for the secular variation, and 2 for the external field. A selection on local time rather than on true illumination of the spacecraft was chosen in order to keep more measurements. Data selection based on geomagnetic indices was used to minimize the external field contributions. Measurements were screened and outliers were carefully removed. The model uses magnetic field intensity measurements at all latitudes and magnetic field vector measurements equatorward of 50° absolute quasi-dipole magnetic latitude. A second model using only the vertical component of the measured magnetic field and the total intensity was computed. This companion model offers a slightly better fit to the measurements. These two models are compared and discussed.We discuss in particular the quality of the model which does not use the full vector measurements and underline that this approach may be used when only partial directional information is known. The candidate models and their associated companion models are retrospectively compared to the adopted IGRF which allows us to criticize our own choices.

  9. Geomagnetic fluctuations during a polarity transition

    NASA Astrophysics Data System (ADS)

    Audunsson, Haraldur; Levi, Shaul

    1997-01-01

    The extensive Roza Member of the Columbia River Basalt Group (Washington State) has intermediate paleomagnetic directions, bracketed by underlying normal and overlying reverse polarity flows. A consistent paleomagnetic direction was measured at 11 widely distributed outcrops; the average direction has a declination of 189° and an inclination of -5°, with greater variation in the inclination [Rietman, 1966]. In this study the Roza Member was sampled in two Pasco Basin drillcores, where it is a single cooling unit and its thickness exceeds 50 m. Excellent core recovery allowed uniform and dense sampling of the drillcores. During its protracted cooling, the Roza flow in the drillcores recorded part of a 15.5 Ma geomagnetic polarity transition. The inclination has symmetric, quasicyclic intraflow variation, while the declination is nearly constant, consistent with the results from the outcrops. Thermal models of the cooling flow provide the timing for remanence acquisition. The inclination is inferred to have progressed from 0° to -15° and back to -3°over a period of 15 to 60 years, at rates of 1.6° to 0.5°/yr. Because the geomagnetic intensity was probably weak during the transition, these apparently high rates of change are not significantly different from present-day secular variation. These results agree with the hypothesis that normal secular variation persists through geomagnetic transitions. The Iow-amplitude quasicyclical fluctuations of the field over tens of years, recorded by Roza, suggest that the geomagnetic field reverses in discrete steps, and that more than 15-60 years were required to complete this reversal.

  10. Fast geomagnetic Field Intensity Variations between 1400 and 400 BCE: New Archaeointensity Data from Germany

    NASA Astrophysics Data System (ADS)

    Hervé, G.; Schnepp, E.; Metzler-Nebelsick, C.; Lhuillier, F.; Gilder, S.; Genevey, A.; Fassbinder, J.; Gallet, Y.

    2017-12-01

    Thirty-five mean archaeointensity data were obtained on ceramic sherds dated between 1400 and 400 BCE from sites located near Munich, Germany. The 453 sherds were collected from 52 graves, pits and wells dated by archaeological correlation, radiocarbon and/or dendrochronology. Rock magnetic analyses indicate that the remanent magnetization was mainly carried by magnetite. Data from Thellier-Thellier experiments were corrected for anisotropy and cooling rate effects. Triaxe and multispecimen (MSP-DSC) protocols were also measured on a subset of specimens. Around 60% of the samples provide reliable results when using stringent criteria selection. The 35 average archaeointensity values based on 154 pots are consistent with previous data and triple the Western Europe database between 1400 and 400 BCE. A secular variation curve for central-western Europe, built using a Bayesian approach, shows a double oscillation in geomagnetic field strength with intensity maxima of 70 μT around 1000-900 BCE and another up to 90 μT around 600-500 BCE. The maximum rate of variation was 0.25 μT/yr circa 700 BCE. The secular variation trend in Western Europe is similar to that observed in the Middle East and the Caucasus except that we find no evidence for hyper-rapid field variations (i.e. geomagnetic spikes). Virtual Axial Dipole Moments from Western Europe, the Middle East and central Asia differ by more than 20 ZA·m2 prior to 600 BCE, which signifies a departure from an axial dipole field especially between 1000 and 600 BCE. Our observations suggest that the regional Levantine Iron Age anomaly has been accompanied by an increase of the axial dipole moment together with a tilt of the dipole.

  11. Morphology of the southern African geomagnetic field derived from observatory and repeat station survey observations: 2005-2014

    NASA Astrophysics Data System (ADS)

    Kotzé, P. B.; Korte, M.

    2016-02-01

    Geomagnetic field data from four observatories and annual field surveys between 2005 and 2015 provide a detailed description of Earth's magnetic field changes over South Africa, Namibia and Botswana on time scales of less than 1 year. The southern African area is characterized by rapid changes in the secular variation pattern and lies in close proximity to the South Atlantic Anomaly (SAA) where the geomagnetic field intensity is almost 30 % weaker than in other regions at similar latitudes around the globe. Several geomagnetic secular acceleration (SA) pulses (geomagnetic jerks) around 2007, 2010 and 2012 could be identified over the last decade in southern Africa. We present a new regional field model for declination and horizontal and vertical intensity over southern Africa (Southern African REGional (SAREG)) which is based on field survey and observatory data and covering the time interval from 2005 to 2014, i.e. including the period between 2010 and 2013 when no low Earth-orbiting vector field satellite data are available. A comparative evaluation between SAREG and global field models like CHAOS-5, the CHAMP, Orsted and SAC-C model of the Earth's magnetic field and International Geomagnetic Reference Field (IGRF-12) reveals that a simple regional field model based on a relatively dense ground network is able to provide a realistic representation of the geomagnetic field in this area. We particularly note that a global field model like CHAOS-5 does not always indicate similar short-period patterns in the field components as revealed by observatory data, while representing the general secular variation reasonably well during the time interval without near-Earth satellite vector field data. This investigation further shows the inhomogeneous occurrence and distribution of secular variation impulses in the different geomagnetic field components and at different locations in southern African.

  12. Geomagnetic main field modeling using magnetohydrodynamic constraints

    NASA Technical Reports Server (NTRS)

    Estes, R. H.

    1985-01-01

    The influence of physical constraints are investigated which may be approximately satisfied by the Earth's liquid core on models of the geomagnetic main field and its secular variation. A previous report describes the methodology used to incorporate nonlinear equations of constraint into the main field model. The application of that methodology to the GSFC 12/83 field model to test the frozen-flux hypothesis and the usefulness of incorporating magnetohydrodynamic constraints for obtaining improved geomagnetic field models is described.

  13. Evaluation of using R-SCHA to simultaneously model main field and secular variation multilevel geomagnetic data for the North Atlantic

    NASA Astrophysics Data System (ADS)

    Talarn, Àngela; Pavón-Carrasco, F. Javier; Torta, J. Miquel; Catalán, Manuel

    2017-02-01

    One efficient approach to modelling the Earth's core magnetic field involves the inclusion of crossover marine data which cover areas lacking in observatory and repeat station data for epochs when precise three-component satellite magnetic field measurements were not common. In this study, we show how the Revised Spherical Cap Harmonic Analysis (R-SCHA) can appropriately provide a continuous-time field model for the North Atlantic region by using multilevel sets of geomagnetic data such as marine, repeat station, observatory, and satellite data. Taking advantage of the properties of the R-SCHA basis functions we can model the radial and horizontal variations of the main field and its secular variation with the most suitable spatial and temporal wavelengths. To assess the best compromise between the data fit and the model roughness, temporal and spatial regularization matrices were implemented in the modelling approach. Two additional strategies were also used to obtain a satisfactory regional model: the opportunity to fit the anomaly bias at each observatory location, and constraining the regional model to the CHAOS-6 model at the end of its period of validity, i.e. 1999-2000, allowing a smooth transition with the predictions of this recent model. In terms of the root mean square error, the degree of success was limited partly because of the high uncertainties associated with some of the datasets (especially the marine ones), but we have produced a model that performs comparably to the global models for the period 1960-2000, thus showing the benefits of using this regional technique.

  14. Geomagnetic field declination: from decadal to centennial scales

    NASA Astrophysics Data System (ADS)

    Dobrica, Venera; Demetrescu, Crisan; Mandea, Mioara

    2018-04-01

    Declination annual mean time series longer than 1 century provided by 24 geomagnetic observatories worldwide, together with 5 Western European reconstructed declination series over the last 4 centuries, have been analyzed in terms of the frequency constituents of the secular variation at inter-decadal and sub-centennial timescales of 20-35 and 70-90 years. Observatory and reconstructed time series have been processed by several types of filtering, namely Hodrick-Prescott, running averages, and Butterworth. The Hodrick-Prescott filtering allows us to separate a quasi-oscillation at a decadal timescale, which is assumed to be related to external variations and called the 11-year constituent, from a long-term trend. The latter has been decomposed into two other oscillations called inter-decadal and sub-centennial constituents by applying a Butterworth filtering with cutoffs at 30 and 73 years, respectively. The analysis shows that the generally accepted geomagnetic jerks occur around extrema in the time derivative of the trend and coincide with extrema in the time derivative of the 11-year constituent. The sub-centennial constituent is traced back to 1600 in the five 400-year-long time series and seems to be a major constituent of the secular variation, geomagnetic jerks included.

  15. Improving geomagnetic observatory data in the South Atlantic Anomaly

    NASA Astrophysics Data System (ADS)

    Matzka, Jürgen; Morschhauser, Achim; Brando Soares, Gabriel; Pinheiro, Katia

    2016-04-01

    The Swarm mission clearly proofs the benefit of coordinated geomagnetic measurements from a well-tailored constellation in order to recover as good as possible the contributions of the various geomagnetic field sources. A similar truth applies to geomagnetic observatories. Their scientific value can be maximised by properly arranging the position of individual observatories with respect to the geometry of the external current systems in the ionosphere and magnetosphere, with respect to regions of particular interest for secular variation, and with respect to regions of anomalous electric conductivity in the ground. Here, we report on our plans and recent efforts to upgrade geomagnetic observatories and to recover unpublished data from geomagnetic observatories at low latitudes in the South Atlantic Anomaly. In particular, we target the magnetic equator with the equatorial electrojet and low latitudes to characterise the Sq- and ring current. The observatory network that we present allows also to study the longitudinal structure of these external current systems. The South Atlantic Anomaly region is very interesting due to its secular variation. We will show newly recovered data and comparisons with existing data sets. On the technical side, we introduce low-power data loggers. In addition, we use mobile phone data transfer, which is rapidly evolving in the region and allows timely data access and quality control at remote sites that previously were not connected to the internet.

  16. Fast geomagnetic field intensity variations between 1400 and 400 BCE: New archaeointensity data from Germany

    NASA Astrophysics Data System (ADS)

    Hervé, Gwenaël; Faβbinder, Jörg; Gilder, Stuart A.; Metzner-Nebelsick, Carola; Gallet, Yves; Genevey, Agnès; Schnepp, Elisabeth; Geisweid, Leonhard; Pütz, Anja; Reuβ, Simone; Wittenborn, Fabian; Flontas, Antonia; Linke, Rainer; Riedel, Gerd; Walter, Florian; Westhausen, Imke

    2017-09-01

    Thirty-five mean archaeointensity data were obtained on ceramic sherds dated between 1400 and 400 BCE from sites located near Munich, Germany. The 453 sherds were collected from 52 graves, pits and wells dated by archaeological correlation, radiocarbon and/or dendrochronology. Rock magnetic analyses indicate that the remanent magnetization was mainly carried by magnetite. Data from Thellier-Thellier experiments were corrected for anisotropy and cooling rate effects. Triaxe and multispecimen (MSP-DSC) protocols were also measured on a subset of specimens. Around 60% of the samples provide reliable results when using stringent criteria selection. The 35 average archaeointensity values based on 154 pots are consistent with previous data and triple the Western Europe database between 1400 and 400 BCE. A secular variation curve for central-western Europe, built using a Bayesian approach, shows a double oscillation in geomagnetic field strength with intensity maxima of ∼70 μT around 1000-900 BCE and another up to ∼90 μT around 600-500 BCE. The maximum rate of variation was ∼0.25 μT/yr circa 700 BCE. The secular variation trend in Western Europe is similar to that observed in the Middle East and the Caucasus except that we find no evidence for hyper-rapid field variations (i.e. geomagnetic spikes). Virtual Axial Dipole Moments from Western Europe, the Middle East and central Asia differ by more than 2·1022 A·m2 prior to 600 BCE, which signifies a departure from an axial dipole field especially between 1000 and 600 BCE. Our observations suggest that the regional Levantine Iron Age anomaly has been accompanied by an increase of the axial dipole moment together with a tilt of the dipole.

  17. Geomagnetic Jerks in the Swarm Era

    NASA Astrophysics Data System (ADS)

    Brown, William; Beggan, Ciaran; Macmillan, Susan

    2016-08-01

    The timely provision of geomagnetic observations as part of the European Space Agency (ESA) Swarm mission means up-to-date analysis and modelling of the Earth's magnetic field can be conducted rapidly in a manner not possible before. Observations from each of the three Swarm constellation satellites are available within 4 days and a database of close-to-definitive ground observatory measurements is updated every 3 months. This makes it possible to study very recent variations of the core magnetic field. Here we investigate rapid, unpredictable internal field variations known as geomagnetic jerks. Given that jerks represent (currently) unpredictable changes in the core field and have been identified to have happened in 2014 since Swarm was launched, we ask what impact this might have on the future accuracy of the International Geomagnetic Reference Field (IGRF). We assess the performance of each of the IGRF-12 secular variation model candidates in light of recent jerks, given that four of the nine candidates are novel physics-based predictive models.

  18. Solar generated quasi-biennial geomagnetic variation

    NASA Technical Reports Server (NTRS)

    Sugiura, M.; Poros, D. J.

    1977-01-01

    The existence of highly correlated quasi-biennial variations in the geomagnetic field and in solar activity is demonstrated. The analysis uses a numerical filter technique applied to monthly averages of the geomagnetic horizontal component and of the Zurich relative sunspot number. Striking correlations are found between the quasi-biennial geomagnetic variations determined from several magnetic observatories located at widely different longitudes, indicating a worldwide nature of the obtained variation. The correlation coefficient between the filtered Dst index and the filtered relative sunspot number is found to be -0.79 at confidence level greater than 99% with a time-lag of 4 months, with solar activity preceding the Dst variation. The correlation between the unfiltered data of Dst and of the sunspot number is also high with a similar time-lag. Such a timelag has not been discussed in the literature, and a further study is required to establish the mode of sun-earth relationship that gives this time delay.

  19. Daily variation characteristics at polar geomagnetic observatories

    NASA Astrophysics Data System (ADS)

    Lepidi, S.; Cafarella, L.; Pietrolungo, M.; Di Mauro, D.

    2011-08-01

    This paper is based on the statistical analysis of the diurnal variation as observed at six polar geomagnetic observatories, three in the Northern and three in the Southern hemisphere. Data are for 2006, a year of low geomagnetic activity. We compared the Italian observatory Mario Zucchelli Station (TNB; corrected geomagnetic latitude: 80.0°S), the French-Italian observatory Dome C (DMC; 88.9°S), the French observatory Dumont D'Urville (DRV; 80.4°S) and the three Canadian observatories, Resolute Bay (RES; 83.0°N), Cambridge Bay (CBB; 77.0°N) and Alert (ALE, 87.2°N). The aim of this work was to highlight analogies and differences in daily variation as observed at the different observatories during low geomagnetic activity year, also considering Interplanetary Magnetic Field conditions and geomagnetic indices.

  20. VO-ESD: a virtual observatory approach to describe the geomagnetic field temporal variations with application to Swarm data

    NASA Astrophysics Data System (ADS)

    Saturnino, Diana; Langlais, Benoit; Amit, Hagay; Mandea, Mioara; Civet, François; Beucler, Éric

    2017-04-01

    A complete description of the main geomagnetic field temporal variation is crucial to understand dynamics in the core. This variation, termed secular variation (SV), is known with high accuracy at ground magnetic observatory locations. However the description of its spatial variability is hampered by the globally uneven distribution of the observatories. For the past two decades a global coverage of the field changes has been allowed by satellites. Their surveys of the geomagnetic field have been used to derive and improve global spherical harmonic (SH) models through some strict data selection schemes to minimise external field contributions. But discrepancies remain between ground measurements and field predictions by these models. Indeed, the global models do not reproduce small spatial scales of the field temporal variations. To overcome this problem we propose a modified Virtual Observatory (VO) approach by defining a globally homogeneous mesh of VOs at satellite altitude. With this approach we directly extract time series of the field and its temporal variation from satellite measurements as it is done at observatory locations. As satellite measurements are acquired at different altitudes a correction for the altitude is needed. Therefore, we apply an Equivalent Source Dipole (ESD) technique for each VO and each given time interval to reduce all measurements to a unique location, leading to time series similar to those available at ground magnetic observatories. Synthetic data is first used to validate the new VO-ESD approach. Then, we apply our scheme to measurements from the Swarm mission. For the first time, a 2.5 degrees resolution global mesh of VO times series is built. The VO-ESD derived time series are locally compared to ground observations as well as to satellite-based model predictions. The approach is able to describe detailed temporal variations of the field at local scales. The VO-ESD time series are also used to derive global SH models. Without

  1. First geomagnetic measurements in the Antarctic region

    NASA Astrophysics Data System (ADS)

    Raspopov, O. M.; Demina, I. M.; Meshcheryakov, V. V.

    2014-05-01

    Based on data from literature and archival sources, we have further processed and analyzed the results of geomagnetic measurements made during the 1772-1775 Second World Expedition by James Cook and the 1819-1821 overseas Antarctic Expedition by Russian mariners Bellingshausen and Lazarev. Comparison with the GUFM historical model showed that there are systematic differences in the spatial structure of both the declination and its secular variation. The results obtained can serve as a basis for the construction of regional models of the geomagnetic field for the Antarctic region.

  2. Results of geomagnetic observations in Central Africa by Portuguese explorers during 1877 1885

    NASA Astrophysics Data System (ADS)

    Vaquero, José M.; Trigo, Ricardo M.

    2006-08-01

    In this short contribution, geomagnetic measurements in Central Africa made by Capelo and Ivens - two Portuguese explorers - during the years 1877 and 1885 are provided. We show the scarce number of geomagnetic observation in Africa compiled until now. These Portuguese explorers performed a considerable amount of measurements of geomagnetic declination (44 measurements), inclination (50) and horizontal component (50) of the geomagnetic field. We compared the results attained by these keen observers with those derived from the global geomagnetic model by Jackson et al. [Jackson, A., Jonkers, A.,Walker, M., 2000. Four centuries of geomagnetic secular variation from historical records. Philos. Trans. R. Soc. Lond. 358, 957-990].

  3. A Secular Variation Model for Igrf-12 Based on Swarm Data and Inverse Geodynamo Modelling

    NASA Astrophysics Data System (ADS)

    Fournier, A.; Aubert, J.; Erwan, T.

    2014-12-01

    We are proposing a secular variation candidate model for the 12th generation of the international geomagnetic reference field, spanning the years 2015-2020. The novelty of our approach stands in the initialization of a 5-yr long integration of a numerical model of Earth's dynamo by means of inverse geodynamo modelling, as introduced by Aubert (GJI, 2014). This inverse technique combines the information coming from the observations (in the form of an instantaneous estimate of the Gauss coefficients for the magnetic field and its secular variation) with that coming from the multivariate statistics of a free run of a numerical model of the geodynamo. The Gauss coefficients and their error covariance properties are determined from Swarm data along the lines detailed by Thébault et al. (EPS, 2010). The numerical model of the geodynamo is the so-called Coupled Earth Dynamo model (Aubert et al., Nature, 2013), whose variability possesses a strong level of similarity with that of the geomagnetic field. We illustrate and assess the potential of this methodology by applying it to recent time intervals, with an initialization based on CHAMP data, and conclude by presenting our SV candidate, whose initialization is based on the 1st year of Swarm data This work is supported by the French "Agence Nationale de la Recherche" under the grant ANR-11-BS56-011 (http://avsgeomag.ipgp.fr) and by the CNES. References: Aubert, J., Geophys. J. Int. 197, 1321-1334, 2014, doi: 10.1093/gji/ggu064 Aubert, J., Finlay, C., Fournier, F. Nature 502, 219-223, 2013, doi: 10.1038/nature12574 Thébault E. , A. Chulliat, S. Maus, G. Hulot, B. Langais, A. Chambodut and M. Menvielle, Earth Planets Space, Vol. 62 (No. 10), pp. 753-763, 2010.

  4. High-resolution chronology of sediment below CCD based on Holocene paleomagnetic secular variations in the Tohoku-oki earthquake rupture zone

    NASA Astrophysics Data System (ADS)

