On uniqueness and continuity for the quasi-linear, bianisotropic Maxwell equations, using an entropy condition

The quasi-linear Maxwell equations describing electromagnetic wave propagation in nonlinear media permit several weak solutions, which may be discontinuous (shock waves). It is often conjectured that the solutions are unique if they satisfy an additional entropy condition. The entropy condition states that the energy contained in the electromagnetic fields is irreversibly dissipated to other energy forms, which are not described by the Maxwell equations. We use the method employed by Kruzkov to scalar conservation laws to analyze the implications of this additional condition in the electromagnetic case, i.e., systems of equations in three dimensions. It is shown that if a cubic term can be ignored, the solutions are unique and depend continuously on given data. (Less)

[1]  E. Hopf,et al.  The Partial Differential Equation u_i + uu_x = μu_t , 1950 .

[2]  G. M.,et al.  Partial Differential Equations I , 2023, Applied Mathematical Sciences.

[3]  C. Dafermos Hyberbolic Conservation Laws in Continuum Physics , 2000 .

[4]  S. Kružkov FIRST ORDER QUASILINEAR EQUATIONS IN SEVERAL INDEPENDENT VARIABLES , 1970 .

[5]  Hean-Teik Chuah,et al.  STABILITY OF CLASSICAL FINITE-DIFFERENCE TIME-DOMAIN (FDTD) FORMULATION WITH NONLINEAR ELEMENTS—A NEW PERSPECTIVE - ABSTRACT , 2003 .

[6]  L. Hörmander,et al.  Lectures on Nonlinear Hyperbolic Differential Equations , 1997 .

[7]  Mats Gustafsson,et al.  Wave Splitting in Direct and Inverse Scattering Problems , 2000 .

[8]  E. Hopf The partial differential equation ut + uux = μxx , 1950 .

[9]  J. Hadamard,et al.  Lectures on Cauchy's Problem in Linear Partial Differential Equations , 1924 .

[10]  E. M. Lifshitz,et al.  Electrodynamics of continuous media , 1961 .

[11]  L. Hörmander The analysis of linear partial differential operators , 1990 .

[12]  Ari Sihvola,et al.  Six-vector formalism in electromagnetics of bi-anisotropic media , 1995 .

[13]  G. Maugin On shock waves and phase-transition fronts in continua , 1998 .

[14]  P. Raviart,et al.  Numerical Approximation of Hyperbolic Systems of Conservation Laws , 1996, Applied Mathematical Sciences.

[15]  P. Lax Hyperbolic Systems of Conservation Laws and the Mathematical Theory of Shock Waves , 1987 .

[16]  Tai-Ping Liu,et al.  The entropy condition and the admissibility of shocks , 1976 .

[17]  P. Lax Shock Waves and Entropy , 1971 .

[18]  Daniel Sjöberg,et al.  Simple wave solutions for the Maxwell equations in bianisotropic, nonlinear media, with application to oblique incidence , 2000 .

[19]  J. Jackson Classical Electrodynamics, 3rd Edition , 1998 .

[20]  D. A. Dunnett Classical Electrodynamics , 2020, Nature.

[21]  D. Serre Systems of Conservation Laws: A Challenge for the XXIst Century , 2001 .

[22]  E. Dill,et al.  Thermodynamic restrictions on the constitutive equations of electromagnetic theory , 1971 .

[23]  Direct and inverse scattering for transient electromagnetic waves in nonlinear media , 1998 .

[24]  D. Sjöberg Reconstruction of nonlinear material properties for homogeneous, isotropic slabs using electromagnetic waves , 1999 .

[25]  Daniel F. Styer,et al.  Insight into entropy , 2000 .

[26]  C. Dafermos The entropy rate admissibility criterion for solutions of hyperbolic conservation laws , 1973 .

[27]  G. Maugin On the universality of the thermomechanics of forces driving singular sets , 2000 .

[28]  Richard Courant,et al.  Supersonic Flow And Shock Waves , 1948 .

[29]  I. Åberg High-frequency switching and Kerr effect - nonlinear problems solved with nonstationary time domain techniques , 1996 .

[30]  Effective Boundary Conditions for a 2d iNhomogeneous Nonlinear Thin Layer Coated On a Metallic Surface - Abstract , 1999 .