The Control and Generation of Magnetic Pulsations on the Ground and in Interplanetary Space by Parameters of the Solar Wind

Total Page:16

File Type:pdf, Size:1020Kb

The Control and Generation of Magnetic Pulsations on the Ground and in Interplanetary Space by Parameters of the Solar Wind -1- THE CONTROL AND GENERATION OF MAGNETIC PULSATIONS ON THE GROUND AND IN INTERPLANETARY SPACE BY PARAMETERS OF THE SOLAR WIND Timothy Joab Odera Doctor of Philosophy University of Edinburgh 1982 S ;. N 0Cb -11- DECLARATION I hereby declare that the work presented in this thesis is my own and has not been presented for a degree in any other University; and that the thesis has been composed by myself. -111- ABSTRACT There is evidence to suggest that some Pc 3, 4 pulsations are controlled by solar wind parameters. The waves have been thought to originate as low- frequency waves generated within the solar wind. Data from five ground stations and the ISEE-2 satellite have been used in an investigation ofthe problems of the control by solar wind parameters of the generation of low-frequency (10 - 80 mHz) waves in the solar wind and their relationship to Pc 3, 4 pulsations on the ground. The five ground stations form part of the IGS array of rubidium magnetometers operated during the Inter- national Magnetospheric Studies (ThIS). The ground data have been correlated with the 7`-hourly values of the solar wind velocity (Vu), the IMF magnitude (B) and the IMF cone angle ®B• Results from statistical analysis of the ground data indicate that (a) the energy level of Pc 3, 4 pulsations on the ground increases with the increase in swV (b) the energy level rises with the decrease in 0 x (c) the Pc 3 pulsation is better related to the IMF cone angle than the Pc 4 pulsation and (d) the frequency of Pc 3, 14 pulsations depends on the IMF magnitude. The quality of the last relationship is found to be improved when the same frequency of Pc 3, 14 activity is observed over a large area of the Earth's surface. Data from the ISEE-2 satellite have been used to study the characteristics of low-frequency upstream waves. Three classes of waves have been identified. These are (a) continuous pulsations similar in type to Pc, (b) quasi- periodic incoherent oscillations, distinguished by mixed period fluctuations which often last for several hours, and (c) relatively isolated wave 'bundles'. - iv- The upstream waves are observed preferentially when the IMF direction is sunwards, and the waves are 145 0 found to be most common when the cone angle is 150 - For a set of selected events the dependence of the frequency of the upstream waves on the IMF magnitude has been tested, and a functional relationship F = C O + C 1 B, between their frequency and the IMF magnitude has been found to be a statistically better fit to the data than the form F = CB which is in common use. The upstream waves aboard the ISEE-2 spacecraft and the Pc 3, 14 pulsations recorded simultaneously on the ground stations CL = 1.8 - 14.3) have been compared. It is found that similarity of the spectra of the waves in the solar wind and the ground is very rare and that correspondence between the events in space and on the ground is extremely low. It is implied that the pulsations in the two media are generated by two different mechanisms. It is concluded that both satellite and ground pulsations are influenced by the parameters of the solar wind; but. that the waves in the solar wind are not transmitted through the magnetosheath and magnetosphere directly to appear as Pc 3, 14 pulsations observed on the ground. -v- LIST OF CONTENTS Page Title page i Declaration Abstract List of contents v List of tables ix List of captions xi CHAPTER 1 GENERAL INTRODUCTORY NOTES 1 1:1 Introduction 1 1:2 Importance of geomagnetic pulsations 2 1:3 This work 1:1 Geomagnetic pulsations 6 1:4-1 Definition 6 1:1-2 Short historical notes 8 1:14-3 Classification of geomagnetic pulsations 9 CHAPTER 2 THEORETICAL BACKGROUND 13 2:1 Solar wind and Magnetosphere 13 2:1-1 Introduction 13 2:1-2 The solar wind 13 2:1-3 Interplanetary magnetic field (IMF) 114 2:1-14 The magnetosphere and its boundaries 15 2:1-5 The dynamics of the magnetosphere 21 2:2 Origin and transmission of micro- pulsations 23 2:2-1 Introduction 23 2:2-2 Hydromagnetic waves 26 2:2-3 Simplified solutions of the hydro- magnetic equations 32 2:2-14 Generation mechanisms for micro- pulsations 314 2:2-5 Field line resonance 36 Me Page 2:2-6 Solar wind irregularities 141 2:2-7 Wave-particles interactions: plasma instabilities 142 2:2-8 Others 1414 2:2-9 Inospheric and atmospheric trans- mission 1411 CHAPTER 3 OBSERVATIONAL BACKGROUND 1.7 3:1 Solar wind controlled pulsations 147 3:1-1 Introduction 147 3:1-2 Period of Pc 3, 11 pulsations 147 3:1-3 Occurrence and/or amplitude of pulsations 53 3:1-li. Models for solar wind control of Pc 3, ii. pulsations 63 3:2 Observations of Pc 3, 14 in the UK 71 CHAPTER 14 CONTROL OF THE SOLAR WIND PARAMETERS ON THE GROUND Pc 3, 14 PULSATIONS 83 14:1 Introduction 83 )4:2 Data 81.. 