    Kanamatsu, Toshiya; Usami, Kazuko; McHugh, Cecilia M. G.; Ikehara, Ken

    2017-08-01

    Using high-resolution paleomagnetic data, we examined the potential for obtaining precise ages from sediment core samples recovered from deep-sea basins close to rupture zones of the 2011 and earlier earthquakes off Tohoku, Japan. Obtaining detailed stratigraphic ages from deep-sea sediments below the calcium compensation depth (CCD) is difficult, but we found that the samples contain excellent paleomagnetic secular variation records to constrain age models. Variations in paleomagnetic directions obtained from the sediments reveal systematic changes in the cores. A stacked paleomagnetic profile closely matches the Lake Biwa data sets in southwest Japan for the past 7000 years, one can establish age models based on secular variations of the geomagnetic field on sediments recovered uniquely below the CCD. Comparison of paleomagnetic directions near a tephra and a paleomagnetic direction of contemporaneous pyroclastic flow deposits acquired by different magnetization processes shows precise depositional ages reflecting the magnetization delay of the marine sediment record.Plain Language SummaryGenerally obtaining detailed ages from deep-sea sediments is difficult, because available dating method is very limited. We found that the deep-see sediment off North Japan recorded past sequential <span class="hlt">geomagnetic</span> directions. If those records correlate well with the reference record in past 7000 years, then we could estimate age of sediment by pattern matching. Additionally a volcanic ash emitted in 915 A.D., which was intercalated in our samples, indicates a time lag in our age model. This observation makes our age model more precise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005PEPI..152...62V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005PEPI..152...62V"><span>A note on some measurements of <span class="hlt">geomagnetic</span> declination in 1776 and 1778</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vaquero, J. M.; Gallego, M. C.; de Sanjosé, J. J.</p> <p>2005-09-01</p> <p>In this short contribution, measurements of magnetic declination across the Atlantic Ocean during the years 1776 and 1778 made by Antonio de Ulloa, a Spanish scientist and sailor, are provided and briefly analysed through a comparison with a global <span class="hlt">geomagnetic</span> model by Jackson et al. [Jackson, A., Jonkers, A., Walker, M., 2000. Four centuries of <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> from historical records. Philos. Trans. R. Soc. Lond. 358, 957-990].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70011657','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70011657"><span>A proposed International <span class="hlt">Geomagnetic</span> Reference Field for 1965- 1985.</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Peddie, N.W.; Fabiano, E.B.</p> <p>1982-01-01</p> <p>A set of spherical harmonic models describing the Earth's main magnetic field from 1965 to 1985 has been developed and is proposed as the next revision of the International <span class="hlt">Geomagnetic</span> Reference Field (IGRF). A tenth degree and order spherical harmonic model of the main field was derived from Magsat data. A series of eighth degree and order spherical harmonic models of the <span class="hlt">secular</span> <span class="hlt">variation</span> of the main field was derived from magnetic observatory annual mean values. Models of the main field at 1965, 1970, 1975, and 1980 were obtained by extrapolating the main-field model using the <span class="hlt">secular</span> <span class="hlt">variation</span> models.-Authors spherical harmonic models Earth main magnetic field Magsat data</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007PEPI..160...97Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007PEPI..160...97Z"><span>Archaeomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> in the UK during the past 4000 years and its application to archaeomagnetic dating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zananiri, I.; Batt, C. M.; Lanos, Ph.; Tarling, D. H.; Linford, P.</p> <p>2007-02-01</p> <p>This paper examines the limitations and deficiencies of the current British archaeomagnetic calibration curve and applies several mathematical approaches in an attempt to produce an improved <span class="hlt">secular</span> <span class="hlt">variation</span> curve for the UK for use in archaeomagnetic dating. The dataset compiled is the most complete available in the UK, incorporating published results, PhD theses and unpublished laboratory reports. It comprises 620 archaeomagnetic (directional) data and 238 direct observations of the <span class="hlt">geomagnetic</span> field, and includes all relevant information available about the site, the archaeomagnetic direction and the archaeological age. A thorough examination of the data was performed to assess their quality and reliability. Various techniques were employed in order to use the data to construct a <span class="hlt">secular</span> <span class="hlt">variation</span> (SV) record: moving window with averaging and median, as well as Bayesian statistical modelling. The SV reference curve obtained for the past 4000 years is very similar to that from France, most differences occurring during the early medieval period (or Dark Ages). Two examples of dating of archaeological structures, medieval and pre-Roman, are presented based on the new SV curve for the UK and the implications for archaeomagnetic dating are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMGP53A3747D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMGP53A3747D"><span>High-Latitude <span class="hlt">Geomagnetic</span> <span class="hlt">Secular</span> <span class="hlt">Variation</span> and Paleointensity during 6-0.5 Ma: Paleomagnetic Results from Eastern Iceland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Døssing, A.; Muxworthy, A. R.; Mac Niocaill, C.; Riishuus, M. S.</p> <p>2014-12-01</p> <p>Statistical analyses of paleomagnetic data from sequential lava flows allow us to study the <span class="hlt">geomagnetic</span> field behaviour on kyr to Myr timescales. Previous paleomagnetic studies lack high-latitude, high-quality measurements and the resolution necessary to investigate the persistence of high-latitude <span class="hlt">geomagnetic</span> field anomalies observed in the recent and historical field records, and replicated in some numerical geodynamo simulations. As part of the Time-Averaged Field Initiative (TAFI) project, lava sequences exposed in Nordurdalur (by Fljótsdalur) and Jökuldalur in eastern Iceland provide an excellent opportunity to improve high-latitude data suitable for investigating the 6-0.5 Ma TAF and paleosecular <span class="hlt">variation</span>. These adjacent valleys, separated by 40 km, host a composite stratigraphic record of lava flows erupted from the Northern Rift Zone between 0.5 and ~6.5 Ma (one lava flow extruded every ~15-40 kyr). Hiatuses are present locally in the younger sections, at ~0.9 Ma and 2 Ma (spanning 200-400 kyr), that contain frequent hyaloclastites and sediments. In 2013, we collected a total of ~2200 cores (10-18 cores/site; mean = ~13 cores/site) from ~140 separate lava flows (165 in total) along eight stratigraphic profiles in Nordurdalur and Jökuldalur. In addition, hand samples were collected from ~70 sites to deliver new 40Ar/39Ar radiometric age determinations. We present the final results of AF- and thermal demagnetization of ~10 specimens/flow, comprising 165 (~140 distinct) paleomagnetic directions, along with updated composite litho-, chrono- and magnetostratigraphy of the exposed volcanic pile in Nordurdalur and Jökuldalur. We present the dispersion of the Arctic virtual <span class="hlt">geomagnetic</span> poles over the last 6.5 Ma. In addition, we present a number of new IZZI paleointensity results from Jökuldalur. The <span class="hlt">geomagnetic</span> results are compared and contrasted with other high-latitude data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.1738O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.1738O"><span>The quasi-biennial <span class="hlt">variation</span> in the <span class="hlt">geomagnetic</span> field: a global characteristics analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ou, Jiaming; Du, Aimin</p> <p>2016-04-01</p> <p>The periodicity of 1.5-3 years, namely the quasi-biennial oscillation (QBO), has been identified in the solar, geophysical, and atmospheric variability. Sugiura (1976) investigated the observatory annual means over 1900-1970 and confirmed the QBO in the <span class="hlt">geomagnetic</span> field. At present, studying the quasi-biennial oscillation becomes substantial for separating the internal/external parts in the <span class="hlt">geomagnetic</span> observations. For the internal field, two typical periodicities, namely the 6-year oscillation in the <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> acceleration (SA) and the <span class="hlt">geomagnetic</span> jerk (occurs in 1-2 years), have close period to the QBO. Recently, a global quasi-biennial fluctuation was identified in the <span class="hlt">geomagnetic</span> core field model (Silva et al., 2012). Silva et al. speculated this 2.5 years signal to either external source remaining in the core field model or consequence of the methods used to construct the model. As more high-quality data from global observatories are available, it is a good opportunity to characterize the <span class="hlt">geomagnetic</span> QBO in the global range. In this paper, we investigate the QBO in the observatory monthly <span class="hlt">geomagnetic</span> field X, Y, and Z components spanning 1985-2010. We employ the observatory hourly means database from the World Data Center for <span class="hlt">Geomagnetism</span> (WDC) for the investigation. Wavelet analysis is used to detect and identify the QBO, while Fast Fourier Transform (FFT) analysis to obtain the statistics of the QBO. We apply the spherical harmonic analysis on QBO's amplitude, in order to quantify and separate internal and external sources. Three salient periods respectively at 2.9, 2.2, and 1.7 years, are identified in the amplitude spectrum over 1988-2008. The oscillation with the period of ~2.2 years is most prominent in all field components and further studied. In the X component the QBO is attenuated towards the polar regions, while in the Z component the amplitude of QBO increases with increasing of the <span class="hlt">geomagnetic</span> latitude. At the high latitudes, the QBO</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4083967-cosmic-ray-equator-geomagnetism','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4083967-cosmic-ray-equator-geomagnetism"><span>THE COSMIC RAY EQUATOR AND THE <span class="hlt">GEOMAGNETISM</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>Sakurai, K.</p> <p>1960-01-01</p> <p>It was formerly thought that the disagreement of the position of <span class="hlt">geomagnetic</span> dipole equator with that of the cosmic ray equator was caused by 45 deg westward shifting of the latter. Referring to the theory of <span class="hlt">geomagnetic</span> effect on cosmic rays, it was determined whether such westward shifting could be existent or not. It was found that the deviation of the cosmic ray equator from the <span class="hlt">geomagnetic</span> dipole equator is negligible even if the magnetic cavity is present around the earth's outer atmosphere. Taking into account such results, the origin of the cosmic ray equator was investigated. It was foundmore » that this equater could be produced by the higher harmonic components combined with the dipole component of <span class="hlt">geomagnetism</span>. The relation of the origin of the cosmic ray equater to the eccentric dipoles, near the outer pant of the earth's core, contributing to the <span class="hlt">secular</span> <span class="hlt">variation</span> of <span class="hlt">geomagnetism</span> was considered. (auth)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70015817','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70015817"><span>What do we mean by accuracy in <span class="hlt">geomagnetic</span> measurements?</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Green, A.W.</p> <p>1990-01-01</p> <p>High accuracy is what distinguishes measurements made at the world's magnetic observatories from other types of <span class="hlt">geomagnetic</span> measurements. High accuracy in determining the absolute values of the components of the Earth's magnetic field is essential to studying <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> and processes at the core mantle boundary, as well as some magnetospheric processes. In some applications of <span class="hlt">geomagnetic</span> data, precision (or resolution) of measurements may also be important. In addition to accuracy and resolution in the amplitude domain, it is necessary to consider these same quantities in the frequency and space domains. New developments in <span class="hlt">geomagnetic</span> instruments and communications make real-time, high accuracy, global <span class="hlt">geomagnetic</span> observatory data sets a real possibility. There is a growing realization in the scientific community of the unique relevance of <span class="hlt">geomagnetic</span> observatory data to the principal contemporary problems in solid Earth and space physics. Together, these factors provide the promise of a 'renaissance' of the world's <span class="hlt">geomagnetic</span> observatory system. ?? 1990.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61.2040K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61.2040K"><span>Statistical analysis of <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> during solar eclipses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Jung-Hee; Chang, Heon-Young</p> <p>2018-04-01</p> <p>We investigate the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> recorded by INTERMAGNET <span class="hlt">geomagnetic</span> observatories, which are observed while the Moon's umbra or penumbra passed over them during a solar eclipse event. Though it is generally considered that the <span class="hlt">geomagnetic</span> field can be modulated during solar eclipses, the effect of the solar eclipse on the observed <span class="hlt">geomagnetic</span> field has proved subtle to be detected. Instead of exploring the <span class="hlt">geomagnetic</span> field as a case study, we analyze 207 <span class="hlt">geomagnetic</span> manifestations acquired by 100 <span class="hlt">geomagnetic</span> observatories during 39 solar eclipses occurring from 1991 to 2016. As a result of examining a pattern of the <span class="hlt">geomagnetic</span> field <span class="hlt">variation</span> on average, we confirm that the effect can be seen over an interval of 180 min centered at the time of maximum eclipse on a site of a <span class="hlt">geomagnetic</span> observatory. That is, demonstrate an increase in the Y component of the <span class="hlt">geomagnetic</span> field and decreases in the X component and the total strength of the <span class="hlt">geomagnetic</span> field. We also find that the effect can be overwhelmed, depending more sensitively on the level of daily <span class="hlt">geomagnetic</span> events than on the level of solar activity and/or the phase of solar cycle. We have demonstrated it by dividing the whole data set into subsets based on parameters of the <span class="hlt">geomagnetic</span> field, solar activity, and solar eclipses. It is suggested, therefore, that an evidence of the solar eclipse effect can be revealed even at the solar maximum, as long as the day of the solar eclipse is magnetically quiet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70024989','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70024989"><span>Holocene <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> recorded by volcanic deposits at Mount St. Helens, Washington</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Hagstrum, J.T.; Hoblitt, R.P.; Gardner, C.A.; Gray, T.E.</p> <p>2002-01-01</p> <p>A compilation of paleomagnetic data from volcanic deposits of Mount St. Helens is presented in this report. The database is used to determine signature paleomagnetic directions of products from its Holocene eruptive events, to assign sampled units to their proper eruptive period, and to begin the assembly of a much larger database of paleomagnetic directions from Holocene volcanic rocks in western North America. The paleomagnetic results from Mount St. Helens are mostly of high quality, and generally agree with the division of its volcanic deposits into eruptive episodes based on previous geologic mapping and radiocarbon dates. The Muddy River andesite's paleomagnetic direction, however, indicates that it is more likely part of the Pine Creek eruptive period rather than the Castle Creek period. In addition, the Two-Fingers andesite flow is more likely part of the Middle Kalama eruptive period and not part of the Goat Rocks period. The paleomagnetic data from Mount St. Helens and Mount Hood document <span class="hlt">variation</span> in the <span class="hlt">geomagnetic</span> field's pole position over the last ~2,500 years. A distinct feature of the new paleosecular <span class="hlt">variation</span> (PSV) record, similar to the Fish Lake record (Oregon), indicates a sudden change from rapid clockwise movement of the pole about the Earth's spin axis to relatively slow counterclockwise movement at ???800 to 900 years B.P.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRA..12110231M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRA..12110231M"><span>Equatorial E region electric fields at the dip equator: 2. Seasonal variabilities and effects over Brazil due to the <span class="hlt">secular</span> <span class="hlt">variation</span> of the magnetic equator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moro, J.; Denardini, C. M.; Resende, L. C. A.; Chen, S. S.; Schuch, N. J.</p> <p>2016-10-01</p> <p>In this work, the seasonal dependency of the E region electric field (EEF) at the dip equator is examined. The eastward zonal (Ey) and the daytime vertical (Ez) electric fields are responsible for the overall phenomenology of the equatorial and low-latitude ionosphere, including the equatorial electrojet (EEJ) and its plasma instability. The electric field components are studied based on long-term backscatter radars soundings (348 days for both systems) collected during <span class="hlt">geomagnetic</span> quiet days (Kp ≤ 3+), from 2001 to 2010, at the São Luís Space Observatory (SLZ), Brazil (2.33°S, 44.20°W), and at the Jicamarca Radio Observatory (JRO), Peru (11.95°S, 76.87°W). Among the results, we observe, for the first time, a seasonal difference between the EEF in these two sectors in South America based on coherent radar measurements. The EEF is more intense in summer at SLZ, in equinox at JRO, and has been highly variable with season in the Brazilian sector compared to the Peruvian sector. In addition, the <span class="hlt">secular</span> <span class="hlt">variation</span> on the <span class="hlt">geomagnetic</span> field and its effect on the EEJ over Brazil resulted that as much farther away is the magnetic equator from SLZ, later more the EEJ is observed (10 h LT) and sooner it ends (16 h LT). Moreover, the time interval of type II occurrence decreased significantly after the year 2004, which is a clear indication that SLZ is no longer an equatorial station due to the <span class="hlt">secular</span> <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1513690M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1513690M"><span>Dating of palaeomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> in Swedish varved lake sediments using radiocarbon wiggle-matching</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mellström, Anette; Nilsson, Andreas; Stanton, Tania; Muscheler, Raimund; Snowball, Ian</p> <p>2013-04-01</p> <p>Well-dated natural archives are crucial when investigating the timing between climate change and climate forcing. Annually laminated (varved) lake sediments, in particular, can provide valuable knowledge about past climatic and environmental conditions as the annual nature of the sediments enables the establishment of high-resolution archives. In addition, lake sediments can record <span class="hlt">variations</span> in the Earth's magnetic field, which has the potential to be used as a dating validation technique if the palaeo-<span class="hlt">secular</span> and -intensity curves are dated correctly. If individual and well-defined <span class="hlt">geomagnetic</span> events can be dated accurately, they can then be used as isochrones, thereby allowing the synchronisation of different records. We therefore aim to date the "f" event, a late Holocene <span class="hlt">secular</span> <span class="hlt">variation</span> change, which is recorded in many sites in the northern hemisphere. Varved sites in Sweden have dated the "f" event to ~2700 cal. yrs BP. In order to constrain this date further, we have used the radiocarbon wiggle-matching method on a lake in central west Sweden, Kälksjön (Stanton et al., 2010), whose chronology has previously been validated using a number of complimentary dating methods. With the radiocarbon wiggle-matching technique, closely spaced samples are measured and matched to distinct wiggles in the radiocarbon calibration curve. The advantage of using varve-dated sediments is that it is possible to know the exact number of years between each sample, and therefore improve the initial age model. We compare the wiggle-match results of Kälksjön with results from a newly discovered varved lake sediment sequence in southern Sweden, Gyltigesjön. This comparison can provide information about magnetisation processes in sediments, such as the length of the palaeomagnetic lock-in delay. Stanton, T., Snowball, I., Zillén, L., Wastegård, S., 2010. Validating a Swedish varve chronology using radiocarbon, palaeomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span>, lead pollution history and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880029595&hterms=Legendre+polynomials&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DLegendre%2Bpolynomials','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880029595&hterms=Legendre+polynomials&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DLegendre%2Bpolynomials"><span>Simultaneous stochastic inversion for <span class="hlt">geomagnetic</span> main field and <span class="hlt">secular</span> <span class="hlt">variation</span>. I - A large-scale inverse problem</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bloxham, Jeremy</p> <p>1987-01-01</p> <p>The method of stochastic inversion is extended to the simultaneous inversion of both main field and <span class="hlt">secular</span> <span class="hlt">variation</span>. In the present method, the time dependency is represented by an expansion in Legendre polynomials, resulting in a simple diagonal form for the a priori covariance matrix. The efficient preconditioned Broyden-Fletcher-Goldfarb-Shanno algorithm is used to solve the large system of equations resulting from expansion of the field spatially to spherical harmonic degree 14 and temporally to degree 8. Application of the method to observatory data spanning the 1900-1980 period results in a data fit of better than 30 nT, while providing temporally and spatially smoothly varying models of the magnetic field at the core-mantle boundary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AnGeo..36..275C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AnGeo..36..275C"><span>Latitudinal <span class="hlt">variation</span> rate of <span class="hlt">geomagnetic</span> cutoff rigidity in the active Chilean convergent margin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cordaro, Enrique G.; Venegas, Patricio; Laroze, David</p> <p>2018-03-01</p> <p>We present a different view of <span class="hlt">secular</span> <span class="hlt">variation</span> of the Earth's magnetic field, through the <span class="hlt">variations</span> in the threshold rigidity known as the <span class="hlt">variation</span> rate of <span class="hlt">geomagnetic</span> cutoff rigidity (VRc). As the <span class="hlt">geomagnetic</span> cutoff rigidity (Rc) lets us differentiate between charged particle trajectories arriving at the Earth and the Earth's magnetic field, we used the VRc to look for internal <span class="hlt">variations</span> in the latter, close to the 70° south meridian. Due to the fact that the empirical data of total magnetic field BF and vertical magnetic field Bz obtained at Putre (OP) and Los Cerrillos (OLC) stations are consistent with the displacement of the South Atlantic magnetic anomaly (SAMA), we detected that the VRc does not fully correlate to SAMA in central Chile. Besides, the lower section of VRc seems to correlate perfectly with important geological features, like the flat slab in the active Chilean convergent margin. Based on this, we next focused our attention on the empirical <span class="hlt">variations</span> of the vertical component of the magnetic field Bz, recorded in OP prior to the Maule earthquake in 2010, which occurred in the middle of the Chilean flat slab. We found a jump in Bz values and main frequencies from 3.510 to 5.860 µHz, in the second derivative of Bz, which corresponds to similar magnetic behavior found by other research groups, but at lower frequency ranges. Then, we extended this analysis to other relevant subduction seismic events, like Sumatra in 2004 and Tohoku in 2011, using data from the Guam station. Similar records and the main frequencies before each event were found. Thus, these results seem to show that magnetic anomalies recorded on different timescales, as VRc (decades) and Bz (days), may correlate with some geological events, as the lithosphere-atmosphere-ionosphere coupling (LAIC).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA21B2521K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA21B2521K"><span>Analysis of <span class="hlt">Geomagnetic</span> Field <span class="hlt">Variations</span> during Total Solar Eclipses Using INTERMAGNET Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>KIM, J. H.; Chang, H. Y.</p> <p>2017-12-01</p> <p>We investigate <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field observed by INTERMAGNET <span class="hlt">geomagnetic</span> observatories over which the totality path passed during a solar eclipse. We compare results acquired by 6 <span class="hlt">geomagnetic</span> observatories during the 4 total solar eclipses (11 August 1999, 1 August 2008, 11 July 2010, and 20 March 2015) in terms of <span class="hlt">geomagnetic</span> and solar ecliptic parameters. These total solar eclipses are the only total solar eclipse during which the umbra of the moon swept an INTERMAGNET <span class="hlt">geomagnetic</span> observatory and simultaneously <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field are recorded. We have confirmed previous studies that increase BY and decreases of BX, BZ and F are conspicuous. Interestingly, we have noted that <span class="hlt">variations</span> of <span class="hlt">geomagnetic</span> field components observed during the total solar eclipse at Isla de Pascua Mataveri (Easter Island) in Chile (IPM) in the southern hemisphere show distinct decrease of BY and increases of BX and BZ on the contrary. We have found, however, that <span class="hlt">variations</span> of BX, BY, BZ and F observed at Hornsund in Norway (HRN) seem to be dominated by other <span class="hlt">geomagnetic</span> occurrence. In addition, we have attempted to obtain any signatures of influence on the temporal behavior of the <span class="hlt">variation</span> in the <span class="hlt">geomagnetic</span> field signal during the solar eclipse by employing the wavelet analysis technique. Finally, we conclude by pointing out that despite apparent success a more sophisticate and reliable algorithm is required before implementing to make quantitative comparisons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMGP23A1028Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMGP23A1028Z"><span>Holocene paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> records from the East China Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, Y.; Zheng, H.; Kissel, C.; Laj, C. E.; Deng, C.</p> <p>2011-12-01</p> <p>Paleomagnetic study on marine sediments can provide continuous, high-resolution records of short-term fluctuations of the Earth's magnetic field, which can be used for inter-core correlations at regional scale. However, Holocene paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> (PSV) records from marine sediment are still rare. Detailed paleomagnetic and rock magnetic studies were conducted on u-channel samples from rapidly deposited sediment core MD06-3040 (27.72°N, 121.78°E; 46 m water depth), on the East China Sea (ECS) inner continental shelf Holocene marine sequence, during IMAGES XIV Marco Polo 2 cruise on the R. V. Marion Dufresne (IPEV). The 19.22 m long core spans the entire Holocene, with theoretical high-resolution of about 20-year for paleomagnetic studies, and paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> (PSV) for the last 7500 years was retrieved from the uppermost 15.8 m fine-grained sediments. The dominant carrier of the remanent magnetization is magnetite, with some contributions from iron sulfide, such as greigite below 3.5 m, due to post-depositional diagenesis. The Characteristic Remanent magnetization (ChRM) is well defined by a single magnetization component and Maximum Angular Deviations (MAD) lower than 5°. Therefore, the information of paleomagnetic directions is still preserved after diagenetic alteration. Inclination of core MD06-3040 presents seven relatively high peaks, and declination presents four obvious eastern ward drifts during the last 7500 years. These <span class="hlt">variations</span> can be well compared to that obtained from lakes in Japan, and some features are also comparable to the records from Europe with temporal offset. The power spectrum analysis shows that the inclination has significant power at the period of ~660 years, and declination at the period of ~3500 years and 1300 years. These periods are similar to that from Japan and North America, in which the period of ~1300 years for declination has been reported in many areas around the world. The observed PSV from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70022403','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70022403"><span>The 2000 revision of the joint UK/US <span class="hlt">geomagnetic</span> field models and an IGRF 2000 candidate model</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Macmillan, S.; Quinn, J.M.</p> <p>2000-01-01</p> <p>The method of derivation of the joint UK/US spherical harmonic <span class="hlt">geomagnetic</span> main-field and <span class="hlt">secular-variation</span> models is presented. Early versions of these models, with the main field truncated at degree 10, are the UK/US candidates for the IGRF 2000 model. The main-field model describes the Earth's magnetic field at the 2000.0 epoch, while the <span class="hlt">secular-variation</span> model predicts the evolution of this field between 2000.0 and 2005.0. A revised 1995.0 main-field model was also generated. Regional models for the continental US, Alaska and Hawaii were also produced as a by-product of the UK/US global modelling effort. Copy right?? The Society of <span class="hlt">Geomagnetism</span> and Earth, Planetary and Space Sciences (SGEPSS); The Seismological Society of Japan; The Volcanological Society of Japan; The Geodetic Society of Japan; The Japanese Society for Planetary Sciences.</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/2017AGUFMGP21A..02C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP21A..02C"><span>The Holocene <span class="hlt">Geomagnetic</span> Field: Spikes, Low Field Anomalies, and Asymmetries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Constable, C.</p> <p>2017-12-01</p> <p>Our understanding of the Holocene magnetic field is constrained by individual paleomagnetic records of variable quality and resolution, composite regional <span class="hlt">secular</span> <span class="hlt">variation</span> curves, and low resolution global time-varying <span class="hlt">geomagnetic</span> field models. Although spatial and temporal data coverages have greatly improved in recent years, typical views of millennial-scale <span class="hlt">secular</span> <span class="hlt">variation</span> and the underlying physical processes continue to be heavily influenced by more detailed field structure and short term variability inferred from the historical record and modern observations. Recent models of gyre driven decay of the <span class="hlt">geomagnetic</span> dipole on centennial time scales, and studies of the evolution of the South Atlantic Anomaly provide one prominent example. Since 1840 dipole decay has largely been driven by meridional flux advection, with generally smaller fairly steady contributions from magnetic diffusion. The decay is dominantly associated with <span class="hlt">geomagnetic</span> activity in the Southern Hemisphere. In contrast to the present decay, dipole strength generally grew between 1500 and 1000 BC, sustaining high but fluctuating values around 90-100 ZAm2 until after 1500 AD. Thus high dipole moments appear to have been present shortly after 1000 AD at the time of the Levantine spikes, which represent extreme <span class="hlt">variations</span> in regional <span class="hlt">geomagnetic</span> field strength. It has been speculated that the growth in dipole moment originated from a strong flux patch near the equatorial region at the core-mantle boundary that migrated north and west to augment the dipole strength, suggesting the presence of a large-scale anticyclonic gyre in the northern hemisphere, not totally unlike the southern hemisphere flow that dominates present day dipole decay. The later brief episodes of high field strength in the Levant may have contributed to prolonged values of high dipole strength until the onset of dipole decay in the late second millennium AD. This could support the concept of a large-scale stable flow</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4850403B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4850403B"><span><span class="hlt">Secular</span> obliquity <span class="hlt">variations</span> for Ceres</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bills, Bruce; Scott, Bryan R.; Nimmo, Francis</p> <p>2016-10-01</p> <p>We have constructed <span class="hlt">secular</span> <span class="hlt">variation</span> models for the orbit and spin poles of the asteroid (1) Ceres, and used them to examine how the obliquity, or angular separation between spin and orbit poles, varies over a time span of several million years. The current obliquity is 4.3 degrees, which means that there are some regions near the poles which do not receive any direct Sunlight. The Dawn mission has provided an improved estimate of the spin pole orientation, and of the low degree gravity field. That allows us to estimate the rate at which the spin pole precesses about the instantaneous orbit pole.The orbit of Ceres is <span class="hlt">secularly</span> perturbed by the planets, with Jupiter's influence dominating. The current inclination of the orbit plane, relative to the ecliptic, is 10.6 degrees. However, it varies between 7.27 and 11.78 degrees, with dominant periods of 22.1 and 39.6 kyr. The spin pole precession rate parameter has a period of 205 kyr, with current uncertainty of 3%, dominated by uncertainty in the mean moment of inertia of Ceres.The obliquity varies, with a dominant period of 24.5 kyr, with maximum values near 26 degrees, and minimum values somewhat less than the present value. Ceres is currently near to a minimum of its <span class="hlt">secular</span> obliquity <span class="hlt">variations</span>.The near-surface thermal environment thus has at least 3 important time scales: diurnal (9.07 hours), annual (4.60 years), and obliquity cycle (24.5 kyr). The annual thermal wave likely only penetrates a few meters, but the much long thermal wave associated with the obliquity cycle has a skin depth larger by a factor of 70 or so, depending upon thermal properties in the subsurface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70197166','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70197166"><span>Book review: <span class="hlt">Geomagnetism</span> of baked clays and recent sediments</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Mankinen, Edward A.</p> <p>1984-01-01</p> <p>This book is an outgrowth of the symposium entitled “Time Scales of <span class="hlt">Geomagnetic</span> <span class="hlt">Secular</span> <span class="hlt">Variations</span>,” which was held at the 4th Assembly of the International Association of <span class="hlt">Geomagnetism</span> and Aeronomy (Edinburgh, U.K., August 1981). The volume includes many of the papers presented, which described paleomagnetic results from both archeologic materials and Holocene geologic deposits, as well as contributions solicited from other researchers in the fields of archeomagnetism and paleomagnetism. In a remarkably short time after the conclusion of the symposium the editors were able to elicit, edit, and assemble a large body of material from 40 individuals into a thoughtful, wellorganized product.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.4043P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.4043P"><span>Applying "domino" model to study dipolar <span class="hlt">geomagnetic</span> field reversals and <span class="hlt">secular</span> <span class="hlt">variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peqini, Klaudio; Duka, Bejo</p> <p>2014-05-01</p> <p>Aiming to understand the physical processes underneath the reversals events of <span class="hlt">geomagnetic</span> field, different numerical models have been conceived. We considered the so named "domino" model, an Ising-Heisenberg model of interacting magnetic spins aligned along a ring [Mazaud and Laj, EPSL, 1989; Mori et al., arXiv:1110.5062v2, 2012]. We will present here some results which are slightly different from the already published results, and will give our interpretation on the differences. Following the empirical studies of the long series of the axial magnetic moment (dipolar moment or "magnetization") generated by the model varying all model parameters, we defined the set of parameters that supply the longest mean time between reversals. Using this set of parameters, a short time series (about 10,000 years) of axial magnetic moment was generated. After de-noising the fluctuation of this time series, we compared it with the series of dipolar magnetic moment values supplied by CALS10K.1b model for the last 10000 years. We found similar behavior of the both series, even if the "domino" model could not supply a full explanation of the <span class="hlt">geomagnetic</span> field SV. In a similar way we will compare a 14000 years long series with the dipolar magnetic moment obtained by the model SHA.DIF.14k [Pavón-Carrasco et al., EPSL, 2014].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040015296&hterms=geomagnetic+reversal&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgeomagnetic%2Breversal','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040015296&hterms=geomagnetic+reversal&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgeomagnetic%2Breversal"><span><span class="hlt">Geomagnetic</span> Field During a Reversal</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heirtzler, J. R.</p> <p>2003-01-01</p> <p>It has frequently been suggested that only the <span class="hlt">geomagnetic</span> dipole, rather than higher order poles, reverse during a <span class="hlt">geomagnetic</span> field reversal. Under this assumption the <span class="hlt">geomagnetic</span> field strength has been calculated for the surface of the Earth for various steps of the reversal process. Even without an eminent a reversal of the field, extrapolation of the present <span class="hlt">secular</span> change (although problematic) shows that the field strength may become zero in some geographic areas within a few hundred years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70036301','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70036301"><span>An empirical model of the quiet daily <span class="hlt">geomagnetic</span> field <span class="hlt">variation</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>Yamazaki, Y.; Yumoto, K.; Cardinal, M.G.; Fraser, B.J.; Hattori, P.; Kakinami, Y.; Liu, J.Y.; Lynn, K.J.W.; Marshall, R.; McNamara, D.; Nagatsuma, T.; Nikiforov, V.M.; Otadoy, R.E.; Ruhimat, M.; Shevtsov, B.M.; Shiokawa, K.; Abe, S.; Uozumi, T.; Yoshikawa, A.</p> <p>2011-01-01</p> <p>An empirical model of the quiet daily <span class="hlt">geomagnetic</span> field <span class="hlt">variation</span> has been constructed based on <span class="hlt">geomagnetic</span> data obtained from 21 stations along the 210 Magnetic Meridian of the Circum-pan Pacific Magnetometer Network (CPMN) from 1996 to 2007. Using the least squares fitting method for <span class="hlt">geomagnetically</span> quiet days (Kp ??? 2+), the quiet daily <span class="hlt">geomagnetic</span> field <span class="hlt">variation</span> at each station was described as a function of solar activity SA, day of year DOY, lunar age LA, and local time LT. After interpolation in latitude, the model can describe solar-activity dependence and seasonal dependence of solar quiet daily <span class="hlt">variations</span> (S) and lunar quiet daily <span class="hlt">variations</span> (L). We performed a spherical harmonic analysis (SHA) on these S and L <span class="hlt">variations</span> to examine average characteristics of the equivalent external current systems. We found three particularly noteworthy results. First, the total current intensity of the S current system is largely controlled by solar activity while its focus position is not significantly affected by solar activity. Second, we found that seasonal <span class="hlt">variations</span> of the S current intensity exhibit north-south asymmetry; the current intensity of the northern vortex shows a prominent annual <span class="hlt">variation</span> while the southern vortex shows a clear semi-annual <span class="hlt">variation</span> as well as annual <span class="hlt">variation</span>. Thirdly, we found that the total intensity of the L current system changes depending on solar activity and season; seasonal <span class="hlt">variations</span> of the L current intensity show an enhancement during the December solstice, independent of the level of solar activity. Copyright 2011 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914631O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914631O"><span>Annual <span class="hlt">Variations</span> of the <span class="hlt">Geomagnetic</span> Field in the Earth's Polar Regions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ou, Jiaming; Du, Aimin</p> <p>2017-04-01</p> <p>The annual <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field play an important role in the coupling processes between the solar wind, magnetosphere and ionosphere. The annual <span class="hlt">variation</span> is a well-established feature of the <span class="hlt">geomagnetic</span> field, and usually is applied for modeling the conductivity of the lower mantle [Parkinson, 1983], and for long-term space weather forecasting [Bartels, 1932; Malin and Mete Isikara, 1976; Gonzalez et al., 1994]. Considerable effort has been devoted toward understanding the causes of the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span>, but the suggested physical mechanisms differ widely. The annual <span class="hlt">variation</span> is relatively weak in many magnetic indices, but it has a distinct signature in the <span class="hlt">geomagnetic</span> components. Thus, we use the components for this analysis. The components have a positive peak in northern summer and a negative dip in winter [Vestine, 1954]. Vestine [1954] suggested that the annual <span class="hlt">variation</span> is caused by an ionospheric dynamo in which electric currents in the ionosphere are generated by meridional winds. The winds blow from north-to-south during northern summer, and south-to-north in northern winter. Malin and Mete Isikara [1976], using near-midnight <span class="hlt">geomagnetic</span> data, concluded that the annual <span class="hlt">variation</span> results from a latitudinal movement of the auroral electrojet or the ring current. Stauning [2011] derived of the seasonal <span class="hlt">variation</span> of the quiet daily <span class="hlt">variations</span> and examined the influence of the sector structure of the interplanetary magnetic field. Ziegger and Mursula [1998] have suggested a third mechanism: that the cause is related to an asymmetric solar wind speed distribution across the heliographic equator. In this paper, we study the annual <span class="hlt">variation</span> problem using long-term magnetic observation and ionospheric conductivity. The sunlight incident on the ionosphere will be calculated. Although a global analysis is done, particular focus will be placed on the polar regions. This study covers the interval 1990-2010, and the cause of the well</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70011454','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70011454"><span>International <span class="hlt">Geomagnetic</span> Reference Field: the third generation.</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Peddie, N.W.</p> <p>1982-01-01</p> <p>In August 1981 the International Association of <span class="hlt">Geomagnetism</span> and Aeronomy revised the International <span class="hlt">Geomagnetic</span> Reference Field (IGRF). It is the second revision since the inception of the IGRF in 1968. The revision extends the earlier series of IGRF models from 1980 to 1985, introduces a new series of definitive models for 1965-1976, and defines a provisional reference field for 1975- 1980. The revision consists of: 1) a model of the main <span class="hlt">geomagnetic</span> field at 1980.0, not continuous with the earlier series of IGRF models together with a forecast model of the <span class="hlt">secular</span> <span class="hlt">variation</span> of the main field during 1980-1985; 2) definitive models of the main field at 1965.0, 1970.0, and 1975.0, with linear interpolation of the model coefficients specified for intervening dates; and 3) a provisional reference field for 1975-1980, defined as the linear interpolation of the 1975 and 1980 main-field models.-from Author</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940019992','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940019992"><span>Steady induction effects in <span class="hlt">geomagnetism</span>. Part 1C: <span class="hlt">Geomagnetic</span> estimation of steady surficial core motions: Application to the definitive <span class="hlt">geomagnetic</span> reference field models</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Voorhies, Coerte V.</p> <p>1993-01-01</p> <p>In the source-free mantle/frozen-flux core magnetic earth model, the non-linear inverse steady motional induction problem was solved using the method presented in Part 1B. How that method was applied to estimate steady, broad-scale fluid velocity fields near the top of Earth's core that induce the <span class="hlt">secular</span> change indicated by the Definitive <span class="hlt">Geomagnetic</span> Reference Field (DGRF) models from 1945 to 1980 are described. Special attention is given to the derivation of weight matrices for the DGRF models because the weights determine the apparent significance of the residual <span class="hlt">secular</span> change. The derived weight matrices also enable estimation of the <span class="hlt">secular</span> change signal-to-noise ratio characterizing the DGRF models. Two types of weights were derived in 1987-88: radial field weights for fitting the evolution of the broad-scale portion of the radial <span class="hlt">geomagnetic</span> field component at Earth's surface implied by the DGRF's, and general weights for fitting the evolution of the broad-scale portion of the scalar potential specified by these models. The difference is non-trivial because not all the <span class="hlt">geomagnetic</span> data represented by the DGRF's constrain the radial field component. For radial field weights (or general weights), a quantitatively acceptable explication of broad-scale <span class="hlt">secular</span> change relative to the 1980 Magsat epoch must account for 99.94271 percent (or 99.98784 percent) of the total weighted variance accumulated therein. Tolerable normalized root-mean-square weighted residuals of 2.394 percent (or 1.103 percent) are less than the 7 percent errors expected in the source-free mantle/frozen-flux core approximation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830007484','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830007484"><span><span class="hlt">Geomagnetic</span> modeling by optimal recursive filtering</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gibbs, B. P.; Estes, R. H.</p> <p>1981-01-01</p> <p>The results of a preliminary study to determine the feasibility of using Kalman filter techniques for <span class="hlt">geomagnetic</span> field modeling are given. Specifically, five separate field models were computed using observatory annual means, satellite, survey and airborne data for the years 1950 to 1976. Each of the individual field models used approximately five years of data. These five models were combined using a recursive information filter (a Kalman filter written in terms of information matrices rather than covariance matrices.) The resulting estimate of the <span class="hlt">geomagnetic</span> field and its <span class="hlt">secular</span> <span class="hlt">variation</span> was propogated four years past the data to the time of the MAGSAT data. The accuracy with which this field model matched the MAGSAT data was evaluated by comparisons with predictions from other pre-MAGSAT field models. The field estimate obtained by recursive estimation was found to be superior to all other models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70016888','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70016888"><span>Evaluation of models proposed for the 1991 revision of the International <span class="hlt">Geomagnetic</span> Reference Field</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Peddie, N.W.</p> <p>1992-01-01</p> <p>The 1991 revision of the International <span class="hlt">Geomagnetic</span> Reference Field (IGRF) comprises a definitive main-field model for 1985.0, a main-field model for 1990.0, and a forecast <span class="hlt">secular-variation</span> model for the period 1990-1995. The five 1985.0 main-field models and five 1990.0 main-field models that were proposed have been evaluated by comparing them with one another, with magnetic observatory data, and with Project MAGNET aerial survey data. The comparisons indicate that the main-field models proposed by IZMIRAN, and the <span class="hlt">secular-variation</span> model proposed jointly by the British Geological Survey and the US Naval Oceanographic Office, should be assigned relatively lower weight in the derivation of the new IGRF models. -Author</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030053446&hterms=dynamo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddynamo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030053446&hterms=dynamo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddynamo"><span>Prospect of Using Numerical Dynamo Model for Prediction of <span class="hlt">Geomagnetic</span> <span class="hlt">Secular</span> <span class="hlt">Variation</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuang, Weijia; Tangborn, Andrew</p> <p>2003-01-01</p> <p>Modeling of the Earth's core has reached a level of maturity to where the incorporation of observations into the simulations through data assimilation has become feasible. Data assimilation is a method by which observations of a system are combined with a model output (or forecast) to obtain a best guess of the state of the system, called the analysis. The analysis is then used as an initial condition for the next forecast. By doing assimilation, not only we shall be able to predict partially <span class="hlt">secular</span> <span class="hlt">variation</span> of the core field, we could also use observations to further our understanding of dynamical states in the Earth's core. One of the first steps in the development of an assimilation system is a comparison between the observations and the model solution. The highly turbulent nature of core dynamics, along with the absence of any regular external forcing and constraint (which occurs in atmospheric dynamics, for example) means that short time comparisons (approx. 1000 years) cannot be made between model and observations. In order to make sensible comparisons, a direct insertion assimilation method has been implemented. In this approach, magnetic field observations at the Earth's surface have been substituted into the numerical model, such that the ratio of the multiple components and the dipole component from observation is adjusted at the core-mantle boundary and extended to the interior of the core, while the total magnetic energy remains unchanged. This adjusted magnetic field is then used as the initial field for a new simulation. In this way, a time tugged simulation is created which can then be compared directly with observations. We present numerical solutions with and without data insertion and discuss their implications for the development of a more rigorous assimilation system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EP%26S...67...79T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EP%26S...67...79T"><span>International <span class="hlt">Geomagnetic</span> Reference Field: the 12th generation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thébault, Erwan; Finlay, Christopher C.; Beggan, Ciarán D.; Alken, Patrick; Aubert, Julien; Barrois, Olivier; Bertrand, Francois; Bondar, Tatiana; Boness, Axel; Brocco, Laura; Canet, Elisabeth; Chambodut, Aude; Chulliat, Arnaud; Coïsson, Pierdavide; Civet, François; Du, Aimin; Fournier, Alexandre; Fratter, Isabelle; Gillet, Nicolas; Hamilton, Brian; Hamoudi, Mohamed; Hulot, Gauthier; Jager, Thomas; Korte, Monika; Kuang, Weijia; Lalanne, Xavier; Langlais, Benoit; Léger, Jean-Michel; Lesur, Vincent; Lowes, Frank J.; Macmillan, Susan; Mandea, Mioara; Manoj, Chandrasekharan; Maus, Stefan; Olsen, Nils; Petrov, Valeriy; Ridley, Victoria; Rother, Martin; Sabaka, Terence J.; Saturnino, Diana; Schachtschneider, Reyko; Sirol, Olivier; Tangborn, Andrew; Thomson, Alan; Tøffner-Clausen, Lars; Vigneron, Pierre; Wardinski, Ingo; Zvereva, Tatiana</p> <p>2015-05-01</p> <p>The 12th generation of the International <span class="hlt">Geomagnetic</span> Reference Field (IGRF) was adopted in December 2014 by the Working Group V-MOD appointed by the International Association of <span class="hlt">Geomagnetism</span> and Aeronomy (IAGA). It updates the previous IGRF generation with a definitive main field model for epoch 2010.0, a main field model for epoch 2015.0, and a linear annual predictive <span class="hlt">secular</span> <span class="hlt">variation</span> model for 2015.0-2020.0. Here, we present the equations defining the IGRF model, provide the spherical harmonic coefficients, and provide maps of the magnetic declination, inclination, and total intensity for epoch 2015.0 and their predicted rates of change for 2015.0-2020.0. We also update the magnetic pole positions and discuss briefly the latest changes and possible future trends of the Earth's magnetic field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PEPI..215...29F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PEPI..215...29F"><span>Archeointensities in Greece during the Neolithic period: New insights into material selection and <span class="hlt">secular</span> <span class="hlt">variation</span> curve</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fanjat, G.; Aidona, E.; Kondopoulou, D.; Camps, P.; Rathossi, C.; Poidras, T.</p> <p>2013-02-01</p> <p>Numerous archeomagnetic studies have provided high quality data for both the direction and the intensity of the <span class="hlt">geomagnetic</span> field, essentially in Europe for the last 10 millennia. In particular, Greece supplies a lot of archeological materials due to its impressive cultural heritage and volcanic activity, so that numerous data have been obtained from burnt clays or historical lava flows. The most recent Greek <span class="hlt">secular</span> <span class="hlt">variation</span> curves are available for the last 8 millennia for the intensity and the last 6 millennia for the direction. Nevertheless, the coverage still presents several gaps for periods older than 2500 BC. In an effort to complete the Greek curve and extend it to older times, we present the archeointensity results from three Neolithic settlements in Northern Greece. The samples are of two different natures: burnt structures from Avgi (5250 ± 150 BC) and Vasili (4800 ± 200 BC), as well as ceramics from Dikili Tash (4830 ± 80 BC) and Vasili (4750 ± 250 BC). The samples have been subjected to standard rock magnetic analyses in order to estimate the thermal stability and the domain state of the magnetic carriers before archeointensity measurements. Surprisingly, very few ceramic samples provided reliable archeointensities whereas samples from burnt structures presented a very good success rate. Complementary studies showed that a detailed examination of the matrix color, following archeological information and classification standards can be a decisive test for pre-selection of sherds. In spite of these unsuccessful measurements from ceramics, we obtained an intensity value of 73.5 ± 1.1 μT for Dikili Tash, a higher value than the other data obtained in the same area, during the same period. However we do not have evidences for a technical artefact during the experiment. The burnt structures yielded two reliable archeointensities of 36.1 ± 1.8 μT and 46.6 ± 3.4 μT for Avgi and Vasili, respectively. Finally, we achieved a new archeomagnetic dating</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA23A2536T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA23A2536T"><span>Seasonal <span class="hlt">Variation</span> of High-latitude <span class="hlt">Geomagnetic</span> Activity Revisited</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tanskanen, E.; Hynönen, R.; Mursula, K.</p> <p>2017-12-01</p> <p>The coupling of the solar wind and auroral region has been examined by using westward electrojet indices since 1966 - 2014. We have studied the seasonal <span class="hlt">variation</span> of high-latitude <span class="hlt">geomagnetic</span> activity in individual years for solar cycles 20 - 24. The classical two-equinox activity pattern in <span class="hlt">geomagnetic</span> activity was seen in multi-year averages but it was found in less than one third of the years examined. We found that the seasonal <span class="hlt">variation</span> of high-latitude <span class="hlt">geomagnetic</span> activity closely follows the solar wind speed. While the mechanisms leading to the two-equinox maxima pattern are in operation, the long-term change of solar wind speed tends to mask the effect of these mechanisms for individual years. We identified the most active and the second most active season based on westward electrojet indices AL (1966 - 2014) and IL (1995 - 2014). The annual maximum is found at either equinox in 2/3 and at either solstice in 1/3 of the years examined. Large cycle-to-cycle <span class="hlt">variation</span> is found in the seasonal pattern: equinox maxima are more common during cycles 21 and 22 than in cycles 23 or 24. An exceptionally long winter dominance in high-latitude activity and solar wind speed is seen in the declining phase of cycle 23, after the appearance of the long-lasting low-latitude coronal hole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP23A0895P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP23A0895P"><span>Linkage between the Biosphere and <span class="hlt">Geomagnetic</span> field: Knowns and Unknowns</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pan, Y.; Zhu, R.</p> <p>2017-12-01</p> <p>The <span class="hlt">geomagnetic</span> field extends from Earth's interior into space, and protects our planets habitability by shielding the planet from solar winds and cosmic rays. Recently, single zircon paleomagnetic study provides evidence of the field to ages as old as 4.2 Ga. Many great questions remain, including whether the emergence of life on Earth was a consequence of the field's protection, how organisms utilize the field, and if field <span class="hlt">variations</span> (polarity reversal, excursion and <span class="hlt">secular</span> <span class="hlt">variation</span>) impact the evolution of the biosphere. In the past decade, great efforts have been made to probe these very complex and great challenging questions through the inter-disciplinary subject of biogeomagnetism. Numerous birds, fish, sea turtles, bats and many other organisms utilize the <span class="hlt">geomagnetic</span> field during orientation and long-distance navigation. We recently found that bats, the second most abundant order of mammals, can use the direction of magnetic field with a weak strength comparable to polarity transitions/excursions, which is indicative of advanced magnetoreception developed in bats co-evolving with the <span class="hlt">geomagnetic</span> field since the Eocene. Magnetotactic bacteria swim along the <span class="hlt">geomagnetic</span> field lines by synthesizing intracellular nano-sized and chain-arranged magnetic minerals (magnetosomes). Recent field surveys in China, Europe, America and Australia have shown that these microbes are ubiquitous in aqueous habitats. Both their biogeography distribution and magnetotactic swimming speed are field intensity dependent. On the other hand, it is increasingly accepted that the <span class="hlt">geomagnetic</span> field influences life through several indirect pathways. For example, it has been discovered that solar wind erosion enhanced the atmospheric oxygen escape during periods of weak magnetic field and global mean ionospheric electron density profiles can be affected by <span class="hlt">geomagnetic</span> field strength <span class="hlt">variation</span>. In addition, depletion of the ozone layer during a weak magnetic field could result in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003RvGeo..41.1004V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003RvGeo..41.1004V"><span>Time <span class="hlt">variations</span> in <span class="hlt">geomagnetic</span> intensity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Valet, Jean-Pierre</p> <p>2003-03-01</p> <p>After many years spent by paleomagnetists studying the directional behavior of the Earth's magnetic field at all possible timescales, detailed measurements of field intensity are now needed to document the <span class="hlt">variations</span> of the entire vector and to analyze the time evolution of the field components. A significant step has been achieved by combining intensity records derived from archeological materials and from lava flows in order to extract the global field changes over the past 12 kyr. A second significant step was due to the emergence of coherent records of relative paleointensity using the remanent magnetization of sediments to retrace the evolution of the dipole field. A third step was the juxtaposition of these signals with those derived from cosmogenic isotopes. Contemporaneous with the acquisition of records, new techniques have been developed to constrain the <span class="hlt">geomagnetic</span> origin of the signals. Much activity has also been devoted to improving the quality of determinations of absolute paleointensity from volcanic rocks with new materials, proper selection of samples, and investigations of complex changes in magnetization during laboratory experiments. Altogether these developments brought us from a situation where the field changes were restricted to the past 40 kyr to the emergence of a coherent picture of the changes in the <span class="hlt">geomagnetic</span> dipole moment for at least the past 1 Myr. On longer timescales the field variability and its average behavior is relatively well documented for the past 400 Myr. Section 3 gives a summary of most methods and techniques that are presently used to track the field intensity changes in the past. In each case, current limits and potential promises are discussed. The section 4 describes the field <span class="hlt">variations</span> measured so far over various timescales covered by the archeomagnetic and the paleomagnetic records. Preference has always been given to composite records and databases in order to extract and discuss major and global <span class="hlt">geomagnetic</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMGP13B1307Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMGP13B1307Y"><span>Study on the <span class="hlt">Geomagnetic</span> Short Period <span class="hlt">Variations</span> of the Northwestern Yunnan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yuan, Y.; Li, Q.; Cai, J.</p> <p>2015-12-01</p> <p>The Northwestern Yunnan is located in the interaction area between the Eurasian plate and the India plate. This area has been the ideal place for the research of continental dynamics and the prediction for risk region of strong earthquake for its complex tectonic environment and frequent seismic activity. Therefore the study on the <span class="hlt">geomagnetic</span> short period <span class="hlt">variations</span> is of great significance in the exploration of deep electrical structure, analysis of the seismic origin and deep geodynamics in the Northwestern Yunnan of China . This paper is based on the <span class="hlt">geomagnetic</span> data from the magnetometer array with 8 sites built in the northwestern Yunnan to explore the deep electrical structure by the method of <span class="hlt">geomagnetic</span> depth sounding. Firstly, we selected a total of 183 <span class="hlt">geomagnetic</span> short period events at the range of 6min to 120min period. And we found a north northwest dividing line, of which two sides has the opposite value in the vertical component <span class="hlt">variation</span> amplitude, which indicates the obvious conductivity anomaly underground. Secondly, the contour maps of the ratio of vertical component and horizontal component <span class="hlt">variation</span> amplitude ΔZ/ΔH in different periods reflects the changes of a high conductivity belt's direction and position. In addition, the induction arrows maps within the period of 2 - 256min also shows that on the two sides of the dividing line the induction vectors deviate from each other, and the amplitude and direction of vectors varies with periods regularly. In the light of this, we infer that a high conductivity belt probably exists, which stretches from the deep crust to uppermost mantle and changes with depth constantly with the reference of magnetotelluric sounding. In the end of this paper, the staggered grid finite difference method is used to model the simplified three-dimensional high conductivity anomaly, and the result shows magnetic field distributions are consistent with the observed <span class="hlt">geomagnetic</span> short period <span class="hlt">variations</span> characteristics in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930049208&hterms=earth+day&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearth%2Bday','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930049208&hterms=earth+day&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearth%2Bday"><span>Present-day <span class="hlt">secular</span> <span class="hlt">variations</span> in the zonal harmonics of earth's geopotential</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mitrovica, J. X.; Peltier, W. R.</p> <p>1993-01-01</p> <p>The mathematical formulation required for predicting <span class="hlt">secular</span> <span class="hlt">variation</span> in the geopotential is developed for the case of a spherically symmetric, self-gravitating, viscoelastic earth model and an arbitrary surface load which can include a gravitational self-consistent ocean loading component. The theory is specifically applied to predict the present-day <span class="hlt">secular</span> <span class="hlt">variation</span> in the zonal harmonics of the geopotenial arising from the surface mass loading associated with the late Pleistocene glacial cycles. A procedure is outlined in which predictions of the present-day geopotential signal due to the late Pleistocene glacial cycles may be used to derive bounds on the net present-day mass flux from the Antarctic and Greenland ice sheets to the local oceans.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.7516M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.7516M"><span>Cosmic rays flux and <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> at midlatitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morozova, Anna; Ribeiro, Paulo; Tragaldabas Collaboration Team</p> <p>2014-05-01</p> <p>It is well known that the cosmic rays flux is modulated by the solar wind and the Earth's magnetic field. The Earth's magnetic field deflects charged particles in accordance with their momentum and the local field strength and direction. The <span class="hlt">geomagnetic</span> cutoffs depend both on the internal and the external components of the <span class="hlt">geomagnetic</span> field, therefore reflecting the geodynamo and the solar activity <span class="hlt">variations</span>. A new generation, high performance, cosmic ray detector Tragaldabas was recently installed at the University of Santiago de Compostela (Spain). The detector has been acquiring test data since September 2013 with a rate of about 80 events/s over a solid angle of ~5 srad. around the vertical direction. To take full advantage of this new facility for the study of cosmic rays arriving to the Earth, an international collaboration has been organized, of about 20 researchers from 10 laboratories of 5 European countries. The Magnetic Observatory of Coimbra (Portugal) has been measuring the <span class="hlt">geomagnetic</span> field components for almost 150 years since the first measurements in 1866. It is presently equipped with up-to-date instruments. Here we present a preliminary analysis of the global cosmic ray fluxes acquired by the new Tragaldabas detector in relation to the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> measured by the Coimbra observatory. We also compare the data from the new cosmic rays detector with results obtained by the Castilla-La Mancha Neutron Monitor (CaLMa, Gadalajara, Spain) that is in operation since October 2011.</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('https://www.ncbi.nlm.nih.gov/pubmed/23410284','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23410284"><span>Domino model for <span class="hlt">geomagnetic</span> field reversals.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mori, N; Schmitt, D; Wicht, J; Ferriz-Mas, A; Mouri, H; Nakamichi, A; Morikawa, M</p> <p>2013-01-01</p> <p>We solve the equations of motion of a one-dimensional planar Heisenberg (or Vaks-Larkin) model consisting of a system of interacting macrospins aligned along a ring. Each spin has unit length and is described by its angle with respect to the rotational axis. The orientation of the spins can vary in time due to spin-spin interaction and random forcing. We statistically describe the behavior of the sum of all spins for different parameters. The term "domino model" in the title refers to the interaction among the spins. We compare the model results with <span class="hlt">geomagnetic</span> field reversals and dynamo simulations and find strikingly similar behavior. The aggregate of all spins keeps the same direction for a long time and, once in a while, begins flipping to change the orientation by almost 180 degrees (mimicking a <span class="hlt">geomagnetic</span> reversal) or to move back to the original direction (mimicking an excursion). Most of the time the spins are aligned or antialigned and deviate only slightly with respect to the rotational axis (mimicking the <span class="hlt">secular</span> <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> pole with respect to the geographic pole). Reversals are fast compared to the times in between and they occur at random times, both in the model and in the case of the Earth's magnetic field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFMGP33B..02D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFMGP33B..02D"><span>Marine Magnetic Anomalies, Oceanic Crust Magnetization, and <span class="hlt">Geomagnetic</span> Time <span class="hlt">Variations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dyment, J.; Arkani-Hamed, J.</p> <p>2005-12-01</p> <p>Since the classic paper of Vine and Matthews (Nature, 1963), marine magnetic anomalies are commonly used to date the ocean floor through comparison with the <span class="hlt">geomagnetic</span> polarity time scale and proper identification of reversal sequences. As a consequence, the classical model of rectangular prisms bearing a normal / reversed magnetization has been dominant in the literature for more than 40 years. Although the model explains major characteristics of the sea-surface magnetic anomalies, it is contradicted by (1) recent advances on the geophysical and petrologic structure of the slow-spreading oceanic crust, and (2) the observation of short-term <span class="hlt">geomagnetic</span> time <span class="hlt">variations</span>, both of which are more complex than assumed in the classical model. Marine magnetic anomalies may also provide information on the magnetization of the oceanic crust as well as short-term temporal fluctuations of the <span class="hlt">geomagnetic</span> field. The "anomalous skewness", a residual phase once the anomalies have been reduced to the pole, has been interpreted either in terms of <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> or crustal structure. The spreading-rate dependence of anomalous skewness rules out the <span class="hlt">geomagnetic</span> hypothesis and supports a spreading-rate dependent magnetic structure of the oceanic crust, with a basaltic layer accounting for most of the anomalies at fast spreading rates and an increasing contribution of the deeper layers with decreasing spreading rate. The slow cooling of the lower crust and uppermost mantle and serpentinization, a low temperature alteration process which produces magnetite, are the likely cause of this contribution, also required to account for satellite magnetic anomalies over oceanic areas. Moreover, the "hook shape" of some sea-surface anomalies favors a time lag in the magnetization acquisition processes between upper and lower magnetic layers: extrusive basalt acquires a thermoremanent magnetization as soon as emplaced, whereas the underlying peridotite and olivine gabbro cool slowly</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.3001A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.3001A"><span><span class="hlt">Geomagnetic</span> inverse problem and data assimilation: a progress report</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aubert, Julien; Fournier, Alexandre</p> <p>2013-04-01</p> <p>In this presentation I will present two studies recently undertaken by our group in an effort to bring the benefits of data assimilation to the study of Earth's magnetic field and the dynamics of its liquid iron core, where the geodynamo operates. In a first part I will focus on the <span class="hlt">geomagnetic</span> inverse problem, which attempts to recover the fluid flow in the core from the temporal <span class="hlt">variation</span> of the magnetic field (known as the <span class="hlt">secular</span> <span class="hlt">variation</span>). <span class="hlt">Geomagnetic</span> data can be downward continued from the surface of the Earth down to the core-mantle boundary, but not further below, since the core is an electrical conductor. Historically, solutions to the <span class="hlt">geomagnetic</span> inverse problem in such a sparsely observed system were thus found only for flow immediately below the core mantle boundary. We have recently shown that combining a numerical model of the geodynamo together with magnetic observations, through the use of Kalman filtering, now allows to present solutions for flow throughout the core. In a second part, I will present synthetic tests of sequential <span class="hlt">geomagnetic</span> data assimilation aiming at evaluating the range at which the future of the geodynamo can be predicted, and our corresponding prospects to refine the current <span class="hlt">geomagnetic</span> predictions. Fournier, Aubert, Thébault: Inference on core surface flow from observations and 3-D dynamo modelling, Geophys. J. Int. 186, 118-136, 2011, doi: 10.1111/j.1365-246X.2011.05037.x Aubert, Fournier: Inferring internal properties of Earth's core dynamics and their evolution from surface observations and a numerical geodynamo model, Nonlinear Proc. Geoph. 18, 657-674, 2011, doi:10.5194/npg-18-657-2011 Aubert: Flow throughout the Earth's core inverted from <span class="hlt">geomagnetic</span> observations and numerical dynamo models, Geophys. J. Int., 2012, doi: 10.1093/gji/ggs051</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA22A..04C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA22A..04C"><span>Modeling of Thermospheric Neutral Density <span class="hlt">Variations</span> in Response to <span class="hlt">Geomagnetic</span> Forcing using GRACE Accelerometer Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calabia, A.; Matsuo, T.; Jin, S.</p> <p>2017-12-01</p> <p>The upper atmospheric expansion refers to an increase in the temperature and density of Earth's thermosphere due to increased <span class="hlt">geomagnetic</span> and space weather activities, producing anomalous atmospheric drag on LEO spacecraft. Increased drag decelerates satellites, moving their orbit closer to Earth, decreasing the lifespan of satellites, and making satellite orbit determination difficult. In this study, thermospheric neutral density <span class="hlt">variations</span> due to <span class="hlt">geomagnetic</span> forcing are investigated from 10 years (2003-2013) of GRACE's accelerometer-based estimates. In order to isolate the <span class="hlt">variations</span> produced by <span class="hlt">geomagnetic</span> forcing, 99.8% of the total variability has been modeled and removed through the parameterization of annual, LST, and solar-flux <span class="hlt">variations</span> included in the primary Empirical Orthogonal Functions. The residual disturbances of neutral density <span class="hlt">variations</span> have been investigated further in order to unravel their relationship to several <span class="hlt">geomagnetic</span> indices and space weather activity indicators. Stronger fluctuations have been found in the southern polar cap, following the dipole-tilt angle <span class="hlt">variations</span>. While the parameterization of the residual disturbances in terms of Dst index results in the best fit to training data, the use of merging electric field as a predictor leads to the best forecasting performance. An important finding is that modeling of neutral density <span class="hlt">variations</span> in response <span class="hlt">geomagnetic</span> forcing can be improved by accounting for the latitude-dependent delay. Our data-driven modeling results are further compared to modeling with TIEGCM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70010407','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70010407"><span>Spectral characteristics of <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> at low and equatorial latitudes</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Campbell, W.H.</p> <p>1977-01-01</p> <p><span class="hlt">Geomagnetic</span> field spectra from eight standard observations at <span class="hlt">geomagnetic</span> latitudes below 30?? were studied to determine the field characteristics unique to the equatorial region. Emphasis was placed upon those <span class="hlt">variations</span> having periods between 5 min and 4 hr for a selection of magnetically quiet, average, and active days in 1965. The power spectral density at the equator was about ten times that the near 30?? latitude. The initial manifestation of the equatorial electrojet as evidenced by the east-west alignment of the horizontal field or the change in vertical amplitudes occurred below about 20?? latitude. Induced current effects upon the vertical component from which the Earth conductivity might be inferred could best be obtained at times and latitudes unaffected by the electrojet current. Values of about 1.6 ?? 103 mhos/m for an effective skin depth of 500-600 km were determined. The spectral amplitudes increased linearly with <span class="hlt">geomagnetic</span> activity index, Ap. The spectral slope had a similar behavior at all latitudes. The slope changed systematically with Ap-index and showed a diurnal <span class="hlt">variation</span>, centered on local noon, that changed form with <span class="hlt">geomagnetic</span> activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70011876','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70011876"><span>International <span class="hlt">geomagnetic</span> reference field 1980: a report by IAGA Division I working group.</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Peddie, N.W.</p> <p>1982-01-01</p> <p>Describes the recommendations of the working group, which suggested additions to IGRF because of the cumulative effect of the inevitable uncertainties in the <span class="hlt">secular</span> <span class="hlt">variation</span> models which had led to unacceptable inaccuracies in the IGRF by the late 1970's. The recommendations were accepted by the International Association of <span class="hlt">Geomagnetism</span> and Aeronomy on August 15, 1981 at the 4th Scientific Assembly, Edinburgh. An extended table sets out spherical harmonic coefficients of the IGRF 1980.-R.House</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://ngmdb.usgs.gov/Prodesc/proddesc_81154.htm','USGSPUBS'); return false;" href="http://ngmdb.usgs.gov/Prodesc/proddesc_81154.htm"><span>The International <span class="hlt">Geomagnetic</span> Reference Field, 2005</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Rukstales, Kenneth S.; Love, Jeffrey J.</p> <p>2007-01-01</p> <p>This is a set of five world charts showing the declination, inclination, horizontal intensity, vertical component, and total intensity of the Earth's magnetic field at mean sea level at the beginning of 2005. The charts are based on the International <span class="hlt">Geomagnetic</span> Reference Field (IGRF) main model for 2005 and <span class="hlt">secular</span> change model for 2005-2010. The IGRF is referenced to the World Geodetic System 1984 ellipsoid. Additional information about the USGS <span class="hlt">geomagnetism</span> program is available at: http://geomag.usgs.gov/</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PEPI..229...98P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PEPI..229...98P"><span>Paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> study of Ar-Ar dated lavas flows from Tacambaro area (Central Mexico): Possible evidence of Intra-Jaramillo <span class="hlt">geomagnetic</span> excursion in volcanic rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peña, Rafael Maciel; Goguitchaichvili, Avto; Guilbaud, Marie-Noëlle; Martínez, Vicente Carlos Ruiz; Rathert, Manuel Calvo; Siebe, Claus; Reyes, Bertha Aguilar; Morales, Juan</p> <p>2014-04-01</p> <p>More than 350 oriented paleomagnetic cores were obtained for rock-magnetic and paleomagnetic analysis from radiometrically dated (40Ar-39Ar) magmatic rocks occurring in the southern segment (Jorullo and Tacámbaro areas) of the Michoacán-Guanajuato Volcanic Field in the Trans-Mexican Volcanic Belt. Most of the lavas (37) stem from monogenetic volcanoes dated at less than 4 Ma. Two additional sites were sampled from the plutonic basement dated at 33-30 Ma. Primary remanences carried by low-Ti titanomagnetites allowed to determining 34 reliable site-mean directions of mostly normal (27) but also reversed (7) polarities. The mean directions of these two populations are antipodal, and suggest neither major vertical-axis rotations with respect to the North America craton nor tilting in the region for the last 4 Ma (rotation and flattening of the inclination parameters being less than -5.9 ± 3.8 and 0.1 ± 3.9, respectively). The corresponding paleomagnetic pole obtained for Pliocene-Pleistocene times is PLAT = 83.4°, PLON = 2.4° (N = 32, A95 = 2.7°). Virtual <span class="hlt">geomagnetic</span> poles also contribute to the time averaged field global database and to the paleosecular <span class="hlt">variation</span> (PSV) investigations at low latitudes from lavas for the last 5 Ma, showing a <span class="hlt">geomagnetic</span> dispersion value that is in agreement with available PSV models. When comparing the magnetic polarities and corresponding radiometric ages of the studied sites with the Cenozoic <span class="hlt">geomagnetic</span> polarity time scale (GPTS), a good correlation is observable. This finding underscores the suitability of data obtained on lavas in Central Mexico for contributing to the GPTS. Furthermore, the detection of short-lived <span class="hlt">geomagnetic</span> features seems possible, since the possible evidence of Intra-Jaramillo <span class="hlt">geomagnetic</span> excursion could be documented for the first time in these volcanic rocks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4233730','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4233730"><span><span class="hlt">Geomagnetic</span> imprinting predicts spatio-temporal <span class="hlt">variation</span> in homing migration of pink and sockeye salmon</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Putman, Nathan F.; Jenkins, Erica S.; Michielsens, Catherine G. J.; Noakes, David L. G.</p> <p>2014-01-01</p> <p>Animals navigate using a variety of sensory cues, but how each is weighted during different phases of movement (e.g. dispersal, foraging, homing) is controversial. Here, we examine the <span class="hlt">geomagnetic</span> and olfactory imprinting hypotheses of natal homing with datasets that recorded <span class="hlt">variation</span> in the migratory routes of sockeye (Oncorhynchus nerka) and pink (Oncorhynchus gorbuscha) salmon returning from the Pacific Ocean to the Fraser River, British Columbia. Drift of the magnetic field (i.e. <span class="hlt">geomagnetic</span> imprinting) uniquely accounted for 23.2% and 44.0% of the <span class="hlt">variation</span> in migration routes for sockeye and pink salmon, respectively. Ocean circulation (i.e. olfactory imprinting) predicted 6.1% and 0.1% of the <span class="hlt">variation</span> in sockeye and pink migration routes, respectively. Sea surface temperature (a variable influencing salmon distribution but not navigation, directly) accounted for 13.0% of the <span class="hlt">variation</span> in sockeye migration but was unrelated to pink migration. These findings suggest that <span class="hlt">geomagnetic</span> navigation plays an important role in long-distance homing in salmon and that consideration of navigation mechanisms can aid in the management of migratory fishes by better predicting movement patterns. Finally, given the diversity of animals that use the Earth's magnetic field for navigation, <span class="hlt">geomagnetic</span> drift may provide a unifying explanation for spatio-temporal <span class="hlt">variation</span> in the movement patterns of many species. PMID:25056214</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70014204','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014204"><span>The <span class="hlt">geomagnetic</span> jerk of 1969 and the DGRFs</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Thompson, D.; Cain, J.C.</p> <p>1987-01-01</p> <p>Cubic spline fits to the DGRF/IGRF series indicate agreement with other analyses showing the 1969-1970 magnetic jerk in the h ??12 and g ??02 <span class="hlt">secular</span> change coefficients, and agreement that the h ??11 term showed no sharp change. The <span class="hlt">variation</span> of the g ??01 term is out of phase with other analyses indicating a likely error in its representation in the 1965-1975 interval. We recommend that future derivations of the 'definitive' <span class="hlt">geomagnetic</span> reference models take into consideration the times of impulses or jerks so as to not be bound to a standard 5 year interval, and otherwise to make more considered analyses before adopting sets of coefficients. ?? 1987.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PEPI..276..118S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PEPI..276..118S"><span>Combining virtual observatory and equivalent source dipole approaches to describe the <span class="hlt">geomagnetic</span> field with Swarm measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saturnino, Diana; Langlais, Benoit; Amit, Hagay; Civet, François; Mandea, Mioara; Beucler, Éric</p> <p>2018-03-01</p> <p>A detailed description of the main <span class="hlt">geomagnetic</span> field and of its temporal <span class="hlt">variations</span> (i.e., the <span class="hlt">secular</span> <span class="hlt">variation</span> or SV) is crucial to understanding the geodynamo. Although the SV is known with high accuracy at ground magnetic observatory locations, the globally uneven distribution of the observatories hampers the determination of a detailed global pattern of the SV. Over the past two decades, satellites have provided global surveys of the <span class="hlt">geomagnetic</span> field which have been used to derive global spherical harmonic (SH) models through some strict data selection schemes to minimise external field contributions. However, discrepancies remain between ground measurements and field predictions by these models; indeed the global models do not reproduce small spatial scales of the field temporal <span class="hlt">variations</span>. To overcome this problem we propose to directly extract time series of the field and its temporal <span class="hlt">variation</span> from satellite measurements as it is done at observatory locations. We follow a Virtual Observatory (VO) approach and define a global mesh of VOs at satellite altitude. For each VO and each given time interval we apply an Equivalent Source Dipole (ESD) technique to reduce all measurements to a unique location. Synthetic data are first used to validate the new VO-ESD approach. Then, we apply our scheme to data from the first two years of the Swarm mission. For the first time, a 2.5° resolution global mesh of VO time series is built. The VO-ESD derived time series are locally compared to ground observations as well as to satellite-based model predictions. Our approach is able to describe detailed temporal <span class="hlt">variations</span> of the field at local scales. The VO-ESD time series are then used to derive global spherical harmonic models. For a simple SH parametrization the model describes well the <span class="hlt">secular</span> trend of the magnetic field both at satellite altitude and at the surface. As more data will be made available, longer VO-ESD time series can be derived and consequently used to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUSMGP11C..02B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUSMGP11C..02B"><span>The First Radiocarbon-Constrained Full-Vector Holocene Paleomagnetic <span class="hlt">Secular</span> <span class="hlt">Variation</span> Reconstruction for Eastern Canada</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barletta, F.; St-Onge, G.; Stoner, J.; Lajeunesse, P.</p> <p>2009-05-01</p> <p>Here we present the first high-resolution Holocene paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> (PSV) master curve and relative paleointensity stack constrained by radiocarbon dates for Eastern Canada. This reconstruction is based on seven sedimentary sequences collected from the St. Lawrence Estuary and Gulf from the head to the mouth of the Laurentian Channel. The natural remanent magnetization (NRM), the anhysteretic remanent magnetization (ARM) and the isothermal remanent magnetization (IRM) were measured on u-channel samples at the Paleomagnetism Laboratory of ISMER using a 2G Enterprises cryogenic magnetometer. Magnetic mineralogy was additionally assessed using a recently installed alternative gradient force magnetometer (AGM). The magnetic mineralogy of the Holocene postglacial sediments is mainly carried by low-coercivity ferrimagnetic minerals (most likely magnetite) in the pseudo-single domain size range. The characteristic remanent magnetization (ChRM), assessed by principal component analysis, reveals the presence of a stable and well-defined magnetization characterized by maximum angular deviation (MAD) values generally lower than 5°. Furthermore, ChRM inclinations fluctuate around the expected geocentric axial dipole (GAD) magnetic inclination for the latitude of the coring sites (from 63° to 66°). The similarity of these records on their own independent timescales implies that all of the individual sedimentary sequences record a reliable Holocene PSV record for Eastern Canada. Relative paleointensity (RPI) was estimated by normalizing the NRM by the ARM which provided the best coercivity match. Lastly, the paleomagnetic directional and RPI records were stacked on a common time scale spanning the last ~10 000 cal BP. The smoothed PSV stack reveal centennial- to millennial-scale <span class="hlt">geomagnetic</span> features concordant with the CALS7K.2 time-varying spherical harmonic model, as well as with the US eastern stack (King and Peck, 2001). Comparisons further a field with the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25056214','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25056214"><span><span class="hlt">Geomagnetic</span> imprinting predicts spatio-temporal <span class="hlt">variation</span> in homing migration of pink and sockeye salmon.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Putman, Nathan F; Jenkins, Erica S; Michielsens, Catherine G J; Noakes, David L G</p> <p>2014-10-06</p> <p>Animals navigate using a variety of sensory cues, but how each is weighted during different phases of movement (e.g. dispersal, foraging, homing) is controversial. Here, we examine the <span class="hlt">geomagnetic</span> and olfactory imprinting hypotheses of natal homing with datasets that recorded <span class="hlt">variation</span> in the migratory routes of sockeye (Oncorhynchus nerka) and pink (Oncorhynchus gorbuscha) salmon returning from the Pacific Ocean to the Fraser River, British Columbia. Drift of the magnetic field (i.e. <span class="hlt">geomagnetic</span> imprinting) uniquely accounted for 23.2% and 44.0% of the <span class="hlt">variation</span> in migration routes for sockeye and pink salmon, respectively. Ocean circulation (i.e. olfactory imprinting) predicted 6.1% and 0.1% of the <span class="hlt">variation</span> in sockeye and pink migration routes, respectively. Sea surface temperature (a variable influencing salmon distribution but not navigation, directly) accounted for 13.0% of the <span class="hlt">variation</span> in sockeye migration but was unrelated to pink migration. These findings suggest that <span class="hlt">geomagnetic</span> navigation plays an important role in long-distance homing in salmon and that consideration of navigation mechanisms can aid in the management of migratory fishes by better predicting movement patterns. Finally, given the diversity of animals that use the Earth's magnetic field for navigation, <span class="hlt">geomagnetic</span> drift may provide a unifying explanation for spatio-temporal <span class="hlt">variation</span> in the movement patterns of many species. © 2014 The Author(s) Published by the Royal Society. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70012123','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70012123"><span>Annual and semiannual <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field at equatorial locations</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Campbell, W.H.</p> <p>1981-01-01</p> <p>For a year of quiet solar-activity level, <span class="hlt">geomagnetic</span> records from American hemisphere observatories located between about 0?? and 30?? north <span class="hlt">geomagnetic</span> latitude were used to compare the annual and semiannual <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field associated with three separate contributions: (a) the quiet-day midnight level, MDT; (b) the solar-quiet daily <span class="hlt">variation</span>, Sq; (c) the quiet-time lunar semidiurnal tidal <span class="hlt">variation</span>, L(12). Four Fourier spectral constituents (24, 12, 8, 6 h periods) of Sq were individually treated. All three orthogonal elements (H, D and Z) were included in the study. The MDT changes show a dominant semiannual <span class="hlt">variation</span> having a range of about 7 gammas in H and a dominant annual <span class="hlt">variation</span> in Z having a range of over 8 gammas. These changes seem to be a seasonal response to the nightside distortions by magnetospheric currents. There is a slow decrease in MDT amplitudes with increasing latitude. The Sq changes follow the patterns expected from an equatorial ionospheric dynamo electrojet current system. The dominant seasonal <span class="hlt">variations</span> occur in H having a range of over 21 gammas for the 24 h period and over 12 gammas for the 12 h period spectral components. The higher-order components are relatively smaller in size. The Sq(H) amplitudes decrease rapidly with increasing latitude. Magnetospheric contributions to the equatorial Sq must be less than a few per cent of the observed magnitude. The L(12) <span class="hlt">variation</span> shows the ionospheric electrojet features by the dominance of H and the rapid decrease in amplitude with latitude away from the equator. However, the seasonal <span class="hlt">variation</span> range of over 7 gammas has a maximum in early February and minimum in late June that is not presently explainable by the known ionospheric conductivity and tidal behavior. ?? 1981.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.agu.org/pubs/crossref/2011/2011GL046751.shtml','USGSPUBS'); return false;" href="http://www.agu.org/pubs/crossref/2011/2011GL046751.shtml"><span>Spring-fall asymmetry of substorm strength, <span class="hlt">geomagnetic</span> activity and solar wind: Implications for semiannual <span class="hlt">variation</span> and solar hemispheric asymmetry</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Marsula, K.; Tanskanen, E.; Love, J.J.</p> <p>2011-01-01</p> <p>We study the seasonal <span class="hlt">variation</span> of substorms, <span class="hlt">geomagnetic</span> activity and their solar wind drivers in 1993–2008. The number of substorms and substorm mean duration depict an annual <span class="hlt">variation</span> with maxima in Winter and Summer, respectively, reflecting the annual change of the local ionosphere. In contradiction, substorm mean amplitude, substorm total efficiency and global <span class="hlt">geomagnetic</span> activity show a dominant annual <span class="hlt">variation</span>, with equinoctial maxima alternating between Spring in solar cycle 22 and Fall in cycle 23. The largest annual <span class="hlt">variations</span> were found in 1994 and 2003, in the declining phase of the two cycles when high-speed streams dominate the solar wind. A similar, large annual <span class="hlt">variation</span> is found in the solar wind driver of substorms and <span class="hlt">geomagnetic</span> activity, which implies that the annual <span class="hlt">variation</span> of substorm strength, substorm efficiency and <span class="hlt">geomagnetic</span> activity is not due to ionospheric conditions but to a hemispherically asymmetric distribution of solar wind which varies from one cycle to another. Our results imply that the overall semiannual <span class="hlt">variation</span> in global <span class="hlt">geomagnetic</span> activity has been seriously overestimated, and is largely an artifact of the dominant annual <span class="hlt">variation</span> with maxima alternating between Spring and Fall. The results also suggest an intimate connection between the asymmetry of solar magnetic fields and some of the largest <span class="hlt">geomagnetic</span> disturbances, offering interesting new pathways for forecasting disturbances with a longer lead time to the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034109','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034109"><span>Spring-fall asymmetry of substorm strength, <span class="hlt">geomagnetic</span> activity and solar wind: Implications for semiannual <span class="hlt">variation</span> and solar hemispheric asymmetry</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Mursula, K.; Tanskanen, E.; Love, J.J.</p> <p>2011-01-01</p> <p>We study the seasonal <span class="hlt">variation</span> of substorms, <span class="hlt">geomagnetic</span> activity and their solar wind drivers in 1993-2008. The number of substorms and substorm mean duration depict an annual <span class="hlt">variation</span> with maxima in Winter and Summer, respectively, reflecting the annual change of the local ionosphere. In contradiction, substorm mean amplitude, substorm total efficiency and global <span class="hlt">geomagnetic</span> activity show a dominant annual <span class="hlt">variation</span>, with equinoctial maxima alternating between Spring in solar cycle 22 and Fall in cycle 23. The largest annual <span class="hlt">variations</span> were found in 1994 and 2003, in the declining phase of the two cycles when high-speed streams dominate the solar wind. A similar, large annual <span class="hlt">variation</span> is found in the solar wind driver of substorms and <span class="hlt">geomagnetic</span> activity, which implies that the annual <span class="hlt">variation</span> of substorm strength, substorm efficiency and <span class="hlt">geomagnetic</span> activity is not due to ionospheric conditions but to a hemispherically asymmetric distribution of solar wind which varies from one cycle to another. Our results imply that the overall semiannual <span class="hlt">variation</span> in global <span class="hlt">geomagnetic</span> activity has been seriously overestimated, and is largely an artifact of the dominant annual <span class="hlt">variation</span> with maxima alternating between Spring and Fall. The results also suggest an intimate connection between the asymmetry of solar magnetic fields and some of the largest <span class="hlt">geomagnetic</span> disturbances, offering interesting new pathways for forecasting disturbances with a longer lead time to the future. Copyright ?? 2011 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018DDA....4920103B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018DDA....4920103B"><span>Transit Duration <span class="hlt">Variations</span> due to <span class="hlt">Secular</span> Interactions in Systems with Tightly-packed Inner Planets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boley, Aaron; Van Laerhoven, Christa; Granados Contreras, A. Paula</p> <p>2018-04-01</p> <p><span class="hlt">Secular</span> interactions among planets in multi-planet systems will lead to <span class="hlt">variations</span> in orbital inclinations and to the precession of orbital nodes. Taking known system architectures at face value, we calculate orbital precession rates for planets in tightly-packed systems using classical second-order <span class="hlt">secular</span> theory, in which the orientation of the orbits can be described as a vector sum of eigenmodes and the eigenstructure is determined only by the masses and semi-major axes of the planets. Using this framework, we identify systems that have fast precession frequencies, and use those systems to explore the range of transit duration <span class="hlt">variation</span> that could occur using amplitudes that are consistent with tightly-packed planetary systems. We then further assess how transit duration <span class="hlt">variations</span> could be used in practice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1410478C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1410478C"><span><span class="hlt">Geomagnetic</span> excursions in the Brunhes and Matuyama Chrons: Do they come in bunches?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Channell, J. E. T.</p> <p>2012-04-01</p> <p><span class="hlt">Geomagnetic</span> excursions, defined here as brief directional aberrations of the main dipole field outside the range of expected <span class="hlt">secular</span> <span class="hlt">variation</span>, remain controversial. Poorly-correlated records of apparent excursions from lavas and sediments can often be assigned to sampling artifacts, sedimentological phenomena, volcanic terrane effects, or local <span class="hlt">secular</span> <span class="hlt">variation</span>, rather than behavior of the main dipole field. Although records of magnetic excursions date from the 1960s, the number of Brunhes excursions in recent reviews of the subject have reached the 12-17 range, of which only about ~7 are adequately and/or consistently recorded. For the Matuyama Chron, the current inventory of excursions stands at about 10. The better quality excursion records, with reasonable age control, imply millennial-scale or even sub-millennial-scale durations. When "adequately" recorded, excursions are manifest as paired polarity reversals flanking virtual <span class="hlt">geomagnetic</span> poles (VGPs) that reach high latitudes in the opposite hemisphere. At the young end of the excursion record, the Mono Lake (~33 ka) and Laschamp (~41 ka) excursions are well documented, although records of the former are not widely distributed. Several excursions younger than the Mono Lake excursion (at 17 ka and 25 ka) have recently been recorded in lavas and sediments, respectively. Is the 17-41 ka interval characterized by multiple excursions? Similarly, multiple excursions have been recorded in the 188-238 ka interval that encompasses records of the Iceland Basin excursion (~188 ka) and the Pringle Falls (PF) excursion. The PF excursion has been assigned ages in the 211-238 ka range. Does this mean that this interval is also characterized by several discrete excursions? The 500-600 ka interval incorporates not only the Big Lost excursion at ~565 ka, but also anomalous magnetization directions from lava flows, particularly in the West Eifel volcanics that yield mid-latitude northern-hemisphere VGPs with a range of Ar</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA33B..03S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA33B..03S"><span>Characteristics of seasonal <span class="hlt">variation</span> and solar activity dependence of the <span class="hlt">geomagnetic</span> solar quiet daily <span class="hlt">variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shinbori, A.; Koyama, Y.; Nose, M.; Hori, T.</p> <p>2017-12-01</p> <p>Characteristics of seasonal <span class="hlt">variation</span> and solar activity dependence of the X- and Y-components of the <span class="hlt">geomagnetic</span> solar quiet (Sq) daily <span class="hlt">variation</span> at Memanbetsu in mid-latitudes and Guam near the equator have been investigated using long-term <span class="hlt">geomagnetic</span> field data with 1-h time resolution from 1957 to 2016. In this analysis, we defined the quiet day when the maximum value of the Kp index is less than 3 for that day. In this analysis, we used the monthly average of the adjusted daily F10.7 corresponding to <span class="hlt">geomagnetically</span> quiet days. For identification of the monthly mean Sq <span class="hlt">variation</span> in the X and Y components (Sq-X and Sq-Y), we first determined the baseline of the X and Y components from the average value from 22 to 2 h (LT: local time) for each quiet day. Next, we calculated a deviation from the baseline of the X- and Y-components of the <span class="hlt">geomagnetic</span> field for each quiet day, and computed the monthly mean value of the deviation for each local time. As a result, Sq-X and Sq-Y shows a clear seasonal <span class="hlt">variation</span> and solar activity dependence. The amplitude of seasonal <span class="hlt">variation</span> increases significantly during high solar activities, and is proportional to the solar F10.7 index. The pattern of the seasonal <span class="hlt">variation</span> is quite different between Sq-X and Sq-Y. The result of the correlation analysis between the solar F10.7 index and Sq-X and Sq-Y shows almost the linear relationship, but the slope and intercept of the linear fitted line varies as function of local time and month. This implies that the sensitivity of Sq-X and Sq-Y to the solar activity is different for different local times and seasons. The local time dependence of the offset value of Sq-Y at Guam and its seasonal <span class="hlt">variation</span> suggest a magnetic field produced by inter-hemispheric field-aligned currents (FACs). From the sign of the offset value of Sq-Y, it is infer that the inter-hemispheric FACs flow from the summer to winter hemispheres in the dawn and dusk sectors and from the winter to summer hemispheres in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002PEPI..133..181H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002PEPI..133..181H"><span><span class="hlt">Geomagnetic</span> field model for the last 5 My: time-averaged field and <span class="hlt">secular</span> <span class="hlt">variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hatakeyama, Tadahiro; Kono, Masaru</p> <p>2002-11-01</p> <p>Structure of the <span class="hlt">geomagnetic</span> field has bee studied by using the paleomagetic direction data of the last 5 million years obtained from lava flows. The method we used is the nonlinear version, similar to the works of Gubbins and Kelly [Nature 365 (1993) 829], Johnson and Constable [Geophys. J. Int. 122 (1995) 488; Geophys. J. Int. 131 (1997) 643], and Kelly and Gubbins [Geophys. J. Int. 128 (1997) 315], but we determined the time-averaged field (TAF) and the paleosecular <span class="hlt">variation</span> (PSV) simultaneously. As pointed out in our previous work [Earth Planet. Space 53 (2001) 31], the observed mean field directions are affected by the fluctuation of the field, as described by the PSV model. This effect is not excessively large, but cannot be neglected while considering the mean field. We propose that the new TAF+PSV model is a better representation of the ancient magnetic field, since both the average and fluctuation of the field are consistently explained. In the inversion procedure, we used direction cosines instead of inclinations and declinations, as the latter quantities show singularity or unstable behavior at the high latitudes. The obtained model gives reasonably good fit to the observed means and variances of direction cosines. In the TAF model, the geocentric axial dipole term ( g10) is the dominant component; it is much more pronounced than that in the present magnetic field. The equatorial dipole component is quite small, after averaging over time. The model shows a very smooth spatial <span class="hlt">variation</span>; the nondipole components also seem to be averaged out quite effectively over time. Among the other coefficients, the geocentric axial quadrupole term ( g20) is significantly larger than the other components. On the other hand, the axial octupole term ( g30) is much smaller than that in a TAF model excluding the PSV effect. It is likely that the effect of PSV is most clearly seen in this term, which is consistent with the conclusion reached in our previous work. The PSV</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('http://adsabs.harvard.edu/abs/2017AGUFMSM23A2591C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM23A2591C"><span>Modeling <span class="hlt">Geomagnetic</span> <span class="hlt">Variations</span> using a Machine Learning Framework</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cheung, C. M. M.; Handmer, C.; Kosar, B.; Gerules, G.; Poduval, B.; Mackintosh, G.; Munoz-Jaramillo, A.; Bobra, M.; Hernandez, T.; McGranaghan, R. M.</p> <p>2017-12-01</p> <p>We present a framework for data-driven modeling of Heliophysics time series data. The Solar Terrestrial Interaction Neural net Generator (STING) is an open source python module built on top of state-of-the-art statistical learning frameworks (traditional machine learning methods as well as deep learning). To showcase the capability of STING, we deploy it for the problem of predicting the temporal <span class="hlt">variation</span> of <span class="hlt">geomagnetic</span> fields. The data used includes solar wind measurements from the OMNI database and <span class="hlt">geomagnetic</span> field data taken by magnetometers at US Geological Survey observatories. We examine the predictive capability of different machine learning techniques (recurrent neural networks, support vector machines) for a range of forecasting times (minutes to 12 hours). STING is designed to be extensible to other types of data. We show how STING can be used on large sets of data from different sensors/observatories and adapted to tackle other problems in Heliophysics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004cosp...35.1353D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004cosp...35.1353D"><span>Relationship Between Human Physiological Parameters And <span class="hlt">Geomagnetic</span> <span class="hlt">Variations</span> Of Solar Origin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dimitrova, S.</p> <p></p> <p> <span class="hlt">variations</span> of solar origin. The examinations and analyses performed show that space weather prediction may be utilized for the purpose of pharmacological and regime measures to limit the adverse physiological reactions to <span class="hlt">geomagnetic</span> storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..12210058T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..12210058T"><span>Seasonal <span class="hlt">Variation</span> of High-Latitude <span class="hlt">Geomagnetic</span> Activity in Individual Years</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tanskanen, E. I.; Hynönen, R.; Mursula, K.</p> <p>2017-10-01</p> <p>We study the seasonal <span class="hlt">variation</span> of high-latitude <span class="hlt">geomagnetic</span> activity in individual years in 1966-2014 (solar cycles 20-24) by identifying the most active and the second most active season based on westward electrojet indices AL (1966-2014) and IL (1995-2014). The annual maximum is found at either equinox in two thirds and at either solstice in one third of the years examined. The traditional two-equinox maximum pattern is found in roughly one fourth of the years. We found that the seasonal <span class="hlt">variation</span> of high-latitude <span class="hlt">geomagnetic</span> activity closely follows the solar wind speed. While the mechanisms leading to the two-equinox maxima pattern are in operation, the long-term change of solar wind speed tends to mask the effect of these mechanisms for individual years. Large cycle-to-cycle <span class="hlt">variation</span> is found in the seasonal pattern: equinox maxima are more common during cycles 21 and 22 than in cycles 23 or 24. Exceptionally long winter dominance in high-latitude activity and solar wind speed is seen in the declining phase of cycle 23, after the appearance of the long-lasting low-latitude coronal hole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900039984&hterms=william+scholl&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dwilliam%2Bscholl','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900039984&hterms=william+scholl&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dwilliam%2Bscholl"><span><span class="hlt">Secular</span> resonances. [of asteroidal dynamics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Scholl, H.; Froeschle, CH.; Kinoshita, H.; Yoshikawa, M.; Williams, J. G.