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Four-current

 
Wikipedia: Four-current
Electromagnetism
Electricity · Magnetism
Covariant formulation
Electromagnetic tensor · EM Stress-energy tensor · Four-current · Electromagnetic four-potential ·

In special and general relativity, the four-current is the Lorentz covariant four-vector that replaces the electromagnetic current density, or indeed any conventional charge current density. Its four components are given by:

J^a = \left(c \rho, \mathbf{j} \right)

where

c is the speed of light
ρ the charge density
j the conventional current density.
a labels the space-time dimensions

In special relativity, the statement of charge conservation (also called the continuity equation) is that the Lorentz invariant divergence of J is zero:

D \cdot J = \partial_a J^a = \frac{\partial \rho}{\partial t} + \nabla \cdot \mathbf{j} = 0

where D is an operator called the four-gradient and given by (1/c ∂/∂t, ∇). The summation convention has been used, so that the space-time dimensions are implicitly summed over. i.e.

 \partial_a J^a =  \sum_{i=0}^{3} \partial_i J^i

Sometimes, the above relation is written as

J^a{}_{,a}=0\,

In general relativity, the continuity equation is written as:

J^a{}_{;a}=0\,

where the semi-colon represents a covariant derivative.

See also


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Wikipedia. This article is licensed under the Creative Commons Attribution/Share-Alike License. It uses material from the Wikipedia article "Four-current" Read more