Quadratic Forms. Change of Variable. Definition

Similar documents
Identifying second degree equations

SECTION 2.2. Distance and Midpoint Formulas; Circles

Ax 2 Cy 2 Dx Ey F 0. Here we show that the general second-degree equation. Ax 2 Bxy Cy 2 Dx Ey F 0. y X sin Y cos P(X, Y) X

Chapter 6. Orthogonality

ax 2 by 2 cxy dx ey f 0 The Distance Formula The distance d between two points (x 1, y 1 ) and (x 2, y 2 ) is given by d (x 2 x 1 )

The Distance Formula and the Circle

Graphing Quadratic Equations

Linear algebra and the geometry of quadratic equations. Similarity transformations and orthogonal matrices

1. a. standard form of a parabola with. 2 b 1 2 horizontal axis of symmetry 2. x 2 y 2 r 2 o. standard form of an ellipse centered

Notes on Orthogonal and Symmetric Matrices MENU, Winter 2013

2.1 Three Dimensional Curves and Surfaces

Affine Transformations

Similarity and Diagonalization. Similar Matrices

5.2 Inverse Functions

LINEAR FUNCTIONS OF 2 VARIABLES

Systems of Linear Equations: Solving by Substitution

MAT188H1S Lec0101 Burbulla

D.2. The Cartesian Plane. The Cartesian Plane The Distance and Midpoint Formulas Equations of Circles. D10 APPENDIX D Precalculus Review

INVESTIGATIONS AND FUNCTIONS Example 1

Section 11.4: Equations of Lines and Planes

LESSON EIII.E EXPONENTS AND LOGARITHMS

2.6. The Circle. Introduction. Prerequisites. Learning Outcomes

x = + x 2 + x

Exponential and Logarithmic Functions

DISTANCE, CIRCLES, AND QUADRATIC EQUATIONS

THE PARABOLA section

Zero and Negative Exponents and Scientific Notation. a a n a m n. Now, suppose that we allow m to equal n. We then have. a am m a 0 (1) a m

Graphing Linear Equations

Rotation of Axes 1. Rotation of Axes. At the beginning of Chapter 5 we stated that all equations of the form

2.6. The Circle. Introduction. Prerequisites. Learning Outcomes

[1] Diagonal factorization

Downloaded from equations. 2.4 The reciprocal function x 1 x

Solving Quadratic Equations by Graphing. Consider an equation of the form. y ax 2 bx c a 0. In an equation of the form

Higher. Polynomials and Quadratics 64

Lecture 1 Introduction Rectangular Coordinate Systems Vectors Lecture 2 Length, Dot Product, Cross Product Length...

SAMPLE. Polynomial functions

Inner Product Spaces and Orthogonality

Slope-Intercept Form and Point-Slope Form

Introduction to Matrices for Engineers

Example 1: Model A Model B Total Available. Gizmos. Dodads. System:

3. Solve the equation containing only one variable for that variable.

1.5 SOLUTION SETS OF LINEAR SYSTEMS

Review Jeopardy. Blue vs. Orange. Review Jeopardy

Inner Product Spaces

Similar matrices and Jordan form

α = u v. In other words, Orthogonal Projection

Plane Stress Transformations

3. Let A and B be two n n orthogonal matrices. Then prove that AB and BA are both orthogonal matrices. Prove a similar result for unitary matrices.

Integrating algebraic fractions

FACTORING QUADRATICS through 8.1.4

Warm-Up y. What type of triangle is formed by the points A(4,2), B(6, 1), and C( 1, 3)? A. right B. equilateral C. isosceles D.

