• DocumentCode
    675357
  • Title

    Accuracy and efficiency of low-order volume integral equation techniques for dielectric bodies modeled with tetrahedral cells

  • Author

    Peterson, A.F.

  • Author_Institution
    Sch. of ECE, Georgia Inst. of Technol., Atlanta, GA, USA
  • fYear
    2013
  • fDate
    7-13 July 2013
  • Firstpage
    159
  • Lastpage
    159
  • Abstract
    Summary form only given. Many computational techniques based on volume integral equations have been proposed for the analysis of heterogeneous dielectric bodies illuminated by electromagnetic fields. The Schaubert-Wilton-Glisson approach (1984) employed the electric field integral equation (EFIE) with an expansion of the D-field in divergence conforming basis functions. This is sometimes called an EFIE-D approach. The Sun-Chew formulation (2009) uses a curl-conforming expansion of the electric field; this has been called an EFIE-E approach. The author recently described an EFIE-H formulation (ACES-2013) where the magnetic field is expanded in curl-conforming bases and the D-field obtained from it; that approach produces a solenoidal (zero-divergence) representation for D like that previously described by Carvalho and Mendes (1999) and recommended by Botha (2006). An EFIE-J formulation using piecewise-constant basis functions was proposed by Markkanen et al. (2012). These formulations share the properties that they employ tetrahedral cells, and can easily be scaled to produce symmetric impedance matrices. Approaches employing the magnetic field integral equation are available but do not produce a symmetric impedance matrix. Formulations based on differential equations are also widespread for heterogeneous bodies, but volume integral formulations remain of interest due to the possibility of obtaining a well-conditioned set of equations for fast iterative solution. By far the most widely-used formulation of the above is the Schaubert-WiltonGlisson EFIE-D approach. However, that approach requires more unknowns for a given model (one per face) than the EFIE-E or EFIE-H discretizations (one per edge), although less than the EFIE-J approach (3 per cell). In addition, the EFIED formulation requires volume-volume, volume-surface, and surface-surface interaction integrals, some over fictitious charge. In contrast, the EFIE-H formulation can be implemented without volume inte- rations. These observations suggest that the EFIE-D approach may not be the best choice. However, to assess the relative efficiency of these formulations, onemust investigate the trade-off between accuracy and computational cost for a given problem. In this presentation, the accuracy of results for internal fields and scattering cross section for several spherical dielectric bodies, as well as the execution times, will be used to compare the performance of the symmetric EFIE-D, EFIE-E, and EFIE-H formulations when used with tetrahedral-cell models.
  • Keywords
    dielectric bodies; differential equations; electric fields; electromagnetic wave scattering; impedance matrix; integral equations; magnetic fields; D-field; EFIE-D approach; EFIE-E approach; EFIE-H formulation; EFIE-J formulation; Schaubert-Wilton-Glisson approach; Sun-Chew formulation; curl-conforming expansion; differential equations; divergence conforming basis functions; electric field integral equation; electromagnetic field; heterogeneous dielectric bodies; low-order volume integral equation technique; magnetic field; magnetic field integral equation; piecewise-constant basis function; solenoidal representation; spherical dielectric bodies; surface-surface interaction integral; symmetric impedance matrix; tetrahedral-cell model; Accuracy; Computational efficiency; Computational modeling; Dielectrics; Electric fields; Integral equations; Mathematical model;
  • fLanguage
    English
  • Publisher
    ieee
  • Conference_Titel
    Radio Science Meeting (Joint with AP-S Symposium), 2013 USNC-URSI
  • Conference_Location
    Lake Buena Vista, FL
  • Print_ISBN
    978-1-4799-1128-8
  • Type

    conf

  • DOI
    10.1109/USNC-URSI.2013.6715465
  • Filename
    6715465