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Ionosphere plasma bubbles and density variations induced by pre-earthquake rock currents and associated surface charges
by
Joyce, G.
, Huba, J. D.
, Lee, L. C.
, Kuo, C. L.
in
Atmosphere
/ Atmospheric sciences
/ Bubbles
/ earthquake precursor
/ Earthquake prediction
/ Earthquakes
/ Electric fields
/ equatorial spread F
/ Ionosphere
/ ionospheric dynamics
/ plasma bubble
/ Rocks
/ Seismic activity
/ total electron content
2011
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Ionosphere plasma bubbles and density variations induced by pre-earthquake rock currents and associated surface charges
by
Joyce, G.
, Huba, J. D.
, Lee, L. C.
, Kuo, C. L.
in
Atmosphere
/ Atmospheric sciences
/ Bubbles
/ earthquake precursor
/ Earthquake prediction
/ Earthquakes
/ Electric fields
/ equatorial spread F
/ Ionosphere
/ ionospheric dynamics
/ plasma bubble
/ Rocks
/ Seismic activity
/ total electron content
2011
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Do you wish to request the book?
Ionosphere plasma bubbles and density variations induced by pre-earthquake rock currents and associated surface charges
by
Joyce, G.
, Huba, J. D.
, Lee, L. C.
, Kuo, C. L.
in
Atmosphere
/ Atmospheric sciences
/ Bubbles
/ earthquake precursor
/ Earthquake prediction
/ Earthquakes
/ Electric fields
/ equatorial spread F
/ Ionosphere
/ ionospheric dynamics
/ plasma bubble
/ Rocks
/ Seismic activity
/ total electron content
2011
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Ionosphere plasma bubbles and density variations induced by pre-earthquake rock currents and associated surface charges
Journal Article
Ionosphere plasma bubbles and density variations induced by pre-earthquake rock currents and associated surface charges
2011
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Overview
Recent ionospheric observations indicate that the total electron content (TEC) may anomalously decrease or increase up to 5–20% before the occurrence of big earthquakes. The ionospheric density variations can be caused by earth surface charges/currents produced from electric currents associated with the stressed rock. We formulate a coupling model for the stressed rock‐Earth surface charges‐atmosphere‐ionosphere system. The stressed‐rock acts as the dynamo to provide the currents for the coupling system. The electric fields and currents in the atmosphere and the lower boundary of ionosphere are obtained by solving the current continuity equation, ∇ • J = 0, where J is the current density. A three‐dimensional ionosphere simulation code is then used to study the ionospheric dynamics based on the obtained electric fields and currents. The simulation results show that a current density Jrock = 0.2–10 μA/m2 in an earthquake fault zone is required to cause daytime TEC variations of 2–25%. The simulation results also show that a current density Jrock = 0.01–1 μA/m2 can lead to nighttime TEC variations of 1–30% as well as the formation of a nighttime plasma bubble (equatorial spread F) extending over the whole magnetic flux tube containing the earthquake epicenter. We suggest that observations of daytime and nighttime TEC variations and a nighttime plasma bubble within the affected region can be used as precursors for earthquake prediction. Key Points Stressed rock current density 0.2–10 μA/m2 causes daytime TEC variations 2–25% Stressed rock current density 0.01–1 μA/m2 causes nighttime TEC variations 1–30% Stressed rock current can lead to formation of the nighttime plasma bubbles
Publisher
Blackwell Publishing Ltd
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