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相关概念视频

Gauss's Law: Planar Symmetry01:27

Gauss's Law: Planar Symmetry

8.0K
A planar symmetry of charge density is obtained when charges are uniformly spread over a large flat surface. In planar symmetry, all points in a plane parallel to the plane of charge are identical with respect to the charges. Suppose the plane of the charge distribution is the xy-plane, and the electric field at a space point P with coordinates (x, y, z) is to be determined. Since the charge density is the same at all (x, y) - coordinates in the z = 0 plane, by symmetry, the electric field at P...
8.0K
Gauss's Law: Spherical Symmetry01:26

Gauss's Law: Spherical Symmetry

7.6K
A charge distribution has spherical symmetry if the density of charge depends only on the distance from a point in space and not on the direction. In other words, if the system is rotated, it doesn't look different. For instance, if a sphere of radius R is uniformly charged with charge density ρ0, then the distribution has spherical symmetry. On the other hand, if a sphere of radius R is charged so that the top half of the sphere has a uniform charge density ρ1 and the bottom half...
7.6K
Electric Field of a Non Uniformly Charged Sphere01:22

Electric Field of a Non Uniformly Charged Sphere

1.6K
Gauss's law states that the electric flux through any closed surface equals the net charge enclosed within the surface. This law is beneficial for determining the expressions for the electric field for a particular charge distribution if the electric flux is known.
Consider a non-uniformly charged sphere, for which the density of charge depends only on the distance from a point in space and not on the direction. Such a sphere has a spherically symmetrical charge distribution. Here, the electric...
1.6K
Electric Field of a Charged Disk01:23

Electric Field of a Charged Disk

2.2K
The simplest case of a surface charge distribution is the uniformly charged disk. Calculating its electric field also helps us calculate the electric field of a large plane of charge.
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
2.2K
Coulomb's Law01:30

Coulomb's Law

9.3K
Experiments with electric charges have shown that if two objects each have an electric charge, they exert an electric force on each other. The magnitude of the force is linearly proportional to the net charge on each object and inversely proportional to the square of the distance between them. The direction of the force vector is along the imaginary line joining the two objects and is dictated by the signs of the charges involved.
Newton's third law applies to the Coulomb force — the...
9.3K
Spherical and Cylindrical Capacitor01:26

Spherical and Cylindrical Capacitor

5.7K
A spherical capacitor consists of two concentric conducting spherical shells of radii R1 (inner shell) and R2 (outer shell). The shells have  equal and opposite charges of +Q and −Q, respectively. For an isolated conducting spherical capacitor, the radius of the outer shell can be considered to be infinite.
Conventionally, considering the  symmetry, the electric field between the concentric shells of a spherical capacitor is directed radially outward. The magnitude of the field,...
5.7K

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相关实验视频

Updated: Jul 15, 2025

Finite Element Modelling of a Cellular Electric Microenvironment
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在两个平面表面之间限制的球形粒子上的静电力.

Zhanwen Wang1, Michael J Miksis2, Petia M Vlahovska2

  • 1Theoretical and Applied Mechanics Program, Northwestern University, Evanston, IL 60208, USA.

Soft matter
|October 2, 2023
PubMed
概括

两个墙壁之间的无电荷粒子经历了受电场影响的力量. 该力对正常场具有吸引力,对触点场具有排斥力,其复杂的行为取决于限制.

科学领域:

  • 物理 物理学 物理
  • 物理化学 物理化学
  • 材料科学 材料科学 材料科学

背景情况:

  • 在均电场中的无电荷粒子在无界域中没有净力.
  • 一个单一的边界打破了对称性,导致吸引或排斥,这取决于场方向.
  • 在实际应用中,第二边界是常见的,需要进一步研究.

研究的目的:

  • 为了研究第二边界对在均电场中的无电荷粒子的影响.
  • 分析作用于悬浮在两个平行墙壁之间的球形粒子的力量.
  • 探索电场方向 (正常或触点) 对粒子边界相互作用的影响.

主要方法:

  • 模拟介质作为漏电介电材料,以允许在接口上免费累积电荷.
  • 使用多极扩张解决拉普拉斯电位方程.
  • 使用一组图像计算边界.

主要成果:

  • 对于一个正常的电场,这种力总是对最近的边界具有吸引力,并且通常比单一的墙体更弱.
  • 颗粒墙力可以随着限制而变化非单调,并且可能超过一个墙的值.
  • 对于触电场,力总是具有排斥性,遵循类似的趋势.

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结论:

  • 第二个边界的存在显著改变了无电荷粒子上的静电力.
  • 应用电场的方向决定了该力是否具有吸引力或排斥力.
  • 限制效应可以导致非直观的力行为,突出显示粒子边界相互作用的复杂性在有限的几何体.