Numerical simulation of formation process and snap-back for a fault band and elastic rock system
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摘要: 采用FLAC模擬了斷層-圍巖系統的形成過程及位移的分布規律.計算中采用了莫爾-庫侖與拉破壞復合的破壞準則,峰后巖石本構關系為線性應變軟化.兩條斷層帶(或剪切帶)匯交時系統形成,之后其承載能力下降.在斷層帶左側,由于在系統承載能力降低的過程中,彈性應變的快速恢復,出現了快速回跳現象(系統失穩).在斷層帶之外,位移分布是均勻的.在斷層帶位置,存在較大的位移梯度.系統承載能力越低,位移梯度越大.遠離加載端的區域先回跳,然后回跳區域逐漸擴大,向加載端傳播,直到整個系統都回跳.上述過程持續的時間步數較少,說明了系統失穩的突發性.系統整體回跳發生于應變軟化階段.Abstract: The formation process of the system composed of fault band and elastic rock block and the shear displacement distribution across a fault band were modeled numerically by FLAC. The adopted failure criterion was a composite Mohr-Coulomb criterion with tension cut-off and the post-peak constitutive relation of rock was linear strain-softening. Once two shear bands combine to form a fault band, the system is formed, subsequently leading to the decrease in load-carrying capacity of the system. On one side of the fault band, snap-back occurs due to the sharp recovery of elastic strain in strain-softening process, indicating the unstable failure. Nearly uniform displacement distribution is observed outside the fault band. A higher displacement gradient exists within the band and increases with the decrease in load-carrying capacity of the system. Snap-back of the zone far away from the loading end is the earliest. Then, the size of the snap-back zone propagating towards the loading end increases until snap-back of the entire system takes place. The process only needs a few time steps, reflecting the abrupt occurrence of instability of the system. Snap-back of the entire system occurs in the strain-softening stage of a stress-strain curve.
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