Seasonal Variability of GPS-VTEC and Model During Low Solar Activity Period (2006–2007) Near the Equatorial Ionization Anomaly Crest Location in Chinese Zone

Total Page:16

File Type:pdf, Size:1020Kb

Seasonal Variability of GPS-VTEC and Model During Low Solar Activity Period (2006–2007) Near the Equatorial Ionization Anomaly Crest Location in Chinese Zone Available online at www.sciencedirect.com Advances in Space Research 51 (2013) 366–376 www.elsevier.com/locate/asr Seasonal variability of GPS-VTEC and model during low solar activity period (2006–2007) near the equatorial ionization anomaly crest location in Chinese zone Guoqi Liu ⇑, Wengeng Huang, Jiancun Gong, Hua Shen Center for Space Science and Applied Research, Chinese Academy of Sciences, Beijing 100190, PR China Received 9 March 2012; received in revised form 3 September 2012; accepted 4 September 2012 Available online 12 September 2012 Abstract Variability of vertical TEC recorded at Fuzhou (26.1°N, 119.3°E, geomagnetic latitude 14.4°N), Xiamen (24.5°N, 118.1°E, geomag- netic latitude 13.2°N), Nanning (22.8°N, 108.3°E, geomagnetic latitude 11.4°N), China, during the low solar activity in 2006–2007 have been analyzed and discussed. Remarkable seasonal anomaly was found over three stations with the highest value during spring and the lowest value during summer. The relative standard deviation of VTEC is over 20% all the time, with steady and smooth variation during daytime while it has a large fluctuation during nighttime. The biggest correlation coefficient was found in the VTEC-sunspot pair with a value of over 0.5. It seems that solar activity has a better correlation ship than geomagnetic activity with the variation of VTEC and better correlations are found with more long-term data when comparing our previous study. The results of comparing observation with model prediction in three sites reveal again that the SPIM model overestimates the measured VTEC in the low latitude area. Ó 2012 COSPAR. Published by Elsevier Ltd. All rights reserved. Keywords: Vertical TEC; Low solar activity; Equatorial ionospheric anomaly; Seasonal variation; SPIM 1. Introduction long compared to the geometric range between the satellite and the receiver, which induces range error in the position- Acting as a dispersive medium, the ionosphere has great ing and navigation (Bagiya et al., 2009). These range errors influence on the satellite navigation and communication, are relatively obvious in the ionosphere above the EIA and the effect is directly proportional to the free electron regions due to the high background electron density and density, which could change the phase and strength of elec- its rapid, complex variation. The EIA, i.e., “equatorial ion- tromagnetic radio frequency wave. When the satellite sig- ization anomaly” or “Appleton anomaly” was reported in nal propagates through the ionosphere, the carrier 1946. This interesting phenomenon of EIA is like as: The experiences a phase advance and the code experiences a distribution of ionization density at the F layer in the vicin- group delay due to the total number of free electrons along ity of magnetic dip equator is characterized by a trough at the path of the signals from the satellite to the receiver. the equator and two crests on either side of the equator (at Therefore, the carrier phase pseudo ranges are measured about ±15° magnetic latitude) during the day. The electro- too short and the code pseudo ranges are measured too dynamics drift and diffusion theories have been used to explain this interesting phenomenon. During the daytime, the mutual perpendicular eastward electric field and north- ⇑ Corresponding author. Address: Room A1106B, NO. 1 Nanertiao, ward geomagnetic field give rise to an upward E Â B drift. Zhongguancun, Haidian District, Beijing 100190, PR China. Tel.: +86 10 After the plasma is lifted to greater heights, it diffuses along 62586419; fax: +86 10 62586416. E-mail addresses: [email protected] (G. Liu), [email protected] magnetic field lines due to the combined influence of (W. Huang), [email protected] (J. Gong), [email protected] (H. Shen). pressure gradient forces and gravity, which forms a trough 0273-1177/$36.00 Ó 2012 COSPAR. Published by Elsevier Ltd. All rights reserved. http://dx.doi.org/10.1016/j.asr.2012.09.002 G. Liu et al. / Advances in Space Research 51 (2013) 366–376 367 at the equator and two crests at higher latitudes on F2 layer mate the GPS-derived value (Bhuyan et al., 2006; Bhuyan (Appleton, 1946; Martyn, 1955; Duncan, 1960; Hanson and Borah, 2007; Obrou et al., 2009; Galav et al., 2010; and Moffett, 1966). In order to reduce the detrimental Aggarwal, 2011; Liu et al., 2012; Adewale et al., 2012). effects on the GPS based navigation, it is very necessary One reason is lack of consecutive long-term observation to have a prior and precise knowledge of the variation in low latitude, another is the