Within the framework of Extended Irreversible Thermodynamics (EIT) a phenomenological theory is proposed for a polarizable and magnetizable plasma in an electromagnetic field. In particular, for the polarization a transport equation is proposed generalizing the well-established Debye's law for dielectric relaxation. For the magnetization a transport equation is proposed generalizing the well-established Langevin's law for magnetic relaxation. The present equations correspond to those obtained by Dixon involving also coupling terms with the heat flux. Finally, in the special case in which cross-effects are not taken into account, the dispersion relation for plane weak electromagnetic disturbances is derived.
Contents
-
Requires Authentication UnlicensedAn Extended Irreversible Thermodynamic Description of Dielectric and Magnetic Relaxation in a Thermal and Viscous PlasmaLicensedJune 1, 2005
-
Requires Authentication UnlicensedStudy of Unstirred Ternary Non-Ionic Solutions Transport in a Double-Membrane SystemLicensedJune 1, 2005
-
Requires Authentication UnlicensedFinite Time Thermodynamic Optimization or Entropy Generation Minimization of Energy SystemsLicensedJune 1, 2005
-
Requires Authentication UnlicensedThermodynamic Limits and Kinetic Probabilities During Homogeneous Nucleation in Liquid Ag-Cu AlloysLicensedJune 1, 2005
-
Requires Authentication UnlicensedGlobal and Local Thermodynamic StabilityLicensedJune 1, 2005
-
Requires Authentication UnlicensedComments on the Continuity Equation in General RelativityLicensedJune 1, 2005