SynopsisIn the paper, a general procedure for realising the state model of an LC «-port network is presented. Realisation procedures of w-port LC networks are well established if the specification is given in the complex-frequency domain. The procedure presented here represents an alternative to these well established methods, and is believed to give new insight into the problem of transformerless realisation of LC networks.List of principal symbols G = network graph T = a tree T = complement of a tree T, cotree B,j = submatrixes in the fundamental circuit matrix C h -diagonal matrix-the element values of tree-branch capacitors C c = diagonal matrix-the element values of link capacitors L h = diagonal matrix-the element values of tree-branch inductors L c -diagonal matrix-the element values of link inductors / 0 = current vector of voltage sources I hc = current vector of tree-branch capacitors J cc = current vector of link capacitors I hl = current vector of tree-branch inductors J cl = current vector of link inductors I x -current source vector V o = voltage source vector V hc = voltage vector of tree-branch capacitors V cc = voltage vector of link capacitors V hl = voltage vector of tree-branch inductors V ct = voltage vector of link inductors V x = voltage vector of current sources Y c -admittance matrix of a capacitor network Z L -impedance matrix of an inductor network
IntroductionRecently, it has been recognised by many investigators that the topological approach to the synthesis problem might offer new insight. Indeed, the problem of synthetising n-terminal resistive networks characterised by the impedance or admittance matrixes of order « -1 is completely solved. 1 Although extension of resistive network synthesis to some very special class of multiterminal RLC networks is also known, 2 the solution of the general problem appears, at best, to be very difficult.One logical approach to the RLC network synthesis is through state models, since, in general, such a model of the network provides more direct information about the network topology than do the more conventional network matrixes. Recently, some works have been initiated in this direction. 3 " 6 This paper considers only the synthesis of LC networks.The general form of the state model of an RLC network, in symbolic form, iswhere X is called the state vector and consists of some treebranch capacitor voltages and some link inductor currents, and Y is a vector which contains the specified voltages and currents in the source branches; Y contains the complementary variables; i.e. the complementary currents and voltages, respectively, in the source branches, of those Y.The coefficient matrix A is real and square, and is called the operator matrix. 7 All other matrixes B, C, P, Q and R are real and, in general, rectangular.In the synthesis procedure presented here, it is necessary to establish these coefficients as a function of the network structure. The voltage components in the state vector X in eqn. so that T 2 contains T|. Then T 2 is a tree in G and ...