established ionosphere model and distribution of ionosphere parameters in different is based on the data more from high and middle latitude region, especially low latitude regions. (Bilitza, 2001). Therefore, as the part of the global iono- The Total Electron Content (TEC) is one of the most sphere characteristic, these results of our work will be good important parameters to characterize the ionosphere prop- complements and be propitious to study and establish a erty, which is calculated as an integral of electron number more accurate model of ionosphere. density along the line of sight from satellite to receiver and In this work, Observation data recorded in Fuzhou could vary intensely from day to day (Huang et al., 1989; (26.1°N, 119.3°E, geomagnetic latitude 14.4°N), Xiamen Rastogi and Klobuchar, 1990). Since the F region density (24.5°N, 118.1°E, geomagnetic latitude 13.2°N), and has a great weight for total electron content and the main Nanning (22.8°N, 108.3°E, geomagnetic latitude 11.4°N) contribution to TEC would occur around the height of the were used to investigate the characteristics of VTEC. We will maximum ionization in the F layer, the development and give an overall description of temporal variation character- variation of EIA is as seen in TEC. Now it is accepted that istics of VTEC in low solar activity period from year 2006 to the magnitude and variation of TEC relate to local time, 2007; we also examine the effect of solar and geomagnetic solar activity, geomagnetic conditions, region of the earth activity on the VTEC in those three sites. As the extension and sudden space weather events. In the low latitude of of our previous study, The results will make one too well East Asia, some studies of TEC have been reported using understand the variation of TEC around 110–120°E near the data recorded round 120°E. Huang and Cheng (1996) the Tropic of Cancer, and the difference between observa- studied the solar cycle variation of EIA in TEC using tion and output of Standard Plasmasphere–Ionosphere observed data from a single ground station at Lunping Model (SPIM, Gulyaeva and Bilitza, 2012). (25.00°N, 121.17°E), and found no significant solar cycle effect in the occurrence time of the most developed 2. Observation data equatorial ionospheric anomaly and the winter crest appears larger and earlier than the summer crest. Wu To study the characteristic of TEC near the Tropic of et al. (2004) found there is a weak correlation between Cancer in Chinese zone, a few dual frequency GPS receiv- EIA and F10.7, and the seasonal variation of EIA is likely ers were established since 2005. There are 28 GPS satellites influenced by the seasonal variations of geomagnetic activ- orbiting the Earth at an inclination of 55°and at a height of ity (Dst) during the solar minimum by analyzing a short- 20,200 km. They broadcast information on two frequency term data set (September 1996 to August 1997). Wu et al. carrier signals, which are f1 (1575.42 MHz) and f2 (2008) studied ten years GPS data and suggested that the (1227.60 MHz), respectively. Ground-based GPS receiver geomagnetic effects (Kp) on the crest are short-term and could record constantly the pseudo-ranges (P1 and P2) solar effects (F10.7) are long-term. Many studies also have and the phases (L1 and L2) corresponding to the two sig- been carried out by other researchers in different country nals. In this work, we used these data to estimate the slant using the observational data recorded in different locations. total electron content (TECsl) in 30 s interval using the Various variation properties, the effects of solar and technique of calculating the VTEC developed by Ma and geomagnetic activities, and model comparative analysis Maruyama (2003). Since the slant TEC is the total number were reported by those works (Tsai et al., 2001; Rao, of electrons in a column of the unit cross section along the 2006; Bhuyan and Borah, 2007; Bagiya et al., 2009; Kumar ray path, it is desirable to calculate an equivalent vertical and Singh, 2009; Mukherjee et al., 2010). value of TEC, which is independent of the elevation of In our previous study (Liu et al., 2012) we were the first the ray path. To convert the slant TECsl to vertical TEC, time to analyze the temporal characteristic of VTEC using we assumed the ionosphere to be a thin screen shell model one-year data observed in Xiamen. We found the remark- and its center is assumed to be the same as that of the able seasonal anomaly of VTEC, and poor correlation with Earth. It is because the main contribution to TEC geomagnetic and solar activity. In this work, we extend the variations would occur around the height of the maximum data-set for two years and use three observational stations, ionization and this allows us to consider the ionosphere as including Xiamen site. We think the results in this paper a thin layer located at the height of ionosphere F2 layer.