COMPLEX STRESS TUTORIAL 3 COMPLEX STRESS AND STRAIN

Algebra 1 Course Title

Linear Equations in Linear Algebra

Addition and Subtraction of Vectors

Five 5. Rational Expressions and Equations C H A P T E R

C3: Functions. Learning objectives

Linear Algebra Review. Vectors

2.3. Finding polynomial functions. An Introduction:

by the matrix A results in a vector which is a reflection of the given

To Be or Not To Be a Linear Equation: That Is the Question

SECTION 7-4 Algebraic Vectors

Section V.2: Magnitudes, Directions, and Components of Vectors

Section 5.0A Factoring Part 1

Lectures notes on orthogonal matrices (with exercises) Linear Algebra II - Spring 2004 by D. Klain

Core Maths C2. Revision Notes

REVIEW OF CONIC SECTIONS

December 4, 2013 MATH 171 BASIC LINEAR ALGEBRA B. KITCHENS

CHAPTER 10 SYSTEMS, MATRICES, AND DETERMINANTS

Solving Absolute Value Equations and Inequalities Graphically

Orthogonal Diagonalization of Symmetric Matrices

The Characteristic Polynomial

MATH REVIEW SHEETS BEGINNING ALGEBRA MATH 60

Chapter 6 Quadratic Functions

Polynomial and Synthetic Division. Long Division of Polynomials. Example 1. 6x 2 7x 2 x 2) 19x 2 16x 4 6x3 12x 2 7x 2 16x 7x 2 14x. 2x 4.

Solving Systems of Equations

Recall the basic property of the transpose (for any A): v A t Aw = v w, v, w R n.

Linear Algebra and TI 89

Section 7.2 Linear Programming: The Graphical Method

Thnkwell s Homeschool Precalculus Course Lesson Plan: 36 weeks

Lines and Planes 1. x(t) = at + b y(t) = ct + d

Complex Numbers. w = f(z) z. Examples

MATH APPLIED MATRIX THEORY

STRAND: ALGEBRA Unit 3 Solving Equations

Chapter 4. Polynomial and Rational Functions. 4.1 Polynomial Functions and Their Graphs

Precalculus REVERSE CORRELATION. Content Expectations for. Precalculus. Michigan CONTENT EXPECTATIONS FOR PRECALCULUS CHAPTER/LESSON TITLES

ACT Math Vocabulary. Altitude The height of a triangle that makes a 90-degree angle with the base of the triangle. Altitude

Eigenvalues and Eigenvectors

More Equations and Inequalities

PROPERTIES OF ELLIPTIC CURVES AND THEIR USE IN FACTORING LARGE NUMBERS

Use order of operations to simplify. Show all steps in the space provided below each problem. INTEGER OPERATIONS

APPLICATIONS. are symmetric, but. are not.

Sample Problems. Practice Problems

PYTHAGOREAN TRIPLES KEITH CONRAD

Numerical Analysis Lecture Notes

y intercept Gradient Facts Lines that have the same gradient are PARALLEL

So, using the new notation, P X,Y (0,1) =.08 This is the value which the joint probability function for X and Y takes when X=0 and Y=1.

x y The matrix form, the vector form, and the augmented matrix form, respectively, for the system of equations are

MEMORANDUM. All students taking the CLC Math Placement Exam PLACEMENT INTO CALCULUS AND ANALYTIC GEOMETRY I, MTH 145:

Inner product. Definition of inner product

Transcription:

