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Volume 8 Issue 5
Sep.  1986
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Liu Ying, Liu Sanyang, Wu Jianping. Multicast routing algorithm for multimedia communication[J]. Journal of Electronics & Information Technology, 2002, 24(7): 948-953.
Citation: Zhou Wenbiao. DETERMINATION OF THE CHARACTERISTICS OF TEM TRANSMISSION LINE WITH ARBITRARY CROSSSECTION BY BOUNDARY ELEMENT METHOD[J]. Journal of Electronics & Information Technology, 1986, 8(5): 389-396.

DETERMINATION OF THE CHARACTERISTICS OF TEM TRANSMISSION LINE WITH ARBITRARY CROSSSECTION BY BOUNDARY ELEMENT METHOD

  • Received Date: 1985-09-13
  • Rev Recd Date: 1986-02-15
  • Publish Date: 1986-09-19
  • The boundary element method of potential theory is described in this paper. It is used to analyze the characteristic impedance of TEM transmission line with arbtrary cross-seetions. It is shown that the boundary element method has some advantages, such as the number of nodes required for this method is less than that for the finite element method, and the accuracy of this method is higher than that of the moment method.
  • C. A. Brebbia, The Boundary Element Method for Engineers, Pentech Press, London, 1978, ch. 2.[2]C. A, Brebbia, Boundary Element Techniques: Theory and Application in Engineering, Springer,Berlin, 1984. [3] S. Kagami and I. Fukai, IEEE Trans. on MTT, MTT-32(1984 ), 455.[3]李忠元,电子科学学刊,7(1985), 161.[4]H. E. Green, IEEE Trans. on MTT, MTT-13 (1965), 676.[5]J. R. Nortier and D. A. McNamara, Microwave J. 27 (1984) 11, 109.[6]杨乃恒,现代雷达,1963,第6期,第77页.[7]R. F. Harrington, Time-Harmonic Electromagnetic Field, McGraw-Hill, New York, 1961.[8]Weigan Lin(林为干),IEEE Trans. on MTT, MTT-30 (1982 ), 1981.[9]林为干,电磁场工程,人民邮电出版社,1982, p. 151.[10]H. E. Green, IEEE Trans. on MTT,MTT-11(1963), 554.[11]R. E. Collin, Field Theory of Guided Waves, McGraw-Hill, New York, 1964, ch. 4.[12]J. J. Skiles and T. J. Higgins, Determination of the Characteristic Impedance of U. H. F. Coaxial Rectangular Transmission Line, Proc. Natl. Electronics Conference, 10, 1954, p, 97.[13]T. S. Chen, IRE Trans. on MTT, MTT-8(1960), 510.
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