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Hamiltonian Duality Equation on Three-Dimensional Problems of Magnetoelectroelastic Solids

机译:哈密​​尔顿二元方程对磁电弹性固体三维问题的二元性方程

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Hamiltonian system used in dynamics is introduced to formulate the three-dimensional problems of the transversely isotropic magnetoelectroelastic solids. The Hamiltonian dual equations in magnetoelectroelastic solids are developed directly from the modified Hellinger-Reissner variational principle derived from generalized Hellinger-Ressner variational principle with two classes of variables. These variables not only include such origin variables as displaces, electric potential and magnetic potential, but also include such their dual variables as lengthways stress, electric displacement and magnetic induction in the symplectic space. Similar to the Hamiltonian formulation in classic dynamics, the z coordinate is treated analogous to the time coordinate so that the method of separation of variables can be used. The governing equations are a set of first order differential equations in z, and the coefficient matrix of the differential equations is Hamiltonian in (x,y).
机译:引入动力学中使用的汉密尔顿系统以制定横向各向同性磁电弹性固体的三维问题。磁电弹性固体中的汉密尔顿双方程直接从改进的Hellinger-Reissner分解原理和两类变量导出的改进的Hellinger-Reissner分解原理开发。这些变量不仅包括这样的原始变量,也包括所取代,电位和磁电位,而且还包括诸如纵向空间中的宽度应力,电力位移和磁感应的这种双变量。与经典动态中的汉密尔顿建构类似,Z坐标类似于时间坐标,使得可以使用变量的分离方法。控制方程是Z中的一组第一阶微分方程,并且微分方程的系数矩阵是哈密顿IN(x,y)。

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