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Inductively induced polarization and its overall assessment using a normalized transient response. / Kozhevnikov, N. O.; Antonov, E. Y.U.

в: Russian Geology and Geophysics, Том 61, № 10, 10.2020, стр. 1173-1186.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

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Kozhevnikov NO, Antonov EYU. Inductively induced polarization and its overall assessment using a normalized transient response. Russian Geology and Geophysics. 2020 окт.;61(10):1173-1186. doi: 10.15372/RGG2019159

Author

Kozhevnikov, N. O. ; Antonov, E. Y.U. / Inductively induced polarization and its overall assessment using a normalized transient response. в: Russian Geology and Geophysics. 2020 ; Том 61, № 10. стр. 1173-1186.

BibTeX

@article{170d17d35de44ae3840a829b01044999,
title = "Inductively induced polarization and its overall assessment using a normalized transient response",
abstract = "The paper considers the basic regularities of inductively induced polarization (IIP) manifestation in the transient electromagnetic method. When calculating inductive transient responses of a polarizable ground, we assumed that the electrical conductivity of geologic materials is described by the Cole-Cole model. To present and analyze the results of computer-based simulation of the IIP phenomenon, we used a normalized transient response. It is defined as the ratio of the transient electromotive force (EMF) response of a polarizable ground to the EMF response of a ground that differs from the polarizable one only in that it has zero chargeability. The coordinates of the minimum of the normalized transient response are useful for an overall assessment of IIP manifestation. We show, by the example of a homogeneous polarizable half-space, how the inductive transient response is affected by the Cole-Cole model parameters and the size of transmitter and receiver loops. For a two-layer ground, IIP manifestation depends also on whether the base or upper layer is polarizable, as well as on the layer thickness. Inductively induced polarization is most pronounced when a conductive polarizable layer overlies a resistive nonpolarizable base. In this case, at a certain thickness of the layer, the IIP effect far exceeds that observed in the presence of a thick polarizable layer and even of a homogeneous polarizable half-space. ",
keywords = "Cole-Cole model, Inductively induced polarization, Transient electromagnetic method",
author = "Kozhevnikov, {N. O.} and Antonov, {E. Y.U.}",
note = "Funding Information: This work was supported by the Fundamental Scientific Research Project No. 0331-2019-0007 {"}Geoelectrics in geological environment research: technologies, field experiment and numerical models{"}. We thank Igor Mikhailov for translating the article into English and Igor Buddo for valuable comments, which were taken into account when preparing the final version of the article. Publisher Copyright: {\textcopyright} 2020, V.S. Sobolev IGM, Siberian Branch of the RAS. Copyright: Copyright 2020 Elsevier B.V., All rights reserved.",
year = "2020",
month = oct,
doi = "10.15372/RGG2019159",
language = "English",
volume = "61",
pages = "1173--1186",
journal = "Russian Geology and Geophysics",
issn = "1068-7971",
publisher = "Elsevier Science B.V.",
number = "10",

}

RIS

TY - JOUR

T1 - Inductively induced polarization and its overall assessment using a normalized transient response

AU - Kozhevnikov, N. O.

AU - Antonov, E. Y.U.

N1 - Funding Information: This work was supported by the Fundamental Scientific Research Project No. 0331-2019-0007 "Geoelectrics in geological environment research: technologies, field experiment and numerical models". We thank Igor Mikhailov for translating the article into English and Igor Buddo for valuable comments, which were taken into account when preparing the final version of the article. Publisher Copyright: © 2020, V.S. Sobolev IGM, Siberian Branch of the RAS. Copyright: Copyright 2020 Elsevier B.V., All rights reserved.

PY - 2020/10

Y1 - 2020/10

N2 - The paper considers the basic regularities of inductively induced polarization (IIP) manifestation in the transient electromagnetic method. When calculating inductive transient responses of a polarizable ground, we assumed that the electrical conductivity of geologic materials is described by the Cole-Cole model. To present and analyze the results of computer-based simulation of the IIP phenomenon, we used a normalized transient response. It is defined as the ratio of the transient electromotive force (EMF) response of a polarizable ground to the EMF response of a ground that differs from the polarizable one only in that it has zero chargeability. The coordinates of the minimum of the normalized transient response are useful for an overall assessment of IIP manifestation. We show, by the example of a homogeneous polarizable half-space, how the inductive transient response is affected by the Cole-Cole model parameters and the size of transmitter and receiver loops. For a two-layer ground, IIP manifestation depends also on whether the base or upper layer is polarizable, as well as on the layer thickness. Inductively induced polarization is most pronounced when a conductive polarizable layer overlies a resistive nonpolarizable base. In this case, at a certain thickness of the layer, the IIP effect far exceeds that observed in the presence of a thick polarizable layer and even of a homogeneous polarizable half-space.

AB - The paper considers the basic regularities of inductively induced polarization (IIP) manifestation in the transient electromagnetic method. When calculating inductive transient responses of a polarizable ground, we assumed that the electrical conductivity of geologic materials is described by the Cole-Cole model. To present and analyze the results of computer-based simulation of the IIP phenomenon, we used a normalized transient response. It is defined as the ratio of the transient electromotive force (EMF) response of a polarizable ground to the EMF response of a ground that differs from the polarizable one only in that it has zero chargeability. The coordinates of the minimum of the normalized transient response are useful for an overall assessment of IIP manifestation. We show, by the example of a homogeneous polarizable half-space, how the inductive transient response is affected by the Cole-Cole model parameters and the size of transmitter and receiver loops. For a two-layer ground, IIP manifestation depends also on whether the base or upper layer is polarizable, as well as on the layer thickness. Inductively induced polarization is most pronounced when a conductive polarizable layer overlies a resistive nonpolarizable base. In this case, at a certain thickness of the layer, the IIP effect far exceeds that observed in the presence of a thick polarizable layer and even of a homogeneous polarizable half-space.

KW - Cole-Cole model

KW - Inductively induced polarization

KW - Transient electromagnetic method

UR - http://www.scopus.com/inward/record.url?scp=85095729918&partnerID=8YFLogxK

U2 - 10.15372/RGG2019159

DO - 10.15372/RGG2019159

M3 - Article

AN - SCOPUS:85095729918

VL - 61

SP - 1173

EP - 1186

JO - Russian Geology and Geophysics

JF - Russian Geology and Geophysics

SN - 1068-7971

IS - 10

ER -

ID: 25992757