14:2-1 Ground data 81.. )4:2-2 Satellite data 90 Analysis and Results 101 li.:3-1 Inter-relation of V , Q and B 101 5W xB 14: 3 General distribution of V , B, -2 sw e xB 106 4:3-3 Geomagnetic pulsations occurrence and variation with local time 107 4:3- 4 Effect of solar wind velocity 109 1i.:3-5 Effect of IMF cone angle 12 14 11:3-6 Effect of IMF magnitude on the frequency of Pc 3, 11 pulsations 151 -vii- Page CHAPTER 5 LOW-FREQUENCY WAVES IN THE INTERPLANETARY MEDIUM 171 5:1 Introduction 171 5:2 Interplanetary magnetic field data selection and processing 178 5:2-1 Introduction 178 5:2-2 Selection procedure 179 5:3 Results 181 5:3-1 Classification of waves in the IMP 181 5:3-2 Period and amplitude of waves in the IMP 188 5:3- 3 Effects of IMP orientation 192 5:3-4 Spectral character of IMP waves 203 CHAPTER 6 CORRELATION OF GROUND AND SATELLITE PULSATIONS 225 6:1 Introduction 225 6:2 Direct comparison 232 6:2-1 High latitude station 232 6:2-2 Mid-latitude station 249 6:3 Statistical comparison 266 CHAPTER 7 SUMMARY, DISCUSSIONS, INTERPRETATIONS AND CONCLUSIONS 271 7:1 Scatter in the E - Vsw relation 271 7:2 Limitation of the use of the cone angle, 274 9x 7:3 Low-frequency waves in the solar wind: summary and discussions 277 7:4 Derived relations, F - B in space and on the ground 292 7:5 Interplanetary origin of Pc 3, it pulsations 294 7:6 What model? 301 -viii - Page 7:7 Summary and conclusions 307 7:8 Suggestions for further work 311 APPENDIX Al 311 ACKNOWLEDGEMENTS 315 REPERECNES 317 -ix- Tables Page 1:1 Periods of geomagnetic variations. 7 1:2 Period ranges of pulsations. 12 3:1 Locations of observations used in the studies of pulsations and solar wind, and quantities that were correlated. 14:1 Recording stations locations. S. 14:2 Orbital parameters of ISEE-2 satellite for different epoch. 01 14:3 Summary: Intreiation of the solar wind parameters. 1014 14:14 Correlation coefficients of the solar wind parameters. 105 11:5 Summary of the EVsw relation. 123 11:6 Summary of the cone angle effect on the pulsation energy. 150 24:7 Summary of the F - B relation of the Pc 3, 14 pulsations on the ground. 159 14:8 Pc 3 regression results. 161 11:9 Regression results of simultaneous events. 1614 5:1 Statistics of Sunward/Antisunward. ThIF in relation to the presence of pulsations in the interplanetary medium. 197 -x- Tables Page 5:2 Summary of result of regression analysis. 218 5:3 Significance test of the slopes and intercepts of the regression lines for the F - B relation. 222 5:11 Significance test: Regression lines forced through origin. 223 7:1 Number of data points. 7:2 Observational relations between solar wind parameters and Pc 3, 4 pulsations. 309 -xi- FIGURE CAPTIONS Figure Caption Page 2:1 The lines of force of the quiet-day inter- planetary magnetic field resulting from extension of the general solar field by an idealized uniform 300 km/sec quiet day solar wind directions (adapted from Parker, 1963). 16 2:2 Schematic view of the magnetosphere in the noon- midnight magnetic meridian, plane (Ness, 1967). 18 2:3 Model of the magnetosphere according to Heikkila (1973). 19 2:4 The symmetry relations at magnetically conju- gate points for oscillation of the lines of magnetic force. H, horizontal component; D, east declination (Sugiura and Wilson, 19614). 33 2:5 Schematic diagram of variation of amplitude and polarization as a function of L for unstable surface wave on the magnetopause coupled to a resonant field line. 39 2:6 Variation of low frequency micropulsation polarization as a function of local time and latitude (Samson et al., 1971). Amplitude is maximum at the lower latitude point (line AB) where polarization changes. 39 3:1 Average interplanetary magnetic field magnitude versus period of magnetic pulsations seen at a mid-latitude observatory (Troitskaya et al., 1972). 49 Figure Caption Page 3:2 Two- versions of the observational results relating the IMF magnitude (B) to the period (T) of daytime pulsations. The curves are drawn from T = 160/B. 0 50 3:3 Histograms of the occurrence of interplanetary field strengths for each level of the Borok-B- index (Russell and Fleming, 1976).