Recommended publications
  • Doc.10100.Space Weather Manual FINAL DRAFT Version
    Doc 10100 Manual on Space Weather Information in Support of International Air Navigation Approved by the Secretary General and published under his authority First Edition – 2018 International Civil Aviation Organization TABLE OF CONTENTS Page Chapter 1. Introduction ..................................................................................................................................... 1-1 1.1 General ............................................................................................................................................... 1-1 1.2 Space weather indicators .................................................................................................................... 1-1 1.3 The hazards ........................................................................................................................................ 1-2 1.4 Space weather mitigation aspects ....................................................................................................... 1-3 1.5 Coordinating the response to a space weather event ......................................................................... 1-3 Chapter 2. Space Weather Phenomena and Aviation Operations ................................................................. 2-1 2.1 General ............................................................................................................................................... 2-1 2.2 Geomagnetic storms ..........................................................................................................................
    [Show full text]
  • National Space Weather Program Implementation Plan, 2Nd Edition, July 2000
    National Space Weather Program Implementation Plan, 2nd Edition, July 2000 http://www.ofcm.gov/ The National Space Weather Program The Implementation Plan 2nd Edition July 2000 National Space Weather Program Implementation Plan, 2nd Edition, July 2000 http://www.ofcm.gov/ NATIONAL SPACE WEATHER PROGRAM COUNCIL Mr. Samuel P. Williamson, Chairman Federal Coordinator Dr. David L. Evans Department of Commerce Colonel Michael A. Neyland, USAF Department of Defense Mr. Robert E. Waldron Department of Energy Mr. James F. Devine Department of the Interior Mr. David Whatley Department of Transportation Dr. Edward J. Weiler National Aeronautics and Space Administration Dr. Margaret S. Leinen National Science Foundation Lt Col Michael R. Babcock, USAF, Executive Secretary Office of the Federal Coordinator for Meteorological Services and Supporting Research National Space Weather Program Implementation Plan, 2nd Edition, July 2000 http://www.ofcm.gov/ NATIONAL SPACE WEATHER PROGRAM Implementation Plan 2nd Edition Prepared by the Committee for Space Weather for the National Space Weather Program Council Office of the Federal Coordinator for Meteorology FCM-P31-2000 Washington, DC July 2000 National Space Weather Program Implementation Plan, 2nd Edition, July 2000 http://www.ofcm.gov/ National Space Weather Program Implementation Plan, 2nd Edition, July 2000 http://www.ofcm.gov/ FOREWORD We are pleased to present this Second Edition of the National Space Weather Program Implementation Plan. We published the program's Strategic Plan in 1995 and the first Implementation Plan in 1997. In the intervening period, we have made tremendous progress toward our goals but much work remains to be accomplished to achieve our ultimate goal of providing the space weather observations, forecasts, and warnings needed by our Nation.
