ULF magnetic emissions connected with under sea bottom earthquakes

Measurements of ULF electromagnetic disturbances were carried out in Japan before and during a seismic active period (1 February 2000 to 26 July 2000). A network consists of two groups of magnetic stations spaced apart at a distance of ≈140 km. Every group consists of three, 3-compone...

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Main Authors: V. S. Ismaguilov, Yu. A. Kopytenko, K. Hattori, P. M. Voronov, O. A. Molchanov, M. Hayakawa
Format: Article
Language:English
Published: Copernicus Publications 2001-01-01
Series:Natural Hazards and Earth System Sciences
Online Access:http://www.nat-hazards-earth-syst-sci.net/1/23/2001/nhess-1-23-2001.pdf
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spelling doaj-4ca13f989e3d43f7a550d7e53e5140012020-11-24T22:37:20ZengCopernicus PublicationsNatural Hazards and Earth System Sciences1561-86331684-99812001-01-0111/22331ULF magnetic emissions connected with under sea bottom earthquakesV. S. IsmaguilovYu. A. KopytenkoK. HattoriP. M. VoronovO. A. MolchanovM. HayakawaMeasurements of ULF electromagnetic disturbances were carried out in Japan before and during a seismic active period (1 February 2000 to 26 July 2000). A network consists of two groups of magnetic stations spaced apart at a distance of &#x2248;140 km. Every group consists of three, 3-component high sensitive magnetic stations arranged in a triangle and spaced apart at a distance of 4–7 km. The results of the ULF magnetic field variation analysis in a frequency range of <i>F</i> = 0.002–0.5 Hz in connection with nearby earth-quakes are presented. Traditional <i>Z</i>/<i>G</i> ratios (<i>Z</i> is the vertical component, <i>G</i> is the total horizontal component), magnetic gradient vectors and phase velocities of ULF waves propagating along the Earth’s surface were constructed in several frequency bands. It was shown that variations of the <i>R</i>(<i>F</i>) = <i>Z</i>/<i>G</i> parameter have a different character in three frequency ranges: <i>F</i><sub>1</sub> = 0.1 ± 0.005, <i>F</i><sub>2</sub> = 0.01 ± 0.005 and <i>F</i><sub>3</sub> = 0.005 ± 0.003 Hz. Ratio <i>R</i>(<i>F</i><sub>3</sub>)/<i>R</i>(<i>F</i><sub>1</sub>)</i> sharply increases 1–3 days before strong seismic shocks. Defined in a frequency range of <i>F</i><sub>2</sub> = 0.01 ± 0.005 Hz during nighttime intervals (00:00–06:00 LT), the amplitudes of <i>Z</i> and <i>G</i> component variations and the <i>Z</i>/<i>G</i> ratio started to increase &#x2248; 1.5 months before the period of the seismic activity. The ULF emissions of higher frequency ranges sharply increased just after the seismic activity start. The magnetic gradient vectors (<b>&#x2207; <i>B</i></b> &#x2248; 1 – 5 pT/km), determined using horizontal component data (<i>G</i> &#x2248; 0.03 – 0.06 nT) of the magnetic stations of every group in the frequency range <i>F</i> = 0.05 ± 0.005 Hz, started to point to the future center of the seismic activity just before the seismoactive period; furthermore they continued following space displacements of the seismic activity center. The phase velocity vectors (<i>V</i> &#x2248; 20 km/s for <i>F</i> = 0.0067 Hz), determined using horizontal component data, were directed from the seismic activity center. Gradient vectors of the vertical component pointed to the closest seashore (known as the 'sea shore' effect). The location of the seismic activity centers by two gradient vectors, constructed at every group of magnetic stations, gives an &#x2248; 10 km error in this experiment.http://www.nat-hazards-earth-syst-sci.net/1/23/2001/nhess-1-23-2001.pdf
collection DOAJ
language English
