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Electric Field of a Non Uniformly Charged Sphere01:22

Electric Field of a Non Uniformly Charged Sphere

2.5K
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...
2.5K
Electric Field of a Charged Disk01:23

Electric Field of a Charged Disk

3.6K
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...
3.6K
Electric Field of Two Equal and Opposite Charges01:30

Electric Field of Two Equal and Opposite Charges

7.6K
Atoms generally contain the same number of positively and negatively charged particles, protons, and electrons. Hence, they are electrically neutral. However, the centers of the positive and negative charges do not always coincide. In such a scenario, the electric field of an atom may not be zero.
A separation of the positive and negative charges can lead to a weak, remnant effect of the positive and negative charges. The expectation is that the more the distance between the positive and...
7.6K
Electrostatic Boundary Conditions in Dielectrics01:27

Electrostatic Boundary Conditions in Dielectrics

2.1K
When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's permittivity....
2.1K
Electric Field Lines01:25

Electric Field Lines

11.5K
The three-dimensional representation of the electric field of a positive point charge requires tracing the electric field vectors, whose lengths decrease as the square of their distance from the charge and which point away from the charge at each point. This vector field is no doubt challenging to visualize. The visualization of electric fields becomes quickly intractable as the number of charges increases.
The solution to this problem is to use electric field lines, which are not vectors but...
11.5K
Electric Field of Parallel Conducting Plates01:16

Electric Field of Parallel Conducting Plates

2.2K
Gauss' law relates the electric flux through a closed surface to the net charge enclosed by that surface. Gauss's law can be applied to find the electric field and the charge enclosed in a region depending on its charge distribution.
Consider a cross-section of a thin, infinite conducting plate having a positive charge. For such a large thin plate, as the thickness of the plate tends to zero, the positive charges lie on the plate's two large faces. Without an external electric field, the...
2.2K

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関連する実験動画

Updated: Apr 17, 2026

Finite Element Modelling of a Cellular Electric Microenvironment
08:23

Finite Element Modelling of a Cellular Electric Microenvironment

Published on: May 18, 2021

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電場の下での不規則な粒子の詰め込み.

Pengcheng Song1, Yufeng Wang, Yu Wang

  • 1Molecular Design Institute and Department of Chemistry, New York University , New York, New York 10003, United States.

Journal of the American Chemical Society
|February 19, 2015
PubMed
まとめ
この要約は機械生成です。

特定の対称性を持つ有電荷のコロイド粒子は,電場下で1D,2D,3Dの構造に自己組み立てられ,新しい包装配列とダブルヘリックス構造を明らかにします.

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Experimental Methods of Dust Charging and Mobilization on Surfaces with Exposure to Ultraviolet Radiation or Plasmas
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Experimental Methods of Dust Charging and Mobilization on Surfaces with Exposure to Ultraviolet Radiation or Plasmas

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Spatial Separation of Molecular Conformers and Clusters
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Spatial Separation of Molecular Conformers and Clusters

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関連する実験動画

Last Updated: Apr 17, 2026

Finite Element Modelling of a Cellular Electric Microenvironment
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Finite Element Modelling of a Cellular Electric Microenvironment

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Experimental Methods of Dust Charging and Mobilization on Surfaces with Exposure to Ultraviolet Radiation or Plasmas
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Spatial Separation of Molecular Conformers and Clusters
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科学分野:

  • コロイドと表面科学 コロイドと表面科学
  • ソフトマター物理学 ソフトマター物理学
  • マテリアルサイエンス 材料科学

背景:

  • コロイド粒子は,材料科学における基本的な構成要素である.
  • セルフアセンブリを理解することは,新しい材料の設計に不可欠です.
  • 充電粒子は,中性粒子と比較して独特の行動を示します.

研究 の 目的:

  • 異なる対称性を持つコロイド粒子の自己組み立てを調査する (2,3,または4つの充電されたパッチ).
  • 1D,2D,3D構造の形成における交流電場の影響を探求する.
  • 結晶の対称性と包装の仕様を特徴づけるため.

主な方法:

  • 制御された数のコロイド粒子の合成と充電パッチの配置.
  • AC電場を適用して極化と自己組み立てを誘導する.
  • 顕微鏡と difraktion テクニックは,結果の構造と対称性を分析します.

主要な成果:

  • 2パッチの粒子は,従来のコロイド結晶とは異なるcmm平面群 (2D) とI4mm空間群 (3D) のパッケージに自己組み立てます.
  • 3つのパッチの粒子は21の螺旋軸対称な鎖を形成し,ペア化し,いくつかのペアは意外にダブルヘリクスを形成します.
  • 4パッチの粒子は,2Dドメインを形成し,電場に並べられた行があり,3パッチのシステムと比較して異なるパッキング密度を示します.

結論:

  • コロイド粒子の電荷のあるパッチの数と対称性は,電気場の下での自己組み立て行動を決定する.
  • 単純な構成要素から,ダブルヘリクスを含む,新しい結晶構造や多形構造が生まれることができます.
  • この研究は,複雑なコロイドアーキテクチャを作成するための自己アセンブリを指示する洞察を提供します.