Jump to content

Schumann resonances

From Wikipedia, the free encyclopedia

This is an old revision of this page, as edited by OAbot (talk | contribs) at 06:39, 31 December 2020 (Open access bot: doi added to citation with #oabot.). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

Diagram of Schumann resonances in Earth's atmosphere

The Schumann resonances (SR) are a set of spectrum peaks in the extremely low frequency (ELF) portion of the Earth's electromagnetic field spectrum. Schumann resonances are global electromagnetic resonances, generated and excited by lightning discharges in the cavity formed by the Earth's surface and the ionosphere.[1]

Description

This global electromagnetic resonance phenomenon is named after physicist Winfried Otto Schumann who predicted it mathematically in 1952. Schumann resonances occur because the space between the surface of the Earth and the conductive ionosphere acts as a closed waveguide. The limited dimensions of the Earth cause this waveguide to act as a resonant cavity for electromagnetic waves in the ELF band. The cavity is naturally excited by electric currents in lightning. Schumann resonances are the principal background in the part of the electromagnetic spectrum[2] from 3 Hz through 60 Hz,[3] and appear as distinct peaks at extremely low frequencies (ELF) around 7.83 Hz (fundamental),[4] 14.3, 20.8, 27.3 and 33.8 Hz.[5]

In the normal mode descriptions of Schumann resonances, the fundamental mode is a standing wave in the Earth–ionosphere cavity with a wavelength equal to the circumference of the Earth. The lowest-frequency mode has highest intensity, and the frequency of all modes can vary slightly owing to solar-induced perturbations to the ionosphere (which compress the upper wall of the closed cavity)[citation needed] amongst other factors. The higher resonance modes are spaced at approximately 6.5 Hz intervals (as may be seen by feeding numbers into the formula), a characteristic attributed to the atmosphere's spherical geometry. The peaks exhibit a spectral width of approximately 20% on account of the damping of the respective modes in the dissipative cavity.

Observations of Schumann resonances have been used to track global lightning activity. Owing to the connection between lightning activity and the Earth's climate it has been suggested that they may also be used to monitor global temperature variations and variations of water vapor in the upper troposphere. It has been speculated that extraterrestrial lightning (on other planets) may also be detected and studied by means of their Schumann resonance signatures. Schumann resonances have been used to study the lower ionosphere on Earth and it has been suggested as one way to explore the lower ionosphere on celestial bodies. Effects on Schumann resonances have been reported following geomagnetic and ionospheric disturbances. More recently, discrete Schumann resonance excitations have been linked to transient luminous events—sprites, ELVES, jets, and other upper-atmospheric lightning.[citation needed] A new field of interest using Schumann resonances is related to short-term earthquake prediction.[citation needed] Interest in Schumann resonances was renewed in 1993 when E. R. Williams showed a correlation between the resonance frequency and tropical air temperatures, suggesting the resonance could be used to monitor global warming.[6][7] In geophysical survey, Schumann resonances are used to locate offshore hydrocarbon deposits.[8][page needed]

History

In 1893, George Francis FitzGerald noted that the upper layers of the atmosphere must be fairly good conductors. Assuming that the height of these layers is about 100 km above ground, he estimated that oscillations (in this case the lowest mode of the Schumann resonances) would have a period of 0.1 second.[9] Because of this contribution, it has been suggested to rename these resonances "Schumann–FitzGerald resonances".[10] However FitzGerald's findings were not widely known as they were only presented at a meeting of the British Association for the Advancement of Science, followed by a brief mention in a column in Nature.

Hence first suggestion that an ionosphere existed, capable of trapping electromagnetic waves, is attributed to Heaviside and Kennelly (1902).[11][12] It took another twenty years before Edward Appleton and Barnett in 1925[13] were able to prove experimentally the existence of the ionosphere.

Although some of the most important mathematical tools for dealing with spherical waveguides were developed by G. N. Watson in 1918,[14] it was Winfried Otto Schumann who first studied the theoretical aspects of the global resonances of the earth–ionosphere waveguide system, known today as the Schumann resonances. In 1952–1954 Schumann, together with H. L. König, attempted to measure the resonant frequencies.[15][16][17][18] However, it was not until measurements made by Balser and Wagner in 1960–1963[19][20][21][22][23] that adequate analysis techniques were available to extract the resonance information from the background noise. Since then there has been an increasing interest in Schumann resonances in a wide variety of fields.

Basic theory

Lightning discharges are considered to be the primary natural source of Schumann resonance excitation; lightning channels behave like huge antennas that radiate electromagnetic energy at frequencies below about 100 kHz.[24] These signals are very weak at large distances from the lightning source, but the Earth–ionosphere waveguide behaves like a resonator at ELF frequencies and amplifies the spectral signals from lightning at the resonance frequencies.[24]

In an ideal cavity, the resonant frequency of the -th mode is determined by the Earth radius and the speed of light .[15]

The real Earth–ionosphere waveguide is not a perfect electromagnetic resonant cavity. Losses due to finite ionosphere electrical conductivity lower the propagation speed of electromagnetic signals in the cavity, resulting in a resonance frequency that is lower than would be expected in an ideal case, and the observed peaks are wide. In addition, there are a number of horizontal asymmetries—day-night difference in the height of the ionosphere, latitudinal changes in the Earth's magnetic field, sudden ionospheric disturbances, polar cap absorption, variation in the Earth radius of ± 11 km from equator to geographic poles, etc. that produce other effects in the Schumann resonance power spectra.