Recommended publications
  • An Abstract of the Dissertation Of
    AN ABSTRACT OF THE DISSERTATION OF Benjamin S. Murphy for the degree of Doctor of Philosophy in Geology presented on May 28, 2019. Title: Magnetotelluric Constraints on Lithospheric Properties in the Southeastern United States Abstract approved: _______________________________________________________ Gary D. Egbert By inverting EarthScope long-period magnetotelluric (MT) data from the southeastern United States (SEUS), we obtain electrical conductivity images that provides key insights into the geodynamics of this region. Significantly, we resolve a highly electrically resistive block that extends to mantle depths beneath the modern Piedmont and Coastal Plain physiographic provinces. As high resistivity values in mantle minerals require cold mantle temperatures, the MT data indicate that the sub- Piedmont thermal lithosphere must extend to greater than 200 km depth. This firm bound appears to conflict with conclusions from seismic results; tomography shows that velocities in this region are generally slightly slow with respect to references models. This observation has led to a seismically-informed view of relatively thin (<150 km), eroded thermal lithosphere beneath the SEUS. However, resolution tests demonstrate that our MT constraints are robust. Furthermore, narrow-band biases in MT transfer functions from the SEUS due to geomagnetic pulsations associated with field-line resonances support the presence of bulk resistive lithosphere in this region. We show that, by considering anelastic prediction of seismic observables, MT and seismic (tomography, attenuation, receiver function) results are in fact consistent with thick (~200 km), coherent thermal lithosphere in this region. Our results demonstrate the danger of interpreting seismic results purely in terms of reference models and the importance of integrating different geophysical techniques when formulating geodynamic interpretations.
    [Show full text]
  • Preseismic ULF Electromagnetic Effect from Observation at Kamchatka
    Natural Hazards and Earth System Sciences (2003) 3: 203–209 c European Geosciences Union 2003 Natural Hazards and Earth System Sciences Preseismic ULF electromagnetic effect from observation at Kamchatka O. Molchanov1, A. Schekotov1, E. Fedorov1, G. Belyaev1, and E. Gordeev2 1Institute of the Physics of the Earth, Moscow, Russia 2Institute of Geophysical Survey, Petropavlovsk-Kamchatski, Russia Received: 28 May 2002 – Revised: 30 September 2002 – Accepted: 7 October 2002 Abstract. Some results of ULF magnetic field observation level after EQ. They found the most clear effect in the fre- at Karimshino site (Kamchatka, Russia) since June 2000 to quency band F = 0.01 − 0.1 Hz. Molchanov et al. (1992), September 2001 are presented here. Using case study we Kopytenko et al. (1993) observed ULF variation at distance have found an effect of suppression of ULF intensity about 130 km from the EQ epicenter and noted only last stage of 2–6 days before rather strong and nearby seismic shocks the process: increase of ULF intensity in time period from (magnitude M = 4.0 − 6.2). It is revealed for nighttime 3 h before to several days after EQ. and horizontal component of ULF field (G) in the frequency range 0.01 − 0.1 Hz. Then we prove the reliability of the Next researches on this subject were mainly produced in effect by computed correlation between G (or 1/G) and spe- Japan. Hayakawa et al. (1996a) reported results of obser- cially calculated seismic indexes K for the whole period vation the ULF magnetic field variations before great EQ at s = of observation.