Quadratic Forms In the stud of linear algebra, we have been concerned with linear epressions, such as, + 9z, 7 + + etc. These are sometimes called linear forms. The most general linear form is a + a + + a k k. These are the simplest algebraic epressions. The net simplest are quadratic forms, such as +, + z, + 6z + z z. So a quadratic form in variables,,..., n is a sum of terms involving products of two variables, a ij i j. We can generate a quadratic form starting with an n n matri. For eample, let A =, 6 and for = (, ), form the product T A = [ ] [ 6 ][ = + + 6 = + 8 6, which is a quadratic form in and. ] = + 6 In general, if A is an n n matri and = (,,..., n ), then the matri product n n T A = a ij i j i= j= produces a quadratic form in,,..., n. Since =, there are man other matrices that produce the same quadratic form, for eample, for + 8 6 we can take A to be an one of 8,,,, 8 6 6 6 6 and millions more. Of those listed, the last one,, is special, because it is smmetric, 6 and we now know that smmetric matrices have nice properties. Furthermore, b averaging the a ij and a ji entries, we can convert an matri into a smmetric one that produces the same quadratic form. This is equivalent to replacing A b (A + AT ). For eample, ( + 6 ) = 8 =. 6 8 6 This means that we can alwas use smmetric matrices to generate quadratic forms. Definition Given a smmetric n n matri A, the quadratic form is the form generated b A. Q A () = T A = n i= j= n a ij i j Eample: For each quadratic form, epress it as A, where A is a smmetric matri: (a) 9 + 7 (b) + + 7 6 Solution: The diagonal entries are the coefficients of the squared terms, and the off-diagonal entries are half the coefficients of the cross terms: 9 / (a) A = (b) A = 7/ / 7 7/ Make sure ou collect collect terms before identifing coefficients. For eample, if we are given the quadratic form + + + 8 + +, we must first simplif it to 6 + 6 + 6, and then we see that the corresponding matri is 6 A = / / 6 /. / 6 Change of Variable If we make a linear substitution, or change of variable in a quadratic form, we get another quadratic form. For eample, given Q() = +, if we introduce new variables u and v and make the linear substitution then we get = u + v, = u v, ( u + v) ( u + v)(u v) + (u v) = (u uv + v ) ( u + 7uv 6v ) + (u uv + 9v ) = ( + + )u + ( 7 )uv + ( + 6 + 9)v = 7u uv + 9v

This particular substitution, chosen more or less at random, isn t particularl useful. However suppose we tr = u + v and = u v. Then + = (u + v) (u + v)(u v) + (u v) = (u + uv + v ) + (u v ) + (u uv + v ) = u + v This form is simpler, in that the cross term uv term is missing. A quadratic form whose cross terms are all zero is sometimes said to be a diagonal form. This is because it comes from a diagonal matri. Theorem Suppose D is a diagonal n n matri whose diagonal entries are λ, λ,..., λ n. Then the quadratic form generated b D is in diagonal form: λ Q D () = T λ D = [ n ].... λ n n = λ + λ + + λ n n. Another name for this is principal aes form. 7 So the following question comes to mind. Given a quadratic form, is there a substitution that will convert it to diagonal form, as in our last eample? If so, how do we find it? To answer these questions, we need to epress our linear substitutions in matri form. For eample, our first substitution, can be written as = u + v, = u v, u =, ][ v and our second substitution as [ u =, ] ][ v 8 Linear Substitution Definition A linear substitution of variables,,..., n, for,,..., n is an equation = P ( ) where P is an n n matri. If P is invertible, this is called a change of variable, and if P is orthogonal, it is an orthogonal change of variable. If we make the substitution ( ) in the quadratic form T A, we get T A = (P) T A(P) = T (P T AP) So the effect of the change of variable is to replace A b P T AP. 9 Now if A is smmetric, it is orthogonall diagonalizable, so we can find an orthogonal matri P that diagonalizes A. Then we have P T AP = D, where D is a diagonal matri with the eigenvalues of A along its diagonal, and we have λ T A = T λ D = [ n ].... λ n n = λ + λ + + λ n n We can sum up the situation in the following theorem. Theorem (The Principal Aes Theorem) If A is a smmetric n n matri, and the matri P orthogonall diagonalizes A, then substituting the change of variable = P into the quadratic form T A produces a quadratic form T D in principal aes form: λ + λ + + λ n n. The coefficient λ j is the eigenvalue corresponding to the j-th column of P.

