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Asymptotic solutions for mode II dynamic rupture with nonlinear damping

机译:具有非线性阻尼的II型动力破裂的渐近解

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In this study, the nonlinear Rayleigh damping (A.H. Nayfeh, Introduction to Perturbation Techniques, Wiley, New York, 1981, pp.147-150, 216-230) is adopted, and the governing equations are two coupled nonlinear PDEs, their unknown functions bearing the amplitude components in x and y directions, respectively. By assuming the unknown functions to be proper vibration pattern functions which fulfill all the boundary conditions, transforming the fixed coordinates into the moving coordinates by Galieo transformation and applying the calculation of Fourier series, the two nonlinear PDEs are reduced to four nonlinear ODEs. Among them, a couple are of order 1, the rest are of order 2. In order to be able to solve them analytically, the nonlinear forms in one ODE of order 1 for the secondary amplitude v are neglected in the first iterative calculation and the rupture velocity is assumed to be a constant value, and the coupled term in one of the order two ODEs to be 0. Then the remaining order two ODEs is reduced to be a homogeneous van der Pol equation. Its solution is readily obtained. Substituting this known function into the other order two ODEs for the unknown function u, it is reduced to be a nonhomogenous van der Pol equation. Its solution is also unknown.
机译:在这项研究中,采用了非线性瑞利阻尼(AH Nayfeh,《微扰技术概论》,威利,纽约,1981年,第147-150页,第216-230页),并且控制方程是两个耦合的非线性PDE,其未知函数分别在x和y方向上承载振幅分量。通过将未知函数假定为满足所有边界条件的适当振动模式函数,通过Galieo变换将固定坐标转换为运动坐标,并应用傅立叶级数的计算,将两个非线性PDE简化为四个非线性ODE。其中,一对为1阶,其余为2阶。为了能够解析地求解它们,在第一次迭代计算中忽略了二次振幅v的一个1阶ODE中的非线性形式。假定破裂速度为常数,并且两个ODE阶之一中的耦合项为0。然后将其余两个ODE简化为齐次Van der Pol方程。它的解决方案很容易获得。将该已知函数代入未知函数u的其他两个ODE中,它被简化为非齐次的van der Pol方程。其解决方案也是未知的。

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