    [Show full text]
  • Where Is the Best Site on Earth? Domes A, B, C, and F, And
    Where is the best site on Earth? Saunders et al. 2009, PASP, 121, 976-992 Where is the best site on Earth? Domes A, B, C and F, and Ridges A and B Will Saunders1;2, Jon S. Lawrence1;2;3, John W.V. Storey1, Michael C.B. Ashley1 1School of Physics, University of New South Wales 2Anglo-Australian Observatory 3Macquarie University, New South Wales [email protected] Seiji Kato, Patrick Minnis, David M. Winker NASA Langley Research Center Guiping Liu Space Sciences Lab, University of California Berkeley Craig Kulesa Department of Astronomy and Steward Observatory, University of Arizona Saunders et al. 2009, PASP, 121 976992 Received 2009 May 26; accepted 2009 July 13; published 2009 August 20 ABSTRACT The Antarctic plateau contains the best sites on earth for many forms of astronomy, but none of the existing bases was selected with astronomy as the primary motivation. In this paper, we try to systematically compare the merits of potential observatory sites. We include South Pole, Domes A, C and F, and also Ridge B (running NE from Dome A), and what we call `Ridge A' (running SW from Dome A). Our analysis combines satellite data, published results and atmospheric models, to compare the boundary layer, weather, aurorae, airglow, precipitable water vapour, thermal sky emission, surface temperature, and the free atmosphere, at each site. We ¯nd that all Antarctic sites are likely to be compromised for optical work by airglow and aurorae. Of the sites with existing bases, Dome A is easily the best overall; but we ¯nd that Ridge A o®ers an even better site.
    [Show full text]
  • Response of the Total Electron Content at Brazilian Low Latitudes to Corotating Interaction Region and High‑Speed Streams During Solar Minimum 2008 Claudia M
    Candido et al. Earth, Planets and Space (2018) 70:104 https://doi.org/10.1186/s40623-018-0875-8 FULL PAPER Open Access Response of the total electron content at Brazilian low latitudes to corotating interaction region and high‑speed streams during solar minimum 2008 Claudia M. N. Candido1,2*, Inez S. Batista2, Virginia Klausner3, Patricia M. de Siqueira Negreti2, Fabio Becker‑Guedes2, Eurico R. de Paula2, Jiankui Shi1 and Emilia S. Correia2,4 Abstract In this work, we investigate the Brazilian low-latitude ionospheric response to two corotating interaction regions (CIRs) and high-speed streams (HSSs) events during the solar minimum of solar cycle 23, in 2008. The studied inter‑ vals are enclosed in the whole heliospheric interval, studied by other authors, for distinct longitudinal sectors. CIRs/ HSSs are structures commonly observed during the descending and low solar activity, and they are related to the occurrence of coronal holes. These events cause weak-to-moderate recurrent geomagnetic storms characterized by negative excursions of the interplanetary magnetic feld, IMF_Bz, as well as long-duration auroral activity, consid‑ ered as a favorable scenario for continuous prompt penetration interplanetary electric feld (PPEF). In this study, we used the vertical total electron content (VTEC) calculated from GPS receivers database from the Brazilian Continu‑ ous Monitoring Network managed by the Brazilian Institute of Geography and Statistics. Moreover, we analyzed the F-layer peak height, hmF2 and the critical plasma frequency, foF2, taken from a Digisonde installed at the southern crest of the equatorial ionization anomaly, in Cachoeira Paulista, CP. It was observed that during the CIRs/HSSs-driven geomagnetic disturbances VTEC increased more than 120% over the quiet times averaged values, which is compa‑ rable to intense geomagnetic storms.
