

From this point of view, a one dimensional propagation phenomenon takes place on a transmission line.
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In the most general terms, a transmission line is a system of metal conductors and/or dielectric insulating media that is capable of “guiding” the energy transfer between a generator and a load, irrespective (at least with a good approximation) of the bends that the line undergoes because of installation needs. In other applications, instead, electromagnetic energy must be transferred from one place to the other along a well defined path without any spreading at all: an example is the cabling of a building. In telecommunications this behavior can be useful when the user position is not known in advance, as in a broadcasting system or in a cell phone network.

Transmission line equations and their solution 1.1Įlectromagnetic energy, once generated in one place, has a natural tendency to spread in the whole space at a speed close to 300.000 Km/s. General solution of transmission line equations. 118 8 Time domain analysis of transmission lines 115 7.10.3 Change of reference impedance for a one-port load. 114 2ħ.10.2 Interconnection of two two-ports by means of a length of transmission line. 112ħ.10 Examples of analysis of structures described by S matricesħ.10.1 Cascade connection of a two-port and a load. Properties of the scattering matrix of a device. 103Ĭomputation of the power dissipated in a device. įrequency dependence of phase constant and characteristic impedance. Loss parameters of some transmission lines. Ĥ Energy dissipation in transmission linesĭielectric losses. Line voltage, current and impedance diagrams. Ģ Parameters of common transmission linesĬoaxial cable. Solution of transmission line equations by the matrix technique. Propagation of the electric state and geometrical interpretations. Transmission line equations in the frequency domain. Review of Fourier transforms and phasors. Lecture Notes on Transmission Line Theoryġ Transmission line equations and their solution
