1) thermally uniaxial materials
热单轴各向异性介质
2) Uniaxial layered structure
单轴各向异性分层介质
3) Uniaxial anisotropic medium
单轴各向异性媒质
4) anisotropic medium
各向异性介质
1.
FCT finite difference modeling of three-component seismic records in anisotropic medium;
各向异性介质中三分量地震记录的FCT有限差分模拟
2.
Experimental researckes on shear wave characteristics in anisotropic medium;
各向异性介质中横波特征的实验研究
3.
Study of parallel FDTD algorithm for anisotropic medium on a PC cluster system;
电各向异性介质FDTD并行算法的研究
5) Anisotropic media
各向异性介质
1.
Using the wavefront spreading method to solve the eikonal equation for anisotropic media;
波前扩展法求解各向异性介质的程函方程
2.
Numeric simulation of S-wave splitting and second splitting in layered anisotropic media;
层状各向异性介质中横波分裂和再分裂数值模拟
3.
Aiming at the reflection of artifical boundary when simulating the seismic prospecting, this paper gives the absorbing boundary conditions for anisotropic media.
针对地震波勘探数值模拟中遇到的人为边界反射问题,提出了适用各种各向异性介质的吸收边界条件,证明了其稳定性,在频率域推出了反射系数算法。
6) anisotropic dielectric
各向异性介质
1.
In this paper,the coupling of finite element method(FEM) and boundary element method(BEM) is used to calculate radar cross section(RCS) by arbitrarily shaped two-dimensional conducting bodies coated with anisotropic dielectric.
应用有限元-边界元耦合法计算任意截面形状二维各向异性介质覆盖导体柱的雷达散射截面,对介质柱内、外区域分别应用有限元和边界元法进行分析,然后通过场的连续性进行耦合,形成待求矩阵方程,最后应用内观法结合多波前法求解该方程。
2.
A nonoverlapping domain decomposition method(DDM) and the finite element method(FEM)/boundary element method(BEM) are combined to analyze transverse electric(TE) wave scattering properties by a two-dimensional open cavity filled with the multilayer anisotropic dielectric.
应用非重叠型区域分解法(DDM)结合有限元法(FEM)和边界元法(BEM)分析了填充多层各向异性介质的二维开口腔体横电波(TE)散射特性。
3.
A domain decomposition method(DDM) and finite element method(FEM)/boundary integral method(BIM) are combined to analyze TM wave scattering property by two-dimensional open cavity filled with multiplayer anisotropic dielectric.
应用区域分解法(DDM)结合有限元(FEM)和边界积分法(BIM)分析了填充多层各向异性介质二维开口腔体TM波散射特性。
补充资料：单轴各向异性
单轴各向异性是磁晶各向异性的最简单形式，即自发磁化的稳定方向（或易磁化方向）平行于一特殊晶轴。如六方晶系钴的自发磁化方向平行于 C轴(见晶体结构)，这就表现出强的单轴各向异性。磁性材料的单轴各向异性值一般都低于其磁晶各向异性值，为103erg/cm3量级。磁性材料经磁场热处理或强的冷加工而产生的感生各向异性，都属于单轴各向异性。
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