    [Show full text]
  • Benchmark Geomagnetic Disturbance Event Description
    Benchmark Geomagnetic Disturbance Event Description Project 2013-03 GMD Mitigation Standard Drafting Team May 12, 2016 NERC | Report Title | Report Date 1 of 23 Table of Contents Preface ........................................................................................................................................................................3 Introduction ................................................................................................................................................................4 Background .............................................................................................................................................................4 General Characteristics ...........................................................................................................................................4 Benchmark GMD Event Description ...........................................................................................................................5 Reference Geoelectric Field Amplitude ..................................................................................................................5 Reference Geomagnetic Field Waveshape .............................................................................................................5 Appendix I – Technical Considerations .......................................................................................................................8 Statistical Considerations ........................................................................................................................................8
    [Show full text]
  • Solar and Geomagnetic Activity During March 1989 and Later Honths and Their Consequences at Earth and in Near-Earth Space
    SOLAR AND GEOMAGNETIC ACTIVITY DURING MARCH 1989 AND LATER HONTHS AND THEIR CONSEQUENCES AT EARTH AND IN NEAR-EARTH SPACE J. H. Allen (NOAA/NESDIS/NGDC) Spacecraft Charging Technology Conference Naval Postgraduate School, Monterey, California October 31-November 3, 1989 ABSTRACT From 6-20 March 1989 the large, complex sunspot group Region 5395 rotated across the visible disc of the Sun producing many large flares that bombdrded Earth with a variety of intense radiation although the energetic particle spectra were unusually "soft". Aurorae were observed worldwide at low latitudes. On 13/14 March a "Great" magnetic storm occurred for which Ap* = 279 and AA* = 450. By both measures, this event rates among the largest historical magnetic storms. Geostationary sate1 1 i tes became interpl anetary monitors when the magnetopause moved earthward of 6.5 Re. Ionospheric condi- ticns were extremely disturbed, affecting hf through X-band comnunications and the operation of satellites used for surveys and navigation. At lower altitudes there were problems with satellite drag and due to the large mag- netic field changes associated with field-a1 igned current sheets. We are seeking reports of satellite anomalies at all altitudes. Reports also have been received about effects of these Sol ar-Terrestria1 di sturbances on other technology at Earth and in near-Earth space. This presentation draws heavily on material in a shorter, summary paper "iri prgss" for "EOS" (Allen, et. al., 1989). Recent major solar activity since the abstract. was submitted happened in mid-August, late September, and mid-October 1989. These events and their consequences at Earth and in Space are covered briefly.
    [Show full text]
  • Improvement of Global Ionospheric TEC Derivation with Multi-Source Data in Modip Latitude
    atmosphere Article Improvement of Global Ionospheric TEC Derivation with Multi-Source Data in Modip Latitude Weizheng Fu 1,2 , Guanyi Ma 1,3,* , Weijun Lu 1,3 , Takashi Maruyama 4, Jinghua Li 1, Qingtao Wan 1, Jiangtao Fan 1 and Xiaolan Wang 1 1 National Astronomical Observatories, Chinese Academy of Sciences, Beijing 100101, China; [email protected] (W.F.); [email protected] (W.L.); [email protected] (J.L.); [email protected] (Q.W.); [email protected] (J.F.); [email protected] (X.W.). 2 Research Institute for Sustainable Humanosphere, Kyoto University, Uji, Kyoto 611-0011, Japan 3 School of Astronomy and Space Science, University of Chinese Academy of Sciences, Beijing 100049, China 4 National Institute of Information and Communications Technology, Tokyo 183-8795, Japan; [email protected] * Correspondence: [email protected] Abstract: Global ionospheric total electron content (TEC) is generally derived with ground-based Global Navigation Satellite System (GNSS) observations based on mathematical models in a solar- geomagnetic reference frame. However, ground-based observations are not well-distributed. There is a lack of observations over sparsely populated areas and vast oceans, where the accuracy of TEC derivation is reduced. Additionally, the modified dip (modip) latitude is more suitable than geomagnetic latitude for the ionosphere. This paper investigates the improvement of global TEC with multi-source data and modip latitude, and a simulation with International Reference Ionosphere (IRI) model is developed. Compared with using ground-based observations in geomagnetic latitude, the mean improvement was about 10.88% after the addition of space-based observations and the adoption Citation: Fu, W.; Ma, G.; Lu, W.; of modip latitude.
