in Control Theory On the General Theory of Control Systems R. E. KALMAN Introduction In no small measure, the great technological progress in automatic control and communication systems during the past two decades has depended on advances and refinements in the mathematical study of such systems. Conversely, the growth of technology brought forth many new problems (such as those related to using digital computers in control, etc.) to challenge the ingenuity and competence of research workers concerned with theoretical questions. Despite the appearance and effective resolution of many new problems, our understanding of fundamental aspects of control has remained superficial. The only basic advance so far appears to be the theory of information created by Shannon 1. The chief significance of his work in our present interpretation is the discovery of general' laws' underlying the process of information transmission, which are quite independent of the particular models being considered or even the methods used for the des- cription and analysis of these models. These results could be compared with the' laws' of physics, with the crucial difference that the' laws' governing man-made objects cannot be discovered by straightforward experimentation but only by a purely abstract analysis guided by intuition gained in observing present-day examples of technology and economic organization. We may thus classify Shannon's result as belonging to the pure theory of communication and control, while everything else can be labelled as the applied theory; this terminology reflects the well- known distinctions between pure and applied physics or mathematics. For reasons pointed out above, in its methodo- logy the pure theory of communication and control closely resembles mathematics, rather than physics; however, it is not a. branch of mathematics because at present we cannot (yet?) d1sregard questions of physical realizability in the study of mathematical models. This paper initiates study of the pure theory of control imitating the spirit of Shannon's investigations but using entirely different techniques. Our ultimate objective is to answer questions of the following type: What kind and how much information is needed to achieve a desired type of control? What intrinsic properties characterize a given unalterable plant as far as control is concerned? At present only superficial answers are available to these questions, and even then only in special cases. Initial results presented in this Note are far from the degree of generality of Shannon's work. By contrast, however, only metho?s are employed here, giving some hope of beIng able to aVOld the well-known difficulty of Shannon's theory: methods of proof which are impractical for actually constructing practical solutions. In fact, this paper arose fr.om the need for a better understanding of some recently d1scovered computation methods of control-system syn- thesis 2-s. Another by-product of the paper is a new com- putation method for the solution of the classical Wiener filtering problem 7. The organization of the paper is as follows: 16 In Section 3 we introduce the models for which a fairly complete theory is available: dynamic systems with a finite dimensional state space and linear transition functions (i.e. systems obeying linear differential or difference equations). The class of random processes considered consists of such dynamic systems excited by an uncorrelated gaussian random process. Other assumptions, such as stationarity, discretiza- tion, single input/single output, etc., are made only to facilitate the presentation and will be absent in detailed future accounts of the theory. In Section 4 we define the concept of controllability and show that this is the' natural' generalization of the so-called' dead- beat' control scheme discovered by Oldenbourg and Sartorius 21 and later rederived independently by Tsypkin22 and the author17• We then show in Section 5 that the general problem of optimal regulation is solvable if and only if the plant is completely controllable. In Section 6 we introduce the concept of observability and solve the problem of reconstructing unmeasurable state variables from the measurable ones in the minimum possible length of time. We formalize the similarities between controllability and observability in Section 7 by means of the Principle of Duality and show that the Wiener filtering problem is the natural dual of the problem of optimal regulation. Section 8 is a brief discussion of possible generalizations and currently unsolved problems of the pure theory of control. Notation and Terminology The reader is assumed to be familiar with elements of linear algebra, as discussed, for instance, by Halmos 8. Consider an n-dimensional real vector space X. A basis in X is a set of vectors at ... , all in X such that any vector x in X can be written uniquely as (I) the Xi being real numbers, the components or coordinates of x. Vectors will be denoted throughout by small bold-face letters. The set X* of all real-valued linear functions x* (= covec- tors) on X. with the' natural' definition of addition and scalar multiplication, is an n-dimensional vector space. The value of a covector y* at any vector x is denoted by [y*, x]. We call this the inner product of y* by x. The vector space X* has a natural basis a* 1 ... , a* n associated with a given basis in X; it is defined by the requirement that [a*j, aj] = Ojj Using the' orthogonality relation' 2, we may write form n X = L [a*j, x]aj j= t which will be used frequently. (2) in the (3) For purposes of numerical computation, a vector may be considered a matrix with one column and a covector a matrix 481 491 J.S.I.A.M. CONTROI Ser. A, Vol. 1, No. Printed in U.,q.A., 1963 MATHEMATICAL DESCRIPTION OF LINEAR DYNAMICAL SYSTEMS* R. E. KALMAN Abstract. There are two different ways of describing dynamical systems: (i) by means of state w.riables and (if) by input/output relations. The first method may be regarded as an axiomatization of Newton’s laws of mechanics and is taken to be the basic definition of a system. It is then shown (in the linear case) that the input/output relations determine only one prt of a system, that which is completely observable and completely con- trollable. Using the theory of controllability and observability, methods are given for calculating irreducible realizations of a given impulse-response matrix. In par- ticular, an explicit procedure is given to determine the minimal number of state varibles necessary to realize a given transfer-function matrix. Difficulties arising from the use of reducible realizations are discussed briefly. 1. Introduction and summary. Recent developments in optimM control system theory are bsed on vector differential equations as models of physical systems. In the older literature on control theory, however, the same systems are modeled by ransfer functions (i.e., by the Laplace trans- forms of the differential equations relating the inputs to the outputs). Two differet languages have arisen, both of which purport to talk about the same problem. In the new approach, we talk about state variables, tran- sition equations, etc., and make constant use of abstract linear algebra. In the old approach, the key words are frequency response, pole-zero pat- terns, etc., and the main mathematical tool is complex function theory. Is there really a difference between the new and the old? Precisely what are the relations between (linear) vector differential equations and transfer- functions? In the literature, this question is surrounded by confusion [1]. This is bad. Communication between research workers and engineers is impeded. Important results of the "old theory" are not yet fully integrated into the new theory. In the writer’s view--which will be argued t length in this paperthe diiIiculty is due to insufficient appreciation of the concept of a dynamical system. Control theory is supposed to deal with physical systems, and not merely with mathematical objects such as a differential equation or a trans- fer function. We must therefore pay careful attention to the relationship between physical systems and their representation via differential equations, transfer functions, etc. * Received by the editors July 7, 1962 and in revised form December 9, 1962. Presented at the Symposium on Multivariable System Theory, SIAM, November 1, 1962 at Cambridge, Massachusetts. This research was supported in part under U. S. Air Force Contracts AF 49 (638)-382 and AF 33(616)-6952 as well as NASA Contract NASr-103. Research Institute for Advanced Studies (RIAS), Baltimore 12, Maryland. 152 Downloaded 11/11/13 to 152.3.159.32. Redistribution subject to SIAM license or copyright; see http://www.siam.org/journals/ojsa.php 1961-62
danilop
afilina
ivargrimstad
kno3a87
dero1to
harunatsujita
seike460
zsmb
biacco42
krpk1900
maaretp
suzukihoge
ammeep
phodgson
mclloyd
jponch
bermonpainter
chriscoyier
gr2m
csswizardry
bryan
geeforr
hannesfritz
sonatard
