Finite difference time domain algorithm for electromagnetic problems involving material movement

The finite difference time domain (FDTD) method, adapted for magnetic field diffusion problems, is used to study the electromagnetic induction in moving materials by including motional emf in standard FDTD electromagnetic equations. The material movement is implemented by continuously changing material properties in each computational cell consistent to material advection. The flux corrected transport (FCT) algorithm is used to transport magnetic field in a fixed eulerian cell. A higher time-step is achieved by artificially increasing permittivity of the medium. This new approach is validated with standard analytical solutions for planar magnetic flux compression system and magnetic field diffusion in moving conductors with a non-relativistic velocity. To our knowledge, this is the first approach to use FDTD method for electromagnetic problems involving material motion.

[1]  Ron J. Litchford,et al.  Magnetic flux compression reactor concepts for spacecraft propulsion and power , 2000 .

[2]  S. Zalesak Fully multidimensional flux-corrected transport algorithms for fluids , 1979 .

[3]  M. Norman,et al.  ZEUS-2D : a radiation magnetohydrodynamics code for astrophysical flows in two space dimensions. II : The magnetohydrodynamic algorithms and tests , 1992 .

[4]  Jay P. Boris,et al.  Flux-corrected transport. I. SHASTA, a fluid transport algorithm that works , 1973 .

[5]  FDTD analysis of nonlinear magnetic diffusion by reduced c , 1995 .

[6]  C. Angelopoulos High resolution schemes for hyperbolic conservation laws , 1992 .

[7]  C.D. Sijoy,et al.  Calculation of Accurate Resistance and Inductance for Complex Magnetic Coils Using the Finite-Difference Time-Domain Technique for Electromagnetics , 2008, IEEE Transactions on Plasma Science.

[8]  R. Luebbers,et al.  The Finite Difference Time Domain Method for Electromagnetics , 1993 .

[9]  Analysis of exponential time-differencing for FDTD in lossy dielectrics , 1997 .

[10]  E. Gombia,et al.  Use of spatially dependent electron capture to profile deep‐level densities in Schottky barriers , 1985 .

[11]  C. Richard DeVore,et al.  Flux-corrected transport techniques for multidimensional compressible magnetohydrodynamics , 1989 .

[12]  Allen Taflove,et al.  Computational Electrodynamics the Finite-Difference Time-Domain Method , 1995 .

[13]  Jack Dongarra,et al.  MPI: The Complete Reference , 1996 .

[14]  C. Longmire,et al.  Development of the GLANC EMP code , 1973 .

[15]  J. Boris,et al.  Flux-Corrected Transport , 1997 .

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

[17]  K. Kunz,et al.  Finite-Difference Analysis of EMP Coupling to Lossy Dielectric Structures , 1980, IEEE Transactions on Electromagnetic Compatibility.

[18]  R. Holland,et al.  Finite-difference time-domain (FDTD) analysis of magnetic diffusion , 1994 .

[19]  Francesco Miniati,et al.  A Divergence-free Upwind Code for Multidimensional Magnetohydrodynamic Flows , 1998 .

[20]  C. M. Fowler,et al.  An Introduction to Explosive Magnetic Flux Compression Generators , 1975 .

[21]  F. Moon,et al.  Magneto-Solid Mechanics , 1986 .

[22]  Jean-Pierre Berenger,et al.  A perfectly matched layer for the absorption of electromagnetic waves , 1994 .

[23]  Application of a finite-difference technique to the human radiofrequency dosimetry problem. , 1985, The Journal of microwave power and electromagnetic energy : a publication of the International Microwave Power Institute.

[24]  D. Katz,et al.  Validation and extension to three dimensions of the Berenger PML absorbing boundary condition for FD-TD meshes , 1994, IEEE Microwave and Guided Wave Letters.

[25]  R. Löhner,et al.  Electromagnetics via the Taylor-Galerkin Finite Element Method on Unstructured Grids , 1994 .

[26]  G. Mur Absorbing Boundary Conditions for the Finite-Difference Approximation of the Time-Domain Electromagnetic-Field Equations , 1981, IEEE Transactions on Electromagnetic Compatibility.

[27]  A. Taflove,et al.  Use of the finite-difference time-domain method for calculating EM absorption in man models , 1988, IEEE Transactions on Biomedical Engineering.

[28]  H. Wilhelm Electromagnetic induction in accelerated conductors with frontal compression and rear dilution of magnetic flux , 1984 .

[29]  Electromagnetic induction in conductors accelerated in magnetic fields amplified by flux compression , 1983 .

[30]  C. D. Sijoy,et al.  Three-Dimensional Calculations of Electrical Parameters in Flux Compression Systems , 2006, 2006 IEEE International Conference on Megagauss Magnetic Field Generation and Related Topics.

[31]  Bruce Archambeault,et al.  The Finite-Difference Time-Domain Method , 1998 .

[32]  J. R. Freeman,et al.  Numerical methods for studying compressed magnetic field generators , 1977 .

[33]  C. D. Sijoy,et al.  Use of 3-D FDTD Method for Magnetic Field Diffusion Calculations in Complex Pinch Geometries , 2005 .

[34]  M. Norman,et al.  ZEUS-2D: A radiation magnetohydrodynamics code for astrophysical flows in two space dimensions. I - The hydrodynamic algorithms and tests. II - The magnetohydrodynamic algorithms and tests , 1992 .

[35]  G. Tóth,et al.  Comparison of Some Flux Corrected Transport and Total Variation Diminishing Numerical Schemes for Hydrodynamic and Magnetohydrodynamic Problems , 1996 .