1) singular electro-elastic fields
奇异电弹性场
2) singular electromechanical field
电弹性场奇异性
3) elastic/nonlinear viscous singular field
弹/非线粘性奇异场
5) electroelastic field
电弹性场
1.
The entire electroelastic field and the asymptotic field near the inclusion tip were obtained under four types of combined mechanical and electric loadi.
在无穷远处受 4种机电组合载荷之一作用下 ,获得了整个平面内的电弹性场和夹杂端点附近处渐近的奇异场 ,并给出了奇异性系数的表达式 。
2.
By solving the resulting equations,the explicit analytic expressions for electroelastic field near to the inclusion tip were obtained.
利用积分变换法将动载荷下嵌入在无穷压电材料中的包体问题化为对偶积分方程组,求解这些方程组可以获得包体尖端附近电弹性场的明显解释表达式。
3.
Solving the resulting equations, the explicit analytic expressions for electroelastic field along the crack line and the intensity factors of relevant quantities near the crack tip and the mechanical strain energy release rate were o.
对受 4种机电载荷的内含裂纹的压电陶瓷板的电弹性行为进行了分析· 利用积分变换方法将非电渗透型反平面裂纹问题化为对偶积分方程组 ,求解这些方程组可以获得裂纹线上电弹性场的明显解析表达式 ,及裂尖处一些量的强度因子和机械应变能释放率· 当板的厚度趋近于无穷大时 ,所得结果还原为熟知结
6) singular field
奇异场
1.
With the constitutive equation supplied by Knowles and Sternberg and the sector division method the large deformation analysis of stress singular field near the notch, a typical defect of rubber-like material under the condition of plane strain is performed.
采用 Knowles和 Sternberg的本构方程,应用分区法,对平面应变情况下橡胶类材 料典型缺陷一缺口附近的应力奇异场进行了大变形分析。
补充资料:场致发光材料(见电致发光材料)
场致发光材料(见电致发光材料)
electroluminescent material
见场致发光材料eleetrolumineseent material 电致发光材料。
说明:补充资料仅用于学习参考,请勿用于其它任何用途。
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