</p> <p>1989-01-01</p> <p>Theories and numerical experiments regarding <span class="hlt">secular</span> resonances are reviewed. The basic dynamics and the positions of <span class="hlt">secular</span> resonances are discussed, and <span class="hlt">secular</span> perturbation theories for the nu16 resonance case, the nu6 resonance, and the nu5 resonance are addressed. What numerical experiments have revealed about asteroids located in <span class="hlt">secular</span> resonances, the stability of <span class="hlt">secular</span> resonances, <span class="hlt">variations</span> of eccentricities and inclinations, and chaotic orbits is considered. Resonant transport of meteorites is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EP%26S...62..787F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EP%26S...62..787F"><span>Evaluation of candidate <span class="hlt">geomagnetic</span> field models for IGRF-11</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Finlay, C. C.; Maus, S.; Beggan, C. D.; Hamoudi, M.; Lowes, F. J.; Olsen, N.; Thébault, E.</p> <p>2010-10-01</p> <p>The eleventh generation of the International <span class="hlt">Geomagnetic</span> Reference Field (IGRF) was agreed in December 2009 by a task force appointed by the International Association of <span class="hlt">Geomagnetism</span> and Aeronomy (IAGA) Division V Working Group V-MOD. New spherical harmonic main field models for epochs 2005.0 (DGRF-2005) and 2010.0 (IGRF-2010), and predictive linear <span class="hlt">secular</span> <span class="hlt">variation</span> for the interval 2010.0-2015.0 (SV-2010-2015) were derived from weighted averages of candidate models submitted by teams led by DTU Space, Denmark (team A); NOAA/NGDC, U.S.A. (team B); BGS, U.K. (team C); IZMIRAN, Russia (team D); EOST, France (team E); IPGP, France (team F); GFZ, Germany (team G) and NASA-GSFC, U.S.A. (team H). Here, we report the evaluations of candidate models carried out by the IGRF-11 task force during October/November 2009 and describe the weightings used to derive the new IGRF-11 model. The evaluations include calculations of root mean square vector field differences between the candidates, comparisons of the power spectra, and degree correlations between the candidates and a mean model. Coefficient by coefficient analysis including determination of weighting factors used in a robust estimation of mean coefficients is also reported. Maps of differences in the vertical field intensity at Earth's surface between the candidates and weighted mean models are presented. Candidates with anomalous aspects are identified and efforts made to pinpoint both troublesome coefficients and geographical regions where large <span class="hlt">variations</span> between candidates originate. A retrospective analysis of IGRF-10 main field candidates for epoch 2005.0 and predictive <span class="hlt">secular</span> <span class="hlt">variation</span> candidates for 2005.0-2010.0 using the new IGRF-11 models as a reference is also reported. The high quality and consistency of main field models derived using vector satellite data is demonstrated; based on internal consistency DGRF-2005 has a formal root mean square vector field error over Earth's surface of 1.0 nT. Difficulties</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70014206','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014206"><span>Assessment of models proposed for the 1985 revision of the international <span class="hlt">geomagnetic</span> reference field</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Peddie, N.W.; Zunde, A.K.</p> <p>1987-01-01</p> <p><span class="hlt">Geomagnetic</span> measurements from land, marine and aerial surveys conducted in the years 1945-1964 were used to test the 14 models proposed as additions, for that period, to the series of definitive <span class="hlt">geomagnetic</span> reference field (DGRF) models. Overall, NASA's 'SFAS' models and the BGS (British Geological Survey) models agree best with these data. Comparisons of the two proposed definitive main-field models for 1980.0, with each other and with the existing IGRF 1980 main-field model, show mostly close agreement, with the greatest absolute differences (several tens of nanotesla) occurring in the region of Antarctica. Comparison of the the three proposed forecast <span class="hlt">secular-variation</span> models for 1985-1990 with estimates of recent rates of change at 148 magnetic observatories shows that the IZMIRAN (U.S.S.R.) and USGS models are in closest agreement with these data. ?? 1987.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930037356&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dearths%2Bouter%2Bcore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930037356&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dearths%2Bouter%2Bcore"><span>The steady part of the <span class="hlt">secular</span> <span class="hlt">variation</span> of the Earth's magnetic field</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bloxham, Jeremy</p> <p>1992-01-01</p> <p>The <span class="hlt">secular</span> <span class="hlt">variation</span> of the Earth's magnetic field results from the effects of magnetic induction in the fluid outer core and from the effects of magnetic diffusion in the core and the mantle. Adequate observations to map the magnetic field at the core-mantle boundary extend back over three centuries, providing a model of the <span class="hlt">secular</span> <span class="hlt">variation</span> at the core-mantle boundary. Here we consider how best to analyze this time-dependent part of the field. To calculate steady core flow over long time periods, we introduce an adaptation of our earlier method of calculating the flow in order to achieve greater numerical stability. We perform this procedure for the periods 1840-1990 and 1690-1840 and find that well over 90 percent of the variance of the time-dependent field can be explained by simple steady core flow. The core flows obtained for the two intervals are broadly similar to each other and to flows determined over much shorter recent intervals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ASPC..424...88G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ASPC..424...88G"><span>Analysis of <span class="hlt">Geomagnetic</span> Disturbances and Cosmic Ray Intensity <span class="hlt">Variations</span> in Relation to Medical Data from Rome</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Giannaropoulou, E.; Papailiou, M.; Mavromichalaki, H.; Tsipis, A.</p> <p>2010-07-01</p> <p>Over the last few years many studies have been conducted concerning the possible influence of <span class="hlt">geomagnetic</span> and solar activity and cosmic ray activity on human physiological state and in particular on human cardio - health state. As it is shown the human organism is sensitive to environmental changes and reacts to them through a series of <span class="hlt">variations</span> of its physiological parameters such as heart rate, arterial systolic and diastolic blood pressure, etc. In this paper daily mean values of heart rate, as they were registered for a group of 2.028 volunteers during medical examinations in the Polyclinico Tor Vergata, Rome, Italy are analyzed in relation to daily cosmic ray intensity <span class="hlt">variations</span>, as measured by the Neutron Monitor of the University of Athens and daily <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> indices Dst, Ap and Kp. The results from this study show that <span class="hlt">geomagnetic</span> activity changes and cosmic rays intensity <span class="hlt">variations</span> may regulate the human homeostasis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110012874','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110012874"><span>Effect of Cross-Correlation on <span class="hlt">Geomagnetic</span> Forecast Accuracies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuang, Weijia; Wei, Zigang; Tangborn, Andrew</p> <p>2011-01-01</p> <p>Surface <span class="hlt">geomagnetic</span> observation can determine up to degree L = 14 time-varying spherical harmonic coefficients of the poloidal magnetic field. Assimilation of these coefficients to numerical dynamo simulation could help us understand better the dynamical processes in the Earth's outer core, and to provide more accurate forecast of <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variations</span> (SV). In our previous assimilation studies, only the poloidal magnetic field in the core is corrected by the observations in the analysis. Unobservable core state variables (the toroidal magnetic field and the core velocity field) are corrected via the dynamical equations of the geodynamo. Our assimilation experiments show that the assimilated core state converges near the CMB, implying that the dynamo state is strongly constrained by surface <span class="hlt">geomagnetic</span> observations, and is pulled closer to the truth by the data. We are now carrying out an ensemble of assimilation runs with 1000 years of <span class="hlt">geomagnetic</span> and archeo/paleo magnetic record. In these runs the cross correlation between the toroidal and the poloidal magnetic fields is incorporated into the analysis. This correlation is derived from the physical boundary conditions of the toroidal field at the core-mantle boundary (CMB). The assimilation results are then compared with those of the ensemble runs without the cross-correlation, aiming at understanding two fundamental issues: the effect of the crosscorrelation on (1) the convergence of the core state, and (2) the SV prediction accuracies. The constrained dynamo solutions will provide valuable insights on interpreting the observed SV, e.g. the near-equator magnetic flux patches, the core-mantle interactions, and possibly other geodynamic observables.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EP%26S...55..327Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EP%26S...55..327Y"><span>Rock-magnetic changes with reduction diagenesis in Japan Sea sediments and preservation of <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> in inclination during the last 30,000 years</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yamazaki, T.; Abdeldayem, A. L.; Ikehara, K.</p> <p>2003-06-01</p> <p>A rock-magnetic and paleomagnetic study was conducted on a sediment core of about 4.4 m long taken from the northeastern part of the Japan Sea. The core covers the last about 30 kyrs, which was dated by nineteen radiocarbon (14C) ages. Remanent magnetization is carried dominantly by magnetite. Reductive dissolution of magnetic minerals occurs between 1.2 and 1.6 m in depth (about 5-8 ka in age). A rapid downcore decrease of anhysteretic remanent magnetization (ARM) begins at the shallowest depth. Saturation isothermal remanent magnetization (SIRM) follows, and a decrease of magnetic susceptibility (k) takes place at the deepest. Within this zone, coercivity of natural remanent magnetization (NRM) and the ratios of ARM to k and SIRM to k also decreases with depth. These observations indicate that finer magnetic grains were lost earlier than larger grains. A decrease of S ratios, wasp-waisted hysteresis curves, and a deviation from a mixing trend of single-domain and multi-domain grains in a Day plot occur as the dissolution proceeds, which suggests that high coercivity minerals like hematite are more resistive to dissolution than low coercivity minerals like magnetite. The start of the dissolution at 1.2 m in depth is synchronous with increases in organic-carbon and total-sulfur contents, but the horizon does not coincide with the present Fe-redox boundary at about 0.02 m below the sediment-water interface. From low-temperature magnetometry, it is estimated that magnetites with maghemite skin are reduced to pure magnetites prior to dissolution. There is no evidence for precipitation of secondary magnetic phases and acquisition of chemical remanent magnetization (CRM). Neither pyrrhotite nor greigite was detected. Information of paleomagnetic directions have survived the reductive dissolution. Inclination <span class="hlt">variations</span> of this core resembles closely to the <span class="hlt">secular</span> <span class="hlt">variation</span> records available around Japan. Well-dated records older than 10 ka are still very rare, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013E%26PSL.363..168F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013E%26PSL.363..168F"><span>First archeointensity determinations on Maya incense burners from Palenque temples, Mexico: New data to constrain the Mesoamerica <span class="hlt">secular</span> <span class="hlt">variation</span> curve</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fanjat, G.; Camps, P.; Alva Valdivia, L. M.; Sougrati, M. T.; Cuevas-Garcia, M.; Perrin, M.</p> <p>2013-02-01</p> <p>We present archeointensity data carried out on pieces of incense burners from the ancient Maya city of Palenque, Chiapas, Mexico, covering much of the Mesoamerican Classic period, from A.D. 400 to A.D. 850. We worked on pieces from 24 incense burners encompassing the five Classic ceramic phases of Palenque: Motiepa (A.D. 400-500), Cascadas (A.D. 500-600), Otulum (A.D. 600-700), Murcielagos (A.D. 700-770), and Balunté (A.D. 770-850). All the samples come from highly elaborate, flanged pedestal of incense burners that are undoubtedly assigned to a ceramic phase by means of their iconographic, morphological and stylistic analyses. Archeointensity measurements were performed with the Thellier-Thellier's method on pre-selected samples by means of their magnetic properties. We obtained archeointensities of very good technical quality from 19 of 24 pieces, allowing the determination of a precise mean value for each ceramic phase, between 29.1±0.9 μT and 32.5±1.2 μT. The firing temperatures of ceramics were estimated with Mössbauer spectroscopy between 700 °C and 1000 °C. These values ensure that a full thermo-remanent magnetization was acquired during the original heating. Our results suggest a relative stability of the field intensity during more than 400 years in this area. The abundance of archeological material in Mesoamerica contrasts with the small amount of archeomagnetic data available that are, in addition, of uneven quality. Thus, it is not possible to establish a trend of intensity <span class="hlt">variations</span> in Mesoamerica, even using the global databases and <span class="hlt">secular</span> <span class="hlt">variation</span> predictions from global models. In this context, our high technical quality data represent a strong constraint for the Mesoamerican <span class="hlt">secular</span> <span class="hlt">variation</span> curve during the first millennium AD. The corresponding Virtual Axial Dipole Moments (VADM) are substantially smaller than the ones predicted by the last global <span class="hlt">geomagnetic</span> models CALS3k.4, suggesting the need for additional data to develop a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.T44A..02C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.T44A..02C"><span><span class="hlt">Secular</span> <span class="hlt">Variation</span> in Slip (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cowgill, E.; Gold, R. D.</p> <p>2010-12-01</p> <p>Faults show temporal <span class="hlt">variations</span> in slip rate at time scales ranging from the hours following a major rupture to the millions of years over which plate boundaries reorganize. One such behavior is <span class="hlt">secular</span> <span class="hlt">variation</span> in slip (SVS), which we define as a pulse of accelerated strain release along a single fault that occurs at a frequency that is > 1 order of magnitude longer than the recurrence interval of earthquakes within the pulse. Although numerous mechanical models have been proposed to explain SVS, it has proven much harder to measure long (5-500 kyr) records of fault displacement as a function of time. Such fault-slip histories may be obtained from morphochronologic data, which are measurements of offset and age obtained from faulted landforms. Here we describe slip-history modeling of morphochronologic data and show how this method holds promise for obtaining long records of fault slip. In detail we place SVS in the context of other types of time-varying fault-slip phenomena, explain the importance of measuring fault-slip histories, summarize models proposed to explain SVS, review current approaches for measuring SVS in the geologic record, and illustrate the slip-history modeling approach we advocate here using data from the active, left-slip Altyn Tagh fault in NW Tibet. In addition to SVS, other types of temporal <span class="hlt">variation</span> in fault slip include post-seismic transients, discrepancies between geologic slip rates and those derived from geodetic and/or paleoseismic data, and single changes in slip rate resulting from plate reorganization. Investigating <span class="hlt">secular</span> <span class="hlt">variation</span> in slip is important for advancing understanding of long-term continental deformation, fault mechanics, and seismic risk. Mechanical models producing such behavior include self-driven mode switching, changes in pore-fluid pressure, viscoelasticity, postseismic reloading, and changes in local surface loads (e.g., ice sheets, large lakes, etc.) among others. However, a key problem in testing these</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..12210796S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..12210796S"><span>Characteristics of Seasonal <span class="hlt">Variation</span> and Solar Activity Dependence of the <span class="hlt">Geomagnetic</span> Solar Quiet Daily <span class="hlt">Variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shinbori, Atsuki; Koyama, Yukinobu; Nosé, Masahito; Hori, Tomoaki; Otsuka, Yuichi</p> <p>2017-10-01</p> <p>Characteristics of seasonal <span class="hlt">variation</span> and solar activity dependence of the X and Y components of the <span class="hlt">geomagnetic</span> solar quiet (Sq) daily <span class="hlt">variation</span> at Memambetsu in midlatitudes and Guam near the equator have been investigated using long-term <span class="hlt">geomagnetic</span> field data with 1 h time resolution from 1957 to 2016. The monthly mean Sq <span class="hlt">variation</span> in the X and Y components (Sq-X and Sq-Y) shows a clear seasonal <span class="hlt">variation</span> and solar activity dependence. The amplitude of seasonal <span class="hlt">variation</span> increases significantly during high solar activities and is proportional to the solar F10.7 index. The pattern of the seasonal <span class="hlt">variation</span> is quite different between Sq-X and Sq-Y. The result of the correlation analysis between the solar F10.7 index and the Sq-X and Sq-Y shows an almost linear relationship, but the slope of the linear fitted line varies as a function of local time and month. This implies that the sensitivity of Sq-X and Sq-Y to the solar activity is different for different local times and seasons. The pattern of the local time and seasonal <span class="hlt">variations</span> of Sq-Y at Guam shows good agreement with that of a magnetic field produced by interhemispheric field-aligned currents (FACs), which flow from the summer to winter hemispheres in the dawn and dusk sectors and from the winter to summer hemispheres in the prenoon to afternoon sectors. The direction of the interhemispheric FAC in the dusk sector is opposite to the concept of Fukushima's model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.3681C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.3681C"><span>Solar and <span class="hlt">Geomagnetic</span> Activity <span class="hlt">Variations</span> Correlated to Italian M6+ Earthquakes Occurred in 2016</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cataldi, Gabriele; Cataldi, Daniele; Straser, Valentino</p> <p>2017-04-01</p> <p>Between August 2016 and October 2016 in Italy were recorded three strong earthquakes: M6.2 on August 2016 at 01:36:32 UTC; M6.1 on October 26, 2016 at 19:18:08 UTC and M6,6 on October 30, 2016 at 06:40:18 UTC. The authors of this study wanted to verify the existence of a correlation between these earthquakes and solar/<span class="hlt">geomagnetic</span> activity. To confirming or not the presence of this kind of correlation, the authors analyzed the conditions of Spaceweather "near Earth" and the characteristics of the Earth's <span class="hlt">geomagnetic</span> field in the hours that preceded the three earthquakes. The data relating to the three earthquakes were provided by the United States Geological Survey (USGS). The data on ion density used to realize the correlation study are represented by: solar wind ion density <span class="hlt">variation</span> detected by ACE (Advanced Composition Explorer) Satellite, in orbit near the L1 Lagrange point, at 1.5 million of km from Earth, in direction of the Sun. The instrument used to perform the measurement of the solar wind ion density is the Electron, Proton, and Alpha Monitor (EPAM) instrument, equipped on the ACE Satellite. To conduct the study, the authors have taken in consideration the <span class="hlt">variation</span> of the solar wind protons density of three different energy fractions: differential proton flux 1060-1900 keV (p/cm^2-sec-ster-MeV); differential proton flux 761-1220 keV (p/cm^2-sec-ster-MeV); differential proton flux 310-580 keV (p/cm^2-sec-ster-MeV). <span class="hlt">Geomagnetic</span> activity data were provided by Tromsø <span class="hlt">Geomagnetic</span> Observatory (TGO), Norway; by Scoresbysund <span class="hlt">Geomagnetic</span> Observatory (SCO), Greenland, Denmark; Dikson <span class="hlt">Geomagnetic</span> Observatory (DIK), Russia and by Pushkov Institute of terrestrial magnetism, ionosphere and radio wave propagation (IZMIRAN), Troitsk, Moscow Region. The results of the study, in agreement with what already ascertained by authors from 2012, have confirmed that the three strong Italian earthquakes were preceded by a clear increase of the solar wind proton density which</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930017232','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930017232"><span>Steady induction effects in <span class="hlt">geomagnetism</span>. Part 1B: <span class="hlt">Geomagnetic</span> estimation of steady surficial core motions: A non-linear inverse problem</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Voorhies, Coerte V.</p> <p>1993-01-01</p> <p>The problem of estimating a steady fluid velocity field near the top of Earth's core which induces the <span class="hlt">secular</span> <span class="hlt">variation</span> (SV) indicated by models of the observed <span class="hlt">geomagnetic</span> field is examined in the source-free mantle/frozen-flux core (SFI/VFFC) approximation. This inverse problem is non-linear because solutions of the forward problem are deterministically chaotic. The SFM/FFC approximation is inexact, and neither the models nor the observations they represent are either complete or perfect. A method is developed for solving the non-linear inverse motional induction problem posed by the hypothesis of (piecewise, statistically) steady core surface flow and the supposition of a complete initial <span class="hlt">geomagnetic</span> condition. The method features iterative solution of the weighted, linearized least-squares problem and admits optional biases favoring surficially geostrophic flow and/or spatially simple flow. Two types of weights are advanced radial field weights for fitting the evolution of the broad-scale portion of the radial field component near Earth's surface implied by the models, and generalized weights for fitting the evolution of the broad-scale portion of the scalar potential specified by the models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995JGR...10024393H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995JGR...10024393H"><span>Late quaternary <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> from historical and 14C-dated lava flows on Hawaii</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hagstrum, Jonathan T.; Champion, Duane E.</p> <p>1995-12-01</p> <p>A paleomagnetic record of <span class="hlt">geomagnetic</span> paleosecular <span class="hlt">variation</span> (PSV) is constructed for the last 4400 years based on 191 sites in historical and 14C-dated lava flows from Mauna Loa, Kilauea, and Hualalai Volcanoes on the island of Hawaii. The features of this new record are similar to those recorded by sediments from Lake Waiau near the summit of Mauna Kea Volcano, but overall mean inclinations for the lava flows (31° to 33°, depending on window size) are nearer the expected dipole-field value (35°) than is that for the sediments (27°). Divergence of the inclination records with increasing age suggests that the Lake Waiau values at depths below 2 m have been affected by compaction-related inclination shallowing, although magnetic terrain effects cannot be ruled out. The rate of PSV indicated by the record presented here is highly variable (<0.5°/century to >20°/century), and a pronounced shift in inclination from 25° to 40° occurred between ~1030 and ~975 years B.P. Paleomagnetic directions from undated materials can be correlated with our calibrated curve, but the resolution is largely dependent on the PSV rate and data densities for both the reference and unknown directions. The upper part of the Puna Basalt (18 lava flows), previously sampled for paleomagnetism along the northern wall of Kilauea's caldera (Uwekahuna Bluff), was likely deposited sometime between 1030 and 750 years B.P., but the lowest two flows beneath the Uwekahuna Ash (~2100 years B.P.) are correlated with an age of ~3034 years B.P. Paleomagnetic data for 54 lava flows of the Ka'u Basalt, exposed in the northwest wall of Mauna Loa's summit caldera (Mokuaweoweo), indicate that they probably accumulated over a relatively short time interval (~200+years) and are assigned to a 1000 to 1199 year B.P. time window. The mean of ages within this window is ~1030 years B.P., but mapping and other 14C dates indicate that these summit overflows are probably closer to ~1200 years B.P. in age.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23038471','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23038471"><span>Dynamical similarity of <span class="hlt">geomagnetic</span> field reversals.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Valet, Jean-Pierre; Fournier, Alexandre; Courtillot, Vincent; Herrero-Bervera, Emilio</p> <p>2012-10-04</p> <p>No consensus has been reached so far on the properties of the <span class="hlt">geomagnetic</span> field during reversals or on the main features that might reveal its dynamics. A main characteristic of the reversing field is a large decrease in the axial dipole and the dominant role of non-dipole components. Other features strongly depend on whether they are derived from sedimentary or volcanic records. Only thermal remanent magnetization of lava flows can capture faithful records of a rapidly varying non-dipole field, but, because of episodic volcanic activity, sequences of overlying flows yield incomplete records. Here we show that the ten most detailed volcanic records of reversals can be matched in a very satisfactory way, under the assumption of a common duration, revealing common dynamical characteristics. We infer that the reversal process has remained unchanged, with the same time constants and durations, at least since 180 million years ago. We propose that the reversing field is characterized by three successive phases: a precursory event, a 180° polarity switch and a rebound. The first and third phases reflect the emergence of the non-dipole field with large-amplitude <span class="hlt">secular</span> <span class="hlt">variation</span>. They are rarely both recorded at the same site owing to the rapidly changing field geometry and last for less than 2,500 years. The actual transit between the two polarities does not last longer than 1,000 years and might therefore result from mechanisms other than those governing normal <span class="hlt">secular</span> <span class="hlt">variation</span>. Such changes are too brief to be accurately recorded by most sediments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFMGP51A0286D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFMGP51A0286D"><span><span class="hlt">Geomagnetic</span> Paleointensity <span class="hlt">Variations</span> as a Cheap, High-Resolution Geochronometer for Recent Mid-Ocean Ridge Processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>DYMENT, J.; HEMOND, C.</p> <p>2001-12-01</p> <p>The sequence of <span class="hlt">geomagnetic</span> field reversals is widely used to date events younger than 160 Ma, with a resolution of a million years. In oceanic domains, Vine and Matthews (1963) magnetic anomalies have been successfully used for more than 35 years. The major limitation of this chronometer is its low temporal resolution, especially for the recent times: the youngest polarity reversal, between Brunhes normal and Matuyama reversed periods, is dated ~800 ka. Studies of pelagic sedimentary cores have shown the existence of consistent <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field intensity within this period. If accurately dated, these <span class="hlt">variations</span> may refine the magnetic geochronometer to a much higher resolution of 10-100 ka. Recent studies have demonstrated that the "tiny wiggles" of lower amplitude and shorter wavelength superimposed to the Vine and Matthews anomalies are of <span class="hlt">geomagnetic</span> origin and correspond to the paleointensity <span class="hlt">variations</span> identified on sediment cores. Using a large set of magnetic data acquired in 1996 on the Mid-Atlantic Ridge at 21° N (surface and submersible magnetic anomalies, natural remanent magnetization and absolute paleointensities measured on samples), we have shown that the oceanic crust confidently records the <span class="hlt">geomagnetic</span> intensity <span class="hlt">variations</span>. It was unfortunately impossible to date the samples, made of basalt too depleted in K2O and in trace elements required by the various methods of radiochronology. In 2000 we have collected a similar data set at the Central Indian Ridge axis at 19° S (surface, deep-tow, and submersible magnetic anomalies, natural remanent magnetization and absolute paleointensities measured on samples). This area offers the advantages of 1) a faster spreading rate, and therefore a higher temporal resolution of the <span class="hlt">geomagnetic</span> signal, and 2) the presence of moderately enriched basalt as a consequence of the interaction of the ridge with the nearby Reunion hotspot, making possible radiochronologic dating. Our first evaluation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70014510','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014510"><span>Comments on 'Remarks on the <span class="hlt">secular</span> change in the energy density spectrum of the <span class="hlt">geomagnetic</span> field' by Joachim Meyer.</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Alldredge, L.R.</p> <p>1986-01-01</p> <p>Meyer has discussed only the Rn aspect of the Alldredge (1984) paper he is criticising. He has ignored the pictorial demonstration of the need for higher harmonics to properly describe the <span class="hlt">secular</span> <span class="hlt">variation</span> field than the main field as demonstrated. This more or less independent demonstration supports the general conclusion of that paper. -from Author</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850026773','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850026773"><span>Estimating the change in asymptotic direction due to <span class="hlt">secular</span> changes in the <span class="hlt">geomagnetic</span> field</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Flueckiger, E. O.; Smart, D. F.; Shea, M. A.; Gentile, L. C.; Bathurat, A. A.</p> <p>1985-01-01</p> <p>The concept of <span class="hlt">geomagnetic</span> optics, as described by the asymptotic directions of approach, is extremely useful in the analysis of cosmic radiation data. However, when changes in cutoff occur as a result of evolution in the <span class="hlt">geomagnetic</span> field, there are corresponding changes in the asymptotic cones of acceptance. A method is introduced of estimating the change in the asymptotic direction of approach for vertically incident cosmic ray particles from a reference set of directions at a specific epoch by considering the change in the <span class="hlt">geomagnetic</span> cutoff.</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/2016AGUFMGP24E..03P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGP24E..03P"><span>Eliminating large-scale magnetospheric current perturbations from long-term <span class="hlt">geomagnetic</span> observatory data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pick, L.; Korte, M. C.</p> <p>2016-12-01</p> <p>Magnetospheric currents generate the largest external contribution to the <span class="hlt">geomagnetic</span> field observed on Earth. Of particular importance is the solar-driven effect of the ring current whose fluctuations overlap with internal field <span class="hlt">secular</span> <span class="hlt">variation</span> (SV). Recent core field models thus co-estimate this effect but their validity is limited to the last 15 years offering satellite data. We aim at eliminating magnetospheric modulation from the whole <span class="hlt">geomagnetic</span> observatory record from 1840 onwards in order to obtain clean long-term SV that will enhance core flow and geodynamo studies.The ring current effect takes form of a southward directed external dipole field aligned with the <span class="hlt">geomagnetic</span> main field axis. Commonly the Dst index (Sugiura, 1964) is used to parametrize temporal <span class="hlt">variations</span> of this dipole term. Because of baseline instabilities, the alternative RC index was derived from hourly means of 21 stations spanning 1997-2013 (Olsen et al., 2014). We follow their methodology based on annual means from a reduced station set spanning 1960-2010. The absolute level of the <span class="hlt">variation</span> so determined is "hidden" in the static lithospheric offsets taken as quiet-time means. We tackle this issue by subtracting crustal biases independently calculated for each observatory from an inversion of combined Swarm satellite and observatory data.Our index reproduces the original annual RC index variability with a reasonable offset of -10 nT in the reference time window 2000-2010. Prior to that it depicts a long-term trend consistent with the external dipole term from COV-OBS (Gillet et al., 2013), being the only long-term field model available for comparison. Sharper <span class="hlt">variations</span> that are better correlated with the Ap index than the COV-OBS solution lend support to the usefulness of our initial modeling approach. Following a detailed sensitivity study of station choice future work will focus on increasing the resolution from annual to hourly means.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMGP53A3757I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMGP53A3757I"><span>Spherical Cap Harmonic Modelling of 400 Years of <span class="hlt">Secular</span> <span class="hlt">Variation</span> in the South-west Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ingham, M.; Alfheid, M.; Ingham, E. M.; Turner, G. M.</p> <p>2014-12-01</p> <p>Historical magnetic data recorded in ship's logs on voyages of exploration and trade in the south-west Pacific have been used as a basis for constructing a model of <span class="hlt">secular</span> <span class="hlt">variation</span> in the region using spherical cap harmonic (SCH) analysis. The spherical cap used is centred on colatitude 115° and longitude 160° and has a radius of 50°, thus covering New Zealand, Australia and parts of Antarctica. Gaps in the observational data have been filled by an iterative procedure started by using IGRF field values to obtain SCH models for 2000, 1950 and 1900 and assuming that the spherical cap coefficients have a linear <span class="hlt">variation</span> in time over the 400 year time period of the model, as is observed to a first approximation for Gauss coefficients calculated from a global spherical harmonic analysis. The resulting field models have generally smooth spatial and temporal <span class="hlt">variations</span> in declination, inclination and intensity which show some differences from the <span class="hlt">variations</span> calculated using the global spherical harmonic model gufm1. The technique clearly shows promise for producing more refined models of <span class="hlt">secular</span> <span class="hlt">variation</span> in the south-west Pacific when the historical data are supplemented by archeomagnetic and paleomagnetic data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFMSA21B0434L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFMSA21B0434L"><span>SAMPEX Measurements of <span class="hlt">Geomagnetic</span>-Cutoff <span class="hlt">Variations</span> During the 4/21/02 Solar Energetic Particle Event</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Labrador, A.; Leske, R.; Kanekal, S.; Klecker, B.; Looper, M.; Mazur, J.; Mewaldt, R.</p> <p>2002-12-01</p> <p>During large solar energetic particle (SEP) events the entry of solar and interplanetary energetic particles into the upper atmosphere is controlled by the <span class="hlt">geomagnetic</span> cutoff. We define the cutoff latitude (Λ c) for a given rigidity particle to be effectively the minimum invariant latitude down to which particles can reach the upper atmosphere. The instruments on the polar-orbiting SAMPEX spacecraft have been used to measure <span class="hlt">geomagnetic</span> cutoffs during a large sample of SEP events from solar cycle 23. During those events in which there is an associated <span class="hlt">geomagnetic</span> storm, there are often large cutoff <span class="hlt">variations</span> of as much as 5° to 10° in invariant latitude over the course of the event. This paper will combine measurements from the HILT, MAST, and PET instruments on SAMPEX to provide a comprehensive view of <span class="hlt">geomagnetic</span> cutoff <span class="hlt">variations</span> during the large SEP event of 4/21/02. We find that during the first two days of the event the cutoff latitude for ~30 MeV protons was at typical quiet-time levels. On April 23, following the arrival of a strong interplanetary shock, there was a sudden drop in the cutoff that lasted ~12 hours, with sizable local-time differences. During the next two days the cutoff steadily increased, giving a total <span class="hlt">variation</span> of ~5° over the five days of the event. We combine these measurements of cutoff <span class="hlt">variations</span> with measurements of the composition and energy spectra in the 4/21/02 event in order to estimate changes in the area of the polar caps over which particles of a given rigidity had access to the upper atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSH51B4158K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSH51B4158K"><span>Nonlinear Behavior of the <span class="hlt">Geomagnetic</span> Fluctuations Recorded in Different <span class="hlt">Geomagnetic</span> Latitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kovacs, P.; Heilig, B.; Koppan, A.; Vadasz, G.; Echim, M.</p> <p>2014-12-01</p> <p>The paper concerns with the nonlinear properties of <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> recorded in different <span class="hlt">geomagnetic</span> latitudes, in the years of solar maximum and minimum. For the study, we use the <span class="hlt">geomagnetic</span> time-series recorded by some of the stations of the EMMA quasi-meridional magnetometer network, established for pulsation study, in September 2001. The stations are located approx. along the magnetic meridian of 100 degree, and the sampling frequency of the series is 1 Hz. It is argued that the <span class="hlt">geomagnetic</span> field exhibits nonlinear intermittent fluctuations in certain temporal scale range. For quantitatively investigating the scaling ranges and the <span class="hlt">variation</span> of intermittent properties with latitude and time, we analyse the higher order moments of the time records (probability density function or structure function analyses). The multifractal or self-similar scaling of the fluctuations is investigated via the fitting of the P model to structure function scaling exponents. We also study the power-law behaviour of the power-spectral density functions of the series in order to evaluate the possible inertial frequency (and temporal) range of the <span class="hlt">geomagnetic</span> field and compare them with the scaling ranges of structure functions. The range where intermittent <span class="hlt">geomagnetic</span> <span class="hlt">variation</span> is found falls typically between 100 and 20.000 s, i.e. covers the temporal range of the main phases of <span class="hlt">geomagnetic</span> storms. It is shown that the intensity of intermittent fluctuations increases from solar minimum to solar maximum. The expected increase in the level of intermittency with the <span class="hlt">geomagnetic</span> latitude can be evidenced only in the years of solar minimum. The research leading to these results has received funding from the European Community's Seventh Framework Programme ([FP7/2007-2013]) under grant agreement n° 313038/STORM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013GeoJI.192..537A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013GeoJI.192..537A"><span>Flow throughout the Earth's core inverted from <span class="hlt">geomagnetic</span> observations and numerical dynamo models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aubert, Julien</p> <p>2013-02-01</p> <p>This paper introduces inverse geodynamo modelling, a framework imaging flow throughout the Earth's core from observations of the <span class="hlt">geomagnetic</span> field and its <span class="hlt">secular</span> <span class="hlt">variation</span>. The necessary prior information is provided by statistics from 3-D and self-consistent numerical simulations of the geodynamo. The core method is a linear estimation (or Kalman filtering) procedure, combined with standard frozen-flux core surface flow inversions in order to handle the non-linearity of the problem. The inversion scheme is successfully validated using synthetic test experiments. A set of four numerical dynamo models of increasing physical complexity and similarity to the <span class="hlt">geomagnetic</span> field is then used to invert for flows at single epochs within the period 1970-2010, using data from the <span class="hlt">geomagnetic</span> field models CM4 and gufm-sat-Q3. The resulting core surface flows generally provide satisfactory fits to the <span class="hlt">secular</span> <span class="hlt">variation</span> within the level of modelled errors, and robustly reproduce the most commonly observed patterns while additionally presenting a high degree of equatorial symmetry. The corresponding deep flows present a robust, highly columnar structure once rotational constraints are enforced to a high level in the prior models, with patterns strikingly similar to the results of quasi-geostrophic inversions. In particular, the presence of a persistent planetary scale, eccentric westward columnar gyre circling around the inner core is confirmed. The strength of the approach is to uniquely determine the trade-off between fit to the data and complexity of the solution by clearly connecting it to first principle physics; statistical deviations observed between the inverted flows and the standard model behaviour can then be used to quantitatively assess the shortcomings of the physical modelling. Such deviations include the (i) westwards and (ii) hemispherical character of the eccentric gyre. A prior model with angular momentum conservation of the core-mantle inner-core system, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910031753&hterms=earths+outer+core&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dearths%2Bouter%2Bcore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910031753&hterms=earths+outer+core&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dearths%2Bouter%2Bcore"><span>On the consequences of strong stable stratification at the top of earth's outer core</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bloxham, Jeremy</p> <p>1990-01-01</p> <p>The consequences of strong stable stratification at the top of the earth's fluid outer core are considered, concentrating on the generation of the <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span>. It is assumed that the core near the core-mantle boundary is both strongly stably stratified and free of Lorentz forces: it is found that this set of assumptions severely limits the class of possible motions, none of which is compatible with the <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span>. Relaxing either assumption is adequate: tangentially geostrophic flows are consistent with the <span class="hlt">secular</span> <span class="hlt">variation</span> if the assumption that the core is strongly stably stratified is relaxed (while retaining the assumption that Lorentz forces are negligible); purely toroidal flows may explain the <span class="hlt">secular</span> <span class="hlt">variation</span> if Lorentz forces are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018FrEaS...6...17K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018FrEaS...6...17K"><span>Archeomagnetic intensity spikes: global or regional <span class="hlt">geomagnetic</span> field features?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Korte, Monika; Constable, Catherine G.</p> <p>2018-03-01</p> <p><span class="hlt">Variations</span> of the <span class="hlt">geomagnetic</span> field prior to direct observations are inferred from archeo- and paleomagnetic experiments. Seemingly unusual <span class="hlt">variations</span> not seen in the present day and historical field are of particular interest to constrain the full range of core dynamics. Recently, archeomagnetic intensity spikes, characterised by very high field values that appear to be associated with rapid <span class="hlt">secular</span> <span class="hlt">variation</span> rates, have been reported from several parts of the world. They were first noted in data from the Levant at around 900 BCE. A recent re-assessment of previous and new Levantine data, involving a rigorous quality assessment, interprets the observations as an extreme local <span class="hlt">geomagnetic</span> high with at least two intensity spikes between the 11^{th} and 8^{th} centuries BCE. Subsequent reports of similar features from Asia, the Canary Islands and Texas raise the question of whether such features might be common occurrences, or whether they might even be part of a global magnetic field feature. Here we use spherical harmonic modelling to test two hypotheses: firstly, whether the Levantine and other potential spikes might be associated with higher dipole field intensity than shown by existing global field models around 1000 BCE, and secondly, whether the observations from different parts of the world are compatible with a westward drifting intense flux patch. Our results suggest that the spikes originate from intense flux patches growing and decaying mostly in situ, combined with stronger and more variable dipole moment than shown by previous global field models. Axial dipole <span class="hlt">variations</span> no more than 60% higher than observed in the present field, probably within the range of normal geodynamo behaviour, seem sufficient to explain the observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AIPC.1203..748P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AIPC.1203..748P"><span>Analysis of Changes of Cardiological Parameters at Middle Latitude Region in Relation to <span class="hlt">Geomagnetic</span> Disturbances and Cosmic Ray <span class="hlt">Variations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Papailiou, M.; Dimitrova, S.; Babayev, E. S.; Mavromichalaki, H.</p> <p>2010-01-01</p> <p>Collaborating scientific groups from Athens (Greece), Baku (Azerbaijan) and Sofia (Bulgaria) have conducted a research work on the possible effects of <span class="hlt">geomagnetic</span> field disturbances (GMF) and cosmic ray intensity (CRI) <span class="hlt">variations</span> on human homeostasis, particularly, the cardio-health state. Electrocardiograms (ECGs) of seven functionally healthy persons were digitally registered at the joint Laboratory of Heliobiology located in the Medical Centre INAM, Baku, on working days and Saturdays. Heart rate values, estimated from ECGs, were analysed in relation to daily values of CRI, as measured by the Neutron Monitor of the University of Athens and daily <span class="hlt">variations</span> of Dst and Ap <span class="hlt">geomagnetic</span> indices and some significant results had been revealed in previous studies. Researches were continued by study of additional cardiologic parameters estimated from the same ECG data. In this study digital data of RR interval (the time elapsing between two consecutive R waves in the ECG), namely RRminimum, RRmaximum and RRaverage were analyzed taking into consideration different levels of GMF disturbances (estimated through <span class="hlt">variations</span> of Dst and Ap indices) and cosmic ray activity (through CRI <span class="hlt">variations</span>). The data refer to the time period 15 July 2006-31 March 2008. <span class="hlt">Variations</span> of RR intervals show connection to GMF disturbances and CRI <span class="hlt">variations</span>. The revealed effects are more pronounced for high levels of <span class="hlt">geomagnetic</span> activity (when <span class="hlt">geomagnetic</span> storms occur) and large CRI decreases as well as on the days before and after these <span class="hlt">variations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/3982943','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/3982943"><span>Geophysical variables and behavior: XXI. <span class="hlt">Geomagnetic</span> <span class="hlt">variation</span> as possible enhancement stimuli for UFO reports preceding earthtremors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Persinger, M A</p> <p>1985-02-01</p> <p>The contribution of <span class="hlt">geomagnetic</span> <span class="hlt">variation</span> to the occurrence of UFORs (reports of UFOs) within the New Madrid States during the 6-mo. increments before increases in the numbers of IV-V or less intensity earthquakes within the central USA was determined. Although statistically significant zero-order correlations existed between measures of earthquakes, UFORs and <span class="hlt">geomagnetic</span> variability, the association between the latter two deteriorated markedly when their shared variance with earthquakes was held constant. These outcomes are compatible with the hypothesis that <span class="hlt">geomagnetic</span> variability (or phenomena associated with it) may enhance UFORs but only if tectonic stress and strain are increasing within the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUSMGP14A..02K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUSMGP14A..02K"><span>Torque Balances on the Taylor Cylinders in the <span class="hlt">Geomagnetic</span> Data Assimilation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuang, W.; Tangborn, A.</p> <p>2004-05-01</p> <p>In this presentation we report on our continuing effort in <span class="hlt">geomagnetic</span> data assimilation, aiming at understanding and predicting <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> on decadal time scales. In particular, we focus on the effect of the torque balances on the cylindrical surfaces in the core co-axial with the Earth's rotation axis (the Taylor cylinders) on the time evolution of assimilated solutions. We use our MoSST core dynamics model and observed <span class="hlt">geomagnetic</span> field at the Earth's surface derived via Comprehensive Field Model (CFM) for the <span class="hlt">geomagnetic</span> data assimilation. In our earlier studies, a model solution is selected randomly from our numerical database. It is then assimilated with the observations such that the poloidal field possesses the same field tomography on the core-mantel boundary (CMB) continued downward from surface observations. This tomography change is assumed to be effective through out the outer core. While this approach allows rapid convergence between model solutions and the observations, it also generates sever numerical instabilities: the delicate balance between weak fluid inertia and the magnetic torques on the Taylor cylinders are completely altered. Consequently, the assimilated solution diverges quickly (in approximately 10% of the magnetic free-decay time in the core). To improve the assimilation, we propose a partial penetration of the assimilation from the CMB: The full-scale modification at the CMB decreases linearly and vanish at an interior radius ra. We shall examine from our assimilation tests possible relationships between the convergence rate of the model solutions to observations and the cut-off radius ra. A better assimilation shall serve our nudging tests in near future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JASTP.171..164H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JASTP.171..164H"><span>Influences of CO2 increase, solar cycle <span class="hlt">variation</span>, and <span class="hlt">geomagnetic</span> activity on airglow from 1960 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>Huang, Tai-Yin</p> <p>2018-06-01</p> <p><span class="hlt">Variations</span> of airglow intensity, Volume Emission Rate (VER), and VER peak height induced by the CO2 increase, and by the F10.7 solar cycle <span class="hlt">variation</span> and <span class="hlt">geomagnetic</span> activity were investigated to quantitatively assess their influences on airglow. This study is an extension of a previous study by Huang (2016) covering a time period of 55 years from 1960 to 2015 and includes <span class="hlt">geomagnetic</span> variability. Two airglow models, OHCD-90 and MACD-90, are used to simulate the induced <span class="hlt">variations</span> of O(1S) greenline, O2(0,1) atmospheric band, and OH(8,3) airglow for this study. Overall, our results demonstrate that airglow intensity and the peak VER <span class="hlt">variations</span> of the three airglow emissions are strongly correlated, and in phase, with the F10.7 solar cycle <span class="hlt">variation</span>. In addition, there is a linear trend, be it increasing or decreasing, existing in the airglow intensities and VERs due to the CO2 increase. On other hand, airglow VER peak heights are strongly correlated, and out of phase, with the Ap index <span class="hlt">variation</span> of <span class="hlt">geomagnetic</span> activity. The CO2 increase acts to lower the VER peak heights of OH(8,3) airglow and O(1S) greenline by 0.2 km in 55 years and it has no effect on the VER peak height of O2(0,1) atmospheric band.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002JASTP..64.1667S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002JASTP..64.1667S"><span>Comment on ``Annual <span class="hlt">variation</span> of <span class="hlt">geomagnetic</span> activity'' by Alicia L. Clúa de Gonzales et al.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sonnemann, G. R.</p> <p>2002-10-01</p> <p>Clúa de Gonzales et al. (J. Atmos. Terr. Phys. 63 (2001) 367) analyzed the monthly means of the <span class="hlt">geomagnetic</span> /aa-index available since 1868 and found enhanced <span class="hlt">geomagnetic</span> activity in July outside of the known seasonal course of semiannual <span class="hlt">variation</span>. They pointed out that this behavior is mainly caused by the high values of the <span class="hlt">geomagnetic</span> activity. Their analysis confirmed results obtained from an analysis of Ap-values nearly 30 years ago but widely unknown to the scientific community. At that time the entire year was analyzed using running means of the activity values averaged to the same date. Aside from the July period, the calculations revealed distinct deviations from the seasonal course-called <span class="hlt">geomagnetic</span> singularities. The most marked singularity occurs from the middle of March to the end of March characterized by a strong increase from, on average, relatively calm values to the actually strongest ones during the entire year. Some typical time patterns around and after equinox are repeated half a year later. An analysis in 1998 on the basis of the available /aa-values confirmed the findings derived from Ap-values and the local activity index Ak from Niemegk, Germany available since 1890. The new results will be presented and discussed. Special attention is paid to the statistical problem of the persistence of <span class="hlt">geomagnetic</span> perturbations. The main problem under consideration is that the <span class="hlt">variation</span> of the mean activity is not caused by an accidental accumulation of strong perturbations occurring within certain intervals of days. We assume that the most marked <span class="hlt">variations</span> of the mean value are not accidental and result from internal processes within the earth's atmosphere but different, particularly small-scale features, are most probably accidental.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9292E..59S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9292E..59S"><span>Active experiments in the ionosphere and <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sivokon, V. P.; Cherneva, N. V.; Khomutov, S. Y.; Serovetnikov, A. S.</p> <p>2014-11-01</p> <p><span class="hlt">Variations</span> of ionospheric-magnetospheric relation energy, as one of the possible outer climatology factors, may be traced on the basis of analysis of natural geophysical phenomena such as ionosphere artificial radio radiation and magnetic storms. Experiments on active impact on the ionosphere have been carried out for quite a long time in Russia as well. The most modern heating stand is located in Alaska; it has been used within the HAARP Program. The possibility of this stand to affect geophysical fields, in particular, the <span class="hlt">geomagnetic</span> field is of interest.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4800496','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4800496"><span>Palaeomagnetism of the Upper Miocene- Lower Pliocene lavas from the East Carpathians: contribution to the paleosecular <span class="hlt">variation</span> of <span class="hlt">geomagnetic</span> field</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Vişan, Mădălina; Panaiotu, Cristian G.; Necula, Cristian; Dumitru, Anca</p> <p>2016-01-01</p> <p>Investigations of the paleosecular <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field on geological timescales depend on globally distributed data sets from lava flows. We report new paleomagnetic results from lava flows of the East Carpathian Mountains (23.6°E, 46.4°N) erupted between 4 and 6 Ma. The average virtual <span class="hlt">geomagnetic</span> pole position (76 sites) includes the North Geographic Pole and the dispersion of virtual <span class="hlt">geomagnetic</span> poles is in general agreement with the data of the Time Averaged <span class="hlt">geomagnetic</span> Field Initiative. Based on this study and previous results from the East Carpathians obtained from 0.04–4 Ma old lava flows, we show that high value of dispersion are characteristic only for 1.5–2.8 Ma old lava flows. High values of dispersion during the Matuyama chron are also reported around 50°N, in the global paleosecular <span class="hlt">variation</span> data set. More data are needed at a global level to determine if these high dispersions reflect the behaviour of the <span class="hlt">geomagnetic</span> field or an artefact of inadequate number of sites. This study of the East Carpathians volcanic rocks brings new data from southeastern Europe and which can contribute to the databases for time averaged field and paleosecular <span class="hlt">variation</span> from lavas in the last 6 Ma. PMID:26997549</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EP%26S...69...58P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EP%26S...69...58P"><span>Effect of a huge crustal conductivity anomaly on the H-component of <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> recorded in central South America</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Padilha, Antonio L.; Alves, Livia R.; Silva, Graziela B. D.; Espinosa, Karen V.</p> <p>2017-04-01</p> <p>We describe here an analysis of the H-component of the <span class="hlt">geomagnetic</span> field recorded in several temporary stations operating simultaneously in the central-eastern region of Brazil during nighttime pulsation events in 1994 and the sudden commencement of the St. Patrick's Day magnetic storm in 2015. A significant amplification in the amplitude of the <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> is consistently observed in one of these stations. Magnetovariational analysis indicates that the amplification factor is period dependent with maximum amplitude around 100 s. Integrated magnetotelluric (MT) and <span class="hlt">geomagnetic</span> depth soundings (GDS) have shown that this station is positioned just over a huge 1200-km-long crustal conductor (estimated bulk conductivity greater than 1 S/m). We propose that the anomalous signature of the <span class="hlt">geomagnetic</span> field at this station is due to the high reflection coefficient of the incident electromagnetic wave at the interface with the very good conductor and by skin effects damping the electromagnetic wave in the conducting layers overlying the conductor. There are some indication from the GDS data that the conductor extends southward beneath the sediments of the Pantanal Basin. In this region is being planned the installation of a new <span class="hlt">geomagnetic</span> observatory, but its preliminary data suggest anomalous <span class="hlt">geomagnetic</span> <span class="hlt">variations</span>. We understand that a detailed MT survey must be carried out around the chosen observatory site to evaluate the possible influence of induced currents on the local <span class="hlt">geomagnetic</span> field.[Figure not available: see fulltext.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P43B2102B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P43B2102B"><span><span class="hlt">Secular</span> Orbit and Spin <span class="hlt">Variations</span> of Asteroid (16) Psyche</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bills, B. G.; Park, R. S.; Scott, B.</p> <p>2016-12-01</p> <p>The obliquity, or angular separation between spin and orbit poles, of asteroid (16) Psyche is currently 95 degrees. We are interested in knowing how much that angular separation varies, on time scales of 104 to 106 years. To answer that question, we have done several related analyses. On short time scales, the orbital element <span class="hlt">variations</span> of Psyche are dominated by perturbations from Jupiter. Jupiter's dominance has two basic causes: first is the large mass and relatively close position of Jupiter, and second is a 19:8 mean motion resonance. Jupiter completes 8 orbits in 94.9009 years, while Psyche takes 94.9107 years to complete 19 orbits. As a result of this, all of the orbital elements of Psyche exhibit significant periodic <span class="hlt">variations</span>, with a 94.9 year period dominating. There are also significant <span class="hlt">variations</span> at the synodic period, which is 8.628 years, or 1/11 of the resonant period. Over a 1000 year time span, centered on the present, the eccentricity varies from 0.133 to 0.140, and the inclination varies from 2.961 to 3.229 degrees. On longer time scales, the orbital elements of Psyche vary considerably more than that, due to <span class="hlt">secular</span> perturbations from the planets. The <span class="hlt">secular</span> <span class="hlt">variations</span> are modeled as the response of interacting mass rings, rather than point masses. Again, Jupiter is the main perturbing influence on Psyche. The eccentricity and inclination both oscillate, with dominant periods of 18.667 kyr. The range of values seen over a million year time span, is 0.057 to 0.147 for eccentricity, and 0.384 to 4.777 degrees for inclination. Using a recent shape model, and assumption of uniform density, to constrain relevant moments of inertia, we estimate the spin pole precession rate parameter to be 8.53 arcsec/year. The current spin pole is at ecliptic {lon, lat} = { 32, -7} deg, whereas the orbit pole is at {lon, lat} = {60.47, 86.91} deg. The current obliquity is thus 94.3 degree. Using nominal values of the input parameters, the recovered spin pole</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016STP.....2c..43L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016STP.....2c..43L"><span><span class="hlt">Geomagnetic</span> effects caused by rocket exhaust jets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lipko, Yuriy; Pashinin, Aleksandr; Khakhinov, Vitaliy; Rahmatulin, Ravil</p> <p>2016-09-01</p> <p>In the space experiment Radar-Progress, we have made 33 series of measurements of <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> during ignitions of engines of Progress cargo spacecraft in low Earth orbit. We used magneto-measuring complexes, installed at observatories of the Institute of Solar-Terrestrial Physics of Siberian Branch of the Russian Academy of Sciences, and magnetotelluric equipment of a mobile complex. We assumed that engine running can cause <span class="hlt">geomagnetic</span> disturbances in flux tubes crossed by the spacecraft. When analyzing experimental data, we took into account space weather factors: solar wind parameters, total daily mid-latitude <span class="hlt">geomagnetic</span> activity index Kp, <span class="hlt">geomagnetic</span> auroral electrojet index AE, global <span class="hlt">geomagnetic</span> activity. The empirical data we obtained indicate that 18 of the 33 series showed <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> in various time ranges.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMPP53A1109W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMPP53A1109W"><span>A High-resolution Palaeomagnetic <span class="hlt">Secular</span> <span class="hlt">Variation</span> Record from the Chukchi Sea, Arctic Ocean for the Last 4200 Years</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>West, G.; O'Regan, M.; Jakobsson, M.; Nilsson, A.; Pearce, C.; Snowball, I.; Wiers, S.</p> <p>2017-12-01</p> <p>The lack of high-temporal resolution and well-dated palaeomagnetic records from the Arctic Ocean hinders our understanding of <span class="hlt">geomagnetic</span> field behaviour in the region, and limits the applicability of these records in the development of accurate age models for Arctic Ocean sediments. We present a palaeomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> (PSV) record from a sediment core recovered from the Chukchi Sea, Arctic Ocean during the SWERUS-C3 Leg 2 Expedition. The 8.24-metre-long core was collected at 57 m water depth in the Herald Canyon (72.52° N 175.32° W), and extends to 4200 years BP based on 14 AMS 14C dates and a tephra layer associated with the 3.6 cal ka BP Aniakchak eruption. Palaeomagnetic measurements and magnetic analyses of discrete samples reveal stable characteristic remanent magnetisation directions, and a magnetic mineralogy dominated by magnetite. Centennial to millennial scale declination and inclination features, which correlate well to other Western Arctic records, can be readily identified. The relative palaeointensity record of the core matches well with spherical harmonic field model outputs of pfm9k (Nilsson et al., 2014) and CALS10k.2 (Constable et al. 2016) for the site location. Supported by a robust chronology, the presented high-resolution PSV record can potentially play a key role in constructing a well-dated master chronology for the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH53A2553H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH53A2553H"><span>Relative Contributions of Coronal Mass Ejections and High-speed Streams to the Long-term <span class="hlt">Variation</span> of Annual <span class="hlt">Geomagnetic</span> Activity: Solar Cycle <span class="hlt">Variation</span> and Latitudinal Differences</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Holappa, L.; Mursula, K.</p> <p>2017-12-01</p> <p>Coronal mass ejections (CMEs) and high-speed solar wind streams (HSSs) are the most important large-scale solar wind structures driving <span class="hlt">geomagnetic</span> activity. It is well known that CMEs cause the strongest <span class="hlt">geomagnetic</span> storms, while HSSs drive mainly moderate or small storms. Here we study the spatial-temporal distribution of <span class="hlt">geomagnetic</span> activity at annual resolution using local <span class="hlt">geomagnetic</span> indices from a wide range of latitudes in 1966-2014. We show that the overall contribution of HSSs to <span class="hlt">geomagnetic</span> activity exceeds that of CMEs at all latitudes. Only in a few sunspot maximum years CMEs have a comparable contribution to HSSs. While the relative contribution of HSSs maximizes at high latitudes, the relative contribution of CMEs maximizes at subauroral and low latitudes. We show that this is related to different latitudinal distribution of CME and HSS-driven substorms. We also show that the contributions of CMEs and HSSs to annual <span class="hlt">geomagnetic</span> activity are highly correlated with the intensity of the interplanetary magnetic field and the solar wind speed, respectively. Thus, a very large fraction of the long-term variability in annual <span class="hlt">geomagnetic</span> activity is described only by the <span class="hlt">variation</span> of IMF strength and solar wind speed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040171523&hterms=nudging&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dnudging','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040171523&hterms=nudging&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dnudging"><span>Torque Balances on the Taylor Cylinders in the <span class="hlt">Geomagnetic</span> Data Assimilation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuang, Weijia; Tangborn, Andrew</p> <p>2004-01-01</p> <p>In this presentation we report on our continuing effort in <span class="hlt">geomagnetic</span> data assimilation, aiming at understanding and predicting <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> on decadal time scales. In particular, we focus on the effect of the torque balances on the cylindrical surfaces in the core co-axial with the Earth's rotation axis (the Taylor cylinders) on the time evolution of assimilated solutions. We use our MoSST core dynamics,model and observed <span class="hlt">geomagnetic</span> field at the Earth's surface derived via Comprehensive Field Model (CFM) for the <span class="hlt">geomagnetic</span> data assimilation. In our earlier studies, a model solution is selected randomly from our numerical database. It is then assimilated with the observations such that the poloidal field possesses the same field tomography on the core-mantel boundary (CMB) continued downward from surface observations. This tomography change is assumed to be effective through out the outer core. While this approach allows rapid convergence between model solutions and the observations, it also generates sevee numerical instabilities: the delicate balance between weak fluid inertia and the magnetic torques on the Taylor cylinders are completely altered. Consequently, the assimilated solution diverges quickly (in approximately 10% of the magnetic free-decay time in the core). To improve the assimilation, we propose a partial penetration of the assimilation from the CMB: The full-scale modification at the CMB decreases linearly and vanish at an interior radius r(sub a). We shall examine from our assimilation tests possible relationships between the convergence rate of the model solutions to observations and the cut-off radius r(sub a). A better assimilation shall serve our nudging tests in near future.</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/2013EGUGA..15.6677Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.6677Z"><span>High resolution paleo-<span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> as recorded in sediments from Prince William Sound, Alaska</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ziegler, Leah; Stoner, Joseph</p> <p>2013-04-01</p> <p>The dynamic changes in the Earth's magnetic field, caused by fluid motions in its outer core, can be captured in global marine sediments. Here we extend recent efforts to reconstruct Holocene paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> and environmental conditions in the mid-high latitude North Pacific with analyses of a marine sediment core taken from Prince William Sound, southern Alaska. Natural and laboratory remanent magnetizations were studied by progressive alternating field (AF) demagnetization of u-channel samples from jumbo piston core EW0408-95JC (60.66278N, 147.70847W, water depth 745m). The lithology is monitored by physical properties measurements, including CT Scans and core descriptions. The lithology of the upper 8.5 m of the 17.6 meter core consists primarily of magnetically homogenous bioturbated muds. Component directions calculated by PCA analysis are characterized by low MAD values (<4°) with inclinations consistent with GAD predictions and declinations varying in a manner consistent with PSV. Normalized remanences are comparable using a variety of normalizers and show minimal scatter through demagnetization suggesting that reliable paleointenisty estimates may be preserved. A detailed chronology developed from calibrated radiocarbon dating of benthic forams shows that the 8.5m spans ~1500 years, and yields sedimentation rates of several hundred cm/kyr - ultra high for marine sediments. Comparison with Pacific Northwest and broader North American records, provides a degree of reproducibility and allows us to assess the spatial scale of signal coherence at centennial resolution . The resulting record of paleosecular <span class="hlt">variation</span> (PSV) and relative paleointensity are consistent with predictions from global <span class="hlt">geomagnetic</span> field models, yet allow investigations of rates of change of the local field, that cannot be accessed from global field models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.492..174L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.492..174L"><span>A 20-15 ka high-resolution paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> record from Black Sea sediments - no evidence for the 'Hilina Pali excursion'?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Jiabo; Nowaczyk, Norbert R.; Frank, Ute; Arz, Helge W.</p> <p>2018-06-01</p> <p>A comprehensive magnetostratigraphic investigation on sixteen sediment cores from the southeastern Black Sea yielded a very detailed high-quality paleosecular <span class="hlt">variation</span> (PSV) record spanning from 20 to 15 ka. The age models are based on radiocarbon dating, stratigraphic correlation, and tephrochronology. Further age constraints were obtained by correlating four meltwater events, described from the western Black Sea, ranging in age from about 17 to 15 ka, with maxima in K/Ti ratios, obtained from X-ray fluorescence (XRF) scanning, and minima in S-ratios, reflecting increased hematite content, in the studied cores. Since the sedimentation rates in the investigated time window are up to 50 cm ka-1, the obtained PSVs records enabled a stacking using 50-yr bins. A directional anomaly at 18.5 ka, associated with pronounced swings in inclination and declination, as well as a low in relative paleointensity (rPI), is probably contemporaneous with the Hilina Pali excursion, originally reported from Hawaiian lava flows. However, virtual <span class="hlt">geomagnetic</span> poles (VGPs) calculated from Black Sea sediments are not located at latitudes lower than 60°N, which denotes normal, though pronounced <span class="hlt">secular</span> <span class="hlt">variations</span>. During the postulated Hilina Pali excursion, the VGPs calculated from Black Sea data migrated clockwise only along the coasts of the Arctic Ocean from NE Canada (20.0 ka), via Alaska (18.6 ka) and NE Siberia (18.0 ka) to Svalbard (17.0 ka), then looping clockwise through the Eastern Arctic Ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011E%26PSL.304...22C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011E%26PSL.304...22C"><span>Saturn's very axisymmetric magnetic field: No detectable <span class="hlt">secular</span> <span class="hlt">variation</span> or tilt</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cao, Hao; Russell, Christopher T.; Christensen, Ulrich R.; Dougherty, Michele K.; Burton, Marcia E.</p> <p>2011-04-01</p> <p>Saturn is the only planet in the solar system whose observed magnetic field is highly axisymmetric. At least a small deviation from perfect symmetry is required for a dynamo-generated magnetic field. Analyzing more than six years of magnetometer data obtained by Cassini close to the planet, we show that Saturn's observed field is much more axisymmetric than previously thought. We invert the magnetometer observations that were obtained in the "current-free" inner magnetosphere for an internal model, varying the assumed unknown rotation rate of Saturn's deep interior. No unambiguous non-axially symmetric magnetic moment is detected, with a new upper bound on the dipole tilt of 0.06°. An axisymmetric internal model with Schmidt-normalized spherical harmonic coefficients g10 = 21,191 ± 24 nT, g20 = 1586 ± 7 nT. g30 = 2374 ± 47 nT is derived from these measurements, the upper bounds on the axial degree 4 and 5 terms are 720 nT and 3200 nT respectively. The <span class="hlt">secular</span> <span class="hlt">variation</span> for the last 30 years is within the probable error of each term from degree 1 to 3, and the upper bounds are an order of magnitude smaller than in similar terrestrial terms for degrees 1 and 2. Differentially rotating conducting stable layers above Saturn's dynamo region have been proposed to symmetrize the magnetic field (Stevenson, 1982). The new upper bound on the dipole tilt implies that this stable layer must have a thickness L >= 4000 km, and this thickness is consistent with our weak <span class="hlt">secular</span> <span class="hlt">variation</span> observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013IAUS..288..322J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013IAUS..288..322J"><span><span class="hlt">Secular</span> <span class="hlt">variation</span> and fluctuation of GPS Total Electron Content over Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jin, Rui; Jin, Shuanggen</p> <p>2013-01-01</p> <p>The total electron content (TEC) is an important parameters in the Earth's ionosphere, related to various space weather and solar activities. However, understanding of the complex ionospheric environments is still a challenge due to the lack of direct observations, particularly in the polar areas, e.g., Antarctica. Now the Global Positioning System (GPS) can be used to retrieve total electron content (TEC) from dual-frequency observations. The continuous GPS observations in Antarctica provide a good opportunity to investigate ionospheric climatology. In this paper, the long-term <span class="hlt">variations</span> and fluctuations of TEC over Antarctica are investigated from CODE global ionospheric maps (GIM) with a resolution of 2.5°×5° every two hours since 1998. The analysis shows significant seasonal and <span class="hlt">secular</span> <span class="hlt">variations</span> in the GPS TEC. Furthermore, the effects of TEC fluctuations are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015DPS....4721008L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015DPS....4721008L"><span>The visible spectrum of Pluto: <span class="hlt">secular</span> and longitudinal <span class="hlt">variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lorenzi, Vania; Pinilla-Alonso, Noemí; Emery, Joshua P.; Licandro, Javier; Cruikshank, Dale P.; Grundy, Will; Binzel, Richard P.</p> <p>2015-11-01</p> <p>Continuous near-infrared spectroscopic observations during the last 30 years enabled the characterization of the Pluto's surface and the study of its variability. Nevertheless, only few data are available in the visible range, where the nature of the complex-organics can be studied.For this reason, we started an observational campaign to obtain the Pluto's relative reflectance in the visible range, with the aim of characterizing the different components of its surface, and providing ground based observations in support of the New Horizons mission. We observed Pluto on six nights in 2014, with the imager/spectrograph ACAM@WHT (La Palma, Spain). We obtained six spectra in the 0.40 - 0.93 µm range, that covered a whole Pluto's rotational period (6.4 days).To study longitudinal <span class="hlt">variations</span>, we computed for all the spectra the spectral slope, and the position and the depth of the methane ice absorption bands. Also, to search for <span class="hlt">secular</span> or seasonal <span class="hlt">variations</span> we compared our data with previously published results.All the spectra present a red slope, indicating the presence of complex organics on Pluto's surface, and show the methane ice absorption bands between 0.73 and 0.90 μm. We also report the detection of the CH4 absorption band at 0.62 μm, already detected in the spectra of Makemake and Eris. The measurement of the band depth at 0.62 μm in the new spectra of Pluto, and in the spectra of Makemake and Eris, permits us to estimate the Lambert coefficient, not measured yet at this wavelength, at a temperature of 30 K and 40 K.We find that all the CH4 bands present a blue shift. This shift is minimum at the Charon-facing hemisphere, where the CH4 is also more abundant, indicating a higher degree of saturation of CH4 in the CH4:N2 dilution at this hemisphere.Comparing with data in the literature, we found that the longitudinal and <span class="hlt">secular</span> <span class="hlt">variations</span> of the parameters measured in our spectra are in accordance with previous results and with the distribution of the dark</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017IBVS.6231....1P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017IBVS.6231....1P"><span><span class="hlt">Secular</span> <span class="hlt">Variation</span> and Physical Characteristics Determination of the HADS Star EH Lib</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pena, J. H.; Villarreal, C.; Pina, D. S.; Renteria, A.; Soni, A., Guillen, J. Calderon, J.</p> <p>2017-12-01</p> <p>Physical parameters of EH Lib have been determined based on observations carried out in 2015 with photometry. They have also served, along with samples from the years 1969 and 1986, to analyse the frequency content of EH Lib with Fourier Transforms. Recent CCD observations increased the times of maximum with twelve new times which helped us study the <span class="hlt">secular</span> <span class="hlt">variation</span> of the period with a method based on the minimization of the standard deviation of the O-C residuals. It is concluded that there may be a long-term period change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61.1850R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61.1850R"><span>Characteristics of nighttime E-region over Arecibo: Dependence on solar flux and <span class="hlt">geomagnetic</span> <span class="hlt">variations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raizada, Shikha; Brum, Christiano G. M.; Mathews, John D.; Gonzalez, Cristina; Franco, Efmi</p> <p>2018-04-01</p> <p>Electron concentration (Ne) inferred from Incoherent Scatter Radar (ISR) measurements has been used to determine the influence of solar flux and <span class="hlt">geomagnetic</span> activity in the ionospheric E-region over Arecibo Observatory (AO). The approach is based on the determination of column integrated Ne, referred to as E-region total electron content (ErTEC) between 80 and 150 km altitude regions. The results discussed in this work are for the AO nighttime period. The study reveals higher ErTEC values during the low solar flux periods for all the seasons except for summer period. It is found that the E-region column abundance is higher in equinox periods than in the winter for low solar activity conditions. The column integrated Ne during the post-sunset/pre-sunrise periods always exceeds the midnight minima, independent of season or solar activity. This behavior has been attributed to the <span class="hlt">variations</span> in the coupling processes from the F-region. The response of ErTEC to the <span class="hlt">geomagnetic</span> variability is also examined for different solar flux conditions and seasons. During high solar flux periods, changes in Kp cause an ErTEC increase in summer and equinox, while producing a negative storm-like effect during the winter. <span class="hlt">Variations</span> in ErTEC due to <span class="hlt">geomagnetic</span> activity during low solar flux periods produce maximum variability in the E-region during equinox periods, while resulting in an increase/decrease in ErTEC before local midnight during the winter/summer periods, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870047342&hterms=function+museums&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dfunction%2Bmuseums','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870047342&hterms=function+museums&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dfunction%2Bmuseums"><span><span class="hlt">Geomagnetic</span> temporal change: 1903-1982 - A spline representation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Langel, R. A.; Kerridge, D. J.; Barraclough, D. R.; Malin, S. R. C.</p> <p>1986-01-01</p> <p>The <span class="hlt">secular</span> <span class="hlt">variation</span> of the earth's magnetic field is itself subject to temporal <span class="hlt">variations</span>. These are investigated with the aid of the coefficients of a series of spherical harmonic models of <span class="hlt">secular</span> <span class="hlt">variation</span> deduced from data for the interval 1903-1982 from the worldwide network of magnetic observatories. For some studies it is convenient to approximate the time <span class="hlt">variation</span> of the spherical harmonic coefficients with a smooth, continuous, function; for this a spline fitting is used. The phenomena that are investigated include periodicities, discontinuities, and correlation with the length of day. The numerical data presented will be of use for further investigations and for the synthesis of <span class="hlt">secular</span> <span class="hlt">variation</span> at any place and at any time within the interval of the data - they are not appropriate for temporal extrapolations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PNAS..114.2160B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PNAS..114.2160B"><span>Six centuries of <span class="hlt">geomagnetic</span> intensity <span class="hlt">variations</span> recorded by royal Judean stamped jar handles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ben-Yosef, Erez; Millman, Michael; Shaar, Ron; Tauxe, Lisa; Lipschits, Oded</p> <p>2017-02-01</p> <p>Earth’s magnetic field, one of the most enigmatic physical phenomena of the planet, is constantly changing on various time scales, from decades to millennia and longer. The reconstruction of <span class="hlt">geomagnetic</span> field behavior in periods predating direct observations with modern instrumentation is based on geological and archaeological materials and has the twin challenges of (i) the accuracy of ancient paleomagnetic estimates and (ii) the dating of the archaeological material. Here we address the latter by using a set of storage jar handles (fired clay) stamped by royal seals as part of the ancient administrative system in Judah (Jerusalem and its vicinity). The typology of the stamp impressions, which corresponds to changes in the political entities ruling this area, provides excellent age constraints for the firing event of these artifacts. Together with rigorous paleomagnetic experimental procedures, this study yielded an unparalleled record of the <span class="hlt">geomagnetic</span> field intensity during the eighth to second centuries BCE. The new record constitutes a substantial advance in our knowledge of past <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> in the southern Levant. Although it demonstrates a relatively stable and gradually declining field during the sixth to second centuries BCE, the new record provides further support for a short interval of extreme high values during the late eighth century BCE. The rate of change during this “<span class="hlt">geomagnetic</span> spike” [defined as virtual axial dipole moment > 160 ZAm2 (1021 Am2)] is further constrained by the new data, which indicate an extremely rapid weakening of the field (losing ˜27% of its strength over ca. 30 y).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011GeoJI.185.1220P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011GeoJI.185.1220P"><span>A new 200 Ma paleomagnetic pole for Africa, and paleo-<span class="hlt">secular</span> <span class="hlt">variation</span> scatter from Central Atlantic Magmatic Province (CAMP) intrusives in Morocco (Ighrem and Foum Zguid dykes)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Palencia-Ortas, A.; Ruiz-Martínez, V. C.; Villalaín, J. J.; Osete, M. L.; Vegas, R.; Touil, A.; Hafid, A.; McIntosh, G.; van Hinsbergen, D. J. J.; Torsvik, T. H.</p> <p>2011-06-01</p> <p>Available apparent polar wander (APW) paths for the 200 Ma configuration of Pangea, just prior to the opening of the Central Atlantic Ocean, differ as much as 10o in arc length. Here, we add new data from northwest Africa for this time, obtained from the northeast-trending Foum-Zguid and Ighrem dykes (ca. 200 Ma). These dykes form part of the northern domain of the Central Atlantic Magmatic Province (CAMP), and crosscut the Anti-Atlas Ranges in Morocco, and compositionally correspond to quartz-normative tholeiites intruded in continental lithosphere shortly before the opening of the Central Atlantic Ocean. The Foum-Zguid dyke has been intensively studied, whereas the Ighrem dyke has received less scientific focus. We sampled both dykes for paleomagnetic investigation along 100 km of each dyke (12 sites for Foum-Zguid and 11 for Ighrem, 188 samples included in the final analyses). Rock magnetic experiments indicate a mixture of multidomain and single-domain magnetite and/or low-Ti titanomagnetite particles as the principal remanence carriers. In both dykes, the primary nature of the characteristic remanent magnetization is supported by positive contact tests, related to Fe-metasomatism or baked overprints of the corresponding sedimentary country rocks. The directions of the characteristic magnetization exhibit exclusively normal polarity. Site-mean virtual <span class="hlt">geomagnetic</span> poles are differently grouped in each dyke, suggesting distinct <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> records. The Foum-Zguid paleomagnetic pole (N= 12, PLat= 67.9°N, PLon= 247.9°E, κ= 125, A95= 3.9°) plots close to that of Ighrem (N= 11, PLat= 78.4°N, PLon= 238.2°E, κ= 47, A95= 6.7°), confirming those mineralogical and geochemical evidences supporting that they represent dissimilar magmatic stages. Virtual <span class="hlt">geomagnetic</span> poles dispersion from both dykes (S= 10.5°13.0°8.1°) is in line with those obtained from recent studies of a CAMP-related dyke in Iberia and results from CAMP lavas in the Argana</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AnGeo..28..917N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AnGeo..28..917N"><span>Results of Russian <span class="hlt">geomagnetic</span> observatories in the 19th century: magnetic activity, 1841-1862</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nevanlinna, H.; Häkkinen, L.</p> <p>2010-04-01</p> <p>Hourly (spot readings) magnetic data (H- and D-components) were digitized from Russian yearbook tables for the years 1850-1862 from four observatories. The pdf pictures for digitization were taken by a normal digital camera. The database obtained consists of about 900 000 single data points. The time series of hourly magnetic values reveal slow <span class="hlt">secular</span> <span class="hlt">variations</span> (declination only) as well as transient and regular <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> of external origin. The quality and homogeneity of the data is satisfactory. Daily Ak-indices were calculated using the index algorithm that has been earlier applied to 19th century data from Helsinki (Finland) as well as modern magnetic observatory recordings. The activity index series derived from the Russian data is consistent with earlier activity index series for 1850-1862. The digitized index data series derived in this study was extended back to 1841 by including magnetic C9 activity index data available from a Russian observatory (St. Petersburg). Magnetic data rescued here is well suitable for various reconstructions for studies of the long-term <span class="hlt">variation</span> of the space weather in the 19th century.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090011775','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090011775"><span>Predicting the Size of Sunspot Cycle 24 on the Basis of Single- and Bi-<span class="hlt">Variate</span> <span class="hlt">Geomagnetic</span> Precursor Methods</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wilson, Robert M.; Hathaway, David H.</p> <p>2009-01-01</p> <p>Examined are single- and bi-<span class="hlt">variate</span> <span class="hlt">geomagnetic</span> precursors for predicting the maximum amplitude (RM) of a sunspot cycle several years in advance. The best single-<span class="hlt">variate</span> fit is one based on the average of the ap index 36 mo prior to cycle minimum occurrence (E(Rm)), having a coefficient of correlation (r) equal to 0.97 and a standard error of estimate (se) equal to 9.3. Presuming cycle 24 not to be a statistical outlier and its minimum in March 2008, the fit suggests cycle 24 s RM to be about 69 +/- 20 (the 90% prediction interval). The weighted mean prediction of 11 statistically important single-<span class="hlt">variate</span> fits is 116 +/- 34. The best bi-<span class="hlt">variate</span> fit is one based on the maximum and minimum values of the 12-mma of the ap index; i.e., APM# and APm*, where # means the value post-E(RM) for the preceding cycle and * means the value in the vicinity of cycle minimum, having r = 0.98 and se = 8.2. It predicts cycle 24 s RM to be about 92 +/- 27. The weighted mean prediction of 22 statistically important bi-<span class="hlt">variate</span> fits is 112 32. Thus, cycle 24's RM is expected to lie somewhere within the range of about 82 to 144. Also examined are the late-cycle 23 behaviors of <span class="hlt">geomagnetic</span> indices and solar wind velocity in comparison to the mean behaviors of cycles 2023 and the <span class="hlt">geomagnetic</span> indices of cycle 14 (RM = 64.2), the weakest sunspot cycle of the modern era.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70019203','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70019203"><span>The 1995 revision of the joint US/UK <span class="hlt">geomagnetic</span> field models. II: Main field</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Quinn, J.M.; Coleman, R.J.; Macmillan, S.; Barraclough, D.R.</p> <p>1997-01-01</p> <p>This paper presents the 1995 main-field revision of the World Magnetic Model (WMM-95). It is based on Project MAGNET high-level (??? 15,000 ft.) vector aeromagnetic survey data collected between 1988 and 1994 and on scalar total intensity data collected by the Polar Orbiting <span class="hlt">Geomagnetic</span> Survey (POGS) satellite during the period 1991 through 1993. The spherical harmonic model produced from these data describes that portion of the Earth's magnetic field generated internal to the Earth's surface at the 1995.0 Epoch. When combined with the spherical harmonic model of the Earth's <span class="hlt">secular</span> <span class="hlt">variation</span> described in paper I, the Earth's main magnetic field is fully characterized between the years 1995 and 2000. Regional magnetic field models for the conterminous United States, Alaska and, Hawaii were generated as by-products of the global modeling process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA34A..09M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA34A..09M"><span>How does the predicted <span class="hlt">geomagnetic</span> main field <span class="hlt">variation</span> alter the thermosphere-ionosphere storm-time response?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maute, A. I.; Lu, G.; Richmond, A. D.</p> <p>2017-12-01</p> <p>Earth's magnetic main field plays an important role in the thermosphere-ionosphere (TI) system, as well as its coupling to Earth's magnetosphere. The ionosphere consists of a weakly ionized plasma strongly influenced by the main field and embedded in the thermosphere. Therefore, ion-neutral coupling and ionospheric electrodynamics can influence the plasma distribution and neutral dynamics. There are strong longitude <span class="hlt">variations</span> of the TI storm response. At high latitude magnetosphere-ionosphere coupling is organized by the <span class="hlt">geomagnetic</span> main field, leading in general to stronger northern middle latitude storm time response in the American sector due to the <span class="hlt">geomagnetic</span> dipole location. In addition, the weak <span class="hlt">geomagnetic</span> main field in the American sector leads to larger local ExB drift and can alter the plasma densities. During <span class="hlt">geomagnetic</span> storms the intense energy input into the high latitude region is redistributed globally, leading to thermospheric heating, wind circulation changes and alterations of the ionospheric electrodynamics. The storm time changes are measurable in the plasma density, ion drift, temperature, neutral composition, and other parameters. All these changes depend, to some degree, on the <span class="hlt">geomagnetic</span> main field which changes on decadal time scales. In this study, we employ a forecast model of the <span class="hlt">geomagnetic</span> main field based on data assimilation and geodynamo modeling [Aubert et al., 2015]. The main field model predicts that in 50 years the South Atlantic Anomaly is further weakened by 2 mT and drifts westward by approximately 10o. The dipole axis moves northward and westward by 2o and 6o, respectively. Simulating the March 2015 <span class="hlt">geomagnetic</span> storm with the Thermosphere-Ionosphere Electrodynamics General Circulation Model (TIE-GCM) driven by the Assimilative Mapping of Ionospheric Electrodynamics (AMIE), we evaluate the thermosphere-ionosphere response using the <span class="hlt">geomagnetic</span> main field of 2015, 2065, and 2115. We compare the TI response for 2015 with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29657117','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29657117"><span>Evidence that Magnetic Navigation and <span class="hlt">Geomagnetic</span> Imprinting Shape Spatial Genetic <span class="hlt">Variation</span> in Sea Turtles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brothers, J Roger; Lohmann, Kenneth J</p> <p>2018-04-23</p> <p>The canonical drivers of population genetic structure, or spatial genetic <span class="hlt">variation</span>, are isolation by distance and isolation by environment. Isolation by distance predicts that neighboring populations will be genetically similar and geographically distant populations will be genetically distinct [1]. Numerous examples also exist of isolation by environment, a phenomenon in which populations that inhabit similar environments (e.g., same elevation, temperature, or vegetation) are genetically similar even if they are distant, whereas populations that inhabit different environments are genetically distinct even when geographically close [2-4]. These dual models provide a widely accepted conceptual framework for understanding population structure [5-8]. Here, we present evidence for an additional, novel process that we call isolation by navigation, in which the navigational mechanism used by a long-distance migrant influences population structure independently of isolation by either distance or environment. Specifically, we investigated the population structure of loggerhead sea turtles (Caretta caretta) [9], which return to nest on their natal beaches by seeking out unique magnetic signatures along the coast-a behavior known as <span class="hlt">geomagnetic</span> imprinting [10-12]. Results reveal that spatial <span class="hlt">variation</span> in Earth's magnetic field strongly predicts genetic differentiation between nesting beaches, even when environmental similarities and geographic proximity are taken into account. The findings provide genetic corroboration of <span class="hlt">geomagnetic</span> imprinting [10, 13]. Moreover, they provide strong evidence that <span class="hlt">geomagnetic</span> imprinting and magnetic navigation help shape the population structure of sea turtles and perhaps numerous other long-distance migrants that return to their natal areas to reproduce [13-17]. Copyright © 2018 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PEPI..276..145L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PEPI..276..145L"><span>On the frequency spectra of the core magnetic field Gauss coefficients</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lesur, Vincent; Wardinski, Ingo; Baerenzung, Julien; Holschneider, Matthias</p> <p>2018-03-01</p> <p>From monthly mean observatory data spanning 1957-2014, <span class="hlt">geomagnetic</span> field <span class="hlt">secular</span> <span class="hlt">variation</span> values were calculated by annual differences. Estimates of the spherical harmonic Gauss coefficients of the core field <span class="hlt">secular</span> <span class="hlt">variation</span> were then derived by applying a correlation based modelling. Finally, a Fourier transform was applied to the time series of the Gauss coefficients. This process led to reliable temporal spectra of the Gauss coefficients up to spherical harmonic degree 5 or 6, and down to periods as short as 1 or 2 years depending on the coefficient. We observed that a k-2 slope, where k is the frequency, is an acceptable approximation for these spectra, with possibly an exception for the dipole field. The monthly estimates of the core field <span class="hlt">secular</span> <span class="hlt">variation</span> at the observatory sites also show that large and rapid <span class="hlt">variations</span> of the latter happen. This is an indication that <span class="hlt">geomagnetic</span> jerks are frequent phenomena and that significant <span class="hlt">secular</span> <span class="hlt">variation</span> signals at short time scales - i.e. less than 2 years, could still be extracted from data to reveal an unexplored part of the core dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/14693348','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/14693348"><span>Schizophrenia and season of birth: relationship to <span class="hlt">geomagnetic</span> storms.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kay, Ronald W</p> <p>2004-01-01</p> <p>An excess pattern of winter and spring birth, of those later diagnosed as schizophrenic, has been clearly identified in most Northern Hemisphere samples with none or lesser <span class="hlt">variation</span> in Equatorial or Southern Hemisphere samples. Pregnancy and birth complications, seasonal <span class="hlt">variations</span> in light, weather, temperature, nutrition, toxins, body chemistry and gene expression have all been hypothesized as possible causes. In this study, the hypothesis was tested that seasonal <span class="hlt">variation</span> in the <span class="hlt">geomagnetic</span> field of the earth primarily as a result of <span class="hlt">geomagnetic</span> storms (GMS) at crucial periods in intrauterine brain development, during months 2 to 7 of gestation could affect the later rate of development of schizophrenia. The biological plausibility of this hypothesis is also briefly reviewed. A sample of eight representative published studies of schizophrenic monthly birth <span class="hlt">variation</span> were compared with averaged <span class="hlt">geomagnetic</span> disturbance using two global indices (AA*) and (aa). Three samples showed a significant negative correlation to both <span class="hlt">geomagnetic</span> indices, a further three a significant negative correlation to one of the <span class="hlt">geomagnetic</span> indices, one showed no significant correlation to either index and one showed a significant positive correlation to one index. It is suggested that these findings are all consistent with the hypothesis and that <span class="hlt">geomagnetic</span> disturbance or factors associated with this disturbance should be further investigated in birth seasonality studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19730026939&hterms=geomagnetic+reversal&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgeomagnetic%2Breversal','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19730026939&hterms=geomagnetic+reversal&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgeomagnetic%2Breversal"><span>Atmospheric helium and <span class="hlt">geomagnetic</span> field reversals.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sheldon, W. R.; Kern, J. W.</p> <p>1972-01-01</p> <p>The problem of the earth's helium budget is examined in the light of recent work on the interaction of the solar wind with nonmagnetic planets. It is proposed that the dominant mode of helium (He4) loss is ion pumping by the solar wind during <span class="hlt">geomagnetic</span> field reversals, when the earth's magnetic field is very small. The interaction of the solar wind with the earth's upper atmosphere during such a period is found to involve the formation of a bow shock. The penetration altitude of the shock-heated solar plasma is calculated to be about 700 km, and ionization rates above this level are estimated for a cascade ionization (electron avalanche) process to average 10 to the 9th power ions/sq cm/sec. The calculated ionization rates and the capacity of the solar wind to remove ionized helium (He4) from the upper atmosphere during <span class="hlt">geomagnetic</span> dipole reversals are sufficient to yield a <span class="hlt">secular</span> equilibrium over geologic time scales. The upward transport of helium from the lower atmosphere under these conditions is found to be adequate to sustain the proposed loss rate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMGP53C1162S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMGP53C1162S"><span>Improvement of <span class="hlt">geomagnetic</span> core field modeling with a priori information about Gauss coefficient correlations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schachtschneider, R.; Rother, M.; Lesur, V.</p> <p>2013-12-01</p> <p>We introduce a method that enables us to account for existing correlations between Gauss coefficients in core field modelling. The information about the correlations are obtained from a highly accurate field model based on CHAMP data, e.g. the GRIMM-3 model. We compute the covariance matrices of the <span class="hlt">geomagnetic</span> field, the <span class="hlt">secular</span> <span class="hlt">variation</span>, and acceleration up to degree 18 and use these in the regularization scheme of the core field inversion. For testing our method we followed two different approaches by applying it to two different synthetic satellite data sets. The first is a short data set with a time span of only three months. Here we test how the information about correlations help to obtain an accurate model when only very little information are available. The second data set is a large one covering several years. In this case, besides reducing the residuals in general, we focus on the improvement of the model near the boundaries of the data set where the accerelation is generally more difficult to handle. In both cases the obtained covariance matrices are included in the damping scheme of the regularization. That way information from scales that could otherwise not be resolved by the data can be extracted. We show that by using this technique we are able to improve the models of the field and the <span class="hlt">secular</span> <span class="hlt">variation</span> for both, the short and the long term data set, compared to approaches using more conventional regularization techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM51A2417S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM51A2417S"><span><span class="hlt">Variations</span> of plasmaspheric field-aligned electron and ion densities (90-4000 km) during quiet to moderately active (Kp < 4) <span class="hlt">geomagnetic</span> conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sonwalkar, V. S.; Reddy, A.</p> <p>2017-12-01</p> <p><span class="hlt">Variation</span> in field-aligned electron and ion densities as a function of <span class="hlt">geomagnetic</span> activity are important parameters in the physics of the thermosphere-ionosphere-magnetosphere coupling. Using whistler mode sounding from IMAGE, we report <span class="hlt">variations</span> in field-aligned electron density and O+/H+ transition height (HT) during two periods (16-23 Aug 2005; 24 Sep-06 Oct 2005) when <span class="hlt">geomagnetic</span> conditions were quiet (maximum Kp in the past 24 hours, Kpmax,24 ≤ 2) to moderately active (2 < Kpmax,24 <4). The measurements were obtained in the L=1.7 to 3.3 range (90- 4000 km, 13 or 15 MLT). Our results show that, under similar <span class="hlt">geomagnetic</span> activity, at similar L-shells but with different geographic longitudes and MLTs, the O+/H+ transition height varied within ±12% of 1100 km at L 2 and within ±8% of 1350 km at L 3. The electron densities along flux tubes varied within 30% and 20%, respectively, below (including F2 peak) and above HT. With increasing L shell: (a) O+/H+ transition height increased; (b) electron density <span class="hlt">variations</span> below HT including F2 peak showed no trend; (c) electron density above HT decreased. For flux tubes at similar longitudes, L-shells, and MLT's, relative to quiet time, during moderate <span class="hlt">geomagnetic</span> activity: (1) O+/H+ transition height was roughly same; (2) electron density <span class="hlt">variations</span> below HT showed no trend; (3) electron density above HT increased ( 10-40 %). The measured electron density is in agreement with in situ measurements from CHAMP (350 km) and DMSP (850 km) and past space borne (e. g., ISIS) measurements but the F2 peak density is a factor of 2 lower relative to that measured by ground ionosondes and that predicted by IRI-2012 empirical model. The measured transition height is consistent with OGO 4, Explorer 31, and C/NOFS measurements but is lower than that from IRI-2012. The observed <span class="hlt">variations</span> in electron density at F2 peak are consistent with past work and are attributed to solar, <span class="hlt">geomagnetic</span>, and meteorological causes [e. g. Risibeth</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/2005AGUFMGP33A0103M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFMGP33A0103M"><span>Do <span class="hlt">Geomagnetic</span> <span class="hlt">Variations</span> Affect the Foliar Spiral Direction of Coconut Palms?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Minorsky, P. V.; Bronstein, N. B.</p> <p>2005-12-01</p> <p>In coconut palms, leaves are attached to the stem in either an ascending clockwise (left-handed or L) or counter-clockwise (right-handed or R) spiral (1). Foliar spiral direction (FSD) is a classic case of morphological antisymmetry, in which dextral and sinistral forms are not inherited and are equally common within a species (2). FSD would seem a simple stochastic process unworthy of further study if not for the observation, based on data collected from 71,640 coconut palms in 42 locations around the world, that the FSD of coconut palms varies with latitude: R-trees predominate in the N Hemisphere and L-trees predominate in the S Hemisphere (3). Hemispheric asymmetries in FSD are significantly better correlated with magnetic latitude than with geographic or <span class="hlt">geomagnetic</span> latitude, suggesting that latitudinal asymmetries in FSD might be associated with the temporally varying component of Earth's magnetic field (4). Here, we present two new lines of evidence that <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> may underlie asymmetries in palm FSD. First, we show that asymmetries occur in the FSD of palm populations on opposite sides of islands, and second, that asymmetries in FSD vary with the 11-year solar cycle. The prediction that asymmetries in coconut palm FSD should exist on opposite sides of islands arises from the fact that because seawater is more electrically conductive than land, induced earth currents divide and stream past an island more strongly in one particular direction. The "<span class="hlt">geomagnetic</span> island effect" is characterized by a complete reversal of the vertical Z component of short-period <span class="hlt">geomagnetic</span> field anomalies at observation points on opposite sides of islands (5). To examine whether FSD varied around the circumferences of islands, we collected data on 6 islands (Puerto Rico, n = 4311; Antigua, n = 2038; Hawaii, n = 3552; Maui, n = 2175; Tahiti, n = 1582; Moorea, n = 2116). For each population, the degree of asymmetry was determined by calculating an "asymmetry quotient</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70018475','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70018475"><span>An 84-kyr paleomagnetic record from the sediments of Lake Baikal, Siberia</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Peck, J.A.; King, J.W.; Colman, Steven M.; Kravchinsky, V.A.