    [Show full text]
  • Book of Abstracts
    St. Petersburg State University St. Petersburg Branch of the EurAsian Geophysical Society 10th International Conference \PROBLEMS OF GEOCOSMOS" Book of Abstracts St. Petersburg, Petrodvorets, October 6{10, 2014 Supported by Russian Foundation of Basic Research St. Petersburg 2014 Programme Committee Prof. V. N. Troyan Chairman, St.Petersburg University Prof. H. K. Biernat Space Research Institute, Austria Dr. N. V. Erkaev Institute of Computational Modelling SB RAS, Russia Prof. M. Hayakawa University of Electro-Com- munications, Tokyo, Japan Prof. B. M. Kashtan St.Petersburg University Prof. Yu. A. Kopytenko SPbF IZMIRAN, Russia Prof. A. A. Kovtun St.Petersburg University Dr. I. N. Petrov St.Petersburg University Prof. V. S. Semenov St.Petersburg University Prof. V. A. Sergeev St.Petersburg University Dr. N. A. Smirnova St.Petersburg University Dr. N. A. Tsyganenko St.Petersburg University Dr. E. Turunen Sodankyl¨aGeophysical Observatory, Finland Dr. I. G. Usoskin University of Oulu, Finland Prof. T. B. Yanovskaya St.Petersburg University Organizing Committee S. V. Apatenkov N. Yu. Bobrov V. V. Karpinsky A. A. Kosterov M. V. Kholeva M. V. Kubyshkina T. A. Kudryavtseva E. L. Lyskova N. P. Legenkova I. A. Mironova A. A. Samsonov E. S. Sergienko R. V. Smirnova ISBN 978-5-98340-334-5 Contents Section C. Conductivity of the Earth . 5 Section P. Paleomagnetism and Rock Magnetism . 34 Section S. Seismology . 84 Section SEMP. Seismo-ElectroMagnetic Phenomena . 106 Section STP. Solar-Terrestrial Physics . 125 Author index . 215 3 4 Section C. Conductivity of the Earth Geoelectrical and geothermal models of the Pripyat Trough Astapenko, V.N. (State Enterprise \RPCG", Minsk, Belarus), Lev- ashkevich, V.G.(National Academy of Sciences of Belarus) and Logvi- nov, I.M.( Institute of Geophysics NAS of Ukraine, Kiev, Ukraine) Pripyat Trough is a part of regional Palaeozoic { Phanerozoics Pripyat { Dnieper { Donets Palaeorift.
    [Show full text]
  • Appraisal of Electromagnetic Induction Effects on Magnetic Pulsation Studies
    c Annales Geophysicae (2001) 19: 171–178 European Geophysical Society 2001 Annales Geophysicae Appraisal of electromagnetic induction effects on magnetic pulsation studies B. R. Arora1, P. B. V. Subba Rao1, N. B. Trivedi2, A. L. Padilha3, and I. Vitorello3 1Indian Institute of Geomagnetism, Colaba, Mumbai 400 005, India 2Southern Regional Center for Space Research - CRSPE LACESM/CT/UFSM, Santa Maria, RS 97119–900 Brazil 3Instituto Nacional de Pesquisas Espaciais, Sao Jose dos Campos, SP 12201–970, Brazil Received: 12 July 2000 – Revised: 25 October 2000 – Accepted: 28 November 2000 Abstract. The quantification of wave polarization character- tospheric processes, in general, and to understand the gener- istics of ULF waves from the geomagnetic field variations ation and propagation mechanisms of ULF waves, in partic- is done under ‘a priori’ assumption that fields of internal in- ular (Hughes, 1994). In such studies, determination of wave duced currents are in-phase with the external inducing fields. polarization parameters (ellipticity, degree and sense of po- Such approximation is invalidated in the regions marked by larization, azimuth and phase etc.) from the recorded geo- large lateral conductivity variations that perturb the flow pat- magnetic variations, inevitably form the first step. In all fre- tern of induced currents. The amplitude and phase changes quency ranges, the geomagnetic field variations are the vec- that these perturbations produce, in the resultant fields at tor sum of the contributions from the external (source) cur- the Earth’s surface, make determination of polarization and rent system in the ionosphere/magnetosphere and their coun- phase of the oscillating external signals problematic.
