Application 5.4 Defective Eigenvalues and Generalized Eigenvectors

Similar documents
Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations

After the completion of this section the student. Theory of Linear Systems of ODEs. Autonomous Systems. Review Questions and Exercises

System of Linear Differential Equations

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

Exercises: Similarity Transformation

Chapter Three Systems of Linear Differential Equations

10. State Space Methods

Solutions for homework 12

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

Math 1. Two-Hours Exam December 10, 2017.

Echocardiography Project and Finite Fourier Series

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Two Coupled Oscillators / Normal Modes

Y 0.4Y 0.45Y Y to a proper ARMA specification.

Announcements: Warm-up Exercise:

Mon Apr 9 EP 7.6 Convolutions and Laplace transforms. Announcements: Warm-up Exercise:

Let ( α, β be the eigenvector associated with the eigenvalue λ i

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Chapter 6. Systems of First Order Linear Differential Equations

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

KEY. Math 334 Midterm III Winter 2008 section 002 Instructor: Scott Glasgow

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.

non -negative cone Population dynamics motivates the study of linear models whose coefficient matrices are non-negative or positive.

Some Basic Information about M-S-D Systems

Ordinary Differential Equations

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

MATH 2050 Assignment 9 Winter Do not need to hand in. 1. Find the determinant by reducing to triangular form for the following matrices.

Chapter 3 Boundary Value Problem

Math 315: Linear Algebra Solutions to Assignment 6

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

Section 4.4 Logarithmic Properties

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

The equation to any straight line can be expressed in the form:

KEY. Math 334 Midterm III Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

The Eigenvalue Problems - 8.8

Section 4.4 Logarithmic Properties

Math 334 Fall 2011 Homework 11 Solutions

Linear Dynamic Models

Stability and Bifurcation in a Neural Network Model with Two Delays

Eigenvalues and Eigenvectors. Eigenvalues and Eigenvectors. Initialization

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

Let us start with a two dimensional case. We consider a vector ( x,

Undetermined coefficients for local fractional differential equations

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

GMM - Generalized Method of Moments

Product Operators. Fundamentals of MR Alec Ricciuti 3 March 2011

SOLUTIONS TO ECE 3084

Math Week 15: Section 7.4, mass-spring systems. These are notes for Monday. There will also be course review notes for Tuesday, posted later.

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

Sections 2.2 & 2.3 Limit of a Function and Limit Laws

t + t sin t t cos t sin t. t cos t sin t dt t 2 = exp 2 log t log(t cos t sin t) = Multiplying by this factor and then integrating, we conclude that

14 Autoregressive Moving Average Models

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis

Short Introduction to Fractional Calculus

Distance Between Two Ellipses in 3D

Spring Ammar Abu-Hudrouss Islamic University Gaza

ENGI 9420 Engineering Analysis Assignment 2 Solutions

KINEMATICS IN ONE DIMENSION

EE363 homework 1 solutions

Kinematics and kinematic functions

1 Differential Equation Investigations using Customizable

THE MATRIX-TREE THEOREM

BEng (Hons) Telecommunications. Examinations for / Semester 2

Chapter 8 The Complete Response of RL and RC Circuits

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)

HOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures.

Outline of Topics. Analysis of ODE models with MATLAB. What will we learn from this lecture. Aim of analysis: Why such analysis matters?

Section 7.4 Modeling Changing Amplitude and Midline

Homework Solution Set # 3. Thursday, September 22, Textbook: Claude Cohen Tannoudji, Bernard Diu and Franck Lalo, Second Volume Complement G X

Analyze patterns and relationships. 3. Generate two numerical patterns using AC

Modal identification of structures from roving input data by means of maximum likelihood estimation of the state space model

Chapter 2. First Order Scalar Equations

Chapter 3 Common Families of Distributions

Lecture 20: Riccati Equations and Least Squares Feedback Control

2. Nonlinear Conservation Law Equations

6.003 Homework #8 Solutions

On-line Adaptive Optimal Timing Control of Switched Systems

Math Final Exam Solutions

Differential Equations

Chapter 3 Kinematics in Two Dimensions

Tests of Nonlinear Resonse Theory. We compare the results of direct NEMD simulation against Kawasaki and TTCF for 2- particle colour conductivity.