Measurements

Today Schumann resonances are recorded at many separate research stations around the world. The sensors used to measure Schumann resonances typically consist of two horizontal magnetic inductive coils for measuring the north-south and east-west components of the magnetic field, and a vertical electric dipole antenna for measuring the vertical component of the electric field. A typical passband of the instruments is 3–100 Hz. The Schumann resonance electric field amplitude (~300 microvolts per meter) is much smaller than the static fair-weather electric field (~150 V/m) in the atmosphere. Similarly, the amplitude of the Schumann resonance magnetic field (~1 picotesla) is many orders of magnitude smaller than the Earth's magnetic field (~30–50 microteslas).[25] Specialized receivers and antennas are needed to detect and record Schumann resonances. The electric component is commonly measured with a ball antenna, suggested by Ogawa et al., in 1966,[26] connected to a high-impedance amplifier. The magnetic induction coils typically consist of tens- to hundreds-of-thousands of turns of wire wound around a core of very high magnetic permeability.

Dependence on global lightning activity

From the very beginning of Schumann resonance studies, it was known that they could be used to monitor global lightning activity. At any given time there are about 2000 thunderstorms around the globe.[27] Producing approximately fifty lightning events per second,[28] these thunderstorms are directly linked to the background Schumann resonance signal.

Determining the spatial lightning distribution from Schumann resonance records is a complex problem: in order to estimate the lightning intensity from Schumann resonance records it is necessary to account for both the distance to lightning sources and the wave propagation between the source and the observer. A common approach is to make a preliminary assumption on the spatial lightning distribution, based on the known properties of lightning climatology. An alternative approach is placing the receiver at the North or South Pole, which remain approximately equidistant from the main thunderstorm centers during the day.[29] One method not requiring preliminary assumptions on the lightning distribution[30] is based on the decomposition of the average background Schumann resonance spectra, utilizing ratios between the average electric and magnetic spectra and between their linear combination. This technique assumes the cavity is spherically symmetric and therefore does not include known cavity asymmetries that are believed to affect the resonance and propagation properties of electromagnetic waves in the system.

Diurnal variations

The best documented and the most debated features of the Schumann resonance phenomenon are the diurnal variations of the background Schumann resonance power spectrum.

A characteristic Schumann resonance diurnal record reflects the properties of both global lightning activity and the state of the Earth–ionosphere cavity between the source region and the observer. The vertical electric field is independent of the direction of the source relative to the observer, and is therefore a measure of global lightning. The diurnal behavior of the vertical electric field shows three distinct maxima, associated with the three "hot spots" of planetary lightning activity: one at 9 UT (Universal Time) linked to the daily peak of thunderstorm activity from Southeast Asia; one at 14 UT linked to the peak of African lightning activity; and one at 20 UT linked to the peak of South American lightning activity. The time and amplitude of the peaks vary throughout the year, linked to seasonal changes in lightning activity.

"Chimney" ranking

In general, the African peak is the strongest, reflecting the major contribution of the African "chimney" to global lightning activity. The ranking of the two other peaks—Asian and American—is the subject of a vigorous dispute among Schumann resonance scientists. Schumann resonance observations made from Europe show a greater contribution from Asia than from South America, while observations made from North America indicate the dominant contribution comes from South America.

Williams and Sátori[31] suggest that in order to obtain "correct" Asia-America chimney ranking, it is necessary to remove the influence of the day/night variations in the ionospheric conductivity (day-night asymmetry influence) from the Schumann resonance records. The "corrected" records presented in the work by Sátori, et al.[32] show that even after the removal of the day-night asymmetry influence from Schumann resonance records, the Asian contribution remains greater than American.

Similar results were obtained by Pechony et al.[33] who calculated Schumann resonance fields from satellite lightning data. It was assumed that the distribution of lightning in the satellite maps was a good proxy for Schumann excitations sources, even though satellite observations predominantly measure in-cloud lightning rather than the cloud-to-ground lightning that are the primary exciters of the resonances. Both simulations—those neglecting the day-night asymmetry, and those taking this asymmetry into account—showed the same Asia-America chimney ranking. On the other hand, some optical satellite and climatological lightning data suggest the South American thunderstorm center is stronger than the Asian center.[28]

The reason for the disparity among rankings of Asian and American chimneys in Schumann resonance records remains unclear, and is the subject of further research.

