带电体

匀速直线运动带电体的电磁场

Electromagnetic field caused by an electrically charged body in uniform rectilinear motion

定轴转动带电体的磁场分布

The magnetic fileds of charged body rotating around fixed axis

库仑推测，两个带电体之间的电力F由两个因素决定。

Coulomb made the conjecture that electrical force F between two charged objects depends on two factors .

俄罗斯（110-750）kV配电装置的带电体至各种部件最小允许距离的规定

The Prescriptions onthe Minimum Allowed Clearances Between Electrically Charged Objects of ( 110 - 750 ) kV Distribution Equipment and All Other Parts Around in Russia

带电体模型对零电位选择的限制

The Limit of the Electric Model to the Selecting Electrical Null

转动带电体的磁矩与转动惯量的类比

A Comparison Between Magnetic Moment Of Turning Electrified Body And Turning Inertia

但应注意不要让身体的任何部分接触带电体，并注意通风。

Attention to avoid touching anything with electricity and notice to ventilate .

关于旋转带电体磁场的求解

On the solution of magnetic field of rotating charged body

电矩张量与旋转带电体的磁矩

Charge moment tensor and the magnetic moment of a rotating charged bodies

旋转带电体转动惯量的另一求解方法

Another solution for the moment of inertia of some charged rotating objects

旋转带电体磁矩计算的若干法则与算例

Principles and examples about calculating the magnetic moment of charged rotational bodies

均匀旋转带电体轴线上的磁场分布

Distribution of Magnetic Field on Axis Line to Even Electric Body of Revolving

带电体定轴转动的磁矩计算

The calculation of magnetic moment of an electrified body rotating about a fixed-axis

用广义协变原理研究非惯性运动带电体的电磁场

The electromagnetic field of charge body in non-inertial movement

论带电体的力密度问题

On the problem of force density of charged bodies

利用电位叠加原理求解球形带电体空间的电位

Calculate the Electric Potential of Spherical Live Object Space with Electric Potential Superposition Principle

人们将相互排斥或相互吸引的物体叫带电体。

The bodies may either repel or attract each other are called electrified body .

旋转带电体的电磁场

Electromagnetic field of electrified rotating body

旋转带电体和电磁场的角动量守恒定律及能量守恒定律

The conservation laws of angular momentum and energy for a charged and revolving system and electromagnetic field

外电场与腔内电荷分布无关，但与腔内带电体电量有关。

It does not relate to the charge distribution inside the cavity , but the charge quantity .

连续带电体和点电荷系的电势能与电场能的定量关系

Quantitative Relations between Electric Potential Energy and Electric Field Energy of Continuous Charged Body and Point Charge System

它们可能反映了流星带电体与地球磁场的相互作用。

It may reflect that the meteoric charged body and the Earth 's magnetic field interact with each other .

你们将在8。02中学到，如果一个带电体改变方向时，产生一个加速度。

You will learn in8.02 that if you have a charged body changing direction , that constitutes an acceleration .

我们检查和测量电荷的唯一方法，是观察带电体间的相互作用。

The only way we have of detecting and measuring electric charges is by observing the interaction of charged bodies .

带电体绕对称轴转动时的转动惯量及在外磁场中所受磁力矩的量纲解法

Revolving inertia and dimensional solution of similar evenly electrified bodies revolving the symmetrical axis as well as under magnetic matrix in outer magnetic field

当穿过原子核后，我们会看到那个电子如同一个带电体朝相反的方向移动。

As we pass an atomic nucleus , to us on the electron it appears as a large charged body moving in the opposite direction .

求定轴匀角速转动带电体的磁场是一类典型的静磁场边值问题。

Computation of the magnetic field , which is produced by a charged body rotating about a fixed axis , is a classical question about magnetostatic boundary-value problem .

假设带电体表面均匀带电，运用积分求电势、电场分布的方法，实际意义不大。

On assumption that the surface of the conductive body is uniformly charged , the method for evaluation of the electric field and potential distribution is insignificant in practice .

空穴是半导体和绝缘体中的一种带电体，其能量小于费米能，并且参与导电。讹科费米原子能电站

Hole is an charged electronic entity in semiconductors and insulators which have energies less than the Fermi level and participate in the electric conduction . enrico fermi atomic power plant

在目前电场计算的文献中，限于计算电位参考点和各带电体间的电位差均为已知时的带电系统中的电场分布。

In current literatures methods of electric field calculations are only applicable to the case , where the potential differences between charged objects and the potential reference point are known .