摘要
横观各向同性电磁弹性固体的耦合特征由5个关于弹性位移、电位和磁位的二阶偏微分方程控制· 基于势函数理论,耦合的方程组被简化为5个非耦合的关于势函数的广义Laplace方程· 弹性场和电磁场由势函数表示。
The coupling feature of transversely isotropic magnetoelectroelastic solids are governed by a system of five partial differnetial equations with respect to the elastic displacements,the electric potential and the magnetic potential.Based on the potential theory,the coupled equations are reduced to the five uncoupled generalized Laplace equations with respect to five potential functions.Further,the elastic fields and electromagnetic fields are expressed in terms of the potential functions.These expressions constitute the general solution of transversely isotropic magnetoelectroelastic media.
出处
《应用数学和力学》
EI
CSCD
北大核心
2003年第7期684-690,共7页
Applied Mathematics and Mechanics
关键词
电磁弹性固体
一般解
势函数
magnetoelectroelastic solids
general solution
potential function