    [Show full text]
  • Scientific Program
    IUGG XXIV GENERAL ASSEMBLY Perugia, July 2-13, 2007 02 July, 2007 J. Taylor, Matt J. Bailey, Natalia Solorzano, Thomas Jeremy, Robert H. 02:16 pm Geophysical survey of the Fagnano pluton. Tierra del UL001 Our Changing Climate: A Global Policy Issue, Holzworth, Steven Cummer, Nicolas Jaugey, Osmar Pinto, Nelson J. Schuch, Fuego. Argentina Robert W. Corell: Invited Speacher Marcos Michels, Vinicius T. Rampinelli. Speaker Sao Sabbas Fernanda Vilas Juan Francisco, Tassone A., Peroni J. I., Lippai H., Oral 2 July, 2007 from 08:30 AM to 09:30 AM - Rectorate Main Hall 12:15 pm Investigating Sprite Halo Optical Signatures and Menichetti M, Lodolo E. Speaker Vilas Juan Francisco US001 Our Changing Planet (Part 1) Associated Lightning Characteristics over South America Conveners: Peltier Richard Taylor Michael, S. Cummer, J. Li, F. Sao Sabbas, J. Thomas, 02:32 pm Paleomagnetism of Late Tertiary lava flows from Oral 2 July, 2007 from 09:30 AM to 12:30 AM - Rectorate Main Hall R. Holzworth, O. Pinto, N. Schuch. Speaker Taylor Michael Lundarhals, Storutjarnir, and Su durdalur, Iceland 09:30 am Solar Forcing Of Global Climate Over The Instrumental Era Oral 2 July, 2007 from 02:00 PM to 05:30 PM - Department of Physics Kono Masaru. Speaker Kono Masaru Lean Judith. Speaker Lean Judith Room B 02:48 pm Break-up of Pangea and early Mesozoic plate motions in 09:55 am Monitoring the Variability in the Atlantic Meridional 02:00 pm Balloon electric field measurements in the vicinity of an the central Atlantic, Atlas and Tethys regions Overturning Circulation at 25_N active convective storm Schettino Antonio, Eugenio Turco.
    [Show full text]
  • Background Electromagnetic Noise Characterization: the Role of External and Internal Earth Sources Antonio Meloni, Cesidio Bianchi*, Giuliana Mele, Paolo Palangio
    ANNALS OF GEOPHYSICS, 58, 3, 2015, G0330; doi:10.4401/ag-6745 Background electromagnetic noise characterization: the role of external and internal Earth sources Antonio Meloni, Cesidio Bianchi*, Giuliana Mele, Paolo Palangio Istituto Nazionale di Geofisica e Vulcanologia, Rome, Italy Article history Received January 29, 2015; accepted June 9, 2015. Subject classification: Radio noise characterization, Ionosphere-magnetosphere, Background EM noise, Crustal/lithospheric EM sources. ABSTRACT but they can also be generated inside the cavity, for ex- The Earth is surrounded by the ionosphere and magnetosphere that can ample by energetic particles acting as forcing mecha- roughly be seen schematically as two concentric shells. These two com- nisms that perturb and modify the ionospheric and posed and inhomogeneous structured shells around the Earth selectively magnetospheric configuration. The EM Power Spectral affect electromagnetic (EM) waves propagation. Both ionosphere and Density (PSD) at the Earth’s surface was deeply stud- magnetosphere interact also with particles and waves coming from ex- ied and reported since the first extensive measurements ternal sources, generating electromagnetic phenomena that in turn might were available, as discussed for example by Lanzerotti become sources of EM waves. Conversely, EM waves generated inside the [1978] and Lanzerotti et al. [1990]. The most intensive ionosphere remain confined at various altitudes in this region, up to a so- near Earth’s sources are associated with the atmos- called critical frequency limit, depending on frequency, EM waves can es- pheric electrical activity, while the external sources cape out of the ionosphere and magnetosphere or get through. The EM mainly originate on the Sun. Relevant information about waves generated inside the magnetospheric cavity mainly originate as a the external EM noise can be found in the CCIR/ITU result of the electrical activity in the atmosphere.
