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Magnetic measurements in electrical prospecting by resistivity methods. / Mogilatov, V. S.; Kozhevnikov, N. O.; Zlobinsky, A. V.

In: Russian Geology and Geophysics, Vol. 59, No. 4, 01.04.2018, p. 432-437.

Research output: Contribution to journalArticlepeer-review

Harvard

Mogilatov, VS, Kozhevnikov, NO & Zlobinsky, AV 2018, 'Magnetic measurements in electrical prospecting by resistivity methods', Russian Geology and Geophysics, vol. 59, no. 4, pp. 432-437. https://doi.org/10.1016/j.rgg.2018.03.011

APA

Mogilatov, V. S., Kozhevnikov, N. O., & Zlobinsky, A. V. (2018). Magnetic measurements in electrical prospecting by resistivity methods. Russian Geology and Geophysics, 59(4), 432-437. https://doi.org/10.1016/j.rgg.2018.03.011

Vancouver

Mogilatov VS, Kozhevnikov NO, Zlobinsky AV. Magnetic measurements in electrical prospecting by resistivity methods. Russian Geology and Geophysics. 2018 Apr 1;59(4):432-437. doi: 10.1016/j.rgg.2018.03.011

Author

Mogilatov, V. S. ; Kozhevnikov, N. O. ; Zlobinsky, A. V. / Magnetic measurements in electrical prospecting by resistivity methods. In: Russian Geology and Geophysics. 2018 ; Vol. 59, No. 4. pp. 432-437.

BibTeX

@article{7743405ecad4435aaf826710bf6021e9,
title = "Magnetic measurements in electrical prospecting by resistivity methods",
abstract = "The electrical resistivity and induced polarization (IP) methods are widely used in geological mapping, prospecting and exploration of mineral deposits, engineering geology, hydrogeology, archaeology, and geotechnical and environmental applications. Historically, these methods have formed the basis of the electrical prospecting technique. In these methods, a DC or low-frequency AC electrical current is introduced into the earth through a grounded transmitter line. The measured quantity is the electric field. However, if the earth's resistivity or chargeability changes horizontally, this change gives rise to an anomalous magnetic field, which is studied by the magnetometric resistivity (MMR) and magnetic induced polarization (MIP) methods, respectively. Along with advantages, some shortcomings are inherent in the MMR and MIP techniques. Apparently, the main drawback of these methods is that the magnetic fields of both the transmitter line wire and ground electrodes on the surface are several orders of magnitude greater than the anomalous magnetic field response. This introduces a significant “noise” to magnetic-resistivity data. We investigate the potential of using a circular electric dipole (CED) in magnetometric resistivity techniques. It has been found that the application of a CED, instead of a conventional transmitter line, dramatically enhances the signal-to-noise ratio.",
keywords = "circular electric dipole, DC, electrical prospecting, magnetic field, MIP, MMR, resistivity methods",
author = "Mogilatov, {V. S.} and Kozhevnikov, {N. O.} and Zlobinsky, {A. V.}",
year = "2018",
month = apr,
day = "1",
doi = "10.1016/j.rgg.2018.03.011",
language = "English",
volume = "59",
pages = "432--437",
journal = "Russian Geology and Geophysics",
issn = "1068-7971",
publisher = "Elsevier Science B.V.",
number = "4",

}

RIS

TY - JOUR

T1 - Magnetic measurements in electrical prospecting by resistivity methods

AU - Mogilatov, V. S.

AU - Kozhevnikov, N. O.

AU - Zlobinsky, A. V.

PY - 2018/4/1

Y1 - 2018/4/1

N2 - The electrical resistivity and induced polarization (IP) methods are widely used in geological mapping, prospecting and exploration of mineral deposits, engineering geology, hydrogeology, archaeology, and geotechnical and environmental applications. Historically, these methods have formed the basis of the electrical prospecting technique. In these methods, a DC or low-frequency AC electrical current is introduced into the earth through a grounded transmitter line. The measured quantity is the electric field. However, if the earth's resistivity or chargeability changes horizontally, this change gives rise to an anomalous magnetic field, which is studied by the magnetometric resistivity (MMR) and magnetic induced polarization (MIP) methods, respectively. Along with advantages, some shortcomings are inherent in the MMR and MIP techniques. Apparently, the main drawback of these methods is that the magnetic fields of both the transmitter line wire and ground electrodes on the surface are several orders of magnitude greater than the anomalous magnetic field response. This introduces a significant “noise” to magnetic-resistivity data. We investigate the potential of using a circular electric dipole (CED) in magnetometric resistivity techniques. It has been found that the application of a CED, instead of a conventional transmitter line, dramatically enhances the signal-to-noise ratio.

AB - The electrical resistivity and induced polarization (IP) methods are widely used in geological mapping, prospecting and exploration of mineral deposits, engineering geology, hydrogeology, archaeology, and geotechnical and environmental applications. Historically, these methods have formed the basis of the electrical prospecting technique. In these methods, a DC or low-frequency AC electrical current is introduced into the earth through a grounded transmitter line. The measured quantity is the electric field. However, if the earth's resistivity or chargeability changes horizontally, this change gives rise to an anomalous magnetic field, which is studied by the magnetometric resistivity (MMR) and magnetic induced polarization (MIP) methods, respectively. Along with advantages, some shortcomings are inherent in the MMR and MIP techniques. Apparently, the main drawback of these methods is that the magnetic fields of both the transmitter line wire and ground electrodes on the surface are several orders of magnitude greater than the anomalous magnetic field response. This introduces a significant “noise” to magnetic-resistivity data. We investigate the potential of using a circular electric dipole (CED) in magnetometric resistivity techniques. It has been found that the application of a CED, instead of a conventional transmitter line, dramatically enhances the signal-to-noise ratio.

KW - circular electric dipole

KW - DC

KW - electrical prospecting

KW - magnetic field

KW - MIP

KW - MMR

KW - resistivity methods

UR - http://www.scopus.com/inward/record.url?scp=85045242896&partnerID=8YFLogxK

U2 - 10.1016/j.rgg.2018.03.011

DO - 10.1016/j.rgg.2018.03.011

M3 - Article

AN - SCOPUS:85045242896

VL - 59

SP - 432

EP - 437

JO - Russian Geology and Geophysics

JF - Russian Geology and Geophysics

SN - 1068-7971

IS - 4

ER -

ID: 12543026