Influence of the day-night asymmetry

In the early literature the observed diurnal variations of Schumann resonance power were explained by the variations in the source-receiver (lightning-observer) geometry.[19] It was concluded that no particular systematic variations of the ionosphere (which serves as the upper waveguide boundary) are needed to explain these variations.[34] Subsequent theoretical studies supported the early estimations of the small influence of the ionosphere day-night asymmetry (difference between day-side and night-side ionosphere conductivity) on the observed variations in Schumann resonance field intensities.[35]

The interest in the influence of the day-night asymmetry in the ionosphere conductivity on Schumann resonances gained new strength in the 1990s, after publication of a work by Sentman and Fraser.[36] Sentman and Fraser developed a technique to separate the global and the local contributions to the observed field power variations using records obtained simultaneously at two stations that were widely separated in longitude. They interpreted the diurnal variations observed at each station in terms of a combination of a diurnally varying global excitation modulated by the local ionosphere height. Their work, which combined both observations and energy conservation arguments, convinced many scientists of the importance of the ionospheric day-night asymmetry and inspired numerous experimental studies. However, recently it was shown that results obtained by Sentman and Fraser can be approximately simulated with a uniform model (without taking into account ionosphere day-night variation) and therefore cannot be uniquely interpreted solely in terms of ionosphere height variation.[37]

Schumann resonance amplitude records show significant diurnal and seasonal variations which in general coincide in time with the times of the day-night transition (the terminator). This time-matching seems to support the suggestion of a significant influence of the day-night ionosphere asymmetry on Schumann resonance amplitudes. There are records showing almost clock-like accuracy of the diurnal amplitude changes.[32] On the other hand, there are numerous days when Schumann resonance amplitudes do not increase at sunrise or do not decrease at sunset. There are studies showing that the general behavior of Schumann resonance amplitude records can be recreated from diurnal and seasonal thunderstorm migration, without invoking ionospheric variations.[33][35] Two recent independent theoretical studies have shown that the variations in Schumann resonance power related to the day-night transition are much smaller than those associated with the peaks of the global lightning activity, and therefore the global lightning activity plays a more important role in the variation of the Schumann resonance power.[33][38]

It is generally acknowledged that source-observer effects are the dominant source of the observed diurnal variations, but there remains considerable controversy about the degree to which day-night signatures are present in the data. Part of this controversy stems from the fact that the Schumann resonance parameters extractable from observations provide only a limited amount of information about the coupled lightning source-ionospheric system geometry. The problem of inverting observations to simultaneously infer both the lightning source function and ionospheric structure is therefore extremely underdetermined, leading to the possibility of non-unique interpretations.

"Inverse problem"

One of the interesting problems in Schumann resonances studies is determining the lightning source characteristics (the "inverse problem"). Temporally resolving each individual flash is impossible because the mean rate of excitation by lightning, ~50 lightning events per second globally, mixes up the individual contributions together. However, occasionally extremely large lightning flashes occur which produce distinctive signatures that stand out from the background signals. Called "Q-bursts", they are produced by intense lightning strikes that transfer large amounts of charge from clouds to the ground and often carry high peak current.[26] Q-bursts can exceed the amplitude of the background signal level by a factor of 10 or more and appear with intervals of ~10 s,[30] which allows them to be considered as isolated events and determine the source lightning location. The source location is determined with either multi-station or single-station techniques and requires assuming a model for the Earth–ionosphere cavity. The multi-station techniques are more accurate, but require more complicated and expensive facilities.

Transient luminous events research

It is now believed that many of the Schumann resonances transients (Q bursts) are related to the transient luminous events (TLEs). In 1995, Boccippio et al.[39] showed that sprites, the most common TLE, are produced by positive cloud-to-ground lightning occurring in the stratiform region of a thunderstorm system, and are accompanied by Q-burst in the Schumann resonances band. Recent observations[39][40] reveal that occurrences of sprites and Q bursts are highly correlated and Schumann resonances data can possibly be used to estimate the global occurrence rate of sprites.[41]

Global temperature

Williams [1992][42] suggested that global temperature may be monitored with the Schumann resonances. The link between Schumann resonance and temperature is lightning flash rate, which increases nonlinearly with temperature.[42] The nonlinearity of the lightning-to-temperature relation provides a natural amplifier of the temperature changes and makes Schumann resonance a sensitive "thermometer". Moreover, the ice particles that are believed to participate in the electrification processes which result in a lightning discharge[43] have an important role in the radiative feedback effects that influence the atmosphere temperature. Schumann resonances may therefore help us to understand these feedback effects. A paper was published in 2006 linking Schumann resonance to global surface temperature,[44] which was followed up with a 2009 study.[45]

Upper tropospheric water vapor

Tropospheric water vapor is a key element of the Earth's climate, which has direct effects as a greenhouse gas, as well as indirect effects through interaction with clouds, aerosols and tropospheric chemistry. Upper tropospheric water vapor (UTWV) has a much greater impact on the greenhouse effect than water vapor in the lower atmosphere,[46] but whether this impact is a positive or a negative feedback is still uncertain.[47] The main challenge in addressing this question is the difficulty in monitoring UTWV globally over long timescales. Continental deep-convective thunderstorms produce most of the lightning discharges on Earth. In addition, they transport large amount of water vapor into the upper troposphere, dominating the variations of global UTWV. Price [2000][48] suggested that changes in the UTWV can be derived from records of Schumann resonances.

