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The collective motion of electrons in a relativistic isotropic plasma which is described by the linearized Maxwell‐Boltzmann equations is treated with time harmonic dependence. It is shown that the electric intensity at any point in an enclosed volume, can be determined when the tangential components of the electric and magnetic field are prescribed along with the electronic distribution function, on the surface enclosing the volume

Representation of Fields in a Relativistic Plasma by a Surface Integral