    [Show full text]
  • Geophysical Abstracts 190 July-September 1962
    Geophysical Abstracts 190 July-September 1962 By JAMES W. CLARKE, DOROTHY B. VITALIANO, VIRGINIA S. NEUSCHEL, and others GEOLOGICAL SURVEY BULLETIN 1166-C Abstracts of current literature pertaining to the physics of the solid earth and to geophysical exploration UNITED STATES GOVERNMENT PRINTING OFFICE, WASHINGTON : 1962 UNITED STATES DEPARTMENT OF THE INTERIOR STEWART L. UDALL, Secretary GEOLOGICAL SURVEY Thomas B. Nolan, Director For sale by the Superintendent of Documents, U.S. Government Printing Office, Washington 25, D.C. Price 40 cents (single copy). Subscription price: $1.75ayear; 50 cents additional for foreign mailing. Use of funds for printing this publication has been approved by the Director of the Bureau of the Budget (March 14, 1962). CONTENTS Page Introduction--------------------------------------------------- 317 Extent of coverage ------------------------------------------ 317 List of journals --------------------------------------------- 317 Form of citation -------------------------------------------- 318 Abstracters ------------------------------------------------ 318 Age determinations -------------------------------------------- 318 Cosmogony --------------------------------------------------- 328 Earth currents ------------------------------------------------ 337 Earthquakes and earthquake waves ------------------------------ 339 Earth tides and related phenomena ------------------------------ 347 Elasticity----------------------------------------------------- 348 Electrical exploration------------------------------------------
    [Show full text]
  • Geomagnetic Observations for Main Field Studies: from Ground to Space
    Space Sci Rev DOI 10.1007/s11214-010-9693-4 Geomagnetic Observations for Main Field Studies: From Ground to Space J. Matzka · A. Chulliat · M. Mandea · C.C. Finlay · E. Qamili Received: 12 February 2010 / Accepted: 30 August 2010 © Springer Science+Business Media B.V. 2010 Abstract Direct measurements of the geomagnetic field have been made for more than 400 years, beginning with individual determinations of the angle between geographic and magnetic North. This was followed by the start of continuous time series of full vector measurements at geomagnetic observatories and the beginning of geomagnetic repeat sta- tions surveys in the 19th century. In the second half of the 20th century, true global coverage with geomagnetic field measurements was accomplished by magnetometer payloads on low- Earth-orbiting satellites. This article describes the procedures and instruments for magnetic field measurements on ground and in space and covers geomagnetic observatories, repeat J. Matzka () DTU Space, Technical University of Denmark, Juliane Maries vej 30, 2100 Copenhagen, Denmark e-mail: [email protected] A. Chulliat Equipe de Géomagnétisme, Institut de Physique du Globe de Paris, Université Paris-Diderot, INSU/CNRS, 4 Place Jussieu, 75005 Paris, France M. Mandea Helmholtz-Zentrum Potsdam Deutsches GeoForschungsZentrum, Telegrafenberg, 14473 Potsdam, Germany Present address: M. Mandea Institut de Physique du Globe de Paris—IPGP, Université Paris-Diderot & CNRS, 5 rue Thomas Mann, 75205 Paris Cedex 13, France C.C. Finlay Institut für Geophysik, ETH Zürich, Sonneggstr. 5, 8092 Zürich, Switzerland E. Qamili Istituto Nazionale di Geofisica e Vulcanologia, Sezione di Roma 2, Via di Vigna Murata 605, 00143 Roma, Italy E.
    [Show full text]
  • THE NATIQNAL GEOMAGNETIC INITIATIVE (NAS-NRC) Unclas Z60 P
    N94-23344 (LC-93-B5739) THE NATIQNAL GEOMAGNETIC INITIATIVE (NAS-NRC) unclas Z60 p 0198598 a _ J THE NATIONAL G OMAGNETIC INITIATIVE U.S. Geodynamics Committee Board on Earth Sciences and Resources Commission on Geosciences, Environment, and Resources National Research Council NATIONAL ACADEMY PRESS Washington, D.C. 1993 NOTICE: The project that is the subject of this report was approved by the Governing Board of the National Research Council, whose members are drawn from the councils of the National Academy of Sciences, the National Academy of Engineering, and the Institute of Medicine. The members of the committee responsible for the report were chosen for their special competences and with regard for appropriate balance. This report has been reviewed by a group other than the authors according to procedures approved by a Report Review Committee consisting of members of the National Academy of Sciences, the National Academy of Engineering, and the Institute of Medicine. Support for this study was provided by the National Aeronautics and Space Administration, National Oceanic and Atmospheric Administration, National Science Foundation, U.S. Air Force, U.S. Department of Energy, and U.S. Geological Survey. Library of Congress Catalog Card No. 93-85739 International Standard Book Number 0-309-04977-6 Copies of this report are available from: National Academy Press 2101 Constitution Avenue, N.W. Washington, D.C. 20418 800-624-6242 202-334-3313 (in the Washington Metropolitan Area) B-201 Cover art by Shelley Myers, Project Assistant for the U.S. Geodynamics Committee, Board on Earth Sciences and Resources, National Research Council. Myers' work is exhibited widely in the Washington, D.C.
