Four-current

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In special and general relativity, the four-current is the Lorentz covariant four-vector that replaces the electromagnetic current density, or indeed any conventional current density.

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

where

c is the speed of light
ρ the charge density
j the conventional current density.


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, ∇). 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 Noether's theorem.

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