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MATH 233 - Linear Algebra I
Lecture Notes
Cesar O. Aguilar
Department of Mathematics
SUNY Geneseo
Lecture 0
Contents
1 Systems of Linear Equations1
1.1 What is a system of linear equations?. . . . . . . . . . . . . . . . . . . . . . 1
1.2 Matrices. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
1.3 Solving linear systems. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
1.4 Geometric interpretation of the solution set. . . . . . . . . . . . . . . . . . 8
2 Row Reduction and Echelon Forms11
2.1 Row echelon form (REF). . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11
2.2 Reduced row echelon form (RREF). . . . . . . . . . . . . . . . . . . . . . . 13
2.3 Existence and uniqueness of solutions. . . . . . . . . . . . . . . . . . . . . . 17
3 Vector Equations19
3.1 Vectors inRn. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19
3.2 The linear combination problem. . . . . . . . . . . . . . . . . . . . . . . . . 21
3.3 The span of a set of vectors. . . . . . . . . . . . . . . . . . . . . . . . . . . 26
4 The Matrix Equation Ax=b31
4.1 Matrix-vector multiplication. . . . . . . . . . . . . . . . . . . . . . . . . . . 31
4.2 Matrix-vector multiplication and linear combinations. . . . . . . . . . . . . 33
4.3 The matrix equation problem. . . . . . . . . . . . . . . . . . . . . . . . . . 34
5 Homogeneous and Nonhomogeneous Systems41
5.1 Homogeneous linear systems. . . . . . . . . . . . . . . . . . . . . . . . . . . 41
5.2 Nonhomogeneous systems. . . . . . . . . . . . . . . . . . . . . . . . . . . . 44
5.3 Summary. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 47
6 Linear Independence49
6.1 Linear independence. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49
6.2 The maximum size of a linearly independent set. . . . . . . . . . . . . . . . 53
7 Introduction to Linear Mappings57
7.1 Vector mappings. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 57
7.2 Linear mappings. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 58
7.3 Matrix mappings. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61
7.4 Examples. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 62
3CONTENTS
8 Onto, One-to-One, and Standard Matrix67
8.1 Onto Mappings. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 67
8.2 One-to-One Mappings. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 69
8.3 Standard Matrix of a Linear Mapping. . . . . . . . . . . . . . . . . . . . . . 71
9 Matrix Algebra75
9.1 Sums of Matrices. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 75
9.2 Matrix Multiplication. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 76
9.3 Matrix Transpose. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 80
10 Invertible Matrices83
10.1 Inverse of a Matrix. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 83
10.2 Computing the Inverse of a Matrix. . . . . . . . . . . . . . . . . . . . . . . 85
10.3 Invertible Linear Mappings. . . . . . . . . . . . . . . . . . . . . . . . . . . . 87
11 Determinants89
11.1 Determinants of 2×2 and 3×3 Matrices. . . . . . . . . . . . . . . . . . . . 89
11.2 Determinants ofn×nMatrices. . . . . . . . . . . . . . . . . . . . . . . . . 93
11.3 Triangular Matrices. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 95
12 Properties of the Determinant97
12.1 ERO and Determinants. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 97
12.2 Determinants and Invertibility of Matrices. . . . . . . . . . . . . . . . . . . 100
12.3 Properties of the Determinant. . . . . . . . . . . . . . . . . . . . . . . . . . 100
13 Applications of the Determinant103
13.1 The Cofactor Method. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 103
13.2 Cramer"s Rule. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 106
13.3 Volumes. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 107
14 Vector Spaces109
14.1 Vector Spaces. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 109
14.2 Subspaces of Vector Spaces. . . . . . . . . . . . . . . . . . . . . . . . . . . . 112
15 Linear Maps117
15.1 Linear Maps on Vector Spaces. . . . . . . . . . . . . . . . . . . . . . . . . . 117
15.2 Null space and Column space. . . . . . . . . . . . . . . . . . . . . . . . . . 121
16 Linear Independence, Bases, and Dimension125
16.1 Linear Independence. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 125
16.2 Bases. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 126
