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A theory of nonlinear networks. I

R. K. Brayton, J. K. Moser

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Source: Crossref

Published: Apr 1, 1964

DOI: 10.1090/qam/169746

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Source abstract

This report describes a new approach to nonlinear RLC-networks which is based on the fact that the system of differential equations for such networks has the special form L(i)didt=∂P(i,v)∂i,C(v)dvdt=−∂P(i,v)∂v.L(i)didt=∂P(i,v)∂i,C(v)dvdt=−∂P(i,v)∂v. L ( i ) d i d t = ∂ P ( i , v ) ∂ i , C ( v ) d v d t = − ∂ P ( i , v ) ∂ v . L\left ( i \right )\frac {{di}}{{dt}} = \frac {{\partial P\left ( {i,v} \right )}}{{\partial i}},C\left ( v \right )\frac {{dv}}{{dt}} = - \frac {{\partial P\left ( {i,v} \right )}}{{\partial v}}. The function, P ( i , v ) P\left ( {i,v} \right ) , called the mixed potential function, can be used to construct Liapounov-type functions to prove stability under certain conditions. Several theorems on the stability of circuits are derived and examples are given to illustrate the results. A procedure is given to construct the mixed potential function directly from the circuit. The concepts of a complete set of mixed variables and a complete circuit are defined.

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