1) magnetoelectroelastic solid
电磁弹性固体
1.
Symplectic solution system and Saint-Venant principle on anti-plane problem of magnetoelectroelastic solids;
电磁弹性固体反平面问题辛求解体系及圣维南原理
2.
By means of the generalized variable principle of magnetoelectroelastic solids,the plane magnetoelectroelastic solids problem was derived to Hamiltonian system.
从电磁弹性固体广义变分原理出发,将平面电磁弹性固体问题导入Hamilton体系。
2) magnetoelectroelastic solids
电磁弹性固体
1.
A virtual boundary element-equivalent collocation method(VBEM) for 3D magnetoelectroelastic solids is proposed based on the fundamental solutions of magnetoelectroelastic solids and the virtual boundary element method for elasticity.
依据弹性力学虚边界元法的基本思想和电磁弹性固体的基本解,提出了电磁弹性固体三维问题的虚边界元-等额配点法。
2.
Based on the fundamental equations of the plane magnetoelectroelastic solids and the basic idea of virtual boundary element method for elasticity, a virtual boundary element—least square collocation method (VBEM) for plane magnetoelectroelastic solids is presented.
从电磁弹性固体平面问题的基本方程出发,依据弹性力学虚边界元法的基本思想,利用电磁弹性固体平面问题的基本解,提出了电磁弹性固体平面问题的虚边界元——最小二乘配点法。
3.
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.
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,这构成了横观各向同性电磁弹性固体的一般解·
3) magnetoelectroelastic body
磁电弹性体
4) magneto-electro-elastic media
压电、压磁弹性体
5) magneto-electro-thermo-elastic
电磁热弹性体
1.
The research on classical problems for thermoelastic、piezothermoelastic and magneto-electro-thermo-elastic structures not only can provide the analytical solution for engineering applications but also acts as the necessary benchmarks for various approximate theories and calculation methods.
本文分别以热弹性体、压电热弹性体和电磁热弹性体为研究对象,研究它们在耦合载荷作用下的全场解析解。
6) magnetic and elastic body
磁弹性体
补充资料：弹性固体
分子式：
CAS号：
性质： 能够产生可逆的弹性变形的固体。在外力作用下，改变物体的形状和尺寸，产生变形；外力除去后，变形完全回复。如果形变的产生与回复与时间无关，称为理想的弹性固体；如果与时间有关，则称为非理想的弹性固体，也称黏弹体。
CAS号：
性质： 能够产生可逆的弹性变形的固体。在外力作用下，改变物体的形状和尺寸，产生变形；外力除去后，变形完全回复。如果形变的产生与回复与时间无关，称为理想的弹性固体；如果与时间有关，则称为非理想的弹性固体，也称黏弹体。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条