</p> <p>1996-01-01</p> <p>We have conducted a paleomagnetic study of sediment cores obtained from the Selenga prodelta region of Lake Baikal, Russia. This record, which spans approximately the last 84 kyr, contributes to a better understanding of the nature of <span class="hlt">geomagnetic</span> field behavior in Siberia and is a useful correlation and dating tool. We demonstrate that the Lake Baikal sediments are recording <span class="hlt">variations</span> in the <span class="hlt">geomagnetic</span> field. The directional record displays <span class="hlt">secular</span> <span class="hlt">variation</span> behavior with a <span class="hlt">geomagnetic</span> excursion at 20 ka and additional excursions appearing as large-amplitude <span class="hlt">secular</span> <span class="hlt">variation</span> at 41, 61, and 67 ka. Smoothing of the <span class="hlt">geomagnetic</span> excursion behavior occurs in Lake Baikal sediments owing to the intermediate sedimentation rate (13 cm kyr-1). The Lake Baikal relative paleointensity record correlates to absolute paleointensity data for the last 10 kyr and to relative paleointensity records from the Mediterranean Sea and Indian Ocean for the last 84 kyr. This correlation suggests a strong global (i.e., dipole) component to these records and further supports the reliability of sediments as recorders of relative <span class="hlt">geomagnetic</span> paleointensity. We show that a relative <span class="hlt">geomagnetic</span> intensity stratigraphy has a potential resolution of 7 kyr by correlating continental and marine records. The <span class="hlt">geomagnetic</span> intensity stratigraphy helps constrain the age of the difficult to date Lake Baikal sediments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70015664','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70015664"><span>An introduction to quiet daily <span class="hlt">geomagnetic</span> fields</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Campbell, W.H.</p> <p>1989-01-01</p> <p>On days that are quiet with respect to solar-terrestrial activity phenomena, the <span class="hlt">geomagnetic</span> field has <span class="hlt">variations</span>, tens of gamma in size, with major spectral components at about 24, 12, 8, and 6 hr in period. These quiet daily field <span class="hlt">variations</span> are primarily due to the dynamo currents flowing in the E region of the earth's ionosphere, are driven by the global thermotidal wind systems, and are dependent upon the local tensor conductivity and main <span class="hlt">geomagnetic</span> field vector. The highlights of the behavior and interpretation of these quiet field changes, from their discovery in 1634 until the present, are discussed as an introduction to the special journal issue on Quiet Daily <span class="hlt">Geomagnetic</span> Fields. ?? 1989 Birkha??user Verlag.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5256419','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5256419"><span>Authigenic 10Be/9Be ratio signatures of the cosmogenic nuclide production linked to <span class="hlt">geomagnetic</span> dipole moment <span class="hlt">variation</span> since the Brunhes/Matuyama boundary</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Thouveny, Nicolas; Bourlès, Didier L.; Valet, Jean‐Pierre; Bassinot, Franck; Ménabréaz, Lucie; Guillou, Valéry; Choy, Sandrine; Beaufort, Luc</p> <p>2016-01-01</p> <p>Abstract <span class="hlt">Geomagnetic</span> dipole moment <span class="hlt">variations</span> associated with polarity reversals and excursions are expressed by large changes of the cosmogenic nuclide beryllium‐10 (10Be) production rates. Authigenic 10Be/9Be ratios (proxy of atmospheric 10Be production) from oceanic cores therefore complete the classical information derived from relative paleointensity (RPI) records. This study presents new authigenic 10Be/9Be ratio results obtained from cores MD05‐2920 and MD05‐2930 collected in the west equatorial Pacific Ocean. Be ratios from cores MD05‐2920, MD05‐2930 and MD90‐0961 have been stacked and averaged. <span class="hlt">Variations</span> of the authigenic 10Be/9Be ratio are analyzed and compared with the <span class="hlt">geomagnetic</span> dipole low series reported from global RPI stacks. The largest 10Be overproduction episodes are related to dipole field collapses (below a threshold of 2 × 1022 Am2) associated with the Brunhes/Matuyama reversal, the Laschamp (41 ka) excursion, and the Iceland Basin event (190 ka). Other significant 10Be production peaks are correlated to <span class="hlt">geomagnetic</span> excursions reported in literature. The record was then calibrated by using absolute dipole moment values drawn from the Geomagia and Pint paleointensity value databases. The 10Be‐derived <span class="hlt">geomagnetic</span> dipole moment record, independent from sedimentary paleomagnetic data, covers the Brunhes‐Matuyama transition and the whole Brunhes Chron. It provides new and complementary data on the amplitude and timing of millennial‐scale <span class="hlt">geomagnetic</span> dipole moment <span class="hlt">variations</span> and particularly on dipole moment collapses triggering polarity instabilities. PMID:28163989</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28163989','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28163989"><span>Authigenic 10Be/9Be ratio signatures of the cosmogenic nuclide production linked to <span class="hlt">geomagnetic</span> dipole moment <span class="hlt">variation</span> since the Brunhes/Matuyama boundary.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Simon, Quentin; Thouveny, Nicolas; Bourlès, Didier L; Valet, Jean-Pierre; Bassinot, Franck; Ménabréaz, Lucie; Guillou, Valéry; Choy, Sandrine; Beaufort, Luc</p> <p>2016-11-01</p> <p><span class="hlt">Geomagnetic</span> dipole moment <span class="hlt">variations</span> associated with polarity reversals and excursions are expressed by large changes of the cosmogenic nuclide beryllium-10 ( 10 Be) production rates. Authigenic 10 Be/ 9 Be ratios (proxy of atmospheric 10 Be production) from oceanic cores therefore complete the classical information derived from relative paleointensity (RPI) records. This study presents new authigenic 10 Be/ 9 Be ratio results obtained from cores MD05-2920 and MD05-2930 collected in the west equatorial Pacific Ocean. Be ratios from cores MD05-2920, MD05-2930 and MD90-0961 have been stacked and averaged. <span class="hlt">Variations</span> of the authigenic 10 Be/ 9 Be ratio are analyzed and compared with the <span class="hlt">geomagnetic</span> dipole low series reported from global RPI stacks. The largest 10 Be overproduction episodes are related to dipole field collapses (below a threshold of 2 × 10 22  Am 2 ) associated with the Brunhes/Matuyama reversal, the Laschamp (41 ka) excursion, and the Iceland Basin event (190 ka). Other significant 10 Be production peaks are correlated to <span class="hlt">geomagnetic</span> excursions reported in literature. The record was then calibrated by using absolute dipole moment values drawn from the Geomagia and Pint paleointensity value databases. The 10 Be-derived <span class="hlt">geomagnetic</span> dipole moment record, independent from sedimentary paleomagnetic data, covers the Brunhes-Matuyama transition and the whole Brunhes Chron. It provides new and complementary data on the amplitude and timing of millennial-scale <span class="hlt">geomagnetic</span> dipole moment <span class="hlt">variations</span> and particularly on dipole moment collapses triggering polarity instabilities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRB..117.7101D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRB..117.7101D"><span>Paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> at the Azores during the last 3 ka</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>di Chiara, Anita; Speranza, Fabio; Porreca, Massimiliano</p> <p>2012-07-01</p> <p>We report on 33 new paleomagnetic directions obtained from 16 lava flows emplaced in the last 3 ka on São Miguel, the largest island of the Azores. The data provide 27 well-dated directions from historical or 14C dated flows which, together with 6 directions previously gathered from the same flows by Johnson et al. (1998), yield the first paleomagnetic directional record of the last 3 ka from the Atlantic Ocean. Within-flow directions are consistent, suggesting that inclination swings from 60° to 25° and declination changes between -10° to 20° reflect <span class="hlt">variations</span> in the <span class="hlt">geomagnetic</span> field over the last 3 ka. To a first approximation, the declination record is consistent with predictions from CALS3k.4 and gufm1 global field models. Conversely, inclination values are lower than model predictions at two different ages: 1) four sites from the 1652 AD flow yield I = 48° instead of I = 63° predicted by gufm1; 2) data from several flows nicely mimic the inclination minimum of 800-1400 AD, but inclination values are lower by ˜10° than CALS3k.4 model predictions. By interpolating a cubic spline fit on declination / inclination versus age data, we tentatively infer the directional evolution of the <span class="hlt">geomagnetic</span> field at the Azores from 1000 BC to 1600 AD. The obtained curve shows three tracks in virtual overlap during the 1000-800 BC, 800-500 BC, and 400-700 AD time spans.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.tmp..161A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.tmp..161A"><span><span class="hlt">Geomagnetic</span> acceleration and rapid hydromagnetic wave dynamics in advanced numerical simulations of the geodynamo</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aubert, Julien</p> <p>2018-04-01</p> <p><span class="hlt">Geomagnetic</span> <span class="hlt">secular</span> acceleration, the second temporal derivative of Earth's magnetic field, is a unique window on the dynamics taking place in Earth's core. In this study, the behaviours of the <span class="hlt">secular</span> acceleration and underlying core dynamics are examined in new numerical simulations of the geodynamo that are dynamically closer to Earth's core conditions than earlier models. These new models reside on a theoretical path in parameter space connecting the region where most classical models are found to the natural conditions. The typical time scale for <span class="hlt">geomagnetic</span> acceleration is found to be invariant along this path, at a value close to 10 years that matches Earth's core estimates. Despite this invariance, the spatio-temporal properties of <span class="hlt">secular</span> acceleration show significant variability along the path, with an asymptotic regime of rapid rotation reached after 30% of this path (corresponding to a model Ekman number E = 3 - 7). In this regime, the energy of <span class="hlt">secular</span> acceleration is entirely found at periods longer than that of planetary rotation, and the underlying flow acceleration patterns acquire a two-dimensional columnar structure representative of the rapid rotation limit. The spatial pattern of the <span class="hlt">secular</span> acceleration at the core-mantle boundary shows significant localisation of energy within an equatorial belt. Rapid hydromagnetic wave dynamics is absent at the start of the path because of insufficient time scale separation with convective processes, weak forcing and excessive damping but can be clearly exhibited in the asymptotic regime. This study reports on ubiquitous axisymmetric geostrophic torsional waves of weak amplitude relatively to convective transport, and also stronger, laterally limited, quasi-geostrophic Alfvén waves propagating in the cylindrical radial direction from the tip of convective plumes towards the core-mantle boundary. In a system similar to Earth's core where the typical Alfvén velocity is significantly larger than the typical</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.214..531A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.214..531A"><span><span class="hlt">Geomagnetic</span> acceleration and rapid hydromagnetic wave dynamics in advanced numerical simulations of the geodynamo</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aubert, Julien</p> <p>2018-07-01</p> <p><span class="hlt">Geomagnetic</span> <span class="hlt">secular</span> acceleration, the second temporal derivative of the Earth's magnetic field, is a unique window on the dynamics taking place in the Earth's core. In this study, the behaviours of the <span class="hlt">secular</span> acceleration and underlying core dynamics are examined in new numerical simulations of the geodynamo that are dynamically closer to the Earth's core conditions than earlier models. These new models reside on a theoretical path in parameter space connecting the region where most classical models are found to the natural conditions. The typical timescale for <span class="hlt">geomagnetic</span> acceleration is found to be invariant along this path, at a value close to 10 yr that matches the Earth's core estimates. Despite this invariance, the spatio-temporal properties of <span class="hlt">secular</span> acceleration show significant variability along the path, with an asymptotic regime of rapid rotation reached after 30 per cent of this path (corresponding to a model Ekman number E = 3 × 10-7). In this regime, the energy of <span class="hlt">secular</span> acceleration is entirely found at periods longer than that of planetary rotation, and the underlying flow acceleration patterns acquire a 2-D columnar structure representative of the rapid rotation limit. The spatial pattern of the <span class="hlt">secular</span> acceleration at the core-mantle boundary shows significant localization of energy within an equatorial belt. Rapid hydromagnetic wave dynamics is absent at the start of the path because of insufficient timescale separation with convective processes, weak forcing and excessive damping but can be clearly exhibited in the asymptotic regime. This study reports on ubiquitous axisymmetric geostrophic torsional waves of weak amplitude relatively to convective transport, and also stronger, laterally limited, quasi-geostrophic Alfvén waves propagating in the cylindrical radial direction from the tip of convective plumes towards the core-mantle boundary. In a system similar to the Earth's core where the typical Alfvén velocity is significantly larger</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMSA44A..06S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMSA44A..06S"><span><span class="hlt">Variation</span> of Equatorial F-region Vertical Neutral Wind and Neutral Temperature during <span class="hlt">Geomagnetic</span> Storms: Brazil FPI Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sheng, C.; De La Garza, J. L.; Deng, Y.; Makela, J. J.; Fisher, D. J.; Meriwether, J. W.; Mesquita, R.</p> <p>2015-12-01</p> <p>An accurate description of vertical neutral winds in the thermosphere is essential to understand how the upper atmosphere responds to the <span class="hlt">geomagnetic</span> storms. However, vertical wind measurements are difficult to obtain and there are still limited data. Recent observation deployments now permit substantial progress on this issue. In this paper, neutral vertical wind data from Brazil FPI observations at around 240 km altitude during 2009 to 2015 are used for the study of the equatorial vertical wind and neutral temperature <span class="hlt">variation</span> during <span class="hlt">geomagnetic</span> activity times. First, the observations during several particular storm periods will be analyzed. Secondly, Epoch analysis will be used to bin all the observed events together to investigate the climatological features of vertical wind and temperature during storms. The results will give us an unprecedented view of the nighttime vertical wind and neutral temperature <span class="hlt">variations</span> at low latitudes, which is critical to specify the dynamics of the upper atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP21A..07S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP21A..07S"><span>Cosmogenic 10Be signature of <span class="hlt">geomagnetic</span> dipole moment <span class="hlt">variations</span> over the last 2 Ma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simon, Q.; Thouveny, N.; Bourlès, D. L.; Valet, J. P.; Bassinot, F. C.; Savranskaia, T.; Duvivier, A.; Choy, S.; Gacem, L.; Villedieu, A.</p> <p>2017-12-01</p> <p>Long-term <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> dipole moment (GDM) during periods of stable polarity and in transitional states (reversals and excursions) provide key information for understanding the geodynamo regime. Authigenic 10Be/9Be ratios (Be-ratio, proxy of atmospheric 10Be production) from marine sedimentary cores give independent and additional insights on the evolution of the <span class="hlt">geomagnetic</span> intensity, completing information from absolute and relative paleointensity (RPI) records. Here we present new Be-ratio results obtained on several marine cores from the North Atlantic, Indian and Pacific Oceans which permit to extent into the Matuyama chron our previous 10Be-derived GDM reconstructions (Simon et al., 2016 JGR 121). Stratigraphic offsets measured between Be-ratio peaks and the corresponding RPI minima in each studied cores are assigned to (post-) detrital remanent magnetization (pDRM) effects leading to magnetization locking-in delays varying from 0 to 16 cm (up to 12 ka). All these results were compiled in order to obtain a continuous Be-ratio record covering the last 2 Ma. 10Be overproduction episodes triggered by <span class="hlt">geomagnetic</span> dipole moment lows (GDL) linked to polarity reversals and excursions confirm the global control exerted by the GDM on cosmogenic radionuclides production. A dipole moment reconstruction derived from the Be-ratio stack (BeDiMo2Ma) was calibrated using absolute paleointensity data. This independent record completes the available paleomagnetic RPI records and permits: 1) to confront and increase the robustness and precision of GDM reconstructions; and, 2) to better constrain <span class="hlt">geomagnetic</span> field instabilities during the mid- to late- Matuyama chron. Our new 10Be derived inventory is fully compatible with the GDL series linked to polarity reversals (Matuyama-Brunhes transition, Jaramillo and Olduvai boundaries), <span class="hlt">geomagnetic</span> events (Cobb Mountain, Réunion) and Brunhes' excursions (e.g. Laschamp, Blake, Iceland-Basin, Big Lost). It further</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI32A..08Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI32A..08Y"><span>Sensitivity of the <span class="hlt">Geomagnetic</span> Octupole to a Stably Stratified Layer in the Earth's Core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yan, C.; Stanley, S.</p> <p>2017-12-01</p> <p>The presence of a stably stratified layer at the top of the core has long been proposed for Earth, based on evidence from seismology and <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span>. Geodynamo modeling offers a unique window to inspect the properties and dynamics in Earth's core. For example, numerical simulations have shown that magnetic field morphology is sensitive to the presence of stably stratified layers in a planet's core. Here we use the mMoSST numerical dynamo model to investigate the effects of a thin stably stratified layer at the top of the fluid outer core in Earth on the resulting large-scale <span class="hlt">geomagnetic</span> field morphology. We find that the existence of a stable layer has significant influence on the octupolar component of the magnetic field in our models, whereas the quadrupole doesn't show an obvious trend. This suggests that observations of the <span class="hlt">geomagnetic</span> field can be applied to provide information of the properties of this plausible stable layer, such as how thick and how stable this layer could be. Furthermore, we have examined whether the dominant thermal signature from mantle tomography at the core-mantle boundary (CMB) (a degree & order 2 spherical harmonic) can influence our results. We found that this heat flux pattern at the CMB has no outstanding effects on the quadrupole and octupole magnetic field components. Our studies suggest that if there is a stably stratified layer at the top of the Earth's core, it must be limited in terms of stability and thickness, in order to be compatible with the observed paleomagnetic record.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AdSpR..55..401K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AdSpR..55..401K"><span><span class="hlt">Variations</span> of solar, interplanetary, and <span class="hlt">geomagnetic</span> parameters with solar magnetic multipole fields during Solar Cycles 21-24</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Bogyeong; Lee, Jeongwoo; Yi, Yu; Oh, Suyeon</p> <p>2015-01-01</p> <p>In this study we compare the temporal <span class="hlt">variations</span> of the solar, interplanetary, and <span class="hlt">geomagnetic</span> (SIG) parameters with that of open solar magnetic flux from 1976 to 2012 (from Solar Cycle 21 to the early phase of Cycle 24) for a purpose of identifying their possible relationships. By the open flux, we mean the average magnetic field over the source surface (2.5 solar radii) times the source area as defined by the potential field source surface (PFSS) model of the Wilcox Solar Observatory (WSO). In our result, most SIG parameters except the solar wind dynamic pressure show rather poor correlations with the open solar magnetic field. Good correlations are recovered when the contributions from individual multipole components are counted separately. As expected, solar activity indices such as sunspot number, total solar irradiance, 10.7 cm radio flux, and solar flare occurrence are highly correlated with the flux of magnetic quadrupole component. The dynamic pressure of solar wind is strongly correlated with the dipole flux, which is in anti-phase with Solar Cycle (SC). The <span class="hlt">geomagnetic</span> activity represented by the Ap index is correlated with higher order multipole components, which show relatively a slow time <span class="hlt">variation</span> with SC. We also found that the unusually low <span class="hlt">geomagnetic</span> activity during SC 23 is accompanied by the weak open solar fields compared with those in other SCs. It is argued that such dependences of the SIG parameters on the individual multipole components of the open solar magnetic flux may clarify why some SIG parameters vary in phase with SC and others show seemingly delayed responses to SC <span class="hlt">variation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/14682133','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/14682133"><span>[<span class="hlt">Geomagnetic</span> field <span class="hlt">variation</span> in early ontogenesis as a risk factor for oncopathology].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Iamshanov, V A</p> <p>2003-01-01</p> <p>The data on 534 cancer patients with tumors of 15 different sites were evaluated to elucidate the influence of <span class="hlt">geomagnetic</span> field (GMF) in certain months of the pre- and early postnatal periods on future incidence of cancer. We identified neoplasms of the breast, lung, urinary bladder, hypophysis, ovary, prostate, liver, Hodgkin's disease, lymphoma and, possibly, gastric cancer as GMF-dependent. This relationship appeared to be idiosyncratic with every cancer variety. It was negligible in cases of esophagus, thyroid, uterine cervix and colorectal cancer. GMF <span class="hlt">variations</span> as a carcinogenic factor in early ontogenesis can be assessed quantitatively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990009388','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990009388"><span>Inner Core Rotation from <span class="hlt">Geomagnetic</span> Westward Drift and a Stationary Spherical Vortex in Earth's Core</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Voorhies, Coerte V.</p> <p>1998-01-01</p> <p>The idea that <span class="hlt">geomagnetic</span> westward drift indicates convective leveling of the planetary momentum gradient within Earth's core is pursued in search of a differentially rotating mean state, upon which various oscillations and <span class="hlt">secular</span> effects might be superimposed. The desired state conforms to roughly spherical boundary conditions, minimizes dissipative interference with convective cooling in the bulk of the core, yet may aid core cooling by depositing heat in the uppermost core and lower mantle. The <span class="hlt">variational</span> calculus of stationary dissipation applied to a spherical vortex within the core yields an interesting differential rotation profile, akin to spherical Couette flow bounded by thin Hartmann layers. Four boundary conditions are required. To concentrate shear induced dissipation near the core-mantle boundary, these are taken to be: (i) no-slip at the core-mantle interface; (ii) <span class="hlt">geomagnetically</span> estimated bulk westward flow at the base of the core-mantle boundary layer; (iii) no-slip at the inner-outer core interface; and, to describe magnetic locking of the inner core to the deep outer core; (iv) hydrodynamically stress-free at the inner-outer core boundary. By boldly assuming the axial core angular momentum anomaly to be zero, the super-rotation of the inner core relative to the mantle is calculated to be at most 1.5 deg./yr.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990115918&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearths%2Bouter%2Bcore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990115918&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearths%2Bouter%2Bcore"><span>Inner Core Rotation from <span class="hlt">Geomagnetic</span> Westward Drift and a Stationary Spherical Vortex in Earth's Core</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Voorhies, C. V.</p> <p>1999-01-01</p> <p>The idea that <span class="hlt">geomagnetic</span> westward drift indicates convective leveling of the planetary momentum gradient within Earth's core is pursued in search of a differentially rotating mean state, upon which various oscillations and <span class="hlt">secular</span> effects might be superimposed. The desired state conforms to roughly spherical boundary conditions, minimizes dissipative interference with convective cooling in the bulk of the core, yet may aide core cooling by depositing heat in the uppermost core and lower mantle. The <span class="hlt">variational</span> calculus of stationary dissipation applied to a spherical vortex within the core yields an interesting differential rotation profile akin to spherical Couette flow bounded by thin Hartmann layers. Four boundary conditions are required. To concentrate shear induced dissipation near the core-mantle boundary, these are taken to be: (i) no-slip at the core-mantle interface; (ii) <span class="hlt">geomagnetically</span> estimated bulk westward flow at the base of the core-mantle boundary layer; (iii) no-slip at the inner-outer core interface; and, to describe magnetic locking of the inner core to the deep outer core, (iv) hydrodynamically stress-free at the inner-outer core boundary. By boldly assuming the axial core angular momentum anomaly to be zero, the super-rotation of the inner core is calculated to be at most 1.5 degrees per year.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19720035492&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D70%26Ntt%3Dlindstrom','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19720035492&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D70%26Ntt%3Dlindstrom"><span>Response of trapped particles to a collapsing dipole moment.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heckman, H. H.; Lindstrom, P. J.</p> <p>1972-01-01</p> <p>Particle motion in the <span class="hlt">secularly</span> varying <span class="hlt">geomagnetic</span> field is investigated in terms of a dipolar magnetic field with decreasing magnetic moment M. For dM/dt equal to the rate of decay of the earth's dipole component, we find there is drift in B-L space, resulting in an inward drift of particles accompanied with increased energy and unidirectional intensity. <span class="hlt">Secular</span> <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field appears to be a dominant mechanism for radial drift in the inner radiation belt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AdSpR..37.1251D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AdSpR..37.1251D"><span>Relationship between human physiological parameters and <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> of solar origin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dimitrova, S.</p> <p></p> <p>Results presented concern influence of increased <span class="hlt">geomagnetic</span> activity on some human physiological parameters. The blood pressure and heart rate of 86 volunteers were measured on working days in autumn 2001 (01/10 09/11) and in spring 2002 (08/04 28/05). These periods were chosen because of maximal expected <span class="hlt">geomagnetic</span> activity. Altogether 2799 recordings were obtained and analysed. Questionnaire information about subjective psycho-physiological complaints was also gathered. MANOVA was employed to check the significance of the influence of three factors on the physiological parameters under consideration. The factors were the following: (1) planetary <span class="hlt">geomagnetic</span> activity level estimated by Ap-index and divided into five levels; (2) gender males and females; (3) blood pressure degree persons in the group examined were divided into hypotensive, normotensive and hypertensive. Post hoc analysis was performed to elicit the significance of differences in the factors’ levels. The average arterial blood pressure of the group was found to increase significantly with the increase of <span class="hlt">geomagnetic</span> activity level. The average increment of systolic and diastolic blood pressure of the group examined reached 9%. This effect was present irrespectively of gender. Results obtained suppose that hypertensive persons have the highest sensitivity and the hypotensive persons have the lowest sensitivity of the arterial blood pressure to increase of <span class="hlt">geomagnetic</span> activity. The results did not show significant changes in the heart rate. The percentage of the persons who reported subjective psycho-physiological complaints was also found to increase significantly with the <span class="hlt">geomagnetic</span> activity increase and the highest sensitivity was revealed for the hypertensive females.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880040223&hterms=fashion+models&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfashion%2Bmodels','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880040223&hterms=fashion+models&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfashion%2Bmodels"><span>A model for solar constant <span class="hlt">secular</span> changes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schatten, Kenneth H.</p> <p>1988-01-01</p> <p>In this paper, contrast models for solar active region and global photospheric features are used to reproduce the observed Active Cavity Radiometer and Earth Radiation Budget <span class="hlt">secular</span> trends in reasonably good fashion. A prediction for the next decade of solar constant <span class="hlt">variations</span> is made using the model. <span class="hlt">Secular</span> trends in the solar constant obtained from the present model support the view that the Maunder Minimum may be related to the Little Ice Age of the 17th century.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRA..117.6102V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRA..117.6102V"><span>Inferring interplanetary magnetic field polarities from <span class="hlt">geomagnetic</span> <span class="hlt">variations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vokhmyanin, M. V.; Ponyavin, D. I.</p> <p>2012-06-01</p> <p>In this paper, we propose a modified procedure to infer the interplanetary magnetic field (IMF) polarities from <span class="hlt">geomagnetic</span> observations. It allows to identify the polarity back to 1905. As previous techniques it is based on the well-known Svalgaard-Mansurov effect. We have improved the quality and accuracy of polarity inference compared with the previous results of Svalgaard (1975) and Vennerstroem et al. (2001) by adding new <span class="hlt">geomagnetic</span> stations and extracting carefully diurnal curve. The data demonstrates an excess of one of the two IMF sectors within equinoxes (Rosenberg-Coleman rule) evidencing polar field reversals at least for the last eight solar cycles. We also found a predominance of the two-sector structure in late of descending phase of solar cycle 16.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1983EOSTr..64..484F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1983EOSTr..64..484F"><span><span class="hlt">Geomagnetism</span> and paleomagnetism 1979-1983</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fuller, M.</p> <p></p> <p>My function, in writing these notes, is to bring you up to date in <span class="hlt">Geomagnetism</span> and Paleomagnetism, in as painless a manner as possible—without tears, as the French language texts for tourists used to promise. In writing this account of progress in the past quadrennium, I must first acknowledge that it is a personal and subjective viewpoint;; another reporter would surely emphasize other developments. Yet, there is some virture in writing of things, about which one knows something, so I leave to future reporters the task of redresssing the balance in matters covered.At the outset, one very sad event must be recorded. On April 3, 1981, Sir Edward Bullard died. His published work alone marks him as one of the leaders of <span class="hlt">geomagnetism</span> in our times. Yet his contribution was much greater; many an American geophysicist, as well as a whole generation of British colleagues, have felt the benefit of his perceptive advice on their research. To those who saw him in the last few months of his life, his courage in the face of his illness was a remarkable example of fortitude. It is by now well known that the definitive paper, which he wrote with Malin, on <span class="hlt">secular</span> <span class="hlt">variation</span> at London, was only completed immediately before his death. The transmittal letter had been typed, but death prevented him from signing it. Bullard returned in this final paper to a topic to which he had contributed much. In it, he notes the role of Halley, who first described the phenomenon of westward drift, to which Bullard gave a new numerical precision, two and a half centuries later. I seem to remember Bullard saying in a lecture years ago that, while the Newtons of this world seem other than mortal, Halley was a scientist whose life and acheivements could encourage one's own efforts. Bullard, like Halley, inspires and encourages us.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910041889&hterms=earths+outer+core&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dearths%2Bouter%2Bcore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910041889&hterms=earths+outer+core&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dearths%2Bouter%2Bcore"><span>Fluid flow near the surface of earth's outer core</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bloxham, Jeremy; Jackson, Andrew</p> <p>1991-01-01</p> <p>This review examines the recent attempts at extracting information on the pattern of fluid flow near the surface of the outer core from the <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span>. Maps of the fluid flow at the core surface are important as they may provide some insight into the process of the geodynamo and may place useful constraints on geodynamo models. In contrast to the case of mantle convection, only very small lateral <span class="hlt">variations</span> in core density are necessary to drive the flow; these density <span class="hlt">variations</span> are, by several orders of magnitude, too small to be imaged seismically; therefore, the <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> is utilized to infer the flow. As substantial differences exist between maps developed by different researchers, the possible underlying reasons for these differences are examined with particular attention given to the inherent problems of nonuniqueness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.7385B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.7385B"><span>Explanation of observable <span class="hlt">secular</span> <span class="hlt">variations</span> of gravity and alternative methods of determination of drift of the center of mass of the Earth</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barkin, Yury</p> <p>2010-05-01</p> <p>The summary. On the basis of geodynamic model of the forced relative displacement of the centers of mass of the core and the mantle of the Earth the <span class="hlt">secular</span> <span class="hlt">variations</span> of a gravity and heights of some gravimetry stations on a surface of the Earth have ben studied. At the account of <span class="hlt">secular</span> drift of the center of mass of the Earth which on our geodynamic model is caused by the unidirectional drift of the core of the Earth relatively to the mantle, the full explanation is given to observable <span class="hlt">secular</span> <span class="hlt">variations</span> of a gravity at stations Ny-Alesund (Norway), Churchill (Canada), Medicine (Italy), Sayowa (Antarctica), Strastburg (France), Membach (Belgium), Wuhan (China) and Metsahovi (Finland). Two new methods of determination of <span class="hlt">secular</span> drift of the center of mass of the Earth, alternative to classical method of a space geodesy are offered: 1) on the basis of gravimetry data about <span class="hlt">secular</span> trends of a gravity at the stations located on all basic regions of the Earth; 2) on the basis of the comparative analysis of altimetry and coastal data about <span class="hlt">secular</span> changes of sea level also in basic regions of ocean. 1. <span class="hlt">Secular</span> drift of the center of mass of the core and the center of mass of the Earth. A <span class="hlt">secular</span> drift of the center of mass of the Earth to the North relatively to special center O on an axis of rotation of the Earth for which the coefficient of third zonal harmonic J3' = 0, has been predicted in the author work [1]. A drift in a direction to a geographical point (pole P) 70°0 N and 104°3 E has been established for the first time theoretically - as a result of the analysis of the global directed redistribution of masses of the Earth, explaining the observed <span class="hlt">secular</span> drift of the pole of an axis of rotation of the Earth and not tidal acceleration of its axial rotation [2]. In [1] velocity of drift it has been estimated in 1-2 cm/yr. For specified center O the figure of a planet is as though deprived of pure-shaped form (J3' = 0). And in this sense the point O can be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70013082','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70013082"><span>More on the alleged 1970 <span class="hlt">geomagnetic</span> jerk</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Alldredge, L.R.</p> <p>1985-01-01</p> <p>French and United Kingdom workers have published reports describing a sudden change in the <span class="hlt">secular</span> acceleration, called an impulse or a jerk, which took place around 1970. They claim that this change took place in a period of a year or two and that the sources of the alleged jerk are internal. An earlier paper by this author questioned their method of analysis pointing out that their method of piecemeal fitting of parabolas to the data will always create a discontinuity in the <span class="hlt">secular</span> acceleration where the parabolas join and that the place where the parabolas join is an a priori assumption and not a result of the analysis. This paper gives a very brief summary of this first paper and then adds additional reasons for questioning the allegation that there was a worldwide sudden jerk in the magnetic field of internal origin around 1970. These new reasons are based largely on new field models which give cubic approximations of the field right through the 1970 timeframe and therefore have no discontinuities in the second derivative (jerk) around 1970. Some recent Japanese work shows several sudden changes in the <span class="hlt">secular</span> <span class="hlt">variation</span> pattern which cover limited areas and do not seem to be closely related to each other or to the irregularity noted in the European area near 1970. The <span class="hlt">secular</span> <span class="hlt">variation</span> picture which seems to be emerging is one with many local or limited-regional <span class="hlt">secular</span> <span class="hlt">variation</span> changes which appear to be almost unrelated to each other in time or space. A worldwide spherical harmonic model including coefficients up to degree 13 could never properly depict such a situation. ?? 1985.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70006358','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70006358"><span><span class="hlt">Geomagnetic</span> referencing in the arctic environment</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Podjono, Benny; Beck, Nathan; Buchanan, Andrew; Brink, Jason; Longo, Joseph; Finn, Carol A.; Worthington, E. William</p> <p>2011-01-01</p> <p><span class="hlt">Geomagnetic</span> referencing is becoming an increasingly attractive alternative to north-seeking gyroscopic surveys to achieve the precise wellbore positioning essential for success in today's complex drilling programs. However, the greater magnitude of <span class="hlt">variations</span> in the <span class="hlt">geomagnetic</span> environment at higher latitudes makes the application of <span class="hlt">geomagnetic</span> referencing in those areas more challenging. Precise, real-time data on those <span class="hlt">variations</span> from relatively nearby magnetic observatories can be crucial to achieving the required accuracy, but constructing and operating an observatory in these often harsh environments poses a number of significant challenges. Operational since March 2010, the Deadhorse Magnetic Observatory (DED), located in Deadhorse, Alaska, was created through collaboration between the United States Geological Survey (USGS) and a leading oilfield services supply company. DED was designed to produce real-time <span class="hlt">geomagnetic</span> data at the required level of accuracy, and to do so reliably under the extreme temperatures and harsh weather conditions often experienced in the area. The observatory will serve a number of key scientific communities as well as the oilfield drilling industry, and has already played a vital role in the success of several commercial ventures in the area, providing essential, accurate data while offering significant cost and time savings, compared with traditional surveying techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70035431','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70035431"><span><span class="hlt">Geomagnetic</span> referencing in the arctic environment</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Poedjono, B.; Beck, N.; Buchanan, A. C.; Brink, J.; Longo, J.; Finn, C.A.; Worthington, E.W.</p> <p>2011-01-01</p> <p><span class="hlt">Geomagnetic</span> referencing is becoming an increasingly attractive alternative to north-seeking gyroscopic surveys to achieve the precise wellbore positioning essential for success in today's complex drilling programs. However, the greater magnitude of <span class="hlt">variations</span> in the <span class="hlt">geomagnetic</span> environment at higher latitudes makes the application of <span class="hlt">geomagnetic</span> referencing in those areas more challenging. Precise, real-time data on those <span class="hlt">variations</span> from relatively nearby magnetic observatories can be crucial to achieving the required accuracy, but constructing and operating an observatory in these often harsh environments poses a number of significant challenges. Operational since March 2010, the Deadhorse Magnetic Observatory (DED), located in Deadhorse, Alaska, was created through collaboration between the United States Geological Survey (USGS) and a leading oilfield services supply company. DED was designed to produce real-time <span class="hlt">geomagnetic</span> data at the required level of accuracy, and to do so reliably under the extreme temperatures and harsh weather conditions often experienced in the area. The observatory will serve a number of key scientific communities as well as the oilfield drilling industry, and has already played a vital role in the success of several commercial ventures in the area, providing essential, accurate data while offering significant cost and time savings, compared with traditional surveying techniques. Copyright 2011, Society of Petroleum Engineers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAsGe...6..131F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAsGe...6..131F"><span>Investigation of <span class="hlt">geomagnetic</span> induced current at high latitude during the storm-time <span class="hlt">variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Falayi, E. O.; Ogunmodimu, O.; Bolaji, O. S.; Ayanda, J. D.; Ojoniyi, O. S.</p> <p>2017-06-01</p> <p>During the <span class="hlt">geomagnetic</span> disturbances, the <span class="hlt">geomagnetically</span> induced current (GIC) are influenced by the geoelectric field flowing in conductive Earth. In this paper, we studied the variability of GICs, the time derivatives of the <span class="hlt">geomagnetic</span> field (dB/dt), <span class="hlt">geomagnetic</span> indices: Symmetric disturbance field in H (SYM-H) index, AU (eastward electrojet) and AL (westward electrojet) indices, Interplanetary parameters such as solar wind speed (v), and interplanetary magnetic field (Bz) during the <span class="hlt">geomagnetic</span> storms on 31 March 2001, 21 October 2001, 6 November 2001, 29 October 2003, 31 October 2003 and 9 November 2004 with high solar wind speed due to a coronal mass ejection. Wavelet spectrum based approach was employed to analyze the GIC time series in a sequence of time scales of one to twenty four hours. It was observed that there are more concentration of power between the 14-24 h on 31 March 2001, 17-24 h on 21 October 2001, 1-7 h on 6 November 2001, two peaks were observed between 5-8 h and 21-24 h on 29 October 2003, 1-3 h on 31 October 2003 and 18-22 h on 9 November 2004. Bootstrap method was used to obtain regression correlations between the time derivative of the <span class="hlt">geomagnetic</span> field (dB/dt) and the observed values of the <span class="hlt">geomagnetic</span> induced current on 31 March 2001, 21 October 2001, 6 November 2001, 29 October 2003, 31 October 2003 and 9 November 2004 which shows a distributed cluster of correlation coefficients at around r = -0.567, -0.717, -0.477, -0.419, -0.210 and r = -0.488 respectively. We observed that high energy wavelet coefficient correlated well with bootstrap correlation, while low energy wavelet coefficient gives low bootstrap correlation. It was noticed that the <span class="hlt">geomagnetic</span> storm has a influence on GIC and <span class="hlt">geomagnetic</span> field derivatives (dB/dt). This might be ascribed to the coronal mass ejection with solar wind due to particle acceleration processes in the solar atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMGP43A1119B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMGP43A1119B"><span>High-resolution palaeomagnetic records of the Laschamp <span class="hlt">geomagnetic</span> excursion from ODP Sites 1061 and 1062</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bourne, M. D.; Henderson, G. M.; Thomas, A. L.; Mac Niocaill, C.</p> <p>2012-12-01</p> <p>The Laschamp <span class="hlt">geomagnetic</span> excursion (~41 ka) was a brief global deviation in <span class="hlt">geomagnetic</span> field behaviour from that expected during normal <span class="hlt">secular</span> <span class="hlt">variation</span>. Previously published records suggest rapid changes in field direction and a concurrent substantial decrease in field intensity. We present here high-resolution palaeomagnetic records of the Laschamp excursion obtained from two Ocean Drilling Program (ODP) Sites 1061 and 1062 on the Blake-Bahama Outer Ridge (ODP Leg 172) and compare this record with previously published records of the Blake and Iceland Basin Excursions. Relatively high sedimentation rates (>10 cm kyr-1) at these locations allow the determination of transitional field behaviour during the excursion. Rather than assuming a constant sedimentation rate between assigned age tie-points, we employ measurements of 230Thxs concentration in the sediment to assess <span class="hlt">variations</span> in the sedimentation rates through the core sections of interest. This allows us to better determine the temporal behaviour of the Laschamp excursion with greater accuracy and known uncertainty. The Laschamp excursion at this location appears to be much shorter in duration than the Blake and Iceland Basin excursions. Palaeomagnetic measurements of discrete samples from four cores reveal a single excursional feature, across an interval of 30 cm, associated with a broader palaeointensity low. The excursion is characterised by rapid transitions (less than 500 years) between a stable normal polarity and a partially-reversed, polarity. Peaks in inclination either side of the directional excursion indicate periods of time when the local field is dominated by vertical flux patches. Similar behaviour has been observed in records of the Iceland Basin Excursion from the same region. The palaeointensity record is in good agreement between the two sites. The palaeointensity record shows two minima, where the second dip in intensity is associated with a more limited directional deviation. Similar</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRA..119.5183L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRA..119.5183L"><span>Centennial <span class="hlt">variations</span> in sunspot number, open solar flux, and streamer belt width: 2. Comparison with the <span class="hlt">geomagnetic</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>Lockwood, M.; Owens, M. J.; Barnard, L.</p> <p>2014-07-01</p> <p>We investigate the relationship between interdiurnal <span class="hlt">variation</span> <span class="hlt">geomagnetic</span> activity indices, IDV and IDV(1d), corrected sunspot number, RC , and the group sunspot number RG . RC uses corrections for both the "Waldmeier discontinuity," as derived in Paper 1, and the "Wolf discontinuity" revealed by Leussu et al. (2013). We show that the simple correlation of the <span class="hlt">geomagnetic</span> indices with RCn or RGn masks a considerable solar cycle <span class="hlt">variation</span>. Using IDV(1d) or IDV to predict or evaluate the sunspot numbers, the errors are almost halved by allowing for the fact that the relationship varies over the solar cycle. The results indicate that differences between RC and RG have a variety of causes and are highly unlikely to be attributable to errors in either RG alone, as has recently been assumed. Because it is not known if RC or RG is a better predictor of open flux emergence before 1874, a simple sunspot number composite is suggested which, like RG , enables modeling of the open solar flux for 1610 onward in Paper 3 but maintains the characteristics of RC .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.2617C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.2617C"><span><span class="hlt">Variations</span> of terrestrial <span class="hlt">geomagnetic</span> activity correlated to M6+ global seismic activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cataldi, Gabriele; Cataldi, Daniele; Straser, Valentino</p> <p>2013-04-01</p> <p>From the surface of the Sun, as a result of a solar flare, are expelled a coronal mass (CME or Coronal Mass Ejection) that can be observed from the Earth through a coronagraph in white light. This ejected material can be compared to an electrically charged cloud (plasma) mainly composed of electrons, protons and other small quantities of heavier elements such as helium, oxygen and iron that run radially from the Sun along the lines of the solar magnetic field and pushing into interplanetary space. Sometimes the CME able to reach the Earth causing major disruptions of its magnetosphere: mashed in the region illuminated by the Sun and expanding in the region not illuminated. This interaction creates extensive disruption of the Earth's <span class="hlt">geomagnetic</span> field that can be detected by a radio receiver tuned to the ELF band (Extreme Low Frequency 0-30 Hz). The Radio Emissions Project (scientific research project founded in February 2009 by Gabriele Cataldi and Daniele Cataldi), analyzing the change in the Earth's <span class="hlt">geomagnetic</span> field through an induction magnetometer tuned between 0.001 and 5 Hz (bandwidth in which possible to observe the <span class="hlt">geomagnetic</span> pulsations) was able to detect the existence of a close relationship between this <span class="hlt">geomagnetic</span> perturbations and the global seismic activity M6+. During the arrival of the CME on Earth, in the Earth's <span class="hlt">geomagnetic</span> field are generated sudden and intensive emissions that have a bandwidth including between 0 and 15 Hz, an average duration of 2-8 hours, that preceding of 0-12 hours M6+ earthquakes. Between 1 January 2012 and 31 December 2012, all M6+ earthquakes recorded on a global scale were preceded by this type of signals which, due to their characteristics, have been called "Seismic <span class="hlt">Geomagnetic</span> Precursors" (S.G.P.). The main feature of Seismic <span class="hlt">Geomagnetic</span> Precursors is represented by the close relationship that they have with the solar activity. In fact, because the S.G.P. are <span class="hlt">geomagnetic</span> emissions, their temporal modulation depends</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23532042','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23532042"><span>Arabidopsis thaliana root elongation growth is sensitive to lunisolar tidal acceleration and may also be weakly correlated with <span class="hlt">geomagnetic</span> <span class="hlt">variations</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barlow, Peter W; Fisahn, Joachim; Yazdanbakhsh, Nima; Moraes, Thiago A; Khabarova, Olga V; Gallep, Cristiano M</p> <p>2013-05-01</p> <p>Correlative evidence suggests a relationship between the lunisolar tidal acceleration and the elongation rate of arabidopsis roots grown under free-running conditions of constant low light. Seedlings of Arabidopsis thaliana were grown in a controlled-climate chamber maintained at a constant temperature and subjected to continuous low-level illumination from fluorescent tubes, conditions that approximate to a 'free-running' state in which most of the abiotic factors that entrain root growth rates are excluded. Elongation of evenly spaced, vertical primary roots was recorded continuously over periods of up to 14 d using high temporal- and spatial-resolution video imaging and were analysed in conjunction with geophysical variables. The results confirm the lunisolar tidal/root elongation relationship. Also presented are relationships between the hourly elongation rates and the contemporaneous <span class="hlt">variations</span> in <span class="hlt">geomagnetic</span> activity, as evaluated from the disturbance storm time and ap indices. On the basis of time series of root elongation rates that extend over ≥4 d and recorded at different seasons of the year, a provisional conclusion is that root elongation responds to <span class="hlt">variation</span> in the lunisolar force and also appears to adjust in accordance with <span class="hlt">variations</span> in the <span class="hlt">geomagnetic</span> field. Thus, both lunisolar tidal acceleration and the <span class="hlt">geomagnetic</span> field should be considered as modulators of root growth rate, alongside other, stronger and more well-known abiotic environmental regulators, and perhaps unexplored factors such as air ions. Major changes in atmospheric pressure are not considered to be a factor contributing to oscillations of root elongation rate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3631336','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3631336"><span>Arabidopsis thaliana root elongation growth is sensitive to lunisolar tidal acceleration and may also be weakly correlated with <span class="hlt">geomagnetic</span> <span class="hlt">variations</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>Barlow, Peter W.; Fisahn, Joachim; Yazdanbakhsh, Nima; Moraes, Thiago A.; Khabarova, Olga V.; Gallep, Cristiano M.</p> <p>2013-01-01</p> <p>Background Correlative evidence suggests a relationship between the lunisolar tidal acceleration and the elongation rate of arabidopsis roots grown under free-running conditions of constant low light. Methods Seedlings of Arabidopsis thaliana were grown in a controlled-climate chamber maintained at a constant temperature and subjected to continuous low-level illumination from fluorescent tubes, conditions that approximate to a ‘free-running’ state in which most of the abiotic factors that entrain root growth rates are excluded. Elongation of evenly spaced, vertical primary roots was recorded continuously over periods of up to 14 d using high temporal- and spatial-resolution video imaging and were analysed in conjunction with geophysical variables. Key Results and Conclusions The results confirm the lunisolar tidal/root elongation relationship. Also presented are relationships between the hourly elongation rates and the contemporaneous <span class="hlt">variations</span> in <span class="hlt">geomagnetic</span> activity, as evaluated from the disturbance storm time and ap indices. On the basis of time series of root elongation rates that extend over ≥4 d and recorded at different seasons of the year, a provisional conclusion is that root elongation responds to <span class="hlt">variation</span> in the lunisolar force and also appears to adjust in accordance with <span class="hlt">variations</span> in the <span class="hlt">geomagnetic</span> field. Thus, both lunisolar tidal acceleration and the <span class="hlt">geomagnetic</span> field should be considered as modulators of root growth rate, alongside other, stronger and more well-known abiotic environmental regulators, and perhaps unexplored factors such as air ions. Major changes in atmospheric pressure are not considered to be a factor contributing to oscillations of root elongation rate. PMID:23532042</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoJI.209.1660N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoJI.209.1660N"><span><span class="hlt">Secular</span> <span class="hlt">variations</span> in zonal harmonics of Earth's geopotential and their implications for mantle viscosity and Antarctic melting history due to the last deglaciation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakada, Masao; Okuno, Jun'ichi</p> <p>2017-06-01</p> <p><span class="hlt">Secular</span> <span class="hlt">variations</span> in zonal harmonics of Earth's geopotential based on the satellite laser ranging observations, {\\dot{J}_n}, contain important information about the Earth's deformation due to the glacial isostatic adjustment (GIA) and recent melting of glaciers and the Greenland and Antarctic ice sheets. Here, we examine the GIA-induced {\\dot{J}_n}, \\dot{J}_n^{GIA} (2 ≤ n ≤ 6), derived from the available geopotential zonal <span class="hlt">secular</span> rate and recent melting taken from the IPCC 2013 Report (AR5) to explore the possibility of additional information on the depth-dependent lower-mantle viscosity and GIA ice model inferred from the analyses of the \\dot{J}_2^{GIA} and relative sea level changes. The sensitivities of the \\dot{J}_n^{GIA} to lower-mantle viscosity and GIA ice model with a global averaged eustatic sea level (ESL) of ∼130 m indicate that the <span class="hlt">secular</span> rates for n = 3 and 4 are mainly caused by the viscous response of the lower mantle to the melting of the Antarctic ice sheet regardless of GIA ice models adopted in this study. Also, the analyses of the \\dot{J}_n^{GIA} based on the available geopotential zonal <span class="hlt">secular</span> rates indicate that permissible lower-mantle viscosity structure satisfying even zonal <span class="hlt">secular</span> rates of n = 2, 4 and 6 is obtained for the GIA ice model with an Antarctic ESL component of ∼20 or ∼30 m, but there is no viscosity solution satisfying \\dot{J}_3^{GIA} and \\dot{J}_5^{GIA} values. Moreover, the inference model for the lower-mantle viscosity and GIA ice model from each odd zonal <span class="hlt">secular</span> rate is distinctly different from that satisfying GIA-induced even zonal <span class="hlt">secular</span> rate. The discrepancy between the inference models for the even and odd zonal <span class="hlt">secular</span> rates may partly be attributed to uncertainties of the geopotential zonal <span class="hlt">secular</span> rates for n > 2 and particularly those for odd zonal <span class="hlt">secular</span> rates due to weakness in the orbital geometry. If this problem is overcome at least for the <span class="hlt">secular</span> rates of n < 5, then the analyses of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750023547','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750023547"><span>Correlation of the earth's rotation rate and the <span class="hlt">secular</span> change of the <span class="hlt">geomagnetic</span> field. [power spectra/harmonic analysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jin, R. S.</p> <p>1975-01-01</p> <p>Power spectral density analysis using Burg's maximum entropy method was applied to the <span class="hlt">geomagnetic</span> dipole field and its rate of change for the years 1901 to 1969. Both spectra indicate relative maxima at 0.015 cycles/year and its harmonics. These maxima correspond approximately to 66, 33, 22, 17, 13, 11, and 9-year spectral lines. The application of the same analysis techniques to the length-of-day (l.o.d) fluctuations for the period 1865 to 1961 reveal similar spectral characteristics. Although peaks were observed at higher harmonics of the fundamental frequency, the 22-year and 11-year lines are not attributed unambiguously to the solar magnetic cycle and the solar cycle. It is suggested that the similarity in the l.o.d fluctuations and the dipole field <span class="hlt">variations</span> is related to the motion within the earth's fluid core during the past one hundred years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70162557','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70162557"><span>Improved <span class="hlt">geomagnetic</span> referencing in the Arctic environment</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Poedjono, B.; Beck, N.; Buchanan, A. C.; Borri, L.; Maus, S.; Finn, Carol; Worthington, E. William; White, Tim</p> <p>2016-01-01</p> <p><span class="hlt">Geomagnetic</span> referencing uses the Earth’s magnetic field to determine accurate wellbore positioning essential for success in today's complex drilling programs, either as an alternative or a complement to north-seeking gyroscopic referencing. However, fluctuations in the <span class="hlt">geomagnetic</span> field, especially at high latitudes, make the application of <span class="hlt">geomagnetic</span> referencing in those areas more challenging. Precise crustal mapping and the monitoring of real-time <span class="hlt">variations</span> by nearby magnetic observatories is crucial to achieving the required <span class="hlt">geomagnetic</span> referencing accuracy. The Deadhorse Magnetic Observatory (DED), located at Prudhoe Bay, Alaska, has already played a vital role in the success of several commercial ventures in the area, providing essential, accurate, real-time data to the oilfield drilling industry. <span class="hlt">Geomagnetic</span> referencing is enhanced with real-time data from DED and other observatories, and has been successfully used for accurate wellbore positioning. The availability of real-time <span class="hlt">geomagnetic</span> measurements leads to significant cost and time savings in wellbore surveying, improving accuracy and alleviating the need for more expensive surveying techniques. The correct implementation of <span class="hlt">geomagnetic</span> referencing is particularly critical as we approach the increased activity associated with the upcoming maximum of the 11-year solar cycle. The DED observatory further provides an important service to scientific communities engaged in studies of ionospheric, magnetospheric and space weather phenomena.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770022104','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770022104"><span><span class="hlt">Geomagnetic</span> activity: Dependence on solar wind parameters</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Svalgaard, L.</p> <p>1977-01-01</p> <p>Current ideas about the interaction between the solar wind and the earth's magnetosphere are reviewed. The solar wind dynamic pressure as well as the influx of interplanetary magnetic field lines are both important for the generation of <span class="hlt">geomagnetic</span> activity. The influence of the geometry of the situation as well as the variability of the interplanetary magnetic field are both found to be important factors. Semi-annual and universal time <span class="hlt">variations</span> are discussed as well as the 22-year cycle in <span class="hlt">geomagnetic</span> activity. All three are found to be explainable by the varying geometry of the interaction. Long term changes in <span class="hlt">geomagnetic</span> activity are examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014E%26PSL.400..233B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014E%26PSL.400..233B"><span>Beryllium isotopes as tracers of Lake Lisan (last Glacial Dead Sea) hydrology and the Laschamp <span class="hlt">geomagnetic</span> excursion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belmaker, Reuven; Stein, Mordechai; Beer, Jürg; Christl, Marcus; Fink, David; Lazar, Boaz</p> <p>2014-08-01</p> <p>The content of the cosmogenic isotope 10Be (t1/2=1.39 Ma) in lacustrine sediments that deposit in lakes with a large watershed is susceptible to both climate and cosmogenic production rate <span class="hlt">variations</span>. In order to distinguish between these two controls, we measured 10Be and major elements in several sections of the annually laminated sediments of the Lake Lisan (the last Glacial precursor of the Dead Sea) that are composed of detrital sediments and primary (evaporitic) aragonites. The sections were selected to represent regional hydrology and climate as reflected by different lake configurations (level rise, drop and high-stands) and rapid change in the 10Be production rate during the Laschamp <span class="hlt">geomagnetic</span> excursion. Since the short-lived cosmogenic “sister” of 10Be, 7Be (t1/2=53.3 d) has virtually no recycled component, the recycled 10Be in Lake Lisan detrital sediments was evaluated by measuring 7Be in their modern equivalents: modern flood suspended matter, dust and mud cracks. Our results demonstrate that although the recycled 10Be component is significant, <span class="hlt">secular</span> <span class="hlt">variations</span> in the 10Be concentration in Lake Lisan sediments correlate with hydrological <span class="hlt">variations</span> and <span class="hlt">geomagnetic</span> excursions. During periods of moderate <span class="hlt">variations</span> in 10Be production rate, the 10Be concentration in the Lisan detrital sediments positively correlates with lake level, Al + Fe content and the (Al + Fe)/(Ca + Mg) ratio. These correlations suggest that the 10Be is adsorbed on the fine silicate component (probably clays) of the detrital laminae. The fine silicates together with carbonates were transported to Dead Sea drainage basin mainly as airborne dust that after a short residence time was washed into Lake Lisan as flood suspended matter. We suggest that preferential dissolution of carbonates in the flood suspended matter concentrated the residual fine component leading to the positive correlation between 10Be and the (Al + Fe)/(Ca + Mg) ratio. During periods of increased water</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH51E2614O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH51E2614O"><span>On the Slow time <span class="hlt">Geomagnetic</span> field Modulation of Cosmic Rays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okpala, K. C.; Egbunu, F.</p> <p>2016-12-01</p> <p>Cosmic rays of galactic origin are modulated by both heliospheric and <span class="hlt">geomagnetic</span> conditions. The mutual (and mutually exclusive) contribution of both heliospheric and <span class="hlt">geomagnetic</span> conditions to galactic cosmic rays (GCR) modulation is still an open question. While the rapid-time association of the galactic cosmic ray <span class="hlt">variation</span> with different heliophysical and geophysical phenomena has been well studied, not so much attention has been paid to slow-time <span class="hlt">variations</span> especially with regards to local effects. In this work, we employed monthly means of cosmic ray count rates from two mid latitude (Hermanus and Rome), and two higher latitude (Inuvik and Oulu) neutron monitors (NM), and compared their variability with <span class="hlt">geomagnetic</span> stations that are in close proximity to the NMs. The data spans 1966 to 2008 and covers four (4) solar cycles. The difference (CRdiff)between the mean count rate of all days and the mean of the five quietest days for each month was compared with the Dst-related disturbance (Hdiff) derived from the nearby <span class="hlt">geomagnetic</span> stations. Zeroth- and First- correlation between the cosmic ray parameters and <span class="hlt">geomagnetic</span> parameters was performed to ascertain statistical association and test for spurious association. Our results show that solar activity is generally strongly correlated (>0.75) with mean strength of GCR count rate and <span class="hlt">geomagnetic</span> field during individual solar cycles. The correlation between mean strength of cosmic ray intensity and <span class="hlt">Geomagnetic</span> field strength is spurious and is basically moderated by the solar activity. The signature of convection driven disturbances at high latitude <span class="hlt">geomagnetic</span> stations was evident during the declining phase of the solar cycles close to the solar minimums. The absence of this feature in the slow-time varying cosmic ray count rates in all stations, and in the mid latitude <span class="hlt">geomagnetic</span> stations suggest that the local <span class="hlt">geomagnetic</span> disturbance do not play a significant role in modulating the cosmic ray flux.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004cosp...35.3952H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004cosp...35.3952H"><span>SAMPEX/PET model of the low altitude trapped proton environment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heynderickx, D.; Looper, M. D.; Blake, J. B.</p> <p></p> <p>The low-altitude trapped proton population exhibits strong time <span class="hlt">variations</span> related to <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> and neutral atmosphere conditions. The flux measurements of the Proton Electron Telescope (PET) onboard the polar satellite SAMPEX constitute an adequate data set to distinguish different time scales and to characterise the respective <span class="hlt">variations</span>. As a first step towards building a dynamic model of the low altitude proton environment we binned the 1995-1996 PET data into a model map with functional dependencies of the proton fluxes on the F10.7 solar radio flux and on the time of year to represent <span class="hlt">variations</span> on the time scale of the solar cycle and seasonal <span class="hlt">variations</span>. Now, a full solar cycle of SAMPEX/PET data is available, so that the preliminary model could be extended. The <span class="hlt">secular</span> <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field is included in the model, as it is constructed using Kaufmann's K=I √{B} instead of McIlwain's L as a map coordinate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E3SWC..2002015S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E3SWC..2002015S"><span>Interactive system for <span class="hlt">geomagnetic</span> data analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Solovev, Igor</p> <p>2017-10-01</p> <p>The paper suggests the methods for analyzing <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span>, which are implemented in "Aurora" software system for complex analysis of geophysical parameters. The software system allows one to perform a detailed magnetic data analysis. The methods allow one to estimate the intensity of <span class="hlt">geomagnetic</span> perturbations and to allocate increased <span class="hlt">geomagnetic</span> activity periods. The software system is publicly available (<ext-link xlink:href="http://aurorasa.ikir.ru%243a8580/" ext-link-type="uri">http://aurorasa.ikir.ru:8580</ext-link>, <ext-link xlink:href="http://www.ikir.ru%243a8280/lsaserver/MagneticPage.jsp" ext-link-type="uri">http://www.ikir.ru:8280/lsaserver/MagneticPage.jsp</ext-link>). This research was supported by the Russian Science Foundation (Project No. 14-11-00194).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26PSL.442..173S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26PSL.442..173S"><span>Large <span class="hlt">geomagnetic</span> field anomalies revealed in Bronze to Iron Age archeomagnetic data from Tel Megiddo and Tel Hazor, Israel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shaar, Ron; Tauxe, Lisa; Ron, Hagai; Ebert, Yael; Zuckerman, Sharon; Finkelstein, Israel; Agnon, Amotz</p> <p>2016-05-01</p> <p><span class="hlt">Geomagnetic</span> field measurements from the past few centuries show heightened <span class="hlt">secular</span> <span class="hlt">variation</span> activity in the southern hemisphere associated with the south Atlantic anomaly (SAA). It is uncertain whether <span class="hlt">geomagnetic</span> anomalies at a similar scale have existed in the past owing to limited coverage and uncertainties in the paleomagnetic database. Here we provide new evidence from archaeological sources in the Levant suggesting a large positive northern hemisphere anomaly, similar in magnitude to the SAA during the 9th-8th centuries BCE, called ;Levantine Iron Age anomaly;. We also report an additional <span class="hlt">geomagnetic</span> spike in the 8th century. The new dataset comprises 73 high precision paleointensity estimates from ca. 3000 BCE to 732 BCE, and five directional measurements between the 14th and the 9th centuries BCE. Well-dated pottery and cooking ovens were collected from twenty archaeological strata in two large contemporaneous stratigraphical mounds (tells) in Israel: Tel Megiddo and Tel Hazor. The new data are combined with previously published data and interpreted automatically using the PmagPy Thellier GUI program. The Tel Megiddo and Tel Hazor data sets demonstrate excellent internal consistency and remarkable agreement with published data from Mesopotamia (Syria). The data illustrate the evolution of an extreme <span class="hlt">geomagnetic</span> high that culminated in at least two spikes between the 11th and the 8th centuries BCE (Iron Age in the Levant). The paleomagnetic directional data of the 9th century BCE show positive inclination anomalies, and deviations of up to 22° from the averaged geocentric axial dipole (GAD) direction. From comparison of the Levantine archaeomagnetic data with IGRF model for 2015 we infer the ;Levantine Iron Age anomaly; between the 10th and the 8th centuries BCE is a local positive anomaly. The eastward extent of the anomaly is currently unknown.</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://adsabs.harvard.edu/abs/2009AAS...21340613B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AAS...21340613B"><span><span class="hlt">Secular</span> Acceleration of Barnard's Star</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bartlett, Jennifer L.; Ianna, P. A.</p> <p>2009-01-01</p> <p>Barnard's Star should have significant <span class="hlt">secular</span> acceleration because it lies close to the Sun and has the highest known proper motion along with a large radial velocity. It will pass within about 1.4 pc in another 9,750 years. <span class="hlt">Secular</span> changes in proper motion and radial velocity are essentially the Coriolis and centrifugal accelerations, respectively, arising from use of a rotating coordinate system defined by the Sun-star radius vector. Although stellar space velocities measured with respect to the Sun are essentially constant, these perspective effects arise with changing distance and viewing angle. Hipparcos-2 plus Nidever et al. (2002) predict a perspective change in the proper motion of 1.285±0.006 mas yr-2 for Barnard's Star. Recent analysis of 900+ photographic plates between 1968 and 1998 with the 26.25-in (0.67-m) McCormick refractor detected a <span class="hlt">secular</span> acceleration of 1.25±0.04 mas yr-2, which agrees with the predicted value within the measurement errors. Earlier, Benedict et al. (1999) measured its <span class="hlt">secular</span> acceleration to be 1.2±0.2 mas yr-2 using 3 years of HST FGS observations. Similarly, a perspective change in radial velocity of 4.50±0.01 m s-1 yr-1 can be predicted for Barnard's Star. Kürster et al. (2003) detected <span class="hlt">variations</span> in their observations of it that are largely attributable to <span class="hlt">secular</span> acceleration along the line of sight with some contribution from stellar activity. Although <span class="hlt">secular</span> acceleration effects have been limited for past studies of stellar motions, they can be significant for observations extending over decades or for high-precision measurements required to detect extrasolar planets. Future studies will need to consider this factor for the nearest stars and for those with large proper motions or radial velocities. NSF grant AST 98-20711; Litton Marine Systems; Peninsula Community Foundation Levinson Fund; UVa Governor's Fellowship, Dean's F&A Fellowship, and Graduate School of Arts and Sciences; and, US Naval Observatory</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990115469&hterms=satellite+radiation+damage&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dsatellite*%2Bradiation%2Bdamage','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990115469&hterms=satellite+radiation+damage&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dsatellite*%2Bradiation%2Bdamage"><span>Future Radiation Damage in Space due to South Atlantic Anomaly</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heirtzler, J. R.</p> <p>1999-01-01</p> <p>Predictions of radiation damage for Low Earth Orbit (LEO) satellites now use semi-empirical models developed from prior satellite data. From these models it is clear that the low field strength of the South Atlantic Anomaly (SAA) controls where the maximum radiation damage occurs. One may make an estimate of future radiation damage to LEO spacecraft if one can predict the future of the SAA. Although reliable maps of the <span class="hlt">geomagnetic</span> field strength and its <span class="hlt">secular</span> change have only been made in the last few decades, certain <span class="hlt">geomagnetic</span> observatories in South America and Africa have recorded the <span class="hlt">geomagnetic</span> field for a much longer time. These observatories show that the present <span class="hlt">geomagnetic</span> field change has persisted for more than 100 years. In spite of the fact that a few observatories have shown sudden changes in <span class="hlt">secular</span> <span class="hlt">variation</span>, those around the SAA have shown a stable <span class="hlt">secular</span> <span class="hlt">variation</span>. Assuming that this will continue for the next 50 to 100 years one can show that the SAA will expand to cover most of the South Atlantic Ocean and will become much weaker. This will greatly intensify the radiation hazard in LEO, put significant new limitations on radiation-hardened hardware, severely restrict the length of time that humans can remain in orbit, and materially change the configuration of the radiation belts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.9626C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.9626C"><span>Tsunami related to solar and <span class="hlt">geomagnetic</span> activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cataldi, Gabriele; Cataldi, Daniele; Straser, Valentino</p> <p>2016-04-01</p> <p>The authors of this study wanted to verify the existence of a correlation between earthquakes of high intensity capable of generating tsunami and <span class="hlt">variations</span> of solar and Earth's <span class="hlt">geomagnetic</span> activity. To confirming or not the presence of this kind of correlation, the authors analyzed the conditions of Spaceweather "near Earth" and the characteristics of the Earth's <span class="hlt">geomagnetic</span> field in the hours that preceded the four earthquakes of high intensity that have generated tsunamis: 1) Japan M9 earthquake occurred on March 11, 2011 at 05:46 UTC; 2) Japan M7.1 earthquake occurred on October 25, 2013 at 17:10 UTC; 3) Chile M8.2 earthquake occurred on April 1, 2014 at 23:46 UTC; 4) Chile M8.3 earthquake occurred on September 16, 2015 at 22:54 UTC. The data relating to the four earthquakes were provided by the United States Geological Survey (USGS). The data on ion density used to realize the correlation study are represented by: solar wind ion density <span class="hlt">variation</span> detected by ACE (Advanced Composition Explorer) Satellite, in orbit near the L1 Lagrange point, at 1.5 million of km from Earth, in direction of the Sun. The instrument used to perform the measurement of the solar wind ion density is the Electron, Proton, and Alpha Monitor (EPAM) instrument, equipped on the ACE Satellite. To conduct the study, the authors have taken in consideration the <span class="hlt">variation</span> of the solar wind protons density of three different energy fractions: differential proton flux 1060-1900 keV (p/cm^2-sec-ster-MeV); differential proton flux 761-1220 keV (p/cm^2-sec-ster-MeV); differential proton flux 310-580 keV (p/cm^2-sec-ster-MeV). <span class="hlt">Geomagnetic</span> activity data were provided by Tromsø <span class="hlt">Geomagnetic</span> Observatory (TGO), Norway; by Scoresbysund <span class="hlt">Geomagnetic</span> Observatory (SCO), Greenland, Denmark and by Space Weather Prediction Center of Pushkov Institute of terrestrial magnetism, ionosphere and radio wave propagation (IZMIRAN), Troitsk, Moscow Region. The results of the study, in agreement with what already</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUSMGP23C..05M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUSMGP23C..05M"><span>High-resolution palaeomagnetic records of the Laschamp <span class="hlt">geomagnetic</span> excursion from the Blake Ridge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mac Niocaill, C.; Bourne, M. D.; Thomas, A. L.; Henderson, G. M.</p> <p>2013-05-01</p> <p><span class="hlt">Geomagnetic</span> excursions are brief (1000s of years) deviations in <span class="hlt">geomagnetic</span> field behaviour from that expected during 'normal <span class="hlt">secular</span>' <span class="hlt">variation</span>. The Laschamp excursion (~41 ka) was a global deviation in <span class="hlt">geomagnetic</span> field behaviour. Previously published records suggest rapid changes in field direction and a concurrent substantial decrease in field intensity. Accurate dating of excursions and determinations of their durations from multiple locations is vital to our understanding to global field behaviour during these deviations. We present here high-resolution palaeomagnetic records of the Laschamp excursion obtained from two Ocean Drilling Program (ODP) Sites 1061 and 1062 on the Blake-Bahama Outer Ridge (ODP Leg 172) Relatively high sedimentation rates (~30-40 cm kyr-1) at these locations allow the determination of transitional field behaviour during the excursion. Despite their advantages, sedimentary records can be limited by the potential for unrecognized <span class="hlt">variations</span> in sedimentation rates between widely spaced age-constrained boundaries. Rather than assuming a constant sedimentation rate between assigned age tie-points, we employ measurements of the concentration of 230Thxs in the sediment. 230Thxs is a constant flux proxy and may be used to assess <span class="hlt">variations</span> in the sedimentation rates through the core sections of interest. Following this approach, we present a new age model for Site 1061 that allows us to better determine the temporal behaviour of the Laschamp excursion with greater accuracy and known uncertainty. Palaeomagnetic measurements of discrete samples from four cores reveal a single excursional feature, across an interval of 30 cm, associated with a broader palaeointensity low. The excursion is characterised by rapid transitions (less than 200 years) between a stable normal polarity and a partially-reversed, polarity. Peaks in inclination either side of the directional excursion indicate periods of time when the local field is dominated by vertical</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AnGeo..31.1957L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AnGeo..31.1957L"><span>Reconstruction of <span class="hlt">geomagnetic</span> activity and near-Earth interplanetary conditions over the past 167 yr - Part 1: A new <span class="hlt">geomagnetic</span> data composite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lockwood, M.; Barnard, L.; Nevanlinna, H.; Owens, M. J.; Harrison, R. G.; Rouillard, A. P.; Davis, C. J.</p> <p>2013-11-01</p> <p>We present a new composite of <span class="hlt">geomagnetic</span> activity which is designed to be as homogeneous in its construction as possible. This is done by only combining data that, by virtue of the locations of the source observatories used, have similar responses to solar wind and IMF (interplanetary magnetic field) <span class="hlt">variations</span>. This will enable us (in Part 2, Lockwood et al., 2013a) to use the new index to reconstruct the interplanetary magnetic field, B, back to 1846 with a full analysis of errors. Allowance is made for the effects of <span class="hlt">secular</span> change in the <span class="hlt">geomagnetic</span> field. The composite uses interdiurnal <span class="hlt">variation</span> data from Helsinki for 1845-1890 (inclusive) and 1893-1896 and from Eskdalemuir from 1911 to the present. The gaps are filled using data from the Potsdam (1891-1892 and 1897-1907) and the nearby Seddin observatories (1908-1910) and intercalibration achieved using the Potsdam-Seddin sequence. The new index is termed IDV(1d) because it employs many of the principles of the IDV index derived by Svalgaard and Cliver (2010), inspired by the u index of Bartels (1932); however, we revert to using one-day (1d) means, as employed by Bartels, because the use of near-midnight values in IDV introduces contamination by the substorm current wedge auroral electrojet, giving noise and a dependence on solar wind speed that varies with latitude. The composite is compared with independent, early data from European-sector stations, Greenwich, St Petersburg, Parc St Maur, and Ekaterinburg, as well as the composite u index, compiled from 2-6 stations by Bartels, and the IDV index of Svalgaard and Cliver. Agreement is found to be extremely good in all cases, except two. Firstly, the Greenwich data are shown to have gradually degraded in quality until new instrumentation was installed in 1915. Secondly, we infer that the Bartels u index is increasingly unreliable before about 1886 and overestimates the solar cycle amplitude between 1872 and 1883 and this is amplified in the proxy data used</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10466E..70G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10466E..70G"><span><span class="hlt">Geomagnetic</span> activity signature in seasonal <span class="hlt">variations</span> of mesopause temperature over Yakutia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gavrilyeva, G. A.; Ammosov, P. P.; Ammosova, A. M.; Koltovskoi, I. I.; Sivtseva, V. I.</p> <p>2017-11-01</p> <p>Research of the seasonal change of mesopause temperature at height of nightglow of hydroxyl excited molecules and its correlation with <span class="hlt">geomagnetic</span> activity during the 23 solar cycle is presented. An infrared digital spectrograph installed at the Maimaga station (63°N, 129.5°E) measured P-branches of the OH(6-2) band. The rotational temperature of OH emission (TOH) is assumed to be equal to the neutral atmosphere temperature at the altitude of 87 km. The database of TOH comprises 2864 nightly average temperatures obtained from August 1999 to May 2015 is considered. The observation starts at the beginning of August and ends in the middle of May. It was revealed that the maximum flux of radio emission from the Sun with a wavelength of 10.7 cm is 2 years ahead of the maximum of seasonally averaged temperature. Temperature is correlated with a change of Ap-index which is a measure of <span class="hlt">geomagnetic</span> activity. Nightly mean TOH were grouped in accordance with the <span class="hlt">geomagnetic</span> activity level: the temperatures measured during years with a high activity (Ap> 8), and low activity (Ap <= 8). It was found that the mesopause temperature from October to February is higher by a factor of about ·10 K than during years with low activity (Ap <= 8). There is no dependence of the TOH on the level of <span class="hlt">geomagnetic</span> activity in autumn and spring.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1212635M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1212635M"><span>Marine sediments and Beryllium-10 record of the <span class="hlt">geomagnetic</span> moment <span class="hlt">variations</span> during the Brunhes period.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ménabréaz, Lucie; Thouveny, Nicolas; Bourlès, Didier; Demory, François</p> <p>2010-05-01</p> <p>Over millennial time scales, the atmospheric production of the cosmonuclid 10Be (half-life 1.387 ± 0.012 Ma [Shmeleff et al., 2009; Korschinek et al., 2009]) is modulated by the <span class="hlt">geomagnetic</span> field strength, following a negative power law (e.g. Lal, 1988; Masarik and Beer, 2009). With respect to paleomagnetic reconstructions, 10Be-derived paleointensity records can therefore constitute an alternative, global and independent reading of the dipole moment <span class="hlt">variations</span>. During the last years, efforts have been made to extract a <span class="hlt">geomagnetic</span> signal from single and stacked 10Be records in natural archives such as ice and marine sediments (e.g. Carcaillet et al., 2004; Christl et al., 2007; Muscheler et al., 2005). In marine sediments, the 10Be concentration results from complex interplay of several processes: cosmogenic production, adsorption on sediment particles, redistribution by fluviatile and oceanic transport, and deposition. Therefore, a correction procedure is required to consider both sediment redistribution and enhanced scavenging, which can alter the primary signatures. To reconstruct the succession of field intensity lows accompanying excursions during the Brunhes chron, we investigated authigenic 10Be/9Be record of marine sequences also studied for paleomagnetism and oxygen isotopes. Mid and low latitude sites were preferred in order to benefit from the most efficient modulation by the magnetospheric shielding. We present a high resolution authigenic 10Be/9Be record of the last 50 ka recovered from the Portuguese Margin, that deciphers the cosmonuclide 10Be overproduction created by the <span class="hlt">geomagnetic</span> dipole low associated with the Laschamp excursion. This record is compared to other proxy records of the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> for the same time interval: (1) the relative paleointensity (RPI) reconstructed from the same sediments and the GLOPIS-75 record (Laj et al., 2004), (2) the absolute VDM record based on absolute paleointensities measured on lava flows</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoJI.202..533K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoJI.202..533K"><span>Crustal structure of Precambrian terranes in the southern African subcontinent with implications for <span class="hlt">secular</span> <span class="hlt">variation</span> in crustal genesis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kachingwe, Marsella; Nyblade, Andrew; Julià, Jordi</p> <p>2015-07-01</p> <p>New estimates of crustal thickness, Poisson's ratio and crustal shear wave velocity have been obtained for 39 stations in Angola, Botswana, the Democratic Republic of Congo, Malawi, Mozambique, Namibia, Rwanda, Tanzania and Zambia by modelling P-wave receiver functions using the H-κ stacking method and jointly inverting the receiver functions with Rayleigh-wave phase and group velocities. These estimates, combined with similar results from previous studies, have been examined for <span class="hlt">secular</span> trends in Precambrian crustal structure within the southern African subcontinent. In both Archean and Proterozoic terranes we find similar Moho depths [38-39 ± 3 km SD (standard deviation)], crustal Poisson's ratio (0.26 ± 0.01 SD), mean crustal shear wave velocity (3.7 ± 0.1 km s-1 SD), and amounts of heterogeneity in the thickness of the mafic lower crust, as defined by shear wave velocities ≥4.0 km s-1. In addition, the amount of variability in these crustal parameters is similar within each individual age grouping as between age groupings. Thus, the results provide little evidence for <span class="hlt">secular</span> <span class="hlt">variation</span> in Precambrian crustal structure, including between Meso- and Neoarchean crust. This finding suggests that (1) continental crustal has been generated by similar processes since the Mesoarchean or (2) plate tectonic processes have reworked and modified the crust through time, erasing <span class="hlt">variations</span> in structure resulting from crustal genesis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.4392B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.4392B"><span>Mechanism of <span class="hlt">secular</span> increasing of mean gravity in Northern hemisphere and <span class="hlt">secular</span> decreasing of mean gravity in Southern hemisphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barkin, Yu. V.; Ferrandiz, J. M.</p> <p>2009-04-01</p> <p> phenomena as cyclicity and synchronism of planetary natural processes, inversion of activity of natural processes in opposite hemispheres. Numerous confirmations give the extensive data of every possible geophysical observations. The phenomenon of synchronism in annual <span class="hlt">variations</span> of activity of various natural processes is rather brightly expressed - their phases are precisely synchronized, and the periods of extreme activity (or passivity) fall to February - March or August - September. In daily <span class="hlt">variations</span> of natural processes similar laws are observed. Here we speak about modern processes, but similar laws take place in various time scales, including geological. In the given report we shall concentrate on the analysis of possible <span class="hlt">secular</span> <span class="hlt">variations</span> of a gravity at displacement of an external core (of its centre of mass) relatively to the elastic mantle. The analysis has shown, that gravitational influence of displaced superfluous mass of the core are a major factor of <span class="hlt">secular</span> <span class="hlt">variations</span> of a gravity. However the displaced core causes directed redistribution of atmospheric masses from a southern hemisphere in northern, and also complex slow redistribution of oceanic masses. Increase of loading of atmospheric and oceanic masses on an elastic crust of northern hemisphere results in its slow lowering. Return processes should observed in a southern hemisphere. All listed factors, certainly, directly influence <span class="hlt">variations</span> of a gravity. In a more comprehensive sense redistribution of all fluid masses, including climatic character also result in changes of a gravity. Hemispheres mean <span class="hlt">secular</span> trends of gravity. For an estimation of a role of factors of redistribution of air and fluid masses in <span class="hlt">variations</span> of a gravity the point model of redistribution of masses of the Earth (Barkin, 2001), obtained very effective applications at studying of fundamental problems of geodynamics, has been used. Let's emphasize, that the Earth is active dynamic object at which activity in the certain</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17657732','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17657732"><span>Lagged association between <span class="hlt">geomagnetic</span> activity and diminished nocturnal pain thresholds in mice.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Galic, M A; Persinger, M A</p> <p>2007-10-01</p> <p>A wide variety of behaviors in several species has been statistically associated with the natural <span class="hlt">variations</span> in <span class="hlt">geomagnetism</span>. To examine whether changes in <span class="hlt">geomagnetic</span> activity are associated with pain thresholds, adult mice were exposed to a hotplate paradigm once weekly for 52 weeks during the dark cycle. Planetary A index values from the previous 6 days of a given hotplate session were correlated with the mean response latency for subjects to the thermal stimulus. We found that hotplate latency was significantly (P < 0.05) and inversely correlated (rho = -0.25) with the daily <span class="hlt">geomagnetic</span> intensity 3 days prior to testing. Therefore, if the <span class="hlt">geomagnetic</span> activity was greater 3 days before a given hotplate trial, subjects tended to exhibit shorter response latencies, suggesting lower pain thresholds or less analgesia. These results are supported by related experimental findings and suggest that natural <span class="hlt">variations</span> in <span class="hlt">geomagnetic</span> intensity may influence nociceptive behaviors in mice. (c) 2007 Wiley-Liss, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850026772','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850026772"><span>The use of the McIlwain L-parameter to estimate cosmic ray vertical cutoff rigidities for different epochs of the <span class="hlt">geomagnetic</span> field</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shea, M. A.; Smart, D. F.; Gentile, L. C.</p> <p>1985-01-01</p> <p><span class="hlt">Secular</span> changes in the <span class="hlt">geomagnetic</span> field between 1955 and 1980 have been large enough to produce significant differences in both the verical cutoff rigidities and in the L-value for a specified position. A useful relationship employing the McIlwain L-parameter to estimate vertical cutoff rigidities has been derived for the twenty-five year period.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009GeoRL..3612706Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009GeoRL..3612706Q"><span>On the <span class="hlt">secular</span> change of spring onset at Stockholm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qian, Cheng; Fu, Congbin; Wu, Zhaohua; Yan, Zhongwei</p> <p>2009-06-01</p> <p>A newly developed method, the Ensemble Empirical Mode Decomposition, was applied to adaptively determine the timing of climatic spring onset from the daily temperature records at Stockholm during 1756-2000. <span class="hlt">Secular</span> <span class="hlt">variations</span> of spring onset and its relationships to the North Atlantic Oscillation (NAO) and to the temperature variability were analyzed. A clear turning point of <span class="hlt">secular</span> trend in spring onset around 1884/1885, from delaying to advancing, was found. The delaying trend of spring onset (6.9 days/century) during 1757-1884 and the advancing one (-7 days/century) during 1885-1999 were both significant. The winter NAO indices were found to be correlated with the spring onset at Stockholm at an inter-annual timescale only for some decades, but unable to explain the change of the long-term trends. The <span class="hlt">secular</span> change from cooling to warming around the 1880s, especially in terms of spring temperature, might have led to the <span class="hlt">secular</span> change of spring onset.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850026754','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850026754"><span>A relation between the short time <span class="hlt">variations</span> of cosmic rays and <span class="hlt">geomagnetic</span> field change</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Saki, T.; Kato, M.</p> <p>1985-01-01</p> <p>An event is reported of approx. 37 min periodicity in cosmic ray intensity observed at Akeno(38 deg 47 N, 138 deg 30 E. 900m above s.l., cutoff 10.4 GV) during 1300 approx. 1900 UT on April 25th, 1984, just a day before Forbush decrease of April 26th. This event seemed to be followed by the periodic <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field observed at Kakioka (36 deg 23 N, 140 deg 18 E). The regression coefficient between them was obtained approx. 0.07%/10nT. It is shown that in general the power spectral density of cosmic rays in the frequency of 0.0001 approx. 0.001Hz correlates positively with the fluctuations of <span class="hlt">geomagnetic</span> field (Dst field) around approx. 1.2x0.0001Hz. From the analysis of 47 days data (April 14th to June 13th, 1984) the regression curve was obtained as y=0.275x sup 0.343 with the correlation coefficient of 0.48, where x and y mean Fourier components of Dst field summed over 1.04 approx. 1.39x0.001Hz and cosmic ray power spectral density averaged over 0.0001 approx. 0.001Hz.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1916450M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1916450M"><span>First archaeointensity catalogue and intensity <span class="hlt">secular</span> <span class="hlt">variation</span> curve for Iberia spanning the last 3000 years</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Molina-Cardín, Alberto; Campuzano, Saioa A.; Rivero, Mercedes; Osete, María Luisa; Gómez-Paccard, Miriam; Pérez-Fuentes, José Carlos; Pavón-Carrasco, F. Javier; Chauvin, Annick; Palencia-Ortas, Alicia</p> <p>2017-04-01</p> <p>In this work we present the first archaeomagnetic intensity database for the Iberian Peninsula covering the last 3 millennia. In addition to previously published archaeointensities (about 100 data), we present twenty new high-quality archaeointensities. The new data have been obtained following the Thellier and Thellier method including pTRM-checks and have been corrected for the effect of the anisotropy of thermoremanent magnetization upon archaeointensity estimates. Importantly, about 50% of the new data obtained correspond to the first millennium BC, a period for which there was not possible to develop an intensity palaeosecular <span class="hlt">variation</span> curve before due to the lack of high-quality archaeointensity data. The different qualities of the data included in the Iberian dataset have been evaluated following different palaeomagnetic criteria, such as the number of specimens analysed, the laboratory protocol applied and the kind of material analysed. Finally, we present the first intensity palaeosecular <span class="hlt">variation</span> curve for the Iberian Peninsula centred at Madrid for the last 3000 years. In order to obtain the most reliable <span class="hlt">secular</span> <span class="hlt">variation</span> curve, it has been generated using only selected high-quality data from the catalogue.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.1949S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.1949S"><span><span class="hlt">Variations</span> in the <span class="hlt">geomagnetic</span> and gravitational background associated with two strong earthquakes of the May 2012 sequence in the Po Valley Plain (Italy).</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Straser, Valentino</p> <p>2013-04-01</p> <p>Reawakening of seismic activity in the Emilian Po Valley Plain (Italy) resulted in 2,492 earthquakes over five and a half months: 2,270 with M<3, 189 with a magnitude from 3.0<= M <4.0, 27 con 4.0<= M <5.0, and 7 M>= 7. The mainshock was recorded during the night of 20 May 2012, at 04:03:52 Italian time (02:03:52 UTC) with epicentre in Finale Emilia, at a depth of 6.3km, by the Italian National Institute of Geophysics and Vulcanology (INGV). A long sequence of telluric shocks occurred in the same seismic district in the areas between the provinces of Modena, Ferrara, Mantua, Reggio Emilia, Bologna and Rovigo. In addition to the general devastation plus damage to civil and industrial buildings and the historical heritage, the earthquakes resulted in a total of 27 victims. Concomitant with the two strongest quakes, recorded on 20 and 29 May 2012, respectively, as in the case of others, <span class="hlt">variations</span> were noted in the <span class="hlt">geomagnetic</span> background by the LTPA monitoring station in Rome (Italy). The <span class="hlt">geomagnetic</span> background <span class="hlt">variations</span> were associated with the appearance of radio-anomalies in a frequency range from 0.1 to 3.0Hz, as well as gravimetric <span class="hlt">variations</span> found around 60km from the epicentre. The peak accelerations, detected in correspondence with the strongest shocks on 20 and 29 May 2012, were respectively 0.31g and 0.29g. The appearance of the radio-anomalies coincided, from a temporal point of view, with average gravimetric <span class="hlt">variations</span> of approximately 30µGal around the epicentre areas, concurrent with the mainshock. In this study, both the appearance of radio-anomalies and the gravitational <span class="hlt">variations</span> recorded before strong earthquakes were related to the dynamics of the fault and a progressive reduction in granulometry in the core of the fracture, until the point of dislocation was reached. The intense friction in the fault and the damping factors produced before the shock are hypothesized as being proportional to the number of radio-anomalies measured. The radio</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JApA...39...36S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JApA...39...36S"><span>Effect of <span class="hlt">geomagnetic</span> storms on VHF scintillations observed at low latitude</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singh, S. B.; Patel, Kalpana; Singh, A. K.</p> <p>2018-06-01</p> <p>A <span class="hlt">geomagnetic</span> storm affects the dynamics and composition of the ionosphere and also offers an excellent opportunity to study the plasma dynamics. In the present study, we have used the VHF scintillations data recorded at low latitude Indian station Varanasi (Geomag. latitude = 14^{°}55^' }N, long. = 154^{°}E) which is radiated at 250 MHz from geostationary satellite UFO-02 during the period 2011-2012 to investigate the effects of <span class="hlt">geomagnetic</span> storms on VHF scintillation. Various <span class="hlt">geomagnetic</span> and solar indices such as Dst index, Kp index, IMF Bz and solar wind velocity (Vx) are used to describe the <span class="hlt">geomagnetic</span> field <span class="hlt">variation</span> observed during <span class="hlt">geomagnetic</span> storm periods. These indices are very helpful to find out the proper investigation and possible interrelation between <span class="hlt">geomagnetic</span> storms and observed VHF scintillation. The pre-midnight scintillation is sometimes observed when the main phase of <span class="hlt">geomagnetic</span> storm corresponds to the pre-midnight period. It is observed that for <span class="hlt">geomagnetic</span> storms for which the recovery phase starts post-midnight, the probability of occurrence of irregularities is enhanced during this time and extends to early morning hours.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JASTP.170...35K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JASTP.170...35K"><span>Effect of <span class="hlt">geomagnetic</span> storms on the daytime low-latitude thermospheric wave dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Karan, Deepak K.; Pallamraju, Duggirala</p> <p>2018-05-01</p> <p>The equatorial- and low-latitude thermospheric dynamics is affected by both equatorial electrodynamics and neutral wave dynamics, the relative <span class="hlt">variation</span> of which is dependent on the prevalent background conditions, which in turn has a seasonal dependence. Depending on the ambient thermospheric conditions, varying effects of the <span class="hlt">geomagnetic</span> disturbances on the equatorial- and low-latitude thermosphere are observed. To investigate the effect of these disturbances on the equatorial- and low-latitude neutral wave dynamics, daytime airglow emission intensities at OI 557.7 nm, OI 630.0 nm, and OI 777.4 nm are used. These emissions from over a large field-of-view (FOV∼1000) have been obtained using a high resolution slit spectrograph, MISE (Multiwavelength Imaging Spectrograph using Echelle grating), from a low-latitude location, Hyderabad (17.50N, 78.40E; 8.90N MLAT), in India. <span class="hlt">Variations</span> of the dayglow emission intensities are investigated during three <span class="hlt">geomagnetic</span> disturbance events that occurred in different seasons. It is seen that the neutral dayglow emission intensities at all the three wavelengths showed different type of <span class="hlt">variations</span> with the disturbance storm time (Dst) index in different seasons. Even though the dayglow emission intensities over low-latitude regions are sensitive to the <span class="hlt">variation</span> in the equatorial electric fields, during periods of <span class="hlt">geomagnetic</span> disturbances, especially in solstices, these are dependent on thermospheric O/N2 values. This shows the dominance of neutral dynamics over electrodynamics in the low-latitude upper atmosphere during <span class="hlt">geomagnetic</span> disturbances. Further, spectral analyses have been carried out to obtain the zonal scale sizes in the gravity wave regime and their diurnal distributions are compared for <span class="hlt">geomagnetic</span> quiet and disturbed days. Broadly, the zonal scales seem to be breaking into various scale sizes on days of <span class="hlt">geomagnetic</span> disturbances when compared to those on quiet days. This contrast in the diurnal distribution of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Ge%26Ae..58..438N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Ge%26Ae..58..438N"><span><span class="hlt">Geomagnetic</span> Field Intensity during the Neolith in the Central East European Plain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nachasova, I. E.; Pilipenko, O. V.; Markov, G. P.; Gribov, S. K.; Tsetlin, Yu. B.</p> <p>2018-05-01</p> <p>The conducted archeomagnetic studies resulted in data on <span class="hlt">variations</span> in the <span class="hlt">geomagnetic</span> field intensity in the central East European Plain (Sakhtysh I site area, ϕ = 56°48' N, λ = 40°33' E) during the time interval of 5-3 ka BC. The <span class="hlt">geomagnetic</span> field intensity varied mainly within the range of 30-60 μT. In the first half of the 5th millennium BC, the mean level of <span class="hlt">geomagnetic</span> field intensity was about 35 μT. In the second half of the 5th-early 4th millennium BC, it rose to about 50 μT and then decreased again to reach a mean value of about 40 μT in the period of 4-3 ka BC. Comparison of the <span class="hlt">geomagnetic</span> field intensity <span class="hlt">variation</span> based on the obtained data and the data on the Caucasus region for the same time interval demonstrates a certain similarity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19720033993&hterms=inequality&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dinequality','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19720033993&hterms=inequality&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dinequality"><span>The influence of the great inequality on the <span class="hlt">secular</span> disturbing function of the planetary system.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Musen, P.</p> <p>1971-01-01</p> <p>This paper derives the contribution by the great inequality to the <span class="hlt">secular</span> disturbing function of the principal planets. Andoyer's expansion of the planetary disturbing function and von Zeipel's method of eliminating the periodic terms is employed; thereby, the corrected <span class="hlt">secular</span> disturbing function for the planetary system is derived. The conclusion is drawn that the canonicity of the equations for the <span class="hlt">secular</span> <span class="hlt">variation</span> of the heliocentric elements can be preserved if there be retained, in the <span class="hlt">secular</span> disturbing function, terms only of the second and fourth order relative to the eccentricity and inclinations. The Krylov-Bogoliubov method is suggested for eliminating periodic terms, if it is desired to include the <span class="hlt">secular</span> perturbations of the fifth and higher order in the heliocentric elements. The additional part of the <span class="hlt">secular</span> disturbing function derived in this paper can be included in existing theories of the <span class="hlt">secular</span> effects of principal planets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..12212534T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..12212534T"><span>Global Distribution and <span class="hlt">Variations</span> of NO Infrared Radiative Flux and Its Responses to Solar Activity and <span class="hlt">Geomagnetic</span> Activity in the Thermosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, Chaoli; Wei, Yuanyuan; Liu, Dong; Luo, Tao; Dai, Congming; Wei, Heli</p> <p>2017-12-01</p> <p>The global distribution and <span class="hlt">variations</span> of NO infrared radiative flux (NO-IRF) are presented during 2002-2016 in the thermosphere covering 100-280 km altitude based on Sounding of the Atmosphere using Broadband Emission Radiometry (SABER) data set. For investigating the spatial <span class="hlt">variations</span> of the mutual relationship between NO-IRF and solar activity, the altitude ranges from 100 km to 280 km are divided into 90 altitude bins, and the latitude regions of 83°S-83°N are divided into 16 latitude bins. By processing about 1.8E9 NO-IRF observation values from about 5E6 vertical nighttime profiles recorded in SABER data set, we obtained more than 4.1E8 samples of NO-IRF. The annual-mean values of NO-IRF are then calculated by all available NO-IRF samples within each latitude and altitude bin. Local latitudinal maxima in NO-IRF are found between 120 and 145 km altitude, and the maximum NO-IRF located at polar regions are 3 times more than that of the minimum at equatorial region. The influences of solar and <span class="hlt">geomagnetic</span> activity on the spatial <span class="hlt">variations</span> of NO-IRF are investigated. Both the NO-IRF and its response to solar and <span class="hlt">geomagnetic</span> activity show nearly symmetric distribution between the two hemispheres. It is demonstrated that the observed changes in NO-IRF at altitudes between 100 and 225 km correlate well with the changes in solar activity. The NO-IRF at solar maximum is about 4 times than that at solar minimum, and the current maximum of NO-IRF in 2014 is less than 70% of the prior maximum in 2001. For the first time, the response ranges of the NO-IRF to solar and <span class="hlt">geomagnetic</span> activity at different altitudes and latitudes are reported.