The complete charge-current density and field strength of an arbitrarily accelerated relativistic point-charge are explicitly calculated. The current density includes, apart from the well-established delta-function term which is sufficient for its global conservation, additional contributions depending on the second and third proper-time derivatives of the position, which are necessary for its local conservation as required by the internal consistency of classical electrodynamics. Similarly, the field strength includes an additional delta-like contribution which is necessary for obtaining this result
A whole electromagnetism carrying four electric charge messengers is studied. Based on light invaria...
International audienceFor classical relativistic field theory in Minkowski space-time, the addition ...
The unified field is a Maxwell-Lorentz field. Maxwell-Lorentz equations for potentials in standard f...
The complete charge-current density and field strength of an arbitrarily accelerated relativistic po...
We reveal a new way in which the Lorenz gauge condition is related to the electric charge conservati...
After a summary of a recently proposed new type of instant form of dynamics (the Wigner-covariant re...
Calculating the electromagnetic fields of a uniformly accelerated charged particle is a surprisingly...
The force law of Maxwell’s classical electrodynamics does not agree with Newton’s third la...
For classical relativistic field theory in Minkowski space-time, the addition of a superpotential te...
The Maxwell–Dirac system describes the interaction of an electron with its self-induced electromagne...
AbstractA local current of particle density for scalar fields in curved background is constructed. T...
The electrostatic discharge occurs between electrically charged regions may be between the two cloud...
The theory of electrodynamics of radiating charges is reviewed with special emphasis on the role of ...
We complete a metric-free axiomatic framework for electrodynamics by introducing the appropriate ene...
A simple argument against the existence of magnetic monopoles is given. The argument is an important...
A whole electromagnetism carrying four electric charge messengers is studied. Based on light invaria...
International audienceFor classical relativistic field theory in Minkowski space-time, the addition ...
The unified field is a Maxwell-Lorentz field. Maxwell-Lorentz equations for potentials in standard f...
The complete charge-current density and field strength of an arbitrarily accelerated relativistic po...
We reveal a new way in which the Lorenz gauge condition is related to the electric charge conservati...
After a summary of a recently proposed new type of instant form of dynamics (the Wigner-covariant re...
Calculating the electromagnetic fields of a uniformly accelerated charged particle is a surprisingly...
The force law of Maxwell’s classical electrodynamics does not agree with Newton’s third la...
For classical relativistic field theory in Minkowski space-time, the addition of a superpotential te...
The Maxwell–Dirac system describes the interaction of an electron with its self-induced electromagne...
AbstractA local current of particle density for scalar fields in curved background is constructed. T...
The electrostatic discharge occurs between electrically charged regions may be between the two cloud...
The theory of electrodynamics of radiating charges is reviewed with special emphasis on the role of ...
We complete a metric-free axiomatic framework for electrodynamics by introducing the appropriate ene...
A simple argument against the existence of magnetic monopoles is given. The argument is an important...
A whole electromagnetism carrying four electric charge messengers is studied. Based on light invaria...
International audienceFor classical relativistic field theory in Minkowski space-time, the addition ...
The unified field is a Maxwell-Lorentz field. Maxwell-Lorentz equations for potentials in standard f...