说明:双击或选中下面任意单词,将显示该词的音标、读音、翻译等;选中中文或多个词,将显示翻译。
您的位置:首页 -> 词典 -> Scott-域
1)  Scotl-Domain
Scott-域
2)  Scott power supply
Scott供电
1.
Regarding the problems found in electric glass furnaces with Scott power supply which are not completely symmetrical, the author calculates the rules of variation of the equivalent current between the electrodes in this case and analyzes the reasons for the problems.
针对玻璃电熔窑电极非完全对称布置下采用Scott供电时所出现的问题,通过电工理论分析,计算非完全对称布置下 Scott供电的电极间内部等效电流的变化规律,从供电的角度分析问题可能出现的原因,证明传统的完全对称的布置方式供电更合理、更有利于玻璃熔制。
3)  modified scott wiring technique
改良Scott法
4)  SCOTT transformer
SCOTT变压器
1.
Based on the electromagnetics analysis of the SCOTT transformer, this paper derives its voltage equations and presents the transformer protection principle, operation equations and operation characteristics.
根据对SCOTT变压器的电磁分析,推导出了其电压平衡方程,进而提出了基于变压器模型的保护理论、动作方程和动作特性,并指出了动作方程参数整定的指导原则。
2.
Based on the principle and fundamental formula of Scott transformer, it presents a internal fault model which composed of 2 single-phase transformers, analyzes the relationship between port voltage of single-phase transformer and power voltage when faults occur and simulates internal fault current and magnetizing inrush current.
结合Scott变压器接线原理与基本方程,建立了由2个单相变压器组成的Scott变压器的内部故障仿真模型,分析了故障发生时单相变压器各端口电压同三相电源之间的关系,仿真计算了其内部故障电流及励磁涌流。
5)  Scott topology
Scott拓扑
1.
The duals of Hausdorff topology and Scott topology;
Hausdorff拓扑与Scott拓扑的对偶
2.
Scott Convergence of Nets and Filters and the Scott Topology on Posets
偏序集中网和滤子的Scott收敛及其Scott拓扑
3.
The paper introduce the concept of S-limit on local dcpo, and S-limit is used to carve Scott topology and continuous local directed complete poset.
在局部dcpo上引入了S极限的概念,并利用S极限来刻划Scott拓扑和连续的局部dcpo。
6)  smei-Scott closed sets
半Scott闭集
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