On other planets and moons

The existence of Schumann-like resonances is conditioned primarily by two factors:

  1. A closed, planetary-sized and approximately spherical cavity, consisting of conducting lower and upper boundaries separated by an insulating medium. For the earth the conducting lower boundary is its surface, and the upper boundary is the ionosphere. Other planets may have similar electrical conductivity geometry, so it is speculated that they should possess similar resonant behavior.
  2. A source of electrical excitation of electromagnetic waves in the ELF range.

Within the Solar System there are five candidates for Schumann resonance detection besides the Earth: Venus, Mars, Jupiter, Saturn, and Saturn's biggest moon Titan. Modeling Schumann resonances on the planets and moons of the Solar System is complicated by the lack of knowledge of the waveguide parameters. No in situ capability exists today to validate the results.

Venus

The strongest evidence for lightning on Venus comes from the impulsive electromagnetic waves detected by Venera 11 and 12 landers. Theoretical calculations of the Schumann resonances at Venus were reported by Nickolaenko and Rabinowicz [1982][49] and Pechony and Price [2004].[50] Both studies yielded very close results, indicating that Schumann resonances should be easily detectable on that planet given a lightning source of excitation and a suitably located sensor.

Mars

In the case of Mars there have been terrestrial observations of radio emission spectra that have been associated with Schumann resonances.[51] The reported radio emissions are not of the primary electromagnetic Schumann modes, but rather of secondary modulations of the nonthermal microwave emissions from the planet at approximately the expected Schumann frequencies, and have not been independently confirmed to be associated with lightning activity on Mars. There is the possibility that future lander missions could carry in situ instrumentation to perform the necessary measurements. Theoretical studies are primarily directed to parameterizing the problem for future planetary explorers.

Detection of lightning activity on Mars has been reported by Ruf et al. [2009].[51] The evidence is indirect and in the form of modulations of the nonthermal microwave spectrum at approximately the expected Schumann resonance frequencies. It has not been independently confirmed that these are associated with electrical discharges on Mars. In the event confirmation is made by direct, in situ observations, it would verify the suggestion of the possibility of charge separation and lightning strokes in the Martian dust storms made by Eden and Vonnegut [1973][52] and Renno et al. [2003].[53] Martian global resonances were modeled by Sukhorukov [1991],[54] Pechony and Price [2004],[50] and Molina-Cuberos et al. [2006].[55] The results of the three studies are somewhat different, but it seems that at least the first two Schumann resonance modes should be detectable. Evidence of the first three Schumann resonance modes is present in the spectra of radio emission from the lightning detected in Martian dust storms.[51]

Titan

It was long ago suggested that lightning discharges may occur on Titan,[56] but recent data from Cassini–Huygens seems to indicate that there is no lightning activity on this largest satellite of Saturn. Due to the recent interest in Titan, associated with the Cassini–Huygens mission, its ionosphere is perhaps the most thoroughly modeled today. Schumann resonances on Titan have received more attention than on any other celestial body, in works by Besser et al. [2002],[57] Morente et al. [2003],[58] Molina-Cuberos et al. [2004],[59] Nickolaenko et al. [2003],[60] and Pechony and Price [2004].[50] It appears that only the first Schumann resonance mode might be detectable on Titan.

Since the landing of the Huygens probe on Titan's surface in January 2005, there have been many reports on observations and theory of an atypical Schumann resonance on Titan. After several tens of fly-bys by Cassini, neither lightning nor thunderstorms were detected in Titan's atmosphere. Scientists therefore proposed another source of electrical excitation: induction of ionospheric currents by Saturn's co-rotating magnetosphere. All data and theoretical models comply with a Schumann resonance, the second eigenmode of which was observed by the Huygens probe. The most important result of this is the proof of existence of a buried liquid water-ammonia ocean under a few tens of km of the icy subsurface crust.[61][62][63][64]

Jupiter and Saturn

Lightning activity has been optically detected on Jupiter. Existence of lightning activity on that planet was predicted by Bar-Nun [1975][65] and it is now supported by data from Galileo, Voyagers 1 and 2, Pioneers 10 and 11, and Cassini. Saturn is also confirmed to have lightning activity.[66] Though three visiting spacecraft (Pioneer 11 in 1979, Voyager 1 in 1980, and Voyager 2 in 1981) failed to provide any convincing evidence from optical observations, in July 2012 the Cassini spacecraft detected visible lightning flashes, and electromagnetic sensors aboard the spacecraft detected signatures that are characteristic of lightning. Little is known about the electrical parameters of the interior of Jupiter or Saturn. Even the question of what should serve as the lower waveguide boundary is a non-trivial one in case of the gaseous planets. There seem to be no works dedicated to Schumann resonances on Saturn. To date there has been only one attempt to model Schumann resonances on Jupiter.[67] Here, the electrical conductivity profile within the gaseous atmosphere of Jupiter was calculated using methods similar to those used to model stellar interiors, and it was pointed out that the same methods could be easily extended to the other gas giants Saturn, Uranus and Neptune. Given the intense lightning activity at Jupiter, the Schumann resonances should be easily detectable with a sensor suitably positioned within the planetary-ionospheric cavity.