Eample: Recall the eample A from lecture : A =. This is a smmetric matri, and gives the quadratic form T A = + Recall that A has eigenvalues and, and we found an orthogonal eigenbasis B = { (,, ), (,, ), (,, ) }. These vectors have norms,, and 6, respectivel, so an orthogonal matri that diagonalizes A is P = 6 6 6 Eercise: Put D =. Verif that P T AP = D. So the substitution = P gives the principal aes form T A = T D = +. For another eample, let Q = + 7. The smmetric matri that produces this form is 6 A = 6 7 The eigenvalues of A are and, with corresponding eigenvectors (, ) and (, ). (Verif this!) Since A is smmetric, these are orthogonal eigenvectors, as epected. An orthonormal eigenbasis is then So we set b = [ ], b = [ ]. P = =. Then we have P T AP = P AP = = D, and the change of variable = P gives the principal aes form Q = T A = T D =. Now the change of variables given b = P is = =, + or = ( ) and = ( + ). Eercise: Verif directl that making this substitution converts + 7 into. 7 Applications There are man uses for quadratic forms, and these can usuall be simplified b reduction to principal aes form. For eample, consider the following question. For n = or n =, what is the geometric interpretation (=graph) of the equation for a constant k? T A = k For geometric problems, it is convenient to change our notation slightl. For n =, we let = (, ), and for n = we let = (,, z). And when we make a change of variable, we will use = (, ), etc. So for n =, equation ( ) takes the form a + b + c = k. The curve (if an) represented b ( ) is called a central conic. ( ) 6 8 The reason we assume k in ( ) is that if k =, we get a degenerate case that is of little geometric interest. If b =, that is if the quadratic form in principal aes form, then ( ) is in standard position, and, ecept for degenerate cases, it can be classified as one of a small number of eamples. Since we assume k, we can after multipling b k, assume we have the form a + c = ( ) If both a < and b <, then equation ( ) is actuall impossible (for real numbers and ), so there is no curve at all.

Avoiding this case, we see that we can choose α = a and β = b in such a wa that we have one of the following possibilities: α + β =, α β =, β α = The first of these represents an ellipse and the others are hperbolas. For the ellipse, there are two cases, depending on which of α and β is larger. (And if α = β, we have a circle of radius α.) 9 Generall, orthogonal change of variables converts the equation T A = into the form λ + λ = where λ and λ are the eigenvalues of A. Then the curve is an ellipse if both λ > and λ >. The curve is a hperbola if both λ and λ have opposite signs. There is no graph if both λ < and λ <. The ellipse or hperbola is in standard position relative to a set of aes pointing along the eigenvectors of A. Finall, note that the parameters α and β in the standard forms are given b α = λ, β = λ. A general central conic is the result of rotating one in standard form through some angle θ. This causes the appearance of a cross term, b. Removing the cross term b an orthogonal substitution amounts to appling the reverse rotation, to bring the conic back to standard form. An alternative interpretation is that the diagonalizing change of variable gives a rotated coordinate sstem, and the conic is in standard position relative to that sstem. With the change of variables = P, where = (, ) we can think of the variables and as coordinates with respect to coordinate aes pointing along the eigenvectors that make up the columns of P. To illustrate this, let s look at our last eample again, where we considered the quadratic form Q = + 7, or, in terms of and, Q = + 7. What is the graph of the equation + 7 =? Now after the change of variables, the equation of the conic has the form = To recognize this in our list of eamples, we rewrite it as =. Then we put α = and β =, and we have the equation α β =. So in the, -plane, this represents a hperbola in standard position. = (, )

Recall that eigenvectors of A were u = (, ) and u = (, ). Plotting these in the, -plane tells us the directions of the, -aes: u u So we transfer the previous, -graph to these rotated aes: 6 And finall, all we need to do is erase all the scaffolding : + 7 = For another eample, consider + = 9. The matri A is A = The eigenvalues are easil found to be λ = and λ =, with corresponding eigenvectors u = (, ) and u = (, ). Again, these are orthogonal, as epected. Since both eigenvalues are positive, we know that the graph will be an ellipse. The principal aes form of the equation is then + = 9 So we will have α = and β =. or 9 + =, 7 In the, -plane, the graph is 8 The and aes point along u and u. So the rotated graph looks like + 9 = 9

And here it is without the primed aes: + = 9