By Clayton R. Paul
An geared up and concise exposition consolidating all study within the literature in this subject. info present tools for fixing multiconductor transmission-line equations to figure out voltage and/or currents prompted on the ends of conductors of the road from signs on different conductors or signs from incident assets. incorporates a disk of FORTRAN codes enforcing all the answer strategies, lots of end-of-chapter difficulties and rankings of computed effects for real traces.
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Additional info for Analysis of Multiconductor Transmission Lines (Wiley Series in Microwave & Optical Engineering, 28)
This decomposition can be obtained by writing, from Fig. 17 Illustration of the decomposition of total currents into differential-mode (transmission-line-mode) and common-mode (antenna-mode)components. 91)represents a nonsingular transformation between the two sets of currents since the transformation matrix is nonsingular. 93) Ordinarily, the common-mode currents are much smaller in magnitude than the differential-mode currents so they do not substantially affect the results of an analysis of currents and voltages of a transmission line.
L. Stratonovich, The Propagation of Electromagnetic Waves in Multiconductor Transmission Lines, Macmillan, NY, 1964. C. Magnuson, Transmission Lines and Wave Propagation, Allyn and Bacon, Newton, MA, 1970. E. , IEEE Press, NY, 1991. J. Zaborsky and J. W. Rittenhouse, Electric Power Transmission, Ronald Press, NY, 1954. E. Matick, Transmission Lines for Digital arid Communication Networks, McGraw-Hill, NY, 1969. L. ), Parallel Coupled Lines and Directional Couplers, Artech House, Dedham, Massachusetts, 1972.
4 Illustration of the identity 4 x dJ x e$ - -4. , u = 0. 13b) ;) PROPERTIES OF THE TRANSVERSE ELECTROMAGNETIC (TEN MODE OF PROPAGATION 11 where the intrinsic impedance of the medium is F (I. 13d) JG The function J+(x, y, t - z/v) represents a forward-traueling waue since as t progresses z must increase to keep the argument constant and track corresponding points on the waveform. Similarly, the function f - ( x , y, t z/v) represents a backward-truueling waue, a wave traveling in the - z direction.