See also

References

  1. ^ "Schumann Resonance". NASA. Retrieved November 8, 2017.
  2. ^ MacGorman, D. R.; Rust, W. D. (1998). The electrical nature of storms. New York: Oxford University Press. p. 114. ISBN 9780195073379. OCLC 35183896.
  3. ^ Volland, Hans (1995). Handbook of atmospheric electrodynamics. Vol. 1. Boca Raton: CRC Press. p. 277. ISBN 9780849386473. OCLC 31408654.
  4. ^ Rusov, V.D. (2012). "Can Resonant Oscillations of the Earth Ionosphere Influence the Human Brain Biorhythm?". arXiv:1208.4970 [physics.gen-ph]. Department of Theoretical and Experimental Nuclear Physics, Odessa National Polytechnic University, Ukraine
  5. ^ Montiel, I.; Bardasano, J.L.; Ramos, J.L. (2005). "Biophysical Device For The Treatment Of Neurodegenerative Diseases". In Méndez-Vilas, A. (ed.). Recent Advances in Multidisciplinary Applied Physics. Proceedings of the First International Meeting on Applied Physics (APHYS-2003) October 13–18th 2003, Badajoz, Spain. pp. 63–69. doi:10.1016/B978-008044648-6.50011-2. ISBN 9780080446486.
  6. ^ Williams, Earle R. (May 22, 1992). "The Schumann resonance: A global tropical thermometer". Science. 256 (5060): 1184–1187. Bibcode:1992Sci...256.1184W. doi:10.1126/science.256.5060.1184. PMID 17795213.
  7. ^ Barr, R.; Llanwyn Jones, David; Rodger, C.J. (2000). "ELF and VLF radio waves" (PDF). Journal of Atmospheric and Solar-Terrestrial Physics. 62 (17–18): 1689–1718. Bibcode:2000JASTP..62.1689B. doi:10.1016/S1364-6826(00)00121-8.
  8. ^ Stéphane, Sainson (2017). Electromagnetic seabed logging : a new tool for geoscientists. Springer. ISBN 978-3-319-45355-2.
  9. ^ FitzGerald, G. F. (1893). "On the period of vibration of electrical disturbances upon the Earth". Report of the British Association for the Advancement of Science. 63rd Meeting: 682.
  10. ^ Jackson, J. D. (August 2008). "Examples of the zeroth theorem of the history of science" (PDF). American Journal of Physics. 76 (8): 704–719. arXiv:0708.4249. Bibcode:2008AmJPh..76..704J. doi:10.1119/1.2904468.
  11. ^ Heaviside, O. (1902). "Telegraphy, Sect. 1, Theory". Encyclopædia Britannica. Vol. 9 (10 ed.). London. pp. 213–218.{{cite encyclopedia}}: CS1 maint: location missing publisher (link)
  12. ^ Kennelly, Arthur E. (1902). "On the elevation of the electrically-conducting strata of the earth's atmosphere". World and Engineer. 32: 473.
  13. ^ Appleton, E. V.; Barnett, M. A. F. (1925). "On Some Direct Evidence for Downward Atmospheric Reflection of Electric Rays". Proceedings of the Royal Society of London A. 109 (752): 621–641. Bibcode:1925RSPSA.109..621A. doi:10.1098/rspa.1925.0149.
  14. ^ Watson, G. N. (1918). "The diffraction of electric waves by the Earth". Proceedings of the Royal Society of London A. 95 (666): 83–99. Bibcode:1918RSPSA..95...83W. doi:10.1098/rspa.1918.0050.
  15. ^ a b Schumann, W. O. (1952). "Über die strahlungslosen Eigenschwingungen einer leitenden Kugel, die von einer Luftschicht und einer Ionosphärenhülle umgeben ist". Zeitschrift für Naturforschung A. 7 (2): 149–154. Bibcode:1952ZNatA...7..149S. doi:10.1515/zna-1952-0202.
  16. ^ Schumann, W. O. (1952). "Über die Dämpfung der elektromagnetischen Eigenschwingnugen des Systems Erde – Luft – Ionosphäre". Zeitschrift für Naturforschung A. 7 (3–4): 250–252. Bibcode:1952ZNatA...7..250S. doi:10.1515/zna-1952-3-404.
  17. ^ Schumann, W. O. (1952). "Über die Ausbreitung sehr Langer elektriseher Wellen um die Signale des Blitzes". Nuovo Cimento. 9 (12): 1116–1138. Bibcode:1952NCim....9.1116S. doi:10.1007/BF02782924.
  18. ^ Schumann, W. O.; König, H. (1954). "Über die Beobactung von Atmospherics bei geringsten Frequenzen". Naturwissenschaften. 41 (8): 183–184. Bibcode:1954NW.....41..183S. doi:10.1007/BF00638174.
  19. ^ a b Balser, M.; Wagner, C. (1960). "Measurement of the spectrum of radio noise from 50 to 100 c/s". Journal of Research of the National Bureau of Standards. 64D (4): 415–418. doi:10.6028/jres.064d.050.