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006JGRA..111.8209M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JGRA..111.8209M"><span>Centennial increase in <span class="hlt">geomagnetic</span> activity: Latitudinal differences and global estimates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mursula, K.; Martini, D.</p> <p>2006-08-01</p> <p>We study here the centennial change in <span class="hlt">geomagnetic</span> activity using the newly proposed Inter-Hour Variability (IHV) index. We correct the earlier estimates of the centennial increase by taking into account the effect of the change of the sampling of the magnetic field from one sample per hour to hourly means in the first years of the previous century. Since the IHV index is a variability index, the larger variability in the case of hourly sampling leads, without due correction, to excessively large values in the beginning of the century and an underestimated centennial increase. We discuss two ways to extract the necessary sampling calibration factors and show that they agree very well with each other. The effect of calibration is especially large at the midlatitude Cheltenham/Fredricksburg (CLH/FRD) station where the centennial increase changes from only 6% to 24% caused by calibration. Sampling calibration also leads to a larger centennial increase of global <span class="hlt">geomagnetic</span> activity based on the IHV index. The results verify a significant centennial increase in global <span class="hlt">geomagnetic</span> activity, in a qualitative agreement with the aa index, although a quantitative comparison is not warranted. We also find that the centennial increase has a rather strong and curious latitudinal dependence. It is largest at high latitudes. Quite unexpectedly, it is larger at low latitudes than at midlatitudes. These new findings indicate interesting long-term changes in near-Earth space. We also discuss possible internal and external causes for these observed differences. The centennial change of <span class="hlt">geomagnetic</span> activity may be partly affected by changes in external conditions, partly by the <span class="hlt">secular</span> decrease of the Earth's magnetic moment whose effect in near-Earth space may be larger than estimated so far.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....7794A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....7794A"><span>High-Resolution Paleomagnetic Observations from Ocean Drilling: Insights from Coring Thick Sediment Drift Deposits</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Acton, G. D.; Clement, B. M.; Lund, S. P.; Okada, M.; Williams, T.</p> <p>2003-04-01</p> <p>With the advent of the Hydraulic Piston Corer at the end of the Deep Sea Drilling Program and its enhanced successor, the Advanced Piston Corer (APC), developed by the Ocean Drilling Program (ODP), coring through thick (>100 m), rapidly deposited sequences of unconsolidated to partially consolidated sediments with near 100% recovery has become common place. Although much of the emphasis for site selection has been based on paleoceanographic objectives, the impact to the field of paleomagnetism has been dramatic, both in the instruments used to analyze the large quantity of core recovered and in the questions that can be answered concerning <span class="hlt">geomagnetic</span> field behavior and paleoenvironmental conditions. The largest change has come in the construction of relative paleointensity records, which have provided previously unimagined details about how the <span class="hlt">geomagnetic</span> field varies in strength during stable polarity intervals as well as during reversals and excursions. These records have allowed more realistic models of the <span class="hlt">geomagnetic</span> field to be developed while also providing a new chronologic tool for high-resolution dating and global correlation of <span class="hlt">geomagnetic</span> events. Studies of how the paleomagnetic direction varies through time have not advanced as rapidly and have instead mainly been focused on short time intervals across a few <span class="hlt">geomagnetic</span> reversals. It should, however, be possible to construct and compare <span class="hlt">secular</span> <span class="hlt">variation</span> records with millennial or better resolution that span the past one million years from sites around the world as correlation and chronologies between sites improve. We will give an overview that focuses on <span class="hlt">secular</span> <span class="hlt">variation</span> records that are being constructed from sediment drifts drilled in the western North Atlantic during ODP Leg 172. Our results will be used to address questions concerning what percent of time the <span class="hlt">geomagnetic</span> field is in a stable state versus transitional or excursional states, what the relationship is between directional</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015BGeo...12.2131A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015BGeo...12.2131A"><span>Reconstruction of <span class="hlt">secular</span> <span class="hlt">variation</span> in seawater sulfate concentrations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Algeo, T. J.; Luo, G. M.; Song, H. Y.; Lyons, T. W.; Canfield, D. E.</p> <p>2015-04-01</p> <p>Long-term <span class="hlt">secular</span> <span class="hlt">variation</span> in seawater sulfate concentrations ([SO42-]SW) is of interest owing to its relationship to the oxygenation history of Earth's surface environment. In this study, we develop two complementary approaches for quantification of sulfate concentrations in ancient seawater and test their application to late Neoproterozoic (635 Ma) to Recent marine units. The "rate method" is based on two measurable parameters of paleomarine systems: (1) the S-isotope fractionation associated with microbial sulfate reduction (MSR), as proxied by Δ34SCAS-PY, and (2) the maximum rate of change in seawater sulfate, as proxied by &partial; δ 34SCAS/∂ t(max). The "MSR-trend method" is based on the empirical relationship of Δ34SCAS-PY to aqueous sulfate concentrations in 81 modern depositional systems. For a given paleomarine system, the rate method yields an estimate of maximum possible [SO42-]SW (although results are dependent on assumptions regarding the pyrite burial flux, FPY), and the MSR-trend method yields an estimate of mean [SO42-]SW. An analysis of seawater sulfate concentrations since 635 Ma suggests that [SO42-]SW was low during the late Neoproterozoic (<5 mM), rose sharply across the Ediacaran-Cambrian boundary (~5-10 mM), and rose again during the Permian (~10-30 mM) to levels that have varied only slightly since 250 Ma. However, Phanerozoic seawater sulfate concentrations may have been drawn down to much lower levels (~1-4 mM) during short (<~2 Myr) intervals of the Cambrian, Early Triassic, Early Jurassic, and Cretaceous as a consequence of widespread ocean anoxia, intense MSR, and pyrite burial. The procedures developed in this study offer potential for future high-resolution quantitative analyses of paleo-seawater sulfate concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.3747L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.3747L"><span>Detection of the significant <span class="hlt">geomagnetic</span> field signals in the interannual <span class="hlt">variations</span> of Length-of-Day using wavelet method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Genyou; Duan, Pengshuo; Hao, Xiaoguang; Hu, Xiaogang</p> <p>2015-04-01</p> <p>The previous studies indicated that the most of the interannual <span class="hlt">variations</span> in Length-Of-Day (LOD) could be explained by the joint effects of ENSO (EI Nino-Southern Oscillations) and QBO (Quasi-Biennial Oscillation) phenomenon in the atmosphere. Due to the limit of the used methods, those results cannot give the 'time-frequency' coherence spectrum between ENSO and LOD, and cannot indicate in which specific periods the weak coherence occurred and difficult to give the reliable reason. This paper uses Daubechies wavelet with 10 order vanishing moment to analyze the LOD monthly time series from 1962 to 2011. Based on cross-wavelet and wavelet coherence methods, the analysis of the time-frequency correlations between ENSO and LOD series (1962-2011) on the 1.3~10.7 year scales is given. We have extracted and reconstructed the LOD signals on 1.3~10.7year scales. The result shows that there is obvious weak coherence on both biennial and 5~8 year scales after 1982 relative to before 1982. According to the previous works, the biennial weak coherence is due to QBO, but the weak coherence on 5~8 year scales cannot be interpreted by the effects of ENSO and QBO. In this study, the <span class="hlt">Geomagnetic</span> field signals (can be characterized as Aa index) are introduced, we have further extracted and reconstructed the LOD, ENSO and Aa signals in 5-8.0 year band using wavelet packet analysis. Through analyzing the standardized series of the three signals, we found a linear time-frequency formula among the original observation series: LOD(t,f) =αENSO(t,f) +βAa(t,f). This study indicates that the LOD signals on 5.3~8.0 year scales can be expressed in term of linear combination of ENSO and Aa signals. Especially after 1982, the contributions of ENSO and Aa to LOD respectively reach about 0.95ms and 1.0ms.The results also imply that there is an obvious <span class="hlt">Geomagnetic</span> field signal in interannual <span class="hlt">variations</span> of LOD. Furthermore, after considering the <span class="hlt">geomagnetic</span> field signal correction, the Pearson</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27737581','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27737581"><span>Craniofacial <span class="hlt">Secular</span> Change in Recent Mexican Migrants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Spradley, Katherine; Stull, Kyra E; Hefner, Joseph T</p> <p>2016-01-01</p> <p>Research by economists suggests that recent Mexican migrants are better educated and have higher socioeconomic status (SES) than previous migrants. Because factors associated with higher SES and improved education can lead to positive <span class="hlt">secular</span> changes in overall body form, <span class="hlt">secular</span> changes in the craniofacial complex were analyzed within a recent migrant group from Mexico. The Mexican group represents individuals in the act of migration, not yet influenced by the American environment, and thus can serve as a starting point for future studies of <span class="hlt">secular</span> change in this population group. The excavation of a historic Hispanic cemetery in Tucson, Arizona, also allows for a comparison between historic Hispanics and recent migrants to explore craniofacial trends over a broad time period, as both groups originate from Mexico. The present research addresses two main questions: (1) Are cranial <span class="hlt">secular</span> changes evident in recent Mexican migrants? (2) Are historic Hispanics and recent Mexican migrants similar? By studying <span class="hlt">secular</span> changes within a migrant population group, <span class="hlt">secular</span> trends may be detected, which will be important for understanding the biological <span class="hlt">variation</span> of the migrants themselves and will serve as a preliminary investigation of <span class="hlt">secular</span> change within Mexican migrants. The comparison of a sample of recent Mexican migrants with a historic Hispanic sample, predominantly of Mexican origin, allows us to explore morphological similarities and differences between early and recent Mexicans within the United States. Vault and face size and a total of 82 craniofacial interlandmark distances were used to explore <span class="hlt">secular</span> changes within the recent Mexican migrants (females, n = 38; males, n = 178) and to explore the morphological similarities between historic Hispanics (females, n = 54; males, n = 58) and recent migrants. Sexes were separated, and multivariate adaptive regression splines and basis splines (quadratic with one knot) were used to assess the direction and magnitude</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EP%26S...68..154D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EP%26S...68..154D"><span>Estimating ionospheric currents by inversion from ground-based <span class="hlt">geomagnetic</span> data and calculating geoelectric fields for studies of <span class="hlt">geomagnetically</span> induced currents</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Villiers, J. S.; Pirjola, R. J.; Cilliers, P. J.</p> <p>2016-09-01</p> <p>This research focuses on the inversion of <span class="hlt">geomagnetic</span> <span class="hlt">variation</span> field measurements to obtain the source currents in the ionosphere and magnetosphere, and to determine the geoelectric fields at the Earth's surface. During <span class="hlt">geomagnetic</span> storms, the geoelectric fields create <span class="hlt">geomagnetically</span> induced currents (GIC) in power networks. These GIC may disturb the operation of power systems, cause damage to power transformers, and even result in power blackouts. In this model, line currents running east-west along given latitudes are postulated to exist at a certain height above the Earth's surface. This physical arrangement results in the fields on the ground being composed of a zero magnetic east component and a nonzero electric east component. The line current parameters are estimated by inverting Fourier integrals (over wavenumber) of elementary <span class="hlt">geomagnetic</span> fields using the Levenberg-Marquardt technique. The output parameters of the model are the ionospheric current strength and the geoelectric east component at the Earth's surface. A conductivity profile of the Earth is adapted from a shallow layered-Earth model for one observatory, together with a deep-layer model derived from satellite observations. This profile is used to obtain the ground surface impedance and therefore the reflection coefficient in the integrals. The inputs for the model are a spectrum of the <span class="hlt">geomagnetic</span> data for 31 May 2013. The output parameters of the model are spectrums of the ionospheric current strength and of the surface geoelectric field. The inverse Fourier transforms of these spectra provide the time <span class="hlt">variations</span> on the same day. The geoelectric field data can be used as a proxy for GIC in the prediction of GIC for power utilities. The current strength data can assist in the interpretation of upstream solar wind behaviour.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMGP31A..02B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMGP31A..02B"><span>Holocene records of <span class="hlt">geomagnetic</span> field behavior from a north-south transect along the western Antarctic Peninsula</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brachfeld, S. A.; Shah, D. P.; St-Onge, M.; St-Onge, G.</p> <p>2013-12-01</p> <p>Geochronology is inherently difficult when working with Antarctic margin sediments. Radiocarbon dating and oxygen isotope stratigraphy are challenging or impossible in sites with poor preservation of biogenic calcite. Radiocarbon dating of the acid insoluble organic matter (AIOM) is further complicated by organically lean sediment and the presence of reworked organic carbon or detrital carbon from sedimentary rocks. These complications limit the ability to interpret a paleoclimate record. <span class="hlt">Geomagnetic</span> paleointensity dating is a proven 'tuning' technique that has been successfully applied in several studies around the Antarctic margin. However, the reference curves to which these sites were tuned were constructed primarily from Northern Hemisphere data. Here we present paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> (PSV) and relative paleointensity (RPI) data from three Antarctic Peninsula sites that possess independent chronologies and which have moderate to ultra-high sedimentation rates (40 - 700 cm/ka). Maxwell Bay, located in the volcanic South Shetland Islands, is an ultra-high-resolution site with strongly magnetic sediments from which the Shallow Drilling (SHALDRIL) program recovered a 108-m record spanning the last 14 ka. Outer Barilari Bay and Hugo Island Trough, which lie to the South along the western Antarctic Peninsula, are moderate resolution sites with a high proportion of biogenic silica. Maxwell Bay and Bariliari Bay are unique in that they possess homogenous sediment and uniform magnetic mineral assemblages, while also preserving biogenic calcite, a rare combination on the Antarctic margin. All three sites preserve strong, stable remanent magnetizations with an easily isolated characteristic component and MAD values generally < 2°, with the exception of turbidites, intervals with abundant dropstones, and biosiliceous ooze intervals. Inclination values fluctuate between the present-day value at the cores sites (-58°) and the <span class="hlt">geomagnetic</span> axial dipole inclination</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PEPI..173..162H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PEPI..173..162H"><span>Paleomagnetic field <span class="hlt">variation</span> with strong negative inclination during the Brunhes chron at the Banda Sea, equatorial southwestern Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, Yin-Sheng; Lee, Teh-Quei; Hsu, Shu-Kun; Yang, Tein-Nan</p> <p>2009-03-01</p> <p>We reconstruct the earth magnetic field in the Brunhes epoch at the Banda Sea by studying the paleomagnetic data from core MD012380, collected during the International Marine Global Change Study (IMAGES) VII Cruise in 2001. Magnetic analysis is carried out for whole core with a sampling spacing of 1 cm by using u-channel. Magnetic susceptibility (χ), nature remanent magnetization (NRM), anhysteretic remanent magnetization (ARM), and isothermal remanent magnetization (IRM) are measured in our paleomagnetic experiment. Results show the low latitude <span class="hlt">geomagnetic</span> field <span class="hlt">variation</span> at the Banda Sea during the last ∼820 kyr. Except for the Brunhes/Matuyama boundary (BMB), there is no clear signal of reverse events in paleo- inclination and paleo-declination patterns. However, the synthetic paleointensity curve displays the asymmetrical saw-tooth pattern that can be used for determining reverse events, and shows a maximum intensity drop at the BMB. The characteristics of paleointensity provide a useful tool to identify reverse signals and improve the difficulties from only using inclination and declination patterns, especially at low latitude. With the help of paleointensity, inclination and declination, we have identified five reverse events. Furthermore if we consider the <span class="hlt">secular</span> <span class="hlt">variation</span> effect, we think that the strong negative inclination observed in our study may be the zonal time-averaged field with paleo <span class="hlt">secular</span> <span class="hlt">variation</span>, rather than non-dipole effect within the Brunhes epoch.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19068295','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19068295"><span>Compliance of Ultra-Orthodox and <span class="hlt">secular</span> pedestrians with traffic lights in Ultra-Orthodox and <span class="hlt">secular</span> locations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rosenbloom, Tova; Shahar, Amit; Perlman, Amotz</p> <p>2008-11-01</p> <p>Following a previous study that revealed the disobedience of Ultra-Orthodox citizens, as compared to <span class="hlt">secular</span> citizens, of traffic lights at crosswalks, the present study examined the road habits of 995 Ultra-Orthodox and <span class="hlt">secular</span> pedestrians in neighboring Ultra-Orthodox and <span class="hlt">secular</span> cities. Using an observation grid designed specially for this study, the pedestrians were observed at two crosswalks--one in an Ultra-Orthodox city and one in a <span class="hlt">secular</span> city--as far as similar traffic parameters, using a logistic regression. The tendency to cross on a red light was assessed as a function of estimated age, gender, religiosity, location (religious/<span class="hlt">secular</span>), the duration of the red light, the number of vehicles crossing and the number of pedestrians waiting at the curb. Ultra-Orthodox pedestrians committed more violations than <span class="hlt">secular</span> pedestrians did, and there were more road violations in the Ultra-Orthodox location than there were in the <span class="hlt">secular</span> location. Fewer traffic violations were committed by "local" pedestrians (Ultra-Orthodox pedestrians in the Ultra-Orthodox location and <span class="hlt">secular</span> pedestrians in the <span class="hlt">secular</span> location) than by "foreigners" (Ultra-Orthodox pedestrians in the <span class="hlt">secular</span> location and <span class="hlt">secular</span> pedestrians in the Ultra-Orthodox location). The odds of crossing on a red light decreased as a function of both the number of people waiting at the curb and the number of vehicles. Consistent with previous research, males crossed on red much more than females did, regardless of religiosity and location. Our discussion focuses on theoretical and practical explanations of the findings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC41A1003N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC41A1003N"><span>Striking Seasonality in the <span class="hlt">Secular</span> Warming of the Northern Continents: Structure and Mechanisms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nigam, S.; Thomas, N. P.</p> <p>2017-12-01</p> <p>The linear trend in twentieth-century surface air temperature (SAT)—a key <span class="hlt">secular</span> warming signal— exhibits striking seasonal <span class="hlt">variations</span> over Northern Hemisphere continents; SAT trends are pronounced in winter and spring but notably weaker in summer and fall. The SAT trends in historical twentieth-century climate simulations informing the Intergovernmental Panel for Climate Change's Fifth Assessment show varied (and often unrealistic) strength and structure, and markedly weaker seasonal <span class="hlt">variation</span>. The large intra-ensemble spread of winter SAT trends in some historical simulations was surprising, especially in the context of century-long linear trends, with implications for the detection of the <span class="hlt">secular</span> warming signal. The striking seasonality of observed <span class="hlt">secular</span> warming over northern continents warrants an explanation and the representation of related processes in climate models. Here, the seasonality of SAT trends over North America is shown to result from land surface-hydroclimate interactions and, to an extent, also from the <span class="hlt">secular</span> change in low-level atmospheric circulation and related thermal advection. It is argued that the winter dormancy and summer vigor of the hydrologic cycle over middle- to high-latitude continents permit different responses to the additional incident radiative energy from increasing greenhouse gas concentrations. The seasonal cycle of climate, despite its monotony, provides an expanded phase space for the exposition of the dynamical and thermodynamical processes generating <span class="hlt">secular</span> warming, and an exceptional cost-effective opportunity for benchmarking climate projection models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP33B0968S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP33B0968S"><span><span class="hlt">Geomagnetic</span> field intensity <span class="hlt">variations</span> in Northwestern-Central Russia between the 12th and 19th century AD</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salnaia, N.; Gallet, Y.; Genevey, A.; Antipov, I.; Elshin, D.</p> <p>2017-12-01</p> <p>We will present a synthesis of the archeointensity data spanning the past millennium that we recently acquired in the European part of Russia. These data were principally obtained from groups of architectural brick fragments sampled in the Novgorod, Moscow and Yaroslavl areas that are precisely dated between the 12th and the 19th century thanks to archives and archeological constraints. All intensity measurements were carried out using the experimental protocol developed for the Triaxe magnetometer. The reliability of the data is attested through the use of stringent selection criteria on the Triaxe data, rock magnetic experiments and by the use of two different cooling rates for laboratory thermoremanent magnetization acquisition. Altogether the new data show a progressive decrease of the <span class="hlt">geomagnetic</span> field intensities in Northwestern-Central Russia over the past millennium. They do not exhibit large and rapid fluctuations, as those previously reported from the Balkan archeointensity dataset. They further allow us to constrain the dipole moment evolution over the past four centuries. Finally, we will discuss the consistency of the <span class="hlt">geomagnetic</span> field intensity <span class="hlt">variations</span> during the second millennium AD at the entire European scale. The research was supported by RSF (project No. 16-17-10097)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750016136','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750016136"><span>A study of <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Patel, V. L.</p> <p>1975-01-01</p> <p>Twenty-one <span class="hlt">geomagnetic</span> storm events during 1966 and 1970 were studied by using simultaneous interplanetary magnetic field and plasma parameters. Explorer 33 and 35 field and plasma data were analyzed on large-scale (hourly) and small-scale (3 min.) during the time interval coincident with initial phase of the <span class="hlt">geomagnetic</span> storms. The solar-ecliptic Bz component turns southward at the end of the initial phase, thus triggering the main phase decrease in Dst <span class="hlt">geomagnetic</span> field. When the Bz is already negative, its value becomes further negative. The By component also shows large fluctuations along with Bz. When there are no clear changes in the Bz component, the By shows abrupt changes at the main phase onet. On the small-scale behavior of the magnetic field and electric field (E=-VxB) studied in details for the three events, it is found that the field fluctuations in By, Bz and Ey and Ez are present in the initial phase. These fluctuations become larger just before the main phase of the storm begins. In the largescale behavior field remains quiet because the small scale <span class="hlt">variations</span> are averaged out.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.5437U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.5437U"><span>Investigation of the Effects of Solar and <span class="hlt">Geomagnetic</span> Changes on the Total Electron Content: Mid-Latitude Region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ulukavak, Mustafa; Yalcinkaya, Mualla</p> <p>2016-04-01</p> <p>The Global Positioning System (GPS) is used as an important tool for ionosphere monitoring and obtaining the Total Electron Content (TEC). GPS satellites, positioned in the Earth's orbit, are used as sensors to investigate the space weather conditions. In this study, solar and <span class="hlt">geomagnetic</span> activity <span class="hlt">variations</span> were investigated between the dates 1 March-30 June 2015 for the mid-latitude region. GPS-TEC <span class="hlt">variations</span> were calculated for each selected International GNSS Service (IGS) station in Europe. GNSS data was obtained from Crustal Dynamics Data and Information System (CDDIS) archive. Solar and <span class="hlt">geomagnetic</span> activity indices (Kp, F10.7 ve Dst) were obtained from the Oceanic and Atmospheric Administration (NOAA), the Canadian Space Weather Forecast Centre (CSWFC) and Data Analysis Center for <span class="hlt">geomagnetism</span> and Space Magnetism Graduate School of Science, Kyoto University (WDC) archives. GPS-TEC <span class="hlt">variations</span> were determined for the quiet periods of the solar and <span class="hlt">geomagnetic</span> activities. GPS-TEC changes were then compared with respect to the quiet periods of the solar and <span class="hlt">geomagnetic</span> activities. Global Ionosphere Maps (GIM) IONEX files, obtained from the IGS analysis center, was used to check the robustness of the GPS-TEC <span class="hlt">variations</span>. The investigations revealed that it is possible to use the GPS-TEC data for monitoring the ionospheric disturbances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFMSA21B0353H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFMSA21B0353H"><span>The Response of Mid-Latitude Ionospheric TEC to <span class="hlt">Geomagnetic</span> Storms and Solar Flares</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, Z.; Roussel-Dupre, R.</p> <p>2004-12-01</p> <p>The effects of <span class="hlt">geomagnetic</span> storms and solar flares on the ionosphere are manifested as large magnitude sudden fluctuations in the Total Electron Content (TEC). In this study, the broadband VHF signal (30-100MHz) data from the Los Alamos Portable Pulser (LAPP) received by the FORTE (Fast Onboard Recording of Transient Events) satellite during the period of 1997-2002 are used to investigate the mean TEC <span class="hlt">variation</span> response to <span class="hlt">geomagnetic</span> storm. A total of 14 <span class="hlt">geomagnetic</span> storms are selected where FORTE-LAPP data are available to derive average TECs during extended storm-time and non-storm time for a given storm. The <span class="hlt">variations</span> in the ionospheric TECs at Los Alamos, New Mexico are investigated for the 14 selected <span class="hlt">geomagnetic</span> storms. In most cases (12 out of 14), we see overall enhancements in TEC as a result of <span class="hlt">geomagnetic</span> storm impact at Los Alamos. The relative enhancements in TEC at Los Alamos due to a <span class="hlt">geomagnetic</span> storm can reach as high as 3-fold of the normal TEC values. The overall absolute enhancements in TEC at Los Alamos are up to about 30 TECU. The magnitude of TEC enhancements is diversified over all storm categories without a clean-cut relationship between the storm intensity and the TEC enhancement. The mean TEC <span class="hlt">variation</span> response to <span class="hlt">geomagnetic</span> storm can be complicated when several consecutive storms occurred in a row and a net TEC reduction may be seen. Data of continuous GPS TEC measurements are collected at a 1-minute time resolution during July 2004 when 5 X-class solar flares occurred from two Allen Osborne Associates ICS-4000Z GPS receivers mounted at the Physics Building at Los Alamos National Laboratory. In detecting effects of solar flares on the ionospheric TEC, we apply appropriate filtering to remove the linear trend of TEC and a coherent processing of TEC <span class="hlt">variations</span> simultaneously for all the visible GPS satellites in a given time interval. The responses of ionospheric TEC at minute time scale to these powerful impulsive solar flares are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvD..91d4009M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvD..91d4009M"><span>Cosmological <span class="hlt">variation</span> of the MOND constant: <span class="hlt">Secular</span> effects on galactic systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Milgrom, Mordehai</p> <p>2015-02-01</p> <p>The proximity of the MOND acceleration constant with cosmological accelerations—for example, a0≈c H0/2 π —points to its possibly decreasing with cosmic time. I begin to consider the <span class="hlt">secular</span> changes induced in galactic systems by such presumed <span class="hlt">variations</span>, which are assumed to be adiabatic. It is important to understand these effects, in isolation from other evolutionary influences, in order to identify or constrain a0 <span class="hlt">variations</span> by detection of induced effects, or lack thereof. I find that as long as the system is fully in the deep-MOND regime—as applies to many galactic systems—the adiabatic response of the system obeys simple scaling laws. For example, in a system that would be stationary for fixed a0, the system expands homologously as a0-1 /4, while internal velocities decrease uniformly as a01 /4. If a0∝c H at all relevant times, this change amounts to a factor of ˜2.5 since redshift 10. For rotating systems, the angular frequency Ω ∝a01 /2. The accelerations increase relative to a0 as a0-1 /4, pushing the system towards the Newtonian regime. All this follows from the appearance of a0 in MOND and the scale invariance of the deep-MOND limit—two basic tenets of MOND. More complicated evolution ensues when parts of the system become Newtonian, or are so from inception. For example, these parts may become unstable since they are not protected by MOND's stabilizing effects. The existence of such regions also modifies the MONDian regime since they affect the potential everywhere, and constituents might migrate between the Newtonian and MONDian regimes. Studying these last effects would require detailed numerical calculations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EP%26S...69..112F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EP%26S...69..112F"><span><span class="hlt">Geomagnetically</span> conjugate observations of ionospheric and thermospheric <span class="hlt">variations</span> accompanied by a midnight brightness wave at low latitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fukushima, D.; Shiokawa, K.; Otsuka, Y.; Kubota, M.; Yokoyama, T.; Nishioka, M.; Komonjinda, S.; Yatini, C. Y.</p> <p>2017-08-01</p> <p>We conducted <span class="hlt">geomagnetically</span> conjugate observations of 630-nm airglow for a midnight brightness wave (MBW) at Kototabang, Indonesia [<span class="hlt">geomagnetic</span> latitude (MLAT): 10.0°S], and Chiang Mai, Thailand (MLAT: 8.9°N), which are <span class="hlt">geomagnetically</span> conjugate points at low latitudes. An airglow enhancement that was considered to be an MBW was observed in OI (630-nm) airglow images at Kototabang around local midnight from 2240 to 2430 LT on February 7, 2011. This MBW propagated south-southwestward, which is <span class="hlt">geomagnetically</span> poleward, at a velocity of 290 m/s. However, a similar wave was not observed in the 630-nm airglow images at Chiang Mai. This is the first evidence of an MBW that does not have <span class="hlt">geomagnetic</span> conjugacy, which also implies generation of MBW only in one side of the hemisphere from the equator. We simultaneously observed thermospheric neutral winds observed by a co-located Fabry-Perot interferometer at Kototabang. The observed meridional winds turned from northward (<span class="hlt">geomagnetically</span> equatorward) to southward (<span class="hlt">geomagnetically</span> poleward) just before the wave was observed. This indicates that the observed MBW was generated by the poleward winds which push ionospheric plasma down along <span class="hlt">geomagnetic</span> field lines, thereby increasing the 630-nm airglow intensity. The bottomside ionospheric heights observed by ionosondes rapidly decreased at Kototabang and slightly increased at Chiang Mai. We suggest that the polarization electric field inside the observed MBW is projected to the northern hemisphere, causing the small height increase observed at Chiang Mai. This implies that electromagnetic coupling between hemispheres can occur even though the original disturbance is caused purely by the neutral wind.[Figure not available: see fulltext.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17663172','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17663172"><span>[<span class="hlt">Geomagnetic</span> field <span class="hlt">variations</span> in the human prenatal period and cancer in adults].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Iamshanov, V A</p> <p>2007-01-01</p> <p>Our earlier evidence pointed to a relationship between <span class="hlt">geomagnetic</span> field (GMF) <span class="hlt">variations</span> in pre- and early postnatal periods and appearance in the future of oncopathology in these patients. It appears to contribute to risk for such malignancies in adults as breast, lung, liver, bladder, kidney, prostate, hypophysis cancer, ovarian carcinoma, skin melanoma, Hodgkin's disease, lymphoma, and probably stomach cancer. No link was detected between esophageal, thyroid, colorectal cancer or cervical carcinoma, on the one hand, and GMF <span class="hlt">variations</span> in prenatal period, on the other. It is suggested that low intensity of GMF is associated with increased death of macrophages and other granulocytes as well as nitric oxide formation both in fetal and maternal organism. The latter factor induces genes responsible for detoxication. In adults, under normal or disturbed GMF conditions, detoxication processes take care of excessive blood-nitric oxide. Both in fetus and mother, due to high GMF intensity, granulocyte decay is inhibited thus causing nitric oxide levels to fall. As a consequence, detoxication fails. That accounts for excessive blood-nitric oxide formation at adult stage when GMF intensity is low or normal. Nitric oxide causes certain nitrosamines to form, which are tissue-specific carcinogens. Therefore, the lower level of GMF oscillations was in pre- and early postnatal periods than in more late terms tumors appeared (for example, the negative correlation for breast cancer took place).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA43B2662O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA43B2662O"><span>A Study of Ionospheric Storm Association with Intense <span class="hlt">Geomagnetic</span> Storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okpala, K. C.</p> <p>2017-12-01</p> <p>The bulk association between ionospheric storms and <span class="hlt">geomagnetic</span> storms have been studied. Hemispheric features of seasonal <span class="hlt">variation</span> of ionospheric storms in the mid-latitude were also investigated. 188 intense <span class="hlt">geomagnetic</span> storms (Dst ≤100nT) that occurred during solar cycle 22 and 23 were considered, of which 143 were observed to be identified with an ionospheric storm. Individual ionospheric storms were identified as maximum deviations of the F2 layer peak electron density from quiet time values. Only ionospheric storms that could clearly be associated with the peak of a <span class="hlt">geomagnetic</span> storms were considered. Data from two mid-latitude ionosonde stations; one in the northern hemisphere (i.e Moscow) and the other in the southern hemisphere (Grahamstown) were used to study ionospheric condition at the time of the individual <span class="hlt">geomagnetic</span> storms. Results show hemispheric and latitudinal differences in the intensity and nature of ionospheric storms association with different types of <span class="hlt">geomagnetic</span> storms. These results are significant for our present understanding of the mechanisms which drive the changes in electron density during different types of ionospheric storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984gwd....29..255P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984gwd....29..255P"><span>Seasonal <span class="hlt">variations</span> of reflexibility and transmissibility of ULF waves propagating through the ionosphere of <span class="hlt">geomagnetic</span> mid-latitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prikner, K.</p> <p></p> <p>Using reference models of the daytime and night ionosphere of <span class="hlt">geomagnetic</span> mid-latitudes in a quiescent period in summer, autumn and winter, the seasonal <span class="hlt">variation</span> of ULF frequency characteristics of amplitude and energy correction factors of the ionosphere - vertical reflexibility, transmissibility, are studied. The existence of two frequency bands within the ULF range with different properties of ionospheric wave filtration is pointed out: (1) continuous band f 0.1-0.2 Hz with the mirror effect of the ionosphere with respect to the incident wave, but with small ionospheric absorption of wave energy; (2) the f 0.2 Hz band with resonance frequency windows and wave emissions with a sharply defined frequency structure. The seasonal <span class="hlt">variation</span> from summer to winter indicates a decrease in wave energy absorption in the ionosphere and a slight displacement of the resonances towards higher frequencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1611550G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1611550G"><span>The disturbed <span class="hlt">geomagnetic</span> field at European observatories. Sources and significance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Greculeasa, Razvan; Dobrica, Venera; Demetrescu, Crisan</p> <p>2014-05-01</p> <p>The disturbed <span class="hlt">geomagnetic</span> field recorded at Earth's surface is given by the effects of electric current systems in the magnetosphere and ionosphere, as a result of the interaction of <span class="hlt">geomagnetic</span> field with the solar wind and the interplanetary magnetic field. In this paper the <span class="hlt">geomagnetic</span> disturbance recorded at European observatories has been investigated as regards its sources, for the time interval August 1-10, 2010, in which a moderate storm (Dstmin= -70 nT) occurred (August 3-4). The disturbance has been evidenced against the solar quiet daily <span class="hlt">variation</span>, for each of the 29 observatories with minute data in the mentioned time interval. Data have been downloaded from the INTERMAGNET web page. The contribution of the magnetospheric ring current and of the auroral electrojet to the observed disturbance field in the X, Z, and D <span class="hlt">geomagnetic</span> elements is discussed and the corresponding geographical distribution is presented.</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('https://www.osti.gov/biblio/7061389-structure-secular-variation-seawater-sup-sr-sup-sr-ivorian-chadian-osagean-lower-carboniferous','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/7061389-structure-secular-variation-seawater-sup-sr-sup-sr-ivorian-chadian-osagean-lower-carboniferous"><span>Structure in the <span class="hlt">secular</span> <span class="hlt">variation</span> of seawater sup 87 Sr/ sup 86 Sr for the Ivorian/Chadian (Osagean, Lower Carboniferous)</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>Douthit, T.L.; Hanson, G.N.; Meyers, W.J.</p> <p>1990-05-01</p> <p>The <span class="hlt">secular</span> <span class="hlt">variations</span> of {sup 87}Sr/{sup 86}Sr in seawater for the Ivorian/Chadian, (equivalent to the Osagean, Lower Carboniferous) were determined through detailed analysis of well-preserved marine cements from the Waulsortian facies of Ireland. The results indicate that marine cements have utility in characterizing marine paleochemistries. Marine cements were judged pristine on the basis of nonluminescent character and stable isotopic composition comparable to previous estimates of Mississippian marine calcite. Analysis of the marine cements yielded {sup 87}Sr/{sup 86}Sr ratios lower than previously reported values for the Ivorian/Chadian. Error resulting from chronostratigraphic correlation between different geographic areas was avoided by restricting themore » sample set to a single 1,406-ft-long core (core P-1). The P-1 core is estimated to represent a minimum of 8.7 m.y. of continuous Waulsortian Limestone deposition. The {sup 87}Sr/{sup 86}Sr ratios of 11 nonluminescent cements document a non-monotonic <span class="hlt">variation</span> in seawater {sup 87}Sr/{sup 86}Sr along the length of the core. {sup 87}Sr/{sup 86}Sr ranges from a high of 0.707908 in the early Ivorian to a low of about 0.707650 in the late Ivorian and middle Chadian with an early Chadian maximum at 0.707800 (all data are adjusted to a value of 0.710140 for SRM 987). The indicated maximum rate of change in seawater {sup 87}Sr/{sup 86}Sr is {minus}0.00011/Ma, comparable in magnitude to Tertiary values. The <span class="hlt">secular</span> <span class="hlt">variation</span> curve of seawater {sup 87}Sr/{sup 86}Sr for the Ivorian/Chadian has previously been thought to decrease monotonically with decreasing age. These data suggest that the seawater {sup 87}Sr/{sup 86}Sr <span class="hlt">variation</span> over this interval may be sinusoidal in nature and emphasize the importance of well-characterized intraformational isotopic base lines.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013seg..book.....F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013seg..book.....F"><span><span class="hlt">Secular</span> Evolution of Galaxies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Falcón-Barroso, Jesús; Knapen, Johan H.</p> <p>2013-10-01</p> <p>Preface; 1. <span class="hlt">Secular</span> evolution in disk galaxies John Kormendy; 2. Galaxy morphology Ronald J. Buta; 3. Dynamics of <span class="hlt">secular</span> evolution James Binney; 4. Bars and <span class="hlt">secular</span> evolution in disk galaxies: theoretical input E. Athanassoula; 5. Stellar populations Reynier F. Peletier; 6. Star formation rate indicators Daniela Calzetti; 7. The evolving interstellar medium Jacqueline van Gorkom; 8. Evolution of star formation and gas Nick Z. Scoville; 9. Cosmological evolution of galaxies Isaac Shlosman.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18225664','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18225664"><span>[Seasonal <span class="hlt">variations</span> in the myocardial infarction incidence and possible effects of <span class="hlt">geomagnetic</span> micropulsations on the cardiovascular system in humans].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kleĭmenova, N G; Kozyreva, O V; Breus, T K; Rapoport, S I</p> <p>2007-01-01</p> <p>The analysis of the ambulance calls in Moscow, related to myocardial infarction (85.000 events), sudden death (71.700 events), and hypertension crises (165.500 events) over the period of 1979-1981 demonstrated their clear seasonal <span class="hlt">variations</span> with a profound summer minimum and a winter maximum. The same results were obtained in the analysis of statistical monthly data on sudden death from infarction in Bulgaria over the period of 15 years (1970-1985). However, there are a great number of clinical and statistical studies confirming the rises in the incidence of myocardial infarction, hypertension crise, and sudden death during <span class="hlt">geomagnetic</span> disturbances, which have maximum occurrence near equinox, not in winter. In order to explain this contradiction, we suggested that one of critical factors that affect the human cardiovascular system is <span class="hlt">geomagnetic</span> micropulsations Pc1 having the frequency comparable with the frequency of heart rate beatings and winter maximum in their occurrence. The results of a comparative analysis of data of ambulance calls in Moscow related to myocardial infarction and sudden death and the catalog of Pc1 observations at the geophysical observatory "Borok" (Yaroslavl region) are presented. It is shown that in approximately 70% of days with an anomalously large number of ambulance calls related to myocardial infarction, Pc1 micropulsations have been registered. The probability of simultaneous occurrence of myocardial infarction and Pc1 in the winter season was 1.5 times greater than their accidental coincidence. Moreover, it was found that in winter the effects of magnetic storms and Pc1 IM(A) were much higher than in summer. We suggested that one of possible reasons for the seasonal <span class="hlt">variations</span> in the occurrence of myocardial infarction is an increase in the production of the pineal hormone melatonin in winter which leads to an unstable state of the human organism and an increase in its sensitivity to the effect of <span class="hlt">geomagnetic</span> pulsations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29295588','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29295588"><span>A Study on the Model of Detecting the <span class="hlt">Variation</span> of <span class="hlt">Geomagnetic</span> Intensity Based on an Adapted Motion Strategy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Hong; Liu, Mingyong; Liu, Kun; Zhang, Feihu</p> <p>2017-12-25</p> <p>By simulating the <span class="hlt">geomagnetic</span> fields and analyzing thevariation of intensities, this paper presents a model for calculating the objective function ofan Autonomous Underwater Vehicle (AUV)<span class="hlt">geomagnetic</span> navigation task. By investigating the biologically inspired strategies, the AUV successfullyreachesthe destination duringgeomagnetic navigation without using the priori <span class="hlt">geomagnetic</span> map. Similar to the pattern of a flatworm, the proposed algorithm relies on a motion pattern to trigger a local searching strategy by detecting the real-time <span class="hlt">geomagnetic</span> intensity. An adapted strategy is then implemented, which is biased on the specific target. The results show thereliabilityandeffectivenessofthe proposed algorithm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMED31B0862M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMED31B0862M"><span>Investigation of Characteristics of Large dB/dt for <span class="hlt">Geomagnetically</span> Induced Currents</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Munoz, D.; Ngwira, C.; Damas, M. C.</p> <p>2016-12-01</p> <p>When <span class="hlt">geomagnetically</span> induced currents (GICs) flow through electrical networks, they become a potential threat for electrical power systems. Changes in the <span class="hlt">geomagnetic</span> field (dB/dt) during severe <span class="hlt">geomagnetic</span> disturbances are the main sources of GICs. These dB/dt phenomena were studied by selecting 24 strong <span class="hlt">geomagnetic</span> storms with Dst ≤ - 150 nT. ACE spacecraft solar wind data: flow speed, proton density, By and Bz IMF components of the solar wind were correlated with measurements of the magnetic field detected on ground stations at different latitudes. This article reports characteristics of the solar wind during time intervals of large changes in the horizontal <span class="hlt">geomagnetic</span> field with a threshold of dB/dt ≥ ± 20 nT/min for the 24 <span class="hlt">geomagnetic</span> storms. The results of this investigation can help scientists to understand the mechanisms responsible for causing large magnetic field <span class="hlt">variations</span> in order to predict and mitigate possible large events in the future, which is critical for our society that relies constantly on electricity for livelihood and security. In addition, this ongoing project will continue to investigate electron flux response before, during, and after large changes in <span class="hlt">geomagnetic</span> field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRA..119.3077K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRA..119.3077K"><span>Advantage of wavelet technique to highlight the observed <span class="hlt">geomagnetic</span> perturbations linked to the Chilean tsunami (2010)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klausner, V.; Mendes, Odim; Domingues, Margarete O.; Papa, Andres R. R.; Tyler, Robert H.; Frick, Peter; Kherani, Esfhan A.</p> <p>2014-04-01</p> <p>The vertical component (Z) of the <span class="hlt">geomagnetic</span> field observed by ground-based observatories of the International Real-Time Magnetic Observatory Network has been used to analyze the induced magnetic fields produced by the movement of a tsunami, electrically conducting sea water through the <span class="hlt">geomagnetic</span> field. We focus on the survey of minutely sampled <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> induced by the tsunami of 27 February 2010 at Easter Island (IPM) and Papeete (PPT) observatories. In order to detect the tsunami disturbances in the <span class="hlt">geomagnetic</span> data, we used wavelet techniques. We have observed an 85% correlation between the Z component <span class="hlt">variation</span> and the tide gauge measurements in period range of 10 to 30 min which may be due to two physical mechanisms: gravity waves and the electric currents in the sea. As an auxiliary tool to verify the disturbed magnetic fields, we used the maximum variance analysis (MVA). At PPT, the analyses show local magnetic <span class="hlt">variations</span> associated with the tsunami arriving in advance of sea surface fluctuations by about 2 h. The first interpretation of the results suggests that wavelet techniques and MVA can be effectively used to characterize the tsunami contributions to the <span class="hlt">geomagnetic</span> field and further used to calibrate tsunami models and implemented to real-time analysis for forecast tsunami scenarios.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5406004','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5406004"><span>Error model of <span class="hlt">geomagnetic</span>-field measurement and extended Kalman-filter based compensation method</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ge, Zhilei; Liu, Suyun; Li, Guopeng; Huang, Yan; Wang, Yanni</p> <p>2017-01-01</p> <p>The real-time accurate measurement of the <span class="hlt">geomagnetic</span>-field is the foundation to achieving high-precision <span class="hlt">geomagnetic</span> navigation. The existing <span class="hlt">geomagnetic</span>-field measurement models are essentially simplified models that cannot accurately describe the sources of measurement error. This paper, on the basis of systematically analyzing the source of <span class="hlt">geomagnetic</span>-field measurement error, built a complete measurement model, into which the previously unconsidered <span class="hlt">geomagnetic</span> daily <span class="hlt">variation</span> field was introduced. This paper proposed an extended Kalman-filter based compensation method, which allows a large amount of measurement data to be used in estimating parameters to obtain the optimal solution in the sense of statistics. The experiment results showed that the compensated strength of the <span class="hlt">geomagnetic</span> field remained close to the real value and the measurement error was basically controlled within 5nT. In addition, this compensation method has strong applicability due to its easy data collection and ability to remove the dependence on a high-precision measurement instrument. PMID:28445508</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.U21C0630L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.U21C0630L"><span>Annual, Seasonal, and <span class="hlt">Secular</span> Changes in Time-Variable Gravity from GRACE</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lemoine, F. G.; Luthcke, S. B.; Klosko, S. M.; Rowlands, D. D.; Chinn, D. S.; McCarthy, J. J.; Ray, R. D.; Boy, J.</p> <p>2007-12-01</p> <p>The NASA/DLR GRACE mission, launched in 2002, has now operated for more than five years, producing monthly and ten-day snapshots of the <span class="hlt">variations</span> of the gravity field of the Earth. The available solutions, either from spherical harmonics or from mascons, allow us new insights into the <span class="hlt">variations</span> of surface gravity on the Earth at annual, inter-annual, and <span class="hlt">secular</span> time scales. Our baseline time series, based on GGM02C, NCEP Atmospheric Gravity with IB, and GOT00 tides now is extended to July 2007, spanning four+ years, and we analyze both mascon and spherical harmonic solutions from this time series with respect to global hydrology <span class="hlt">variations</span>. Our 4degx4deg mascon solutions are extended to cover all continental regions of the globe. Comparisons with hydrology (land-surface) models can offer insights into how these models might be improved. We compare our baseline time series, with new time series that include an updated Goddard Ocean Tide (GOT) model, ECMWF- 3hr atmosphere de-aliasing data, and the MOG-2D ocean dealiasing product. Finally, we intercompare the spherical harmonic solutions at low degree from GRACE from the various product centers (e.g., GFZ, CSR, GRGS), and look for <span class="hlt">secular</span> signals in both the GSFC mascon and spherical harmonic solutions, taking care to compare the results for <span class="hlt">secular</span> gravity field change with independent solutions developed over 25 years of independent tracking to geodetic satellites by Satellite Laser Ranging (SLR) and DORIS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=conflict+AND+management&pg=7&id=EJ900152','ERIC'); return false;" href="https://eric.ed.gov/?q=conflict+AND+management&pg=7&id=EJ900152"><span>The Incidence and Management of Conflicts in <span class="hlt">Secular</span> and Non-<span class="hlt">Secular</span> Tertiary Institutions in South West Nigeria</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>Ayodele, Joseph Babatola; Adewumi, Joseph Olukayode</p> <p>2007-01-01</p> <p>This paper compared the incidence and management of conflicts in <span class="hlt">secular</span> and non-<span class="hlt">secular</span> tertiary institutions in Nigeria. The sample of this study was made of sixty staff, and two hundred and forty students randomly selected each from two <span class="hlt">secular</span> and two non-<span class="hlt">secular</span> tertiary institutions in south western Nigeria. A validated questionnaire was…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123..567S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123..567S"><span><span class="hlt">Variations</span> of High-Latitude <span class="hlt">Geomagnetic</span> Pulsation Frequencies: A Comparison of Time-of-Flight Estimates and IMAGE Magnetometer Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sandhu, J. K.; Yeoman, T. K.; James, M. K.; Rae, I. J.; Fear, R. C.</p> <p>2018-01-01</p> <p>The fundamental eigenfrequencies of standing Alfvén waves on closed <span class="hlt">geomagnetic</span> field lines are estimated for the region spanning 5.9≤L < 9.5 over all MLT (Magnetic Local Time). The T96 magnetic field model and a realistic empirical plasma mass density model are employed using the time-of-flight approximation, refining previous calculations that assumed a relatively simplistic mass density model. An assessment of the implications of using different mass density models in the time-of-flight calculations is presented. The calculated frequencies exhibit dependences on field line footprint magnetic latitude and MLT, which are attributed to both magnetic field configuration and spatial <span class="hlt">variations</span> in mass density. In order to assess the validity of the time-of-flight calculated frequencies, the estimates are compared to observations of FLR (Field Line Resonance) frequencies. Using IMAGE (International Monitor for Auroral <span class="hlt">Geomagnetic</span> Effects) ground magnetometer observations obtained between 2001 and 2012, an automated FLR identification method is developed, based on the cross-phase technique. The average FLR frequency is determined, including <span class="hlt">variations</span> with footprint latitude and MLT, and compared to the time-of-flight analysis. The results show agreement in the latitudinal and local time dependences. Furthermore, with the use of the realistic mass density model in the time-of-flight calculations, closer agreement with the observed FLR frequencies is obtained. The study is limited by the latitudinal coverage of the IMAGE magnetometer array, and future work will aim to extend the ground magnetometer data used to include additional magnetometer arrays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984TraGe..29..255P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984TraGe..29..255P"><span>Seasonal <span class="hlt">variations</span> of reflexibility and transmissibility of ULF waves propagating through the ionosphere of <span class="hlt">geomagnetic</span> mid-latitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prikner, K.</p> <p></p> <p>Using reference models of the daytime and night ionosphere of <span class="hlt">geomagnetic</span> mid-latitudes in a quiescent period in summer, autumn and winter, the seasonal <span class="hlt">variation</span> of ULF frequency characteristics of amplitude and energy correction factors of the ionosphere - vertical reflexibility, transmissibility and absorption, are studied. The existence of two frequency bands within the ULF range with different properties of ionospheric wave filtration is pointed out: (a) continuous band f of less than 0.1 to 0.2 Hz with the mirror effect of the ionosphere with respect to the incident wave, but with small ionospheric absorption of wave energy; and (b) a Hz band of greater than 0.2 Hz with resonance frequency windows and wave emissions with a sharply defined frequency structure. The seasonal <span class="hlt">variation</span> from summer to winter indicates a decrease in wave energy absorption in the ionosphere and a slight displacement of the resonances towards higher frequencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Ge%26Ae..58...36K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Ge%26Ae..58...36K"><span>Paleointensity Behavior and Intervals Between <span class="hlt">Geomagnetic</span> Reversals in the Last 167 Ma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kurazhkovskii, A. Yu.; Kurazhkovskaya, N. A.; Klain, B. I.</p> <p>2018-01-01</p> <p>The results of comparative analysis of the behavior of paleointensity and polarity (intervals between reversals) of the <span class="hlt">geomagnetic</span> field for the last 167 Ma are presented. Similarities and differences in the behavior of these characteristics of the <span class="hlt">geomagnetic</span> field are discussed. It is shown that bursts of paleointensity and long intervals between reversals occurred at high mean values of paleointensity in the Cretaceous and Paleogene. However, there are differences between the paleointensity behavior and the reversal regime: (1) the characteristic times of paleointensity <span class="hlt">variations</span> are less than the characteristic times of the frequency of <span class="hlt">geomagnetic</span> reversals, (2) the achievement of maximum values of paleointensity at the Cretaceous-Paleogene boundary and the termination of paleointensity bursts after the boundary of 45-40 Ma are not marked by explicit features in the <span class="hlt">geomagnetic</span> polarity behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013GeoJI.195.1519B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013GeoJI.195.1519B"><span>High-resolution record of the Laschamp <span class="hlt">geomagnetic</span> excursion at the Blake-Bahama Outer Ridge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bourne, Mark D.; Mac Niocaill, Conall; Thomas, Alex L.; Henderson, Gideon M.</p> <p>2013-12-01</p> <p><span class="hlt">Geomagnetic</span> excursions are brief deviations of the <span class="hlt">geomagnetic</span> field from behaviour expected during `normal <span class="hlt">secular</span>' <span class="hlt">variation</span>. The Laschamp excursion at ˜41 ka was one such deviation. Previously published records suggest rapid changes in field direction and a concurrent substantial decrease in field intensity associated with this excursion. Accurate dating of excursions, and determination of their durations from multiple locations, is vital to our understanding of global field behaviour during these deviations. We present here high-resolution palaeomagnetic records of the Laschamp excursion obtained from two Ocean Drilling Program (ODP) Sites, 1061 and 1062 on the Blake-Bahama Outer Ridge (ODP Leg 172). High sedimentation rates (˜30-40 cm kyr-1) at these locations allow determination of transitional field behaviour during the excursion. Palaeomagnetic measurements of discrete samples from four cores reveal a single excursional feature, across an interval of 30 cm, associated with a broader palaeointensity low. We determine the age and duration of the Laschamp excursion using a stratigraphy linked to the δ18O record from the Greenland ice cores. This chronology dates the Laschamp excursion at the Blake Ridge to 41.3 ka. The excursion is characterized by rapid transitions (less than 200 yr) between stable normal polarity and a partially reversed polarity state. The palaeointensity record is in good agreement between the two sites, revealing two prominent minima. The first minimum is associated with the Laschamp excursion at 41 ka and the second corresponds to the Mono Lake excursion at ˜35.5 ka. We determine that the directional excursion during the Laschamp at this location was no longer than ˜400 yr, occurring within a palaeointensity minimum that lasted 2000 yr. The Laschamp excursion at this location is much shorter in duration than the Blake and Iceland Basin excursions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61.1858O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61.1858O"><span>On the mid-latitude ionospheric storm association with intense <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okpala, Kingsley Chukwudi; Ogbonna, Chinasa Edith</p> <p>2018-04-01</p> <p>The bulk association between ionospheric storms and <span class="hlt">geomagnetic</span> storms has been studied. Hemispheric features of seasonal <span class="hlt">variation</span> of ionospheric storms in the mid-latitude were also investigated. 188 intense <span class="hlt">geomagnetic</span> storms (Dst ≤ 100 nT) that occurred during solar cycles 22 and 23 were considered, of which 143 were observed to be identified with an ionospheric storm. Individual ionospheric storms were identified as maximum deviations of the F2 layer peak electron density from quiet time values. Only ionospheric storms that could clearly be associated with the peak of a <span class="hlt">geomagnetic</span> storm were considered. Data from two mid-latitude ionosonde stations; one in the northern hemisphere (i.e. Moscow) and the other in the southern hemisphere (Grahamstown) were used to study ionospheric conditions at the time of the individual <span class="hlt">geomagnetic</span> storms. Results show hemispheric and latitudinal differences in the intensity and nature of ionospheric storms association with different types of <span class="hlt">geomagnetic</span> storms. These results are significant for our present understanding of the mechanisms which drive the changes in electron density during different types of ionospheric storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUSMGP21A..03H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUSMGP21A..03H"><span>Ultrasensitive <span class="hlt">Geomagnetic</span> Field Temporal <span class="hlt">Variations</span> and its Relationship to Stress in the Earth's Crust: an Experiment in the Oaxaca Coast, Mexico.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hernandez, J.; Cifuentes-Nava, G.; Cabral-Cano, E.; Hrvoic, I.; Lopez, F.; Wilson, M.</p> <p>2007-05-01</p> <p>We present the different assignments developed since June 2004 designed to set up an ultrasensitive magnetometer (Supergrad) built by GEM Systems (Canada). Several <span class="hlt">geomagnetic</span> surveys, micro-surveys, regional profiles, and Declination-Inclination absolute measurements were carried out, as well as magnetic diurnal <span class="hlt">variation</span> recording during these tasks. The objective was to reveal areas with a stable magnetic anisotropy inside the site of at least a 200m X 400m area, in order to install three supergradiometer's high sensitivity potassium sensors. This project is undergoing in one of the most seismogenic areas in Mexico: El Trapiche, San Francisco Cozoaltepec, in Santa Maria Tonameca municipality (state of Oaxaca). Different methods of measurement are assessed and a short base gradient method explained. Supersensitive (50fT), potassium 3 sensor gradiometer is described and some field data presented. In the up-to-date significant investments in Earthquake studies and especially in detection of Earthquake precursors there is a lot of emotional and in general non-critical measurements of precursors. We are trying to establish some kind of reference conditions for detection of precursors. For this purpose we are supported by the Supergrad resolution (0.001 pT) and sampling rate (20 Hz). At the same time, a <span class="hlt">Geomagnetic</span> data-base will be achieved in order to examine the relationship between Earth crust stress and its influence in local <span class="hlt">geomagnetic</span> field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011CosRe..49...21Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011CosRe..49...21Y"><span>Statistical study of interplanetary condition effect on <span class="hlt">geomagnetic</span> storms: 2. <span class="hlt">Variations</span> of parameters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yermolaev, Yu. I.; Lodkina, I. G.; Nikolaeva, N. S.; Yermolaev, M. Yu.</p> <p>2011-02-01</p> <p>We investigate the behavior of mean values of the solar wind’s and interplanetary magnetic field’s (IMF) parameters and their absolute and relative <span class="hlt">variations</span> during the magnetic storms generated by various types of the solar wind. In this paper, which is a continuation of paper [1], we, on the basis of the OMNI data archive for the period of 1976-2000, have analyzed 798 <span class="hlt">geomagnetic</span> storms with D st ≤ -50 nT and their interplanetary sources: corotating interaction regions CIR, compression regions Sheath before the interplanetary CMEs; magnetic clouds MC; “Pistons” Ejecta, and an uncertain type of a source. For the analysis the double superposed epoch analysis method was used, in which the instants of the magnetic storm onset and the minimum of the D st index were taken as reference times. It is shown that the set of interplanetary sources of magnetic storms can be sub-divided into two basic groups according to their slowly and fast varying characteristics: (1) ICME (MC and Ejecta) and (2) CIR and Sheath. The mean values, the absolute and relative <span class="hlt">variations</span> in MC and Ejecta for all parameters appeared to be either mean or lower than the mean value (the mean values of the electric field E y and of the B z component of IMF are higher in absolute value), while in CIR and Sheath they are higher than the mean value. High values of the relative density <span class="hlt">variation</span> sN/< N> are observed in MC. At the same time, the high values for relative <span class="hlt">variations</span> of the velocity, B z component, and IMF magnitude are observed in Sheath and CIR. No noticeable distinctions in the relationships between considered parameters for moderate and strong magnetic storms were observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010cosp...38.2135R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38.2135R"><span>Long periods (1 -10 mHz) <span class="hlt">geomagnetic</span> pulsations <span class="hlt">variation</span> with solar cycle in South Atlantic Magnetic Anomaly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rigon Silva, Willian; Schuch, Nelson Jorge; Guimarães Dutra, Severino Luiz; Babulal Trivedi, Nalin; Claudir da Silva, Andirlei; Souza Savian, Fernando; Ronan Coelho Stekel, Tardelli; de Siqueira, Josemar; Espindola Antunes, Cassio</p> <p></p> <p>The occurrence and intensity of the <span class="hlt">geomagnetic</span> pulsations Pc-5 (2-7 mHz) and its relationship with the solar cycle in the South Atlantic Magnetic Anomaly -SAMA is presented. The study of <span class="hlt">geomagnetic</span> pulsations is important to help the understanding of the physical processes that occurs in the magnetosphere region and help to predict <span class="hlt">geomagnetic</span> storms. The fluxgate mag-netometers H, D and Z, three axis <span class="hlt">geomagnetic</span> field data from the Southern Space Observatory -SSO/CRS/INPE -MCT, São Martinho da Serra (29.42° S, 53.87° W, 480m a.s.l.), RS, Brasil, a were analyzed and correlated with the solar wind parameters (speed, density and temperature) from the ACE and SOHO satellites. A digital filtering to enhance the 2-7 mHz <span class="hlt">geomagnetic</span> pulsations was used. Five quiet days and five perturbed days in the solar minimum and in the solar maximum were selected for this analysis. The days were chosen based on the IAGA definition and on the Bartels Musical Diagrams (Kp index) for 2001 (solar maximum) and 2008 (solar minimum). The biggest Pc-5 amplitude averages differences between the H-component is 78,35 nT for the perturbed days and 1,60nT for the quiet days during the solar maximum. For perturbed days the average amplitude during the solar minimum is 8,32 nT, confirming a direct solar cycle influence in the <span class="hlt">geomagnetic</span> pulsations intensity for long periods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSA23A4051F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSA23A4051F"><span><span class="hlt">Geomagnetically</span> conjugate observations of ionospheric and thermospheric <span class="hlt">variations</span> accompanied with a midnight brightness wave at low latitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fukushima, D.; Shiokawa, K.; Otsuka, Y.; Kubota, M.; Yokoyama, T.; Nishioka, M.; Komonjinda, S.; Yatini, C. Y.</p> <p>2014-12-01</p> <p>A midnight brightness wave (MBW) is the phenomenon that the OI (630-nm) airglow enhancement propagates poleward once at local midnight. In this study, we first conducted <span class="hlt">geomagnetically</span> conjugate observations of 630nm airglow for an MBW at conjugate stations. An airglow enhancement which is considered to be an MBW was observed in the 630-nm airglow images at Kototabang, Indonesia (<span class="hlt">geomagnetic</span> latitude (MLAT): 10.0S) at around local midnight from 1540 to 1730 UT (from 2240 to 2430 LT) on 7 February 2011. This MBW was propagating south-southwestward, which is <span class="hlt">geomagnetically</span> poleward, with a velocity of 290 m/s. However, similar wave was not observed in the 630-nm airglow images at Chiang Mai, Thailand (MLAT: 8.9N), which is close to being conjugate point of Kototabang. This result indicates that the MBW does not have <span class="hlt">geomagnetic</span> conjugacy. We simultaneously observed thermospheric neutral winds observed by a co-located Fabry-Perot interferometer at Kototabang. The observed meridional winds turned from northward (<span class="hlt">geomagnetically</span> equatorward) to southward (<span class="hlt">geomagnetically</span> poleward) just before the MBW was observed. The bottomside ionospheric heights observed by ionosondes rapidly decreased at Kototabang and slightly increased at Chiang Mai simultaneously with the MBW passage. In the presentation, we discuss the MBW generation by the observed poleward neutral winds at Kototabang, and the cause of the coinciding small height increase at Chiang Mai by the polarization electric field inside the observed MBW at Kototabang.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMGP23A1286S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMGP23A1286S"><span>Authigenic 10Be/9Be Ratio Signatures of the Cosmogenic Nuclide Production Linked to <span class="hlt">Geomagnetic</span> Dipole Moment <span class="hlt">Variation</span> During and Since the Brunhes/Matuyama Boundary</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simon, Q.; Thouveny, N.; Bourles, D. L.; Ménabréaz, L.; Valet, J. P.; Valery, G.; Choy, S.</p> <p>2015-12-01</p> <p>The atmospheric production rate of cosmogenic nuclides is linked to the <span class="hlt">geomagnetic</span> dipole moment (GDM) by a non-linear inverse relationship. Large amplitude GDM <span class="hlt">variations</span> associated with reversals and excursions can potentially be reconstructed using time <span class="hlt">variation</span> of the cosmogenic beryllium-10 (10Be) production recorded in ocean sediments. Downcore profiles of authigenic 10Be/9Be ratios (proxy of atmospheric 10Be production) in oceanic cores provide independent and additional records of the evolution of the <span class="hlt">geomagnetic</span> intensity and complete previous information derived from relative paleointensity (RPI). Here are presented new authigenic 10Be/9Be results obtained from cores MD05-2920 and from the top of core MD05-2930 collected in the West Equatorial Pacific Ocean. Completing data of Ménabréaz et al. (2012, 2014), these results provide the first continuous 10Be production rate sedimentary record covering the last 800 ka. Along these cores, authigenic 10Be/9Be ratio peaks are recorded - within methodological errors - at the stratigraphic level of RPI lows. High-resolution chronologies (δ18O-derived) lead to interpret these peaks as successive global 10Be overproduction events triggered by <span class="hlt">geomagnetic</span> dipole lows present in the PISO-1500 and Sint-2000 stacks. The largest amplitude 10Be production enhancement is synchronous to the very large decrease of the dipole field associated with the last polarity reversal (772 ka). It is consistent in shape and duration with the peak recorded in core MD90-0961 from the Maldive area (Indian Ocean) (Valet et al. 2014). Two significant 10Be production enhancements are coeval with the Laschamp (41 ka) and Icelandic basin (190 ka) excursions, while 10Be production peaks of lower amplitude correlate to other recognized excursions such as the Blake (120 ka), Pringle-Falls (215 ka), Portuguese Margin (290 ka), Big Lost (540 ka) among others. This study provides new data on the amplitude and timing of dipole field <span class="hlt">variations</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMGP53D..05B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMGP53D..05B"><span>Towards an effective record of dipole moment <span class="hlt">variations</span> since the Precambrian using new reliability criteria and outputs from numerical dynamo simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Biggin, A. J.; Suttie, N.; Paterson, G. A.; Aubert, J.; Hurst, E.; Clarke, A.</p> <p>2013-12-01</p> <p> address challenge 2, we take an approach using the outputs of numerical dynamo simulations. This involves subsampling synthetic global time series of full-vector magnetic field data, converting these datasets into virtual (axial) dipole moments, and comparing these to the entire distribution to ascertain how well <span class="hlt">secular</span> <span class="hlt">variation</span> is averaged and characterised. Finally, the two approaches will be combined. Datasets of real dipole moment estimates, filtered by QPI, will be compared to the synthetic distributions in order to present more robust characterisations of <span class="hlt">geomagnetic</span> behaviour in different time intervals than has previously been possible.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Icar..280..300T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Icar..280..300T"><span><span class="hlt">Secular</span> resonances with Ceres and Vesta</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsirvoulis, Georgios; Novaković, Bojan</p> <p>2016-12-01</p> <p>In this work we explore dynamical perturbations induced by the massive asteroids Ceres and Vesta on main-belt asteroids through <span class="hlt">secular</span> resonances. First we determine the location of the linear <span class="hlt">secular</span> resonances with Ceres and Vesta in the main belt, using a purely numerical technique. Then we use a set of numerical simulations of fictitious asteroids to investigate the importance of these <span class="hlt">secular</span> resonances in the orbital evolution of main-belt asteroids. We found, evaluating the magnitude of the perturbations in the proper elements of the test particles, that in some cases the strength of these <span class="hlt">secular</span> resonances is comparable to that of known non-linear <span class="hlt">secular</span> resonances with the giant planets. Finally we explore the asteroid families that are crossed by the <span class="hlt">secular</span> resonances we studied, and identified several cases where the latter seem to play an important role in their post-impact evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6997191-introduction-geomagnetism','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6997191-introduction-geomagnetism"><span>Introduction to <span class="hlt">geomagnetism</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>Parkinson, W.D.</p> <p>1983-01-01</p> <p>This book examines a wide range of subjects in <span class="hlt">geomagnetism</span>. It presents a brief introduction to physical principles of magnetism, and then focuses on the properties of the <span class="hlt">geomagnetic</span> field as the sum of four interrelated phenomena: the main field, the local or crustal field, the external field, and the induced field. Additional topics, including paleomagnetism and magnetic methods in exploration, and the history of <span class="hlt">geomagnetism</span>, are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900018878','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900018878"><span>Lower thermosphere (80-100 km) dynamics response to solar and <span class="hlt">geomagnetic</span> activity: Overview</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kazimirovsky, E. S.</p> <p>1989-01-01</p> <p>The <span class="hlt">variations</span> of solar and <span class="hlt">geomagnetic</span> activity may affect the thermosphere circulation via plasma heating and electric fields, especially at high latitudes. The possibility exists that the energy involved in auroral and magnetic storms can produce significant changes of mesosphere and lower thermosphere wind systems. A study of global radar measurements of winds at 80 to 100 km region revealed the short term effects (correlation between wind field and <span class="hlt">geomagnetic</span> storms) and long term <span class="hlt">variations</span> over a solar cycle. It seems likely that the correlation results from a modification of planetary waves and tides propagated from below, thus altering the dynamical regime of the thermosphere. Sometimes the long term behavior points rather to a climatic <span class="hlt">variation</span> with the internal atmospheric cause than to a direct solar control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000E%26PSL.180..225A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000E%26PSL.180..225A"><span>The tectonic and <span class="hlt">geomagnetic</span> significance of paleomagnetic observations from volcanic rocks from central Afar, Africa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Acton, Gary D.; Tessema, Abera; Jackson, Michael; Bilham, Roger</p> <p>2000-08-01</p> <p>Deformation throughout Afar over the past 2 myr has been characterized by widespread and intense crustal fragmentation that results from inhomogeneous extension across the region. In eastern Afar, this situation has evolved to localized extension associated with the westward propagation of the Gulf of Aden/Gulf of Tadjurah seafloor spreading system into the Asal-Ghoubbet Rift. During the gradual process of rift propagation and localization, crustal blocks in eastern Afar sustained clockwise rotations of ˜11°. To better understand the processes of rift propagation and localization and how they affect the rest of Afar, we have collected and analyzed over 400 oriented paleomagnetic samples from 67 lava flows from central and southern Afar. Unlike eastern Afar, the mean paleomagnetic direction from central Afar indicates that vertical-axis rotations are statistically insignificant (3.6°±4.4°), though small clockwise rotations (<8°) are permitted. Thus, propagation and localization in central Afar have not had the same influence in causing crustal block rotations or, perhaps more likely, have not reached the same stage of evolution as seen in eastern Afar. In addition, several of the lava flows record intriguing <span class="hlt">geomagnetic</span> field behavior associated with polarity transitions, excursions, or large <span class="hlt">secular</span> <span class="hlt">variation</span> events. Interestingly, the transitional or anomalous virtual <span class="hlt">geomagnetic</span> poles (VGPs) tend to cluster in two nearly antipodal regions, one in the northern Pacific Ocean and the other in the southwest Indian Ocean. One lava flow has recorded both of the antipodal transitional components, with the two components residing in magnetic minerals with unblocking temperatures above and below ˜500°C, respectively. Reheating and partial remagnetization by the overlying flow cannot explain either of the transitional directions because both differ significantly from that of the reversely magnetized overlying flow. The high-temperature component gives a VGP in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060036601&hterms=climate+change+anthropogenic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dclimate%2Bchange%2Banthropogenic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060036601&hterms=climate+change+anthropogenic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dclimate%2Bchange%2Banthropogenic"><span>(abstract) A <span class="hlt">Geomagnetic</span> Contribution to Climate Change in this Century</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Feynman, J.; Ruzmaikin, A.; Lawrence, J.</p> <p>1996-01-01</p> <p>There is a myth that all solar effects can be parameterized by the sun spot number. This is not true. For example, the level of <span class="hlt">geomagnetic</span> activity during this century was not proportional to the sunspot number. Instead there is a large systematic increase in <span class="hlt">geomagnetic</span> activity, not reflected in the sunspot number. This increase occurred gradually over at least 60 years. The 11 year solar cycle <span class="hlt">variation</span> was superimposed on this systematic increase. Here we show that this systematic increase in activity is well correlated to the simultaneous increase in terrestrial temperature that occurred during the first half of this century. We discuss these findings in terms of mechanisms by which <span class="hlt">geomagnetics</span> can be coupled to climate. These mechanisms include possible changes in weather patterns and cloud cover due to increased cosmic ray fluxes, or to increased fluxes of high energy electrons. We suggest that this systematic increase in <span class="hlt">geomagnetic</span> activity contributed (along with anthropogenic effects and possible changes in solar irradiance) to the changes in climate recorded during this period.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E1334J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E1334J"><span>A case study of the thermospheric neutral wind response to <span class="hlt">geomagnetic</span> storm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Guoying; Zhang, Shunrong; Wang, Wenbin; Yuan, Wei; Wu, Qian; Xu, Jiyao</p> <p></p> <p>A minor <span class="hlt">geomagnetic</span> storm (Kp=5) occurred on March 27-28, 2012. The response of the thermospheric neutral wind at ~ 250 km to this storm was investigated by the 630.0 nm nightglow measurements of Fabry-Perot interferometers (FPIs) over Xinglong (geographic location: 40.2N, 117.4E; <span class="hlt">geomagnetic</span> location: 29.8N, 193.2E) and Millstone Hill (geographic location: 42.6N, 71.5W; <span class="hlt">geomagnetic</span> location: 53.1N, 65.1W). Our results show that the minor storm on March 27-28, 2012 obviously effected on the thermospheric neutral winds over Xinglong and Millstone Hill, especially Millstone Hill had larger response because of its higher <span class="hlt">geomagnetic</span> latitude. Another interesting result is that a small <span class="hlt">variation</span> in <span class="hlt">geomagnetic</span> activity (Kp=2.7) could enough introduce a clear disturbance in the nighttime thermospheric neutral wind over Millstone hill. NCAR-TIME-GCM (National Center for Atmospheric Research-Thermosphere Ionosphere Mesosphere Electrodynamics-General Circulation Model) was employed to study the evolution and mechanism of the thermospheric neutral wind response.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011GeoJI.184.1119M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011GeoJI.184.1119M"><span><span class="hlt">Secular</span> gravity <span class="hlt">variation</span> at Svalbard (Norway) from ground observations and GRACE satellite data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mémin, A.; Rogister, Y.; Hinderer, J.; Omang, O. C.; Luck, B.</p> <p>2011-03-01</p> <p>The Svalbard archipelago, Norway, is affected by both the present-day ice melting (PDIM) and Glacial Isostatic Adjustment (GIA) subsequent to the Last Pleistocene deglaciation. The induced deformation of the Earth is observed by using different techniques. At the Geodetic Observatory in Ny-Ålesund, precise positioning measurements have been collected since 1991, a superconducting gravimeter (SG) has been installed in 1999, and six campaigns of absolute gravity (AG) measurements were performed between 1998 and 2007. Moreover, the Gravity Recovery and Climate Experiment (GRACE) satellite mission provides the time <span class="hlt">variation</span> of the Earth gravity field since 2002. The goal of this paper is to estimate the present rate of ice melting by combining geodetic observations of the gravity <span class="hlt">variation</span> and uplift rate with geophysical modelling of both the GIA and Earth's response to the PDIM. We estimate the <span class="hlt">secular</span> gravity <span class="hlt">variation</span> by superimposing the SG series with the six AG measurements. We collect published estimates of the vertical velocity based on GPS and VLBI data. We analyse the GRACE solutions provided by three groups (CSR, GFZ, GRGS). The crux of the problem lies in the separation of the contributions from the GIA and PDIM to the Earth's deformation. To account for the GIA, we compute the response of viscoelastic Earth models having different radial structures of mantle viscosity to the deglaciation histories included in the models ICE-3G or ICE-5G. To account for the effect of PDIM, we compute the deformation of an elastic Earth model for six models of ice-melting extension and rates. Errors in the gravity <span class="hlt">variation</span> and vertical velocity are estimated by taking into account the measurement uncertainties and the variability of the GRACE solutions and GIA and PDIM models. The ground observations agree with models that involve a current ice loss of 25 km3 water equivalent yr-1 over Svalbard, whereas the space observations give a value in the interval [5, 18] km3</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JASTP.154..167C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JASTP.154..167C"><span>Thermospheric density estimation and responses to the March 2013 <span class="hlt">geomagnetic</span> storm from GRACE GPS-determined precise orbits</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calabia, Andres; Jin, Shuanggen</p> <p>2017-02-01</p> <p>The thermospheric mass density <span class="hlt">variations</span> and the thermosphere-ionosphere coupling during <span class="hlt">geomagnetic</span> storms are not clear due to lack of observables and large uncertainty in the models. Although accelerometers on-board Low-Orbit-Earth (LEO) satellites can measure non-gravitational accelerations and derive thermospheric mass density <span class="hlt">variations</span> with unprecedented details, their measurements are not always available (e.g., for the March 2013 <span class="hlt">geomagnetic</span> storm). In order to cover accelerometer data gaps of Gravity Recovery and Climate Experiment (GRACE), we estimate thermospheric mass densities from numerical derivation of GRACE determined precise orbit ephemeris (POE) for the period 2011-2016. Our results show good correlation with accelerometer-based mass densities, and a better estimation than the NRLMSISE00 empirical model. Furthermore, we statistically analyze the differences to accelerometer-based densities, and study the March 2013 <span class="hlt">geomagnetic</span> storm response. The thermospheric density enhancements at the polar regions on 17 March 2013 are clearly represented by POE-based measurements. Although our results show density <span class="hlt">variations</span> better correlate with Dst and k-derived <span class="hlt">geomagnetic</span> indices, the auroral electroject activity index AE as well as the merging electric field Em picture better agreement at high latitude for the March 2013 <span class="hlt">geomagnetic</span> storm. On the other side, low-latitude <span class="hlt">variations</span> are better represented with the Dst index. With the increasing resolution and accuracy of Precise Orbit Determination (POD) products and LEO satellites, the straightforward technique of determining non-gravitational accelerations and thermospheric mass densities through numerical differentiation of POE promises potentially good applications for the upper atmosphere research community.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMGP23A1296S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMGP23A1296S"><span><span class="hlt">Secular</span> <span class="hlt">variation</span> between 5 and 10c CE in Japan: remeasurements of 2000 samples collected between 1960-70's from Sueki earthenware kilns in Osaka.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shibuya, H.; Mochizuki, N.; Hatakeyama, T.</p> <p>2015-12-01</p> <p>In Japan, archeomagnetic measurements are vigorously developed for years, though it is not well known to paleomagnetism community in english. One of the works is massive archeomagnetic study of Suemura kiln group carried out in Osaka University in 1960's to early 70's. More than 500 kilns were excavated in Sakai city and vicinities, Osaka Prefecture, Japan. The kiln group is called as Suemura Kilns, and are for Sueki earthenware of 5c to 10c CE. About 300 kilns were sampled and most of the samples were measured at the time, and the results are reported in e.g. Hirooka (1971) and Shibuya (1980). However, the results have significant scatter in direction, which may be due to the limitation of old astatic magnetometer measurements and handwriting graphic determination of magnetic direction, and/or the lack of demagnetization. We recently inherited many of those samples and remeasured them with spinner magnetometer applying alternation field demagnetization (afd). The magnetizations are generally very stable, as usual as other archeomagnetic samples, and afd does not change the magnetic direction mostly. However, significant number of sites show large scatter in magnetic directions, which might be due to the wrong identification of kiln floor or disturbance at the time of collapsing or excavation. Taking kilns of α95<4o, we recovered 131 paleomagnetic directions. Although third of them are dated by pottery shape chronology, the range of each pottery style is not precisely known and the relation of the baked floor and the potteries excavated around kilns are not always clear. The carbon dating of those kilns are very scares. Thus we first try to draw <span class="hlt">secular</span> <span class="hlt">variation</span> curve in declination-inclination plot. With the rough ages of those kilns, it is pretty easy to draw the SVC. It is also numerically determined taking the distance of each direction from nearest point in SVC and the velocity change of the SVC as penalty function, within a couple of degrees in the error</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1986EOSTr..67...49B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1986EOSTr..67...49B"><span><span class="hlt">Geomagnetic</span> Workshop, Canberra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barton, C. E.; Lilley, F. E. M.; Milligan, P. R.</p> <p></p> <p>On May 14-15, 1985, 63 discerning geomagnetists flocked to Canberra to attend the <span class="hlt">Geomagnetic</span> Workshop coorganized by the Australian Bureau of Mineral Resources (BMR) and the Research School of Earth Sciences, Australian National University (ANU). With an aurorally glowing cast that included an International Association of <span class="hlt">Geomagnetism</span> and Aeronomy (IAGA) president, former president, and division chairman, the Oriental Magneto-Banquet (which was the center of the meeting), was assured of success. As a cunning ploy to mask the true nature of this gastronomic extravagance from the probings of income tax departments, a presentation of scientific papers on Australian <span class="hlt">geomagnetism</span> in its global setting was arranged.The Australian region, including New Zealand, Papua New Guinea, Indonesia, and a large sector of the Antarctic, covers one eighth of the Earth's surface and historically has played an important role in the study of <span class="hlt">geomagnetism</span>. The region contains both the south magnetic and <span class="hlt">geomagnetic</span> poles, and two Australian Antarctic stations (Casey and Davis) are situated in the region of the south polar cusp (see Figure 1).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001hell.confE..32B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001hell.confE..32B"><span>Environmental and <span class="hlt">geomagnetic</span> factors in relation to self-destructive ideation and behaviour</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bergiannaki, J. D.; Psarros, C.; Nastos, P. Th.; Paparigopoulos, T.; Paliatsos, A. G.; Tritakis, V. P.; Stefanis, C. N.</p> <p>2001-09-01</p> <p>Besides the individual factors such as the reaction to conflicts, several exogenous factors environmental and social may exert a pathogenic influence on suicidal behavior, suicide attempts and complete suicide on predisposed individuals. In the turn of the century many reports accord for the seasonality of suicides, which seems to have a bimodal distribution with a major peak around the spring-summer (April-May) and a second minor in autumn. On the other hand, the seasonal <span class="hlt">variation</span> of environmental factors (daylight, sunlight duration, weather, temperature, air pressure, humidity, <span class="hlt">geomagnetism</span>, solar activity, etc), of biological factors (melatonin, serotonin, serotonin precursors, etc) as also of sociological factors (ethnic events, major holidays, weekends etc) possibly influences the seasonal pattern of self-destructive behavior. Bimodal seasonal <span class="hlt">variation</span> is also reported for biochemical parameters (L-tryptophan, serotonin, endorphin I fraction) that matches seasonal pattern in the prevalence of violent suicide in the total population and also in the incidence of the affective disorders. The aim of this study is to investigate the relation of environmental factors expressed by the Discomfort Index (DI) and <span class="hlt">geomagnetic</span> factors expressed by the <span class="hlt">geomagnetic</span> field Index DST in relation to suicidal behavior. The total number (4803) of patients recorded in the Ambulance of a Phychiatric Hospital (Eginition) throughout 1994 was used along with the records of 2750 patients of the year 1989. The Index DI is a function of dry and wet-bulb temperature. DST is probably one of the <span class="hlt">geomagnetic</span> indices that expresses and monitors with the greatest accuracy the equatorial ring current <span class="hlt">variations</span>. Our results show that there is a seasonal <span class="hlt">variation</span> of suicidal behavior (Fourier analysis) with a major peak during summer (July) and a minor one during spring. A difference in the occurrence of the peaks was observed among genders. A relation of self-destructive behavior and the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP33B0980B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP33B0980B"><span>Toward constructing a time-series of <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> from thermal remanence in slowly cooled igneous rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burns, Z.; Gee, J. S.</p> <p>2017-12-01</p> <p>Analysis of paleomagnetic data can not only help us to understand the behavior of the ancient magnetic field but may also further our understanding of the current field, as well as of the mechanisms and constraints of the geodynamo and <span class="hlt">geomagnetic</span> reversals. A question of particular interest is the possible relationship between reversal frequency and <span class="hlt">geomagnetic</span> field intensity. Some research appears to indicate a correlation between low intensity and high reversal frequency, seeming to support the theory that low field intensity is what makes reversals possible. In order to study this correlation, we obtained several hundred samples from the 182 Ma Dufek Massif, in Antarctica. This intrusion was cooled slowly, at depth, during the high reversal frequency era of the early Jurassic, and most of our samples record multiple polarity intervals. This, combined with their particularly homogeneous magnetic characteristics, makes them ideally suited for recovering a record of <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span>. On approximately 300 samples from the lower portion of the intrusion, we performed step-wise thermal demagnetization of the natural remanent magnetization (NRM), followed by thermal demagnetization of a laboratory thermoremance (TRM), imparted as partial TRMs in three orthogonal directions to assess the reliability of the remanence. These two sets of measurements can tell us about the amount and direction of magnetization acquired at each temperature step and the sample's capacity to acquire a remanence. Corrected for anisotropy, the ratio of the NRM/TRM values at each step multiplied by the value of the lab field can give us an estimate of the paleofield intensity. When convolved with a thermal cooling model for the intrusion, this yields a model of the time-varying ancient field during the intrusion's cooling period. Initial analysis of our data shows average field values of around 20 µT and a minimum of four reversals. The average at this high-latitude site is lower</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760025658','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760025658"><span>Comparison of periodic and other characteristics of <span class="hlt">geomagnetic</span> and meterological rocket data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nastrom, G. D.; Belmont, A. D.</p> <p>1976-01-01</p> <p>The temporal <span class="hlt">variations</span> in stratospheric winds and temperatures with the <span class="hlt">geomagnetic</span> field elements were compared. From a periodic analysis of the <span class="hlt">geomagnetic</span> field elements the amplitude and phase of the quasibiennial, annual, and semiannual waves are given for stations from 1 degree S to 89 degree N. These results are then compared with corresponding waves reported in rocketsonde wind and temperature data. The annual waves are found to be coupled as a result of the annual <span class="hlt">variation</span> in the dynamo effect of the wind in the lower ionosphere. The semiannual waves are also found to be coupled and three possible causes for the extra tropical stratospheric semiannual wind wave are discussed. Time variance spectra for the interval from 4 days to 44 days in both zonal winds and horizontal <span class="hlt">geomagnetic</span> field intensity are compared for years when major midwinter warmings occur and years when only minor warmings occur. The noted differences are suggested to arise from upward propagating planetary waves which are absorbed or refracted in varying amounts depending on the prevailing circulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP33B0965S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP33B0965S"><span>Fast directional changes in the <span class="hlt">geomagnetic</span> field recovered from archaeomagnetism of ancient Israel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shaar, R.; Hassul, E.; Raphael, K.; Ebert, Y.; Marco, S.; Nowaczyk, N. R.; Ben-Yosef, E.; Agnon, A.</p> <p>2017-12-01</p> <p>Recent archaeomagnetic intensity data from the Levant revealed short-term sub-centennial changes in the <span class="hlt">geomagnetic</span> field such as `archaeomagnetic jerks' and `<span class="hlt">geomagnetic</span> spikes'. To fully understand the nature of these fast <span class="hlt">variations</span> a complementary high-precision time-series of <span class="hlt">geomagnetic</span> field direction is required. To this end we investigated 35 heat impacted archaeological objects from Israel, including cooking ovens, furnaces, and burnt walls. We combine the new dataset with previously unpublished data and construct the first archaeomagnetic compilation of Israel which, at the moment, consists of a total of 57 directions. Screening out poor quality data leaves 30 acceptable archaeomagnetic directions, 25 of which spanning the period between 1700 BCE to 400 BCE. The most striking result of this dataset is a large directional anomaly with deviation of 20°-25° from geocentric axial dipole direction during the 9th century BCE. This anomaly in field direction is contemporaneous with the Levantine Iron Age Anomaly (LIAA) - a local <span class="hlt">geomagnetic</span> anomaly over the Levant that was characterized by a high averaged <span class="hlt">geomagnetic</span> field (nearly twice of today's field) and short decadal-scale <span class="hlt">geomagnetic</span> spikes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CeMDA.130....6A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CeMDA.130....6A"><span><span class="hlt">Secular</span> dynamics of multiplanetary circumbinary systems: stationary solutions and binary-planet <span class="hlt">secular</span> resonance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrade-Ines, Eduardo; Robutel, Philippe</p> <p>2018-01-01</p> <p>We present an analytical formalism to study the <span class="hlt">secular</span> dynamics of a system consisting of N-2 planets orbiting a binary star in outer orbits. We introduce a canonical coordinate system and expand the disturbing function in terms of canonical elliptic elements, combining both Legendre polynomials and Laplace coefficients, to obtain a general formalism for the <span class="hlt">secular</span> description of this type of configuration. With a quadratic approximation of the development, we present a simplified analytical solution for the planetary orbits for both the single planet and the two-planet cases. From the two-planet model, we show that the inner planet accelerates the precession rate of the binary pericenter, which, in turn, may enter in resonance with the <span class="hlt">secular</span> frequency of the outer planet, characterizing a <span class="hlt">secular</span> resonance. We calculate an analytical expression for the approximate location of this resonance and apply it to known circumbinary systems, where we show that it can occur at relatively close orbits, for example at 2.4 au for the Kepler-38 system. With a more refined model, we analyse the dynamics of this <span class="hlt">secular</span> resonance and we show that a bifurcation of the corresponding fixed points can affect the long- term evolution and stability of planetary systems. By comparing our results with complete integrations of the exact equations of motion, we verified the accuracy of our analytical model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70035944','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70035944"><span><span class="hlt">Geomagnetic</span> observations on tristan da cunha, south atlantic ocean</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Matzka, J.; Olsen, N.; Maule, C.F.; Pedersen, L.W.; Berarducci, A.M.; Macmillan, S.</p> <p>2009-01-01</p> <p>Few <span class="hlt">geomagnetic</span> ground observations exist of the Earth's strongest core field anomaly, the South Atlantic Anomaly (SAA). The <span class="hlt">geomagnetic</span> repeat station on the island Tristan da Cunha, located half-way between South Africa and South America at 37?? 05' S, 12?? 18' W, is therefore of crucial importance. We have conducted several sets of repeat station measurements during magnetically quiet conditions (Kp 2o or less) in 2004. The procedures are described and the results are compared to those from earlier campaigns and to the predictions of various global field models. Features of the local crustal bias field and the solar quiet daily <span class="hlt">variation</span> are discussed. We also evaluate the benefit of continuous magnetic field recordings from Tristan da Cunha, and argue that such a data set is a very valuable addition to <span class="hlt">geomagnetic</span> satellite data. Recently, funds were set up to establish and operate a magnetometer station on Tristan da Cunha during the Swarm magnetic satellite mission (2011-2014).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AdSpR..40.1941B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AdSpR..40.1941B"><span>Effects of <span class="hlt">geomagnetic</span> activity <span class="hlt">variations</span> on the physiological and psychological state of functionally healthy humans: Some results of Azerbaijani studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Babayev, Elchin S.; Allahverdiyeva, Aysel A.</p> <p></p> <p>There are collaborative and cross-disciplinary space weather studies in the Azerbaijan National Academy of Sciences conducted with purposes of revealing possible effects of solar, <span class="hlt">geomagnetic</span> and cosmic ray variability on certain technological, biological and ecological systems. This paper describes some results of the experimental studies of influence of the periodical and aperiodical changes of <span class="hlt">geomagnetic</span> activity upon human brain, human health and psycho-emotional state. It also covers the conclusions of studies on influence of violent solar events and severe <span class="hlt">geomagnetic</span> storms of the solar cycle 23 on the mentioned systems in middle-latitude location. It is experimentally established that weak and moderate <span class="hlt">geomagnetic</span> storms do not cause significant changes in the brain's bioelectrical activity and exert only stimulating influence while severe disturbances of <span class="hlt">geomagnetic</span> conditions cause negative influence, seriously disintegrate brain's functionality, activate braking processes and amplify the negative emotional background of an individual. It is concluded that <span class="hlt">geomagnetic</span> disturbances affect mainly emotional and vegetative spheres of human beings while characteristics reflecting personality properties do not undergo significant changes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060035442&hterms=GIM+TEC+Map&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DGIM%2BTEC%2BMap','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060035442&hterms=GIM+TEC+Map&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DGIM%2BTEC%2BMap"><span><span class="hlt">Variations</span> of total electron content during <span class="hlt">geomagnetic</span> disturbances: A model/observation comparison</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Roble, G. Lu X. Pi A. D. Richmond R. G.</p> <p>1997-01-01</p> <p>This paper studies the ionospheric response to major <span class="hlt">geomagnetic</span> storm of October 18-19, 1995, using the thermosphere-ionosphere electrodynamic general circulation model (TIE-GCM) simulations and the global ionospheric maps (GIM) of total electron content (TEC) observations from the Global Positioning System (GPS) worldwide network.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017BrJPh..47..552O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017BrJPh..47..552O"><span><span class="hlt">Geomagnetically</span> Induced Currents: Principles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oliveira, Denny M.; Ngwira, Chigomezyo M.</p> <p>2017-10-01</p> <p>The geospace, or the space environment near Earth, is constantly subjected to changes in the solar wind flow generated at the Sun. The study of this environment variability is called Space Weather. Examples of effects resulting from this variability are the occurrence of powerful solar disturbances, such as coronal mass ejections (CMEs). The impact of CMEs on the Earth's magnetosphere very often greatly perturbs the <span class="hlt">geomagnetic</span> field causing the occurrence of <span class="hlt">geomagnetic</span> storms. Such extremely variable <span class="hlt">geomagnetic</span> fields trigger <span class="hlt">geomagnetic</span> effects measurable not only in the geospace but also in the ionosphere, upper atmosphere, and on and in the ground. For example, during extreme cases, rapidly changing <span class="hlt">geomagnetic</span> fields generate intense <span class="hlt">geomagnetically</span> induced currents (GICs). Intense GICs can cause dramatic effects on man-made technological systems, such as damage to high-voltage power transmission transformers leading to interruption of power supply, and/or corrosion of oil and gas pipelines. These space weather effects can in turn lead to severe economic losses. In this paper, we supply the reader with theoretical concepts related to GICs as well as their general consequences. As an example, we discuss the GIC effects on a North American power grid located in mid-latitude regions during the 13-14 March 1989 extreme <span class="hlt">geomagnetic</span> storm. That was the most extreme storm that occurred in the space era age.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMSM41C2493P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMSM41C2493P"><span>Identification of the different magnetic field contributions during a <span class="hlt">geomagnetic</span> storm in magnetosphere and at ground.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Piersanti, M.; Alberti, T.; Vecchio, A.; Lepreti, F.; Villante, U.; Carbone, V.; De Michelis, P.</p> <p>2015-12-01</p> <p><span class="hlt">Geomagnetic</span> storms (GS) are global <span class="hlt">geomagnetic</span> disturbances that result from the interaction between magnetized plasma that propagates from the Sun and plasma and magnetic fields in the near-Earth space plasma environment. The Dst (Disturbance Storm Time) global Ring Current index is still taken to be the definitive representation for <span class="hlt">geomagnetic</span> storm and is used widely by researcher. Recent in situ measurements by satellites passing through the ring-current region (i.e. Van Allen probes) and computations with magnetospheric field models showed that there are many other field contributions on the <span class="hlt">geomagnetic</span> storming time <span class="hlt">variations</span> at middle and low latitudes. Appling the Empirical Mode Decomposition [Huang et al., 1998] to magnetospheric and ground observations, we detect the different magnetic field contributions during a GS and introduce the concepts of modulated baseline and fluctuations of the <span class="hlt">geomagnetic</span> field. This allows to define local <span class="hlt">geomagnetic</span> indices that can be used in discriminating the ionospheric from magnetospheric origin contribution.