Theory of Higher-Order Linear Differential Equations

Similar documents
Basic Theory of Linear Differential Equations

Atoms An atom is a term with coefficient 1 obtained by taking the real and imaginary parts of x j e ax+icx, j = 0, 1, 2,...,

Lecture Notes for Math 251: ODE and PDE. Lecture 12: 3.3 Complex Roots of the Characteristic Equation

Solution of Constant Coefficients ODE

Ordinary Differential Equations

Examples: Solving nth Order Equations

MATH 312 Section 4.5: Undetermined Coefficients

17.2 Nonhomogeneous Linear Equations. 27 September 2007

Chapter 4. Higher-Order Differential Equations

Chapter 3. Reading assignment: In this chapter we will cover Sections dx 1 + a 0(x)y(x) = g(x). (1)

Homework #6 Solutions

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation. is called the reduced equation of (N).

Essential Ordinary Differential Equations

Math 240 Calculus III

Math 3313: Differential Equations Second-order ordinary differential equations

Math 4B Notes. Written by Victoria Kala SH 6432u Office Hours: T 12:45 1:45pm Last updated 7/24/2016

The Corrected Trial Solution in the Method of Undetermined Coefficients

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation. is called the reduced equation of (N).

A Brief Review of Elementary Ordinary Differential Equations

3.4.1 Distinct Real Roots

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation

Ordinary Differential Equations

Math 2142 Homework 5 Part 1 Solutions

dx n a 1(x) dy

Alan H. SteinUniversity of Connecticut. Linear Differential Equations With Constant Coefficients

Chapter 4: Higher-Order Differential Equations Part 1

Math 201 Lecture 08 Undetermined Coefficients

Find the Fourier series of the odd-periodic extension of the function f (x) = 1 for x ( 1, 0). Solution: The Fourier series is.

Differential Equations Revision Notes

Review for Exam 2. Review for Exam 2.

Constant coefficients systems

ODE classification. February 7, Nasser M. Abbasi. compiled on Wednesday February 07, 2018 at 11:18 PM

LINEAR DIFFERENTIAL EQUATIONS. Theorem 1 (Existence and Uniqueness). [1, NSS, Section 6.1, Theorem 1] 1 Suppose. y(x)

Section 3.4. Second Order Nonhomogeneous. The corresponding homogeneous equation. is called the reduced equation of (N).

6. Linear Differential Equations of the Second Order

LECTURE 14: REGULAR SINGULAR POINTS, EULER EQUATIONS

Math 54. Selected Solutions for Week 10

4. Higher Order Linear DEs

Chapter 4: Higher Order Linear Equations

Consider an ideal pendulum as shown below. l θ is the angular acceleration θ is the angular velocity

Section 1.4: Second-Order and Higher-Order Equations. Consider a second-order, linear, homogeneous equation with constant coefficients

2. Second-order Linear Ordinary Differential Equations

Polytechnic Institute of NYU MA 2132 Final Practice Answers Fall 2012

B Ordinary Differential Equations Review

MATH 312 Section 4.3: Homogeneous Linear Equations with Constant Coefficients

1 Systems of Differential Equations

Higher-order ordinary differential equations

A: Brief Review of Ordinary Differential Equations

Linear differential equations with constant coefficients Method of undetermined coefficients

4.2 Homogeneous Linear Equations

3. Identify and find the general solution of each of the following first order differential equations.

McGill University Math 325A: Differential Equations LECTURE 12: SOLUTIONS FOR EQUATIONS WITH CONSTANTS COEFFICIENTS (II)

Lecture 9. Scott Pauls 1 4/16/07. Dartmouth College. Math 23, Spring Scott Pauls. Last class. Today s material. Group work.

6 - Theory of Higher-Order Linear Differential Equations

Math 2Z03 - Tutorial # 4. Oct. 5th, 6th, 7th, 2015

APPLIED MATHEMATICS. Part 1: Ordinary Differential Equations. Wu-ting Tsai

A( x) B( x) C( x) y( x) 0, A( x) 0

First Order Differential Equations

Ma 221. The material below was covered during the lecture given last Wed. (1/29/14). Homogeneous Linear Equations with Constant Coefficients

2nd-Order Linear Equations

Differential Equations Class Notes

CHAPTER 5. Higher Order Linear ODE'S

SECOND ORDER ODE S. 1. A second order differential equation is an equation of the form. F (x, y, y, y ) = 0.