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

1 Solutions to selected problems

Linear Response Theory: The connection between QFT and experiments

Lie Derivatives operator vector field flow push back Lie derivative of

Wednesday, November 7 Handout: Heteroskedasticity

Convergence of the Neumann series in higher norms

For example, the comb filter generated from. ( ) has a transfer function. e ) has L notches at ω = (2k+1)π/L and L peaks at ω = 2π k/l,

Second Order Linear Differential Equations

Practice Problems - Week #4 Higher-Order DEs, Applications Solutions

THE WAVE EQUATION. part hand-in for week 9 b. Any dilation v(x, t) = u(λx, λt) of u(x, t) is also a solution (where λ is constant).

Selective peracetic acid determination in the presence of hydrogen peroxide using the molecular absorption properties of catalase

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

Mathcad Lecture #7 In-class Worksheet "Smart" Solve Block Techniques Handout

Γ(h)=0 h 0. Γ(h)=cov(X 0,X 0-h ). A stationary process is called white noise if its autocovariance

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Homework 10 (Stats 620, Winter 2017) Due Tuesday April 18, in class Questions are derived from problems in Stochastic Processes by S. Ross.

Transcription:

Applicaion 5.4 Defecive Eigenvalues and Generalized Eigenvecors The goal of his applicaion is he soluion of he linear sysems like where he coefficien marix is he exoic 5-by-5 marix x = Ax, (1) 9 11 21 63 252 70 69 141 42684 A = 575 575 1149 3451 13801 (2) 3891 3891 7782 23345 93365 1024 1024 2048 6144 24572 ha is generaed by he MATLAB command gallery(5). Wha is so exoic abou his paricular marix? Well, ener i in your calculaor or compuer sysem of choice, and hen use appropriae commands o show ha: Firs, he characerisic equaion of A reduces o single eigenvalue λ = 0 of mulipliciy 5. 5 λ = 0, so A has he Second, here is only a single eigenvecor associaed wih his eigenvalue, which hus has defec 4. To seek a chain of generalized eigenvecors, show ha A 4 0 bu 5 5 zero marix). Hence any nonzero 5-vecor u 1 saisfies he equaion A 5 = 0 (he ( A λ I) u = A u = 0. 5 5 Calculae he vecors u 2 = Au 1, u 3 = Au 2, u 4 = Au 3, and u 5 = Au 4 in urn. You should find ha u 5 is nonzero, and is herefore (o wihin a consan muliple) he unique eigenvecor v of he marix A. Bu can his eigenvecor v you find possibly be independen of your original choice of he saring vecor u 1 0? Invesigae his quesion by repeaing he process wih several differen choices of u 1. Finally, having found a lengh 5 chain {u 5, u 4, u 3 } of generalized eigenvecors based on he (ordinary) eigenvecor u 5 associaed wih he single eigenvalue λ = 0 of he marix A, wrie five linearly independen soluions of he 5-dimensional homogeneous linear sysem x = Ax. Applicaion 5.4 151

In he secions ha follow we illusrae appropriae Maple, Mahemaica, and MATLAB echniques o analyze he 4 4 marix 35 12 4 30 22 8 3 19 A = (3) 10 3 0 9 27 9 3 23 of Problem 31 in Secion 5.4 of he ex. You can use any of he oher problems here (especially Problems 23 30 and 32) o pracice hese echniques. Using Maple Firs we ener he marix in (3): wih(linalg): A := marix(4,4, [ 35, -12, 4, 30, 22, -8, 3, 19, -10, 3, 0, -9, -27, 9, -3, -23 ] ): Then we explore is characerisic polynomial, eigenvalues, and eigenvecors: charpoly(a,lambda); 4 3 2 λ λ λ λ 4 + 6 4 + 1 (ha is, 4 ( λ 1) ) eigenvals(a); 1,1,1,1 eigenvecs(a); [1, 4, {[0 1 3 0], [ 1 0 ] } ] Thus Maple finds only he wo independen eigenvecors w1 := marix(4,1, [ 0, 1, 3, 0]): w2 := marix(4,1, [-1, 0, 1, 1]): associaed wih he mulipliciy 4 eigenvalue λ = 1, which herefore has defec 2. To explore he siuaion we se up he 4 4 ideniy marix and he marix B = A λ I: 152 Chaper 5

