Drag-out effect of piezomagnetic signals due to a borehole: the Mogi source as an example
Author(s)
Date Issued
February 2007
Issue/vol(year)
1/50 (2007)
Language
English
Abstract
We show that using borehole measurements in tectonomagnetic experiments allows enhancement of the observed
signals. New magnetic dipoles, which vary with stress changes from mechanical sources, are produced
on the walls of the borehole. We evaluate such an effect quantitatively. First we formulate a general expression
for the borehole effect due to any arbitrary source models. This is valid everywhere above the ground surface as
well as within the cylindrical hole. A first-order approximate solution is given by a line of horizontal dipoles and
vertical quadrupoles along the central axis of the borehole, which is valid above the ground surface and a slightly
away (several tens of cm) from the top of the borehole. Selecting the Mogi model as an example, we numerically
evaluated the borehole effect. It turned out that the vertical quadrupoles produce two orders of magnitude
more intense magnetic field than the horizontal dipoles. The borehole effect is very local, i.e. detectable only
within a few m from its outlet, since it is of the same order or more than the case without a borehole. However,
magnetic lines of force cannot reach the ground surface from a deeper portion (>10 m) of a borehole.
signals. New magnetic dipoles, which vary with stress changes from mechanical sources, are produced
on the walls of the borehole. We evaluate such an effect quantitatively. First we formulate a general expression
for the borehole effect due to any arbitrary source models. This is valid everywhere above the ground surface as
well as within the cylindrical hole. A first-order approximate solution is given by a line of horizontal dipoles and
vertical quadrupoles along the central axis of the borehole, which is valid above the ground surface and a slightly
away (several tens of cm) from the top of the borehole. Selecting the Mogi model as an example, we numerically
evaluated the borehole effect. It turned out that the vertical quadrupoles produce two orders of magnitude
more intense magnetic field than the horizontal dipoles. The borehole effect is very local, i.e. detectable only
within a few m from its outlet, since it is of the same order or more than the case without a borehole. However,
magnetic lines of force cannot reach the ground surface from a deeper portion (>10 m) of a borehole.
References
EASON, G., B. NOBLE and I.N. SNEDDON (1955): On certain
integrals of Lipschitz-Hankel type involving products
of Bessel functions, Phil. Trans. R. Soc. London Ser. A,
247, 529-551.
HASHIMOTO, T.,Y. TANAKA, M.J.S. JOHNSTON, M. UTSUGI, Y.
SASAI and S. SAKANAKA (2003): On the annual variations
in geomagnetic differences observed in Long Valley
Caldera, California, Ann. Disas. Prev. Res. Inst., Kyoto
Univ., 46B, 765-777 (in Japanese with English abstract).
JOHNSTON, M.J.S., D.P. HILL and A.M. PITT (2000): Strain
transient recorded in the Long Valley Caldera during
triggered seismicity from the October 16, 1999, M 7.1
Hector Mine, California, earthquake, Eos, Trans. Am.
Geophys. Un., 81, WP1384.
MOGI, K. (1958): Relations between the eruptions of various
volcanoes and the deformations of the ground surfaces
around them, Bull. Earthqake Res. Inst., Univ.
Tokyo, 36, 99-134.
MUELLER, R. and M.J.S. JOHNSTON (1998): Review of magnetic
field monitoring near active faults and volcanic
calderas in California: 1974-1995, Phys. Earth Planet.
Inter., 105, 131-144.
SASAI, Y. (1983): A surface integral representation of the
tectonomagnetic field based on the linear piezomagnetic
effect, Bull. Earthq. Res. Inst., Univ. Tokyo, 58, 763-785.
SASAI, Y. (1991a): Piezomagnetic field associated with the
Mogi model revisited: analytic solution for finite
spherical source, J. Geomag. Geoelectr., 43, 21-64.
SASAI, Y. (1991b): Tectonomagnetic modeling on the basis
of the linear piezomagnetic effect, Bull. Earthquake
Res. Inst., Univ. Tokyo, 66, 585-722.
SASAI, Y. (1994): Enhancement of piezomagnetic signals
within a borehole, in Electromagnetic Phenomena Related
to Earthquake Prediction, edited by M. HAYAKAWA
and Y. FUJINAWA (Terra Scientific Publishing Co.,
Tokyo), 51-54.
UTADA, H., M. NEKI and T. KAGIYAMA (2000): A study of
annual variations in the geomagnetic total intensity
with special attention to detecting volcanomagnetic
signals, Earth Planets Space, 52, 91-103.
UTSUGI, M., Y. NISHIDA and Y. SASAI (2000): Piezomagnetic
potentials due to an inclined rectangular fault in a semi-
infinite medium, Geophys. J. Int., 140, 479-492.
YAMAMOTO, T. (1990): Geomagnetic three components observations
using a borehole, in Proceedings of Conductivity
Anomaly Symposium, 187-194 (in Japanese).
integrals of Lipschitz-Hankel type involving products
of Bessel functions, Phil. Trans. R. Soc. London Ser. A,
247, 529-551.
HASHIMOTO, T.,Y. TANAKA, M.J.S. JOHNSTON, M. UTSUGI, Y.
SASAI and S. SAKANAKA (2003): On the annual variations
in geomagnetic differences observed in Long Valley
Caldera, California, Ann. Disas. Prev. Res. Inst., Kyoto
Univ., 46B, 765-777 (in Japanese with English abstract).
JOHNSTON, M.J.S., D.P. HILL and A.M. PITT (2000): Strain
transient recorded in the Long Valley Caldera during
triggered seismicity from the October 16, 1999, M 7.1
Hector Mine, California, earthquake, Eos, Trans. Am.
Geophys. Un., 81, WP1384.
MOGI, K. (1958): Relations between the eruptions of various
volcanoes and the deformations of the ground surfaces
around them, Bull. Earthqake Res. Inst., Univ.
Tokyo, 36, 99-134.
MUELLER, R. and M.J.S. JOHNSTON (1998): Review of magnetic
field monitoring near active faults and volcanic
calderas in California: 1974-1995, Phys. Earth Planet.
Inter., 105, 131-144.
SASAI, Y. (1983): A surface integral representation of the
tectonomagnetic field based on the linear piezomagnetic
effect, Bull. Earthq. Res. Inst., Univ. Tokyo, 58, 763-785.
SASAI, Y. (1991a): Piezomagnetic field associated with the
Mogi model revisited: analytic solution for finite
spherical source, J. Geomag. Geoelectr., 43, 21-64.
SASAI, Y. (1991b): Tectonomagnetic modeling on the basis
of the linear piezomagnetic effect, Bull. Earthquake
Res. Inst., Univ. Tokyo, 66, 585-722.
SASAI, Y. (1994): Enhancement of piezomagnetic signals
within a borehole, in Electromagnetic Phenomena Related
to Earthquake Prediction, edited by M. HAYAKAWA
and Y. FUJINAWA (Terra Scientific Publishing Co.,
Tokyo), 51-54.
UTADA, H., M. NEKI and T. KAGIYAMA (2000): A study of
annual variations in the geomagnetic total intensity
with special attention to detecting volcanomagnetic
signals, Earth Planets Space, 52, 91-103.
UTSUGI, M., Y. NISHIDA and Y. SASAI (2000): Piezomagnetic
potentials due to an inclined rectangular fault in a semi-
infinite medium, Geophys. J. Int., 140, 479-492.
YAMAMOTO, T. (1990): Geomagnetic three components observations
using a borehole, in Proceedings of Conductivity
Anomaly Symposium, 187-194 (in Japanese).
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