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PEPI..279...79G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PEPI..279...79G"><span>Last three millennia Earth's Magnetic field strength in Mesoamerica and southern United States: Implications in <span class="hlt">geomagnetism</span> and archaeology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goguitchaichvili, Avto; Ruiz, Rafael García; Pavón-Carrasco, F. Javier; Contreras, Juan Julio Morales; Arechalde, Ana María Soler; Urrutia-Fucugauchi, Jaime</p> <p>2018-06-01</p> <p>Earth's Magnetic Field <span class="hlt">variation</span> strength may provide crucial information to understand the geodynamo mechanism and elucidate the conditions on the physics of the Earth's deep interiors. Aimed to reveal the fine characteristics of the <span class="hlt">geomagnetic</span> field during the last three millennia in Mesoamerica, we analyzed the available absolute <span class="hlt">geomagnetic</span> intensities associated to absolute radiometric dating as well some ages provided by historical documents. This analysis is achieved using thermoremanent magnetization carried by volcanic lava flows and burned archaeological artefacts. A total of 106 selected intensities from Mesoamerica and other 100 from the southern part of the United States represent the main core of the dataset to construct the <span class="hlt">variation</span> curve using both combined bootstrap method and temporal penalized B-spline methods. The obtained intensity paleosecular <span class="hlt">variation</span> curve for Mesoamerica generally disagrees with the values predicted by the global <span class="hlt">geomagnetic</span> field models. There is rather firm evidence of eastward drift when compared to similar reference curves in Western Europe, Asia and Pacific Ocean. The recent hypothesis about the relationship between the <span class="hlt">geomagnetic</span> field strength and paleoclimate is also critically analyzed in the light of this new data compilation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JASTP..69.1871P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JASTP..69.1871P"><span>Anomalous night-time peaks in diurnal <span class="hlt">variations</span> of NmF2 close to the <span class="hlt">geomagnetic</span> equator: A statistical study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pavlov, A. V.; Pavlova, N. M.</p> <p>2007-11-01</p> <p>We present a study of anomalous night-time NmF2 peaks, ANNPs, observed by the La Paz, Natal, Djibouti, Kodaikanal, Madras, Manila, Talara, and Huancayo Jicamarca ionosonde stations close to the <span class="hlt">geomagnetic</span> equator. It is shown for the first time that the probabilities of occurrence of the first and second ANNPs depend on the <span class="hlt">geomagnetic</span> longitude, and there is a longitude sector close to 110° <span class="hlt">geomagnetic</span> longitude where the first and second ANNPs occur less frequently in comparison with the longitude regions located close to and below about 34° <span class="hlt">geomagnetic</span> longitude and close to and above about 144° <span class="hlt">geomagnetic</span> longitude. The found frequencies of occurrence of the ANNPs increase with increasing solar activity, except of the Djibouti and Kodaikanal ionosonde stations, where the probability of the first ANNP occurrence is found to decrease with increasing solar activity from low to moderate solar activity, and except of the Natal ionosonde station, where the frequencies of occurrence of the first and second ANNPs decrease with increasing solar activity from moderate to high solar activity. We found that the occurrence probabilities of ANNPs during <span class="hlt">geomagnetically</span> disturbed conditions are greater than those during <span class="hlt">geomagnetically</span> quiet conditions. The ANNP probabilities are largest in summer and are lowest in winter for the La-Paz, Talara, and Huancayo Jicamarca sounders. These probabilities are lowest in summer for the Djibouti, Madras, and Manila ionosonde stations, and in spring for the Kodaikanal sounder. The maximums in the probabilities are found to be in autumn for the Djibouti, Madras, and Manila ionosonde stations, and in winter for the Kodaikanal sounder.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/circ/1995/1109/report.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/circ/1995/1109/report.pdf"><span><span class="hlt">Geomagnetism</span> applications</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Campbell, Wallace H.</p> <p>1995-01-01</p> <p>The social uses of <span class="hlt">geomagnetism</span> include the physics of the space environment, satellite damage, pipeline corrosion, electric power-grid failure, communication interference, global positioning disruption, mineral-resource detection, interpretation of the Earth's formation and structure, navigation, weather, and magnetoreception in organisms. The need for continuing observations of the <span class="hlt">geomagnetic</span> field, together with careful archiving of these records and mechanisms for dissemination of these data, is emphasized.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018FrASS...5...18B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018FrASS...5...18B"><span>Proper motion and <span class="hlt">secular</span> <span class="hlt">variations</span> of Keplerian orbital elements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Butkevich, Alexey G.</p> <p>2018-05-01</p> <p>High-precision observations require accurate modelling of <span class="hlt">secular</span> changes in the orbital elements in order to extrapolate measurements over long time intervals, and to detect deviation from pure Keplerian motion caused, for example, by other bodies or relativistic effects. We consider the evolution of the Keplerian elements resulting from the gradual change of the apparent orbit orientation due to proper motion. We present rigorous formulae for the transformation of the orbit inclination, longitude of the ascending node and argument of the pericenter from one epoch to another, assuming uniform stellar motion and taking radial velocity into account. An approximate treatment, accurate to the second-order terms in time, is also given. The proper motion effects may be significant for long-period transiting planets. These theoretical results are applicable to the modelling of planetary transits and precise Doppler measurements as well as analysis of pulsar and eclipsing binary timing observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUSMGP41D..05K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUSMGP41D..05K"><span>Anomalous <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> associated with Parkfield (Ms=6.0, 28-SEP-2004, California, USA) earthquake</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kotsarenko, A. A.; Pilinets, S. A.; Perez Enriquez, R.; Lopez Cruz Abeyro, J. A.</p> <p>2007-05-01</p> <p>Analysis of <span class="hlt">geomagnetic</span> and telluric data, measured at the station PRK (Parkfield, ULF flux-gate 3-axial magnetometer) 1 week before (including) the day of the major EQ (EarthQuake, Ms=6.0, 28-SEP-2004, 17:15:24) near Parkfield, California, USA, are presented. Spectral analysis reveal the ULF <span class="hlt">geomagnetic</span> disturbances observed the day before the event, Sep 27, at 15:00- 20:00 by UT, and at the day of the EQ, Sep 28, at 11:00-19:00. Filtering in the corresponding frequency band f = 0.25-0.5 Hz gives the following estimations of the amplitudes of the signals: up to 20 pT for the magnetic channels and 1.5 mkV/km for the telluric ones. Observed phenomena occurs under quiet <span class="hlt">geomagnetic</span> conditions (|Dst|<20 nT); revision of the referent stations data situated far away from the EQ epicenter (330 km) does not reveal any similar effect. Moreover, the Quake Finder research group (http:www.quakefinder.com) received very similar results (ELF range instrument, placed about 50 km from the EQ epicenter) for the day of the EQ. Mentioned above suggests the localized character of the source, possibly of the ionosphere or tectonic origin rather than of magnetosphere. Comparative analysis of the mentioned 2 stations show that we observed the lower-frequency part of the ULF- ELF burst, localized in the frequency range 0.25-1 Hz, generated 9 hours before the earthquake. Acknowledgements. The authors are grateful to Malcolm Johnston for providing us with the <span class="hlt">geomagnetic</span> data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006GRA.....8.2699C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006GRA.....8.2699C"><span>Observational investigation of ionospheric turbulent spectral content in relation to <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> and local seismicity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Contadakis, M. E.; Arambelos, D.; Asteriadis, G.; Pikridas, Ch.; Spatalas, S.; Chatzinikos, M.</p> <p>2006-04-01</p> <p>Atmospheric and underground explosions as well as shallow earthquakes producing strong vertical ground displacement, are known to produce pressure waves that propagates at infrasonic speeds in the atmosphere. At ionospheric altitudes these waves are coupled to ionospheric gravity waves and induce <span class="hlt">variations</span> in the ionospheric electron density. On the other hand local lithospheric density, ion inhalation, temperature or electromagnetic field <span class="hlt">variations</span>, produced by the local tectonic activity during the earthquake preparation period, induces near surface atmospheric <span class="hlt">variations</span> and affect the ionospheric density through the Lithospher-Atmosphere- Ionosphere Coupling. That is the lithospheric near surface tectonic activity results to local pre- co- and post seismic disturbances on the ionospheric Total Electron Content (TEC). Nevertheless these disturbances are mixed with disturbances induced to the ionospher by a number of agents such as tropospheric jets, magnetic storms and sub-storms, solar activity, ionosphere-magnetosphere coupling etc, and a major problem is to discriminate the influence of those agents from the influence of the local tectonic activity. In this paper we present the results of the wavelet analysis of TVEC <span class="hlt">variations</span> over a network of 4 GPS stations, depicted from EUREF-EPN network, covering the whole area of Greece. Our results indicate that 1) Disturbances with period higher than 3 hours have a Universal origin i.e. earth-tides, Aurora or Equatorial anomaly. 2) Disturbances with periods equal or smaller than 3 hours are of local origin. 3) Strong <span class="hlt">Variations</span> of <span class="hlt">geomagnetic</span> field affect the disturbances of all periods. 4) Disturbances with period 3 hours present a good coherency in the measurements of more than one GPS stations. In concluding disturbances with period equal or less than 3 hours are suitable for de</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUSMGP21A..05C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUSMGP21A..05C"><span>Bias Corrections for Regional Estimates of the Time-averaged <span class="hlt">Geomagnetic</span> Field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Constable, C.; Johnson, C. L.</p> <p>2009-05-01</p> <p>We assess two sources of bias in the time-averaged <span class="hlt">geomagnetic</span> field (TAF) and paleosecular <span class="hlt">variation</span> (PSV): inadequate temporal sampling, and the use of unit vectors in deriving temporal averages of the regional <span class="hlt">geomagnetic</span> field. For the first temporal sampling question we use statistical resampling of existing data sets to minimize and correct for bias arising from uneven temporal sampling in studies of the time- averaged <span class="hlt">geomagnetic</span> field (TAF) and its paleosecular <span class="hlt">variation</span> (PSV). The techniques are illustrated using data derived from Hawaiian lava flows for 0-5~Ma: directional observations are an updated version of a previously published compilation of paleomagnetic directional data centered on ± 20° latitude by Lawrence et al./(2006); intensity data are drawn from Tauxe & Yamazaki, (2007). We conclude that poor temporal sampling can produce biased estimates of TAF and PSV, and resampling to appropriate statistical distribution of ages reduces this bias. We suggest that similar resampling should be attempted as a bias correction for all regional paleomagnetic data to be used in TAF and PSV modeling. The second potential source of bias is the use of directional data in place of full vector data to estimate the average field. This is investigated for the full vector subset of the updated Hawaiian data set. Lawrence, K.P., C.G. Constable, and C.L. Johnson, 2006, Geochem. Geophys. Geosyst., 7, Q07007, DOI 10.1029/2005GC001181. Tauxe, L., & Yamazkai, 2007, Treatise on Geophysics,5, <span class="hlt">Geomagnetism</span>, Elsevier, Amsterdam, Chapter 13,p509</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23297205','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23297205"><span>Midlatitude cooling caused by <span class="hlt">geomagnetic</span> field minimum during polarity reversal.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kitaba, Ikuko; Hyodo, Masayuki; Katoh, Shigehiro; Dettman, David L; Sato, Hiroshi</p> <p>2013-01-22</p> <p>The climatic effects of cloud formation induced by galactic cosmic rays (CRs) has recently become a topic of much discussion. The CR-cloud connection suggests that <span class="hlt">variations</span> in <span class="hlt">geomagnetic</span> field intensity could change climate through modulation of CR flux. This hypothesis, however, is not well-tested using robust geological evidence. Here we present paleoclimate and paleoenvironment records of five interglacial periods that include two <span class="hlt">geomagnetic</span> polarity reversals. Marine oxygen isotope stages 19 and 31 contain both anomalous cooling intervals during the sea-level highstands and the Matuyama-Brunhes and Lower Jaramillo reversals, respectively. This contrasts strongly with the typical interglacial climate that has the temperature maximum at the sea-level peak. The cooling occurred when the field intensity dropped to <40% of its present value, for which we estimate >40% increase in CR flux. The climate warmed rapidly when field intensity recovered. We suggest that <span class="hlt">geomagnetic</span> field intensity can influence global climate through the modulation of CR flux.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3557043','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3557043"><span>Midlatitude cooling caused by <span class="hlt">geomagnetic</span> field minimum during polarity reversal</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kitaba, Ikuko; Hyodo, Masayuki; Katoh, Shigehiro; Dettman, David L.; Sato, Hiroshi</p> <p>2013-01-01</p> <p>The climatic effects of cloud formation induced by galactic cosmic rays (CRs) has recently become a topic of much discussion. The CR–cloud connection suggests that <span class="hlt">variations</span> in <span class="hlt">geomagnetic</span> field intensity could change climate through modulation of CR flux. This hypothesis, however, is not well-tested using robust geological evidence. Here we present paleoclimate and paleoenvironment records of five interglacial periods that include two <span class="hlt">geomagnetic</span> polarity reversals. Marine oxygen isotope stages 19 and 31 contain both anomalous cooling intervals during the sea-level highstands and the Matuyama–Brunhes and Lower Jaramillo reversals, respectively. This contrasts strongly with the typical interglacial climate that has the temperature maximum at the sea-level peak. The cooling occurred when the field intensity dropped to <40% of its present value, for which we estimate >40% increase in CR flux. The climate warmed rapidly when field intensity recovered. We suggest that <span class="hlt">geomagnetic</span> field intensity can influence global climate through the modulation of CR flux. PMID:23297205</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMSM11B2292K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMSM11B2292K"><span>Diurnal global variability of the Earth's magnetic field during <span class="hlt">geomagnetically</span> quiet conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klausner, V.</p> <p>2012-12-01</p> <p>This work proposes a methodology (or treatment) to establish a representative signal of the global magnetic diurnal <span class="hlt">variation</span>. It is based on a spatial distribution in both longitude and latitude of a set of magnetic stations as well as their magnetic behavior on a time basis. We apply the Principal Component Analysis (PCA) technique using gapped wavelet transform and wavelet correlation. This new approach was used to describe the characteristics of the magnetic <span class="hlt">variations</span> at Vassouras (Brazil) and 12 other magnetic stations spread around the terrestrial globe. Using magnetograms from 2007, we have investigated the global dominant pattern of the Sq <span class="hlt">variation</span> as a function of low solar activity. This year was divided into two seasons for seasonal <span class="hlt">variation</span> analysis: solstices (June and December) and equinoxes (March and September). We aim to reconstruct the original <span class="hlt">geomagnetic</span> data series of the H component taking into account only the diurnal <span class="hlt">variations</span> with periods of 24 hours on <span class="hlt">geomagnetically</span> quiet days. We advance a proposal to reconstruct the Sq baseline using only the PCA first mode. The first interpretation of the results suggests that PCA/wavelet method could be used to the reconstruction of the Sq baseline.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810060080&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=19810060080&hterms=Solar+power+filters&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSolar%2Bpower%2Bfilters"><span>Solar wind control of auroral zone <span class="hlt">geomagnetic</span> activity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Clauer, C. R.; Mcpherron, R. L.; Searls, C.; Kivelson, M. G.</p> <p>1981-01-01</p> <p>Solar wind magnetosphere energy coupling functions are analyzed using linear prediction filtering with 2.5 minute data. The relationship of auroral zone <span class="hlt">geomagnetic</span> activity to solar wind power input functions are examined, and a least squares prediction filter, or impulse response function is designed from the data. Computed impulse response functions are observed to have characteristics of a low pass filter with time delay. The AL index is found well related to solar wind energy functions, although the AU index shows a poor relationship. High frequency <span class="hlt">variations</span> of auroral indices and substorm expansions are not predictable with solar wind information alone, suggesting influence by internal magnetospheric processes. Finally, the epsilon parameter shows a poorer relationship with auroral <span class="hlt">geomagnetic</span> activity than a power parameter, having a VBs solar wind dependency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740008403','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740008403"><span>Observations of interactions between interplanetary and <span class="hlt">geomagnetic</span> fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Burch, J. L.</p> <p>1973-01-01</p> <p>Magnetospheric effects associated with <span class="hlt">variations</span> of the north-south component of the interplanetary magnetic field are examined in light of recent recent experimental and theoretical results. Although the occurrence of magnetospheric substorms is statistically related to periods of southward interplanetary magnetic field, the details of the interaction are not understood. In particular, attempts to separate effects resulting directly from the interaction between the interplanetary and <span class="hlt">geomagnetic</span> fields from those associated with substorms have produced conflicting results. The transfer of magnetic flux from the dayside to the nightside magnetosphere is evidenced by equatorward motion of the polar cusp and increases of the magnetic energy density in the lobes of the <span class="hlt">geomagnetic</span> tail. The formation of a macroscopic X-type neutral line at tail distances less than 35 R sub E appears to be a substorm phenomenon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990018406','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990018406"><span>Evidence for Solar-Cycle Forcing and <span class="hlt">Secular</span> <span class="hlt">Variation</span> in the Armagh Observatory Temperature Record</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wilson, Robert M.</p> <p>1998-01-01</p> <p>A prominent feature of previous long-term temperature studies has been the appearance of warming since the 1880s, this often being taken as evidence for anthropogenic-induced global warming. In this investigation, the long-term, annual, mean temperature record (1844-1992) of the Armagh Observatory (Armagh, North Ireland), a set of temperature data based on maximum and minimum thermometers that predates the 1880s and correlates well with northern hemispheric and global standards, is examined for evidence of systematic <span class="hlt">variation</span>, in particular, as related to solar-cycle forcing and <span class="hlt">secular</span> <span class="hlt">variation</span>. Indeed, both appear to be embedded within the Armagh data. Removal of these effects, each contributing about 8% to the overall reduction in variance, yields residuals that are randomly distributed. Application of the 10-year moving average to the residuals, furthermore, strongly suggests that the behavior of the residuals is episodic, inferring that (for extended periods of time) temperatures at Armagh sometimes were warmer or cooler (than expected), while at other times they were stable. Comparison of cyclic averages of annual mean temperatures against the lengths of the associated Hale cycles (i.e., the length of two, sequentially numbered, even-odd sunspot cycle pairs) strongly suggests that the temperatures correlate inversely (r = -0.886 at less than 2% level of significance) against the length of the associated Hale cycle. Because sunspot cycle 22 ended in 1996, the present Hale cycle probably will be shorter than average, implying that temperatures at Armagh over this Hale cycle will be warmer (about 9.31 q 0.23 C at the 90% confidence level) than average (= 9.00 C).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRA..12010622H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRA..12010622H"><span>Estimation of cold plasma outflow during <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haaland, S.; Eriksson, A.; André, M.; Maes, L.; Baddeley, L.; Barakat, A.; Chappell, R.; Eccles, V.; Johnsen, C.; Lybekk, B.; Li, K.; Pedersen, A.; Schunk, R.; Welling, D.</p> <p>2015-12-01</p> <p>Low-energy ions of ionospheric origin constitute a significant contributor to the magnetospheric plasma population. Measuring cold ions is difficult though. Observations have to be done at sufficiently high altitudes and typically in regions of space where spacecraft attain a positive charge due to solar illumination. Cold ions are therefore shielded from the satellite particle detectors. Furthermore, spacecraft can only cover key regions of ion outflow during segments of their orbit, so additional complications arise if continuous longtime observations, such as during a <span class="hlt">geomagnetic</span> storm, are needed. In this paper we suggest a new approach, based on a combination of synoptic observations and a novel technique to estimate the flux and total outflow during the various phases of <span class="hlt">geomagnetic</span> storms. Our results indicate large <span class="hlt">variations</span> in both outflow rates and transport throughout the storm. Prior to the storm main phase, outflow rates are moderate, and the cold ions are mainly emanating from moderately sized polar cap regions. Throughout the main phase of the storm, outflow rates increase and the polar cap source regions expand. Furthermore, faster transport, resulting from enhanced convection, leads to a much larger supply of cold ions to the near-Earth region during <span class="hlt">geomagnetic</span> storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9181091','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9181091"><span>Lunisolar tidal waves, <span class="hlt">geomagnetic</span> activity and epilepsy in the light of multivariate coherence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mikulecky, M; Moravcikova, C; Czanner, S</p> <p>1996-08-01</p> <p>The computed daily values of lunisolar tidal waves, the observed daily values of Ap index, a measure of the planetary <span class="hlt">geomagnetic</span> activity, and the daily numbers of patients with epileptic attacks for a group of 28 neurology patients between 1987 and 1992 were analyzed by common, multiple and partial cross-spectral analysis to search for relationships between periodicities in these time series. Significant common and multiple coherence between them was found for rhythms with a period length over 3-4 months, in agreement with seasonal <span class="hlt">variations</span> of all three variables. If, however, the coherence between tides and epilepsy was studied excluding the influence of <span class="hlt">geomagnetism</span>, two joint infradian periodicities with period lengths of 8.5 and 10.7 days became significant. On the other hand, there were no joint rhythms for <span class="hlt">geomagnetism</span> and epilepsy when the influence of tidal waves was excluded. The result suggests a more primary role of gravitation, compared with <span class="hlt">geomagnetism</span>, in the multivariate process studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Biblical+AND+theory&pg=2&id=EJ396465','ERIC'); return false;" href="https://eric.ed.gov/?q=Biblical+AND+theory&pg=2&id=EJ396465"><span>Apocalypticism in <span class="hlt">Secular</span> Public Discourse: A Proposed Theory.</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>Mixon, Harold; Hopkins, Mary Frances</p> <p>1989-01-01</p> <p>Examines Biblical apocalyptic theory and <span class="hlt">secular</span> apocalyptic literature. Proposes a new theory of apocalypticism in <span class="hlt">secular</span> public discourse derived from those two major theories. Provides examples of apocalypticism in <span class="hlt">secular</span> public discourse. (MM)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..122.5043O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.5043O"><span>Quasi-biennial oscillations in the <span class="hlt">geomagnetic</span> field: Their global characteristics and origin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ou, Jiaming; Du, Aimin; Finlay, Christopher C.</p> <p>2017-05-01</p> <p>Quasi-biennial oscillations (QBOs), with periods in the range 1-3 years, have been persistently observed in the <span class="hlt">geomagnetic</span> field. They provide unique information on the mechanisms by which magnetospheric and ionospheric current systems are modulated on interannual timescales and are also of crucial importance in studies of rapid core field <span class="hlt">variations</span>. In this paper, we document the global characteristics of the <span class="hlt">geomagnetic</span> QBO, using ground-based data collected by <span class="hlt">geomagnetic</span> observatories between 1985 and 2010, and reexamine the origin of the signals. Fast Fourier transform analysis of second-order derivatives of the <span class="hlt">geomagnetic</span> X, Y, and Z components reveals salient QBO signals at periods of 1.3, 1.7, 2.2, 2.9, and 5.0 years, with the most prominent peak at 2.2 years. The signature of <span class="hlt">geomagnetic</span> QBO is generally stronger in the X and Z components and with larger amplitudes on <span class="hlt">geomagnetically</span> disturbed days. The amplitude of the QBO in the X component decreases from the equator to the poles, then shows a local maximum at subauroral and auroral zones. The QBO in the Z component enhances from low latitudes toward the polar regions. At high latitudes (poleward of 50°) the <span class="hlt">geomagnetic</span> QBO exhibits stronger amplitudes during LT 00:00-06:00, depending strongly on the <span class="hlt">geomagnetic</span> activity level, while at low latitudes the main effect is in the afternoon sector. These results indicate that the QBOs at low-to-middle latitudes and at high latitudes are influenced by different magnetospheric and ionospheric current systems. The characteristics of the multiple peaks in the QBO range are found to display similar latitudinal and local time distributions, suggesting that these oscillations are derived from a common source. The features, including the strong amplitudes seen on disturbed days and during postmidnight sectors, and the results from spherical harmonic analysis, verify that the majority of <span class="hlt">geomagnetic</span> QBO is of external origin. We furthermore find a very high</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JASTP.123...13N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JASTP.123...13N"><span>A southern Africa harmonic spline core field model derived from CHAMP satellite data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nahayo, E.; Kotzé, P. B.; McCreadie, H.</p> <p>2015-02-01</p> <p>The monitoring of the Earth's magnetic field time <span class="hlt">variation</span> requires a continuous recording of <span class="hlt">geomagnetic</span> data with a good spatial coverage over the area of study. In southern Africa, ground recording stations are limited and the use of satellite data is needed for the studies where high spatial resolution data is required. We show the fast time <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field in the southern Africa region by deriving an harmonic spline model from CHAMP satellite measurements recorded between 2001 and 2010. The derived core field model, the Southern Africa Regional Model (SARM), is compared with the global model GRIMM-2 and the ground based data recorded at Hermanus magnetic observatory (HER) in South Africa and Tsumeb magnetic observatory (TSU) in Namibia where the focus is mainly on the long term <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field. The results of this study suggest that the regional model derived from the satellite data alone can be used to study the small scale features of the time <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field where ground data is not available. In addition, these results also support the earlier findings of the occurrence of a 2007 magnetic jerk and rapid <span class="hlt">secular</span> <span class="hlt">variation</span> fluctuations of 2003 and 2004 in the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.1722B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.1722B"><span>Prediction of <span class="hlt">secular</span> acceleration of axial rotation of Mars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barkin, Yu. V.</p> <p>2009-04-01</p> <p><span class="hlt">Secular</span> motion of the Earth pole and non-tidal acceleration of its diurnal rotation have obtained rather precise explanation with the help of simple one-point model of the directed transport of fluid masses from a southern hemisphere in northern hemisphere with the general direction, given by geocentric axis OP directed to pole P with coordinates 700N, 10403 E[1]. The another generalized model represents a system of two material points with masses m2 and m1, located on surface of the Earth at poles of geocentric axis OP. Masses are linearly changed in the time with velocities [2]: ṁ2 = 0.179 × 1015kg/yrand ṁ1 = 0.043 × 1015kg/yr. A reduction of fluid masses of the appropriate thin spherical layer of the Earth correspond to <span class="hlt">secular</span> increasing of masses of model points. The specified model has allowed to explain values of fundamental geodynamic parameters observably and determined during decades: a direction and velocity of drift of a pole of the Earth; value of non-tidal acceleration of axial rotation; to explain a <span class="hlt">secular</span> <span class="hlt">variations</span> of coefficients of the second, third, fourth, sixth and eighth zonal harmonics of a geopotential; coefficients of <span class="hlt">secular</span> changes of a surface of ocean for the last approximately 150 years; a direction of <span class="hlt">secular</span> drift of a geocenter and other planetary phenomena [3]. The role of the angular momentum of redistributed masses of the Earth in rotation of the Earth appeared not essential at the given stage of researches. On the essence the offered model has semi-empirical character as it bases on values of velocities of change of masses of points and the given position of axis OP. For their determination and estimations the part of the observant data was used, and other parameters were designed under analytical formulas. The obtained results have precisely confirmed competency and affectivity of geodynamic model [4] about existence of <span class="hlt">secular</span> drift of a liquid core along radial direction OP with velocity about 2.6 cm/yr in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ESASP.722E.369T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ESASP.722E.369T"><span>Comparison Of The Global Analytic Models Of The Main <span class="hlt">Geomagnetic</span> Field With The Stratospheric Balloon Magnetic Data 335</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsvetkov, Yu.; Filippov, S.; Frunze, A.</p> <p>2013-12-01</p> <p>Three global analytical models of a main <span class="hlt">geomagnetic</span> field constructed by satellite data are used: model IGRF, Daily Mean Spherical Harmonic Models (DMSHM), and model EMM/2010, and also scalar data of <span class="hlt">geomagnetic</span> field and its gradients, received in stratospheric balloon gradient magnetic surveys at altitudes of ~30 km. At these altitudes the regional magnetic field is formed from all sources of the Earth's crust. It enables to receive along lengthy routes of surveys the fullest data on regional and longwave-lenght magnetic anomalies. Model DMSHM is used at extracting of magnetic anomalies for elimination of a <span class="hlt">secular</span> <span class="hlt">variation</span> up to significant value 0,2 nT. The model can be constructed within the limits of ± 1 months from the moment stratospheric balloon surveys with beneficial day terms with magnetic activity up to Kp <20, that leads to an error of representation of main MFE equal ±5 нТл. It is possible at presence acting for the period of stratospheric balloon magnetic survey of the satellite, for example, Swarm. On stratospheric balloon data it is shown, that model EMM/2010 unsatisfactorily displays MFE at altitude of 30 km. Hence, the qualitative model of the constant (main and anomaly) magnetic field cannot be constructed only with use of satellite and ground data. The improved model constant MFE, constructed according to satellite and stratospheric balloon magnetic surveys, developed up to a degree and the order m=n=720, will have a reliable data about regional crust magnetic field, hence, and about deep magnetic structure of the Earth's crust. The use gradient magnetic surveys aboard stratospheric balloons allows to find the places alternating approximately through 3000 km in which there are no magnetic anomalies. In these places probably to supervise satellite magnetic models for a range of altitude of 20-40 km, timed to stratospheric balloon magnetic surveys.</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://adsabs.harvard.edu/abs/2013AGUFMGP41E..02L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMGP41E..02L"><span>A Comparison of Paleomagnetic <span class="hlt">Secular</span> <span class="hlt">Variation</span> during MIS 7-10 between the Bering Sea (IODP Ex. 323) and North Atlantic Ocean (ODP Leg 172): Implications for the space/time pattern of field and environmental variability (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lund, S.; Okada, M.; Acton, G.; Clement, B. M.; Stoner, J. S.; Platzman, E. S.</p> <p>2013-12-01</p> <p>Detailed records of Brunhes paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> (PSV) during Marine Isotope Stages (MIS) 7-10 have been recovered from four IODP Ex. 323 sites in the Bering Sea (U1339, U1343-U1345) and four ODP Leg 172 sites from the subtropical North Atlantic Ocean (1060-1063). Reproducible records of PSV (both directions and paleointensity) have been recovered from three or more holes at each site and correlated among the four independent sites in each region. These PSV records provide an unprecedented database for considering patterns of long-term <span class="hlt">secular</span> <span class="hlt">variation</span> and evidence for excursional field behavior on a larger than individual regional scale. We will present reproducible evidence for sustained long-term <span class="hlt">secular</span> <span class="hlt">variation</span> in each region and assess the extent to which they may be interrelated. We have identified the times of magnetic field excursions 7α, 7β, 8α, 9α, and 9β in the Atlantic records and correlated those times to the Bering Sea records. There are no true excursions in the Bering Sea at those times, but several of these intervals mark the most anomalous field behavior in the Bering Sea during MIS 7-10. In both regions, the PSV also serves as a high-resolution chronostratigraphic tool for regional correlation of environmental variability. Both regions show clear, reproducible evidence among the sites for synchronous millennial-scale environmental variability that has not been diagnosed previously.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSM31A4179J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSM31A4179J"><span>Simulating <span class="hlt">Geomagnetically</span> Induced Currents in the Irish Power Network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jones, A. G.; Blake, S. P.; Gallagher, P.; McCauley, J.; Hogg, C.; Beggan, C.; Thomson, A. W. P.; Kelly, G.; Walsh, S.</p> <p>2014-12-01</p> <p><span class="hlt">Geomagnetic</span> storms are known to cause <span class="hlt">geomagnetically</span> induced currents (GICs) which can damage or destroy transformers on power grids. Previous studies have examined the vulnerability of power networks in countries such as the UK, New Zealand, Canada and South Africa. Here we describe the application of a British Geological Survey (BGS) thin-sheet conductivity model to compute the geo-electric field from the <span class="hlt">variation</span> of the magnetic field, in order to better quantify the risk of space weather to Ireland's power network. This was achieved using DIAS magnetotelluric data from across Ireland. As part of a near-real-time warning package for Eirgrid (who oversee Ireland's transmission network), severe storm events such as the Halloween 2003 storm and the corresponding GIC flows at transformers are simulated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991BOBeo.144....5B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991BOBeo.144....5B"><span><span class="hlt">Geomagnetic</span> field observations in the Kopaonik thrust region, Yugoslavia.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bicskei, T.; Popeskov, M.</p> <p>1991-09-01</p> <p>In the absence of continuous registrations of the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> in the surveyed region, the nearest permanent observatory records had to be used in the data reduction procedure. The proposed method estimates the differences between the hourly mean values at the particular measuring site, which are not actually known, and at the observatory on the basis of a series of instantaneous total field intensity values measured simultaneously at these two places. The application of this method to the <span class="hlt">geomagnetic</span> field data from the wider area of the Kopaonik thrust region has revealed local field changes which show connection with pronounced seismic activity that has been going on in this region since it was affected by the M = 6.0 earthquake on May 18, 1980.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850026749','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850026749"><span>Transient cosmic ray increase associated with a <span class="hlt">geomagnetic</span> storm</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kudo, S.; Wada, M.; Tanskanen, P.; Kodama, M.</p> <p>1985-01-01</p> <p>On the basis of worldwide network data of cosmic ray nucleonic components, the transient cosmic ray increase due to the depression of cosmic ray cutoff rigidity during a severe <span class="hlt">geomagnetic</span> storm was investigated in terms of the longitudinal dependence. Multiple correlation analysis among isotropic and diurnal terms of cosmic ray intensity <span class="hlt">variations</span> and Dst term of the <span class="hlt">geomagnetic</span> field is applied to each of various station's data. It is shown that the amplitude of the transient cosmic ray increase associated with Dst depends on the local time of the station, and that its maximum phase is found in the evening sector. This fact is consistent with the theoretical estimation based on the azimuthally asymmetric ring current model for the magnetic DS field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SGeo...27..557P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SGeo...27..557P"><span>Solar and <span class="hlt">geomagnetic</span> activity, extremely low frequency magnetic and electric fields and human health at the Earth's surface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Palmer, S. J.; Rycroft, M. J.; Cermack, M.</p> <p>2006-09-01</p> <p>The possibility that conditions on the Sun and in the Earth’s magnetosphere can affect human health at the Earth’s surface has been debated for many decades. This work reviews the research undertaken in the field of heliobiology, focusing on the effect of <span class="hlt">variations</span> of <span class="hlt">geomagnetic</span> activity on human cardiovascular health. Data from previous research are analysed for their statistical significance, resulting in support for some studies and the undermining of others. Three conclusions are that <span class="hlt">geomagnetic</span> effects are more pronounced at higher magnetic latitudes, that extremely high as well as extremely low values of <span class="hlt">geomagnetic</span> activity seem to have adverse health effects and that a subset of the population (10-15%) is predisposed to adverse health due to <span class="hlt">geomagnetic</span> <span class="hlt">variations</span>. The reported health effects of anthropogenic sources of electric and magnetic fields are also briefly discussed, as research performed in this area could help to explain the results from studies into natural electric and magnetic field interactions with the human body. Possible mechanisms by which <span class="hlt">variations</span> in solar and geophysical parameters could affect human health are discussed and the most likely candidates investigated further. Direct effects of natural ELF electric and magnetic fields appear implausible; a mechanism involving some form of resonant absorption is more likely. The idea that the Schumann resonance signals could be the global environmental signal absorbed by the human body, thereby linking <span class="hlt">geomagnetic</span> activity and human health is investigated. Suppression of melatonin secreted by the pineal gland, possibly via desynchronised biological rhythms, appears to be a promising contender linking <span class="hlt">geomagnetic</span> activity and human health. There are indications that calcium ions in cells could play a role in one or more mechanisms. It is found to be unlikely that a single mechanism can explain all of the reported phenomena.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.7128E..2JZ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.7128E..2JZ"><span>Analysis of key technologies in <span class="hlt">geomagnetic</span> navigation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Xiaoming; Zhao, Yan</p> <p>2008-10-01</p> <p>Because of the costly price and the error accumulation of high precise Inertial Navigation Systems (INS) and the vulnerability of Global Navigation Satellite Systems (GNSS), the <span class="hlt">geomagnetic</span> navigation technology, a passive autonomous navigation method, is paid attention again. <span class="hlt">Geomagnetic</span> field is a natural spatial physical field, and is a function of position and time in near earth space. The navigation technology based on <span class="hlt">geomagnetic</span> field is researched in a wide range of commercial and military applications. This paper presents the main features and the state-of-the-art of <span class="hlt">Geomagnetic</span> Navigation System (GMNS). <span class="hlt">Geomagnetic</span> field models and reference maps are described. Obtaining, modeling and updating accurate Anomaly Magnetic Field information is an important step for high precision <span class="hlt">geomagnetic</span> navigation. In addition, the errors of <span class="hlt">geomagnetic</span> measurement using strapdown magnetometers are analyzed. The precise <span class="hlt">geomagnetic</span> data is obtained by means of magnetometer calibration and vehicle magnetic field compensation. According to the measurement data and reference map or model of <span class="hlt">geomagnetic</span> field, the vehicle's position and attitude can be obtained using matching algorithm or state-estimating method. The tendency of <span class="hlt">geomagnetic</span> navigation in near future is introduced at the end of this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760050119&hterms=Storm+Japan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DStorm%2BJapan','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760050119&hterms=Storm+Japan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DStorm%2BJapan"><span>Interplanetary field and plasma during initial phase of <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Patel, V. L.; Wiskerchen, M. J.</p> <p>1975-01-01</p> <p>A study has been conducted of a large number of <span class="hlt">geomagnetic</span> storms occurring during the period from 1966 to 1970. Questions of data selection are discussed and the large-scale interplanetary magnetic field during the initial phase is examined. Small-scale interplanetary fields during the initial phase are also considered, taking into account important features of small-scale <span class="hlt">variations</span> in the interplanetary field and plasma for three storms. Details concerning 23 <span class="hlt">geomagnetic</span> storms and the interplanetary magnetic field are presented in a table. A study of the initial phase of these storms indicates that in most of these events, the solar-ecliptic Z component of the interplanetary magnetic field turns southward when the main phase decrease begins.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008cosp...37.2371P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008cosp...37.2371P"><span>Anomalous night-time peaks in diurnal <span class="hlt">variations</span> of NmF2 close to the <span class="hlt">geomagnetic</span> equator: a statistical study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pavlov, Anatoli</p> <p></p> <p>We present a study of anomalous night-time NmF2 peaks, ANNPs, observed by the La Paz, Natal, Djibouti, Kodaikanal, Madras, Manila, Talara, and Huancayo-Jicamarca ionosonde stations close to the <span class="hlt">geomagnetic</span> equator. It is shown that the probabilities of occurrence of the first and second ANNPs depend on the <span class="hlt">geomagnetic</span> longitude, and there is a longitude sector close to 110° <span class="hlt">geomagnetic</span> longitude where the first and second ANNPs occur less frequently in comparisons with the longitude regions located close to and below about 34° <span class="hlt">geomagnetic</span> longitude and close to and above about 144° <span class="hlt">geomagnetic</span> longitude. The found frequencies of occurrence of the ANNPs increase with increasing solar activity, except of the Djibouti and Kodaikanal ionosonde stations, where the probability of the first ANNP occurrence is found to decrease with increasing solar activity from low (F10.7<100) to moderate (100≤F10.7≤170) solar activity, and except of the Natal ionosonde station, where the frequencies of occurrence of the first and second ANNPs decrease with increasing solar activity from moderate to high (F10.7>170) solar activity. We found that the occurrence probabilities of ANNPs during <span class="hlt">geomagnetically</span> disturbed conditions are greater than those during <span class="hlt">geomagnetically</span> quiet conditions. The calculated values of these probabilities have pronounced maximums in June (La-Paz and Talara) and in July (Huancayo-Jicamarca) at the ionosonde stations located in the southern geographic hemisphere. The first ANNP is least frequently observed in January (La-Paz, Talara, and Huancayo-Jicamarca), and the second ANNP is least frequently measured in January (La-Paz and Huancayo-Jicamarca) and in December (Talara). In the northern geographic hemisphere, the studied probabilities are lowest in June (Djibouti and Madras), in July (Manila), and in April (Kodaikanal). The maximums in the probabilities of occurrence of the first and second ANNPs are found to be in September (Djibouti), in October</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060050130','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060050130"><span>Examination of the Armagh Observatory Annual Mean Temperature Record, 1844-2004</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wilson, Robert M.; Hathaway, David H.</p> <p>2006-01-01</p> <p>The long-term annual mean temperature record (1844-2004) of the Armagh Observatory (Armagh, Northern Ireland, United Kingdom) is examined for evidence of systematic <span class="hlt">variation</span>, in particular, as related to solar/<span class="hlt">geomagnetic</span> forcing and <span class="hlt">secular</span> <span class="hlt">variation</span>. Indeed, both are apparent in the temperature record. Moving averages for 10 years of temperature are found to highly correlate against both 10-year moving averages of the aa-<span class="hlt">geomagnetic</span> index and sunspot number, having correlation coefficients of approx. 0.7, inferring that nearly half the variance in the 10-year moving average of temperature can be explained by solar/<span class="hlt">geomagnetic</span> forcing. The residuals appear episodic in nature, with cooling seen in the 1880s and again near 1980. Seven of the last 10 years of the temperature record has exceeded 10 C, unprecedented in the overall record. <span class="hlt">Variation</span> of sunspot cyclic averages and 2-cycle moving averages of temperature strongly associate with similar averages for the solar/<span class="hlt">geomagnetic</span> cycle, with the residuals displaying an apparent 9-cycle <span class="hlt">variation</span> and a steep rise in temperature associated with cycle 23. Hale cycle averages of temperature for even-odd pairs of sunspot cycles correlate against similar averages for the solar/<span class="hlt">geomagnetic</span> cycle and, especially, against the length of the Hale cycle. Indications are that annual mean temperature will likely exceed 10 C over the next decade.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70013786','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70013786"><span>Range indices of <span class="hlt">geomagnetic</span> activity</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Stuart, W.F.; Green, A.W.</p> <p>1988-01-01</p> <p>The simplest index of <span class="hlt">geomagnetic</span> activity is the range in nT from maximum to minimum value of the field in a given time interval. The hourly range R was recommended by IAGA for use at observatories at latitudes greater than 65??, but was superceded by AE. The most used <span class="hlt">geomagnetic</span> index K is based on the range of activity in a 3 h interval corrected for the regular daily <span class="hlt">variation</span>. In order to take advantage of real time data processing, now available at many observatories, it is proposed to introduce a 1 h range index and also a 3 h range index. Both will be computed hourly, i.e. each will have a series of 24 per day, the 3 h values overlapping. The new data will be available as the range (R) of activity in nT and also as a logarithmic index (I) of the range. The exponent relating index to range in nT is based closely on the scale used for computing K values. The new ranges and range indices are available, from June 1987, to users in real time and can be accessed by telephone connection or computer network. Their first year of production is regarded as a trial period during which their value to the scientific and commercial communities will be assessed, together with their potential as indicators of regional and global disturbances' and in which trials will be conducted into ways of eliminating excessive bias at quiet times due to the rate of change of the daily <span class="hlt">variation</span> field. ?? 1988.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985stan.reptQ....B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985stan.reptQ....B"><span>A real time index of <span class="hlt">geomagnetic</span> background noise for the MAD (Magnetic Anomaly Detection) frequency band</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bernardi, A.; Fraser-Smith, A. C.; Villard, O. G.</p> <p>1985-02-01</p> <p>An index of <span class="hlt">geomagnetic</span> activity in the upper part of the ultra low frequency (ULF) range (less than 4.55 Hz) has been developed. This index will be referred to as the MA index (magnetic activity index). The MA index is prepared every half hour and is a measure of the strength of the <span class="hlt">geomagnetic</span> activity in the Pc1-Pc3 pulsation frequency range during that half hour period. Activity in the individual Pc pulsation ranges can also be measured, if desired. The index is calculated from the running average of the full-wave rectified values of the band pass filtered <span class="hlt">geomagnetic</span> signals and thus it provides a better indication of the magnitude of these band pass filtered magnetic pulsations than does the ap index, for example. Daily <span class="hlt">variations</span> of the band pass filtered magnetic signals are also better captured by the MA index. To test this system we used analog tape recordings of wide-band <span class="hlt">geomagnetic</span> signals. The indices for these tapes are presented in the form of plots, together with a comparison with the ap indices of the same time intervals. The MA index shows the daily <span class="hlt">variation</span> of the geometric signals quite clearly during times when there is strong activity, i.e., when the ap index values are large. Because impulsive signals, such as lightning discharges, tend to be suppressed in the averaging process, the MA index is insensitive to impulsive noise. It is found that the time <span class="hlt">variation</span> of the MA index is in general markedly different from the <span class="hlt">variation</span> of the ap index for the same time intervals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018IzPSE..54..466A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IzPSE..54..466A"><span>Mathematical Simulation of Convective Processes in the Liquid Core of the Earth and Implications for the Interpretation of <span class="hlt">Geomagnetic</span> Field <span class="hlt">Variations</span> in Polar Latitudes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abakumov, M. V.; Chechetkin, V. M.; Shalimov, S. L.</p> <p>2018-05-01</p> <p>The flow structure induced by thermal convection in a rotating spherical shell with viscous boundary conditions is considered under the assumption that the differential rotation of the core relative to the mantle is absent. The radial, azimuthal, and meridional components of the flow's velocity and helicity are studied. With the magnetic field assumed to be frozen into a liquid (frozen-flux hypothesis), it is shown that the numerical results fit the observations of the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> close to the pole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820013801','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820013801"><span>Comparison of storm-time changes of <span class="hlt">geomagnetic</span> field at ground and at MAGSAT altitudes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kane, R. P.; Trivedi, N. B.</p> <p>1981-01-01</p> <p>Computations concerning <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field at MAGSAT altitudes were investigated. Using MAGSAT data for the X, Y, and Z components of the <span class="hlt">geomagnetic</span> field, a computer conversion to yield the H component was performed. Two methods of determining delta H normalized to a constant geocentric distance R sub 0 = 6800 were investigated, and the utility of elta H at times of magnetic storms was considered. Delta H at a geographical latitude of 0 at dawn and dusk, the standard Dst, and K sub p histograms were plotted and compared. Magnetic anomalies are considered. Examination of data from the majority of the 400 passes of MAGSAT considered show a reasonable delta H versus latitude <span class="hlt">variation</span>. Discrepancies in values are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1483825','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1483825"><span><span class="hlt">Secular</span> humanism and "scientific psychiatry"</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Szasz, Thomas</p> <p>2006-01-01</p> <p>The Council for <span class="hlt">Secular</span> Humanism identifies <span class="hlt">Secular</span> Humanism as a "way of thinking and living" committed to rejecting authoritarian beliefs and embracing "individual freedom and responsibility ... and cooperation." The paradigmatic practices of psychiatry are civil commitment and insanity defense, that is, depriving innocent persons of liberty and excusing guilty persons of their crimes: the consequences of both are confinement in institutions ostensibly devoted to the treatment of mental diseases. Black's Law Dictionary states: "Every confinement of the person is an 'imprisonment,' whether it be in a common prison, or in private house, or in the stocks, or even by forcibly detaining one in the public streets." Accordingly, I maintain that <span class="hlt">Secular</span> Humanism is incompatible with the principles and practices of psychiatry. PMID:16759353</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16759353','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16759353"><span><span class="hlt">Secular</span> humanism and "scientific psychiatry".</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Szasz, Thomas</p> <p>2006-04-25</p> <p>The Council for <span class="hlt">Secular</span> Humanism identifies <span class="hlt">Secular</span> Humanism as a "way of thinking and living" committed to rejecting authoritarian beliefs and embracing "individual freedom and responsibility ... and cooperation." The paradigmatic practices of psychiatry are civil commitment and insanity defense, that is, depriving innocent persons of liberty and excusing guilty persons of their crimes: the consequences of both are confinement in institutions ostensibly devoted to the treatment of mental diseases. Black's Law Dictionary states: "Every confinement of the person is an 'imprisonment,' whether it be in a common prison, or in private house, or in the stocks, or even by forcibly detaining one in the public streets." Accordingly, I maintain that <span class="hlt">Secular</span> Humanism is incompatible with the principles and practices of psychiatry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SpWea..15.1020M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SpWea..15.1020M"><span>Long-term <span class="hlt">geomagnetically</span> induced current observations in New Zealand: Earth return corrections and <span class="hlt">geomagnetic</span> field driver</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mac Manus, Daniel H.; Rodger, Craig J.; Dalzell, Michael; Thomson, Alan W. P.; Clilverd, Mark A.; Petersen, Tanja; Wolf, Moritz M.; Thomson, Neil R.; Divett, Tim</p> <p>2017-08-01</p> <p>Transpower New Zealand Limited has measured DC currents in transformer neutrals in the New Zealand electrical network at multiple South Island locations. Near-continuous archived DC current data exist since 2001, starting with 12 different substations and expanding from 2009 to include 17 substations. From 2001 to 2015 up to 58 individual transformers were simultaneously monitored. Primarily, the measurements were intended to monitor the impact of the high-voltage DC system linking the North and South Islands when it is operating in "Earth return" mode. However, after correcting for Earth return operation, as described here, the New Zealand measurements provide an unusually long and spatially detailed set of <span class="hlt">geomagnetically</span> induced current (GIC) measurements. We examine the peak GIC magnitudes observed from these observations during two large <span class="hlt">geomagnetic</span> storms on 6 November 2001 and 2 October 2013. Currents of 30-50 A are observed, depending on the measurement location. There are large spatial <span class="hlt">variations</span> in the GIC observations over comparatively small distances, which likely depend upon network layout and ground conductivity. We then go on to examine the GIC in transformers throughout the South Island during more than 151 h of <span class="hlt">geomagnetic</span> storm conditions. We compare the GIC to the various magnitude and rate of change components of the magnetic field. Our results show that there is a strong correlation between the magnitude of the GIC and the rate of change of the horizontal magnetic field (<fi>H'</fi>). This correlation is particularly clear for transformers that show large GIC current during magnetic storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFMGP41A..06B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFMGP41A..06B"><span><span class="hlt">Secular</span> <span class="hlt">Variation</span> and Paleomagnetic Studies of Southern Patagonian Plateau Lavas, 46S to 52S, Argentina</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brown, L.; Gorring, M.; Mason, D.; Condit, C.; Lillydahl-Schroeder, H.</p> <p>2007-12-01</p> <p>Regional studies of paleosecular <span class="hlt">variation</span> of the Earth's magnetic field can provide us with information beyond that available from one location. Southern Patagonia, Argentina (46S to 52S latitude and 68W to 72W longitude) is a place where numerous Plio-Pleistocene lava flows are available for such a study. Volcanic activity in this area is related to back arc volcanism due to slab window activity as the South Chile Ridge is subducted beneath western South America, producing Neogene volcanic centers capping Mesozoic basement extending far to the east of the active plate boundary. Published studies on young lavas from both the northern (Meseta del Lago Buenos Aires, Brown et al, 2004) and southern (Pali Aike Volcanic Field, Mejia et al, 2004) portions provide stable paleomagnetic data on nearly 70 lava flows. Paleosecular <span class="hlt">variation</span> values for the two studies differ, with 17.1 degrees obtained from the Pali Aike field and 20.0 degrees from the Lago Buenos Aires field. Recent fieldwork in the plateau lavas between these two locations has provided some 80 new sites allowing us to better investigate <span class="hlt">secular</span> <span class="hlt">variation</span> and the time-averaged field over this entire region during the past 5 myr. Rock magnetic studies on selected new samples (isothermal remanent magnetization and hysteresis measurements) as well as optical observations indicate low titanium magnetite as the primary carrier of remanence. Hysteresis properties range from 0.1 to 0.4 for Mr/Ms and 1.4 to 3.0 for Hcr/Hc indicating psuedo-single domain behavior. Mean destructive fields for AF demagnetization average 40 to 60 mT. Thirty-three new sites, mostly from Gran Meseta Central (48°S), yield a mean direction of inclination -61.8, declination of 356.6 with an alpha-95 of 5.7 degrees. These directions, with additional sites recently collected from Meseta de la Muerte south to Rio Santa Cruz, will allow us to further investigate paleosecular <span class="hlt">variation</span> over this wide region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA470541','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA470541"><span><span class="hlt">Secular</span> Evolution of Spiral Galaxies</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2003-01-01</p> <p>recombination (z=1000). Furthermore, the BigBang nucleosynthesis model also requires a signi cantamount of non- baryonic dark matter (Primack 1999) ifthe universe...momentum (as well as energy) outward. Associ-ated with this outward angular momentum transport isan expected <span class="hlt">secular</span> redistribution of disk matter , co...mode, a <span class="hlt">secular</span> transfer of energy andangular momentum between the disk matter and thedensity wave. The existence of the phase shift betweenthe</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860019850','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860019850"><span>Zonal wind observations during a <span class="hlt">geomagnetic</span> storm</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miller, N. J.; Spencer, N. W.</p> <p>1986-01-01</p> <p>In situ measurements taken by the Wind and Temperature Spectrometer (WATS) onboard the Dynamics Explorer 2 spacecraft during a <span class="hlt">geomagnetic</span> storm display zonal wind velocities that are reduced in the corotational direction as the storm intensifies. The data were taken within the altitudes 275 to 475 km in the dusk local time sector equatorward of the auroral region. Characteristic <span class="hlt">variations</span> in the value of the Dst index of horizontal <span class="hlt">geomagnetic</span> field strength are used to monitor the storm evolution. The detected global rise in atmospheric gas temperature indicates the development of thermospheric heating. Concurrent with that heating, reductions in corotational wind velocities were measured equatorward of the auroral region. Just after the sudden commencement, while thermospheric heating is intense in both hemispheres, eastward wind velocities in the northern hemisphere show reductions ranging from 500 m/s over high latitudes to 30 m/s over the <span class="hlt">geomagnetic</span> equator. After 10 hours storm time, while northern thermospheric heating is diminishing, wind velocity reductions, distinct from those initially observed, begin to develop over southern latitudes. In the latter case, velocity reductions range from 300 m/s over the highest southern latitudes to 150 m/s over the <span class="hlt">geomagnetic</span> equator and extend into the Northern Hemisphere. The observations highlight the interhemispheric asymmetry in the development of storm effects detected as enhanced gas temperatures and reduced eastward wind velocities. Zonal wind reductions over high latitudes can be attributed to the storm induced equatorward spread of westward polar cap plasma convection and the resulting plasma-neutral collisions. However, those collisions are less significant over low latitudes; so zonal wind reductions over low latitudes must be attributed to an equatorward extension of a thermospheric circulation pattern disrupted by high latitude collisions between neutrals transported via eastward winds and ions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMGP23A1018G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMGP23A1018G"><span>Improving our knowledge of the rapid <span class="hlt">geomagnetic</span> field intensity <span class="hlt">variation</span> observed in Europe around 800 AD</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gómez-Paccard, M.; Chauvin, A.; Lanos, P.; Dufresne, P.; Kovacheva, M.; Hill, M. J.; Beamud, E.; Gutiérrez-Lloret, S.; Cañavate, V.; Blain, S.; Bouvier, A.; Oberlin, C.; Guibert, P.; Sapin, C.; Pringent, D.</p> <p>2011-12-01</p> <p>Available European data indicate that during the past 2500 years there have been periods of rapid intensity <span class="hlt">geomagnetic</span> fluctuations interspersed with periods of little change. The challenge now is to precisely describe these rapid changes. The aim of this study is to obtain an improved description of the sharp <span class="hlt">geomagnetic</span> intensity change that took place in Western Europe around 800 yrs AD as well as to investigate if this peak is observed at a continental scale. For this purpose 13 precisely dated early medieval Spanish pottery fragments, 4 archeological French kilns and a 3 collections of bricks used for the construction of different historical buildings from France and with ages ranging between 330 to 1290 AD have been studied. The material collected has been dated by archeological/historical constraints together with radiocarbon,thermoluminiscence (TL) and archeomagentic analysis. From classical Thellier experiments including TRM anisotropy and cooling rate corrections upon archeointensity estimates and conducted on 164 specimens (119 of them giving reliable results) ten new high-quality mean intensities have been obtained. The new intensity data together with a selection of the most reliable data from Western Europe have been relocated to the latitude of Paris and confirm the existence of an intensity maxima of ~85 μT centred at ~850 AD and related to intensity changes up to 20 μT per century. The results also indicate that a previous abrupt intensity change (reaching a maximum value of ~ 90 μT) took place in Western Europe around 650 AD. A selection of high-quality intensity data from Bulgaria, Italy and Greece indicate a very similar intensity trend for Eastern Europe. Although available data indicate that the duration of such periods of high intensities may be of less than one century more data are needed to infer the exact duration of these maximums. A comparison between the selected data and regional and global <span class="hlt">geomagnetic</span> field models indicates that</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('http://adsabs.harvard.edu/abs/2000DPS....32.1507R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000DPS....32.1507R"><span>Galileo magnetometer results from the Millennium Mission: Rotation rate and <span class="hlt">secular</span> <span class="hlt">variation</span> of the internal magnetic field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Russell, C. T.; Yu, Z. J.; Kivelson, M. G.; Khurana, K. K.</p> <p>2000-10-01</p> <p>The System III (1965.0) rotation period of Jupiter, as defined by the IAU based on early radio astronomical data, is 9h 55m 29.71s. Higgins et al. (JGR, 22033, 1997) have suggested, based on more recent radio data, that this period is too high by perhaps 25 ms. In the 25 years since the Pioneer and Voyager measurements, such an error would cause a 6 degree shift in apparent longitude of features tied to the internal magnetic field. A comparison of the longitude of the projection of the dipole moment obtained over the period 1975-1979 with that obtained by Galileo today shows that the average dipole location has drifted only one degree eastward in System III (1965.0). This one-degree shift is not significant given the statistical errors. A possible resolution to this apparent paradox is that the dipole moment observation is sensitive to the lower order field while the radio measurement is sensitive to the high order field at low altitude. Estimates of the <span class="hlt">secular</span> <span class="hlt">variation</span> from the in situ data are being pursued.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..122.4571S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.4571S"><span>Solar and lunar tidal variabilities in GPS-TEC and <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span>: Seasonal as well as during the sudden stratospheric warming of 2010</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sridharan, S.</p> <p>2017-04-01</p> <p>The Global Positioning System (GPS) deduced total electron content (TEC) data at 15°N (<span class="hlt">geomagnetic</span>), which is the northern crest region of equatorial ionization anomaly, are used to study solar and lunar tidal variabilities during the years 2008 and 2009 and also during the 2009-2010 winter, when a major sudden stratospheric warming (SSW) event has occurred. The diurnal and semidiurnal tidal amplitudes show semiannual <span class="hlt">variation</span> with maximum amplitudes during February-March and September-November, whereas terdiurnal tide is larger during April-September. They show significant longitudinal variability with larger (smaller) amplitudes over 250°E-150°E (200°E-250°E). Lunar semidiurnal tidal amplitudes show sporadic enhancements during northern winter months and negligible amplitudes during northern summer months. They also show notable longitudinal variabilities. The solar migrating tides DW1 and SW2 show semiannual <span class="hlt">variation</span> with larger amplitudes during spring equinox months, whereas TW3 maximizes during northern summer. DW2 shows larger amplitudes during summer months. During the SSW, except TW3, the migrating tides DW1 and SW2 show considerable enhancements. Among solar nonmigrating tides, SW1, TW2, and DS0 show larger enhancements. Solar tides in TEC and equatorial electrojet strength over Tirunelveli vary with the time scale of 60 days during October 2009-March 2010 similar to ozone mass mixing ratio at 10 hPa, and this confirms the vital role of ozone in tidal variabilities in ionospheric parameters. Lunar tidal amplitudes in changes in horizontal component of <span class="hlt">geomagnetic</span> field (ΔH) are larger over Tirunelveli, a station near dip equator. Solar semidiurnal tides in ΔH have larger amplitudes than lunar tides over polar stations, Mawson and Godhavn.<abstract type="synopsis"><title type="main">Plain Language SummaryIn this paper, the <span class="hlt">variations</span> of solar and lunar tides in a few ionospheric parameters during the years 2008 and 2009 and during a disturbed</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA51C..07Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA51C..07Z"><span>Unusual subauroral neutral wind disturbances during <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, S.; Erickson, P. J.; Holt, J. M.</p> <p>2016-12-01</p> <p>Under the influence of <span class="hlt">geomagnetic</span> storms, general circulation of the global thermosphere undergoes substantial changes that vary with latitudes. High latitude heating processes establish pressure gradients both vertically and horizontally. The equatorward wind surge and the associated westward wind enhancement are a typical disturbance wind characteristic that affacts ionosphere and thermosphere dynamics at mid-, low, and equatorial latitudes. At subauroral latitudes, however, new observations of neutral wind disturbances show some "abnormal" (unusual) behaviors in responding to complicated ion-neutral coupling processes. During the 2015 St. Patrick's Day great <span class="hlt">geomagnetic</span> storm, incoherent scatter radar measurements at Millstone Hill show the following salient <span class="hlt">variations</span>: (1) oscillating meridional wind disturbances with the Traveling Atmosphere Disturbance (TAD) feature; (2) vertical wind signature; (3) pre-mindnight poleward wind surges. The latter two <span class="hlt">variations</span> appear to be associated with strong ion-neutral interaction developed during the subauroral polarization streams (SAPS) presence. Strong frictional heating caused by the relative velocity between the ions with SAPS speed and the neutrals leads to appreciable thermospheric upperwelling. Strong westward ion drifts shown as SAPS also enhance the wseward neutral flow, which subsequently causes a poleward component of the meridional wind due to the Coriolis force. This paper will present these observations of the wind and discuss ion-neutral coupling effects associated with SAPS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17792941','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17792941"><span>Paleomagnetic Study of a Reversal of the Earth's Magnetic Field.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dunn, J R; Fuller, M; Ito, H; Schmidt, V A</p> <p>1971-05-21</p> <p>A detailed record of a field reversal has been obtained from the natural remanent magnetization of the Tatoosh intrusion in Mount Rainier National Park, Washington. The reversal took place at 14.7 +/- 1 million years and is interpreted to be from reverse to normal. A decrease in the intensity of the field of about an order of magnitude occurs immediately before the reversal, while its orientation remains substantially unchanged. The onset of the reversal is marked by abrupt swinging of the virtual <span class="hlt">geomagnetic</span> pole along an arc of a great circle. During the reversal the pole traces a path across the Pacific. In the last stage of the process recorded in the sections, the succession of virtual <span class="hlt">geomagnetic</span> poles is very similar to those generated by <span class="hlt">secular</span> <span class="hlt">variation</span> in the recent past. Although the cooling rate of the intrusion is not sufficiently well known to permit a useful calculation of the duration of the reversal process, an estimate based on the length of the supposed <span class="hlt">secular</span> <span class="hlt">variation</span> cycles gives 1 to 4 x 103 years for the reversal of field direction and approximately 1 x 104 years for the time scale of the intensity changes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..122.3632C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.3632C"><span>Extraction of the <span class="hlt">geomagnetic</span> activity effect from TEC data: A comparison between the spectral whitening method and 28 day running median</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Zhou; Wang, Jing-Song; Deng, Yue; Huang, Chun-Ming</p> <p>2017-03-01</p> <p>The spectral whitening method (SWM) has been previously proved to be very effective at identifying ionospheric disturbances on foF2 (the critical frequency of ionospheric F2 layer). To continuously investigate the strength of the new method, in this paper SWM has been used to extract the effect of <span class="hlt">geomagnetic</span> activity on total electron content (TEC) and has been compared with the traditional 28 day running median centered (RMC) method. First, ionospheric <span class="hlt">variations</span> during quiet and disturbed conditions are analyzed by both SWM and RMC. The results from RMC, compared with those from SWM, overestimate the disturbance occurrence by about 5-20% during the <span class="hlt">geomagnetic</span> storms and up to 35% during the quiet time. The possible reason is that the results can be contaminated by the residuals of periodic components in the RMC identified disturbances. Meanwhile, the power spectral analysis of the disturbance field shows that the annual and diurnal <span class="hlt">variations</span> are still significant in RMC results but very weak in SWM results, which indicates that SWM has some advantage to clean up the background <span class="hlt">variation</span>. Finally, the analysis of the spatial correlation of the disturbance field with F10.7 and Ap illustrates that the effects of solar and <span class="hlt">geomagnetic</span> activities from SWM are significantly reduced and enhanced, respectively. It suggests that the SWM is more effective in extracting the effect of <span class="hlt">geomagnetic</span> activity from TEC than RMC. The relative deviation of TEC derived by SWM is more sensitive to <span class="hlt">geomagnetic</span> activity than solar activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM43B2728B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM43B2728B"><span>VLF Wave Properties During <span class="hlt">Geomagnetic</span> Storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Blancarte, J.; Artemyev, A.; Mozer, F.; Agapitov, O. V.</p> <p>2017-12-01</p> <p>Whistler-mode chorus is important for the global dynamics of the inner magnetosphere electron population due to its ability to scatter and accelerate electrons of a wide energy range in the outer radiation belt. The parameters of these VLF emissions change dynamically during <span class="hlt">geomagnetic</span> storms. Presented is an analysis of four years of Van Allen probe data, utilizing electric and magnetic field in the VLF range focused on the dynamics of chorus wave properties during the enhancement of <span class="hlt">geomagnetic</span> activity. It is found that VLF emissions respond to <span class="hlt">geomagnetic</span> storms in more complicated ways than just by affecting the waves' amplitude growth or depletion. Oblique wave amplitudes grow together with parallel waves during periods of intermediate <span class="hlt">geomagnetic</span> activity, while the occurrence rate of oblique waves decreases during larger <span class="hlt">geomagnetic</span> storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1407895-dependence-emic-wave-parameters-during-quiet-geomagnetic-storm-geomagnetic-storm-phase-times','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1407895-dependence-emic-wave-parameters-during-quiet-geomagnetic-storm-geomagnetic-storm-phase-times"><span>Dependence of EMIC wave parameters during quiet, <span class="hlt">geomagnetic</span> storm, and <span class="hlt">geomagnetic</span> storm phase times</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Halford, Alexa J.; Fraser, Brian J; Morley, Steven Karl; ...</p> <p>2016-06-08</p> <p>As electromagnetic ion cyclotron (EMIC) waves may play an important role in radiation belt dynamics, there has been a push to better include them into global simulations. How to best include EMIC wave effects is still an open question. Recently many studies have attempted to parameterize EMIC waves and their characteristics by <span class="hlt">geomagnetic</span> indices. However, this does not fully take into account important physics related to the phase of a <span class="hlt">geomagnetic</span> storm. In this paper we first consider how EMIC wave occurrence varies with the phase of a <span class="hlt">geomagnetic</span> storm and the SYM-H, AE, and Kp indices. Here we showmore » that the storm phase plays an important role in the occurrence probability of EMIC waves. The occurrence rates for a given value of a <span class="hlt">geomagnetic</span> index change based on the <span class="hlt">geomagnetic</span> condition. Then in this study we also describe the typical plasma and wave parameters observed in L and magnetic local time for quiet, storm, and storm phase. These results are given in a tabular format in the supporting information so that more accurate statistics of EMIC wave parameters can be incorporated into modeling efforts.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1407895','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1407895"><span>Dependence of EMIC wave parameters during quiet, <span class="hlt">geomagnetic</span> storm, and <span class="hlt">geomagnetic</span> storm phase times</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>Halford, Alexa J.; Fraser, Brian J; Morley, Steven Karl</p> <p></p> <p>As electromagnetic ion cyclotron (EMIC) waves may play an important role in radiation belt dynamics, there has been a push to better include them into global simulations. How to best include EMIC wave effects is still an open question. Recently many studies have attempted to parameterize EMIC waves and their characteristics by <span class="hlt">geomagnetic</span> indices. However, this does not fully take into account important physics related to the phase of a <span class="hlt">geomagnetic</span> storm. In this paper we first consider how EMIC wave occurrence varies with the phase of a <span class="hlt">geomagnetic</span> storm and the SYM-H, AE, and Kp indices. Here we showmore » that the storm phase plays an important role in the occurrence probability of EMIC waves. The occurrence rates for a given value of a <span class="hlt">geomagnetic</span> index change based on the <span class="hlt">geomagnetic</span> condition. Then in this study we also describe the typical plasma and wave parameters observed in L and magnetic local time for quiet, storm, and storm phase. These results are given in a tabular format in the supporting information so that more accurate statistics of EMIC wave parameters can be incorporated into modeling efforts.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA22A..02C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA22A..02C"><span>Induction Hazard Assessment: The Variability of Geoelectric Responses During <span class="hlt">Geomagnetic</span> Storms Within Common Hazard Zones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cuttler, S. W.; Love, J. J.; Swidinsky, A.</p> <p>2017-12-01</p> <p><span class="hlt">Geomagnetic</span> field data obtained through the INTERMAGNET program are convolved with four validated EarthScope USArray impedances to estimate the geoelectric <span class="hlt">variations</span> throughout the duration of a <span class="hlt">geomagnetic</span> storm. A four day long <span class="hlt">geomagnetic</span> storm began on June 22, 2016, and was recorded at the Brandon (BRD), Manitoba and Fredericksburg (FRD), Virginia magnetic observatories over four days. Two impedance tensors corresponding to each magnetic observatory produce extremely different responses, despite being within close geographical proximity. Estimated time series of the geoelectric field throughout the duration of the <span class="hlt">geomagnetic</span> storm were calculated, providing an understanding of how the geoelectric field differs across small geographic distances within the same <span class="hlt">geomagnetic</span> hazard zones derived from prior <span class="hlt">geomagnetic</span> hazard assessment. We show that the geoelectric response of two sites within 200km of one another can differ by up to two orders of magnitude (4245 mV/km at one location and 38 mV/km at another location 125km away). In addition, we compare these results with estimations of the geoelectric field generated from synthetic 1-dimensional resistivity models commonly used to represent large geographic regions when assessing <span class="hlt">geomagnetically</span> induced current (GIC) hazards. This comparison shows that estimations of the <span class="hlt">geomagnetic</span> field from these models differ greatly from estimations produced from Earthscope USArray sites (1205 mV/km in the 1D and 4245 mV/km in the 3D case in one example). This study demonstrates that the application of uniform 1-dimensional resistivity models of the subsurface to wide geographic regions is insufficient to predict the geoelectric hazard at a given location. Furthermore an evaluation of the 3-dimensional resistivity distribution at a given location is necessary to produce a reliable estimation of how the geoelectric field evolves over the course of a <span class="hlt">geomagnetic</span> storm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Freedom+AND+religion&pg=4&id=ED545295','ERIC'); return false;" href="https://eric.ed.gov/?q=Freedom+AND+religion&pg=4&id=ED545295"><span>Unsafe Gods: Security, <span class="hlt">Secularism</span> and Schooling</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>Davies, Lynn</p> <p>2014-01-01</p> <p>This book makes the compelling argument that religion can be complicit in conflict and that a new <span class="hlt">secularism</span> is vital to foster security. Using insights from complexity science, it shows how dynamic <span class="hlt">secularism</span> can be used to accommodate diverse faiths and beliefs within worldly politics. Exploration of the interplay of religion and education in…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSM41A2219S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSM41A2219S"><span>Effect of severe <span class="hlt">geomagnetic</span> disturbances on the atomic oxygen airglow emissions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sunil Krishna, M.; Bag, T.</p> <p>2013-12-01</p> <p>The atomic oxygen greenline (557.7nm) and redline emission (630.0 nm) are the most readily observed and prominent lines in the nightglow. These emissions can be used as precursors for a variety of physical and chemical processes that occur in the upper mesosphere and lower thermosphere. There are a multitude of effects of space weather on the Earth's atmosphere. The decay of ring current is a very important parameter which can induce <span class="hlt">variation</span> in the densities of few important species in the atmosphere which are of airglow interest. The connection of <span class="hlt">variation</span> of airglow emissions with the extreme space weather conditions is not very well established. In the present study, severe <span class="hlt">geomagnetic</span> storms and their effect on the airglow emissions such as 557.7 nm and 630.0 nm emissions is studied. This study is primarily based on photochemical models with the necessary input obtained from a combination of experimental observations and empirical models. We have tried to understand the effect of severe space weather conditions on few very important airglow emissions in terms of volume emission rates, change in the peak emission height. Based on the <span class="hlt">variation</span> an attempt has been made to understand the cause of the <span class="hlt">variation</span> and further to link the <span class="hlt">variations</span> in the ring current to the airglow chemistry. The study presents the results of calculations performed for the most severe <span class="hlt">geomagnetic</span> storms occurred over the recent past because of variety of causes on Sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA31A2378P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA31A2378P"><span>Impact of the Lower Atmosphere on the Ionosphere Response to a <span class="hlt">Geomagnetic</span> Superstorm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pedatella, N. M.</p> <p>2016-12-01</p> <p>Numerical simulations in the National Center for Atmospheric Research (NCAR) Thermosphere-Ionosphere-Electrodynamics General Circulation Model (TIE-GCM) are performed to elucidate the impacts of lower atmosphere forcing on the ionosphere response to a <span class="hlt">geomagnetic</span> superstorm. In particular, how the ionosphere variability due to the October 2003 Halloween storm would be different if it occurred in January coincident with a major sudden stratosphere warming (SSW) event is investigated. The TIE-GCM simulations reveal that the E x B vertical drift velocity and total electron content (TEC) respond differently to the <span class="hlt">geomagnetic</span> disturbance when the lower atmosphere forcing is representative of SSW conditions compared to climatological lower atmosphere forcing conditions. Notably, the storm time <span class="hlt">variations</span> in the E x B vertical drift velocity differ when the effects of the SSW are considered, and this is in part due to effects of the SSW on the equatorial ionosphere being potentially misinterpreted as being of <span class="hlt">geomagnetic</span> origin. Differences in the TEC response to the <span class="hlt">geomagnetic</span> storm can be up to 100% ( 30 TECU) of the storm induced TEC change, and the temporal variability of the TEC during the storm recovery phase is considerably different if SSW effects are considered. The results demonstrate that even during periods of extreme <span class="hlt">geomagnetic</span> forcing it is important to consider the effects of lower atmosphere forcing on the ionosphere variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFMSM31A0298L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFMSM31A0298L"><span>A Coupling Function Linking Solar Wind /IMF <span class="hlt">Variations</span> and <span class="hlt">Geomagnetic</span> Activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lyatsky, W.; Lyatskaya, S.; Tan, A.</p> <p>2006-12-01</p> <p>From a theoretical consideration we have obtained expressions for the coupling function linking solar wind and IMF parameters to <span class="hlt">geomagnetic</span> activity. While deriving these expressions, we took into account (1) a scaling factor due to polar cap expansion while increasing a reconnected magnetic flux in the dayside magnetosphere, and (2) a modified Akasofu function for the reconnected flux for combined IMF Bz and By components. The resulting coupling function may be written as Fa = aVsw B^1/2 sina (q/2), where Vsw is the solar wind speed, B^ is the magnitude of the IMF vector in the Y-Z plane, q is the clock angle between the Z axis and IMF vector in the Y-Z plane, a is a coefficient, and the exponent, a, is derived from the experimental data and equals approximately to 2. The Fa function differs primary by the power of B^ from coupling functions proposed earlier. For testing the obtained coupling function, we used solar wind and interplanetary magnetic field data for four years for maximum and minimum solar activity. We computed 2-D contour plots for correlation coefficients for the dependence of <span class="hlt">geomagnetic</span> activity indices on solar wind parameters for different coupling functions. The obtained diagrams showed a good correspondence to the theoretic coupling function Fa for a »2. The maximum correlation coefficient for the dependence of the polar cap PC index on the Fa coupling function is significantly higher than that computed for other coupling functions used researchers, for the same time intervals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70016860','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70016860"><span>Quiet <span class="hlt">geomagnetic</span> field representation for all days and latitudes</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Campbell, W.H.; Schiffmacher, E.R.; Arora, B.R.</p> <p>1992-01-01</p> <p>Describes a technique for obtaining the quiet-time <span class="hlt">geomagnetic</span> field <span class="hlt">variation</span> expected for all days of the year and distribution of latitudes from a limited set of selected quiet days within a year at a discrete set of locations. A data set of observatories near 75??E longitude was used as illustration. The method relies upon spatial smoothing of the decomposed spectral components. An evaluation of the fidelity of the resulting model shows correlation coefficients usually above 0.9 at the lower latitudes and near 0.7 at the higher latitudes with <span class="hlt">variations</span> identified as dependent upon season and field element. -from Authors</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Loss+AND+cultures&pg=5&id=EJ1103617','ERIC'); return false;" href="https://eric.ed.gov/?q=Loss+AND+cultures&pg=5&id=EJ1103617"><span>The <span class="hlt">Secular</span> University and Its Critics</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>Jobani, Yuval</p> <p>2016-01-01</p> <p>Universities in the USA have become bastions of <span class="hlt">secularity</span> in a distinctly religious society. As such, they are subjected to a variety of robust and rigorous religious critiques. In this paper I do not seek to engage in the debate between the supporters of the <span class="hlt">secular</span> university and its opponents. Furthermore, I do not claim to summarize the…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA51B2399C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA51B2399C"><span>Analysis of Total Electron Content and Electron Density Profile during Different <span class="hlt">Geomagnetic</span> Storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chapagain, N. P.; Rana, B.; Adhikari, B.</p> <p>2017-12-01</p> <p>Total Electron content (TEC) and electron density are the key parameters in the mitigation of ionospheric effects on radio communication system. Detail study of the TEC and electron density <span class="hlt">variations</span> has been carried out during <span class="hlt">geomagnetic</span> storms, with longitude and latitude, for four different locations: (13˚N -17˚N, 88˚E -98˚E), (30˚N-50˚N, 120˚W -95˚W), (29˚S-26˚S, 167˚W-163˚W,) and (60˚S-45˚S, 120˚W-105˚W) using the Gravity Recovery and Climate Experiment (GRACE) satellite observations. In order to find the <span class="hlt">geomagnetic</span> activity, the solar wind parameters such as north-south component of inter planetary magnetic field (Bz), plasma drift velocity (Vsw), flow pressure (nPa), AE, Dst and Kp indices were obtained from Operating Mission as Nodes on the Internet (OMNI) web system. The data for <span class="hlt">geomagnetic</span> indices have been correlated with the TEC and electron density for four different events of <span class="hlt">geomagnetic</span> storms on 6 April 2008, 27 March 2008, 4 September 2008, and 11 October 2008. The result illustrates that the observed TEC and electron density profile significantly vary with longitudes and latitudes. This study illustrates that the values of TEC and the vertical electron density profile are influenced by the solar wind parameters associated with solar activities. The peak values of electron density and TEC increase as the <span class="hlt">geomagnetic</span> storms become stronger. Similarly, the electron density profile varies with altitudes, which peaks around the altitude range of about 250- 350 km, depending on the strength of <span class="hlt">geomagnetic</span> storms. The results clearly show that the peak electron density shifted to higher altitude (from about 250 km to 350 km) as the <span class="hlt">geomagnetic</span> disturbances becomes stronger.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70047671','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70047671"><span>Surface electric fields for North America during historical <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Wei, Lisa H.; Homeier, Nichole; Gannon, Jennifer L.</p> <p>2013-01-01</p> <p>To better understand the impact of <span class="hlt">geomagnetic</span> disturbances on the electric grid, we recreate surface electric fields from two historical <span class="hlt">geomagnetic</span> storms—the 1989 “Quebec” storm and the 2003 “Halloween” storms. Using the Spherical Elementary Current Systems method, we interpolate sparsely distributed magnetometer data across North America. We find good agreement between the measured and interpolated data, with larger RMS deviations at higher latitudes corresponding to larger magnetic field <span class="hlt">variations</span>. The interpolated magnetic field data are combined with surface impedances for 25 unique physiographic regions from the United States Geological Survey and literature to estimate the horizontal, orthogonal surface electric fields in 1 min time steps. The induced horizontal electric field strongly depends on the local surface impedance, resulting in surprisingly strong electric field amplitudes along the Atlantic and Gulf Coast. The relative peak electric field amplitude of each physiographic region, normalized to the value in the Interior Plains region, varies by a factor of 2 for different input magnetic field time series. The order of peak electric field amplitudes (largest to smallest), however, does not depend much on the input. These results suggest that regions at lower magnetic latitudes with high ground resistivities are also at risk from the effect of <span class="hlt">geomagnetically</span> induced currents. The historical electric field time series are useful for estimating the flow of the induced currents through long transmission lines to study power flow and grid stability during <span class="hlt">geomagnetic</span> disturbances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17387252','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17387252"><span>Physical fitness of children and adolescents in the United States: status and <span class="hlt">secular</span> change.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Malina, Robert M</p> <p>2007-01-01</p> <p>The physical fitness of school-age children in the United States is considered from two perspectives--status and <span class="hlt">secular</span> change. This chapter principally examines health-related fitness, including the BMI, though performance-related fitness is briefly considered. Concepts of reference data and standards and factors that may influence <span class="hlt">secular</span> change are initially discussed. National data on the physical fitness status of school children in the continental United States are limited to the 1980s. Ethnic <span class="hlt">variation</span> in physical fitness is not considered except for the prevalence of overweight and obesity. More recent physical fitness data, including examination of ethnic <span class="hlt">variation</span>, are based on several statewide and more local surveys. Although results vary by test, the majority of American school children meet or exceed criterion-referenced standards, although sex differences are not consistent. Poor morphological fitness manifest in obesity is an exception. The prevalence of overweight and obesity has increased since the early 1980s. <span class="hlt">Secular</span> data for specific fitness items are less extensive. Regression analyses suggest a recent decline in maximal aerobic power in girls, but fairly stable levels between the 1930s and today in boys. However, the highest values for boys occur in the 1960s and 1970s and more recent values are somewhat lower. The general trend may be consistent with the decline since the 1980s in aerobic performance assessed with the 20 m shuttle run. These trends highlight the need for updated national physical fitness data for American youth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19060188','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19060188"><span><span class="hlt">Geomagnetic</span> imprinting: A unifying hypothesis of long-distance natal homing in salmon and sea turtles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lohmann, Kenneth J; Putman, Nathan F; Lohmann, Catherine M F</p> <p>2008-12-09</p> <p>Several marine animals, including salmon and sea turtles, disperse across vast expanses of ocean before returning as adults to their natal areas to reproduce. How animals accomplish such feats of natal homing has remained an enduring mystery. Salmon are known to use chemical cues to identify their home rivers at the end of spawning migrations. Such cues, however, do not extend far enough into the ocean to guide migratory movements that begin in open-sea locations hundreds or thousands of kilometers away. Similarly, how sea turtles reach their nesting areas from distant sites is unknown. However, both salmon and sea turtles detect the magnetic field of the Earth and use it as a directional cue. In addition, sea turtles derive positional information from two magnetic elements (inclination angle and intensity) that vary predictably across the globe and endow different geographic areas with unique magnetic signatures. Here we propose that salmon and sea turtles imprint on the magnetic field of their natal areas and later use this information to direct natal homing. This novel hypothesis provides the first plausible explanation for how marine animals can navigate to natal areas from distant oceanic locations. The hypothesis appears to be compatible with present and recent rates of field change (<span class="hlt">secular</span> <span class="hlt">variation</span>); one implication, however, is that unusually rapid changes in the Earth's field, as occasionally occur during <span class="hlt">geomagnetic</span> polarity reversals, may affect ecological processes by disrupting natal homing, resulting in widespread colonization events and changes in population structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2614721','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2614721"><span><span class="hlt">Geomagnetic</span> imprinting: A unifying hypothesis of long-distance natal homing in salmon and sea turtles</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lohmann, Kenneth J.; Putman, Nathan F.; Lohmann, Catherine M. F.</p> <p>2008-01-01</p> <p>Several marine animals, including salmon and sea turtles, disperse across vast expanses of ocean before returning as adults to their natal areas to reproduce. How animals accomplish such feats of natal homing has remained an enduring mystery. Salmon are known to use chemical cues to identify their home rivers at the end of spawning migrations. Such cues, however, do not extend far enough into the ocean to guide migratory movements that begin in open-sea locations hundreds or thousands of kilometers away. Similarly, how sea turtles reach their nesting areas from distant sites is unknown. However, both salmon and sea turtles detect the magnetic field of the Earth and use it as a directional cue. In addition, sea turtles derive positional information from two magnetic elements (inclination angle and intensity) that vary predictably across the globe and endow different geographic areas with unique magnetic signatures. Here we propose that salmon and sea turtles imprint on the magnetic field of their natal areas and later use this information to direct natal homing. This novel hypothesis provides the first plausible explanation for how marine animals can navigate to natal areas from distant oceanic locations. The hypothesis appears to be compatible with present and recent rates of field change (<span class="hlt">secular</span> <span class="hlt">variation</span>); one implication, however, is that unusually rapid changes in the Earth's field, as occasionally occur during <span class="hlt">geomagnetic</span> polarity reversals, may affect ecological processes by disrupting natal homing, resulting in widespread colonization events and changes in population structure. PMID:19060188</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.7905J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.7905J"><span>Responses of the lower thermospheric temperature to the 9 day and 13.5 day oscillations of recurrent <span class="hlt">geomagnetic</span> activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Guoying; Wang, Wenbin; Xu, Jiyao; Yue, Jia; Burns, Alan G.; Lei, Jiuhou; Mlynczak, Martin G.; Rusell, James M., III</p> <p>2015-04-01</p> <p>Responses of the lower thermospheric temperature to the 9 day and 13.5 day oscillations of recurrent <span class="hlt">geomagnetic</span> activity and solar EUV radiation have been investigated using neutral temperature data observed by the TIMED/SABER (Thermosphere IonosphereMesosphere Energetics and Dynamics/Sounding of the Atmosphere using Broadband Emission Radiometry) instrument and numerical experiments by the NCAR-TIME-GCM (National Center for Atmospheric Research-thermosphere-ionosphere-mesosphere electrodynamics-general circulation model). The TIMED/SABER data analyzed were for the period from 2002 to 2007 during the declining phase of solar cycle 23. The observations show that the zonal mean temperature in the lower thermosphere oscillated with periods of near 9 and 13.5 days in the height range of 100-120 km. These oscillations were more strongly correlated with the recurrent <span class="hlt">geomagnetic</span> activity than with the solar EUV variability of the same periods. The 9 day and 13.5 day oscillations of lower thermospheric temperature had greater amplitudes at high latitudes than at low latitudes; they also had larger amplitudes at higher altitudes, and the oscillations could penetrate down to ~105 km, depending on the strength of the recurrent <span class="hlt">geomagnetic</span> activity for a particular time period. The data further show that the periodic responses of the lower thermospheric temperature to recurrent <span class="hlt">geomagnetic</span> activity were different in the two hemispheres. In addition, numerical experiments have been carried out using the NCAR-TIME-GCM to investigate the causal relationship between the temperature oscillations and the <span class="hlt">geomagnetic</span> activity and solar EUV <span class="hlt">variations</span> of the same periods. Model simulations showed the same periodic oscillations as those seen in the observations when the real <span class="hlt">geomagnetic</span> activity index, Kp, was used to drive the model. These numerical results show that recurrent <span class="hlt">geomagnetic</span> activity is the main cause of the 9 day and 13.5 day <span class="hlt">variations</span> in the lower thermosphere</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRA..119.4841J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRA..119.4841J"><span>Responses of the lower thermospheric temperature to the 9 day and 13.5 day oscillations of recurrent <span class="hlt">geomagnetic</span> activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Guoying; Wang, Wenbin; Xu, Jiyao; Yue, Jia; Burns, Alan G.; Lei, Jiuhou; Mlynczak, Martin G.; Rusell, James M.</p> <p>2014-06-01</p> <p>Responses of the lower thermospheric temperature to the 9 day and 13.5 day oscillations of recurrent <span class="hlt">geomagnetic</span> activity and solar EUV radiation have been investigated using neutral temperature data observed by the TIMED/SABER (Thermosphere Ionosphere Mesosphere Energetics and Dynamics/Sounding of the Atmosphere using Broadband Emission Radiometry) instrument and numerical experiments by the NCAR-TIME-GCM (National Center for Atmospheric Research-thermosphere-ionosphere-mesosphere electrodynamics-general circulation model). The TIMED/SABER data analyzed were for the period from 2002 to 2007 during the declining phase of solar cycle 23. The observations show that the zonal mean temperature in the lower thermosphere oscillated with periods of near 9 and 13.5 days in the height range of 100-120 km. These oscillations were more strongly correlated with the recurrent <span class="hlt">geomagnetic</span> activity than with the solar EUV variability of the same periods. The 9 day and 13.5 day oscillations of lower thermospheric temperature had greater amplitudes at high latitudes than at low latitudes; they also had larger amplitudes at higher altitudes, and the oscillations could penetrate down to 105 km, depending on the strength of the recurrent <span class="hlt">geomagnetic</span> activity for a particular time period. The data further show that the periodic responses of the lower thermospheric temperature to recurrent <span class="hlt">geomagnetic</span> activity were different in the two hemispheres. In addition, numerical experiments have been carried out using the NCAR-TIME-GCM to investigate the causal relationship between the temperature oscillations and the <span class="hlt">geomagnetic</span> activity and solar EUV <span class="hlt">variations</span> of the same periods. Model simulations showed the same periodic oscillations as those seen in the observations when the real <span class="hlt">geomagnetic</span> activity index, Kp, was used to drive the model. These numerical results show that recurrent <span class="hlt">geomagnetic</span> activity is the main cause of the 9 day and 13.5 day <span class="hlt">variations</span> in the lower thermosphere</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA11A2247J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA11A2247J"><span>Mesospheric Na Variability and Dependence on <span class="hlt">Geomagnetic</span> and Solar Activity over Arecibo</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jain, K.; Raizada, S.; Brum, C. G. M.</p> <p>2017-12-01</p> <p>The Sodium (Na) resonance lidars located at the Arecibo Observatory offer an excellent opportunity to study the mesosphere/lower thermosphere(MLT) region. Different metals like Fe, Mg, Na, K, Ca and their ions are deposited in the 80 - 120 km altitude range due to the ablation of meteors caused by frictional heating during their entry into the Earth's atmosphere. We present an investigation of the neutral mesospheric Na atom layers over Arecibo. Data on the Na concentrations was collected using a resonance lidar tuned to the of Na wavelength at 589 nm. This wavelength is achieved with a dye-laser pumped by the second harmonic (532 nm) generated from a state-of-the-art commercial Nd:YAG laser. The backscattered signal is received on a 0.8 m (diameter) Cassegrain telescope. The study is based on this data acquired from 1998-2017 and its relation to <span class="hlt">variations</span> in <span class="hlt">geomagnetic</span> and solar conditions. We also investigate seasonal and long term trends in the data. The nightly-averaged altitude profiles were modeled as Gaussian curves. From this modeled data we obtain parameters such as the peak, abundance, centroid and width of the main Na layer. Preliminary results show that the Na abundance is more sensitive to changes in <span class="hlt">geomagnetic</span> and solar <span class="hlt">variations</span> as compared to the width and centroid height. The seasonal <span class="hlt">variation</span> exhibits higher peak densities during the local summer and has a secondary maximum during the winter [as shown in the attached figure]. Our analysis demonstrates a decrease in the peak and the abundance of Na atoms with the increase of solar and <span class="hlt">geomagnetic</span> activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018FBS....59....4V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018FBS....59....4V"><span><span class="hlt">Secular</span> Effect of Sun Oblateness on the Orbital Parameters of Mars and Jupiter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vaishwar, Avaneesh; Kushvah, Badam Singh; Mishra, Devi Prasad</p> <p>2018-01-01</p> <p>In this paper we considered the Mars-Jupiter system to study the behaviour of Near Earth Asteroids (NEAs) as most of the NEAs originate in the main asteroid belt located between Mars and Jupiter. The materials obtained from NEAs are very useful for space industrialisation. The <span class="hlt">variations</span> in orbital parameters, such as eccentricity, inclination, longitude of pericenter and longitude of ascending node of Mars and Jupiter were investigated for a time span of 200,000 years centered on J2000 (January 2000) using <span class="hlt">secular</span> perturbation theory. We considered the Sun oblateness and studied the effect of Sun oblateness on orbital parameters of Mars and Jupiter. Moreover, we determined the orbital parameters for asteroids moving under the perturbation effect of Mars and Jupiter by using a <span class="hlt">secular</span> solution of Mars-Jupiter system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760024037','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760024037"><span>A mechanism for inducing climatic <span class="hlt">variations</span> through ozone destruction: Screening of galactic cosmic rays by solar and terrestrial magnetic fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chamberlain, J. W.