16.3 Dimension of a Vector Space. . . . . . . . . . . . . . . . . . . . . . . . . . . 128
17 The Rank Theorem133
17.1 The Rank of a Matrix. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 133
4Lecture 0
18 Coordinate Systems137
18.1 Coordinates. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 137
18.2 Coordinate Mappings. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 141
18.3 Matrix Representation of a Linear Map. . . . . . . . . . . . . . . . . . . . . 142
19 Change of Basis147
19.1 Review of Coordinate Mappings onRn. . . . . . . . . . . . . . . . . . . . . 147
19.2 Change of Basis. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 149
20 Inner Products and Orthogonality153
20.1 Inner Product onRn. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 153
20.2 Orthogonality. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 156
20.3 Coordinates in an Orthonormal Basis. . . . . . . . . . . . . . . . . . . . . . 158
21 Eigenvalues and Eigenvectors163
21.1 Eigenvectors and Eigenvalues. . . . . . . . . . . . . . . . . . . . . . . . . . 163
21.2 Whenλ= 0 is an eigenvalue. . . . . . . . . . . . . . . . . . . . . . . . . . . 168
22 The Characteristic Polynomial169
22.1 The Characteristic Polynomial of a Matrix. . . . . . . . . . . . . . . . . . . 169
22.2 Eigenvalues and Similarity Transformations. . . . . . . . . . . . . . . . . . 176
23 Diagonalization179
23.1 Eigenvalues of Triangular Matrices. . . . . . . . . . . . . . . . . . . . . . . 179
23.2 Diagonalization. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 180
23.3 Conditions for Diagonalization. . . . . . . . . . . . . . . . . . . . . . . . . . 182
24 Diagonalization of Symmetric Matrices187
24.1 Symmetric Matrices. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 187
24.2 Eigenvectors of Symmetric Matrices. . . . . . . . . . . . . . . . . . . . . . . 188
24.3 Symmetric Matrices are Diagonalizable. . . . . . . . . . . . . . . . . . . . . 188
25 The PageRank Algortihm191
25.1 Search Engine Retrieval Process. . . . . . . . . . . . . . . . . . . . . . . . . 191
25.2 A Description of the PageRank Algorithm. . . . . . . . . . . . . . . . . . . 192
25.3 Computation of the PageRank Vector. . . . . . . . . . . . . . . . . . . . . . 195
26 Discrete Dynamical Systems197
26.1 Discrete Dynamical Systems. . . . . . . . . . . . . . . . . . . . . . . . . . . 197
26.2 Population Model. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 197
26.3 Stability of Discrete Dynamical Systems. . . . . . . . . . . . . . . . . . . . 199
5Lecture 1
Lecture 1
Systems of Linear Equations
In this lecture, we will introduce linear systems and the method of row reduction to solve them. We will introduce matrices as a convenient structure to represent and solve linear systems. Lastly, we will discuss geometric interpretations of the solution set of a linear system in 2- and 3-dimensions.1.1 What is a system of linear equations?
Definition 1.1:Asystem ofmlinear equationsinnunknown variablesx1,x2,...,xn is a collection ofmequations of the form a11x1+a12x2+a13x3+···+a1nxn=b1
a21x1+a22x2+a23x3+···+a2nxn=b2
a31x1+a32x2+a33x3+···+a3nxn=b3.
a The numbersaijare called thecoefficientsof the linear system; because there aremequa- tions andnunknown variables there are theforem×ncoefficients. The main problem with a linear system is of course to solve it: Problem:Find a list ofnnumbers (s1,s2,...,sn) that satisfy the system of linear equa- tions ( 1.1). In other words, if we substitute the list of numbers (s1,s2,...,sn) for the unknown variables (x1,x2,...,xn) in equation (1.1) then the left-hand side of theith equation will
equalbi. We call such a list (s1,s2,...,sn)a solutionto the system of equations. Notice that we say "a solution" because there may be more than one. Thesetof all solutions to a linear system is called itssolution set. As an example of a linear system, below is a linear 1Systems of Linear Equations
system consisting ofm= 2 equations andn= 3 unknowns: x1-5x2-7x3= 0
5x2+ 11x3= 1
Here is a linear system consisting ofm= 3 equations andn= 2 unknowns: -5x1+x2=-1 πx1-5x2= 0
63x1-⎷
2x2=-7
And finally, below is a linear system consisting ofm= 4 equations andn= 6 unknowns: -5x1+x3-44x4-55x6=-1 πx1-5x2-x3+ 4x4-5x5+⎷
5x6= 0
63x1-⎷
2x2-15x3+ ln(3)x4+ 4x5-133x6= 0
63x1-⎷
2x2-15x3-18x4-5x6= 5
Example 1.2.Verify that (1,2,-4) is a solution to the system of equations2x1+ 2x2+x3= 2
x1+ 3x2-x3= 11.