  20. ^ Balser, M.; Wagner, C. (1960). "Observations of Earth–ionosphere cavity resonances". Nature. 188 (4751): 638–641. Bibcode:1960Natur.188..638B. doi:10.1038/188638a0.
  21. ^ Balser, M.; Wagner, C. (1962). "Diurnal power variations of the Earth–ionosphere cavity modes and their relationship to worldwide thunderstorm activity". Journal of Geophysical Research. 67 (2): 619–625. Bibcode:1962JGR....67..619B. doi:10.1029/JZ067i002p00619.
  22. ^ Balser, M.; Wagner, C. (1962). "On frequency variations of the Earth–ionosphere cavity modes". Journal of Geophysical Research. 67 (10): 4081–4083. Bibcode:1962JGR....67.4081B. doi:10.1029/JZ067i010p04081.
  23. ^ Balser, M.; Wagner, C. (1963). "Effect of a high-altitude nuclear detonation on the Earth–ionosphere cavity". Journal of Geophysical Research. 68 (13): 4115–4118. Bibcode:1963JGR....68.4115B. doi:10.1029/jz068i013p04115.
  24. ^ a b Volland, H. (1984). Atmospheric Electrodynamics. Springer-Verlag, Berlin.
  25. ^ Price, C.; Pechony, O.; Greenberg, E. (2006). "Schumann resonances in lightning research". Journal of Lightning Research. 1: 1–15.
  26. ^ a b Ogawa, T.; Tanka, Y.; Miura, T.; Yasuhara, M. (1966). "Observations of natural ELF electromagnetic noises by using the ball antennas". Journal of Geomagnetism and Geoelectricity. 18 (4): 443–454. Bibcode:1966JGG....18..443O. doi:10.5636/jgg.18.443.
  27. ^ Heckman, S. J.; Williams, E. (1998). "Total global lightning inferred from Schumann resonance measurements". Journal of Geophysical Research. 103 (D24): 31775–31779. Bibcode:1998JGR...10331775H. doi:10.1029/98JD02648.
  28. ^ a b Christian, H. J.; Blakeslee, R. J.; Boccippio, D. J.; Boeck, W. L.; et al. (2003). "Global frequency and distribution of lightning as observed from space by the Optical Transient Detector". Journal of Geophysical Research. 108 (D1): 4005. Bibcode:2003JGRD..108.4005C. doi:10.1029/2002JD002347.
  29. ^ Nickolaenko, A. P. (1997). "Modern aspects of Schumann resonance studies". Journal of Atmospheric and Solar-Terrestrial Physics. 59 (7): 806–816. Bibcode:1997JASTP..59..805N. doi:10.1016/s1364-6826(96)00059-4.
  30. ^ a b Shvets, A. V. (2001). "A technique for reconstruction of global lightning distance profile from background Schumann resonance signal". Journal of Atmospheric and Solar-Terrestrial Physics. 63 (10): 1061–1074. Bibcode:2001JASTP..63.1061S. doi:10.1016/s1364-6826(01)00024-4.
  31. ^ Williams, E. R.; Sátori, G. (2004). "Lightning, thermodynamic and hydrological comparison of the two tropical continental chimneys". Journal of Atmospheric and Solar-Terrestrial Physics. 66 (13–14): 1213–1231. Bibcode:2004JASTP..66.1213W. doi:10.1016/j.jastp.2004.05.015.
  32. ^ a b Sátori, G.; Neska, M.; Williams, E.; Szendrői, J. (2007). "Signatures of the non-uniform Earth–ionosphere cavity in high time-resolution Schumann resonance records". Radio Science. 42 (2): RS003483. Bibcode:2007RaSc...42.2S10S. doi:10.1029/2006RS003483.
  33. ^ a b c Pechony, O.; Price, C.; Nickolaenko, A. P. (2007). "Relative importance of the day-night asymmetry in Schumann resonance amplitude records". Radio Science. 42 (2): RS2S06. Bibcode:2007RaSc...42.2S06P. doi:10.1029/2006RS003456.
  34. ^ Madden, T.; Thompson, W. (1965). "Low-frequency electromagnetic oscillations of the Earth–ionosphere cavity". Reviews of Geophysics. 3 (2): 211. Bibcode:1965RvGSP...3..211M. doi:10.1029/RG003i002p00211.
  35. ^ a b Nickolaenko, A. P.; Hayakawa, M. (2002). Resonances in the Earth–ionosphere cavity. Kluwer Academic Publishers, Dordrecht-Boston-London.
  36. ^ Sentman, D. D.; Fraser, B. J. (1991). "Simultaneous observations of Schumann resonances in California and Australia – Evidence for intensity modulation by the local height of the D region". Journal of Geophysical Research. 96 (9): 15973–15984. Bibcode:1991JGR....9615973S. doi:10.1029/91JA01085.