format Article
sources DOAJ
author V. S. Ismaguilov
Yu. A. Kopytenko
K. Hattori
P. M. Voronov
O. A. Molchanov
M. Hayakawa
spellingShingle V. S. Ismaguilov
Yu. A. Kopytenko
K. Hattori
P. M. Voronov
O. A. Molchanov
M. Hayakawa
ULF magnetic emissions connected with under sea bottom earthquakes
Natural Hazards and Earth System Sciences
author_facet V. S. Ismaguilov
Yu. A. Kopytenko
K. Hattori
P. M. Voronov
O. A. Molchanov
M. Hayakawa
author_sort V. S. Ismaguilov
title ULF magnetic emissions connected with under sea bottom earthquakes
title_short ULF magnetic emissions connected with under sea bottom earthquakes
title_full ULF magnetic emissions connected with under sea bottom earthquakes
title_fullStr ULF magnetic emissions connected with under sea bottom earthquakes
title_full_unstemmed ULF magnetic emissions connected with under sea bottom earthquakes
title_sort ulf magnetic emissions connected with under sea bottom earthquakes
publisher Copernicus Publications
series Natural Hazards and Earth System Sciences
issn 1561-8633
1684-9981
publishDate 2001-01-01
description Measurements of ULF electromagnetic disturbances were carried out in Japan before and during a seismic active period (1 February 2000 to 26 July 2000). A network consists of two groups of magnetic stations spaced apart at a distance of &#x2248;140 km. Every group consists of three, 3-component high sensitive magnetic stations arranged in a triangle and spaced apart at a distance of 4–7 km. The results of the ULF magnetic field variation analysis in a frequency range of <i>F</i> = 0.002–0.5 Hz in connection with nearby earth-quakes are presented. Traditional <i>Z</i>/<i>G</i> ratios (<i>Z</i> is the vertical component, <i>G</i> is the total horizontal component), magnetic gradient vectors and phase velocities of ULF waves propagating along the Earth’s surface were constructed in several frequency bands. It was shown that variations of the <i>R</i>(<i>F</i>) = <i>Z</i>/<i>G</i> parameter have a different character in three frequency ranges: <i>F</i><sub>1</sub> = 0.1 ± 0.005, <i>F</i><sub>2</sub> = 0.01 ± 0.005 and <i>F</i><sub>3</sub> = 0.005 ± 0.003 Hz. Ratio <i>R</i>(<i>F</i><sub>3</sub>)/<i>R</i>(<i>F</i><sub>1</sub>)</i> sharply increases 1–3 days before strong seismic shocks. Defined in a frequency range of <i>F</i><sub>2</sub> = 0.01 ± 0.005 Hz during nighttime intervals (00:00–06:00 LT), the amplitudes of <i>Z</i> and <i>G</i> component variations and the <i>Z</i>/<i>G</i> ratio started to increase &#x2248; 1.5 months before the period of the seismic activity. The ULF emissions of higher frequency ranges sharply increased just after the seismic activity start. The magnetic gradient vectors (<b>&#x2207; <i>B</i></b> &#x2248; 1 – 5 pT/km), determined using horizontal component data (<i>G</i> &#x2248; 0.03 – 0.06 nT) of the magnetic stations of every group in the frequency range <i>F</i> = 0.05 ± 0.005 Hz, started to point to the future center of the seismic activity just before the seismoactive period; furthermore they continued following space displacements of the seismic activity center. The phase velocity vectors (<i>V</i> &#x2248; 20 km/s for <i>F</i> = 0.0067 Hz), determined using horizontal component data, were directed from the seismic activity center. Gradient vectors of the vertical component pointed to the closest seashore (known as the 'sea shore' effect). The location of the seismic activity centers by two gradient vectors, constructed at every group of magnetic stations, gives an &#x2248; 10 km error in this experiment.
url http://www.nat-hazards-earth-syst-sci.net/1/23/2001/nhess-1-23-2001.pdf
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