Is (1,-1,2) a solution to the system?
Solution.The number of equations ism= 2 and the number of unknowns isn= 3. There arem×n= 6 coefficients:a11= 2,a12= 1,a13= 1,a21= 1,a22= 3, anda23=-1. And b1= 0 andb2= 11. The list of numbers (1,2,-4) is a solution because
2·(1) + 2(2) + (-4) = 2
(1) + 3·(2)-(-4) = 11On the other hand, for (1,-1,2) we have that
2(1) + 2(-1) + (2) = 2
but1 + 3(-1)-2 =-4?= 11.
Thus, (1,-1,2) is not a solution to the system.
A linear system may not have a solution at all. If this is the case, we saythat the linear system isinconsistent: 2Lecture 1
INCONSISTENT?NO SOLUTION
A linear system is calledconsistentif it has at least one solution:CONSISTENT?AT LEAST ONE SOLUTION
We will see shortly that a consistent linear system will have either just one solution or infinitely many solutions. For example, a linear system cannot have just 4 or 5 solutions. If it has multiple solutions, then it will have infinitely many solutions. Example 1.3.Show that the linear system does not have a solution. -x1+x2= 3 x1-x2= 1.
Solution.If we add the two equations we get
0 = 4 which is a contradiction. Therefore, there does not exist a list (s1,s2) that satisfies the system because this would lead to the contradiction 0 = 4. Example 1.4.Lettbe an arbitrary real number and let s 1=-3 2-2t s 2=3 2+t s 3=t. Show that for any choice of the parametert, the list (s1,s2,s3) is a solution to the linear system x1+x2+x3= 0
x1+ 3x2-x3= 3.
Solution.Substitute the list (s1,s2,s3) into the left-hand-side of the first equation ?-32-2t?+?32+t?+t= 0
and in the second equation ?-32-2t?+ 3(32+t)-t=-32+92= 3
Both equations are satisfied for any value oft. Because we can varytarbitrarily, we get an infinite number of solutions parameterized byt. For example, compute the list (s1,s2,s3) fort= 3 and confirm that the resulting list is a solution to the linear system. 3Systems of Linear Equations
1.2 Matrices
We will usematricesto develop systematic methods to solve linear systems and to study the properties of the solution set of a linear system. Informally speaking, amatrixis an array or table consisting ofrowsandcolumns. For example, A=??1-2 1 0
0 2-8 8
-4 7 11-5?? is a matrix havingm= 3 rows andn= 4 columns. In general, a matrix withmrows and ncolumns is am×nmatrix and the set of all such matrices will be denoted byMm×n. Hence,Aabove is a 3×4 matrix. The entry ofAin theith row andjth column will be denoted byaij. A matrix containing only one column is called acolumn vectorand a matrix containing only one row is called arow vector. For example, here is a row vector u=?1-3 4? and here is a column vector v=?3 -1? We can associate to a linear system three matrices: (1) the coefficient matrix, (2) the output column vector, and (3) the augmented matrix. For example, for the linear system5x1-3x2+ 8x3=-1
x1+ 4x2-6x3= 0
2x2+ 4x3= 3
the coefficient matrixA, the output vectorb, and the augmented matrix [A b] are: A=?? 5-3 8 1 4-60 2 4??
,b=?? -1 0 3?? ,[A b] =??5-3 8-1
1 4-6 0
0 2 4 3??
If a linear system hasmequations andnunknowns then the coefficient matrixAmust be a m×nmatrix, that is,Ahasmrows andncolumns. Using our previously defined notation, we can write this asA?Mm×n. If we are given an augmented matrix, we can write down the associated linear system in an obvious way. For example, the linear system associated to the augmented matrix??1 4-2 8 120 1-7 2-4
0 0 5-1 7??
is x1+ 4x2-2x3+ 8x4= 12
x2-7x3+ 2x4=-4
5x3-x4= 7.