  37. ^ Pechony, O.; Price, C. (2006). "Schumann Resonances: interpretation of local diurnal intensity modulations". Radio Science. 42 (2): RS2S05. Bibcode:2006RaSc...41.2S05P. doi:10.1029/2006RS003455.
  38. ^ Yang, H.; Pasko, V. P. (2007). "Three-dimensional finite difference time domain modeling of the diurnal and seasonal variations in Schumann resonance parameters". Radio Science. 41 (2): RS2S14. Bibcode:2006RaSc...41.2S14Y. doi:10.1029/2005RS003402.
  39. ^ a b Boccippio, D. J.; Williams, E. R.; Heckman, S. J.; Lyons, W. A.; et al. (1995). "Sprites, ELF transients, and positive ground strokes". Science. 269 (5227): 1088–1091. Bibcode:1995Sci...269.1088B. doi:10.1126/science.269.5227.1088. PMID 17755531.
  40. ^ Price, C.; Greenberg, E.; Yair, Y.; Sátori, G.; et al. (2004). "Ground-based detection of TLE-producing intense lightning during the MEIDEX mission on board the Space Shuttle Columbia". Geophysical Research Letters. 31 (20): L20107. Bibcode:2004GeoRL..3120107P. doi:10.1029/2004GL020711.
  41. ^ Hu, W.; Cummer, S. A.; Lyons, W. A.; Nelson, T. E. (2002). "Lightning charge moment changes for the initiation of sprites". Geophysical Research Letters. 29 (8): 1279. Bibcode:2002GeoRL..29.1279H. doi:10.1029/2001GL014593.
  42. ^ a b Williams, E.R. (1992). "The Schumann resonance: a global tropical thermometer". Science. 256 (5060): 1184–1186. Bibcode:1992Sci...256.1184W. doi:10.1126/science.256.5060.1184. PMID 17795213.
  43. ^ Williams, E.R. (1989). "The tripole structure of thunderstorms". Journal of Geophysical Research. 94 (D11): 13151–13167. Bibcode:1989JGR....9413151W. doi:10.1029/JD094iD11p13151.
  44. ^ Sekiguchi, M.; Hayakawa, M.; Nickolaenko, A. P.; Hobara, Y. (2006). "Evidence on a link between the intensity of Schumann resonance and global surface temperature". Annales Geophysicae. 24 (7): 1809–1817. Bibcode:2006AnGeo..24.1809S. doi:10.5194/angeo-24-1809-2006.
  45. ^ Hobara, Y.; Harada, T.; Hayakawa, M.; Sekiguchi, M.; Ohta, K. (2009). "Study on monitoring global warming by using the data of Schumann resonance". AGU Fall Meeting Abstracts. 2009: AE43B–0267. Bibcode:2009AGUFMAE43B0267H.
  46. ^ Hansen, J.; Lacis, A.; Rind, D.; Russel, G.; et al. (1984). "Climate sensitivity: Analysis of feedback mechanisms". In Hansen, J. E.; Takahashi, T. (eds.). Climate Processes and Climate Sensitivity. AGU Geophysical Monograph Series. Vol. 29. pp. 130–163. Bibcode:1984GMS....29..130H. doi:10.1029/gm029p0130. ISBN 978-0-87590-404-7.
  47. ^ Rind, D. (1998). "Just add water vapor". Science. 28 (5380): 1152–1153. doi:10.1126/science.281.5380.1152.
  48. ^ Price, C. (2000). "Evidence for a link between global lightning activity and upper tropospheric water vapor". Nature. 406 (6793): 290–293. Bibcode:2000Natur.406..290P. doi:10.1038/35018543. PMID 10917527.
  49. ^ Nickolaenko, A. P.; Rabinowicz, L. M. (1982). "On the possibility of existence of global electromagnetic resonances on the planets of Solar system". Space Research. 20: 82–89.
  50. ^ a b c Pechony, O.; Price, C. (2004). "Schumann resonance parameters calculated with a partially uniform knee model on Earth, Venus, Mars, and Titan". Radio Science. 39 (5): RS5007. Bibcode:2004RaSc...39.5007P. doi:10.1029/2004RS003056.
  51. ^ a b c Ruf, C.; Renno, N. O.; Kok, J. F.; Bandelier, E.; et al. (2009). "Emission of Non-thermal Microwave Radiation by a Martian Dust Storm" (PDF). Geophysical Research Letters. 36 (13): L13202. Bibcode:2009GeoRL..3613202R. CiteSeerX 10.1.1.872.939. doi:10.1029/2009GL038715. hdl:2027.42/94934.
  52. ^ Eden, H. F.; Vonnegut, B. (1973). "Electrical breakdown caused by dust motion in low-pressure atmospheres: consideration for Mars". Science. 180 (4089): 962–963. Bibcode:1973Sci...180..962E. doi:10.1126/science.180.4089.962. PMID 17735929.
