1) repeated similar sub-domain
重复相似子域法
1.
The boundary node method was used for a 2-D numerical analysis of a piezoelectric composite material with regular shaped inclusions using the repeated similar sub-domain approach.
针对含规则形状夹杂的压电复合材料平面问题,将边界点法和重复相似子域法相结合,实现了一种用于含有大量圆形夹杂的横观各向同性压电复合材料的分析方法,并通过相应的计算模型求得压电复合材料的等效材料性质。
2) reduplicate multi-sub-region
重复子域法
3) similar sub-domain
相似子域
1.
Based on the similarity of integration area of random inclusions, similar sub-domain boundary element method scheme has been presented for the first time in this paper.
根据夹杂相积分区域的相似性 ,提出了相似子域边界元法求解方案。
4) boundary element duplicated sub domain method
重复子域边界元法
1.
This paper deduced the basic formulae of the 2 D boundary element duplicated sub domain method and formulae of the coupling method of 2 D boundary element with finite element sub structure, taking account of peculiarity of duplicated open corner structure.
针对具有重复结构的开口角隅应力集中问题建立了重复子域边界元法及有限元子结构与边界元耦合求解的基本列式，编制了相应的计算程序并进行了考题检
5) similarity factor method
相似因子法
1.
The experiment data were analyzed by similarity factor method and Regter Peppas .
方法:转篮法,用紫外分光光度法检测,描绘其三维释放图像,将释放数据用相似因子法、Peppas方程进行分析。
2.
The accumul ation release percentage of tramadol hydrochloride sustained-release tablets un der the different pH conditions was determined by ultraviolet spectrophotometry at λ=270nm, then the release characteristics were explored by similarity factor method, Zero grade model, First grade mod.
方法 转篮法,用紫外分光光度法检测,描绘其三维释放图像,对释放数据分别用相似因子法分析,以零级,一级,Higuchi,Peppas方程进行拟合。
3.
Also the media were selected,then the release equations were established,which were compared to an imported preparation with similarity factor method.
方法 湿法制粒压制双层片 ,HPLC检测释放度 ,并对释放介质进行筛选 ,建立了释药方程 ,采用相似因子法与国外制剂进行比较。
6) similar factor
相似因子法
1.
The similar factor was 84.
方法 :桨法 ,高效液相色谱法检测 ,提取溶出参数T50 、Td、m进行统计分析 ,并采用相似因子法评价试验药品和进口对照品溶出度的相似程度。
2.
The similar factor was 81.
方法桨法,蒸馏水为溶出介质,用HPLC检测,计算累积溶出百分率,提取溶出参数(T50,Td,m)进行统计分析,并采用相似因子法评价试验药品和进口对照药品溶出度的相似程度。
补充资料：超导电性的局域和非局域理论（localizedandnon-localizedtheoriesofsuperconductivity）
超导电性的局域和非局域理论（localizedandnon-localizedtheoriesofsuperconductivity）
伦敦第二个方程（见“伦敦规范”）表明，在伦敦理论中实际上假定了js(r)是正比于同一位置r的矢势A(r)，而与其他位置的A无牵连；换言之，局域的A(r)可确定该局域的js(r)，反之亦然，即理论具有局域性，所以伦敦理论是一种超导电性的局域理论。若r周围r'位置的A(r')与j(r)有牵连而影响j(r)的改变，则A(r)就为非局域性质的。由于`\nabla\timesbb{A}=\mu_0bb{H}`，所以也可以说磁场强度H是非局域性的。为此，超导电性需由非局域性理论来描绘，称超导电性的非局域理论。皮帕德非局域理论就是典型的超导电性非局域唯象理论。
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