Bostwick F. Wyman

On the zeros and poles of a transfer function

Abstract The poles and zeros of a linear transfer function can be studied by means of the pole module and the transmission zero module. These algebraic constructions yield finite dimensional vector spaces whose dimensions are the number of poles and the number of multivariable zeros of the transfer function. In addition, these spaces carry the structure of a module over a ring of polynomials, which gives them a dynamical or state space structure. The analogous theory at infinity gives finite dimensional spaces which are modules over the valuation ring of proper rational functions. Following ideas of Wedderburn and Forney, we introduce new finite dimensional vector spaces which measure generic zeros which arise when a transfer function fails to be injective or surjective. A new exact sequence relates the global spaces of zeros, the global spaces of poles, and the new generic zero spaces. This sequence gives a structural result which can be summarized as follows: “The number of zeros of any transfer function is equal to the number of poles (when everything is counted appropriately).” The same result unifies and extends a number of results of geometric control theory by relating global poles and zeros of general (possibly improper) transfer functions to controlled invariant and controllability subspaces (including such spaces at infinity).

Fixed poles in transfer function equations

In this paper we study the pole structure of the solutions

Module theoretic zero structures for system matrices

H(z)

On the zeros of a minimal realization

, if any, of equations of the form

Poles and Zeros of Matrices of Rational Functions

T(z) = H(z)G(z)

On the design of pole modules for inverse systems

or, dually,

Duality and the regulator problem for linear systems over commutative rings

T(z) = F(z)H(z)

Rigid Body Dynamics, Constraints, and Inverses

, where

The zero module and invariant subspaces

T(z)

A simple strategy for jumping straight up.

and