# Difference between revisions of "Coulomb interaction"

Line 33: | Line 33: | ||

<math>U_{12}=\frac{1}{4\pi\varepsilon_0}\frac{q_1q_2}{r_{12}}</math>. | <math>U_{12}=\frac{1}{4\pi\varepsilon_0}\frac{q_1q_2}{r_{12}}</math>. | ||

+ | Similarly, the Coulomb interaction potential of two bodies with continuous charge distribution is | ||

+ | |||

+ | <math>\U_{12}=\int\int\frac{1}{4\pi\varepsilon_0}\frac{\rho(\mathbf r_1)\rho(\mathbf r_2)}{|\mathbf r_1-\mathbf r_2|}d^3\mathbf r_1d^3\mathbf r_2</math>, | ||

== Keyword in references: == | == Keyword in references: == | ||

[[Photonic Properties of Strongly Correlated Colloidal Liquids]] | [[Photonic Properties of Strongly Correlated Colloidal Liquids]] |

## Revision as of 21:44, 8 December 2011

Written by Yuhang Jin, AP225 2011 Fall.

## Introduction

Coulomb interaction is the electrostatic interactions between electric charges, and follows the Coulomb's law, which is a basis of classical electrodynamics. In general, Coulomb interaction can manifest itself on various scales from microscopic particles to macroscopic bodies. The microscopic theory of Coulomb interaction has been developed in the frame of quantum field theory.

## Basic properties and formulae of Coulomb interaction

The electrostatic interaction of two point charges <math>q_1</math> at position <math>\mathbf r_1</math> and <math>q_2</math> at position <math>\mathbf r_2</math> is described by the Coulomb's law:

<math>\mathbf F_{12}=\frac{1}{4\pi\varepsilon_0}\frac{q_1q_2(\mathbf r_1-\mathbf r_2)}{|\mathbf r_1-\mathbf r_2|^3}</math>,

where <math>\mathbf F</math> is the electrostatic force experience by <math>q_1</math> (solely) due to the presence of <math>q_2</math>, and <math>\epsilon_0</math> is the vacuum permittivity, which has a value of <math>8.85\times10^{-12}</math> approximately.

Coulomb interaction obeys the principle of linear superstition, and therefore the force on a point charge at position <math>\mathbf r</math> exerted by a object with continuous charge distribution is give as

<math>\mathbf F=\int\frac{1}{4\pi\varepsilon_0}\frac{\rho(\mathbf r')(\mathbf r-\mathbf r')}{|\mathbf r-\mathbf r'|^3}d^3\mathbf r'</math>,

where <math>\rho(\mathbf r')</math> is the charge density of the body, and furthermore, the Coulomb interaction between two bodies with continuous charge distribution is

<math>\mathbf F=\int\int\frac{1}{4\pi\varepsilon_0}\frac{\rho(\mathbf r_1)\rho(\mathbf r_2)(\mathbf r_1-\mathbf r_2)}{|\mathbf r_1-\mathbf r_2|^3}d^3\mathbf r_1d^3\mathbf r_2</math>.

Coulomb forces are conservative, and as a result Coulomb interaction can be described using the Coulomb potential. The potential created by a point charge <math>q_1</math> is

<math>U=\frac{1}{4\pi\varepsilon_0}\frac{q_1}{r}</math>,

where <math>r</math> is the distance from <math>q_1</math> charge. The force experienced by another point charge <math>q_2</math> due to <math>q_1</math> is given by

<math>\mathbf F_{21}=-q_2\nabla U</math>.

The interaction potential between two point charges is given as

<math>U_{12}=\frac{1}{4\pi\varepsilon_0}\frac{q_1q_2}{r_{12}}</math>.

Similarly, the Coulomb interaction potential of two bodies with continuous charge distribution is

<math>\U_{12}=\int\int\frac{1}{4\pi\varepsilon_0}\frac{\rho(\mathbf r_1)\rho(\mathbf r_2)}{|\mathbf r_1-\mathbf r_2|}d^3\mathbf r_1d^3\mathbf r_2</math>,

## Keyword in references:

Photonic Properties of Strongly Correlated Colloidal Liquids