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Amplification of tsunami heights by delayed rupture of great earthquakes along the Nankai trough
Author(s) -
Kentaro Imai,
Kenji Satake,
Takashi Furumura
Publication year - 2010
Publication title -
earth planets and space
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.835
H-Index - 74
eISSN - 1880-5981
pISSN - 1343-8832
DOI - 10.5047/eps.2009.12.005
Subject(s) - geology , bay , seismology , tsunami earthquake , trough (economics) , tsunami wave , channel (broadcasting) , oceanography , engineering , electrical engineering , economics , macroeconomics
We investigated the effect of delayed rupture of great earthquakes along the Nankai trough on tsunami heights on the Japanese coast. As the tsunami source, we used a model of the 1707 Hoei earthquake, which consists of four segments: Tokai, Tonankai, and two Nankai segments. We first searched for the worst case, in terms of coastal tsunami heights, of rupture delay time on each segment, on the basis of superposition principle for the linear long wave theory. When the rupture starts on the Tonankai segment, followed by rupture on the Tokai segment 21 min later, as well as the eastern and western Nankai segments 15 and 28 min later, respectively, the average coastal tsunami height becomes the largest. To quantify the tsunami amplification, we compared the coastal tsunami heights from the delayed rupture with those from the simultaneous rupture model. Along the coasts of the sea of Hyu’uga and in the Bungo Channel, the tsunami heights become significantly amplified (>1.4 times larger) relative to the simultaneous rupture. Along the coasts of Tosa Bay and in the Kii Channel, the tsunami heights become amplified about 1.2 times. Along the coasts of the sea of Kumano and Ise Bay, and the western Enshu coast, the tsunami heights become slightly smaller for the delayed rupture. Along the eastern Enshu coast, the coast of Suruga Bay, and the west coast of Sagami Bay, the tsunami heights become amplified about 1.1 times.

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