</p> <p>1976-01-01</p> <p>A perturbation analysis, allowing for temperature and opacity feedbacks, is developed to calculate depletions in the O3 abundance and reductions of stratospheric solar heating that result from increases in NOx concentration. A pair of perturbation coefficients give the reduction in O3 and temperature through the stratosphere for a specified NOx increase. This type of analysis illustrates the tendency for various levels to self-heal when a perturbation occurs. Physical arguments indicate that the expected sign of the climatic effect is correct, with colder surface temperatures produced by reduced magnetic shielding. In addition, four qualitative reasons are suggested for thinking that significant ozone reductions by cosmic ray influxes will lead to an increased terrestrial albedo from stratospheric condensation. In this view, long-term (approximately 10,000 years) climatic changes have resulted from <span class="hlt">secular</span> <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> while shorter (approximately 100 years) excursions are related to changes in solar activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130013899','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130013899"><span>Space Weather Monitoring for ISS <span class="hlt">Geomagnetic</span> Storm Studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Minow, Joseph I.; Parker, Neergaard</p> <p>2013-01-01</p> <p>The International Space Station (ISS) space environments community utilizes near real time space weather data to support a variety of ISS engineering and science activities. The team has operated the Floating Potential Measurement Unit (FPMU) suite of plasma instruments (two Langmuir probes, a floating potential probe, and a plasma impedance probe) on ISS since 2006 to obtain in-situ measurements of plasma density and temperature along the ISS orbit and <span class="hlt">variations</span> in ISS frame potential due to electrostatic current collection from the plasma environment (spacecraft charging) and inductive (vxB) effects from the vehicle motion across the Earth s magnetic field. An ongoing effort is to use FPMU for measuring the ionospheric response to <span class="hlt">geomagnetic</span> storms at ISS altitudes and investigate auroral charging of the vehicle as it passes through regions of precipitating auroral electrons. This work is challenged by restrictions on FPMU operations that limit observation time to less than about a third of a year. As a result, FPMU campaigns ranging in length from a few days to a few weeks are typically scheduled weeks in advance for ISS engineering and payload science activities. In order to capture <span class="hlt">geomagnetic</span> storm data under these terms, we monitor near real time space weather data from NASA, NOAA, and ESA sources to determine solar wind disturbance arrival times at Earth likely to be geoeffective (including coronal mass ejections and high speed streams associated with coronal holes) and activate the FPMU ahead of the storm onset. Using this technique we have successfully captured FPMU data during a number of <span class="hlt">geomagnetic</span> storm periods including periods with ISS auroral charging. This presentation will describe the strategies and challenges in capturing FPMU data during <span class="hlt">geomagnetic</span> storms, the near real time space weather resources utilized for monitoring the space weather environment, and provide examples of auroral charging data obtained during storm operations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19730042176&hterms=palestine&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpalestine','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19730042176&hterms=palestine&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpalestine"><span>Measurement of <span class="hlt">geomagnetic</span> cutoff rigidities and particle fluxes below <span class="hlt">geomagnetic</span> cutoff near Palestine, Texas.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pennypacker, C. R.; Smoot, G. F.; Buffington, A.; Muller, R. A.; Smith, L. H.</p> <p>1973-01-01</p> <p>We report a high-statistics magnetic spectrometer measurement of the <span class="hlt">geomagnetic</span> cutoff rigidity and related effects at Palestine, Texas. The effective cutoffs we observe are in agreement with computer-calculated cutoffs. We also report measured spectra of albedo and atmospheric secondary particles that come below <span class="hlt">geomagnetic</span> cutoff.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4385909-measurement-geomagnetic-cutoff-rigidities-particle-fluxes-below-geomagnetic-cutoff-near-palestine-texas','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4385909-measurement-geomagnetic-cutoff-rigidities-particle-fluxes-below-geomagnetic-cutoff-near-palestine-texas"><span>Measurement of <span class="hlt">geomagnetic</span> cutoff rigidities and particle fluxes below <span class="hlt">geomagnetic</span> cutoff near Palestine, Texas</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>Pennypacker, C.R.; Smoot, G.F.; Buffington, A.</p> <p>1973-04-01</p> <p>A high-statistics magnetic spectrometer measurement of the <span class="hlt">geomagnetic</span> cutoff rigidity and related effects at Palestine, Texas is reported. The effective cutoffs observed are in agreement with computer-calculated cutoffs. Measured spectra of albedo and atmospheric secondary particles that come below <span class="hlt">geomagnetic</span> cutoff are also reported. (auth)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMGP51B0761Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMGP51B0761Y"><span><span class="hlt">Geomagnetic</span> field <span class="hlt">variations</span> during the last 400 kyr in the western equatorial Pacific: Paleointensity-inclination correlation revisited</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yamazaki, T.; Kanamatsu, T.; Mizuno, S.; Hokanishi, N.; Gaffar, E. Z.</p> <p>2008-12-01</p> <p>A paleomagnetic study was conducted on four piston cores newly obtained from the West Caroline Basin in the western equatorial Pacific in order to investigate <span class="hlt">variations</span> in paleointensity and inclination during the last 400 kyr. An inclination-intensity correlation was previously reported in this region using giant piston cores, but the quality of the paleomagnetic data of the younger end, the last ca. 300 kyr, was needed to be checked because the upper part of the giant piston cores could suffer from perturbation by oversampling. Age control is based on the oxygen-isotope ratios for one core and inter-core correlation using relative paleointensity for other cores. The mean inclinations of the four cores show negative inclination anomalies ranging from -5.2 to -11.2 degree. The western equatorial Pacific is documented as a region of a large negative inclination anomalies, and the observed values are comparable to those expected from the time-averaged field (TAF) models [Johnson and Constable, 1997; Hatakeyama and Kono, 2002]. Stacked curves of paleointensity and inclination were constructed from the four cores. It was confirmed that <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> on the order of 10 to 100 kyrs occur in inclination as well as paleointensity. A cross-correlation analysis showed that significant in-phase correlation occurs between intensity and inclination for periods longer than about 25 kyr, and power spectra of both paleointensity and inclination <span class="hlt">variations</span> have peaks at ~100 kyr periods. The regional paleointensity stack with higher resolution than the Sint-800 stack [Guyodo and Valet, 1999] should be useful for paleointensity-assisted chronostratigraphy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011epsc.conf..991M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011epsc.conf..991M"><span>Modeling the <span class="hlt">secular</span> evolution of migrating planet pairs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Michtchenko, T. A.; Rodríguez, A.</p> <p>2011-10-01</p> <p>The <span class="hlt">secular</span> regime of motion of multi-planetary systems is universal; in contrast with the 'accidental' resonant motion, characteristic only for specific configurations of the planets, <span class="hlt">secular</span> motion is present everywhere in phase space, even inside the resonant region. The <span class="hlt">secular</span> behavior of a pair of planets evolving under dissipative forces is the principal subject of this study, particularly, the case when the dissipative forces affect the planetary semi-major axes and the planets move inward/outward the central star, the process known as planet migration. Based on the fundamental concepts of conservative and dissipative dynamics of the three-body problem, we develop a qualitative model of the <span class="hlt">secular</span> evolution of the migrating planetary pair. Our approach is based on analysis of the energy and the orbital angular momentum exchange between the two-planet system and an external medium; thus no specific kind of dissipative forces is invoked. We show that, under assumption that dissipation is weak and slow, the evolutionary routes of the migrating planets are traced by the Mode I and Mode II stationary solutions of the conservative <span class="hlt">secular</span> problem. The ultimate convergence and the evolution of the system along one of these <span class="hlt">secular</span> modes of motion is determined uniquely by the condition that the dissipation rate is sufficiently smaller than the proper <span class="hlt">secular</span> frequency of the system. We show that it is possible to reassemble the starting configurations and migration history of the systems on the basis of their final states and consequently to constrain the parameters of the physical processes involved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004PEPI..147..103H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004PEPI..147..103H"><span>On the suitability of refractory bricks from a mediaeval brass melting and working site near Dinant (Belgium) as <span class="hlt">geomagnetic</span> field recorders</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hus, J.; Geeraerts, R.; Plumier, J.</p> <p>2004-11-01</p> <p>Directional field archaeomagnetic data from two oval shaped kilns, of which still one was lined with refractory bricks, unearthed in a brass melting and working site in Bouvignes-sur-Meuse in Belgium, confirm the archaeologic dating as 14-15th century A.D. for the main site activities. The archaeomagnetic dates, obtained using reference <span class="hlt">secular</span> <span class="hlt">variation</span> curves of the <span class="hlt">geomagnetic</span> field direction for France and Great Britain, lead to better time constraints for the cessation of kiln operations. Refractory bricks (firebricks) that are used for their chemical and thermal properties, and in particular for their resistance to high temperatures and temperature changes, are not unusual in metal melting and working sites. The firebricks from the examined site are coarse-grained and very porous inside but possess a very stable remanent magnetisation and revealed to be suitable magnetic field recorders. Although the firebricks have a single-component remanent magnetization, non-random deviations in remanence direction in function of the relative azimuth from the centre of the kiln or with the position of the bricks in the kiln wall, were observed. Several hypotheses for the origin of the deviations were considered: anisotropy, refraction, magnetic interaction, magnetic field distortion and the presence of a local disturbing magnetic source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860029592&hterms=electromagnetism&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Delectromagnetism','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860029592&hterms=electromagnetism&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Delectromagnetism"><span>On the coupling of fluid dynamics and electromagnetism at the top of the earth's core</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Benton, E. R.</p> <p>1985-01-01</p> <p>A kinematic approach to short-term <span class="hlt">geomagnetism</span> has recently been based upon pre-Maxwell frozen-flux electromagnetism. A complete dynamic theory requires coupling fluid dynamics to electromagnetism. A geophysically plausible simplifying assumption for the vertical vorticity balance, namely that the vertical Lorentz torque is negligible, is introduced and its consequences are developed. The simplified coupled magnetohydrodynamic system is shown to conserve a variety of magnetic and vorticity flux integrals. These provide constraints on eligible models for the <span class="hlt">geomagnetic</span> main field, its <span class="hlt">secular</span> <span class="hlt">variation</span>, and the horizontal fluid motions at the top of the core, and so permit a number of tests of the underlying assumptions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22181512','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22181512"><span><span class="hlt">Variational</span> data assimilation for the initial-value dynamo problem.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Kuan; Jackson, Andrew; Livermore, Philip W</p> <p>2011-11-01</p> <p>The <span class="hlt">secular</span> <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field as observed at the Earth's surface results from the complex magnetohydrodynamics taking place in the fluid core of the Earth. One way to analyze this system is to use the data in concert with an underlying dynamical model of the system through the technique of <span class="hlt">variational</span> data assimilation, in much the same way as is employed in meteorology and oceanography. The aim is to discover an optimal initial condition that leads to a trajectory of the system in agreement with observations. Taking the Earth's core to be an electrically conducting fluid sphere in which convection takes place, we develop the continuous adjoint forms of the magnetohydrodynamic equations that govern the dynamical system together with the corresponding numerical algorithms appropriate for a fully spectral method. These adjoint equations enable a computationally fast iterative improvement of the initial condition that determines the system evolution. The initial condition depends on the three dimensional form of quantities such as the magnetic field in the entire sphere. For the magnetic field, conservation of the divergence-free condition for the adjoint magnetic field requires the introduction of an adjoint pressure term satisfying a zero boundary condition. We thus find that solving the forward and adjoint dynamo system requires different numerical algorithms. In this paper, an efficient algorithm for numerically solving this problem is developed and tested for two illustrative problems in a whole sphere: one is a kinematic problem with prescribed velocity field, and the second is associated with the Hall-effect dynamo, exhibiting considerable nonlinearity. The algorithm exhibits reliable numerical accuracy and stability. Using both the analytical and the numerical techniques of this paper, the adjoint dynamo system can be solved directly with the same order of computational complexity as that required to solve the forward problem. These numerical</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUSMGP72A..06M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUSMGP72A..06M"><span>Time Average Field and <span class="hlt">Secular</span> <span class="hlt">Variations</span> of Pleistocene to Recent Lava Flows From the Ruiz-Tolima Volcanic Complex (Colombia)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mejia, V.; Sánchez-Duque, A.; Opdyke, N. D.; Huang, K.; Rosales, A.</p> <p>2009-05-01</p> <p>Thirty three Pleistocene to recent lava flows from the Ruiz-Tolima Volcanic Complex (Colombian Andes) have been sampled for time average field (TAF) and paleosecular <span class="hlt">variation</span> studies. A total of 10 cores were drilled per flow (site) and stepwise AF demagnetization has been carried out. After principal component analysis and mean-site direction calculations, 29 sites (25 and 4 with normal and reverse polarity, respectively), with α95 < 5.5° were selected for further calculations. The overall mean direction among the sites (D = 1.8°, I = 6.3°, α95 = 5.6°) closely fits (at the 95% confidence level) the expected paleomagnetic direction (at the area of study) of a <span class="hlt">geomagnetic</span> field composed primarily by a geocentric axial dipole with 5% axial quadrupole component (I = 5.72°), but also coincides with a simple GAD model. VGP scatter (13°) is similar to that expected from Model G (12.8°).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970026618','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970026618"><span>Upper Thermosphere Winds and Temperatures in the <span class="hlt">Geomagnetic</span> Polar Cap: Solar Cycle, <span class="hlt">Geomagnetic</span> Activity, and Interplanetary Magnetic Field Dependencies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Killeen, T. L.; Won, Y.-I.; Niciejewski, R. J.; Burns, A. G.</p> <p>1995-01-01</p> <p> central polar cap (greater than approx. 80 magnetic latitude) antisunward wind speed is found to be a strong function of both solar and <span class="hlt">geomagnetic</span> activity. The polar cap temperatures show <span class="hlt">variations</span> in both solar and <span class="hlt">geomagnetic</span> activity, with temperatures near 800 K for low K(sub p) and F(sub 10.7) and greater than about 2000 K for high K(sub p) and F(sub 10.7). The observed temperatures are significantly greater than those predicted by the mass spectrometer/incoherent scatter model for high activity conditions. Theoretical analysis based on the NCAR TIGCM indicates that the antisunward upper thermospheric winds, driven by upstream ion drag, basically 'coast' across the polar cap. The relatively small changes in wind velocity and direction within the polar cap are induced by a combination of forcing terms of commensurate magnitude, including the nonlinear advection term, the Coriolis term, and the pressure gradient force term. The polar cap thennospheric thermal balance is dominated by horizontal advection, and adiabatic and thermal conduction terms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SpWea...8.5002M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SpWea...8.5002M"><span>Spectral analysis of pipe-to-soil potentials with <span class="hlt">variations</span> of the Earth's magnetic field in the Australian region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marshall, R. A.; Waters, C. L.; Sciffer, M. D.</p> <p>2010-05-01</p> <p>Long, steel pipelines used to transport essential resources such as gas and oil are potentially vulnerable to space weather. In order to inhibit corrosion, the pipelines are usually coated in an insulating material and maintained at a negative electric potential with respect to Earth using cathodic protection units. During periods of enhanced <span class="hlt">geomagnetic</span> activity, potential differences between the pipeline and surrounding soil (referred to as pipe-to-soil potentials (PSPs)) may exhibit large voltage swings which place the pipeline outside the recommended "safe range" and at an increased risk of corrosion. The PSP <span class="hlt">variations</span> result from the "geoelectric" field at the Earth's surface and associated <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span>. Previous research investigating the relationship between the surface geoelectric field and <span class="hlt">geomagnetic</span> source fields has focused on the high-latitude regions where line currents in the ionosphere E region are often the assumed source of the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span>. For the Australian region Sq currents also contribute to the <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> and provide the major contribution during <span class="hlt">geomagnetic</span> quiet times. This paper presents the results of a spectral analysis of PSP measurements from four pipeline networks from the Australian region with <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> from nearby magnetometers. The pipeline networks extend from Queensland in the north of Australia to Tasmania in the south and provide PSP <span class="hlt">variations</span> during both active and quiet <span class="hlt">geomagnetic</span> conditions. The spectral analyses show both consistent phase and amplitude relationships across all pipelines, even for large separations between magnetometer and PSP sites and for small-amplitude signals. Comparison between the observational relationships and model predictions suggests a method for deriving a geoelectric field proxy suitable for indicating PSP-related space weather conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRB..123.2597X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRB..123.2597X"><span>Paleomagnetic <span class="hlt">Secular</span> <span class="hlt">Variation</span> Constraints on the Rapid Eruption of the Emeishan Continental Flood Basalts in Southwestern China and Northern Vietnam</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Yingchao; Yang, Zhenyu; Tong, Ya-Bo; Jing, Xianqing</p> <p>2018-04-01</p> <p>Estimating the duration of magma eruptions using isotopic dating methods is difficult because of the intrinsic errors of the technique regarding the dated materials (such as zircon). However, the long-term <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> field recorded by lava flows can be used to estimate the net duration of an eruption sequence. The Emeishan basalts at Dongchuan, with a thickness of 630 m, yielded a reliable characteristic remanent magnetization of normal polarity and which passed the fold test (Tauxe & Watson, 1994, https://doi.org/10.1016/0012-821X(94)90006-X). Stratigraphic and magnetostratigraphic correlations of the Emeishan basalts in the Dongchuan section with other sections indicate that the eruption of the Emeishan basalts at Dongchuan spans the entire normal polarity zone in the early stage of the Emeishan large igneous province. A flow-by-flow analysis of <span class="hlt">geomagnetic</span> directions of the Emeishan basalts at Dongchuan indicates that four directional groups and fifteen individual lava directions were recorded, with a net duration (excluding quiescent intervals) of no more than 3100 years. The averaged site directions from the Emeishan basalts with normal polarity conforming to a geocentric axial dipole direction indicate that this interval is longer than 104-105 years. In addition, a magnetostratigraphic study indicates that the normal polarity interval recorded by the Emeishan basalts was shorter than 2-20 × 104 years. Thus, the total duration of the normal polarity stage of the Emeishan large igneous province was roughly 105 years. There is a possible relationship between the rapid eruption and the Late Capitanian mass extinction (259.8 ± 0.4 Ma, Henderson et al., 2012).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20393759','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20393759"><span>Tree-stem diameter fluctuates with the lunar tides and perhaps with <span class="hlt">geomagnetic</span> activity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barlow, Peter W; Mikulecký, Miroslav; Střeštík, Jaroslav</p> <p>2010-11-01</p> <p>Our initial objective has been to examine the suggestion of Zürcher et al. (Nature 392:665–666, 1998) that the naturally occurring <span class="hlt">variations</span> in stem diameter of two experimental trees of Picea alba were related to near simultaneous <span class="hlt">variations</span> in the lunisolar tidal acceleration. The relationship was positive: Lunar peaks were roughly synchronous with stem diameter peaks. To extend the investigation of this putative relationship, additional data on stem diameter <span class="hlt">variations</span> from six other tree species were gathered from published literature. Sixteen sets of data were analysed retrospectively using graphical representations as well as cosinor analysis, statistical cross-correlation and cross-spectral analysis, together with estimated values of the lunisolar tidal acceleration corresponding to the sites, dates and times of collection of the biological data. Positive relationships were revealed between the daily <span class="hlt">variations</span> of stem diameter and the <span class="hlt">variations</span> of the lunisolar tidal acceleration. Although this relationship could be mediated by a 24.8-h lunar rhythm, the presence of a solar rhythm of 24.0 h could not be ruled out. Studies of transpiration in two of the observed trees indicated that although this variable was not linked to stem diameter <span class="hlt">variation</span>, it might also be subject to lunisolar gravitational regulation. In three cases, the <span class="hlt">geomagnetic</span> Thule index showed a weak but reciprocal relationship with stem diameter <span class="hlt">variation</span>, as well as a positive relationship with the lunisolar tidal force. In conclusion, it seems that lunar gravity alone could influence stem diameter <span class="hlt">variation</span> and that, under certain circumstances, additional regulation may come from the <span class="hlt">geomagnetic</span> flux.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JASTP.110...28K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JASTP.110...28K"><span>An experimental study of the biological effects of <span class="hlt">geomagnetic</span> disturbances: The impact of a typical <span class="hlt">geomagnetic</span> storm and its constituents on plants and animals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krylov, Viacheslav V.; Zotov, Oleg D.; Klain, Boris I.; Ushakova, Natalia V.; Kantserova, Nadezhda P.; Znobisheva, Anna V.; Izyumov, Yuri G.; Kuz'mina, Victoria V.; Morozov, Alexey A.; Lysenko, Liudmila A.; Nemova, Nina N.; Osipova, Elena A.</p> <p>2014-04-01</p> <p>Naturally occurring <span class="hlt">geomagnetic</span> storms have been shown to correlate with changes in organisms' biological processes. Changes in the <span class="hlt">geomagnetic</span> field during a <span class="hlt">geomagnetic</span> storm are complex and contain both slow changes of the <span class="hlt">geomagnetic</span> field with frequencies of up to 0.001 Hz, and various <span class="hlt">geomagnetic</span> pulsations observed in general to be within the range of 0.001-5 Hz. Little is known about what frequency constituent of <span class="hlt">geomagnetic</span> storms has the strongest effect on living organisms. This paper uses an experimental approach to demonstrate that organisms from different taxa principally respond to slow changes of the <span class="hlt">geomagnetic</span> field corresponding with the main phase and the initial period of the recovery phase of a <span class="hlt">geomagnetic</span> storm. Pc1 type pulsations, which are commonly regarded as biologically effective elements of <span class="hlt">geomagnetic</span> disturbances, did not affect controlled parameters in our experiments. This paper may serve as a starting point for a thorough inquiry into the influence of slow fluctuations of the <span class="hlt">geomagnetic</span> field on organisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26654502','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26654502"><span>[Nursing care at home and <span class="hlt">secularism</span>].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lecointre, Brigitte</p> <p>2015-12-01</p> <p>The question of <span class="hlt">secularism</span>, long-time confined to schools and the relationships between the Church and State, is today being raised in the field of public health. Nurses are directly affected and are integrating this dimension of <span class="hlt">secularism</span> into their care practices. A private practice nurse describes the effect these changes are having on her practice in patients' homes. Copyright © 2015 Elsevier Masson SAS. All rights reserved.</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/2013EGUGA..15..217K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15..217K"><span>A coupling between geometry of the main <span class="hlt">geomagnetic</span> field tectonic margins and seismicity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khachikyan, Galina</p> <p>2013-04-01</p> <p>Integrated studies involving <span class="hlt">geomagnetism</span>, geodynamics, and seismology are essential for advances in understanding the Earth dynamics. This work presents recent results based of the International <span class="hlt">Geomagnetic</span> Reference Field (IGRF-10) model, Digital Tectonic Activity Map (DTAM-1), and the global seismological catalogue (173477 events for 1973-2010 with ?≥4.5). It will be shown that: 1. The geometry of the main <span class="hlt">geomagnetic</span> field controls a spatial distribution of seismicity around the globe. This becomes apparent when <span class="hlt">geomagnetic</span> field components are analyzed using the geocentric solar magnetospheric (GSM) coordinate system. Earthquakes prefer occur in the regions where <span class="hlt">geomagnetic</span> Z_GSM component reaches large positive value, that takes place at low and middle latitudes. In the areas of strongest seismicity, that takes place at low and mid latitudes in the eastern hemisphere, the Z_GSM values are largest compared to all other regions of the planet. The possible maximal magnitude of earthquake (Mmax) has a linear dependence on the logarithm of absolute Z_GSM value in the epicenter in the moment of earthquake occurrence. 2. There is a <span class="hlt">geomagnetic</span> conjugacy between certain tectonic structures. In particular, the middle ocean ridges located in the southern hemisphere along the boundary of the Antarctic tectonic plate are magnetically conjugate with the areas of junction of continental orogens and platforms in the northern hemisphere. Close magnetic conjugacy exists between southern boundary of the Nazca tectonic plate and northern boundaries of the Cocos and Caribbean plates. 3. <span class="hlt">Variations</span> in the total strength of the main <span class="hlt">geomagnetic</span> field could be associated, to some extent, with the earthquake occurrence. In particular, the IGRF-10 model shows that in the area of the major 2004 Sumatra earthquake (epicenter 3.3N; 95.98E), the strength of the main <span class="hlt">geomagnetic</span> field steadily increased from ~ 41338 nT in 1980 to ~ 41855 nT in 2004 with a mean change per year of about</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..559Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..559Z"><span>Applying the new method of time-frequency transforms to the analysis of the characteristics of <span class="hlt">geomagnetic</span> Pc5 pulsations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zelinsky, N. R.; Kleimenova, N. G.; Gromova, L. I.</p> <p>2017-09-01</p> <p>This study considers the possibility of using the new methods of time-frequency transforms, such as chirplet and warblet transforms, to analyze the digital observational data of <span class="hlt">geomagnetic</span> pulsations of Pc5 type. For this purpose, necessary algorithms of calculation and appropriate software were developed. The chirplet transform method (CT) is used to analyze signals with a linear frequency modulation. A chirplet <span class="hlt">variation</span>, the so-called warblet transform, is used to analyze signals with a nonlinear frequency modulation. Since, in studying <span class="hlt">geomagnetic</span> pulsations, it is difficult to make assumptions on the character of the behavior of the instantaneous frequency of the signal, the special generalized warblet transform (GWT) was used for the analysis. The GWT has a high spatiotemporal resolution and was developed to analyze oscillations both with a periodic and nonperiodic change of the instantaneous frequency. The software developed for GWT calculation was used to study daytime <span class="hlt">geomagnetic</span> Pc5 pulsations with durations of several hours that were detected via the network of ground-based magnetometers of the Scandinavian IMAGE profile during the magnetic storm of May 29-30, 2003. For the first time, temporal <span class="hlt">variations</span> of the instantaneous frequency of <span class="hlt">geomagnetic</span> pulsations are determined and their possible use in studying the fine spatial structure of Pc5 waves is shown.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AnGeo..26.3989S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AnGeo..26.3989S"><span>Forecasting intense <span class="hlt">geomagnetic</span> activity using interplanetary magnetic field data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saiz, E.; Cid, C.; Cerrato, Y.</p> <p>2008-12-01</p> <p>Southward interplanetary magnetic fields are considered traces of geoeffectiveness since they are a main agent of magnetic reconnection of solar wind and magnetosphere. The first part of this work revises the ability to forecast intense <span class="hlt">geomagnetic</span> activity using different procedures available in the literature. The study shows that current methods do not succeed in making confident predictions. This fact led us to develop a new forecasting procedure, which provides trustworthy results in predicting large <span class="hlt">variations</span> of Dst index over a sample of 10 years of observations and is based on the value Bz only. The proposed forecasting method appears as a worthy tool for space weather purposes because it is not affected by the lack of solar wind plasma data, which usually occurs during severe <span class="hlt">geomagnetic</span> activity. Moreover, the results obtained guide us to provide a new interpretation of the physical mechanisms involved in the interaction between the solar wind and the magnetosphere using Faraday's law.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060041462&hterms=geomagnetism&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dgeomagnetism','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060041462&hterms=geomagnetism&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dgeomagnetism"><span>The Causes of <span class="hlt">Geomagnetic</span> Storms During Solar Maximum</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsurutani, B. T.; Gonzalez, W. D.</p> <p>1998-01-01</p> <p>One of the oldest mysteries in <span class="hlt">geomagnetism</span> is the linkage between solar and <span class="hlt">geomagnetic</span> activity. The 11-year cycles of both the numbers of sunspots and Earth <span class="hlt">geomagnetic</span> storms were first noted by Sabine (1852).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20184151','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20184151"><span>[Influence of some weather factors and the <span class="hlt">geomagnetic</span> activity on the development of severe cardiological pathologies].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ozheredov, V A; Breus, T K; Gurfinkel', Iu I; Revich, B A; Mitrofanova, T A</p> <p>2010-01-01</p> <p>The influence of weather factors (atmospheric pressure and temperature) and the <span class="hlt">geomagnetic</span> activity on the development of severe cardiological pathologies has been studied using the daily data from two Moscow clinics, accumulated over a period of 12 and 7 years. It was shown that the most biotropic factors are <span class="hlt">variations</span> of atmospheric temperature. The relative contribution of the <span class="hlt">geomagnetic</span> activity to the development of diseases is only 20%; however, its action is combined with the effect of ordinary weather because both these factors affect the vascular tonus of humans.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApJ...807L...5N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApJ...807L...5N"><span>Asteroid <span class="hlt">Secular</span> Dynamics: Ceres’ Fingerprint Identified</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Novaković, Bojan; Maurel, Clara; Tsirvoulis, Georgios; Knežević, Zoran</p> <p>2015-07-01</p> <p>Here we report on the significant role of a so far overlooked dynamical aspect, namely, a <span class="hlt">secular</span> resonance between the dwarf planet Ceres and other asteroids. We demonstrate that this type of <span class="hlt">secular</span> resonance can be the dominant dynamical factor in certain regions of the main asteroid belt. Specifically, we performed a dynamical analysis of the asteroids belonging to the (1726) Hoffmeister family. To identify which dynamical mechanisms are actually at work in this part of the main asteroid belt, i.e., to isolate the main perturber(s), we study the evolution of this family in time. The study is accomplished using numerical integrations of test particles performed within different dynamical models. The obtained results reveal that the post-impact evolution of the Hoffmeister asteroid family is a direct consequence of the nodal <span class="hlt">secular</span> resonance with Ceres. This leads us to the conclusion that similar effects must exist in other parts of the asteroid belt. In this respect, the obtained results shed light on an important and entirely new aspect of the long-term dynamics of small bodies. Ceres’ fingerprint in asteroid dynamics, expressed through the discovered <span class="hlt">secular</span> resonance effect, completely changes our understanding of the way in which perturbations by Ceres-like objects affect the orbits of nearby bodies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770007709','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770007709"><span>The causes of recurrent <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Burlaga, L. F.; Lepping, R. P.</p> <p>1976-01-01</p> <p>The causes of recurrent <span class="hlt">geomagnetic</span> activity were studied by analyzing interplanetary magnetic field and plasma data from earth-orbiting spacecraft in the interval from November 1973 to February 1974. This interval included the start of two long sequences of <span class="hlt">geomagnetic</span> activity and two corresponding corotating interplanetary streams. In general, the <span class="hlt">geomagnetic</span> activity was related to an electric field which was due to two factors: (1) the ordered, mesoscale pattern of the stream itself, and (2) random, smaller-scale fluctuations in the southward component of the interplanetary magnetic field Bz. The <span class="hlt">geomagnetic</span> activity in each recurrent sequence consisted of two successive stages. The first stage was usually the most intense, and it occurred during the passage of the interaction region at the front of a stream. These large amplitudes of Bz were primarily produced in the interplanetary medium by compression of ambient fluctuations as the stream steepened in transit to 1 A.U. The second stage of <span class="hlt">geomagnetic</span> activity immediately following the first was associated with the highest speeds in the stream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040021339','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040021339"><span>The <span class="hlt">Geomagnetic</span> Field During a Reversal</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heirtzler, James R.</p> <p>2003-01-01</p> <p>By modifying the IGRF it is possible to learn what may happen to the <span class="hlt">geomagnetic</span> field during a <span class="hlt">geomagnetic</span> reversal. If the entire IGRF reverses then the declination and inclination only reverse when the field strength is zero. If only the dipole component of the IGRF reverses a large <span class="hlt">geomagnetic</span> field remains when the dipole component is zero and he direction of the field at the end of the reversal is not exactly reversed from the directions at the beginning of the reversal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFMSM43A1135K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFMSM43A1135K"><span>Earth-ionosphere transmission line model for an impulsive <span class="hlt">geomagnetic</span> disturbance at the dayside <span class="hlt">geomagnetic</span> equator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kikuchi, T.</p> <p>2004-12-01</p> <p>The near instantaneous onset of a <span class="hlt">geomagnetic</span> impulse such as the preliminary reverse impulse (PRI) of the <span class="hlt">geomagnetic</span> sudden commencement at high latitude and at the dayside <span class="hlt">geomagnetic</span> equator has been explained by means of the TM0 mode waves in the Earth-ionosphere waveguide (Kikuchi and Araki, J. Atmosph. Terrest. Phys., 41, 927-936, 1979). There is, on the other hand, a time lag of the order of 10 sec in the peak amplitude of the magnetic impulse at the dayside equator. To explain these two temporal aspects, we examine transmission of the TM0 mode in a finite-length Earth-ionosphere transmission line composed of a finitely conducting ionosphere and the perfectly conducting Earth, with a fixed electric potential at one end and null potential at the other end of the transmission line, corresponding to the foot of a field-aligned current on the dawn- or dusk-side in the polar cap and middle point on the noon-midnight meridian at low latitude, respectively. Successive transmission and reflection in the bounded transmission line lead to that the ionospheric currents start to grow instantaneously, but reach a steady state with a relaxation time proportional to the length of the transmission line and the ionospheric conductivity. The relaxation time is of the order of 10 sec when we give high conductivity applicable to the equatorial ionosphere, which matches the observed time lag in the peak amplitude of the equatorial <span class="hlt">geomagnetic</span> impulse. Consequently, the TM0 mode in the finite-length Earth-ionosphere transmission line explains both the instantaneous onset and time lag in the peak amplitude of the <span class="hlt">geomagnetic</span> impulse at the dayside <span class="hlt">geomagnetic</span> equator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930060109&hterms=alicia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dalicia%2Bd','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930060109&hterms=alicia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dalicia%2Bd"><span>Periodic <span class="hlt">variation</span> in the <span class="hlt">geomagnetic</span> activity - A study based on the Ap index</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>De Gonzalez, Alicia L. C.; Gonzalez, Walter D.; Dutra, Severino L. G.; Tsurutani, Bruce T.</p> <p>1993-01-01</p> <p>The monthly and daily samples of the Ap index for the interval from 1932 through 1982 were studied using the power spectrum technique. Results obtained for Bartel's period (about 27 days), the semiannual period, the dual-peak solar cycle distribution of <span class="hlt">geomagnetic</span> storms, and certain other medium-scale periodicities are examined in detail. In addition, results on the cumulative occurrence number of storms per decade as a function of the Ap and Dst indices for the storm are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP33B0975B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP33B0975B"><span>Five millions years of paleosecular <span class="hlt">variations</span> from the Golan Heights volcanic field, Israel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Behar, N.; Shaar, R.; Asefaw, H.; Ebert, Y.; Koppers, A.; Tauxe, L.</p> <p>2017-12-01</p> <p>One of the most fundamental assumption in paleomagnetism is that the averaged <span class="hlt">geomagnetic</span> field on geological timescales is a geocentric axial dipole (GAD). Given the first order importance of the GAD hypothesis, it is essential to rigorously test its validity and to understand the limits of its use. Additionally, it is equally vital to characterize statistically paleomagnetic <span class="hlt">secular</span> <span class="hlt">variations</span> (PSV) over timescales of 106 years. The Plio-Pleistocene volcanic field in the Golan Heights, Israel (32.7°N-33.3°N) is a nearly ideal location to investigate these issues, owing to excellent exposure of basaltic flows, dated using more than 100 radiometric (K/Ar and Ar/Ar) ages covering the past 5 Myr. Here we present new data from 89 basalt flows from the Golan Heights with ages spanning from 5.4 Ma to 0.1 Ma, and 18 new Ar/Ar ages. This relatively large dataset allows us to calculate three different Virtual <span class="hlt">Geomagnetic</span> Poles (VGP): Pleistocene, Pliocene, and a combined Plio-Pleistocene. From each pole we calculate the inclination anomaly (ΔI) and the VGP scatter parameter (SB). The Pleistocene pole yields a VGP scatter parameter around SB =13, lower than predictions of PSV models. Also, it demonstrates negligible inclination anomaly of less than 2°, suggesting validation of the GAD model. The Pliocene pole shows a larger scatter (SB 18) and a negative inclination anomaly around ΔI = -7°. We discuss these results in view of the worldwide paleomagnetic database and the available PSV models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSM33C2518C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSM33C2518C"><span>Solar Cycle and <span class="hlt">Geomagnetic</span> Activity <span class="hlt">Variation</span> of Topside Ionospheric Upflow as Measured by DMSP</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coley, W. R.; Hairston, M. R.</p> <p>2016-12-01</p> <p>Under the proper conditions a considerable amount of plasma can escape the Earth's ionosphere into the magnetosphere. Indeed, there are indications that at least part of the time the ionosphere may be the dominant source of ions for the plasma sheet and near-Earth portion of the magnetosphere. The upward flux of thermal O+ from the lower part of the topside ionosphere actively provides plasma into intermediate altitudes where they may be given escape energy by various mechanisms. Previous work has indicated that there is considerable time <span class="hlt">variation</span> of upwelling low energy ionospheric plasma to these intermediate altitudes during moderate to high solar activity. Here we use the SSIES thermal plasma instruments on board the Defense Meteorological Satellite Program (DMSP) F13-F19 series of spacecraft to examine the vertical flux of thermal O+ from the deep solar minimum of 2008-2009 to the moderately active period of 2012-2015. Separately integrating the upward and downward fluxes over the high-latitude region (auroral zone and polar cap) allows the observation of the total upflow/downflow as a function of the current <span class="hlt">geomagnetic</span> conditions, solar cycle, and solar wind conditions. In particular we investigate the incidence of high upward flux events as a function of solar wind velocity and density during the deepest solar minimum since the space age began.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4219698','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4219698"><span><span class="hlt">Secular</span> Trends in Menarcheal Age in India-Evidence from the Indian Human Development Survey</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Pathak, Praveen Kumar; Tripathi, Niharika; Subramanian, S. V.</p> <p>2014-01-01</p> <p>Background Evidence from a number of countries in Europe and North America point towards the <span class="hlt">secular</span> declining trend in menarcheal age with considerable spatial <span class="hlt">variations</span> over the past two centuries. Similar trends were reported in several developing countries from Asia, Africa and Latin America. However, data corroborating any <span class="hlt">secular</span> trend in the menarcheal age of the Indian population remained sparse and inadequately verified. Methods We examined <span class="hlt">secular</span> trends, regional heterogeneity and association of socioeconomic, anthropometric and contextual factors with menarcheal age among ever-married women (15–49 years) in India. Using the pseudo cohort data approach, we fit multiple linear regression models to estimate <span class="hlt">secular</span> trends in menarcheal age of 91394 ever-married women using the Indian Human Development Survey. Results The mean age at menarche among Indian women was 13.76 years (95 % CI: 13.75, 13.77) in 2005. It declined by three months from 13.83 years (95% CI: 13.81, 13.85) among women born prior to 1955–1964, to nearly 13.62 years (95% CI: 13.58, 13.67) among women born during late 1985–1989. However, these aggregate national figures mask extensive spatial heterogeneity as mean age at menarche varied from 15.0 years in Himachal Pradesh during 1955–1964 (95% CI: 14.89–15.11) to about 12.1 years in Assam (95% CI: 11.63–12.56) during 1985–1989. Conclusion The regression analysis established a reduction of nearly one month per decade, suggesting a <span class="hlt">secular</span> decline in age at menarche among Indian women. Notably, the menarcheal age was significantly associated with the area of residence, geographic region, linguistic groups, educational attainment, wealth status, caste and religious affiliations among Indian women. PMID:25369507</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007EP%26S...59..807H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007EP%26S...59..807H"><span>Environmental magnetic record and paleosecular <span class="hlt">variation</span> data for the last 40 kyrs from the Lake Biwa sediments, Central Japan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hayashida, Akira; Ali, Mohammed; Kuniko, Yoshiki; Kitagawa, Hiroyuki; Torii, Masayuki; Takemura, Keiji</p> <p>2007-07-01</p> <p>We have conducted paleomagnetic and environmental magnetic analysis of a sediment piston core recovered from Lake Biwa, central Japan. Tephrochronology and AMS radiocarbon dating showed that this core covers the time period since about 40 kyr BP. The <span class="hlt">variation</span> of paleomagnetic direction shows a good agreement with the PSV record for the last 10 kyrs from the deeper water site (BIWA SV-3; Ali et al., 1999), although the amplitudes are subdued probably due to the relatively lower accumulation rate at the shallower site. Inclination lows of the pre-Holocene interval are correlated to PSV records reported from the marine sediments off Shikoku and in the Japan Sea. In addition, the <span class="hlt">variation</span> of magnetic mineral concentration reflects environmental changes during the last glacial period. It is suggested that the flux of fine-grained magnetite, probably associated with greater precipitation, was increased during interstadial periods. The <span class="hlt">variation</span> of anhysteretic remanent magnetization is likely correlated to the Dansgaard-Oeschger (D-O) cycles recorded in Greenland ice cores. An apparent swing of the PSV curve is recognized at about 27 ka, but evidence for the Mono Lake excursion at 32 ka around the D-O events 6 and 7 is unclear. Combination of the detailed paleomagnetic record and the sub-Milankovitch climate cycles thus provides better resolution for understanding <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> and polarity excursions in space and time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20857575','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20857575"><span>Sex, <span class="hlt">secularism</span> and religious influence in US politics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bernstein, Elizabeth; Jakobsen, Janet R</p> <p>2010-01-01</p> <p>Through an analysis of alliances between <span class="hlt">secular</span> and religious actors in US politics and a specific case study on anti-trafficking policy, we show that the intertwining of religion and politics in the US comes from two sources: 1) the <span class="hlt">secular</span> political and cultural institutions of American public life that have developed historically out of Protestantism, and which predominantly operate by presuming Protestant norms and values; and 2) the direct influence on US politics of religious groups and organisations, particularly in the past quarter-century of lobby groups and political action committees identified with conservative evangelical Christianity. The sources of policies that promote gender and sexual inequality in the US are both <span class="hlt">secular</span> and religious and we conclude that it is inaccurate to assume that religious influence in politics is necessarily conservative or that more <span class="hlt">secular</span> politics will necessarily be more progressive than the religious varieties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70045124','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70045124"><span>Uncovering the nonadiabatic response of geosynchronous electrons to <span class="hlt">geomagnetic</span> disturbance</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Gannon, Jennifer; Elkington, Scot R.; Onsager, Terrance G.</p> <p>2012-01-01</p> <p>We describe an energy spectrum method for scaling electron integral flux, which is measured at a constant energy, to phase space density at a constant value of the first adiabatic invariant which removes much of the <span class="hlt">variation</span> due to reversible adiabatic effects. Applying this method to nearly a solar cycle (1995 - 2006) of geosynchronous electron integral flux (E>2.0MeV) from the GOES satellites, we see that much of the diurnal <span class="hlt">variation</span> in electron phase space density at constant energy can be removed by the transformation to phase space density at constant μ (4000 MeV/G). This allows us a clearer picture of underlying non-adiabatic electron population changes due to <span class="hlt">geomagnetic</span> activity. Using scaled phase space density, we calculate the percentage of <span class="hlt">geomagnetic</span> storms resulting in an increase, decrease or no change in geosynchronous electrons as 38%, 7%, and 55%, respectively. We also show examples of changes in the electron population that may be different than the unscaled fluxes alone suggest. These examples include sudden electron enhancements during storms which appear during the peak of negative Dst for μ-scaled phase space density, contrary to the slow increase seen during the recovery phase for unscaled phase space density for the same event.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP33C..02A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP33C..02A"><span>Towards a fully self-consistent inversion combining historical and paleomagnetic data for <span class="hlt">geomagnetic</span> field reconstructions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arneitz, P.; Leonhardt, R.; Fabian, K.; Egli, R.</p> <p>2017-12-01</p> <p>Historical and paleomagnetic data are the two main sources of information about the long-term <span class="hlt">geomagnetic</span> field evolution. Historical observations extend to the late Middle Ages, and prior to the 19th century, they consisted mainly of pure declination measurements from navigation and orientation logs. Field reconstructions going back further in time rely solely on magnetization acquired by rocks, sediments, and archaeological artefacts. The combined dataset is characterized by a strongly inhomogeneous spatio-temporal distribution and highly variable data reliability and quality. Therefore, an adequate weighting of the data that correctly accounts for data density, type, and realistic error estimates represents the major challenge for an inversion approach. Until now, there has not been a fully self-consistent <span class="hlt">geomagnetic</span> model that correctly recovers the <span class="hlt">variation</span> of the <span class="hlt">geomagnetic</span> dipole together with the higher-order spherical harmonics. Here we present a new <span class="hlt">geomagnetic</span> field model for the last 4 kyrs based on historical, archeomagnetic and volcanic records. The iterative Bayesian inversion approach targets the implementation of reliable error treatment, which allows different record types to be combined in a fully self-consistent way. Modelling results will be presented along with a thorough analysis of model limitations, validity and sensitivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Ge%26Ae..58..201K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Ge%26Ae..58..201K"><span><span class="hlt">Geomagnetic</span> Storm Effects at F1 Layer Altitudes in Various Periods of Solar Activity (Irkutsk Station)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kushnarenko, G. P.; Yakovleva, O. E.; Kuznetsova, G. M.</p> <p>2018-03-01</p> <p>The influence of <span class="hlt">geomagnetic</span> disturbances on electron density Ne at F1 layer altitudes in different conditions of solar activity during the autumnal and vernal seasons of 2003-2015, according to the data from the Irkutsk digital ionospheric station (52° N, 104° E) is examined. <span class="hlt">Variations</span> of Ne at heights of 150-190 km during the periods of twenty medium-scale and strong <span class="hlt">geomagnetic</span> storms have been analyzed. At these specified heights, a vernal-autumn asymmetry of <span class="hlt">geomagnetic</span> storm effects is discovered in all periods of solar activity of 2003-2015: a considerable Ne decrease at a height of 190 km and a weaker effect at lower levels during the autumnal storms. During vernal storms, no significant Ne decrease as compared with quiet conditions was registered over the entire analyzed interval of 150-190 km.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770048052&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dearths%2Bouter%2Bcore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770048052&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dearths%2Bouter%2Bcore"><span>Thermal interaction of the core and the mantle and long-term behavior of the <span class="hlt">geomagnetic</span> field</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jones, G. M.</p> <p>1977-01-01</p> <p>The effects of temperature changes at the earth's core-mantle boundary on the velocity field of the core are analyzed. It is assumed that the <span class="hlt">geomagnetic</span> field is maintained by thermal convection in the outer core. A model for the thermal interaction of the core and the mantle is presented which is consistent with current views on the presence of heat sources in the core and the properties of the lower mantle. Significant long-term <span class="hlt">variations</span> in the frequency of <span class="hlt">geomagnetic</span> reversals may be the result of fluctuating temperatures at the core-mantle boundary, caused by intermittent convection in the lower mantle. The thermal structure of the lower mantle region D double prime, extending from 2700 to 2900 km in depth, constitutes an important test of this hypothesis and offers a means of deciding whether the <span class="hlt">geomagnetic</span> dynamo is thermally driven.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914014M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914014M"><span>Electrical conductivity structure of the mantle derived from inversion of <span class="hlt">geomagnetic</span> observatory data: implications for lateral <span class="hlt">variations</span> in temperature, composition and water content.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Munch, Federico; Grayver, Alexander; Khan, Amir; Kuvshinov, Alexey</p> <p>2017-04-01</p> <p>As most of Earth's interior remains geochemically unsampled, geophysical techniques based on seismology, geodesy, gravimetry, and electromagnetic studies play prominent roles because of their ability to sense structure at depth. Although seismic tomography maps show a variety of structures, separating thermal and compositional contributions from seismic velocities alone still remains a challenging task. Alternatively, as electrical conductivity is sensitive to temperature, chemical composition, oxygen fugacity, water content, and the presence of melt, it can serve for determining chemistry, mineralogy, and physical structure of the deep mantle. In this work we estimate and invert local C-responses (period range 3-100 days) for a number of worldwide <span class="hlt">geomagnetic</span> observatories to map lateral <span class="hlt">variations</span> of electrical conductivity in Earth's mantle (400-1600 km depth). The obtained conductivity profiles are interpreted in terms of basalt fraction in a basalt-harzburgite mixture, temperature structure, and water content <span class="hlt">variations</span>. Interpretation is based on a self-consistent thermodynamic calculation of mineral phase equilibria, electrical conductivity databases, and probabilistic inverse methods.</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('https://www.ncbi.nlm.nih.gov/pubmed/23700198','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23700198"><span>The influence of meteorological and <span class="hlt">geomagnetic</span> factors on acute myocardial infarction and brain stroke in Moscow, Russia.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shaposhnikov, Dmitry; Revich, Boris; Gurfinkel, Yuri; Naumova, Elena</p> <p>2014-07-01</p> <p>Evidence of the impact of air temperature and pressure on cardiovascular morbidity is still quite limited and controversial, and even less is known about the potential influence of <span class="hlt">geomagnetic</span> activity. The objective of this study was to assess impacts of air temperature, barometric pressure and <span class="hlt">geomagnetic</span> activity on hospitalizations with myocardial infarctions and brain strokes. We studied 2,833 myocardial infarctions and 1,096 brain strokes registered in two Moscow hospitals between 1992 and 2005. Daily event rates were linked with meteorological and <span class="hlt">geomagnetic</span> conditions, using generalized linear model with controls for day of the week, seasonal and long-term trends. The number of myocardial infarctions decreased with temperature, displayed a U-shaped relationship with pressure and <span class="hlt">variations</span> in pressure, and increased with <span class="hlt">geomagnetic</span> activity. The number of strokes increased with temperature, daily temperature range and <span class="hlt">geomagnetic</span> activity. Detrimental effects on strokes of low pressure and falling pressure were observed. Relative risks of infarctions and strokes during <span class="hlt">geomagnetic</span> storms were 1.29 (95% CI 1.19-1.40) and 1.25 (1.10-1.42), respectively. The number of strokes doubled during cold spells. The influence of barometric pressure on hospitalizations was relatively greater than the influence of <span class="hlt">geomagnetic</span> activity, and the influence of temperature was greater than the influence of pressure. Brain strokes were more sensitive to inclement weather than myocardial infarctions. This paper provides quantitative estimates of the expected increases in hospital admissions on the worst days and can help to develop preventive health plans for cardiovascular diseases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4329055-solar-plasma-geomagnetism-aurora','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4329055-solar-plasma-geomagnetism-aurora"><span>Solar plasma <span class="hlt">geomagnetism</span> and aurora</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>Chapman, S.</p> <p>1968-01-01</p> <p>This book is based on lectures given in July 1962 at the 12th session of the Les Houches Summer School of Theoretical Physics. Topics considered include <span class="hlt">geomagnetism</span> and related phenomena, solar plasma in interplanetary space, mutual influence of the solar gas and the <span class="hlt">geomagnetic</span> field. magnetic disturbance and aurorae, and the ring current and its DR field. (WDM)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EOSTr..84..586H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EOSTr..84..586H"><span>Introduction to <span class="hlt">Geomagnetic</span> Fields</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hinze, William J.</p> <p></p> <p>Coincidentally, as I sat down in late October 2003 to read and review the second edition of Wallace H. Campbell's text, Introduction to <span class="hlt">Geomagnetic</span> Fields, we received warnings from the news media of a massive solar flare and its possible effect on power supply systems and satellite communications. News programs briefly explained the source of Sun-Earth interactions. If you are interested in learning more about the physics of the connection between sun spots and power supply systems and their impact on orbiting satellites, I urge you to become acquainted with Campbell's book. It presents an interesting and informative explanation of the <span class="hlt">geomagnetic</span> field and its applications to a wide variety of topics, including oil exploration, climate change, and fraudulent claims of the utility of magnetic fields for alleviating human pain. <span class="hlt">Geomagnetism</span>, the study of the nature and processes of the Earth's magnetic fields and its application to the investigation of the Earth, its processes, and history, is a mature science with a well-developed theoretical foundation and a vast array of observations. It is discussed in varied detail in Earth physics books and most entry-level geoscience texts. The latter treatments largely are driven by the need to discuss paleomagnetism as an essential tool in studying plate tectonics. A more thorough explanation of <span class="hlt">geomagnetism</span> is needed by many interested scientists in related fields and by laypersons. This is the objective of Campbell's book. It is particularly germane in view of a broad range of <span class="hlt">geomagnetic</span> topics that are at the forefront of today's science, including environmental magnetism, so-called ``jerks'' observed in the Earth's magnetic field, the perplexing magnetic field of Mars, improved satellite magnetic field observations, and the increasing availability of high-quality continental magnetic anomaly maps, to name only a few.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/fs/0177-97/report.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/fs/0177-97/report.pdf"><span>On the watch for <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Green, Arthur W.; Brown, William M.</p> <p>1997-01-01</p> <p><span class="hlt">Geomagnetic</span> storms, induced by solar activity, pose significant hazards to satellites, electrical power distribution systems, radio communications, navigation, and geophysical surveys. Strong storms can expose astronauts and crews of high-flying aircraft to dangerous levels of radiation. Economic losses from recent <span class="hlt">geomagnetic</span> storms have run into hundreds of millions of dollars. With the U.S. Geological Survey (USGS) as the lead agency, an international network of <span class="hlt">geomagnetic</span> observatories monitors the onset of solar-induced storms and gives warnings that help diminish losses to military and commercial operations and facilities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1710135D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1710135D"><span>On the scaling features of high-latitude <span class="hlt">geomagnetic</span> field fluctuations during a large <span class="hlt">geomagnetic</span> storm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>De Michelis, Paola; Federica Marcucci, Maria; Consolini, Giuseppe</p> <p>2015-04-01</p> <p>Recently we have investigated the spatial distribution of the scaling features of short-time scale magnetic field fluctuations using measurements from several ground-based <span class="hlt">geomagnetic</span> observatories distributed in the northern hemisphere. We have found that the scaling features of fluctuations of the horizontal magnetic field component at time scales below 100 minutes are correlated with the <span class="hlt">geomagnetic</span> activity level and with changes in the currents flowing in the ionosphere. Here, we present a detailed analysis of the dynamical changes of the magnetic field scaling features as a function of the <span class="hlt">geomagnetic</span> activity level during the well-known large <span class="hlt">geomagnetic</span> storm occurred on July, 15, 2000 (the Bastille event). The observed dynamical changes are discussed in relationship with the changes of the overall ionospheric polar convection and potential structure as reconstructed using SuperDARN data. This work is supported by the Italian National Program for Antarctic Research (PNRA) - Research Project 2013/AC3.08 and by the European Community's Seventh Framework Programme ([FP7/2007-2013]) under Grant no. 313038/STORM and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.3474B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.3474B"><span>Sparkling <span class="hlt">Geomagnetic</span> Field: Involving Schools in <span class="hlt">Geomagnetic</span> Research</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bailey, Rachel; Leonhardt, Roman; Leichter, Barbara</p> <p>2014-05-01</p> <p>Solar activity will be reaching a maximum in 2013/2014 as the sun reaches the end of its cycle, bringing with it an opportunity to study in greater detail the effect of solar wind or "space weather" on our planet's magnetic field. Heightened solar activity leads to a larger amount of clouds of energetic particles bombarding the Earth. Although the Earth's magnetic field shields us from most of these particles, the field becomes distorted and compacted by the solar wind, which leads to magnetic storms that we detect from the surface. These storms cause aurorae at higher latitudes and can lead to widespread disruption of communication and navigation equipment all over the Earth when sufficiently strong. This project, "Sparkling <span class="hlt">Geomagnetic</span> Field," is a part of Austria's Sparkling Science programme, which aims to involve schools in active scientific research to encourage interest in science from a young age. Researchers from the Central Institute for Meteorology and Geodynamics (ZAMG) in Vienna have worked hand-in-hand with three schools across Austria to set up regional <span class="hlt">geomagnetic</span> stations consisting of state-of-the-art scalar and vector magnetometers to monitor the effects of the solar wind on the <span class="hlt">geomagnetic</span> field. The students have been an active part of the research team from the beginning, first searching for a suitable location to set up the stations as well as later overseeing the continued running of the equipment and analysing the data output. Through this project the students will gain experience in contemporary scientific methods: data processing and analysis, field work, as well as equipment setup and upkeep. A total of three stations have been established with schools in Innsbruck, Tamsweg and Graz at roughly equal distances across Austria to run alongside the already active station in the Conrad Observatory near Vienna. Data acquisition runs through a data logger and software developed to deliver data in near realtime. This network allows for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999RvGeo..37..201M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999RvGeo..37..201M"><span><span class="hlt">Geomagnetic</span> polarity transitions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Merrill, Ronald T.; McFadden, Phillip L.</p> <p>1999-05-01</p> <p>The top of Earth's liquid outer core is nearly 2900 km beneath Earth's surface, so we will never be able to observe it directly. This hot, dense, molten iron-rich body is continuously in motion and is the source of Earth's magnetic field. One of the most dynamic manifestations at Earth's surface of this fluid body is, perhaps, a reversal of the <span class="hlt">geomagnetic</span> field. Unfortunately, the most recent polarity transition occurred at about 780 ka, so we have never observed a transition directly. It seems that a polarity transition spans many human lifetimes, so no human will ever witness the phenomenon in its entirety. Thus we are left with the tantalizing prospect that paleomagnetic records of polarity transitions may betray some of the secrets of the deep Earth. Certainly, if there are systematics in the reversal process and they can be documented, then this will reveal substantial information about the nature of the lowermost mantle and of the outer core. Despite their slowness on a human timescale, polarity transitions occur almost instantaneously on a geological timescale. This rapidity, together with limitations in the paleomagnetic recording process, prohibits a comprehensive description of any reversal transition both now and into the foreseeable future, which limits the questions that may at this stage be sensibly asked. The natural model for the <span class="hlt">geomagnetic</span> field is a set of spherical harmonic components, and we are not able to obtain a reliable model for even the first few harmonic terms during a transition. Nevertheless, it is possible, in principle, to make statements about the harmonic character of a <span class="hlt">geomagnetic</span> polarity transition without having a rigorous spherical harmonic description of one. For example, harmonic descriptions of recent <span class="hlt">geomagnetic</span> polarity transitions that are purely zonal can be ruled out (a zonal harmonic does not change along a line of latitude). Gleaning information about transitions has proven to be difficult, but it does seem</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010GeoJI.183.1239K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010GeoJI.183.1239K"><span>Anomaly of the <span class="hlt">geomagnetic</span> Sq <span class="hlt">variation</span> in Japan: effect from 3-D subterranean structure or the ocean effect?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuvshinov, Alexei; Utada, Hisashi</p> <p>2010-12-01</p> <p>Many years ago Rikitake et al. described the anomalous behaviour of the vertical component Z of the <span class="hlt">geomagnetic</span> solar quiet (Sq) daily <span class="hlt">variation</span> field at observatories in central and northern Japan - namely about 2 hr shift of the local noontime peak towards morning hours. They suggested that this anomaly is associated with the anomalous distribution of electrical conductivity in the mantle beneath central Japan. Although a few works have been done to confirm or argue this explanation, no clear answer has been obtained so far. The goal of this work is to understand the nature of this anomaly using our 3-D forward solution. The conductivity model of the Earth includes oceans of laterally variable conductance and conducting mantle either spherically symmetric or 3-D underneath. Data from six Japanese observatories at four seasons for two different years of the solar cycle are analysed. As an inducing ionospheric (Sq) current system, we use those provided by the Comprehensive Model (CM4) of Sabaka et al. Our analysis clearly demonstrates that 3-D induction in the ocean is responsible for the anomalous behaviour of Z daily <span class="hlt">variations</span> in this region. We also show that the effects from a suite of 3-D mantle models that include mantle wedge and subducting slab are minor compared with the ocean effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5551208','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5551208"><span>Synchronization of Human Autonomic Nervous System Rhythms with <span class="hlt">Geomagnetic</span> Activity in Human Subjects</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>McCraty, Rollin; Atkinson, Mike; Stolc, Viktor; Alabdulgader, Abdullah A.; Vainoras, Alfonsas</p> <p>2017-01-01</p> <p>A coupling between <span class="hlt">geomagnetic</span> activity and the human nervous system’s function was identified by virtue of continuous monitoring of heart rate variability (HRV) and the time-varying <span class="hlt">geomagnetic</span> field over a 31-day period in a group of 10 individuals who went about their normal day-to-day lives. A time series correlation analysis identified a response of the group’s autonomic nervous systems to various dynamic changes in the solar, cosmic ray, and ambient magnetic field. Correlation coefficients and p values were calculated between the HRV variables and environmental measures during three distinct time periods of environmental activity. There were significant correlations between the group’s HRV and solar wind speed, Kp, Ap, solar radio flux, cosmic ray counts, Schumann resonance power, and the total <span class="hlt">variations</span> in the magnetic field. In addition, the time series data were time synchronized and normalized, after which all circadian rhythms were removed. It was found that the participants’ HRV rhythms synchronized across the 31-day period at a period of approximately 2.5 days, even though all participants were in separate locations. Overall, this suggests that daily autonomic nervous system activity not only responds to changes in solar and <span class="hlt">geomagnetic</span> activity, but is synchronized with the time-varying magnetic fields associated with <span class="hlt">geomagnetic</span> field-line resonances and Schumann resonances. PMID:28703754</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70197163','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70197163"><span>Geophysics: A reversal of <span class="hlt">geomagnetic</span> polarity</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Mankinen, Edward A.</p> <p>1986-01-01</p> <p>The detailed behaviour of the <span class="hlt">geomagnetic</span> field during reversals is documented by palaeomagnetists to constrain models of the <span class="hlt">geomagnetic</span> dynamo. Reversals are studied by measuring the magnetic remanence preserved in rocks to obtain both the direction and intensity of the ancient magnetic field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830057091&hterms=geomagnetism&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgeomagnetism','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830057091&hterms=geomagnetism&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgeomagnetism"><span><span class="hlt">Geomagnetism</span> of earth's core</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Benton, E. R.</p> <p>1983-01-01</p> <p>Instrumentation, analytical methods, and research goals for understanding the behavior and source of geophysical magnetism are reviewed. Magsat, launched in 1979, collected global magnetometer data and identified the main terrestrial magnetic fields. The data has been treated by representing the curl-free field in terms of a scalar potential which is decomposed into a truncated series of spherical harmonics. Solutions to the Laplace equation then extend the field upward or downward from the measurement level through intervening spaces with no source. Further research is necessary on the interaction between harmonics of various spatial scales. Attempts are also being made to analytically model the main field and its <span class="hlt">secular</span> <span class="hlt">variation</span> at the core-mantle boundary. Work is also being done on characterizing the core structure, composition, thermodynamics, energetics, and formation, as well as designing a new Magsat or a tethered satellite to be flown on the Shuttle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17735224','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17735224"><span><span class="hlt">Geomagnetic</span> Reversals during the Phanerozoic.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McElhinny, M W</p> <p>1971-04-09</p> <p>An antalysis of worldwide paleomagnetic measurements suggests a periodicity of 350 x 10(6) years in the polarity of the <span class="hlt">geomagnetic</span> field. During the Mesozoic it is predominantly normal, whereas during the Upper Paleozoic it is predominantly reversed. Although <span class="hlt">geomagnetic</span> reversals occur at different rates throughout the Phanerozoic, there appeaars to be no clear correlation between biological evolutionary rates and reversal frequency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914028M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914028M"><span>Long series of <span class="hlt">geomagnetic</span> measurements - unique at satellite era</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mandea, Mioara; Balasis, Georgios</p> <p>2017-04-01</p> <p>We have long appreciated that magnetic measurements obtained at Earth's surface are of great value in characterizing <span class="hlt">geomagnetic</span> field behavior and then probing the deep interior of our Planet. The existence of new magnetic satellite missions data offer a new detailed global understanding of the <span class="hlt">geomagnetic</span> field. However, when our interest moves over long-time scales, the very long series of measurements play an important role. Here, we firstly provide an updated series of <span class="hlt">geomagnetic</span> declination in Paris, shortly after a very special occasion: its value has reached zero after some 350 years of westerly values. We take this occasion to emphasize the importance of long series of continuous measurements, mainly when various techniques are used to detect the abrupt changes in <span class="hlt">geomagnetic</span> field, the <span class="hlt">geomagnetic</span> jerks. Many novel concepts originated in dynamical systems or information theory have been developed, partly motivated by specific research questions from the geosciences. This continuously extending toolbox of nonlinear time series analysis is a key to understand the complexity of <span class="hlt">geomagnetic</span> field. Here, motivated by these efforts, a series of entropy analysis are applied to <span class="hlt">geomagnetic</span> field time series aiming to detect dynamical complex changes associated with <span class="hlt">geomagnetic</span> jerks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950058567&hterms=geomagnetism&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dgeomagnetism','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950058567&hterms=geomagnetism&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dgeomagnetism"><span>The causes of <span class="hlt">geomagnetic</span> storms during solar maximum</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsurutani, Bruce T.; Gonzalez, Walter D.</p> <p>1994-01-01</p> <p>One of the oldest mysteries in <span class="hlt">geomagnetism</span> is the linkage between solar and <span class="hlt">geomagnetic</span> activity. In investigating the causes of <span class="hlt">geomagnetic</span> storms occurring during solar maximum, the following topics are discussed: solar phenomena; types of solar wind; magnetic reconnection and magnetic storms; an interplanetary example; and future space physics missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMSA31D2362H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMSA31D2362H"><span>Great Lakes Region Morphology and Impacts of March 17, 2015 SED <span class="hlt">Geomagnetic</span> Storm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heine, T.; Moldwin, M.; Zou, S.</p> <p>2015-12-01</p> <p>Under quiet <span class="hlt">geomagnetic</span> conditions, the mid-latitude ionosphere is relatively uniform with little spatial <span class="hlt">variation</span> in electron density. However, during intense <span class="hlt">geomagnetic</span> storms, density gradients associated with Storm Enhanced Density (SED) plumes and Sub-auroral Polarization Streams (SAPS) can move across the dayside mid-latitude ionosphere producing small spatial scale density structure that may be connected to ionospheric scintillation. The evolution of the SED plume during the March 17, 2015 "St. Patrick's Day Storm" is investigated using aggregated data from high resolution GPS receivers at the University of Michigan and throughout the Great Lakes region. Structural density features in the SED gradient can be observed and compared to GPS scintillation measurements—providing insight into the physical mechanisms behind ionospheric scintillation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/EJ1051719.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/EJ1051719.pdf"><span>Rethinking Institutional <span class="hlt">Secularization</span> as an (Im)possible "Policy"</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>Gomez Caride, Ezequiel</p> <p>2015-01-01</p> <p>The paper analyzes through a genealogical discourse analysis how religion as a cultural practice escapes into the borders of state institutions. While most studies about <span class="hlt">secularization</span> focus on institutional aspects, such approaches tend to link state secularist policies with cultural <span class="hlt">secularization</span>. This essay argues that state promotion of…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1814496C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1814496C"><span>Spurious behavior in volcanic records of <span class="hlt">geomagnetic</span> field reversals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carlut, Julie; Vella, Jerome; Valet, Jean-Pierre; Soler, Vicente; Legoff, Maxime</p> <p>2016-04-01</p> <p>Very large directional <span class="hlt">variations</span> of magnetization have been reported in several lava flows recording a <span class="hlt">geomagnetic</span> reversal. Such behavior could reflect real <span class="hlt">geomagnetic</span> changes or be caused by artifacts due to post-emplacement alteration and/or non-ideal magnetic behavior. More recently, a high resolution paleomagnetic record from sediments pleads also for an extremely rapid reversal process during the last reversal. Assuming that the <span class="hlt">geomagnetic</span> field would have moved by tens of degrees during cooling of moderate thickness lava flows implies brief episodes of rapid changes by a few degrees per day that are difficult to reconcile with the rate of liquid motions at the core surface. Systematical mineralogical bias is a most likely explanation to promote such behavior as recently reconsidered by Coe et al., 2014 for the rapid field changes recorded at Steens Mountain. We resampled three lava flows at La Palma island (Canarias) that are sandwiched between reverse polarity and normal polarity flows associated with the last reversal. The results show an evolution of the magnetization direction from top to bottom. Thermal demagnetization experiments were conducted using different heating and cooling rates. Similarly, continuous demagnetization and measurements. In both cases, we did not notice any remagnetization associated with mineralogical transformations during the experiments. Magnetic grain sizes do not show any correlation with the amplitude of the deviations. Microscopic observations indicate poor exsolution, which could suggests post-cooling thermochemical remagnetization processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SpWea..14.1136B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SpWea..14.1136B"><span><span class="hlt">Geomagnetically</span> induced currents in the Irish power network during <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Blake, Seán. P.; Gallagher, Peter T.; McCauley, Joe; Jones, Alan G.; Hogg, Colin; Campanyà, Joan; Beggan, Ciarán. D.; Thomson, Alan W. P.; Kelly, Gemma S.; Bell, David</p> <p>2016-12-01</p> <p><span class="hlt">Geomagnetically</span> induced currents (GICs) are a well-known terrestrial space weather hazard. They occur in power transmission networks and are known to have adverse effects in both high-latitude and midlatitude countries. Here we study GICs in the Irish power transmission network (<span class="hlt">geomagnetic</span> latitude 54.7-58.5°N) during five <span class="hlt">geomagnetic</span> storms (6-7 March 2016, 20-21 December 2015, 17-18 March 2015, 29-31 October 2003, and 13-14 March 1989). We simulate electric fields using a plane wave method together with two ground resistivity models, one of which is derived from magnetotelluric measurements (magnetotelluric (MT) model). We then calculate GICs in the 220, 275, and 400 kV transmission network. During the largest of the storm periods studied, the peak electric field was calculated to be as large as 3.8 V km-1, with associated GICs of up to 23 A using our MT model. Using our homogenous resistivity model, those peak values were 1.46 V km-1 and 25.8 A. We find that three 400 and 275 kV substations are the most likely locations for the Irish transformers to experience large GICs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23394828','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23394828"><span>Evidence for <span class="hlt">geomagnetic</span> imprinting as a homing mechanism in Pacific salmon.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Putman, Nathan F; Lohmann, Kenneth J; Putman, Emily M; Quinn, Thomas P; Klimley, A Peter; Noakes, David L G</p> <p>2013-02-18</p> <p>In the final phase of their spawning migration, Pacific salmon use chemical cues to identify their home river, but how they navigate from the open ocean to the correct coastal area has remained enigmatic. To test the hypothesis that salmon imprint on the magnetic field that exists where they first enter the sea and later seek the same field upon return, we analyzed a 56-year fisheries data set on Fraser River sockeye salmon, which must detour around Vancouver Island to approach the river through either a northern or southern passageway. We found that the proportion of salmon using each route was predicted by <span class="hlt">geomagnetic</span> field drift: the more the field at a passage entrance diverged from the field at the river mouth, the fewer fish used the passage. We also found that more fish used the northern passage in years with warmer sea surface temperature (presumably because fish were constrained to more northern latitudes). Field drift accounted for 16% of the <span class="hlt">variation</span> in migratory route used, temperature 22%, and the interaction between these variables 28%. These results provide the first empirical evidence of <span class="hlt">geomagnetic</span> imprinting in any species and imply that forecasting salmon movements is possible using <span class="hlt">geomagnetic</span> models. Copyright © 2013 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...854...31J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...854...31J"><span>The JCMT Transient Survey: Stochastic and <span class="hlt">Secular</span> Variability of Protostars and Disks In the Submillimeter Region Observed over 18 Months</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Johnstone, Doug; Herczeg, Gregory J.; Mairs, Steve; Hatchell, Jennifer; Bower, Geoffrey C.; Kirk, Helen; Lane, James; Bell, Graham S.; Graves, Sarah; Aikawa, Yuri; Chen, Huei-Ru Vivien; Chen, Wen-Ping; Kang, Miju; Kang, Sung-Ju; Lee, Jeong-Eun; Morata, Oscar; Pon, Andy; Scicluna, Peter; Scholz, Aleks; Takahashi, Satoko; Yoo, Hyunju; The JCMT Transient Team</p> <p>2018-02-01</p> <p>We analyze results from the first 18 months of monthly submillimeter monitoring of eight star-forming regions in the JCMT Transient Survey. In our search for stochastic variability in 1643 bright peaks, only the previously identified source, EC 53, shows behavior well above the expected measurement uncertainty. Another four sources—two disks and two protostars—show moderately enhanced standard deviations in brightness, as expected for stochastic variables. For the two protostars, this apparent variability is the result of single epochs that are much brighter than the mean. In our search for <span class="hlt">secular</span> brightness <span class="hlt">variations</span> that are linear in time, we measure the fractional brightness change per year for 150 bright peaks, 50 of which are protostellar. The ensemble distribution of slopes is well fit by a normal distribution with σ ∼ 0.023. Most sources are not rapidly brightening or fading at submillimeter wavelengths. Comparison against time-randomized realizations shows that the width of the distribution is dominated by the uncertainty in the individual brightness measurements of the sources. A toy model for <span class="hlt">secular</span> variability reveals that an underlying Gaussian distribution of linear fractional brightness change σ = 0.005 would be unobservable in the present sample, whereas an underlying distribution with σ = 0.02 is ruled out. Five protostellar sources, 10% of the protostellar sample, are found to have robust <span class="hlt">secular</span> measures deviating from a constant flux. The sensitivity to <span class="hlt">secular</span> brightness <span class="hlt">variations</span> will improve significantly with a sample over a longer time duration, with an improvement by factor of two expected by the conclusion of our 36 month survey.</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://hdl.handle.net/2060/19730017649','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730017649"><span>Plate motion and the <span class="hlt">secular</span> shift of the mean pole</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liu, H.; Carpenter, L.; Agreen, R. W.</p> <p>1973-01-01</p> <p>The global plate motion indicates that changes in the products of inertia of the earth due to tectonic plate movement may provide a <span class="hlt">secular</span> shift of the mean pole. A mathematical procedure for calculating this shift based on the plate theory is presented. Explicit expressions were obtained for the dependence of the <span class="hlt">secular</span> polar shift on the dimensions and locations of the plate boundaries. Numerical results show that the <span class="hlt">secular</span> motion of the mean pole is 0.0002 sec/year in the direction of 67 W. Hence, it is deduced that the influence of the plate motion on the <span class="hlt">secular</span> polar shift may account for 10% of the observed value.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011MNRAS.415.2275M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011MNRAS.415.2275M"><span>Modelling the <span class="hlt">secular</span> evolution of migrating planet pairs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Michtchenko, T. A.; Rodríguez, A.</p> <p>2011-08-01</p> <p>The subject of this paper is the <span class="hlt">secular</span> behaviour of a pair of planets evolving under dissipative forces. In particular, we investigate the case when dissipative forces affect the planetary semimajor axes and the planets move inwards/outwards the central star, in a process known as planet migration. To perform this investigation, we introduce fundamental concepts of conservative and dissipative dynamics of the three-body problem. Based on these concepts, we develop a qualitative model of the <span class="hlt">secular</span> evolution of the migrating planetary pair. Our approach is based on the analysis of the energy and the orbital angular momentum exchange between the two-planet system and an external medium; thus no specific kind of dissipative forces is invoked. We show that, under the assumption that dissipation is weak and slow, the evolutionary routes of the migrating planets are traced by the Mode I and Mode II stationary solutions of the conservative <span class="hlt">secular</span> problem. The ultimate convergence and the evolution of the system along one of these <span class="hlt">secular</span> modes of motion are determined uniquely by the condition that the dissipation rate is sufficiently smaller than the proper <span class="hlt">secular</span> frequency of the system. We show that it is possible to reassemble the starting configurations and the migration history of the systems on the basis of their final states and consequently to constrain the parameters of the physical processes involved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFMSA21A0284K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFMSA21A0284K"><span>Study of Proton cutoffs during <span class="hlt">geomagnetically</span> disturbed times</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kanekal, S. G.; Looper, M. D.; Baker, D. N.; Blake, J. B.</p> <p>2005-12-01</p> <p>It is currently believed that solar energetic particles (SEP) may be accelerated at solar flares and/or at interplanetary shocks driven by coronal mass ejections (CMEs). CMEs also cause intense <span class="hlt">geomagnetic</span> storms during which the <span class="hlt">geomagnetic</span> field can be highly distorted.SEP fluxes penetrate the terrestrial magnetosphere and reach specific regions depending upon the <span class="hlt">geomagnetic</span> field configuration. The cutoff latitude is a well defined latitude below which a charged particle of a given rigidity (momentum per unit charge) arriving from a given direction cannot penetrate. SEP cutoff location can therefore be potentially useful in determining the <span class="hlt">geomagnetic</span> field configuration. This paper reports on the measurements of solar energetic proton cutoffs made by two satellites, SAMPEX and Polar during <span class="hlt">geomagnetically</span> disturbed times. We study select SEP events and compare our measurements with cutoffs calculated by a charged particle tracing code which utilizes several currently used models of the <span class="hlt">geomagnetic</span> field. The measured SEP proton cutoffs cover a wide range of rigidities and are obtained at high-altitudes by the HIST detector onboard Polar and at low-altitudes by the PET detctor onboard SAMPEX.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28483361','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28483361"><span><span class="hlt">Secular</span> trends in growth.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fudvoye, Julie; Parent, Anne-Simone</p> <p>2017-06-01</p> <p>Human adult height has been increasing world-wide for a century and a half. The rate of increase depends on time and place of measurement. Final height appears to have reached a plateau in Northern European countries but it is still increasing in southern European countries as well as Japan. While mean birth length has not changed recently in industrialized countries, the <span class="hlt">secular</span> trend finally observed in adult height mostly originates during the first 2 years of life. <span class="hlt">Secular</span> trend in growth is a marker of public health and provides insights into the interaction between growth and environment. It has been shown to be affected by income, social status, infections and nutrition. While genetic factors cannot explain such rapid changes in average population height, epigenetic factors could be the link between growth and environment. Copyright © 2017. Published by Elsevier Masson SAS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGeod..91..613J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGeod..91..613J"><span>Positive and negative ionospheric responses to the March 2015 <span class="hlt">geomagnetic</span> storm from BDS observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jin, Shuanggen; Jin, Rui; Kutoglu, H.</p> <p>2017-06-01</p> <p>The most intense <span class="hlt">geomagnetic</span> storm in solar cycle 24 occurred on March 17, 2015, and the detailed ionospheric storm morphologies are difficultly obtained from traditional observations. In this paper, the Geostationary Earth Orbit (GEO) observations of BeiDou Navigation Satellite System (BDS) are for the first time used to investigate the ionospheric responses to the <span class="hlt">geomagnetic</span> storm. Using BDS GEO and GIMs TEC series, negative and positive responses to the March 2015 storm are found at local and global scales. During the main phase, positive ionospheric storm is the main response to the <span class="hlt">geomagnetic</span> storm, while in the recovery phase, negative phases are pronounced at all latitudes. Maximum amplitudes of negative and positive phases appear in the afternoon and post-dusk sectors during both main and recovery phases. Furthermore, dual-peak positive phases in main phase and repeated negative phase during the recovery are found from BDS GEO observations. The <span class="hlt">geomagnetic</span> latitudes corresponding to the maximum disturbances during the main and recovery phases show large differences, but they are quasi-symmetrical between southern and northern hemispheres. No clear zonal propagation of traveling ionospheric disturbances is detected in the GNSS TEC disturbances at high and low latitudes. The thermospheric composition <span class="hlt">variations</span> could be the dominant source of the observed ionospheric storm effect from GUVI [O]/[N2] ratio data as well as storm-time electric fields. Our study demonstrates that the BDS (especially the GEO) observations are an important data source to observe ionospheric responses to the <span class="hlt">geomagnetic</span> storm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=hre&pg=3&id=EJ979083','ERIC'); return false;" href="https://eric.ed.gov/?q=hre&pg=3&id=EJ979083"><span>Human Rights Education and the Post <span class="hlt">Secular</span> Turn</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>Bowie, Bob</p> <p>2012-01-01</p> <p>This article questions whether human rights education (HRE) scholarship is responding adequately to the post <span class="hlt">secular</span> turn in thinking about the place and nature of religion in society. Here the post <span class="hlt">secular</span> turn is used to describe the discrediting of secularisation theory, the recognition of religion as an enduring and pervasive global cultural…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27094916','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27094916"><span>Artificial reproduction of magnetic fields produced by a natural <span class="hlt">geomagnetic</span> storm increases systolic blood pressure in rats.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martínez-Bretón, J L; Mendoza, B; Miranda-Anaya, M; Durán, P; Flores-Chávez, P L</p> <p>2016-11-01</p> <p>The incidence of <span class="hlt">geomagnetic</span> storms may be associated with changes in circulatory physiology. The way in which the natural <span class="hlt">variations</span> of the <span class="hlt">geomagnetic</span> field due to solar activity affects the blood pressure are poorly understood and require further study in controlled experimental designs in animal models. In the present study, we tested whether the systolic arterial pressure (AP) in adult rats is affected by simulated magnetic fields resembling the natural changes of a <span class="hlt">geomagnetic</span> storm. We exposed adult rats to a linear magnetic profile that simulates the average changes associated to some well-known <span class="hlt">geomagnetic</span> storm phases: the sudden commencement and principal phase. Magnetic stimulus was provided by a coil inductor and regulated by a microcontroller. The experiments were conducted in the electromagnetically isolated environment of a semi-anechoic chamber. After exposure, AP was determined with a non-invasive method through the pulse on the rat's tail. Animals were used as their own control. Our results indicate that there was no statistically significant effect in AP when the artificial profile was applied, neither in the sudden commencement nor in the principal phases. However, during the experimental period, a natural <span class="hlt">geomagnetic</span> storm occurred, and we did observe statistically significant AP increase during the sudden commencement phase. Furthermore, when this storm phase was artificially replicated with a non-linear profile, we noticed a 7 to 9 % increase of the rats' AP in relation to a reference value. We suggested that the changes in the <span class="hlt">geomagnetic</span> field associated with a <span class="hlt">geomagnetic</span> storm in its first day could produce a measurable and reproducible physiological response in AP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E3353T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E3353T"><span>Major <span class="hlt">geomagnetic</span> storm due to solar activity (2006-2013).</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tiwari, Bhupendra Kumar</p> <p></p> <p>Major <span class="hlt">geomagnetic</span> storm due to solar activity (2006-2013). Bhupendra Kumar Tiwari Department of Physics, A.P.S.University, Rewa(M.P.) Email: - btiwtari70@yahoo.com mobile 09424981974 Abstract- The geospace environment is dominated by disturbances created by the sun, it is observed that coronal mass ejection (CME) and solar flare events are the causal link to solar activity that produces <span class="hlt">geomagnetic</span> storm (GMS).CMEs are large scale magneto-plasma structures that erupt from the sun and propagate through the interplanetary medium with speeds ranging from only a few km/s to as large as 4000 km/s. When the interplanetary magnetic field associated with CMEs impinges upon the earth’s magnetosphere and reconnect occur <span class="hlt">geomagnetic</span> storm. Based on the observation from SOHO/LASCO spacecraft for solar activity and WDC for <span class="hlt">geomagnetism</span> Kyoto for <span class="hlt">geomagnetic</span> storm events are characterized by the disturbance storm time (Dst) index during the period 2006-2013. We consider here only intense <span class="hlt">geomagnetic</span> storm Dst <-100nT, are 12 during 2006-2013.<span class="hlt">Geomagnetic</span> storm with maximum Dst< -155nT occurred on Dec15, 2006 associated with halo CME with Kp-index 8+ and also verify that halo CME is the main cause to produce large <span class="hlt">geomagnetic</span> storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001RaSc...36..671J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001RaSc...36..671J"><span>Using <span class="hlt">geomagnetic</span> birefringence to locate sources of impulsive, terrestrial VHF signals detected by satellites on orbit</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jacobson, Abram R.; Shao, Xuan-Min</p> <p>2001-07-01</p> <p>The Earth's ionosphere is magnetized by the <span class="hlt">geomagnetic</span> field and imposes birefringent modulation on VHF radio signals propagating through the ionosphere. Satellites viewing VHF emissions from terrestrial sources receive ordinary and extraordinary modes successively from each broadband pulse emitted by the source. The birefringent intermode frequency separation can be used to determine the value of ƒce cos β, where ƒce is the electron gyrofrequency and β is the angle between the wave vector k and the <span class="hlt">geomagnetic</span> field B at the point where the VHF ray path intersects the ionosphere. Successive receptions of multiple signals (from the same source) cause <span class="hlt">variation</span> in ƒce cos β, and from the resulting <span class="hlt">variation</span> in the signal intermode frequency separation the source location on Earth can be inferred. We test the method with signals emitted by the Los Alamos Portable Pulser and received by the FORTE satellite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28527477','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28527477"><span><span class="hlt">Secular</span> Trends in Anthropometrics and Physical Fitness of Young Portuguese School-Aged Children.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Costa, Aldo Matos; Costa, Mário Jorge; Reis, António Antunes; Ferreira, Sandra; Martins, Júlio; Pereira, Ana</p> <p>2017-02-27</p> <p>The purpose of this study was to analyze <span class="hlt">secular</span> trends in anthropometrics and physical fitness of Portuguese children. A group of 1819 students (881 boys and 938 girls) between 10 and 11 years old was assessed in their 5th and 6th scholar grade throughout a 20 years' time-frame. ANCOVA models were used to analyze <span class="hlt">variations</span> in anthropometrics (height, weight and body mass index) and physical fitness (sit and reach, curl-up, horizontal jump and sprint time) across four quinquennials (1993 - 1998; 1998 - 2003; 2003 - 2008; 2008 - 2013). <span class="hlt">Secular</span> trends showed the presence of heavier boys and girls with higher body mass index in the 5th and 6th grade throughout the last 20 years. There was also a presence of taller girls but just until the 3rd quinquennial. Both boys and girls were able to perform better on the core strength test and sprint time but become less flexible over the years. Mean jumping performance remained unchanged for both genders. The present study provides novel data on anthropometrics and physical fitness trends over the last two decades in young Portuguese children, consistent with the results reported in other developed countries. Evidence for the start of a positive <span class="hlt">secular</span> trend in body mass index and in some physical fitness components over the last two decades among the Portuguese youth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI32A..02D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI32A..02D"><span><span class="hlt">Geomagnetic</span> spikes on the core-mantle boundary</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davies, C. J.; Constable, C.</p> <p>2017-12-01</p> <p>Extreme <span class="hlt">variations</span> of Earth's magnetic field occurred in the Levantine region around 1000 BC, where the field intensity rose and fell by a factor of 2-3 over a short time and confined spatial region. There is presently no coherent link between this intensity spike and the generating processes in Earth's liquid core. Here we test the attribution of a surface spike to a flux patch visible on the core-mantle boundary (CMB), calculating geometric and energetic bounds on resulting surface <span class="hlt">geomagnetic</span> features. We show that the Levantine intensity high must span at least 60 degrees in longitude. Models providing the best trade-off between matching surface spike intensity, minimizing L1 and L2 misfit to the available data and satisfying core energy constraints produce CMB spikes 8-22 degrees wide with peak values of O(100) mT. We propose that the Levantine spike grew in place before migrating northward and westward, contributing to the growth of the axial dipole field seen in Holocene field models. Estimates of Ohmic dissipation suggest that diffusive processes, which are often neglected, likely govern the ultimate decay of <span class="hlt">geomagnetic</span> spikes. Using these results, we search for the presence of spike-like features in geodynamo simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMSM53B..06H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMSM53B..06H"><span>Estimation of cold plasma outflow during <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haaland, S.; Eriksson, A. I.; Andre, M.; Maes, L.; Baddeley, L. J.; Barakat, A. R.; Chappell, C. R.; Eccles, V.; Johnsen, C.; Lybekk, B.; Li, K.; Pedersen, A.; Schunk, R. W.; Welling, D. T.</p> <p>2015-12-01</p> <p>Low energy ions of ionospheric origin provide a significant contributon to the magnetospheric plasmapopulation. Measuring cold ions is difficult though. Observations have to be done at sufficiently high altitudes and typically in regions of space where spacecraft attain a positive charge due to solar illumination. Cold ions are therefore shielded from the satellite particle detectors. Furthermore, spacecraft can only cover key regions of ion outflow during segments of their orbit, so additional complications arise arise if continuous longtime observations such as the during a <span class="hlt">geomagnetic</span> storms are needed. In this paper we suggest a new approach, based on a combination of synoptic observations and a novel technique to estimate the flux and total outflow during the various phases of <span class="hlt">geomagnetic</span> storms. Our results indicate large <span class="hlt">variations</span> in both outflow rates and transport throughout the storm. Prior to the storm main phase, outflow rates are moderate, and the cold ions are mainly emanating from moderately sized polar cap regions. Throughout the main phase of the storm, outflow rates increase and the polar cap source regions expand. Furthermore, faster transport, resulting from enhanced convection, leads to a much larger supply of cold ions to the near Earth region during gemagnetic storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4432418-observations-narrow-microburst-trains-geomagnetic-storm-august','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4432418-observations-narrow-microburst-trains-geomagnetic-storm-august"><span>Observations of narrow microburst trains in the <span class="hlt">geomagnetic</span> storm of August 4-6, 1972</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, R.R.</p> <p>1973-04-01</p> <p>In the intense <span class="hlt">geomagnetic</span> disturbances of early August 1972, auroral zone microburst trains were observed at balloon altitude and found to be significantly narrower in burst width and spacing than microbursts found previously at the same site. These observations suggest that the spacing of microburst peaks, as well as their width, is related to <span class="hlt">variations</span> in the power spectrum of a magnetospheric acceleration process rather than the bounce motions of electrons in the <span class="hlt">geomagnetic</span> field or the modulation of electron precipitation by drift waves in magnetospheric plasma. In the <span class="hlt">geomagnetic</span> activity that followed the solar flares in early August 1972,more » intense fluxes of auroral x rays were encountered during balloon flights launched from College, Alaska. Although much of the time <span class="hlt">variations</span> of the x-ray fluxes observed during these flights represented known features of electron precipitation at auroral latitudes, one new and distinct feature was evident. In particular, it was found that the widths and spacings of auroral zone microbursts (Anderson and Milton, 1964) on this occasion were significantly smaller than those observed previously on many balloon flights from the same site. Thus, instead of microburst trains with widths at half-intensity points of ~0.2 sec and spacings of ~0.6 sec, the majority of the microbursts encountered on two flights from College had widths of ~0.1 sec and spacings of ~0.4 sec. (auth)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.8339F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.8339F"><span>Progress of <span class="hlt">Geomagnetism</span> towards integration of data and services in EPOS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Flower, Simon; Hejda, Pavel; Chambodut, Aude; Curto, Juan-Jose; Matzka, Jürgen; Thomson, Alan; Korja, Toivo; Rasmussen, Thorkild; Smirnov, Maxim; Viljanen, Ari; Kauristie, Kirsti</p> <p>2017-04-01</p> <p>The <span class="hlt">geomagnetism</span> community is involved in the European Plate Observing System (EPOS), a European Research Infrastructure through which science communities will offer a number of services that will integrate to simplify cross-disciplinary research. The <span class="hlt">Geomagnetism</span> community will provide data from <span class="hlt">geomagnetic</span> observatories, from producers of <span class="hlt">geomagnetic</span> indices and events, from <span class="hlt">geomagnetic</span> models and from magneto-telluric observations. A number of these services (data from the INTERMAGNET network and the World Data Centre, indices and events from the International Service of <span class="hlt">Geomagnetic</span> Indices and the access to the International <span class="hlt">Geomagnetic</span> Reference Field and World Magnetic Model) will be integrated into EPOS systems in the first wave of services to be connected. This poster will describe the contribution from <span class="hlt">geomagnetism</span> to EPOS. It will include a description of the data and services that the <span class="hlt">geomagnetic</span> community will provide and also discuss how metadata will be made available from the community to the EPOS core IT systems. Finally it will describe how the provision of <span class="hlt">geomagnetic</span> services in EPOS will be guided and governed by members of the community .