关于S.P. Timoshenko型细弹冲击问题的一种方法

V. Bogdanov
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引用次数: 0

摘要

研究了求解第二类无穷积分方程组Volterra的输出动力学问题的方法及其解的收敛性。该方法已成功地应用于研究硬体和Kirchhoff-Love型弹性细壳对弹性半空间和层的冲击问题。本文尝试用求解第二类无穷积分方程组Volterra的输出动力学问题的方法,求解了S.P. Timoshenko型弹性细圆柱壳和球壳在弹性半空间上碰撞的平面和轴对称问题。利用数值积分的Gregory方法和求解第二类Volterra方程组的约简无穷系统的Adams方法进行离散化,得到一个定义不清的线性代数方程组:随着约简的大小增大,该方程组的行列式趋于无穷。这种方法不允许求解S.P. Timoshenko型细壳和弹性体的平面和轴对称动力学问题。结果表明,该方法不适用于本文研究的平面和轴对称问题。这表明了这种方法的局限性,并导致开发其他数学方法和模型的可行性。需要注意的是,为了在弹性阶段对弹塑性公式中的变形计算过程进行校正,使用输出动力学问题的技术来求解第二类无穷积分方程组Volterra是方便和方便的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
About one approach to the problems of impact of fine shells of the S.P. Timoshenko type
The method of the outcoming dynamics problems to solve an infinite system of integral equations Volterra of the second kind and the convergence of this solution are well studied. Such approach has been successfully used for cases of the investigation of problems of the impact a hard bodies and an elastic fine shells of the Kirchhoff–Love type on elastic a half-space and a layer. In this paper an attempt is made to solve the plane and the axisymmetric problems of the impact of an elastic fine cylindric and spheric shells of the S.P. Timoshenko type on an elastic half-space using the method of the outcoming dynamics problems to solve an infinite system of integral equations Volterra of the second kind. The discretization using the Gregory methods for numerical integration and Adams for solving the Cauchy problem of the reduced infinite system of Volterra equations of the second kind results in a poorly defined system of linear algebraic equations: as the size of reduction increases the determinant of such a system to aim at infinity. This technique does not allow to solve plane and axisymmetric problems of dynamics for fine shells of the S.P. Timoshenko type and elastic bodies. It is shown that this approach is not acceptable for investigated in this paper the plane and the axisymmetric problems. This shows the limitations of this approach and leads to the feasibility of developing other mathematical approaches and models. It should be noted that to calibrate the computational process of deformation in the elastoplastic formulation at the elastic stage, it is convenient and expedient to use the technique of the outcoming dynamics problems to solve an infinite system of integral equations Volterra of the second kind.
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