Huygens and the computer-a powerful alliance in numerical electromagnetics

A time domain technique based on equivalent transmission line interconnections, referred to as the transmission line matrix model (TLM), is presented. The author retraces the history of TLM, from the original concepts of Huygens to the pioneering work of Peter B. Johns, and on to the latest developments in TLM modeling. The most important two-dimensional and three-dimensional TLM algorithms are explained, and new concepts in time-domain representation of frequency-dispersive boundaries are discussed. Some typical applications are described. >

[1]  P. B. Johns On the Relationship Between TLM and Finite-Difference Methods for Maxwell's Equations (Short Paper) , 1987 .

[2]  P. B. Johns,et al.  The Solution of Inhomogeneous Waveguide Problems Using a Transmission-Line Matrix , 1974 .

[3]  W.J.R. Hoefer,et al.  Dominant and Second-Order Mode Cutoff Frequencies in Fin Lines Calculated with a Two-Dimensional TLM Program , 1980 .

[4]  P. B. Johns,et al.  The use of time domain diakoptics in time discrete models of fields , 1981 .

[5]  I. Fukai,et al.  Transient Analysis of a Stripline Having a Corner in Three-Dimensional Space , 1984 .

[6]  Eswarappa,et al.  Transmission line matrix modeling of disperse wide-band absorbing boundaries with time-domain diakoptics for S-parameter extraction , 1990 .

[7]  P. B. Johns,et al.  Numerical solution of lossy waveguides: t.l.m. computer program , 1974 .

[8]  P. Johns A Symmetrical Condensed Node for the TLM Method , 1987 .

[9]  Wolfgang J. R. Hoefer,et al.  The Simulation of Three-Dimensional Wave Propagation by a Scalar TLM Model , 1984 .

[10]  P. B. Johns,et al.  Generalised elements for t.l.m. method of numerical analysis , 1975 .

[11]  Sina Akhtarzad Analysis of lossy microwave structures and microstrip resonators by the TLM method , 1975 .

[12]  P.P.M. So,et al.  New procedures for 2-D and 3-D microwave circuit analysis with the TLM method , 1990, IEEE International Digest on Microwave Symposium.

[13]  Wolfgang J. R. Hoefer,et al.  The discrete time-domain green's function or Johns matrix - A new powerful concept in transmission line modelling(TLM). , 1989 .

[14]  C. Concordia,et al.  Network Analyzer Studies of Electromagnetic Cavity Resonators , 1944, Proceedings of the IRE.

[15]  Wolfgang J. R. Hoefer,et al.  The Transmission-Line Matrix Method--Theory and Applications , 1985 .

[16]  P. B. Johns,et al.  Three-Dimensional Transmission-Line Matrix Computer Analysis of Microstrip Resonators , 1975 .

[17]  P.P.M. So,et al.  A two-dimensional transmission line matrix microwave field simulator using new concepts and procedures , 1989 .

[18]  P. B. Johns,et al.  Application of the transmission-line-matrix method to homogeneous waveguides of arbitrary cross-section , 1972 .

[19]  S. Ramo,et al.  A New Approach to the Solution of High-Frequency Field Problems , 1944, Proceedings of the IRE.

[20]  P. B. Johns,et al.  On the construction and numerical solution of transmission‐line and lumped network models of Maxwell's equations , 1980 .

[21]  Thomas Weiland,et al.  Solution of Maxwell's equations , 1992 .

[22]  P. Johns,et al.  Solution of Maxwell's equations in three space dimensions and time by the t.l.m. method of numerical analysis , 1975 .

[23]  P. Saguet,et al.  An improvement for the t.l.m. method , 1980 .

[24]  P. B. Johns,et al.  A new mathematical model to the physics of propagation , 1974 .

[25]  G. Kron,et al.  Equivalent Circuit of the Field Equations of Maxwell-I , 1944, Proceedings of the IRE.

[26]  P. Saguet,et al.  Utilisation d'un nouveau type de noeud dans la méthode TLM en 3 dimensions (Usage of a new type of node in the 3D TLM method) , 1982 .

[27]  P. B. Johns,et al.  Time domain approximations in the solution of fields by time domain diakoptics , 1982 .

[28]  J. M. Undrill,et al.  Diakoptics and networks , 1971 .

[29]  A. Brameller,et al.  Practical Diakoptics for Electrical Networks , 1969 .

[30]  P. Saguet,et al.  Le maillage rectangulaire et le changement de maille dans la méthode TLM en deux dimensions (Rectangular meshing and mesh change in the 2D TLM method) , 1981 .

[31]  P. B. Johns,et al.  Solution of 6-component electromagnetic fields in three space dimensions and time by the t.l.m. method , 1974 .

[32]  P. B. Johns New symmetrical condensed node for three-dimensional solution of electromagnetic-wave problems by TLM , 1986 .

[33]  P.P.M. So,et al.  A general planar circuit simulator based on two-dimensional TLM method , 1989, IEEE MTT-S International Microwave Symposium Digest.

[34]  J. E. Sitch,et al.  Transmission-line matrix method with irregularly graded space , 1981 .

[35]  P. B. Johns,et al.  Dispersion characteristic of a microstrip line with a step discontinuity , 1975 .

[36]  Peter B. Johns,et al.  Numerical solution of 2-dimensional scattering problems using a transmission-line matrix , 1971 .