日本地球惑星科学連合2014年大会

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セッション記号 S (固体地球科学) » S-SS 地震学

[S-SS30_28PM2] 海溝型巨大地震の新しい描像

2014年4月28日(月) 16:15 〜 18:00 メインホール (1F)

コンビーナ:*金川 久一(千葉大学大学院理学研究科)、古村 孝志(東京大学大学院情報学環総合防災情報研究センター)、小平 秀一(海洋研究開発機構 地球内部ダイナミクス領域)、宍倉 正展(産業技術総合研究所 活断層・地震研究センター)、座長:井出 哲(東京大学大学院理学系研究科地球惑星科学専攻)

16:45 〜 17:00

[SSS30-20] 沈み込み帯でのプレート境界面破壊に関する構造力学モデル

*江口 孝雄1 (1.防衛大学校 地球海洋学科)

キーワード:沈み込み帯, プレート間相互作用, 構造力学, 系の破壊確率, 系の安全確率

There are unidentified and unveiled properties concerning the physical process of greater inter-plate earthquakes at subduction zones. We, here, present a stochastic fracture model of the plate-interface with dynamic discrete interaction blocks. The stochastic treatment in this study is mainly based on structural mechanics. Here, in the four-dimensional point of view, regarded as significant long-wavelength components of the mechanical inter-plate coupling, we assign several discrete lattice-like blocks being connected each other on a hypothesized plate boundary system. The representative mechanical interaction vector (or tensor) for each discrete block should be variable on the plate boundary system. The total number of the discrete blocks and their nesting pattern should also vary with time during the long-term subduction process with intermittent greater seismic events.Hereafter, we treat the inter-plate coupling at discrete blocks, using parameters such as failure probability (Psf) and safe probability (Pss) of the total system of the plate boundary. Here, Psf + Pss = 1.The system fracture for the case of parallel connecting blocks is defined as the breakdown of all parallel blocks. Whereas, for the case of a series connecting block system, the system fracture is defined as the failure of one of the series block, or more. The system failure probability of a simple mechanical system being coupled in parallel N blocks is given as a product of p(i) from i = 1 to i = N. Here, p(i) is the failure probability of the i-th block of the system. For the case of a mechanical system connected in series N blocks, the system safe probability becomes a product of {1-p(i)} from i = 1 to i = N. For a mechanical system composed of both parallel and series blocks, the system failure probability and system safe probability can be estimated with the above definition. Then, we assume that the inter-plate shear coupling of the plate-interface progresses only at discrete blocks of brittle fracture. We consider two different configuration models for a two-by-four matrix (2x4) system of discrete coupling blocks, consist of four columns in the trench-parallel direction and two rows of deep side and a shallow side in the dip direction, as follows.Configuration model A is a series-connected system of both the shallower parallel-connected column blocks and the deeper parallel-connected ones.Configuration model B is a parallel-connected system of the four columns of the shallower and deeper rows being directly series-connected in the dip direction.By setting the failure probability, p(i,j), of (i,j)-th block, we can estimate the system failure probability (Psf) and system safe probability (Pss) for the configuration models, A and B. For the configuration models A and B, the system safe probability, Pss(A) and Pss(B) can be obtained. In the case of p(i,j) less than 0.5 for all blocks, Pss(A) becomes larger than Pss(B), indicating that the configuration model A is safer than the model B. When the representative pattern of the inter-plate coupling changes from the configuration model A to B, or vice versa, we should carefully estimate the system probabilities.We also demonstrated the detailed hypothetical expression form of p(i,j) by considering the effect of preceding larger seismic ruptures at blocks and the subsequent healing process, etc.