Four-current

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In special and general relativity, the four-current is the four-dimensional analogue of the electric current density, which is used in the geometric context of four-dimensional spacetime, rather than three-dimensional space and time separately. Mathematically it is a four-vector, and is Lorentz covariant.

Analogously, it is possible to have any form of "current density", meaning the flow of a quantity per unit time per unit area, see current density for more on this quantity.

This article uses the summation convention for indices, see covariance and contravariance of vectors for background on raised and lowered indices, and raising and lowering indices on how to switch between them.

Definition[edit]

Using the Minkowski metric \eta_{\mu\nu} of metric signature (+−−−), its four components are given by:

J^\alpha = \left(c \rho, j^1 , j^2 , j^3 \right) = \left(c \rho, \mathbf{j} \right)

where c is the speed of light, ρ is the charge density and j the conventional current density. The dummy index α labels the spacetime dimensions.

Motion of charges in spacetime[edit]

This can also be expressed in terms of the four-velocity by the equation:[1][2]

J^\alpha = \rho_0 U^\alpha = \rho\sqrt{1-\frac{u^2}{c^2}} U^\alpha

where ρ is the charge density measured by an observer at rest observing the electric current, and ρ0 the charge density for an observer moving at the speed u (the magnitude of the 3-velocity) along with the charges.

Qualitatively, the change in charge density (charge per unit volume) is due to the contracted volume of charge due to Lorentz contraction.

Physical interpretation[edit]

Charges (free or as a distribution) at rest will appear to remain at the same spatial position for some interval of time (as long as they're stationary). When they do move, this corresponds to changes in position, therefore the charges have velocity, and the motion of charge constitutes an electric current. This means that charge density is related to time, while current density is related to space.

The four-current unifies charge density (related to electricity) and current density (related to electricity magnetism) in one electromagnetic entity.

Continuity equation[edit]

Main article: Continuity equation

In special relativity, the statement of charge conservation is that the Lorentz invariant divergence of J is zero:[3]

\dfrac{\partial J^\alpha}{\partial x^\alpha} = \frac{\partial \rho}{\partial t} + \nabla \cdot \mathbf{j} = 0

where \partial/\partial x^\alpha is the 4-gradient. This is the continuity equation.

In general relativity, the continuity equation is written as:

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

where the semi-colon represents a covariant derivative.

Maxwell's equations[edit]

Main article: Maxwell's equations

The four-current appears in two equivalent formulations of Maxwell's equations, in terms of the four-potential:[4]

\Box A^\alpha = \mu_0 J^\alpha

where \Box is the D'Alembert operator, or the electromagnetic field tensor:

\partial_\beta F^{\alpha\beta} = \mu_0 J^\alpha

where μ0 is the permeability of free space.

General Relativity[edit]

In general relativity, the four-current is defined as the divergence of the electromagnetic displacement, defined as

\mathcal{D}^{\mu \nu} \, = \, \frac{1}{\mu_{0}} \, g^{\mu \alpha} \, F_{\alpha \beta} \, g^{\beta \nu} \, \sqrt{-g} \,

then

J^\mu = \partial_\nu \mathcal{D}^{\mu \nu}

See also[edit]

References[edit]

  1. ^ Roald K. Wangsness, Electromagnetic Fields, 2nd edition (1986), p. 518, 519
  2. ^ Melvin Schwartz, Principles of Electrodynamics, Dover edition (1987), p. 122, 123
  3. ^ J. D. Jackson, Classical Electrodynamics, 3rd Edition (1999), p. 554
  4. ^ as [ref. 1, p519]