Magnetotelluric Fields of a Gaussian Electrojet

In a previous paper (Hermance and Peltier 1970), integral expressions for the magnetotelluric fields of a line source over a stratified conductor were obtained and numerically evaluated for a sequence of simple conductivity structures. This calculation was intended to simulate the magnetotelluric &#...

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Published in:Canadian Journal of Earth Sciences
Main Authors: Peltier, W. R., Hermance, J. F.
Format: Article in Journal/Newspaper
Language:English
Published: Canadian Science Publishing 1971
Subjects:
Online Access:http://dx.doi.org/10.1139/e71-034
http://www.nrcresearchpress.com/doi/pdf/10.1139/e71-034
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spelling crcansciencepubl:10.1139/e71-034 2024-05-19T07:42:51+00:00 Magnetotelluric Fields of a Gaussian Electrojet Peltier, W. R. Hermance, J. F. 1971 http://dx.doi.org/10.1139/e71-034 http://www.nrcresearchpress.com/doi/pdf/10.1139/e71-034 en eng Canadian Science Publishing http://www.nrcresearchpress.com/page/about/CorporateTextAndDataMining Canadian Journal of Earth Sciences volume 8, issue 3, page 338-346 ISSN 0008-4077 1480-3313 journal-article 1971 crcansciencepubl https://doi.org/10.1139/e71-034 2024-05-02T06:51:25Z In a previous paper (Hermance and Peltier 1970), integral expressions for the magnetotelluric fields of a line source over a stratified conductor were obtained and numerically evaluated for a sequence of simple conductivity structures. This calculation was intended to simulate the magnetotelluric 'source effect' which is anticipated at auroral and equatorial latitudes. The most serious flaw in this line source model of an electrojet is that it does not take into account the laterally diffuse nature of the real current distribution. By assuming that the current density in the electrojet has a Gaussian dependence upon the horizontal coordinate a more realistic source model can be constructed. Representative solutions to the induction problem employing this source are analyzed in an effort to obtain a more accurate measure of the effect of finite source geometry on magnetotelluric interpretations in auroral and equatorial regions where strong electrojets exist at E-layer altitudes. In tectonically active areas such as Iceland (which is under the auroral electrojet), it appears that Cagniard's assumption of a "plane-wave" source leads to a correct interpretation of the subsurface conductivity structure in the commonly employed U.L.F. frequency band (10 −4 Hz–1 Hz). A relationship, Tozer (1969), is here assumed to exist between tectonism, anomalously high near surface temperatures, and corresponding increases in electrical conductivity. In tectonically stable shield areas, however, the effect of finite source geometry is more pronounced and could lead to significant errors in interpretation. Article in Journal/Newspaper Iceland Canadian Science Publishing Canadian Journal of Earth Sciences 8 3 338 346
institution Open Polar
collection Canadian Science Publishing
op_collection_id crcansciencepubl
language English
description In a previous paper (Hermance and Peltier 1970), integral expressions for the magnetotelluric fields of a line source over a stratified conductor were obtained and numerically evaluated for a sequence of simple conductivity structures. This calculation was intended to simulate the magnetotelluric 'source effect' which is anticipated at auroral and equatorial latitudes. The most serious flaw in this line source model of an electrojet is that it does not take into account the laterally diffuse nature of the real current distribution. By assuming that the current density in the electrojet has a Gaussian dependence upon the horizontal coordinate a more realistic source model can be constructed. Representative solutions to the induction problem employing this source are analyzed in an effort to obtain a more accurate measure of the effect of finite source geometry on magnetotelluric interpretations in auroral and equatorial regions where strong electrojets exist at E-layer altitudes. In tectonically active areas such as Iceland (which is under the auroral electrojet), it appears that Cagniard's assumption of a "plane-wave" source leads to a correct interpretation of the subsurface conductivity structure in the commonly employed U.L.F. frequency band (10 −4 Hz–1 Hz). A relationship, Tozer (1969), is here assumed to exist between tectonism, anomalously high near surface temperatures, and corresponding increases in electrical conductivity. In tectonically stable shield areas, however, the effect of finite source geometry is more pronounced and could lead to significant errors in interpretation.
format Article in Journal/Newspaper
author Peltier, W. R.
Hermance, J. F.
spellingShingle Peltier, W. R.
Hermance, J. F.
Magnetotelluric Fields of a Gaussian Electrojet
author_facet Peltier, W. R.
Hermance, J. F.
author_sort Peltier, W. R.
title Magnetotelluric Fields of a Gaussian Electrojet
title_short Magnetotelluric Fields of a Gaussian Electrojet
title_full Magnetotelluric Fields of a Gaussian Electrojet
title_fullStr Magnetotelluric Fields of a Gaussian Electrojet
title_full_unstemmed Magnetotelluric Fields of a Gaussian Electrojet
title_sort magnetotelluric fields of a gaussian electrojet
publisher Canadian Science Publishing
publishDate 1971
url http://dx.doi.org/10.1139/e71-034
http://www.nrcresearchpress.com/doi/pdf/10.1139/e71-034
genre Iceland
genre_facet Iceland
op_source Canadian Journal of Earth Sciences
volume 8, issue 3, page 338-346
ISSN 0008-4077 1480-3313
op_rights http://www.nrcresearchpress.com/page/about/CorporateTextAndDataMining
op_doi https://doi.org/10.1139/e71-034
container_title Canadian Journal of Earth Sciences
container_volume 8
container_issue 3
container_start_page 338
op_container_end_page 346
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