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LINEAR ALGEBRA OUTLINE 600+ Q & A WITH RATIONALES GUARANTEED A+

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1.1 Introduction There are two ways to motivate the notion of a vector: one is by means of lists of numbers and subscripts, and the other is by means of certain objects in physics. We discuss these two ways below. Here we assume the reader is familiar with the elementary properties of the field of real numbers, denoted by R. On the other hand, we will review properties of the field of complex numbers, denoted by C. In the context of vectors, the elements of our number fields are called scalars. Although we will restrict ourselves in this chapter to vectors whose elements come from R and then from C, many of our operations also apply to vectors whose entries come from some arbitrary field K. Lists of Numbers Suppose the weights (in pounds) of eight students are listed as follows: 156; 125; 145; 134; 178; 145; 162; 193 One can denote all the values in the list using only one symbol, say w, but with different subscripts; that is, w1; w2; w3; w4; w5; w6; w7; w8 Observe that each subscript denotes the position of the value in the list. For example, w1 ¼ 156; the first number; w2 ¼ 125; the second number; ... Such a list of values, w ¼ ðw1;w2;w3; ... ; w8Þ is called a linear array or vector. Vectors in Physics Many physical quantities, such as temperature and speed, possess only ‘‘magnitude.’’ These quantities can be represented by real numbers and are called scalars. On the other hand, there are also quantities, such as force and velocity, that possess both ‘‘magnitude’’ and ‘‘direction.’’ These quantities, which can be represented by arrows having appropriate lengths and directions and emanating from some given reference point O, are called vectors. Now we assume the reader is familiar with the space R3 where all the points in space are represented by ordered triples of real numbers. Suppose the origin of the axes in R3 is chosen as the reference point O for the vectors discussed above. Then every vector is uniquely determined by the coordinates of its endpoint, and vice versa. There are two important operations, vector addition and scalar multiplication, associated with vectors in physics. The definition of these operations and the relationship between these operations and the endpoints of the vectors are as follows. 1 CHAPTER 1 (i) Vector Addition: The resultant u þ v of two vectors u and v is obtained by the parallelogram law; that is, u þ v is the diagonal of the parallelogram formed by u and v. Furthermore, if ða; b; cÞ and ða0 ; b0 ; c0 Þ are the endpoints of the vectors u and v, then ða þ a0 ; b þ b0 ; c þ c0 Þ is the endpoint of the vector u þ v. These properties are pictured in Fig. 1-1(a). (ii) Scalar Multiplication: The product ku of a vector u by a real number k is obtained by multiplying the magnitude of u by k and retaining the same direction if k 0 or the opposite direction if k 0. Also, if ða; b; cÞ is the endpoint of the vector u, then ðka; kb; kcÞ is the endpoint of the vector ku. These properties are pictured in Fig. 1-1(b). Mathematically, we identify the vector u with its ða; b; cÞ and write u ¼ ða; b; cÞ. Moreover, we call the ordered triple ða; b; cÞ of real numbers a point or vector depending upon its interpretation. We generalize this notion and call an n-tuple ða1; a2; ... ; anÞ of real numbers a vector. However, special notation may be used for the vectors in R3 called spatial vectors (Section 1.6). 1.2 Vectors in Rn The set of all n-tuples of real numbers, denoted by Rn , is called n-space. A particular n-tuple in Rn , say u ¼ ða1; a2; ... ; anÞ is called a point or vector. The numbers ai are called the coordinates, components, entries, or elements of u. Moreover, when discussing the space Rn, we use the term scalar for the elements of R. Two vectors, u and v, are equal, written u ¼ v, if they have the same number of components and if the corresponding components are equal. Although the vectors ð1; 2; 3Þ and ð2; 3; 1Þ contain the same three numbers, these vectors are not equal because corresponding entries are not equal. The vector ð0; 0; ... ; 0Þ whose entries are all 0 is called the zero vector and is usually denoted by 0. EXAMPLE 1.1 (a) The following are vectors: ð2; 5Þ; ð7; 9Þ; ð0; 0; 0Þ; ð3; 4; 5Þ The first two vectors belong to R2 , whereas the last two belong to R3 . The third is the zero vector in R3. (b) Find x; y;z such that ðx  y; x þ y; z  1Þ¼ð4; 2; 3Þ. By definition of equality of vectors, corresponding entries must be equal. Thus, x  y ¼ 4; x þ y ¼ 2; z  1 ¼ 3 Solving the above system of equations yields x ¼ 3, y ¼ 1, z ¼

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,SCHAUM’S SCHAUM’S
outlines outlines



Linear Algebra
Fourth Edition




Seymour Lipschutz, Ph.D.
Temple University


Marc Lars Lipson, Ph.D.
University of Virginia




Schaum’s Outline Series




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,Copyright © 2009, 2001, 1991, 1968 by The McGraw-Hill Companies, Inc. All rights reserved. Except as permitted under the United States Copyright Act of
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, Preface
Linear algebra has in recent years become an essential part of the mathematical background required by
mathematicians and mathematics teachers, engineers, computer scientists, physicists, economists, and
statisticians, among others. This requirement reflects the importance and wide applications of the subject
matter.
This book is designed for use as a textbook for a formal course in linear algebra or as a supplement to all
current standard texts. It aims to present an introduction to linear algebra which will be found helpful to all
readers regardless of their fields of specification. More material has been included than can be covered in most
first courses. This has been done to make the book more flexible, to provide a useful book of reference, and to
stimulate further interest in the subject.
Each chapter begins with clear statements of pertinent definitions, principles, and theorems together with
illustrative and other descriptive material. This is followed by graded sets of solved and supplementary
problems. The solved problems serve to illustrate and amplify the theory, and to provide the repetition of basic
principles so vital to effective learning. Numerous proofs, especially those of all essential theorems, are
included among the solved problems. The supplementary problems serve as a complete review of the material
of each chapter.
The first three chapters treat vectors in Euclidean space, matrix algebra, and systems of linear equations.
These chapters provide the motivation and basic computational tools for the abstract investigations of vector
spaces and linear mappings which follow. After chapters on inner product spaces and orthogonality and on
determinants, there is a detailed discussion of eigenvalues and eigenvectors giving conditions for representing
a linear operator by a diagonal matrix. This naturally leads to the study of various canonical forms,
specifically, the triangular, Jordan, and rational canonical forms. Later chapters cover linear functions and
the dual space V*, and bilinear, quadratic, and Hermitian forms. The last chapter treats linear operators on
inner product spaces.
The main changes in the fourth edition have been in the appendices. First of all, we have expanded
Appendix A on the tensor and exterior products of vector spaces where we have now included proofs on the
existence and uniqueness of such products. We also added appendices covering algebraic structures, including
modules, and polynomials over a field. Appendix D, ‘‘Odds and Ends,’’ includes the Moore–Penrose
generalized inverse which appears in various applications, such as statistics. There are also many additional
solved and supplementary problems.
Finally, we wish to thank the staff of the McGraw-Hill Schaum’s Outline Series, especially Charles Wall,
for their unfailing cooperation.

SEYMOUR LIPSCHUTZ
MARC LARS LIPSON




iii

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