• DocumentCode
    781488
  • Title

    Comments on "On the use of /spl rho/-algorithm in series acceleration"

  • Author

    Pyati, Vittal P.

  • Author_Institution
    Dept. of Electr. & Comput. Eng., Air Force Inst. of Technol., Wright-Patterson AFB, OH, USA
  • Volume
    44
  • Issue
    4
  • fYear
    1996
  • fDate
    4/1/1996 12:00:00 AM
  • Firstpage
    590
  • Abstract
    The author draws the attention of the readers to the paper of Singh and Singh (see ibid., vol.39, p.1514-16, Oct. 1991) that an extremely simple and elegant method of handling this age-old problem may be found in Morse and Feshbach (1953). Suggested by the geometry of the original problem for the Helmholtz equation, one first determines the solution of the Poisson´s equation (setting the wavenumber to zero) with appropriate boundary conditions and sources in closed form, as well as an infinite series. A useful feature of the series solution is that each term resembles a corresponding term in the original series solution of the Helmholtz equation, and for large values of the summation index, term by term, equality is approached. By adding the closed form answer, subtracting the series solution, and rearranging, one realizes fast convergence. Yet another gratifying feature is that convergence of the transformed series can be easily proven.
  • Keywords
    Helmholtz equations; convergence of numerical methods; series (mathematics); Helmholtz equation; Poisson´s equation; boundary conditions; closed form; fast convergence; infinite series; problem geometry; rho-algorithm; series acceleration; series solution; sources; summation index; transformed series; wavenumber; Accelerated aging; Acceleration; Antennas and propagation; Boundary conditions; Geometry; Microwave propagation; Microwave theory and techniques; Phased arrays; Physics; Poisson equations;
  • fLanguage
    English
  • Journal_Title
    Antennas and Propagation, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-926X
  • Type

    jour

  • DOI
    10.1109/8.489313
  • Filename
    489313