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Bernard Friedland - Control System Design: An Introduction to State-Space Methods

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Bernard Friedland Control System Design: An Introduction to State-Space Methods
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    Control System Design: An Introduction to State-Space Methods
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Introduction to state-space methods covers feedback control; state-space representation of dynamic systems and dynamics of linear systems; frequency-domain analysis; controllability and observability; and shaping the dynamic response. Additional subjects encompass linear observers; compensator design by the separation principle; linear, quadratic optimum control; random processes; and Kalman filters. 1986 edition.

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Table of Contents APPENDIX MATRIX ALGEBRA AND ANALYSIS A1 - photo 1
Table of Contents

APPENDIX
MATRIX ALGEBRA AND ANALYSIS
A.1 INTRODUCTION

Matrices are widely applied in many branches of contemporary engineering, ranging from stress analysis, to electrical circuits, to engineering economics. An engineering curriculum without an introduction to matrix theory is difficult to conceive.

This appendix is not intended as a substitute for a text on matrices and their applications in engineering; there are many excellent texts available for this purpose. Rather it is intended as a concise summary of the facts about matrices that the reader will need to know in reading this book. Having them all at hand will minimize the need to consult a standard reference book. It also serves to define the notation and terminology which are, regrettably, not entirely standard.

While some derivations and proofs are given to provide motivation and insight, no attempt has been made at proving or even justifying every statement that is made. The interested reader is urged to consult a suitable textbook for details of proof, for other properties of matrices, and for many additional applications.

A.2 LINEAR EQUATIONS AND MATRIX NOTATION

Consider a system of linear equations

A1 To reduce the amount of writing A1 can be expressed as A2 - photo 2

(A.1)

To reduce the amount of writing, (A.1 ) can be expressed as

A2 The arrays of numbers enclosed by the square brackets are known as - photo 3

(A.2)

The arrays of numbers enclosed by the square brackets are known as matrices. In general a rectangular array having m columns and n rows, of the form

A3 is called an n m matrix A single letter A is used to designate the - photo 4

(A.3)

is called an n m matrix. A single letter A is used to designate the entire n m matrix. The matrices in (A.2) having only one column, namely

A4 are generally called vectors The three-dimensional vectors of - photo 5

(A.4)

are generally called vectors . (The three-dimensional vectors of classical physics are special cases of the general mathematical vectors used in this book. When, as in Chap. 3, we want to refer specifically to a physical vector such as force or velocity, we use an arrow over the letter, viz., Picture 6 )

Since a vector is a 1 n matrix, any result that applies to all n m matrices also applies to vectors. As is customary in texts on systems, vectors are generally denoted by lowercase letters and other matrices are generally denoted by capital letters.

In terms of the notation introduced above, the system of linear equations (A.1) can be written simply as

Control System Design An Introduction to State-Space Methods - image 7

(A.5)

Equation (A.5) can be read as (the vector) y is the result of multiplying (the vector) x by (the matrix) A . Thus we have defined the operation of multiplying a vector by a matrix, as the equivalent of the system of linear equations (A.1). Multiplying a vector by a matrix is a special case of multiplying one matrix by another. We shall consider this operation and others in the next section.

A 1 x 1 matrix (i.e., a single component vector) which is just a single number, is known as a scalar .

To save writing, the matrix A is sometimes exhibited as

A = [ a ij ]

where a ij is a typical element of the matrix A.

A.3 MATRIX OPERATIONS

Addition and subtraction Matrices can be combined by use of the operations of addition, subtraction, and multiplication in much the same manner as scalars. These operations may be defined in terms of systems of simultaneous equations. Thus, suppose

A6 and A7 then adding each equation in A6 to the corresponding - photo 8

(A.6)

and

A7 then adding each equation in A6 to the corresponding equation in - photo 9

(A.7)

then, adding each equation in (A.6) to the corresponding equation in (A.7) gives

or in the matrix shorthand or y z A Bx Cx where A8 T - photo 10

or, in the matrix shorthand,

or y z A Bx Cx where A8 Thus each term in the sum of two - photo 11

or

y + z = (A + B)x = Cx

where

A8 Thus each term in the sum of two matrices is the sum of the - photo 12

(A.8)

Thus each term in the sum of two matrices is the sum of the corresponding elements of the summands. It is clear from the definition that two matrices can be added only when they are both of the same dimensions: m n , and, when A + B is defined,

A9 Subtraction of two matrices is defined by A10 Multiplication - photo 13

(A.9)

Subtraction of two matrices is defined by

A10 Multiplication Multiplication of matrices is defined in terms of - photo 14

(A.10)

Multiplication Multiplication of matrices is defined in terms of substitution of one linear system of equations into another. Consider

A11 and A12 Substitute A11 into A12 to obtain A1 - photo 15

(A.11)

and

A12 Substitute A11 into A12 to obtain A13 Collecting - photo 16

(A.12)

Substitute (A.11) into (A.12) to obtain

A13 Collecting coefficients of the wi in A13 gives A14 or - photo 17

(A.13)

Collecting coefficients of the wi in (A.13) gives

A14 or where A15 Now since in shorthand notation A11 and - photo 18

(A.14)

or

where A15 Now since in shorthand notation A11 and A12 are y - photo 19

where

A15 Now since in shorthand notation A11 and A12 are y Ax and x - photo 20

(A.15)

Now, since in shorthand notation (A.11) and (A.12) are

y = Ax and x = Bw

we can write

y = A ( Bw ) = ABw = Cw

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