  53. ^ Renno, N. O.; Wong, A.; Atreya, S. K.; de Pater, I.; Roos-Serote, M. (2003). "Electrical discharges and broadband radio emission by Martian dust devils and dust storms" (PDF). Geophysical Research Letters. 30 (22): 2140. Bibcode:2003GeoRL..30.2140R. doi:10.1029/2003GL017879. hdl:2027.42/95558.
  54. ^ Sukhorukov, A. I. (1991). "On the Schumann resonances on Mars". Planet. Space Sci. 39 (12): 1673–1676. Bibcode:1991P&SS...39.1673S. doi:10.1016/0032-0633(91)90028-9.
  55. ^ Molina-Cuberos, G. J.; Morente, J. A.; Besser, B. P.; Porti, J.; et al. (2006). "Schumann resonances as a tool to study the lower ionosphere of Mars". Radio Science. 41 (1): RS1003. Bibcode:2006RaSc...41.1003M. doi:10.1029/2004RS003187.
  56. ^ Lammer, H.; Tokano, T.; Fischer, G.; Stumptner, W.; et al. (2001). "Lightning activity of Titan: can Cassiny/Huygens detect it?". Planetary and Space Science. 49 (6): 561–574. Bibcode:2001P&SS...49..561L. doi:10.1016/S0032-0633(00)00171-9.
  57. ^ Besser, B. P.; Schwingenschuh, K.; Jernej, I.; Eichelberger, H. U.; et al. (2002). "Schumann resonances as indicators for lighting on Titan". Proceedings of the Second European Workshop on Exo/Astrobiology, Graz, Austria, September 16–19.
  58. ^ Morente, J. A.; Molina-Cuberos, G. J.; Porti, J. A.; Schwingenschuh, K.; et al. (2003). "A study of the propagation of electromagnetic waves in Titan's atmosphere with the TLM numerical method". Icarus. 162 (2): 374–384. Bibcode:2003Icar..162..374M. doi:10.1016/S0019-1035(03)00025-3.
  59. ^ Molina-Cuberos, G. J.; Porti, J.; Besser, B. P.; Morente, J. A.; et al. (2004). "Shumann resonances and electromagnetic transparence in the atmosphere of Titan". Advances in Space Research. 33 (12): 2309–2313. Bibcode:2004AdSpR..33.2309M. doi:10.1016/S0273-1177(03)00465-4.
  60. ^ Nickolaenko, A. P.; Besser, B. P.; Schwingenschuh, K. (2003). "Model computations of Schumann resonance on Titan". Planetary and Space Science. 51 (13): 853–862. Bibcode:2003P&SS...51..853N. doi:10.1016/S0032-0633(03)00119-3.
  61. ^ Béghin, C.; Simões, F.; Krasnoselskikh, V.; Schwingenschuh, K.; et al. (November 1, 2007). "A Schumann-like resonance on Titan driven by Saturn's magnetosphere possibly revealed by the Huygens Probe". Icarus. 191 (1): 251–266. Bibcode:2007Icar..191..251B. doi:10.1016/j.icarus.2007.04.005.
  62. ^ Béghin, C.; Canu, P.; Karkoschka, E.; Sotin, C.; et al. (December 2009). "New insights on Titan's plasma-driven Schumann resonance inferred from Huygens and Cassini data". Planetary and Space Science. 57 (14–15): 1872–1888. Bibcode:2009P&SS...57.1872B. doi:10.1016/j.pss.2009.04.006.
  63. ^ Béghin, Christian; Sotin, Christophe; Hamelin, Michel (June 2010). "Titan's native ocean revealed beneath some 45km of ice by a Schumann-like resonance". Comptes Rendus Geoscience. 342 (6): 425–433. Bibcode:2010CRGeo.342..425B. doi:10.1016/j.crte.2010.03.003.
  64. ^ Béghin, Christian; Randriamboarison, Orélien; Hamelin, Michel; Karkoschka, Erich; et al. (2012). "Analytic theory of Titan's Schumann resonance: Constraints on ionospheric conductivity and buried water ocean". Icarus. 218 (2): 1028–1042. Bibcode:2012Icar..218.1028B. doi:10.1016/j.icarus.2012.02.005. hdl:2060/20140002248.
  65. ^ Bar-Nun, A. (1975). "Thunderstorms on Jupiter". Icarus. 24 (1): 86–94. Bibcode:1975Icar...24...86B. doi:10.1016/0019-1035(75)90162-1.
  66. ^ "Lightning Flashing in Daylight (Saturn Images from NASA's Cassini Spacecraft)". www.ciclops.org. Retrieved November 8, 2017.
  67. ^ Sentman, D. D. (1990). "Electrical conductivity of Jupiter's Shallow interior and the formation of a resonant planetary-ionosphere cavity". Icarus. 88 (1): 73–86. Bibcode:1990Icar...88...73S. doi:10.1016/0019-1035(90)90177-B.

External articles and references

Wikimedia Commons has media related to Schumann resonance.
General references
Websites
Animation
Retrieved from "https://en.wikipedia.org/w/index.php?title=Schumann_resonances&oldid=997382635"