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Coupled Simulation of Seismic Wave Propagation and Failure Phenomena by Use of an MPS Method
Authors:Junichi Takekawa  Hitoshi Mikada  Tada-nori Goto  Yoshinori Sanada  Yuzuru Ashida
Institution:1. Kyoto University, C1-1-111, Kyotodaigaku-Katsura, Nishikyo-ku, Kyoto, 615-8540, Japan
2. Kyoto University, C1-1-112, Kyotodaigaku-Katsura, Nishikyo-ku, Kyoto, 615-8540, Japan
3. Kyoto University, C1-1-113, Kyotodaigaku-Katsura, Nishikyo-ku, Kyoto, 615-8540, Japan
4. Japan Agency for Marine-Earth Science and Technology (JAMSTEC), 3173-25, Showa-machi, Kanazawa-ku, Yokohama, Kanagawa, 236-0001, Japan
5. Environment, Energy, Forestry and Agriculture Network (EEFA), Suzakuhaitsu4-G, 27-1, Mibusuzaku-cho, Nakakyo-ku, Kyoto, 604-8871, Japan
Abstract:The failure of brittle materials, for example glasses and rock masses, is commonly observed to be discontinuous. It is, however, difficult to simulate these phenomena by use of conventional numerical simulation methods, for example the finite difference method or the finite element method, because of the presence of computational grids or elements artificially introduced before the simulation. It is, therefore, important for research on such discontinuous failures in science and engineering to analyze the phenomena seamlessly. This study deals with the coupled simulation of elastic wave propagation and failure phenomena by use of a moving particle semi-implicit (MPS) method. It is simple to model the objects of analysis because no grid or lattice structure is necessary. In addition, lack of a grid or lattice structure makes it simple to simulate large deformations and failure phenomena at the same time. We first compare analytical and MPS solutions by use of Lamb’s problem with different offset distances, material properties, and source frequencies. Our results show that analytical and numerical seismograms are in good agreement with each other for 20 particles in a minimum wavelength. Finally, we focus our attention on the Hopkinson effect as an example of failure induced by elastic wave propagation. In the application of the MPS, the algorithm is basically the same as in the previous calculation except for the introduction of a failure criterion. The failure criterion applied in this study is that particle connectivity must be disconnected when the distance between the particles exceeds a failure threshold. We applied the developed algorithm to a suspended specimen that was modeled as a long bar consisting of thousands of particles. A compressional wave in the bar is generated by an abrupt pressure change on one edge. The compressional wave propagates along the interior of the specimen and is visualized clearly. At the other end of the bar, the spalling of the bar is reproduced numerically, and a broken piece of the bar is formed and falls away from the main body of the bar. Consequently, these results show that the MPS method effectively reproduces wave propagation and failure phenomena at the same time.
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