面电荷密度
- 网络surface charge density;Charge Area Density;CHRGS;Charge Areal Density
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分析V形槽静电超声传感器微气隙结构研究静电场不均匀性,用解拉普拉斯方程的方法解的单个V形槽面电荷密度。
In this paper , by analyzing micro air-gap structure for electrostatic ultrasonic transducers with V-grooved backplates , a research on electrostatic field asymmetry of ultrasonic transducers is indicated . A single V-grooved surface charge density is solved by solving Laplace 's equation .
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导体椭球的面电荷密度和曲率的关系
The relationship between the surface charge density and curvature for an ellipsoidal conductor
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分析了得到的各原子分态密度、面电荷密度分布以及表面能带结构等性质,比较了GaN(001)的Ga端表面和N端表面两种情况。
Atomic partial densities of states , charge density distributions , and surface band structures are calculated and analyzed on both Ga terminated surface and N terminated surface .
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研究表明用密度泛函理论预测的不同膜面电荷密度和不同离子直径比情况下离子在半透膜附近密度分布与MonteCarlo模拟数据符合得很好。
The ionic density profiles predicted by the density functional theory are in excellent agreement with Monte Carlo results for various membrane surface charge densities and ionic diameter ratios .
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Al一Ag二元合金在时效过程中的亚稳相尸(AgZAI)相(。001)面的界面与基体一Al(111)面的面电荷密度连续,对合金起到了强化的作用。
On the interphase boundaries between the matrix and the precipitate y ' ( Ag2Al ) ( 0001 ) , electronic density is continued in Al-Ag binary alloy . The functions of aging hardening are remarkable in the alloy .
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参数保角变换与孤立导体面电荷密度
On Conformal Transformation by Parameter and Charge Density on the Surface of an Isolated Conductor
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带电导体椭球的面电荷密度与主曲率半径的关系
The relation between the surface charge density of a charged ellipsoidal conductor and its principal radii
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用一种新方法,计算了孤立导体旋转椭球的面电荷密度、电容、电势和电场强度,并得出相应的解析表达式。
By using a new method , the surface charge density , electric capacity , electric potential and electric field intensity will be calculated of the isolated revolving spheroid with the relevant expression of solution obtained .
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本文利用电象法给出了两个接触球孤立带电导体的电容、电势及面电荷密度分布和曲率的关系。
Using the method of images , this paper gives the capacitance , the potential , and the relation between the surface charge distribution and the curvature for an isolated charged conductor of two contacting spheres .
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通过对导体椭球面的面电荷密度的计算与讨论,说明了带电导体的电荷面密度分布的不均匀性。
The calculation and analysis of electric charge area density of ellipsoid-shaped conductor are presented in this paper . It is recognized that the electric charge area density of electrified conductors are distributed unevenly . Keyword : conductor ;
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根据双辉光放电3个电极极板上的电势,利用边界元积分方程建立以面电荷密度为未知量的离散方程,通过求解线性方程组计算3个电极极板上面电荷的不均匀分布。
With electric potential of three electrodes , discrete equations of surface electric charge density was founded with boundary element integral equations . The distribution of surface electric charge on the electrodes was calculated by solving a linear equation group .
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同以往的常规算法相比,当微结构变形微小时,使用该方法,微结构变形后的面电荷密度可以在微结构未变形中计算,从而大大提高了静电-结构耦合数值计算效率。
Comparing with previous methods , when the microstructures undergo small deformations , the surface charge densities on the deformed geometry can be computed without updating the geometry of the microstructures using the new approach , so the computational efficiency for coupled electromechanical analysis is improved effectively .
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用δ函数把均匀带电圆环表象成为过圆环所在坐标面上的电荷面密度,并结合推广了的静电场边值关系分区求解了介质球与带电圆环静电问题。
By means of δ function , uniform charged ring is expressed into surface charge density function on coordinate surfaces . The expression is used in electrostatic problem of uniform charged ring and spherical medium .