Charge density

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Charge Density

Illustration of charge distribution in a system.

Charge density is a measure of electric charge per unit area of a surface, or per unit volume of a body or field. It is a fundamental concept in electromagnetism and is used to describe how charge is distributed in a given space.

Types of Charge Density[edit | edit source]

Charge density can be categorized into three main types:

Linear Charge Density[edit | edit source]

Linear charge density, denoted by \( \lambda \), is the amount of electric charge per unit length. It is used when charge is distributed along a line, such as a charged wire. The formula for linear charge density is:

\[ \lambda = \frac{Q}{L} \]

where \( Q \) is the total charge and \( L \) is the length over which the charge is distributed.

Surface Charge Density[edit | edit source]

Surface charge density, denoted by \( \sigma \), is the amount of electric charge per unit area. It is applicable when charge is distributed over a surface, such as a charged plate. The formula for surface charge density is:

\[ \sigma = \frac{Q}{A} \]

where \( Q \) is the total charge and \( A \) is the area over which the charge is distributed.

Volume Charge Density[edit | edit source]

Volume charge density, denoted by \( \rho \), is the amount of electric charge per unit volume. It is used when charge is distributed throughout a volume, such as a charged sphere. The formula for volume charge density is:

\[ \rho = \frac{Q}{V} \]

where \( Q \) is the total charge and \( V \) is the volume over which the charge is distributed.

Applications of Charge Density[edit | edit source]

Charge density is a crucial concept in various fields of physics and engineering. It is used in:

  • Electrostatics: To calculate electric fields and potentials.
  • Capacitance: To determine the charge storage capacity of capacitors.
  • Semiconductor physics: To analyze charge distribution in semiconductor devices.

Mathematical Representation[edit | edit source]

In mathematical terms, charge density is often represented as a function of position, \( \rho(\mathbf{r}) \), where \( \mathbf{r} \) is the position vector. This allows for the calculation of electric fields using Gauss's law and other integral equations.

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Contributors: Prab R. Tumpati, MD