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.3130U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.3130U"><span><span class="hlt">Geomagnetic</span> Storm Impact On GPS Code Positioning</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uray, Fırat; Varlık, Abdullah; Kalaycı, İbrahim; Öǧütcü, Sermet</p> <p>2017-04-01</p> <p>This paper deals with the <span class="hlt">geomagnetic</span> storm impact on GPS code processing with using GIPSY/OASIS research software. 12 IGS stations in mid-latitude were chosen to conduct the experiment. These IGS stations were classified as non-cross correlation receiver reporting P1 and P2 (NONCC-P1P2), non-cross correlation receiver reporting C1 and P2 (NONCC-C1P2) and cross-correlation (CC-C1P2) receiver. In order to keep the code processing consistency between the classified receivers, only P2 code observations from the GPS satellites were processed. Four extreme <span class="hlt">geomagnetic</span> storms October 2003, day of the year (DOY), 29, 30 Halloween Storm, November 2003, DOY 20, November 2004, DOY 08 and four <span class="hlt">geomagnetic</span> quiet days in 2005 (DOY 92, 98, 99, 100) were chosen for this study. 24-hour rinex data of the IGS stations were processed epoch-by-epoch basis. In this way, receiver clock and Earth Centered Earth Fixed (ECEF) Cartesian Coordinates were solved for a per-epoch basis for each day. IGS combined broadcast ephemeris file (brdc) were used to partly compensate the ionospheric effect on the P2 code observations. There is no tropospheric model was used for the processing. Jet Propulsion Laboratory Application Technology Satellites (JPL ATS) computed coordinates of the stations were taken as true coordinates. The differences of the computed ECEF coordinates and assumed true coordinates were resolved to topocentric coordinates (north, east, up). Root mean square (RMS) errors for each component were calculated for each day. The results show that two-dimensional and vertical accuracy decreases significantly during the <span class="hlt">geomagnetic</span> storm days comparing with the <span class="hlt">geomagnetic</span> quiet days. It is observed that vertical accuracy is much more affected than the horizontal accuracy by <span class="hlt">geomagnetic</span> storm. Up to 50 meters error in vertical component has been observed in <span class="hlt">geomagnetic</span> storm day. It is also observed that performance of Klobuchar ionospheric correction parameters during <span class="hlt">geomagnetic</span> storm</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH21A2627I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH21A2627I"><span>Regional 3-D Modeling of Ground Geoelectric Field for the Northeast United States due to Realistic <span class="hlt">Geomagnetic</span> Disturbances</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ivannikova, E.; Kruglyakov, M.; Kuvshinov, A. V.; Rastaetter, L.; Pulkkinen, A. A.; Ngwira, C. M.</p> <p>2017-12-01</p> <p>During extreme space weather events electric currents in the Earth's magnetosphere and ionosphere experience large <span class="hlt">variations</span>, which leads to dramatic intensification of the fluctuating magnetic field at the surface of the Earth. According to Faraday's law of induction, the fluctuating <span class="hlt">geomagnetic</span> field in turn induces electric field that generates harmful currents (so-called "<span class="hlt">geomagnetically</span> induced currents"; GICs) in grounded technological systems. Understanding (via modeling) of the spatio-temporal evolution of the geoelectric field during enhanced <span class="hlt">geomagnetic</span> activity is a key consideration in estimating the hazard to technological systems from space weather. We present the results of ground geoelectric field modeling for the Northeast United States, which is performed with the use of our novel numerical tool based on integral equation approach. The tool exploits realistic regional three-dimensional (3-D) models of the Earth's electrical conductivity and realistic global models of the spatio-temporal evolution of the magnetospheric and ionospheric current systems responsible for <span class="hlt">geomagnetic</span> disturbances. We also explore in detail the manifestation of the coastal effect (anomalous intensification of the geoelectric field near the coasts) in this region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI32A..03S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI32A..03S"><span>Large short-term deviations from dipolar field during the Levantine Iron Age <span class="hlt">Geomagnetic</span> Anomaly ca. 1050-700 BCE</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shaar, R.; Tauxe, L.; Ebert, Y.</p> <p>2017-12-01</p> <p>Continuous decadal-resolution paleomagnetic data from archaeological and sedimentary sources in the Levant revealed the existence a local high-field anomaly, which spanned the first 350 years of the first millennium BCE. This so-called "the Levantine Iron Age <span class="hlt">geomagnetic</span> Anomaly" (LIAA) was characterized by a high averaged <span class="hlt">geomagnetic</span> field (virtual axial dipole moments, VADM > 140 Z Am2, nearly twice of today's field), short decadal-scale <span class="hlt">geomagnetic</span> spikes (VADM of 160-185 Z Am2), fast directional and intensity <span class="hlt">variations</span>, and substantial deviation (20°-25°) from dipole field direction. Similar high field values in the time frame of LIAA have been observed north, and northeast to the Levant: Eastern Anatolia, Turkmenistan, and Georgia. West of the Levant, in the Balkans, field values in the same time are moderate to low. The overall data suggest that the LIAA is a manifestation of a local positive <span class="hlt">geomagnetic</span> field anomaly similar in magnitude and scale to the presently active negative South Atlantic Anomaly. In this presentation we review the overall archaeomagnetic and sedimentary evidences supporting the local anomaly hypothesis, and compare these observations with today's IGRF field. We analyze the global data during the first two millennia BCE, which suggest some unexpected large deviations from a simple dipolar <span class="hlt">geomagnetic</span> structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=religious+AND+belief&pg=5&id=EJ979082','ERIC'); return false;" href="https://eric.ed.gov/?q=religious+AND+belief&pg=5&id=EJ979082"><span>Faith and Reason in a Post <span class="hlt">Secular</span> Age</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>Radford, Mike</p> <p>2012-01-01</p> <p>The problems that this article seeks to address are those that are raised in the context of the bilateralism that is established when we think in terms of <span class="hlt">secularism</span> as primarily orientated towards reason and post <span class="hlt">secularism</span>, towards faith. The objective of the article is to show that the distinction between the two can be collapsed. Post…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Department+AND+War&pg=5&id=EJ930710','ERIC'); return false;" href="https://eric.ed.gov/?q=Department+AND+War&pg=5&id=EJ930710"><span>Unholy Trinity? <span class="hlt">Secularism</span> Institute Renews Liberal Arts Curriculum</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>Keysar, Ariela</p> <p>2010-01-01</p> <p><span class="hlt">Secularism</span> is controversial in today's political debates, championed by some and vilified by others. So when Trinity College in Hartford, Conn., opened a center for the study of <span class="hlt">secularism</span> in September 2005, some people worried that it could become a source of friction on campus--yet another battleground in the culture wars that are wreaking havoc…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUSMGP51A..03G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUSMGP51A..03G"><span>Paleosecular Type Curves for South America Based on Holocene-Pleistocene Lake Sediments Studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gogorza, C. S.</p> <p>2007-05-01</p> <p>Most of the high-resolution paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> (PSV) results were obtained from records on sediments from the Northern Hemisphere. Experimental results from South America are scarce. The first results were obtained by Creer et al. (1983) and have been continued since few years ago by the author and collaborators. This review deals with studies of PSV records from bottom sediments from three lakes: Escondido, Moreno and El Trébol (south-western Argentina, 41° S, 71° 30'W). Measurements of directions (declination D and inclination I) and intensity of natural remanent magnetization (NRM), magnetic susceptibility at low and high frequency (specific, X and volumetric, k), isothermal remanent magnetization (IRM), saturation isothermal remanent magnetization (SIRM), and back field were carried out. Stability of the NRM was investigated by alternating-field demagnetization. Rock magnetic studies suggest that the main carriers of magnetization are ferrimagnetic minerals, predominantly pseudo single domain magnetite. The correlation between cores was based on magnetic parameters as X and NRM. The tephra layers were identified from the lithologic profiles and also from the magnetic susceptibility logs. Due to their different chronological meaning and their rather bad behavior as magnetic recorder, these layers were removed from the sequence and the gaps that were produced along the profiles by the removal were closed, obtaining a "shortened depth". Radiocarbon age estimates from these cores and from earlier studies allow us to construct paleosecular <span class="hlt">variation</span> records for the past 22,000 years. Inclination and declination curves (Gogorza et al., 2000a; Gogorza et al., 2002; Irurzun et al., 2006) show trends that are similar to a paleomagnetic <span class="hlt">secular</span> <span class="hlt">variation</span> curve for SW of Argentina (Gogorza et al., 2000b). References Creer, K.M., Tucholka, P. and Barton, C.E. 1983. Paleomagnetism of lake sediments, in <span class="hlt">Geomagnetism</span> of Baked Clays and Recent Sediments, edited</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://pubs.er.usgs.gov/publication/70045158','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70045158"><span>Sunspot random walk and 22-year <span class="hlt">variation</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>Love, Jeffrey J.; Rigler, E. Joshua</p> <p>2012-01-01</p> <p>We examine two stochastic models for consistency with observed long-term <span class="hlt">secular</span> trends in sunspot number and a faint, but semi-persistent, 22-yr signal: (1) a null hypothesis, a simple one-parameter random-walk model of sunspot-number cycle-to-cycle change, and, (2) an alternative hypothesis, a two-parameter random-walk model with an imposed 22-yr alternating amplitude. The observed <span class="hlt">secular</span> trend in sunspots, seen from solar cycle 5 to 23, would not be an unlikely result of the accumulation of multiple random-walk steps. Statistical tests show that a 22-yr signal can be resolved in historical sunspot data; that is, the probability is low that it would be realized from random data. On the other hand, the 22-yr signal has a small amplitude compared to random <span class="hlt">variation</span>, and so it has a relatively small effect on sunspot predictions. Many published predictions for cycle 24 sunspots fall within the dispersion of previous cycle-to-cycle sunspot differences. The probability is low that the Sun will, with the accumulation of random steps over the next few cycles, walk down to a Dalton-like minimum. Our models support published interpretations of sunspot <span class="hlt">secular</span> <span class="hlt">variation</span> and 22-yr <span class="hlt">variation</span> resulting from cycle-to-cycle accumulation of dynamo-generated magnetic energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810061837&hterms=sputnik&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsputnik','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810061837&hterms=sputnik&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsputnik"><span>Magnetic space-based field measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Langel, R. A.</p> <p>1981-01-01</p> <p>Satellite measurements of the <span class="hlt">geomagnetic</span> field began with the launch of Sputnik 3 in May 1958 and have continued sporadically in the intervening years. A list of spacecraft that have made significant contributions to an understanding of the near-earth <span class="hlt">geomagnetic</span> field is presented. A new era in near-earth magnetic field measurements began with NASA's launch of Magsat in October 1979. Attention is given to <span class="hlt">geomagnetic</span> field modeling, crustal magnetic anomaly studies, and investigations of the inner earth. It is concluded that satellite-based magnetic field measurements make global surveys practical for both field modeling and for the mapping of large-scale crustal anomalies. They are the only practical method of accurately modeling the global <span class="hlt">secular</span> <span class="hlt">variation</span>. Magsat is providing a significant contribution, both because of the timeliness of the survey and because its vector measurement capability represents an advance in the technology of such measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3202908','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3202908"><span><span class="hlt">Secular</span> trends and smoke-free policy development in rural Kentucky</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Fallin, Amanda; Parker, Lindsay; Lindgreen, Janine; Riker, Carol; Kercsmar, Sarah; Hahn, Ellen J.</p> <p>2011-01-01</p> <p>Secondhand smoke (SHS) exposure causes cardiovascular disease, lung cancer and pulmonary disorders. Smoke-free policies are the most effective way to prevent exposure to SHS. A 5-year community-based randomized control trial (RCT) is in progress to assess factors associated with smoke-free policy development in rural communities. Considering <span class="hlt">secular</span> trends is critical when conducting community-based RCTs as they may threaten the internal validity of the study. For the purposes of this paper, <span class="hlt">secular</span> trends are defined as patterns or recurring events that are not directly related to smoke-free policy but have the potential to influence policy development. There are no established protocols to monitor <span class="hlt">secular</span> trends in the study of smoke-free policy in rural communities. The purpose of this paper is to (i) describe the development of a protocol to identify and monitor <span class="hlt">secular</span> trends that may threaten the internal validity of a community-based RCT to promote smoke-free policy development and (ii) describe <span class="hlt">secular</span> trends identified in the first 2 years of the RCT. The sample includes 854 <span class="hlt">secular</span> events captured from media outlets covering the 40 study counties over the first 2 years of the RCT. Of these 854 events, there were 281 <span class="hlt">secular</span> events in Year 1 and 573 in Year 2. This paper focuses on five specific categories: ‘tobacco use and cessation activities’, ‘farming’, ‘economics’, ‘city/county infrastructure’ and ‘wellness’. This protocol is a feasible yet time-intensive method of identifying events that may threaten the internal validity of a community-based RCT. PMID:21558440</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910047153&hterms=ethane&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dethane','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910047153&hterms=ethane&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dethane"><span>Seasonal cycle and <span class="hlt">secular</span> trend of the total and tropospheric column abundance of ethane above the Jungfraujoch</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ehhalt, D. H.; Schmidt, U.; Zander, R.; Demoulin, P.; Rinsland, C. P.</p> <p>1991-01-01</p> <p>The <span class="hlt">secular</span> trend and the seasonal cycle of the total and the tropospheric column abundances of C2H6 over the Jungfraujoch Station (Switzerland) were deduced from infrared solar spectra recorded in 1951 and from 1984 to 1988. Results show a definite seasonal <span class="hlt">variation</span> in the total vertical column abundance of C2H6, with a maximum of (1.43 + or - 0.03) x 10 to the 16th molecules/sq cm during March and April and a minimum in the fall; the ratio between the maximum and the minimum column abundances was found to be 1.62 + or - 0.11. The <span class="hlt">secular</span> trend in the tropospheric burden above the Jungfraujoch was found to be (0.85 + or - 0.3) percent/yr.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/1016435','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/1016435"><span>Are migrating raptors guided by a <span class="hlt">geomagnetic</span> compass?</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Thorup, Kasper; Fuller, Mark R.; Alerstam, T.; Hake, M.; Kjellen, N.; Standberg, R.</p> <p>2006-01-01</p> <p>We tested whether routes of raptors migrating over areas with homogeneous topography follow constant <span class="hlt">geomagnetic</span> courses more or less closely than constant geographical courses. We analysed the routes taken over land of 45 individual raptors tracked by satellite-based radiotelemetry: 25 peregrine falcons, Falco peregrinus, on autumn migration between North and South America, and seven honey buzzards, Pernis apivorus, and 13 ospreys, Pandion haliaetus, on autumn migration between Europe and Africa. Overall, migration directions showed a better agreement with constant geographical than constant <span class="hlt">geomagnetic</span> courses. Tracks deviated significantly from constant <span class="hlt">geomagnetic</span> courses, but were not significantly different from geographical courses. After we removed movements directed far from the mean direction, which may not be migratory movements, migration directions still showed a better agreement with constant geographical than constant <span class="hlt">geomagnetic</span> courses, but the directions of honey buzzards and ospreys were not significantly different from constant <span class="hlt">geomagnetic</span> courses either. That migration routes of raptors followed by satellite telemetry are in closer accordance with constant geographical compass courses than with constant <span class="hlt">geomagnetic</span> compass courses may indicate that geographical (e.g. based on celestial cues) rather than magnetic compass mechanisms are of dominating importance for the birds' long-distance orientation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoJI.207..228W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoJI.207..228W"><span>Decadal variability in core surface flows deduced from <span class="hlt">geomagnetic</span> observatory monthly means</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Whaler, K. A.; Olsen, N.; Finlay, C. C.</p> <p>2016-10-01</p> <p>Monthly means of the magnetic field measurements at ground observatories are a key data source for studying temporal changes of the core magnetic field. However, when they are calculated in the usual way, contributions of external (magnetospheric and ionospheric) origin may remain, which make them less favourable for studying the field generated by dynamo action in the core. We remove external field predictions, including a new way of characterizing the magnetospheric ring current, from the data and then calculate revised monthly means using robust methods. The <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variation</span> (SV) is calculated as the first annual differences of these monthly means, which also removes the static crustal field. SV time-series based on revised monthly means are much less scattered than those calculated from ordinary monthly means, and their variances and correlations between components are smaller. On the annual to decadal timescale, the SV is generated primarily by advection in the fluid outer core. We demonstrate the utility of the revised monthly means by calculating models of the core surface advective flow between 1997 and 2013 directly from the SV data. One set of models assumes flow that is constant over three months; such models exhibit large and rapid temporal <span class="hlt">variations</span>. For models of this type, less complex flows achieve the same fit to the SV derived from revised monthly means than those from ordinary monthly means. However, those obtained from ordinary monthly means are able to follow excursions in SV that are likely to be external field contamination rather than core signals. Having established that we can find models that fit the data adequately, we then assess how much temporal variability is required. Previous studies have suggested that the flow is consistent with torsional oscillations (TO), solid body-like oscillations of fluid on concentric cylinders with axes aligned along the Earth's rotation axis. TO have been proposed to explain decadal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820018881','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820018881"><span>Comparison of storm-time changes of <span class="hlt">geomagnetic</span> field at ground and MAGSAT altitudes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dejesusparada, N. (Principal Investigator); Kane, R. P.; Trivedi, N. B.</p> <p>1982-01-01</p> <p>The MAGSAT data for the period Nov. 2-20, 1979 were studied. From the observed H, the HMD predicted by model was subtracted. The residue delta H = H-HMD shows storm-time <span class="hlt">variations</span> similar to <span class="hlt">geomagnetic</span> Dst, at least qualitatively. Delta H sub 0, i.e., equatorial values of delta H were studied separately for dusk and dawn and show some differences.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830007471','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830007471"><span>Data use investigation for the magnetic field satellite (MAGSAT) mission: <span class="hlt">Geomagnetic</span> field forecasting and fluid dynamics of the core</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Benton, E. R. (Principal Investigator)</p> <p>1982-01-01</p> <p>MAGSAT data were used to construct a variety of spherical harmonic models of the main <span class="hlt">geomagnetic</span> field emanating from Earth's liquid core at poch 1980. These models were used to: (1) accurately determine the radius of Earth's core by a magnetic method, (2) calculate estimates, of the long-term ange of <span class="hlt">variation</span> of <span class="hlt">geomagnetic</span> Gauss coefficients; (3) establish a preferred truncation level for current spherical harmonic models of the main <span class="hlt">geomagnetic</span> field from the core; (4) evaluate a method for taking account of electrical conduction in the mantle when the magnetic field is downward continued to the core-mantle boundary; and (5) establish that upwelling and downwelling of fluid motion at the top of the core is probably detectable, observationally. A fluid dynamics forecast model was not produced because of insufficient data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSM11B2140L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSM11B2140L"><span>Enhancement of low energy particle flux around plasmapause under quiet <span class="hlt">geomagnetic</span> condition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, J.</p> <p>2016-12-01</p> <p>Plasmapause is the boundary of the plasmaspheric region where cold plasma is dominant. In this boundary, the plasma density shows depletion to 1 10 on direction from the plasmasphere to magnetosphere and changes composition of energy distribution of particle. Some previous study provides that the location of the plasmapause expand beyond geosynchronous orbit under the quiet <span class="hlt">geomagnetic</span> conditions. In this work, we study the changed characteristic of particle flux around the plasmapause using measurement from Van Allen Probes. On 23 April 2013, the satellites observed simultaneously proton and electron fluxes enhancement with E > 100 eV. During 12 hours prior to this event, the <span class="hlt">geomagnetic</span> conditions were very quiet, Kp < 1, and <span class="hlt">geomagnetic</span> storm did not occur. This event maintain for 15 minutes and only proton flux decrease rapidly in the magnetosphere. In this period SYM-H index enhanced abruptly in response to the impact of the dynamic pressure enhancement and AE index increased gradually up to about 200 nT. Electric field started to perturb in coincidence with enhancement of particle flux from the plasmapause. To explain the <span class="hlt">variation</span> of low energy particle flux we will compare kinetic property of low energy particle by using velocity space distribution function at region of inner and outer boundary of the plasmapause.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=existential+AND+humanist&id=ED548600','ERIC'); return false;" href="https://eric.ed.gov/?q=existential+AND+humanist&id=ED548600"><span>The Jesuit Imaginary: Higher Education in a <span class="hlt">Secular</span> Age</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>Hendrickson, Daniel Scott</p> <p>2012-01-01</p> <p>The philosopher Charles Taylor argues in "A <span class="hlt">Secular</span> Age" (2007) that people who live in <span class="hlt">secular</span> cultures are losing the capacity to experience genuine "fullness." Described by Taylor as a philosophical-anthropological conception of human flourishing that corresponds with existential senses of meaning and purpose, fullness is…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010cosp...38..921K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38..921K"><span>Variability Analysis of the Horizontal <span class="hlt">Geomagnetic</span> Component: A Case Study Based on Records from Vassouras Observatory (Brazil)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klausner, Virginia; Papa, Andres; Mendes, Odim; Oliveira Domingues, Margarete</p> <p></p> <p>It is well known that any of the components of the magnetic field measured on the Earth's surface presents characteristic frequencies with 24, 12, 8 and 6-hour period. Those typical kinds of oscillations of the <span class="hlt">geomagnetic</span> field are known as solar quiet <span class="hlt">variation</span> and are primary due to the global thermotidal wind systems which conduct currents flowing in the "dynamo region" of the ionosphere, the E-region. In this study, the horizontal component amplitude observed by ground-based observatories belonged to the INTERMAGNET network have been used to analyze the global pattern variance of the Sq <span class="hlt">variation</span>. In particular we focused our attention on Vassouras Observatory (VSS), Rio de Janeiro, Brazil, which has been active since 1915. In the next years, a brazilian network of magnetometers will be implemented and VSS can be used as reference. This work aims mainly to highlight and interpret these quiet daily <span class="hlt">variations</span> over the Brazilian sector compared to the features from other magnetic stations reasonably distributed over the whole Earth's surface. The methodological approach is based on wavelet cross-correlation technique. This technique is useful to isolate the period of the spectral components of <span class="hlt">geomagnetic</span> field in each station and to correlate them as function of scale (period) between VSS and the other stations. The wavelet cross-correlation coefficient strongly depends on the scale. We study the <span class="hlt">geomagnetically</span> quiet days at equinox and solstice months during low and high solar activity. As preliminary remarks, the results show that the records in the magnetic stations have primary a latitudinal dependence affected by the time of year and level of solar activity. On the other hand, records of magnetic stations located at the same dip latitude but at different longitude presented some peculiarities. These results indicated that the winds driven the dynamo are very sensitive of the location of the <span class="hlt">geomagnetic</span> station, i. e., its effects depend upon the direction</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=attractive&pg=7&id=EJ1025939','ERIC'); return false;" href="https://eric.ed.gov/?q=attractive&pg=7&id=EJ1025939"><span>Re-Imagining a Christian University in a <span class="hlt">Secular</span> Age</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>Warner, Rob</p> <p>2013-01-01</p> <p>The contours of a <span class="hlt">secular</span> age, as delineated by classical and contemporary sociologists of religion, have tended to result in secularising trajectories for church-founded institutions of Higher Education, some of which have migrated towards <span class="hlt">secular</span> normativity. This article explores these trends and then proposes five characteristics of an…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PEPI..276..172N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PEPI..276..172N"><span>On the thermo-chemical origin of the stratified region at the top of the Earth's core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakagawa, Takashi</p> <p>2018-03-01</p> <p>I developed a combined model of the thermal and chemical evolution of the Earth's core and investigated its influence on a thermochemically stable region beneath the core-mantle boundary (CMB). The chemical effects of the growing stable region are caused by the equilibrium chemical reaction between silicate and the metallic core. The thermal effects can be characterized by the growth of the sub-isentropic shell, which may have a rapid growth rate compared to that of the chemically stable region. When the present-day CMB heat flow was varied, the origin of the stable region changed from chemical to thermochemical to purely thermal because the rapid growth of the sub-isentropic shell can replace the chemically stable region. Physically reasonable values of the present-day CMB heat flow that can maintain the geodynamo action over 4 billion years should be between 8 and 11 TW. To constrain the thickness of the thermochemically stable region beneath the CMB, the chemical diffusivity is important and should be ∼O(10-8) m2/s to obtain a thickness of the thermochemically stable region beneath the CMB consistent with that inferred from <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variations</span> (140 km). However, the strength of the stable region found in this study is too high to be consistent with the constraint on the stability of the stable region inferred from <span class="hlt">geomagnetic</span> <span class="hlt">secular</span> <span class="hlt">variations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004cosp...35.1708N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004cosp...35.1708N"><span>Possible <span class="hlt">Geomagnetic</span> and Environmental Symptoms in the Area of Athens During the Solar Cycle No 22</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nastos, P. T.; Paliatsos, A. G.; Korbakis, G. K.; Tritakis, V. P.; Bergiannaki, A.; Psarros, K.; Paparrigopoulos, P.; Stafanis, K.</p> <p></p> <p>The goal of this research is to confirm possible influences of environmental and <span class="hlt">geomagnetic</span> variability in psychiatric hygiene of sensitive and heavily psychological patients. Three yearly samples of psychological patients consisted by four thousand cases (4000) each have been studied. The patients have been filed by the psychiatric clinic of the Eginition hospital in Athens where the three samples have been compiled during three very characteristic years of the No 22 11-year cycle, the maximum (1989), the minimum (1996) and one intermediate year of the descending branch (1994). A file with five to eight psychological symptoms like depression, sleep disturbance anxiety, aggressiveness etc. is attached to every patient. Each of these symptoms is correlated to the local <span class="hlt">geomagnetic</span> index (k-index), the international <span class="hlt">geomagnetic</span> index (Dst) and the environmental index (DI, Discomfort Index) in both daily and monthly basis. A clear seasonal <span class="hlt">variation</span> in almost all symptoms and samples is present with maximum at the end of summer (August/September) and minimum at the end of winter (February-March). In addition very significant correlations among DI, Dst and some psychological symptoms appear. The main conclusion is that meteorological and <span class="hlt">geomagnetic</span> factors play a significant role in the formation of sensitive psychological patients, behavior</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PEPI..280...40G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PEPI..280...40G"><span>A continuous Late Holocene paleosecular <span class="hlt">variation</span> record from Carmen Lake (Tierra del Fuego, Argentina)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gogorza, Claudia S. G.; Irurzun, María A.; Orgeira, María J.; Palermo, Pedro; Llera, María</p> <p>2018-07-01</p> <p>Paleomagnetic <span class="hlt">secular</span> <span class="hlt">variations</span> (PSV) give us information on the mechanisms of the geodynamo and can also be used for stratigraphic correlation on a regional scale. In this article we present a high-resolution paleomagnetic and rock magnetic study of two cores, LCTF1 and LCTF2, collected at Carmen Lake (Tierra del Fuego, Argentina). An analysis of rock magnetic data suggests that the remanence signal is carried by Titanomagnetite grains in stable pseudo single domain (PSD) state. Notwithstanding the special mechanism of sedimentary deposition, the sequence is characterised by good paleomagnetic properties and can be used to reconstruct a continuous stratigraphic record that provides high-resolution declination, inclination and relative paleointensity curves for the period 1000-4000 cal years BP. The constructed PSV curves are in very good agreement with the available records of Southern Argentina, implying very promising results in the construction of curve patterns for the region. A comparison of the records of southern Argentina with the most recent models available demonstrates that there is a noticeable lack of agreement, which is interpreted as the critical need to add more data from the southern hemisphere in the construction of the <span class="hlt">geomagnetic</span> field models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4749623-space-geomagnetism-radiation-belts-auroral-zones','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4749623-space-geomagnetism-radiation-belts-auroral-zones"><span>SPACE <span class="hlt">GEOMAGNETISM</span>, RADIATION BELTS, AND AURORAL ZONES</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>Vestine, E.H.</p> <p>1962-07-01</p> <p>The nature of the <span class="hlt">geomagnetic</span> field and a few <span class="hlt">variations</span> from ground level out to about 10 earth radii is discussed. Regions of trapped radiation are noted. The unshielded dosages during a great solar event on a few days per decade exceed limits of human safety. Modest shielding of somewhat less than 1 gm/sq cm will not remove the hazards. The chance is probably only one in several thousand that this will not suffice to preserve life on any given day. Transient accelerations of trapped particles result in atmospheric effects such as the aurora, and the polar electrojets, but themore » cause of these accelerative actions is quite obscure. (auth)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70019868','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70019868"><span>Scaling laws from <span class="hlt">geomagnetic</span> time series</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Voros, Z.; Kovacs, P.; Juhasz, A.; Kormendi, A.; Green, A.W.</p> <p>1998-01-01</p> <p>The notion of extended self-similarity (ESS) is applied here for the X - component time series of <span class="hlt">geomagnetic</span> field fluctuations. Plotting nth order structure functions against the fourth order structure function we show that low-frequency <span class="hlt">geomagnetic</span> fluctuations up to the order n = 10 follow the same scaling laws as MHD fluctuations in solar wind, however, for higher frequencies (f > l/5[h]) a clear departure from the expected universality is observed for n > 6. ESS does not allow to make an unambiguous statement about the non triviality of scaling laws in "<span class="hlt">geomagnetic</span>" turbulence. However, we suggest to use higher order moments as promising diagnostic tools for mapping the contributions of various remote magnetospheric sources to local observatory data. Copyright 1998 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70197169','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70197169"><span><span class="hlt">Geomagnetic</span> paleointensities from excursion sequences in lavas on Oahu, Hawaii</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Coe, Robert S.; Gromme, Sherman; Mankinen, Edward A.</p> <p>1984-01-01</p> <p>Paleomagnetic data demonstrating three late Tertiary excursions in the direction of the <span class="hlt">geomagnetic</span> field recorded in sequences of basaltic lavas on the island of Oahu, Hawaii were published by R. R. Doell and G. B. Dalrymple in 1973. We have determined <span class="hlt">geomagnetic</span> paleointensities by the Thelliers' method for 14 lavas from the three sites. During these experiments, considerable difficulty was encountered because of the presence of titanomaghemite in many lavas and the contamination of natural remanent magnetization by lightning in many others. Moreover, we often observed the production of spurious high‐temperature chemical remanent magnetization during the Thellier experiments. An analysis of this particularly troublesome problem is presented. Two of the sites showed low paleointensities associated with angular departures of the paleomagnetic field direction from that of a geocentric axial dipole, which suggests that these excursions represent aborted reversals or fragments of reversals. At the third site, however, the paleointensity did not become low as the field diverged. This excursion may reflect the <span class="hlt">variation</span> of a large nondipole source near Hawaii.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930009997','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930009997"><span>Asteroid proper elements and <span class="hlt">secular</span> resonances</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Knezevic, Zoran; Milani, Andrea</p> <p>1992-01-01</p> <p>In a series of papers (e.g., Knezevic, 1991; Milani and Knezevic, 1990; 1991) we reported on the progress we were making in computing asteroid proper elements, both as regards their accuracy and long-term stability. Additionally, we reported on the efficiency and 'intelligence' of our software. At the same time, we studied the associated problems of resonance effects, and we introduced the new class of 'nonlinear' <span class="hlt">secular</span> resonances; we determined the locations of these <span class="hlt">secular</span> resonances in proper-element phase space and analyzed their impact on the asteroid family classification. Here we would like to summarize the current status of our work and possible further developments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993nbi..book......','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993nbi..book......"><span>The national <span class="hlt">geomagnetic</span> initiative</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></p> <p>The Earth's magnetic field, through its variability over a spectrum of spatial and temporal scales, contains fundamental information on the solid Earth and geospace environment (the latter comprising the atmosphere, ionosphere, and magnetosphere). Integrated studies of the <span class="hlt">geomagnetic</span> field have the potential to address a wide range of important processes in the deep mantle and core, asthenosphere, lithosphere, oceans, and the solar-terrestrial environment. These studies have direct applications to important societal problems, including resource assessment and exploration, natural hazard mitigation, safe navigation, and the maintenance and survivability of communications and power systems on the ground and in space. Studies of the Earth's magnetic field are supported by a variety of federal and state agencies as well as by private industry. Both basic and applied research is presently supported by several federal agencies, including the National Science Foundation (NSF), U.S. Geological Survey (USGS), U.S. Department of Energy (DOE), National Oceanic and Atmospheric Administration (NOAA), National Aeronautics and Space Administration (NASA), and U.S. Department of Defense (DOD) (through the Navy, Air Force, and Defense Mapping Agency). Although each agency has a unique, well-defined mission in <span class="hlt">geomagnetic</span> studies, many areas of interest overlap. For example, NASA, the Navy, and USGS collaborate closely in the development of main field reference models. NASA, NSF, and the Air Force collaborate in space physics. These interagency linkages need to be strengthened. Over the past decade, new opportunities for fundamental advances in <span class="hlt">geomagnetic</span> research have emerged as a result of three factors: well-posed, first-order scientific questions; increased interrelation of research activities dealing with <span class="hlt">geomagnetic</span> phenomena; and recent developments in technology. These new opportunities can be exploited through a national <span class="hlt">geomagnetic</span> initiative to define objectives and</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('http://hdl.handle.net/2060/19940018871','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940018871"><span>The national <span class="hlt">geomagnetic</span> initiative</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1993-01-01</p> <p>The Earth's magnetic field, through its variability over a spectrum of spatial and temporal scales, contains fundamental information on the solid Earth and geospace environment (the latter comprising the atmosphere, ionosphere, and magnetosphere). Integrated studies of the <span class="hlt">geomagnetic</span> field have the potential to address a wide range of important processes in the deep mantle and core, asthenosphere, lithosphere, oceans, and the solar-terrestrial environment. These studies have direct applications to important societal problems, including resource assessment and exploration, natural hazard mitigation, safe navigation, and the maintenance and survivability of communications and power systems on the ground and in space. Studies of the Earth's magnetic field are supported by a variety of federal and state agencies as well as by private industry. Both basic and applied research is presently supported by several federal agencies, including the National Science Foundation (NSF), U.S. Geological Survey (USGS), U.S. Department of Energy (DOE), National Oceanic and Atmospheric Administration (NOAA), National Aeronautics and Space Administration (NASA), and U.S. Department of Defense (DOD) (through the Navy, Air Force, and Defense Mapping Agency). Although each agency has a unique, well-defined mission in <span class="hlt">geomagnetic</span> studies, many areas of interest overlap. For example, NASA, the Navy, and USGS collaborate closely in the development of main field reference models. NASA, NSF, and the Air Force collaborate in space physics. These interagency linkages need to be strengthened. Over the past decade, new opportunities for fundamental advances in <span class="hlt">geomagnetic</span> research have emerged as a result of three factors: well-posed, first-order scientific questions; increased interrelation of research activities dealing with <span class="hlt">geomagnetic</span> phenomena; and recent developments in technology. These new opportunities can be exploited through a national <span class="hlt">geomagnetic</span> initiative to define objectives and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4497462','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4497462"><span>Ionospheric redistribution during <span class="hlt">geomagnetic</span> storms</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Immel, T J; Mannucci, A J</p> <p>2013-01-01</p> <p>[1]The abundance of plasma in the daytime ionosphere is often seen to grow greatly during <span class="hlt">geomagnetic</span> storms. Recent reports suggest that the magnitude of the plasma density enhancement depends on the UT of storm onset. This possibility is investigated over a 7year period using global maps of ionospheric total electron content (TEC) produced at the Jet Propulsion Laboratory. The analysis confirms that the American sector exhibits, on average, larger storm time enhancement in ionospheric plasma content, up to 50% in the afternoon middle-latitude region and 30% in the vicinity of the high-latitude auroral cusp, with largest effect in the Southern Hemisphere. We investigate whether this effect is related to the magnitude of the causative magnetic storms. Using the same advanced Dst index employed to sort the TEC maps into quiet and active (Dst<−100 nT) sets, we find <span class="hlt">variation</span> in storm strength that corresponds closely to the TEC <span class="hlt">variation</span> but follows it by 3–6h. For this and other reasons detailed in this report, we conclude that the UT-dependent peak in storm time TEC is likely not related to the magnitude of external storm time forcing but more likely attributable to phenomena such as the low magnetic field in the South American region. The large Dst <span class="hlt">variation</span> suggests a possible system-level effect of the observed <span class="hlt">variation</span> in ionospheric storm response on the measured strength of the terrestrial ring current, possibly connected through UT-dependent modulation of ion outflow. PMID:26167429</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26167429','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26167429"><span>Ionospheric redistribution during <span class="hlt">geomagnetic</span> storms.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Immel, T J; Mannucci, A J</p> <p>2013-12-01</p> <p>[1]The abundance of plasma in the daytime ionosphere is often seen to grow greatly during <span class="hlt">geomagnetic</span> storms. Recent reports suggest that the magnitude of the plasma density enhancement depends on the UT of storm onset. This possibility is investigated over a 7year period using global maps of ionospheric total electron content (TEC) produced at the Jet Propulsion Laboratory. The analysis confirms that the American sector exhibits, on average, larger storm time enhancement in ionospheric plasma content, up to 50% in the afternoon middle-latitude region and 30% in the vicinity of the high-latitude auroral cusp, with largest effect in the Southern Hemisphere. We investigate whether this effect is related to the magnitude of the causative magnetic storms. Using the same advanced Dst index employed to sort the TEC maps into quiet and active ( D s t <-100 nT) sets, we find <span class="hlt">variation</span> in storm strength that corresponds closely to the TEC <span class="hlt">variation</span> but follows it by 3-6h. For this and other reasons detailed in this report, we conclude that the UT-dependent peak in storm time TEC is likely not related to the magnitude of external storm time forcing but more likely attributable to phenomena such as the low magnetic field in the South American region. The large Dst <span class="hlt">variation</span> suggests a possible system-level effect of the observed <span class="hlt">variation</span> in ionospheric storm response on the measured strength of the terrestrial ring current, possibly connected through UT-dependent modulation of ion outflow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001JASTP..63.1649S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001JASTP..63.1649S"><span><span class="hlt">Geomagnetic</span> research in the 19th century: a case study of the German contribution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schröder, W.; Wiederkehr, K.-H.</p> <p>2001-10-01</p> <p>Even before the discovery of electromagnetism by Oersted, and before the work of Ampère, who attributed all magnetism to the flux of electrical currents, A.v. Humboldt and Hansteen had turned to <span class="hlt">geomagnetism</span>. Through the ``Göttinger Magnetischer Verein'', a worldwide cooperation under the leadership of Gauss came into existence. Even today, Gauss's theory of <span class="hlt">geomagnetism</span> is one of the pillars of <span class="hlt">geomagnetic</span> research. Thereafter, J.v. Lamont, in Munich, took over the leadership in Germany. In England, the Magnetic Crusade was started by the initiative of John Herschel and E. Sabine. At the beginning of the 1840s, James Clarke Ross advanced to the vicinity of the southern magnetic pole on the Antarctic Continent, which was then quite unknown. Ten years later, Sabine was able to demonstrate solar-terrestrial relations from the data of the colonial observatories. In the 1980s, Arthur Schuster, following Balfour Stewart's ideas, succeeded in interpreting the daily <span class="hlt">variations</span> of the electrical process in the high atmosphere. <span class="hlt">Geomagnetic</span> research work in Germany was given a fresh impetus by the programme of the First Polar Year 1882-1883. Georg Neumayer, director of the ``Deutsche Seewarte'' in Hamburg, was one of the initiators of the Polar Year. He forged a close cooperation with the newly founded ``Kaiserliches Marineobservatorium'' in Wilhelmshaven, and also managed to gain the collaboration of the ``Gauss-Observatorium für Erdmagnetismus'' in Göttingen under E. Schering. In the Polar Year, the first automatic recording magnetometers (Kew-Model) were used in the German observatory at Wilhelmshaven. Here, M. Eschenhagen, who later became director of the <span class="hlt">geomagnetic</span> section in the new Meteorological Magnetic Observatory in Potsdam, deserves special credit. Early hypotheses of <span class="hlt">geomagnetism</span> and pioneering palaeomagnetic experiments are briefly reviewed. The essential seismological investigations at the turn of the 19th to the 20th century are also briefly described as</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGeod..88..839B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGeod..88..839B"><span><span class="hlt">Secular</span> changes in Earth's shape and surface mass loading derived from combinations of reprocessed global GPS networks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Booker, David; Clarke, Peter J.; Lavallée, David A.</p> <p>2014-09-01</p> <p>The changing distribution of surface mass (oceans, atmospheric pressure, continental water storage, groundwater, lakes, snow and ice) causes detectable changes in the shape of the solid Earth, on time scales ranging from hours to millennia. Transient changes in the Earth's shape can, regardless of cause, be readily separated from steady <span class="hlt">secular</span> <span class="hlt">variation</span> in surface mass loading, but other <span class="hlt">secular</span> changes due to plate tectonics and glacial isostatic adjustment (GIA) cannot. We estimate <span class="hlt">secular</span> station velocities from almost 11 years of high quality combined GPS position solutions (GPS weeks 1,000-1,570) submitted as part of the first international global navigation satellite system service reprocessing campaign. Individual station velocities are estimated as a linear fit, paying careful attention to outliers and offsets. We remove a suite of a priori GIA models, each with an associated set of plate tectonic Euler vectors estimated by us; the latter are shown to be insensitive to the a priori GIA model. From the coordinate time series residuals after removing the GIA models and corresponding plate tectonic velocities, we use mass-conserving continental basis functions to estimate surface mass loading including the <span class="hlt">secular</span> term. The different GIA models lead to significant differences in the estimates of loading in selected regions. Although our loading estimates are broadly comparable with independent estimates from other satellite missions, their range highlights the need for better, more robust GIA models that incorporate 3D Earth structure and accurately represent 3D surface displacements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/79501-month-periodicity-low-latitude-geomagnetic-field-its-connection-stratospheric-qbo','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/79501-month-periodicity-low-latitude-geomagnetic-field-its-connection-stratospheric-qbo"><span>A 27-month periodicity in the low latitude <span class="hlt">geomagnetic</span> field and its connection to the stratospheric QBO</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>Olsen, N.</p> <p>1994-06-01</p> <p><span class="hlt">Geomagnetic</span> daily <span class="hlt">variations</span> are produced at a height of about 100 to 130 km due to dynamo action of thermospheric winds in combination with the ionospheric conductivity. They are influenced by longterm variability of thermospheric dynamics and are used as tool for investigating a QBO (Quasi-Biennial-Oscillation) in thermospheric winds. Power spectrum analysis has been applied to monthly means of the daily range of the <span class="hlt">geomagnetic</span> field. In addition to an annual modulation (and subharmonics) there is clear evidence for a sharp peak at about 27 months in the H-component at low-latitude observatories (delta H approximately equal to 0.5 nT). Atmore » single observatories, statistical significance is at the 99% confidence level, squared coherency between distant observatories is highly significant, too. However, there is no global modulation of the S(sub q) current system because: (1) the D-component contain no 27-month periodicity; and (2) the oscillation is not present at mid-latitude observatories. In order to explain the observations, a 27-month oscillation in the low-latitude prevailing zonal winds with an amplitude of few m/s at a height of about 100-130 km is postulated. Squared Coherency between <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> and prevailing winds in the equatorial stratosphere is significant at the 95%-level.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720010021','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720010021"><span>Natural <span class="hlt">variations</span> in the <span class="hlt">geomagnetically</span> trapped electron population</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vampola, A. L.</p> <p>1972-01-01</p> <p>Temporal <span class="hlt">variations</span> in the trapped natural electron flux intensities and energy spectra are discussed and demonstrated using recent satellite data. These data are intended to acquaint the space systems engineer with the types of natural <span class="hlt">variations</span> that may be encountered during a mission and to augment the models of the electron environment currently being used in space system design and orbit selection. An understanding of the temporal <span class="hlt">variations</span> which may be encountered should prove helpful. Some of the <span class="hlt">variations</span> demonstrated here which are not widely known include: (1) addition of very energetic electrons to the outer zone during moderate magnetic storms: (2) addition of energetic electrons to the inner zone during major magnetic storms; (3) inversions in the outer zone electron energy spectrum during the decay phase of a storm injection event and (4) occasional formation of multiple maxima in the flux vs altitude profile of moderately energetic electrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.467...79A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.467...79A"><span>Asymmetry in growth and decay of the <span class="hlt">geomagnetic</span> dipole revealed in seafloor magnetization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Avery, Margaret S.; Gee, Jeffrey S.; Constable, Catherine G.</p> <p>2017-06-01</p> <p><span class="hlt">Geomagnetic</span> intensity fluctuations provide important constraints on time-scales associated with dynamical processes in the outer core. PADM2M is a reconstructed time series of the 0-2 Ma axial dipole moment (ADM). After smoothing to reject high frequency <span class="hlt">variations</span> PADM2M's average growth rate is larger than its decay rate. The observed asymmetry in rates of change is compatible with longer term diffusive decay of the ADM balanced by advective growth on shorter time scales, and provides a potentially useful diagnostic for evaluating numerical geodynamo simulations. We re-analyze the PADM2M record using improved low-pass filtering to identify asymmetry and quantify its uncertainty via bootstrap methods before applying the new methodology to other kinds of records. Asymmetry in distribution of axial dipole moment derivatives is quantified using the <span class="hlt">geomagnetic</span> skewness coefficient, sg. A positive value indicates the distribution has a longer positive tail and the average growth rate is greater than the average decay rate. The original asymmetry noted by Ziegler and Constable (2011) is significant and does not depend on the specifics of the analysis. A long-term record of <span class="hlt">geomagnetic</span> intensity should also be preserved in the thermoremanent magnetization of oceanic crust recovered by inversion of stacked profiles of marine magnetic anomalies. These provide an independent means of verifying the asymmetry seen in PADM2M. We examine three near-bottom surveys: a 0 to 780 ka record from the East Pacific Rise at 19°S, a 0 to 5.2 Ma record from the Pacific Antarctic Ridge at 51°S, and a chron C4Ar-C5r (9.3-11.2 Ma) record from the NE Pacific. All three records show an asymmetry similar in sense to PADM2M with <span class="hlt">geomagnetic</span> skewness coefficients, sg > 0. Results from PADM2M and C4Ar-C5r are most robust, reflecting the higher quality of these <span class="hlt">geomagnetic</span> records. Our results confirm that marine magnetic anomalies can carry a record of the asymmetric <span class="hlt">geomagnetic</span> field behavior</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001JGR...10618651J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001JGR...10618651J"><span>Period and phase comparisons of near-decadal oscillations in solar, <span class="hlt">geomagnetic</span>, and cosmic ray time series</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Juckett, David A.</p> <p>2001-09-01</p> <p>A more complete understanding of the periodic dynamics of the Sun requires continued exploration of non-11-year oscillations in addition to the benchmark 11-year sunspot cycle. In this regard, several solar, <span class="hlt">geomagnetic</span>, and cosmic ray time series were examined to identify common spectral components and their relative phase relationships. Several non-11-year oscillations were identified within the near-decadal range with periods of ~8, 10, 12, 15, 18, 22, and 29 years. To test whether these frequency components were simply low-level noise or were related to a common source, the phases were extracted for each component in each series. The phases were nearly identical across the solar and <span class="hlt">geomagnetic</span> series, while the corresponding components in four cosmic ray surrogate series exhibited inverted phases, similar to the known phase relationship with the 11-year sunspot cycle. Cluster analysis revealed that this pattern was unlikely to occur by chance. It was concluded that many non-11-year oscillations truly exist in the solar dynamical environment and that these contribute to the complex <span class="hlt">variations</span> observed in <span class="hlt">geomagnetic</span> and cosmic ray time series. Using the different energy sensitivities of the four cosmic ray surrogate series, a preliminary indication of the relative intensities of the various solar-induced oscillations was observed. It provides evidence that many of the non-11-year oscillations result from weak interplanetary magnetic field/solar wind oscillations that originate from corresponding <span class="hlt">variations</span> in the open-field regions of the Sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/50520-some-topics-historical-episodes-geomagnetism-aeronomy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/50520-some-topics-historical-episodes-geomagnetism-aeronomy"><span>Some topics and historical episodes in <span class="hlt">geomagnetism</span> and aeronomy</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>Fukushima, N.</p> <p>1994-10-01</p> <p>The author provides historical perspective on work in the area of <span class="hlt">geomagnetism</span> and aeronomy. He discusses early ideas discussed in the literature, work by Birkelund on current flows, ideas on the curl-freeness of the <span class="hlt">geomagnetic</span> fields, studies of auroral records recorded by man, studies of magnetic storms, <span class="hlt">geomagnetic</span> field measurements, and of late the wealth of satellite information of the magnetosphere and solar wind effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.484...15N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.484...15N"><span>A high-resolution paleosecular <span class="hlt">variation</span> record from Black Sea sediments indicating fast directional changes associated with low field intensities during marine isotope stage (MIS) 4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nowaczyk, Norbert R.; Jiabo, Liu; Frank, Ute; Arz, Helge W.</p> <p>2018-02-01</p> <p>A total of nine sediment cores recovered from the Archangelsky Ridge in the SE Black Sea were systematically subjected to intense paleo- and mineral magnetic analyses. Besides 16 accelerator mass spectrometry (AMS) 14C ages available for another core from this area, dating was accomplished by correlation of short-term warming events during the last glacial monitored by high-resolution X-ray fluorescence (XRF) scanning as maxima in both Ca/Ti and K/Ti ratios in Black Sea sediments to the so-called 'Dansgaard-Oeschger events' recognized from Greenland ice cores. Thus, several hiatuses could be identified in the various cores during the last glacial/interglacial cycle. Finally, core sections documenting marine isotope stage (MIS) 4 at high resolution back to 69 ka were selected for detailed analyses. At 64.5 ka, according to obtained results from Black Sea sediments, the second deepest minimum in relative paleointensity during the past 69 ka occurred, with the Laschamp <span class="hlt">geomagnetic</span> excursion at 41 ka being associated with the lowest field intensities. The field minimum during MIS 4 is associated with large declination swings beginning about 3 ka before the minimum. While a swing to 50°E is associated with steep inclinations (50-60°) according to the coring site at 42°N, the subsequent declination swing to 30°W is associated with shallow inclinations of down to 40°. Nevertheless, these large deviations from the direction of a geocentric axial dipole field (I = 61 °, D = 0 °) still can not yet be termed as 'excursional', since latitudes of corresponding virtual <span class="hlt">geomagnetic</span> poles (VGP) only reach down to 51.5°N (120°E) and 61.5°N (75°W), respectively. However, these VGP positions at opposite sides of the globe are linked with VGP drift rates of up to 0.2° per year in between. These extreme <span class="hlt">secular</span> <span class="hlt">variations</span> might be the mid-latitude expression of a <span class="hlt">geomagnetic</span> excursion with partly reversed inclinations found at several sites much further North in Arctic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70182720','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70182720"><span>Ionospheric current source modeling and global <span class="hlt">geomagnetic</span> induction using ground <span class="hlt">geomagnetic</span> observatory data</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Sun, Jin; Kelbert, Anna; Egbert, G.D.</p> <p>2015-01-01</p> <p>Long-period global-scale electromagnetic induction studies of deep Earth conductivity are based almost exclusively on magnetovariational methods and require accurate models of external source spatial structure. We describe approaches to inverting for both the external sources and three-dimensional (3-D) conductivity <span class="hlt">variations</span> and apply these methods to long-period (T≥1.2 days) <span class="hlt">geomagnetic</span> observatory data. Our scheme involves three steps: (1) Observatory data from 60 years (only partly overlapping and with many large gaps) are reduced and merged into dominant spatial modes using a scheme based on frequency domain principal components. (2) Resulting modes are inverted for corresponding external source spatial structure, using a simplified conductivity model with radial <span class="hlt">variations</span> overlain by a two-dimensional thin sheet. The source inversion is regularized using a physically based source covariance, generated through superposition of correlated tilted zonal (quasi-dipole) current loops, representing ionospheric source complexity smoothed by Earth rotation. Free parameters in the source covariance model are tuned by a leave-one-out cross-validation scheme. (3) The estimated data modes are inverted for 3-D Earth conductivity, assuming the source excitation estimated in step 2. Together, these developments constitute key components in a practical scheme for simultaneous inversion of the catalogue of historical and modern observatory data for external source spatial structure and 3-D Earth conductivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.4111S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.4111S"><span>PCN-index derivation at World Data Center for <span class="hlt">Geomagnetism</span>, Copenhagen, DTU Space</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stolle, C.; Matzka, J.</p> <p>2012-04-01</p> <p>The Polar Cap North (PCN) index is based on a correlation between <span class="hlt">geomagnetic</span> disturbances at the Qaanaaq <span class="hlt">geomagnetic</span> observatory (IAGA code THL) and the merging electric field derived from solar wind parameters. The index is therefore meant to provide a fast ground based single station indicator for <span class="hlt">variations</span> in the merging electric field without being dependent on satellite observations. The PC index will be subject to an IAGA endorsement process during IAGA Scientific Assembly 2013. Actually the WDC provides near real time PC-indices and post-processed final PC-indices based on former developed algorithms. However, the coefficients used for calculating the PCN distributed by the WDC Copenhagen are presently not reproducible. In the frame of the IAGA endorsement, DTU Space tests new coefficients mainly based on published algorithms. This presentation will report on activities at the WDC Copenhagen and on the current status at DTU Space with respect to the preparation for the IAGA endorsement process of the PCN-index.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.7530B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.7530B"><span>Noise Reduction of 1sec <span class="hlt">Geomagnetic</span> Observatory Data without Information Loss</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brunke, Heinz-Peter; Korte, Monika; Rudolf, Widmer-Schnidrig</p> <p>2017-04-01</p> <p>Traditional fluxgate magnetometers used at <span class="hlt">geomagnetic</span> observatories are optimized towards long-term stability. Typically, such instruments can only resolve background <span class="hlt">geomagnetic</span> field <span class="hlt">variations</span> up to a frequency of approximately 0.04 Hz and are limited by instrumental self-noise above this frequency. However, recently the demand for low noise 1 Hz observatory data has increased. IAGA has defined a standard for definitive 1sec data. Induction coils have low noise at these high frequencies, but lack long-term stability. We present a method to numerically combine the data from a three axis induction coil system with a typical low-drift observatory fluxgate magnetometer. The resulting data set has a reduced noise level above 0.04 Hz while maintaining the long term stability of the fluxgate magnetometer. Numerically we fit a spline to the fluxgate data. But in contrast to such a low pass filtering process, our method reduces the noise level at high frequencies without any loss of information. In order to experimentally confirm our result, we compared it to a very low noise scalar magnetometer: an optically pumped potassium magnetometer. In the frequency band from [0.03Hz to 0.5Hz] we found an rms-noise reduction from 80pT for the unprocessed fluxgate data to about 25pT for the processed data. We show how our method improves <span class="hlt">geomagnetic</span> 1 sec observatory data for, e.g., the study of magnetospheric pulsations and EMIC waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1713304W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1713304W"><span>Contributions from the data samples in NOC technique on the extracting of the Sq <span class="hlt">variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Yingyan; Xu, Wenyao</p> <p>2015-04-01</p> <p> using different number of data sample from 5 to 365. The result shows the first eigenmode expresses the Sq in most cases. 1.Campbell, W, Introduction to <span class="hlt">Geomagnetic</span> Fields, Cambridge Univ. Press, New York. 1997 2.Hasegawa, M, <span class="hlt">Geomagnetic</span> Sq current system, J. Geophys. Res., 1960, 65: 1437~ 1447 3.Tarpley J D. The Ionospheric wind dynanmo 2 solar tides. Planet. Space Sci., 1970, 18: 1091~ 1103 4.Richmond A D. Modeling the ionospheric wind dynamo a review. Pure Appl. Geophys., 1989, 131: 413 ~ 435 5.Suzuki, A., and H. Maeda (1978), Equivalent current systems of the daily <span class="hlt">geomagnetic</span> <span class="hlt">variations</span> in December 1964, Data Book No. 1, World Data Center C2 for <span class="hlt">Geomagnetic</span>. 6.Hibberd, F H. Day-to-day variability of the Sq <span class="hlt">geomagnetic</span> field <span class="hlt">variation</span>, Aust. J. Phys., 1981, 34: 81~ 90 7.Xu, W.-Y., and Y. Kamide (2004), Decomposition of daily <span class="hlt">geomagnetic</span> <span class="hlt">variation</span> by using method of natural orthogonal component, J. Geophys. Res., 109(A5), A05218, doi:10.1029/2003JA010216. 8.Chen G X, Xu W Y, Du A M, and et al, Statistical characteristics of the day-to-day variability in the <span class="hlt">geomagnetic</span> Sq field, J. Geophys. Res.,2007, 112, A06320, doi:10.1029/2006JA012059 9.Michelis P. De. Principal components' features of mid-latitude <span class="hlt">geomagnetic</span> daily <span class="hlt">variation</span>. Ann. Geophys., 2010,28: 1-14</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMGP53A3755K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMGP53A3755K"><span>New Sediment Data to Constrain Southern Atlantic Holocene <span class="hlt">Secular</span> <span class="hlt">Variation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Korte, M. C.; Frank, U.; Nowaczyk, N. R.; Frederichs, T.; Brown, M. C.</p> <p>2014-12-01</p> <p>The present day <span class="hlt">geomagnetic</span> field shows a notable weak zone stretching from South America to southern Africa. This is known as the South Atlantic Anomaly caused by a growing patch of reversed magnetic flux at the core-mantle boundary. The investigation of existence and evolution of similar features over the past millennia using global spherical harmonic models is hampered by the fact that at present only very few paleomagnetic data from equatorial and many southern hemisphere regions are available to constrain models well in these regions. Here, we present the results of paleomagnetic investigations of sediment cores from four locations at low latitudes. OPD 1078 and 1079 lie off the coast of Angola, GeoB6517-2 and ODP 1076D are located in the Congo Fan and M35003-4 is situated southeast of Grenada in the Tobago Basin. In addition to the paleomagnetic work all cores were subjected to a comprehensive set of rock magnetic measurements. Detailed age models based on radiocarbon dating are available for all locations, since the sites were already subjects of different aspects of climatic studies. We include these new records and previously presented data from two Ethiopian locations in millennial scale global models of the CALSxk type. Agreement of the new data to previous models and modifications of models due to the additional data are discussed, focussing in particular on magnetic field structures resembling the present-day South Atlantic Anomaly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19720034229&hterms=kinematics+reverse&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dkinematics%2Breverse','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19720034229&hterms=kinematics+reverse&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dkinematics%2Breverse"><span>Kinematic reversal schemes for the <span class="hlt">geomagnetic</span> dipole.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levy, E. H.</p> <p>1972-01-01</p> <p>Fluctuations in the distribution of cyclonic convective cells, in the earth's core, can reverse the sign of the <span class="hlt">geomagnetic</span> field. Two kinematic reversal schemes are discussed. In the first scheme, a field maintained by cyclones concentrated at low latitude is reversed by a burst of cyclones at high latitude. Conversely, in the second scheme, a field maintained predominantly by cyclones in high latitudes is reversed by a fluctuation consisting of a burst of cyclonic convection at low latitude. The precise fluid motions which produce the <span class="hlt">geomagnetic</span> field are not known. However, it appears that, whatever the details are, a fluctuation in the distribution of cyclonic cells over latitude can cause a <span class="hlt">geomagnetic</span> reversal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..132a2003S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..132a2003S"><span>Indonesian <span class="hlt">Geomagnetic</span> Maps for Epoch 2015.0 to cover of Indonesian Regions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Syirojudin, M.; Murjaya, J.; Zubaidah, S.; Hasanudin; Ahadi, S.; Efendi, N.; Suroyo, T.</p> <p>2018-03-01</p> <p>In compliance with the resolutions of IAGA (International Association of <span class="hlt">Geomagnetism</span> and Aeronomy), Since 1960’s, every five years BMKG or Meteorology, Climatology and Geophysics Agency of Indonesia made <span class="hlt">geomagnetic</span> field maps based on actual measurements in 53 repeat stations. It’s the map for more accurate result of <span class="hlt">Geomagnetic</span> maps Epoch 2015.0, the number of repeat stations has been increased to 68 locations. Analysis data was conducted by spatial analyses using collocated co-kriging and kriging with external drift to map the observation data in five components, such as Declination (D), Inclination (I), Vertical (Z), Horizontal (H), and Total <span class="hlt">Geomagnetic</span> Field (F). The data reduction used one permanent observatory i.e., Kupang Geophysical Observatory, as a reference standard. The results of this <span class="hlt">Geomagnetic</span> Maps, that the contour lines of Indonesian <span class="hlt">geomagnetic</span> declination in range -1 to 4.5 degree, Inclination component are -5 to -37 degree, Vertical component are -4000 to -28000 nT, Horizontal component are 36000 to 42000 nT, and Total <span class="hlt">Geomagnetic</span> Field are 39000 to 46000 nT. In conclusion, Indonesian <span class="hlt">Geomagnetic</span> Maps for Epoch 2015.0 can be used to compute <span class="hlt">geomagnetic</span> data around Indonesian regions until next 5 years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SpWea..15..441S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SpWea..15..441S"><span>Predicting the magnetic vectors within coronal mass ejections arriving at Earth: 2. <span class="hlt">Geomagnetic</span> response</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Savani, N. P.; Vourlidas, A.; Richardson, I. G.; Szabo, A.; Thompson, B. J.; Pulkkinen, A.; Mays, M. L.; Nieves-Chinchilla, T.; Bothmer, V.</p> <p>2017-02-01</p> <p>This is a companion to Savani et al. (2015) that discussed how a first-order prediction of the internal magnetic field of a coronal mass ejection (CME) may be made from observations of its initial state at the Sun for space weather forecasting purposes (Bothmer-Schwenn scheme (BSS) model). For eight CME events, we investigate how uncertainties in their predicted magnetic structure influence predictions of the <span class="hlt">geomagnetic</span> activity. We use an empirical relationship between the solar wind plasma drivers and Kp index together with the inferred magnetic vectors, to make a prediction of the time <span class="hlt">variation</span> of Kp (Kp(BSS)). We find a 2σ uncertainty range on the magnetic field magnitude (|B|) provides a practical and convenient solution for predicting the uncertainty in <span class="hlt">geomagnetic</span> storm strength. We also find the estimated CME velocity is a major source of error in the predicted maximum Kp. The time <span class="hlt">variation</span> of Kp(BSS) is important for predicting periods of enhanced and maximum <span class="hlt">geomagnetic</span> activity, driven by southerly directed magnetic fields, and periods of lower activity driven by northerly directed magnetic field. We compare the skill score of our model to a number of other forecasting models, including the NOAA/Space Weather Prediction Center (SWPC) and Community Coordinated Modeling Center (CCMC)/SWRC estimates. The BSS model was the most unbiased prediction model, while the other models predominately tended to significantly overforecast. The True skill score of the BSS prediction model (TSS = 0.43 ± 0.06) exceeds the results of two baseline models and the NOAA/SWPC forecast. The BSS model prediction performed equally with CCMC/SWRC predictions while demonstrating a lower uncertainty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGP51A1377K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGP51A1377K"><span>Investigation of Magnetotelluric Source Effect Based on Twenty Years of Telluric and <span class="hlt">Geomagnetic</span> Observation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kis, A.; Lemperger, I.; Wesztergom, V.; Menvielle, M.; Szalai, S.; Novák, A.; Hada, T.; Matsukiyo, S.; Lethy, A. M.</p> <p>2016-12-01</p> <p>Magnetotelluric method is widely applied for investigation of subsurface structures by imaging the spatial distribution of electric conductivity. The method is based on the experimental determination of surface electromagnetic impedance tensor (Z) by surface <span class="hlt">geomagnetic</span> and telluric registrations in two perpendicular orientation. In practical explorations the accurate estimation of Z necessitates the application of robust statistical methods for two reasons:1) the <span class="hlt">geomagnetic</span> and telluric time series' are contaminated by man-made noise components and2) the non-homogeneous behavior of ionospheric current systems in the period range of interest (ELF-ULF and longer periods) results in systematic deviation of the impedance of individual time windows.Robust statistics manage both load of Z for the purpose of subsurface investigations. However, accurate analysis of the long term temporal <span class="hlt">variation</span> of the first and second statistical moments of Z may provide valuable information about the characteristics of the ionospheric source current systems. Temporal <span class="hlt">variation</span> of extent, spatial variability and orientation of the ionospheric source currents has specific effects on the surface impedance tensor. Twenty year long <span class="hlt">geomagnetic</span> and telluric recordings of the Nagycenk Geophysical Observatory provides unique opportunity to reconstruct the so called magnetotelluric source effect and obtain information about the spatial and temporal behavior of ionospheric source currents at mid-latitudes. Detailed investigation of time series of surface electromagnetic impedance tensor has been carried out in different frequency classes of the ULF range. The presentation aims to provide a brief review of our results related to long term periodic modulations, up to solar cycle scale and about eventual deviations of the electromagnetic impedance and so the reconstructed equivalent ionospheric source effects.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.7159H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.7159H"><span>Calibration of historical <span class="hlt">geomagnetic</span> observations from Prague-Klementinum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hejda, Pavel</p> <p>2015-04-01</p> <p>The long tradition of <span class="hlt">geomagnetic</span> observations on the Czech territory dates back to 1839, when regular observations were started by Karl Kreil at the Astronomical Observatory Prague-Klementinum. Observations were carried out manually, at the beginning more than ten times per day and the frequency later decreased to 5 daily observations. Around the turn of century the observations became to be disturbed by the increasing urban magnetic noise and the observatory was closed down in 1926. The <span class="hlt">variation</span> measurements were completed by absolute measurements carried out several times per year. Thanks to the diligence and carefulness of Karl Kreil and his followers all results were printed in the yearbooks Magnetische und meteorologische Beobachtungen zu Prag and have thus been saved until presence. The entire collection is kept at the Central Library of the Czech Academy of Sciences. As the oldest <span class="hlt">geomagnetic</span> data have been recently recognized as an important source of information for Space Weather studies, digitization and analysis of the data have been now started. Although all volumes have been scanned with the OCR option, the low quality of original books does not allow for an automatic transformation to digital form. The data were typed by hand to Excel files with a primary check and further processed. <span class="hlt">Variation</span> data from 1839 to 1871 were published in measured units (scales of divisions). Their reduction to physical units was not as straight forward as we are used in recent observatories. There were several reasons: (i) the large heavy magnetic rods were not as stable as recent systems, (ii) the absolute measurements of horizontal components were carried out by the genius but rather complicated Gauss method, (iii) the intervals between absolute measurements was on the scale of months and eventual errors were not recognized timely. The presentation will discuss several methods and give examples how to cope with the problem.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11875208','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11875208"><span>Natural variability of atmospheric temperatures and <span class="hlt">geomagnetic</span> intensity over a wide range of time scales.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pelletier, Jon D</p> <p>2002-02-19</p> <p>The majority of numerical models in climatology and <span class="hlt">geomagnetism</span> rely on deterministic finite-difference techniques and attempt to include as many empirical constraints on the many processes and boundary conditions applicable to their very complex systems. Despite their sophistication, many of these models are unable to reproduce basic aspects of climatic or <span class="hlt">geomagnetic</span> dynamics. We show that a simple stochastic model, which treats the flux of heat energy in the atmosphere by convective instabilities with random advection and diffusive mixing, does a remarkable job at matching the observed power spectrum of historical and proxy records for atmospheric temperatures from time scales of one day to one million years (Myr). With this approach distinct changes in the power-spectral form can be associated with characteristic time scales of ocean mixing and radiative damping. Similarly, a simple model of the diffusion of magnetic intensity in Earth's core coupled with amplification and destruction of the local intensity can reproduce the observed 1/f noise behavior of Earth's <span class="hlt">geomagnetic</span> intensity from time scales of 1 (Myr) to 100 yr. In addition, the statistics of the fluctuations in the polarity reversal rate from time scales of 1 Myr to 100 Myr are consistent with the hypothesis that reversals are the result of <span class="hlt">variations</span> in 1/f noise <span class="hlt">geomagnetic</span> intensity above a certain threshold, suggesting that reversals may be associated with internal fluctuations rather than changes in mantle thermal or magnetic boundary conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=128574','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=128574"><span>Natural variability of atmospheric temperatures and <span class="hlt">geomagnetic</span> intensity over a wide range of time scales</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Pelletier, Jon D.</p> <p>2002-01-01</p> <p>The majority of numerical models in climatology and <span class="hlt">geomagnetism</span> rely on deterministic finite-difference techniques and attempt to include as many empirical constraints on the many processes and boundary conditions applicable to their very complex systems. Despite their sophistication, many of these models are unable to reproduce basic aspects of climatic or <span class="hlt">geomagnetic</span> dynamics. We show that a simple stochastic model, which treats the flux of heat energy in the atmosphere by convective instabilities with random advection and diffusive mixing, does a remarkable job at matching the observed power spectrum of historical and proxy records for atmospheric temperatures from time scales of one day to one million years (Myr). With this approach distinct changes in the power-spectral form can be associated with characteristic time scales of ocean mixing and radiative damping. Similarly, a simple model of the diffusion of magnetic intensity in Earth's core coupled with amplification and destruction of the local intensity can reproduce the observed 1/f noise behavior of Earth's <span class="hlt">geomagnetic</span> intensity from time scales of 1 (Myr) to 100 yr. In addition, the statistics of the fluctuations in the polarity reversal rate from time scales of 1 Myr to 100 Myr are consistent with the hypothesis that reversals are the result of <span class="hlt">variations</span> in 1/f noise <span class="hlt">geomagnetic</span> intensity above a certain threshold, suggesting that reversals may be associated with internal fluctuations rather than changes in mantle thermal or magnetic boundary conditions. PMID:11875208</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSM41B2225X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSM41B2225X"><span>Conjugate Event Study of <span class="hlt">Geomagnetic</span> ULF Pulsations with Wavelet-based Indices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Z.; Clauer, C. R.; Kim, H.; Weimer, D. R.; Cai, X.</p> <p>2013-12-01</p> <p>The interactions between the solar wind and <span class="hlt">geomagnetic</span> field produce a variety of space weather phenomena, which can impact the advanced technology systems of modern society including, for example, power systems, communication systems, and navigation systems. One type of phenomena is the <span class="hlt">geomagnetic</span> ULF pulsation observed by ground-based or in-situ satellite measurements. Here, we describe a wavelet-based index and apply it to study the <span class="hlt">geomagnetic</span> ULF pulsations observed in Antarctica and Greenland magnetometer arrays. The wavelet indices computed from these data show spectrum, correlation, and magnitudes information regarding the <span class="hlt">geomagnetic</span> pulsations. The results show that the <span class="hlt">geomagnetic</span> field at conjugate locations responds differently according to the frequency of pulsations. The index is effective for identification of the pulsation events and measures important characteristics of the pulsations. It could be a useful tool for the purpose of monitoring <span class="hlt">geomagnetic</span> pulsations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009GGG....10.8003S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009GGG....10.8003S"><span><span class="hlt">Geomagnetic</span> paleointensity between 1300 and 1750 A.D. derived from a bread oven floor sequence in Lübeck, Germany</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schnepp, Elisabeth; Lanos, Philippe; Chauvin, Annick</p> <p>2009-08-01</p> <p><span class="hlt">Geomagnetic</span> paleointensities have been determined from a single archaeological site in Lübeck, Germany, where a sequence of 25 bread oven floors has been preserved in a bakery from medieval times until today. Age dating confines the time interval from about 1300 A.D. to about 1750 A.D. Paleomagnetic directions have been published from each oven floor and are updated here. The specimens have very stable directions and no or only weak secondary components. The oven floor material was characterized rock magnetically using Thellier viscosity indices, median destructive field values, Curie point determinations, and hysteresis measurements. Magnetic carriers are mixtures of SD, PSD, and minor MD magnetite and/or maghemite together with small amounts of hematite. Paleointensity was measured from selected specimens with the double-heating Thellier method including pTRM checks and determination of TRM anisotropy tensors. Corrections for anisotropy as well as for cooling rate turned out to be unnecessary. Ninety-two percent of the Thellier experiments passed the assigned acceptance criteria and provided four to six reliable paleointensity estimates per oven floor. Mean paleointensity values derived from 22 oven floors show maxima in the 15th and early 17th centuries A.D., followed by a decrease of paleointensity of about 20% until 1750 A.D. Together with the directions the record represents about 450 years of full vector <span class="hlt">secular</span> <span class="hlt">variation</span>. The results compare well with historical models of the Earth's magnetic field as well as with a selected high-quality paleointensity data set for western and central Europe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AdSpR..45..940M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AdSpR..45..940M"><span>Effects of <span class="hlt">geomagnetic</span> activity and atmospheric power <span class="hlt">variations</span> on quantitative measures of brain activity: Replication of the Azerbaijani studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mulligan, Bryce P.; Hunter, Mathew D.; Persinger, Michael A.</p> <p>2010-04-01</p> <p>This study replicates and extends the observations by Babayev and Allahveriyeva that changes in right hemispheric electroencephalographic activity are correlated with increases in <span class="hlt">geomagnetic</span> activity. During the <span class="hlt">geomagnetically</span> quiet interface between solar cycle 23 and 24 quantitative electroencephalographic (QEEG) measurements were completed for normal young adults in three separate experiments involving about 120 samples over 1.5 years. The most consistent, moderate strength correlations occurred for the changes in power within the gamma and theta ranges over the right frontal lobe. Real-time measures of atmospheric power obtained from polar orbiting satellites showed similar effects. The preferential involvement of the right frontal lobe and the regions subject to its inhibition with environmental energetic changes are consistent with the behavioural correlations historically associated with these conditions. They include increased incidence of emotional lability, erroneous reconstruction of experiences, social confrontations, and unusual perceptions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016IAUS..318...46N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016IAUS..318...46N"><span><span class="hlt">Secular</span> evolution of asteroid families: the role of Ceres</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Novaković, Bojan; Tsirvoulis, Georgios; Marò, Stefano; Đošović, Vladimir; Maurel, Clara</p> <p>2016-01-01</p> <p>We consider the role of the dwarf planet Ceres on the <span class="hlt">secular</span> dynamics of the asteroid main belt. Specifically, we examine the post impact evolution of asteroid families due to the interaction of their members with the linear nodal <span class="hlt">secular</span> resonance with Ceres. First, we find the location of this resonance and identify which asteroid families are crossed by its path. Next, we summarize our results for three asteroid families, namely (1726) Hoffmeister, (1128) Astrid and (1521) Seinajoki which have irregular distributions of their members in the proper elements space, indicative of the effect of the resonance. We confirm this by performing a set of numerical simulations, showcasing that the perturbing action of Ceres through its linear nodal <span class="hlt">secular</span> resonance is essential to reproduce the actual shape of the families.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EP%26S...69...70W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EP%26S...69...70W"><span><span class="hlt">Geomagnetic</span> storms of cycle 24 and their solar sources</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Watari, Shinichi</p> <p>2017-05-01</p> <p>Solar activity of cycle 24 following the deep minimum between cycle 23 and cycle 24 is the weakest one since cycle 14 (1902-1913). <span class="hlt">Geomagnetic</span> activity is also low in cycle 24. We show that this low <span class="hlt">geomagnetic</span> activity is caused by the weak dawn-to-dusk solar wind electric field ( E d-d) and that the occurrence rate of E d-d > 5 mV/m decreased in the interval from 2013 to 2014. We picked up seventeen <span class="hlt">geomagnetic</span> storms with the minimum Dst index of less than -100 nT and identified their solar sources in cycle 24 (2009-2015). It is shown that the relatively slow coronal mass ejections contributed to the <span class="hlt">geomagnetic</span> storms in cycle 24.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..12212517M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..12212517M"><span>Equatorial E Region Electric Fields and Sporadic E Layer Responses to the Recovery Phase of the November 2004 <span class="hlt">Geomagnetic</span> Storm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moro, J.; Resende, L. C. A.; Denardini, C. M.; Xu, J.; Batista, I. S.; Andrioli, V. F.; Carrasco, A. J.; Batista, P. P.; Schuch, N. J.</p> <p>2017-12-01</p> <p>Equatorial E region electric fields (EEFs) inferred from coherent radar data, sporadic-E (Es) layers observed from a digital ionosonde data, and modeling results are used to study the responses of the equatorial E region over São Luís (SLZ, 2.3°S, 44.2°W, -7° dip angle), Brazil, during the super storm of November 2004. The EEF is presented in terms of the zonal (Ey) and vertical (Ez) components in order to analyze the corresponding characteristics of different types of Es seen in ionograms and simulated with the E region ionospheric model. We bring out the variabilities of Ey and Ez components with storm time changes in the equatorial E region. In addition, some aspects of the electric fields and Es behavior in three cases of weak, very weak, and strong Type II occurrences during the recovery phase of the <span class="hlt">geomagnetic</span> storm are discussed. The connection between the enhanced occurrence and suppressions of the Type II irregularities and the q-type Es (Esq) controlled by electric fields, with the development or disruption of the blanketing sporadic E (Esb) layers produced by wind shear mechanism, is also presented. The mutual presence of Esq along with the Esb occurrences is a clear indicator of the <span class="hlt">secular</span> drift of the magnetic equator and hence that of the equatorial electrojet (EEJ) over SLZ. The results show evidence about the EEJ and Es layer electrodynamics and coupling during <span class="hlt">geomagnetic</span> disturbance time electric fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760037806&hterms=coronary+heart+disease&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dcoronary%2Bheart%2Bdisease','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760037806&hterms=coronary+heart+disease&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dcoronary%2Bheart%2Bdisease"><span>Search for correlation between <span class="hlt">geomagnetic</span> disturbances and mortality</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lipa, B. J.; Sturrock, P. A.; Rogot, F.</p> <p>1976-01-01</p> <p>A search is conducted for a possible correlation between solar activity and myocardial infarction and stroke in the United States. A statistical analysis is performed using data on <span class="hlt">geomagnetic</span> activity and the daily U.S. mortality due to coronary heart disease and stroke for the years 1962 through 1966. None of the results are found to yield any evidence of a correlation. It is concluded that correlations claimed by Soviet workers between <span class="hlt">geomagnetic</span> activity and the incidence of various human diseases are probably not statistically significant or probably are not due to a causal relation between <span class="hlt">geomagnetic</span> activity and disease.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991STIN...9124036B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991STIN...9124036B"><span><span class="hlt">Geomagnetic</span> storms: Potential economic impacts on electric utilities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barnes, P. R.; Vandyke, J. W.</p> <p>1991-03-01</p> <p><span class="hlt">Geomagnetic</span> storms associated with sunspot and solar flare activity can disturb communications and disrupt electric power. A very severe <span class="hlt">geomagnetic</span> storm could cause a major blackout with an economic impact of several billion dollars. The vulnerability of electric power systems in the northeast United States will likely increase during the 1990s because of the trend of transmitting large amounts of power over long distance to meet the electricity demands of this region. A comprehensive research program and a warning satellite to monitor the solar wind are needed to enhance the reliability of electric power systems under the influence of <span class="hlt">geomagnetic</span> storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1989CeMDA..46..231F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1989CeMDA..46..231F"><span>The three principal <span class="hlt">secular</span> resonances nu(5), nu(6), and nu(16) in the asteroidal belt</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Froeschle, Ch.; Scholl, H.</p> <p>1989-09-01</p> <p>Theoretical and numerical results obtained for <span class="hlt">secular</span> resonant motion in the asteroidal belt are reviewed. William's (1969) theory yields the locations of the principal <span class="hlt">secular</span> resonances nu(5), Nu(6), and nu(16) in the asteroidal belt. Theories by Nakai and Kinoshita (1985) and by Yoshikawa (1987) make it possible to model the basic features of orbital evolution at the <span class="hlt">secular</span> resonances nu(16) and nu(6), respectively. No theory is available for the <span class="hlt">secular</span> resonance nu(5). Numerical experiments by Froeschle and Scholl yield quantitative and new qualitative results for orbital evolutions at the three principal <span class="hlt">secular</span> resonances nu(5), nu(6), and nu(16). These experiments indicate possible chaotic motion due to overlapping resonances. A <span class="hlt">secular</span> resonance may overlap with another <span class="hlt">secular</span> resonance or with a mean motion resonance. The role of the <span class="hlt">secular</span> resonances as possible sources of meteorites is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=euro&pg=3&id=EJ1027760','ERIC'); return false;" href="https://eric.ed.gov/?q=euro&pg=3&id=EJ1027760"><span>The Other Partition: Religious and <span class="hlt">Secular</span> Education in British Palestine</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>Schneider, Suzanne</p> <p>2014-01-01</p> <p>The recent critical turn toward post-<span class="hlt">secularism</span>, particularly on behalf of theorists working from the perspective of Christian societies, has highlighted the difficulty of approaching the history of the Middle East through the binary of religion and <span class="hlt">secularism</span>. This article argues that such terms are of little explanatory value in and of…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22998435','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22998435"><span><span class="hlt">Geomagnetic</span> disturbances may be environmental risk factor for multiple sclerosis: an ecological study of 111 locations in 24 countries.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sajedi, Seyed Aidin; Abdollahi, Fahimeh</p> <p>2012-09-24</p> <p>We noticed that a hypothesis based on the effect of <span class="hlt">geomagnetic</span> disturbances (GMD) has the ability to explain special features of multiple sclerosis (MS). Areas around <span class="hlt">geomagnetic</span> 60 degree latitude (GM60L) experience the greatest amount of GMD. The easiest way to evaluate our hypothesis was to test the association of MS prevalence (MSP) with angular distance to <span class="hlt">geomagnetic</span> 60 degree latitude (AMAG60) and compare it with the known association of MS with geographical latitude (GL). We did the same with angular distance to geographic 60 degree latitude (AGRAPH60) as a control. English written papers with MSP keywords, done in Europe (EUR), North America (NA) or Australasia (AUS) were retrieved from the PubMed. <span class="hlt">Geomagnetic</span> coordinates were determined for each location and AMAG60 was calculated as absolute value of numerical difference between its <span class="hlt">geomagnetic</span> latitude from GM60L. By an ecological study with using meta-regression analyses, the relationship of MSP with GL, AMAG60 and AGRAPH60 were evaluated separately. MSP data were weighted by square root of number of prevalent cases. Models were compared by their adjusted R square (AR2) and standard error of estimate (SEE). 111 MSP data were entered in the study. In each continent, AMAG60 had the best correlation with MSP, the largest AR2 (0.47, 0.42 and 0.84 for EUR, NA and AUS, respectively) and the least SEE. Merging both hemispheres data, AMAG60 explained 56% of MSP <span class="hlt">variations</span> with the least SEE (R = 0.75, AR2 = 0.56, SEE = 57), while GL explained 17% (R = 0.41, AR2 = 0.17, SEE = 78.5) and AGRAPH60 explained 12% of that <span class="hlt">variations</span> with the highest SEE (R = 0.35, AR2 = 0.12, SEE = 80.5). Our results confirmed that AMAG60 is the best describer of MSP <span class="hlt">variations</span> and has the strongest association with MSP distribution. They clarified that the well-known latitudinal gradient of MSP may be actually a gradient related to GM60L. Moreover, the location of GM60L can elucidate why MSP has parabolic and linear gradient in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.6488R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.6488R"><span>ULF <span class="hlt">geomagnetic</span> activity effects on tropospheric temperature, specific humidity, and cloud cover in Antarctica, during 2003-2010</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Regi, Mauro; Redaelli, Gianluca; Francia, Patrizia; De Lauretis, Marcello</p> <p>2017-06-01</p> <p>In the present study we investigated the possible relationship between the ULF <span class="hlt">geomagnetic</span> activity and the <span class="hlt">variations</span> of several atmospheric parameters. In particular, we compared the ULF activity in the Pc1-2 frequency band (100 mHz-5 Hz), computed from <span class="hlt">geomagnetic</span> field measurements at Terra Nova Bay in Antarctica, with the tropospheric temperature T, specific humidity Q, and cloud cover (high cloud cover, medium cloud cover, and low cloud cover) obtained from reanalysis data set. The statistical analysis was conducted during the years 2003-2010, using correlation and Superposed Epoch Analysis approaches. The results show that the atmospheric parameters significantly change following the increase of <span class="hlt">geomagnetic</span> activity within 2 days. These changes are evident in particular when the interplanetary magnetic field Bz component is oriented southward (Bz<0) and the By component duskward (By>0). We suggest that both the precipitation of electrons induced by Pc1-2 activity and the intensification of the polar cap potential difference, modulating the microphysical processes in the clouds, can affect the atmosphere conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AdSpR..51...96K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AdSpR..51...96K"><span>Helio-<span class="hlt">geomagnetic</span> influence in cardiological cases</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Katsavrias, Ch.; Preka-Papadema, P.; Moussas, X.; Apostolou, Th.; Theodoropoulou, A.; Papadima, Th.</p> <p>2013-01-01</p> <p>The effects of the energetic phenomena of the Sun, flares and coronal mass ejections (CMEs) on the Earth's ionosphere-magnetosphere, through the solar wind, are the sources of the <span class="hlt">geomagnetic</span> disturbances and storms collectively known as Space Weather. The research on the influence of Space Weather on biological and physiological systems is open. In this work we study the Space Weather impact on Acute Coronary Syndromes (ACS) distinguishing between ST-segment elevation acute coronary syndromes (STE-ACS) and non-ST-segment elevation acute coronary syndromes (NSTE-ACS) cases. We compare detailed patient records from the 2nd Cardiologic Department of the General Hospital of Nicaea (Piraeus, Greece) with characteristics of <span class="hlt">geomagnetic</span> storms (DST), solar wind speed and statistics of flares and CMEs which cover the entire solar cycle 23 (1997-2007). Our results indicate a relationship of ACS to helio-<span class="hlt">geomagnetic</span> activity as the maximum of the ACS cases follows closely the maximum of the solar cycle. Furthermore, within very active periods, the ratio NSTE-ACS to STE-ACS, which is almost constant during periods of low to medium activity, changes favouring the NSTE-ACS. Most of the ACS cases exhibit a high degree of association with the recovery phase of the <span class="hlt">geomagnetic</span> storms; a smaller, yet significant, part was found associated with periods of fast solar wind without a storm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.1366P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.1366P"><span>Possible Connection of Geological Composition With <span class="hlt">Geomagnetic</span> Field Change In Kopaonik Thrust Region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Popeskov, Mirjana; Cukavac, Milena; Lazovic, Caslav</p> <p></p> <p>This paper should consider interpretation of <span class="hlt">geomagnetic</span> field changes on the basis of possible connection with geological composition of deformation zone. Analysis of total magnetic field intensity data from 38 surveys, carried out in the period may 1980 ­ november 2001 in Kopaonik thrust region, central Serbia, reveals anomalous behaviour of local field changes in particular time intervals. These data give us possibility to observe <span class="hlt">geomagnetic</span> changes in long period of time. This paper shall consider if and how different magnetizations of geological composition of array are in connection with anomalous <span class="hlt">geomagnetic</span> field change. We shall consider how non-uniform geological structure or rocks with different magnetizations can effect <span class="hlt">geomagnetic</span> observations and weather sharp contrast in rock magnetization between neighbour layers can give rise to larger changes in the <span class="hlt">geomagnetic</span> total intensity than those for a uniform layer. For that purpose we are going to consider geological and tectonical map of Kopaonik region. We shall also consider map of vertical component of <span class="hlt">geomagnetic</span> field because Kopaonik belongs to high magnetic anomaly zone. Corelation of <span class="hlt">geomagnetic</span> and geological data is supposed to give us some answers to the question of origine of some anomalious <span class="hlt">geomagnetic</span> changes in total intensity of <span class="hlt">geomagnetic</span> field. It can also represent first step in corelationof <span class="hlt">geomagnetic</span> field changes to other geophysical, seismological or geological data that can be couse of <span class="hlt">geomagnetic</span> field change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750012117','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750012117"><span>Search for correlation between <span class="hlt">geomagnetic</span> disturbances and mortality</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lipa, B. J.; Barnes, C. W.; Sturrock, P. A.; Feinleib, M.; Rogot, E.</p> <p>1975-01-01</p> <p>Statistical evaluation of death rates in the U.S.A. from heart diseases or stroke did not show any correlation with measured <span class="hlt">geomagnetic</span> pulsations and thus do not support a claimed relationship between <span class="hlt">geomagnetic</span> activity and mortality rates to low frequency fluctuations of the earth's magnetic field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoRL..45.1845B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoRL..45.1845B"><span>A Probabilistic Assessment of the Next <span class="hlt">Geomagnetic</span> Reversal</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buffett, Bruce; Davis, William</p> <p>2018-02-01</p> <p>Deterministic forecasts for the next <span class="hlt">geomagnetic</span> reversal are not feasible due to large uncertainties in the present-day state of the Earth's core. A more practical approach relies on probabilistic assessments using paleomagnetic observations to characterize the amplitude of fluctuations in the <span class="hlt">geomagnetic</span> dipole. We use paleomagnetic observations for the past 2 Myr to construct a stochastic model for the axial dipole field and apply well-established methods to evaluate the probability of the next <span class="hlt">geomagnetic</span> reversal as a function of time. For a present-day axial dipole moment of 7.6 × 1022 A m2, the probability of the dipole entering a reversed state is less than 2% after 20 kyr. This probability rises to 11% after 50 kyr. An imminent <span class="hlt">geomagnetic</span> reversal is not supported by paleomagnetic observations. The current rate of decline in the dipole moment is unusual but within the natural variability predicted by the stochastic model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28357508','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28357508"><span>Influence of <span class="hlt">geomagnetic</span> activity and atmospheric pressure in hypertensive adults.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Azcárate, T; Mendoza, B</p> <p>2017-09-01</p> <p>We performed a study of the systolic and diastolic arterial blood pressure behavior under natural variables such as the atmospheric pressure and the horizontal <span class="hlt">geomagnetic</span> field component. We worked with a group of eight adult hypertensive volunteers, four men and four women, with ages between 18 and 27 years in Mexico City during a <span class="hlt">geomagnetic</span> storm in 2014. The data was divided by gender, age, and day/night cycle. We studied the time series using three methods: correlations, bivariate analysis, and superposed epoch (within a window of 2 days around the day of occurrence of a <span class="hlt">geomagnetic</span> storm) analysis, between the systolic and diastolic blood pressure and the natural variables. The correlation analysis indicated a correlation between the systolic and diastolic blood pressure and the atmospheric pressure and the horizontal <span class="hlt">geomagnetic</span> field component, being the largest during the night. Furthermore, the correlation and bivariate analyses showed that the largest correlations are between the systolic and diastolic blood pressure and the horizontal <span class="hlt">geomagnetic</span> field component. Finally, the superposed epoch analysis showed that the largest number of significant changes in the blood pressure under the influence of <span class="hlt">geomagnetic</span> field occurred in the systolic blood pressure for men.</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. Their policies may differ from this site.</div> </div><!-- container --> <footer><a id="backToTop" href="#top"> </a><nav><a id="backToTop" href="#top"> </a><ul class="links"><a id="backToTop" href="#top"> </a><li><a id="backToTop" href="#top"></a><a href="/sitemap.html">Site Map</a></li> <li><a href="/members/index.html">Members Only</a></li> <li><a href="/website-policies.html">Website Policies</a></li> <li><a href="https://doe.responsibledisclosure.com/hc/en-us" target="_blank">Vulnerability Disclosure Program</a></li> <li><a href="/contact.html">Contact Us</a></li> </ul> <div class="small">Science.gov is maintained by the U.S. Department of Energy's <a href="https://www.osti.gov/" target="_blank">Office of Scientific and Technical Information</a>, in partnership with <a href="https://www.cendi.gov/" target="_blank">CENDI</a>.</div> </nav> </footer> <script type="text/javascript"><!-- // var lastDiv = ""; function showDiv(divName) { // hide last div if (lastDiv) { document.getElementById(lastDiv).className = "hiddenDiv"; } //if value of the box is not nothing and an object with that name exists, then change the class if (divName && document.getElementById(divName)) { document.getElementById(divName).className = "visibleDiv"; lastDiv = divName; } } //--> </script> <script> /** * Function that tracks a click on an outbound link in Google Analytics. * This function takes a valid URL string as an argument, and uses that URL string * as the event label. */ var trackOutboundLink = function(url,collectionCode) { try { h = window.open(url); setTimeout(function() { ga('send', 'event', 'topic-page-click-through', collectionCode, url); }, 1000); } catch(err){} }; </script> <!-- Google Analytics --> <script> (function(i,s,o,g,r,a,m){i['GoogleAnalyticsObject']=r;i[r]=i[r]||function(){ (i[r].q=i[r].q||[]).push(arguments)},i[r].l=1*new Date();a=s.createElement(o), m=s.getElementsByTagName(o)[0];a.async=1;a.src=g;m.parentNode.insertBefore(a,m) })(window,document,'script','//www.google-analytics.com/analytics.js','ga'); ga('create', 'UA-1122789-34', 'auto'); ga('send', 'pageview'); </script> <!-- End Google Analytics --> <script> showDiv('page_1') </script> </body> </html>