4Lecture 1
We can study matrices without interpreting them as coefficient matrices or augmented ma- trices associated to a linear system.Matrix algebrais a fascinating subject with numerous applications in every branch of engineering, medicine, statistics, mathematics, finance, biol- ogy, chemistry, etc.1.3 Solving linear systems
In algebra, you learned to solve equations by first "simplifying" themusing operations that do not alter the solution set. For example, to solve 2x= 8-2xwe can add to both sides2xand obtain 4x= 8 and then multiply both sides by1
4yieldingx= 2. We can do
similar operations on a linear system. There are three basic operations, calledelementary operations, that can be performed:1.Interchange two equations.
2.Multiply an equation by a nonzero constant.
3.Add a multiple of one equation to another.
These operations do not alter the solution set. The idea is to apply these operations itera- tively to simplify the linear system to a point where one can easily write down the solution set. It is convenient to apply elementary operations on the augmented matrix [A b] repre- senting the linear system. In this case, we call the operationselementary row operations, and the process of simplifying the linear system using these operations is calledrow reduc- tion. The goal with row reducing is to transform the original linear system into one having atriangular structureand then performback substitutionto solve the system. This is best explained via an example. Example 1.5.Use back substitution on the augmented matrix??1 0-2-40 1-1 0
0 0 1 1??
to solve the associated linear system. Solution.Notice that the augmented matrix has a triangular structure. Thethird row corresponds to the equationx3= 1. The second row corresponds to the equation x2-x3= 0
and thereforex2=x3= 1. The first row corresponds to the equation x1-2x3=-4
and therefore x1=-4 + 2x3=-4 + 2 =-2.
Therefore, the solution is (-2,1,1).
5Systems of Linear Equations
Example 1.6.Solve the linear system using elementary row operations. -3x1+ 2x2+ 4x3= 12 x1-2x3=-4
2x1-3x2+ 4x3=-3
Solution.Our goal is to perform elementary row operations to obtain a triangular structure and then use back substitution to solve. The augmented matrix is ?-3 2 4 121 0-2-4
2-3 4-3??
Interchange Row 1 (R1) and Row 2 (R2):
?-3 2 4 121 0-2-4
2-3 4-3??
R1↔R2----→??
1 0-2-4
-3 2 4 122-3 4-3??
As you will see, this first operation will simplify the next step. Add 3R1toR2: ?1 0-2-4 -3 2 4 122-3 4-3??
3R1+R2----→??
1 0-2-4
0 2-2 0
2-3 4-3??
Add-2R1toR3:
?1 0-2-40 2-2 0
2-3 4-3??
-2R1+R3-----→??1 0-2-4
0 2-2 0
0-3 8 5??
MultiplyR2by1
2:??1 0-2-4
0 2-2 0
0-3 8 5??
12R2--→??
1 0-2-4
0 1-1 0
0-3 8 5??
Add 3R2toR3:??1 0-2-4
0 1-1 0
0-3 8 5??
3R2+R3----→??
1 0-2-4
0 1-1 0
0 0 5 5??
MultiplyR3by1
5:??1 0-2-4
0 1-1 0
0 0 5 5??
15R3--→??
1 0-2-4
0 1-1 0
0 0 1 1??
We can continue row reducing but the row reduced augmented matrix is in triangular form. So now use back substitution to solve. The linear system associatedto the row reduced 6Lecture 1
augmented matrix is x1-2x3=-4
x2-x3= 0
x 3= 1 The last equation gives thatx3= 1. From the second equation we obtain thatx2-x3= 0, and thusx2= 1. The first equation then gives thatx1=-4+2(1) =-2. Thus, the solution to the original system is (-2,1,1). You should verify that (-2,1,1) is a solution to the original system. The original augmented matrix of the previous example is M=?? -3 2 4 121 0-2-4
2-3 4-3??
→-3x1+ 2x2+ 4x3= 12 x1-2x3=-4
2x1-3x2+ 4x3=-3.
After row reducing we obtained the row reduced matrix N=??1 0-2-4
0 1-1 0
0 0 1 1??
→x1-2x3=-4 x2-x3= 0
x 3= 1. Although the two augmented matricesMandNare clearly distinct, it is a fact that they have the same solution set.quotesdbs_dbs17.pdfusesText_23[PDF] mathcounts 2018 2019
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