取决于电荷分布的不同形态,定义静态分布的四种形式: 点电荷分布形式(point charge) qr ( r ——源点的位矢) 体电荷密度(volume charge density) q r dq r r lim C/m 3 V 0 V dV E P x y z eR R r r r Q x y z...
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pin-point charge [矿业] 定向药包
Point-charge Model 点电荷模型
intensity of point charge 点电荷的场强
point-charge 点电荷
zero-point charge [电] 零点电荷
point charge group 点电荷系
moving point charge 运动电荷
The electric potential and the field of point charge are resolved with a special function.
利用特殊函数求解电势、电场,计算了点电荷与磁偶极子相互作用的电磁角动量。
In order to optimize the computation method, the charge simulation method has been developed combined with the equivalent line and point charge.
为了优化计算,提出了线电荷与点电荷相结合的等效电荷法。
Then by the principle of superposition and solving two sets of algebraic equations, the interaction between the point force and the point charge was uncoupled.
利用线性叠加原理,通过求解两组代数方程组,从而分离出点力与点电荷的耦合作用。
And the point that I also want to make is the way that they differ, z effective actually differs from the total charge in the nucleus due to an idea called shielding.
我也想指出的一点是它们不同的方式,有效的z事实上不同于原子核的,总电荷量,因为屏蔽效应。
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