    [Show full text]
  • Spatial and Seasonal Effects on the Delayed Ionospheric Response to Solar EUV Changes
    Spatial and seasonal effects on the delayed ionospheric response to solar EUV changes Erik Schmölter1, Jens Berdermann1, Norbert Jakowski1, and Christoph Jacobi2 1German Aerospace Center, Kalkhorstweg 53, 17235 Neustrelitz, Germany 2Leipzig Institute for Meteorology, Universität Leipzig, Stephanstr. 3, 04103 Leipzig, Germany Correspondence: Erik Schmölter ([email protected]) Abstract. This study correlates different ionospheric parameters with the integrated solar EUV radiation to analyze the delayed ionospheric response, testing and improving upon previous studies on the ionospheric delay. Several time series of correlation coefficients and delays are presented to characterize the trend of the ionospheric delay from January 2011 to December 2013. The impact of the diurnal variations of ionospheric parameters in the analysis at an hourly resolution for fixed locations are 5 discussed and specified with calculations in different time scales and with comparison to solar and geomagnetic activity. An average delay for TEC of ≈ 18:7 hours and for foF2 of ≈ 18:6 hours is calculated at four European stations. The difference between northern and southern hemisphere is analyzed by comparisons with the Australian region. A seasonal variation of the delay between northern and southern hemisphere is calculated for TEC with ≈ 5 ± 0:7 hours and foF2 with ≈ 8 ± 0:8 hours. The latitudinal and longitudinal variability of the delay is analyzed for the European region, and found to be characterized by 10 a decrease in the delay from ≈ 21:5 hours at 30◦N to ≈ 19:0 hours at 70◦N for summer months. For winter months, a roughly constant delay of ≈ 19:5 hours is calculated. The results based on solar and ionospheric data at hourly resolution and the analysis of the delayed ionospheric response to solar EUV show the seasonal and latitudinal variations.
    [Show full text]
  • Interhemispheric Comparison of GPS Phase Scintillation at High Latitudes During the Magnetic-Cloud-Induced Geomagnetic Storm of 5–7 April 2010
    Ann. Geophys., 29, 2287–2304, 2011 www.ann-geophys.net/29/2287/2011/ Annales doi:10.5194/angeo-29-2287-2011 Geophysicae © Author(s) 2011. CC Attribution 3.0 License. Interhemispheric comparison of GPS phase scintillation at high latitudes during the magnetic-cloud-induced geomagnetic storm of 5–7 April 2010 P. Prikryl1, L. Spogli2, P. T. Jayachandran3, J. Kinrade4, C. N. Mitchell4, B. Ning5, G. Li5, P. J. Cilliers6, M. Terkildsen7, D. W. Danskin8, E. Spanswick9, E. Donovan9, A. T. Weatherwax10, W. A. Bristow11, L. Alfonsi2, G. De Franceschi2, V. Romano2, C. M. Ngwira6, and B. D. L. Opperman6 1Communications Research Centre Canada, Ottawa, ON, Canada 2Istituto Nazionale di Geofisica e Vulcanologia, Rome, Italy 3Physics Department, University of New Brunswick, Fredericton, NB, Canada 4Department of Electronic and Electrical Engineering, University of Bath, Bath, UK 5Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing, China 6South African National Space Agency, Hermanus, South Africa 7IPS Radio and Space Services, Bureau of Meteorology, Haymarket, NSW, Australia 8Geomagnetic Laboratory, Natural Resources Canada, ON, Canada 9Department of Physics and Astronomy, University of Calgary, AB, Canada 10Department of Physics and Astronomy, Siena College, Loudonville, NY, USA 11Geophysical Institute, University of Alaska Fairbanks, Fairbanks, AK, USA Received: 1 September 2011 – Revised: 2 December 2011 – Accepted: 9 December 2011 – Published: 21 December 2011 Abstract. Arrays of GPS Ionospheric Scintillation and TEC while it was significantly higher in Cambridge Bay (77.0◦ N; Monitors (GISTMs) are used in a comparative scintillation 310.1◦ E) than at Mario Zucchelli (80.0◦ S; 307.7◦ E). In the study focusing on quasi-conjugate pairs of GPS receivers in polar cap, when the interplanetary magnetic field (IMF) was the Arctic and Antarctic.
