Four-current
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In special and general relativity, the four-current (technically the four-current density)<ref>Rindler, Wolfgang (1991). Introduction to Special Relativity (2nd ed.). Oxford Science Publications. pp. 103–107. ISBN 978-0-19-853952-0.</ref> is the four-dimensional analogue of the current density, with units of charge per unit time per unit area. Also known as vector current, it is used in the geometric context of four-dimensional spacetime, rather than separating time from three-dimensional space. Mathematically it is a four-vector and is Lorentz covariant.
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
Using the Minkowski metric <math>\eta_{\mu\nu}</math> of metric signature (+ − − −), the four-current components are given by:
- <math>J^\alpha = \left(c \rho, j^1 , j^2 , j^3 \right) = \left(c \rho, \mathbf{j} \right)</math>
where:
- c is the speed of light;
- ρ is the volume charge density;
- j is the conventional current density;
- The dummy index α labels the spacetime dimensions.
Motion of charges in spacetime
This can also be expressed in terms of the four-velocity by the equation:<ref>Roald K. Wangsness, Electromagnetic Fields, 2nd edition (1986), p. 518, 519</ref><ref>Melvin Schwartz, Principles of Electrodynamics, Dover edition (1987), p. 122, 123</ref>
- <math>J^\alpha = \rho_0 U^\alpha = \rho_u \sqrt{1 - \frac{u^2}{c^2}} U^\alpha</math>
where:
- <math>\rho_u</math> is the charge density measured by an inertial observer O who sees the electric current moving at speed u (the magnitude of the 3-velocity);
- <math>\rho_0</math> is “the rest charge density”, i.e., the charge density for a comoving observer (an observer moving at the speed u - with respect to the inertial observer O - 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
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 magnetism) in one electromagnetic entity.
Continuity equation
In special relativity, the statement of charge conservation is that the Lorentz invariant divergence of J is zero:<ref>J. D. Jackson, Classical Electrodynamics, 3rd Edition (1999), p. 554</ref>
- <math>\dfrac{\partial J^\alpha}{\partial x^\alpha} = \frac{\partial \rho}{\partial t} + \nabla \cdot \mathbf{j} = 0\,,</math>
where <math>\partial/\partial x^\alpha </math> is the four-gradient. This is the continuity equation.
In general relativity, the continuity equation is written as:
- <math>J^\alpha{}_{;\alpha}=0\,,</math>
where the semi-colon represents a covariant derivative.
Maxwell's equations
The four-current appears in two equivalent formulations of Maxwell's equations, in terms of the four-potential<ref>as [ref. 1, p519]</ref> when the Lorenz gauge condition is fulfilled:
- <math>\Box A^\alpha = \mu_0 J^\alpha </math>
where <math>\Box </math> is the D'Alembert operator, or the electromagnetic field tensor:
- <math>\nabla_\alpha F^{\alpha\beta} = \mu_0 J^\beta</math>
where μ0 is the permeability of free space and ∇α is the covariant derivative.
General relativity
In general relativity, the four-current is defined as the divergence of the electromagnetic displacement, defined as:
- <math>\mathcal{D}^{\mu \nu} \, = \, \frac{1}{\mu_{0}} \, g^{\mu \alpha} \, F_{\alpha \beta} \, g^{\beta \nu} \, \sqrt{-g} \,</math>
then:
- <math>J^\mu = \partial_\nu \mathcal{D}^{\mu \nu}</math>
Quantum field theory
The four-current density of charge is an essential component of the Lagrangian density used in quantum electrodynamics.<ref>Cottingham, W. Noel; Greenwood, Derek A. (2003). An introduction to the standard model of particle physics. Cambridge University Press. p. 67. ISBN 9780521588324.</ref> In 1956 Gershtein and Zeldovich considered the conserved vector current (CVC) hypothesis for electroweak interactions.<ref>Marshak, Robert E. (1993). Conceptual foundations of modern particle physics. World Scientific Publishing Company. p. 20. ISBN 9789813103368.</ref><ref>Gershtein, S. S.; Zeldovich, Y. B. (1956), Soviet Phys. JETP, 2 576.</ref><ref>Thomas, Anthony W. (1996). "CVC in particle physics". arXiv:nucl-th/9609052.</ref>
See also
References
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