• DocumentCode
    2084917
  • Title

    TLM and Maxwell´s equations

  • Author

    Krumpholz, M. ; Russer, P.

  • Author_Institution
    Ferdinand-Braun-Institut fur Hochstfrequenztechnik, Germany
  • fYear
    1994
  • fDate
    12-14 Apr 1994
  • Firstpage
    12
  • Lastpage
    15
  • Abstract
    Applying the method of moments to Maxwell´s equations, the two-dimensional TLM method is derived from first principles of field theory. Sampling Maxwell´s equations with pulse functions yields three discretized field equations for the three electric and magnetic field components at the center of a TLM cell. For the field components at the cell boundaries, the mean values of the field components in the two neighbouring TLM cells are taken. The authors call these mean values the cell boundary mean (CBM) values. Introducing the CBM values of the electric and magnetic field components yields four discretized field equations per TLM unit cell. Applying the cell boundary mapping, they obtain four discretized field equations for wave amplitudes which determine the scattering matrix of the two-dimensional TLM method uniquely
  • Keywords
    Maxwell equations; S-matrix theory; transmission line theory; Maxwell´s equations; TLM; TLM cell; cell boundaries; cell boundary mapping; cell boundary mean values; discretized field equations; electric field components; field theory; magnetic field components; method of moments; scattering matrix; two-dimensional TLM method; wave amplitudes;
  • fLanguage
    English
  • Publisher
    iet
  • Conference_Titel
    Computation in Electromagnetics, 1994. Second International Conference on
  • Conference_Location
    London
  • Print_ISBN
    0-85296-609-1
  • Type

    conf

  • DOI
    10.1049/cp:19940004
  • Filename
    324118