• DocumentCode
    975072
  • Title

    A short way of solving advanced problems in electromagnetic fields and other linear systems

  • Author

    Rumsey, V.H.

  • Author_Institution
    University of California, Berkeley, CA, USA
  • Volume
    11
  • Issue
    1
  • fYear
    1963
  • fDate
    1/1/1963 12:00:00 AM
  • Firstpage
    73
  • Lastpage
    86
  • Abstract
    A linear system is characterized in the abstract by a source vector a , a response vector \\alpha and a system matrix R , connected by \\alpha = Ra . Specific interpretations for a , \\alpha and R are given for electromagnetic fields, the scalar product a \\dot Rb being the reaction. The advantages of this method are illustrated by application to various problems. Mode expansions are defined by the eigenvector equation Rm = C_{m}m , C_{m} being the eigenvalue and m the mode source. This means the mode is generated by a combination of electric and magnetic sources which, apart from the constant multiplier C_{m} , are everywhere equal to the electric and magnetic fields, respectively. Such mode expansions are applied to typical waveguide problems. Waveguide theory is set up in terms of unit voltage and unit current mode sources, v and i , where v \\dot v = 1 = i \\dot i . Then the definitions of waveguide current and voltage coincide with those for circuit theory, e.g., the mode current at cross section P is the reaction on a unit voltage source placed at P . The method also greatly simplifies scattering and antenna problems, such as the pattern of a monopole antenna which is immersed in a layer of gyrotropic plasma.
  • Keywords
    Electromagnetic analysis; Linear systems; Eigenvalues and eigenfunctions; Electromagnetic fields; Electromagnetic waveguides; Equations; Linear systems; Magnetic fields; Transmission line matrix methods; Vectors; Voltage; Waveguide theory;
  • fLanguage
    English
  • Journal_Title
    Antennas and Propagation, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-926X
  • Type

    jour

  • DOI
    10.1109/TAP.1963.1137982
  • Filename
    1137982