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IUGG XXIV General Assembly July 2-13, 2007 Perugia, Italy<br />

(S) - <strong>IASPEI</strong> - International Association of Seismology and Physics of the Earth's<br />

Interior<br />

JSS002 Poster presentation 1825<br />

Numerical simulation of tsunamis around Shanghai on the East China Sea<br />

Coast Due To Great Nankai, Japan, earthquakes<br />

Dr. Tomoya Harada<br />

Research Center for Urban Safety and Security Kobe University <strong>IASPEI</strong><br />

Katsuhiko Ishibashi<br />

There has been a controversy among Japanese scientists whether Chinas Shanghai and its vicinity on<br />

the East China Sea coast were struck by large tsunamis or not due to the great interplate Nankai<br />

earthquakes along the Pacific coast of southwest Japan. Chinese historical documents report remarkable<br />

water disturbances in rivers, canals, ponds and wells around Shanghai in 1498, 1707 and 1854. The<br />

dates in 1707 and 1854 coincide with those of the Nankai earthquakes and the date in 1498, with that<br />

of a large earthquake in southwest Japan. Tsuji and Ueda (1997) claimed that these water disturbances<br />

meant large tsunamis and that the 1498 earthquake had also been the Nankai earthquake. Utsu (1988)<br />

and Ishibashi (1998), on the contrary, considered the water disturbances not to be tsunamis but seiches<br />

caused by long-period seismic waves. In this study, in order to terminate this controversy, we carried<br />

out the numerical simulation of tsunami propagation in the East China Sea for the 1707 Hoei, the 1854<br />

Ansei and the 1946 Showa Nankai earthquakes, though the computation was the first-order<br />

approximation. We assumed six static fault models of the 1707, 1854 and 1946 earthquakes proposed<br />

by Ando (1975, 1982) and Aida (1979, 1981a, b). Tsunami propagations were computed by the finitedifference<br />

method for the liner long-wave equations in the area of 120-140E and 2036N using 1-minute<br />

bathymetry data provided by GEBCO. The time step of the computation is 3.0 sec to satisfy a stability<br />

condition of the grid system. The friction with Mannings roughness coefficient of 0.03 is provided at the<br />

ocean bottom where the water depth is shallower than 100m. Initial conditions of tsunami propagation<br />

are ocean bottom deformation due to earthquake faulting, which were computed by Okadas (1985)<br />

program. Concerning boundary conditions, the total reflection on the coast and open boundary to<br />

outside the computational area were used. As the results, tsunamis caused by great Nankai earthquakes<br />

propagate into the East China Sea mainly through the Tokara strait, and they reach the coast around<br />

Shanghai about nine hours after the earthquake occurrence. The tsunami height on the China coast is<br />

not large, less than 1 meter, even for presumably overestimated fault slip of the 1707 Hoei Nankai<br />

earthquake model. Thus, water disturbances recorded in China are considered not to be tsunamis but<br />

effects of seismic waves. However, it should be noted that tsunami and seismic effect due to the next<br />

Nankai earthquake, which is anticipated to recur around the middle of this century, may affect to<br />

considerable extent to the modernized society of China. We thank Yuichiro Tanioka for providing us his<br />

tsunami computation program.<br />

Keywords: tsunami simulation, east china sea, great nankai earthquake

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