    [Show full text]
  • Prediction of Geomagnetically Induced Currents
    Ebihara et al. Earth, Planets and Space (2021) 73:163 https://doi.org/10.1186/s40623-021-01493-2 TECHNICAL REPORT Open Access Prediction of geomagnetically induced currents (GICs) fowing in Japanese power grid for Carrington-class magnetic storms Yusuke Ebihara1* , Shinichi Watari2 and Sandeep Kumar3 Abstract Large-amplitude geomagnetically induced currents (GICs) are the natural consequences of the solar–terrestrial con- nection triggered by solar eruptions. The threat of severe damage of power grids due to the GICs is a major concern, in particular, at high latitudes, but is not well understood as for low-latitude power grids. The purpose of this study is to evaluate the lower limit of the GICs that could fow in the Japanese power grid against a Carrington-class severe magnetic storm. On the basis of the geomagnetic disturbances (GMDs) observed at Colaba, India, during the Car- rington event in 1859, we calculated the geoelectric disturbances (GEDs) by a convolution theory, and calculated GICs fowing through transformers at 3 substations in the Japanese extra-high-voltage (500-kV) power grid by a linear combination of the GEDs. The estimated GEDs could reach ~ 2.5 V/km at Kakioka, and the GICs could reach, at least, 89 30 A near the storm maximum. These values are several times larger than those estimated for the 13–14 March 1989± storm (in which power blackout occurred in Canada), and the 29–31 October 2003 storm (in which power blackout occurred in Sweden). The GICs estimated here are the lower limits, and there is a probability of stronger GICs at other substations.
    [Show full text]
  • Introduction to Geomagnetic Fields
    INTRODUCTION TO GEOMAGNETIC FIELDS Second Edition WALLACE H. CAMPBELL PUBLISHED BY THE PRESS SYNDICATE OF THE UNIVERSITY OF CAMBRIDGE The Pitt Building, Trumpington Street, Cambridge, United Kingdom CAMBRIDGE UNIVERSITY PRESS The Edinburgh Building, Cambridge CB2 2RU, UK 40 West 20th Street, New York, NY 10011-4211, USA 477 Williamstown Road, Port Melbourne, VIC 3207, Australia Ruizde Alarc´on 13, 28014 Madrid, Spain Dock House, The Waterfront, Cape Town 8001, South Africa http://www.cambridge.org C Wallace H. Campbell 1997, 2003 This book is in copyright. Subject to statutory exception and to the provisions of relevant collective licensing agreements, no reproduction of any part may take place without the written permission of Cambridge University Press. First published 1997 Second edition 2003 Printed in the United Kingdom at the University Press, Cambridge Typefaces Times Roman 10/13 pt and Stone Sans System LATEX2ε [] A catalog record for this book is available from the British Library Library of Congress Cataloging in Publication data ISBN 0 521 82206 8 hardback ISBN 0 521 52953 0 paperback Contents Preface page ix Acknowledgements xii 1 The Earth’s main field 1 1.1 Introduction 1 1.2 Magnetic Components 4 1.3 Simple Dipole Field 8 1.4 Full Representation of the Main Field 15 1.5 Features of the Main Field 34 1.6 Charting the Field 41 1.7 Field Values for Modeling 47 1.8 Earth’s Interior as a Source 51 1.9 Paleomagnetism 58 1.10 Planetary Fields 62 1.11 Main Field Summary 63 1.12 Exercises 65 2 Quiet-time field variations and dynamo
    [Show full text]
  • Beidou Navigation Satellite System Signal in Space Interface Control Document Open Service Signal B2b (Version 1.0)
    China Satellite Navigation Office 2020 BeiDou Navigation Satellite System Signal In Space Interface Control Document Open Service Signal B2b (Version 1.0) China Satellite Navigation Office July, 2020 China Satellite Navigation Office 2020 TABLE OF CONTENTS 1 Statement ····························································································· 1 2 Scope ·································································································· 2 3 BDS Overview ······················································································· 3 3.1 Space Constellation ········································································· 3 3.2 Coordinate System ·········································································· 3 3.3 Time System ················································································· 4 4 Signal Characteristics ··············································································· 5 4.1 Signal Structure ·············································································· 5 4.2 Signal Modulation ··········································································· 5 4.3 Logic Levels ·················································································· 6 4.4 Signal Polarization ·········································································· 6 4.5 Carrier Phase Noise ········································································· 6 4.6 Spurious ·······················································································
    [Show full text]