Linear Network Theory by K. F. Sander and P. Hammond (Auth.)

Linear Network Theory by K. F. Sander and P. Hammond (Auth.)

By K. F. Sander and P. Hammond (Auth.)

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4 7\ = 0. RELATIONS BETWEEN PARAMETERS OF A RECIPROCAL 2-PORT NETWORK The particular relations existing in each set of parameters when reciprocity applies may be deduced by expressing them in terms CLASSIFICATION AND DESCRIPTION OF NETWORKS of the elements of of equation (11) experiments such V2 = 0. Equation 43 the impedance matrix, or by direct application of Chapter 1. (24) INTERCONNECTION OF 2-PORT NETWORKS The interconnection of 2-port networks is a matter of consider­ able importance. The most important is that of cascading.

In the cascade matrix A and D are real, B and C purely imaginary. m-TERMINAL + REFERENCE NETWORKS If of the n nodes of a network, only m(

The equation for this branch will be written 24 LINEAR NETWORK THEORY Since the combination }ù is the only one in which j occurs, it is algebraically convenient to writef J = P This gives the final branch equation /r = j r + y r ( p ) i / r (io) where Yr (p) = — + Cr p + ~(11) Lrp Rr This expression is of course the admittance of the parallel L, C, R circuit. The general parallel branch has been chosen because it is intended to formulate the network equation in nodal form. f. It is also possible to transform the circuit of Fig.

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