Id := diag(1,1,1,1): L = 1: B := evalm( A - L*Id): When we calculae B 2 and B 3, B2 := evalm(b &* B); B3 := evalm(b2 &* B); 2 we find ha B 0 bu λ = 1. Choosing B 3 = 0, so here should be a lengh 3 chain associaed wih u1 := marix(4,1,[1,0,0,0]); we calculae he furher generalized eigenvecors u2 := evalm( B &* u1); 34 22 u2 : = 10 27 and u3 := evalm( B &* u2); 42 7 u3 : = 21 42 Thus we have found he lengh 3 chain {u 3 } based on he (ordinary) eigenvecor u 3. (To reconcile his resul wih Maple's eigenvecs calculaion, you can check ha u3 + 42 w2 = 7w 1.) Consequenly four linearly independen soluions of he sysem x = Ax are given by x () = w e, x ( ) = u e, 2 3 x ( ) = ( u + u e ), 3 2 3 x ( ) = ( u + u + u ) e. 1 2 4 1 2 2 3 Applicaion 5.4 153

Using Mahemaica Firs we ener he marix in (3): A = { { 35, -12, 4, 30 }, { 22, -8, 3, 19 }, {-10, 3, 0, -9 }, {-27, 9, -3, -23 } }; Then we explore is characerisic polynomial, eigenvalues, and eigenvecors: CharacerisicPolynomial[A, r] 2 3 4 1-4 r + 6 r - 4 r + r (ha is, 4 ( r 1) ) Eigenvalues[A] {1, 1, 1, 1} Eigenvecors[A] {{-3,-1,0,3}, {0,1,3,0}, {0,0,0,0}, {0,0,0,0}} Thus Mahemaica finds only he wo independen (nonzero) eigenvecors w1 = {-3,-1, 0, 3}; w2 = { 0, 1, 3, 0}; associaed wih he mulipliciy 4 eigenvalue λ = 1, which herefore has defec 2. To explore he siuaion we se up he 4 4 ideniy marix and he marix B = A λ I: Id = DiagonalMarix[1,1,1,1]; L = 1; B = A - L*Id; When we calculae B 2 and B 3, B2 = B.B B3 = B2.B 2 we find ha B 0 bu λ = 1. Choosing B 3 = 0, so here should be a lengh 3 chain associaed wih u1 = {{1},{0},{0},{0}} 154 Chaper 5

we calculae u2 = B.u1 {{34}, {22}, {-10}, {-27}} u3 = B.u2 {{42}, {7}, {-21}, {-42}} Thus we have found he lengh 3 chain {u 3 } based on he (ordinary) eigenvecor u 3. (To reconcile his resul wih Mahemaica's Eigenvecors calculaion, you can check ha u3 + 14 w1 = 7w 2.) Consequenly four linearly independen soluions of he sysem x = Ax are given by x () = w e, x ( ) = u e, 2 3 x ( ) = ( u + u e ), 3 2 3 x ( ) = ( u + u + u ) e. 1 2 4 1 2 2 3 Using MATLAB Firs we ener he marix in (3): A = [ 35-12 4 30 22-8 3 19-10 3 0-9 -27 9-3 -23 ]; Then we proceed o explore is characerisic polynomial, eigenvalues, and eigenvecors. poly(a) ans = 1.0000-4.0000 6.0000-4.0000 1.0000 These are he coefficiens of he characerisic polynomial, which hence is Then 4 ( λ 1). [V, D] = eigensys(a) V = [ 1, 0] [ 0, 1] [-1, 3] [-1, 0] Applicaion 5.4 155

D = Thus MATLAB finds only he wo independen eigenvecors w1 = [1 0-1 -1]'; w2 = [0 1 3 0]'; associaed wih he single mulipliciy 4 eigenvalue λ = 1, which herefore has defec 2. To explore he siuaion we se up he 4 4 ideniy marix and he marix B = A λ I: Id = eye(4); B = A - L*Id; When we calculae B 2 and B 3, B2 = B*B B3 = B2*B 2 3 We find ha B 0 bu B = 0, so here should be a lengh 3 chain associaed wih he eigenvalue λ = 1. Choosing he firs generalized eigenvecor u1 = [1 0 0 0]'; we calculae he furher generalized eigenvecors and u2 = B*u1 u2 = 34 22-10 -27 u3 = B*u2 u3 = 42 7-21 -42 156 Chaper 5

Thus we have found he lengh 3 chain {u 3 } based on he (ordinary) eigenvecor u 3. (To reconcile his resul wih MATLAB's eigensys calculaion, you can check ha u3 42 w1 = 7w 2.) Consequenly four linearly independen soluions of he sysem x = Ax are given by x () = w e, x ( ) = u e, 2 3 x ( ) = ( u + u e ), 3 2 3 x ( ) = ( u + u + u ) e. 1 2 4 1 2 2 3 Applicaion 5.4 157