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Four-current

In special and general relativity, the four-current is the Lorentz covariant four-vector that replaces the electromagnetic current density

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

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

In special relativity, the statement of charge conservation (sometimes also called the contnuity 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

Ja,a = 0

In general relativity, the continuity equation is written as:

Ja;a = 0

where the semi-colon represents a covariant derivative.

Last updated: 08-24-2005 11:45:52
Last updated: 01-04-2007 01:18:57
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