    [Show full text]
  • C. Constable, Earth's Electromagnetic Environment
    Surv Geophys (2016) 37:27–45 DOI 10.1007/s10712-015-9351-1 Earth’s Electromagnetic Environment Catherine Constable1 Received: 28 April 2015 / Accepted: 17 November 2015 / Published online: 1 December 2015 Ó Springer Science+Business Media Dordrecht 2015 Abstract The natural spectrum of electromagnetic variations surrounding Earth extends across an enormous frequency range and is controlled by diverse physical processes. Electromagnetic (EM) induction studies make use of external field variations with fre- quencies ranging from the solar cycle which has been used for geomagnetic depth sounding through the 10À4–104 Hz frequency band widely used for magnetotelluric and audio-magnetotelluric studies. Above 104 Hz, the EM spectrum is dominated by man- made signals. This review emphasizes electromagnetic sources at 1 Hz and higher, describing major differences in physical origin and structure of short- and long-period signals. The essential role of Earth’s internal magnetic field in defining the magnetosphere through its interactions with the solar wind and interplanetary magnetic field is briefly outlined. At its lower boundary, the magnetosphere is engaged in two-way interactions with the underlying ionosphere and neutral atmosphere. Extremely low-frequency (3 Hz– 3 kHz) electromagnetic signals are generated in the form of sferics, lightning, and whis- tlers which can extend to frequencies as high as the VLF range (3–30 kHz).The roughly spherical dielectric cavity bounded by the ground and the ionosphere produces the Schumann resonance at around 8 Hz and its harmonics. A transverse resonance also occurs at 1.7–2.0 kHz arising from reflection off the variable height lower boundary of the ionosphere and exhibiting line splitting due to three-dimensional structure.
    [Show full text]
  • Seismo-Geomagnetic Pulsations Triggered by Rayleigh Waves of the 11 March 2011 M 9.0 Tohoku-Oki Earthquake
    Terr. Atmos. Ocean. Sci., Vol. 26, No. 2, Part I, 95-101, April 2015 doi: 10.3319/TAO.2014.10.09.01(T) Seismo-Geomagnetic Pulsations Triggered by Rayleigh Waves of the 11 March 2011 M 9.0 Tohoku-Oki Earthquake Horng-Yuan Yen1, *, Chun-Rong Chen1, Yu-Tsung Lo1, Tzay-Chyn Shin 2, and Qi Li 3 1 Department of Earth Sciences, National Central University, Jhongli City, Taiwan, R.O.C. 2 Central Weather Bureau, Taipei, Taiwan, R.O.C. 3 Institute of Geophysics, China Earthquake Administration, Beijing, China, P.R.C. Received 4 March 2014, revised 6 October 2014, accepted 9 October 2014 ABSTRACT This study reports on geomagnetic pulsations excited by traveling Rayleigh waves. The geomagnetic total intensity fields recorded using 12 magnetometers are utilized to examine seismo-magnetic pulsations induced by the 2011 M 9.0 Tohoku-oki earthquake. Geomagnetic data and seismograms from 4 co-located seismometers are examined and cross-compared to deter- mine whether magnetic variations result changes in space weather or traveling Rayleigh waves. A 150 - 250 s band-pass filter was adopted to determine the arrival times and amplitudes of the seismo-magnetic pulsations. Seismo-magnetic pulsations with pronounced periods of about 200 s and amplitudes of 0.2 - 1.2 nT appear at distances ranging from 190 - 4600 km from the epicenter. Pulse speed of 3.8 km s-1 estimated from the epicentral distances and arrival times indicates that the seismo-mag- netic pulsations were induced by Rayleigh waves produced by the Tohoku-oki earthquake. The seismo-magnetic pulsations constantly lag seismic wave pulses by about 6.3 minutes, confirming that ionospheric conductivity affects magnetic fields.
    [Show full text]