Solution to Homework 2

MATH 308 Differential Equations

Assignment # 7, Math 370, Fall 2018 SOLUTIONS: y = e x. y = e 3x + 4xe 3x. y = e x cosx.

Math 250B Final Exam Review Session Spring 2015 SOLUTIONS

Linear DifferentiaL Equation

2. Determine whether the following pair of functions are linearly dependent, or linearly independent:

ODEs Cathal Ormond 1

3. Identify and find the general solution of each of the following first order differential equations.

Homogeneous Linear ODEs of Second Order Notes for Math 331

LINEAR EQUATIONS OF HIGHER ORDER. EXAMPLES. General framework

MATHEMATICS FOR ENGINEERS & SCIENTISTS 23

Nonhomogeneous Linear Differential Equations with Constant Coefficients - (3.4) Method of Undetermined Coefficients

Ordinary Differential Equations (ODEs)

The Method of Undetermined Coefficients and the Shifting Rule. Math 5330, Spring 1996

2.3 Linear Equations 69

Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Undetermined Coefficients Page 1

Math 651 Introduction to Numerical Analysis I Fall SOLUTIONS: Homework Set 1

Lesson 3: Linear differential equations of the first order Solve each of the following differential equations by two methods.

PRELIMINARY THEORY LINEAR EQUATIONS

Ordinary Differential Equation Theory

MATH 251 Examination I February 23, 2017 FORM A. Name: Student Number: Section:

Georgia Tech PHYS 6124 Mathematical Methods of Physics I

VANDERBILT UNIVERSITY. MATH 2610 ORDINARY DIFFERENTIAL EQUATIONS Practice for test 1 solutions

2 Linear Differential Equations General Theory Linear Equations with Constant Coefficients Operator Methods...

Higher Order Linear Equations Lecture 7

Ordinary Differential Equations Lake Ritter, Kennesaw State University

IV Higher Order Linear ODEs

HW2 Solutions. MATH 20D Fall 2013 Prof: Sun Hui TA: Zezhou Zhang (David) October 14, Checklist: Section 2.6: 1, 3, 6, 8, 10, 15, [20, 22]

Introductory Differential Equations

Assignment # 8, Math 370, Fall 2018 SOLUTIONS:

Elementary Differential Equations, Section 2 Prof. Loftin: Practice Test Problems for Test Find the radius of convergence of the power series

24. x 2 y xy y sec(ln x); 1 e x y 1 cos(ln x), y 2 sin(ln x) 25. y y tan x 26. y 4y sec 2x 28.

1 Method for Ordinary Differential Equations

MA 266 Review Topics - Exam # 2 (updated)

Solutions for Math 225 Assignment #4 1

MATH 307: Problem Set #7

0.1 Problems to solve

Transcription:

Chapter 6 Theory of Higher-Order Linear Differential Equations 6.1 Basic Theory A linear differential equation of order n has the form a n (x)y (n) (x) + a n 1 (x)y (n 1) (x) + + a 0 (x)y(x) = b(x), (6.1.1) where a 0 (x),, a n (x) and b(x) depend only on x. constant coefficients: When a 0, a 1,, a n are all constants. variable coefficients: When some of a 0, a 1,, a n are not constants. homogeneous: When b(x) = 0. nonhomogeneous: When b(x) 0. standard form: Divide (6.1.1) by a n (x) to get y (n) (x) + p 1 (x)y (n 1) (x) + + p n (x)y(x) = g(x) Theorem 6.1 (Existence and Uniqueness). If p 1 (x),, p n (x) and g(x) are each continuous on (a, b) that contains x 0. Then for any initial values γ 0, γ 1,, γ n 1, there exists a unique solution y(x) on the whole interval (a, b) to the following IVP: y (n) (x) + p 1 (x)y (n 1) (x) + + p n (x)y(x) = g(x), (6.1.2) Ex. (ex1, p343) y(x 0 ) = γ 0, y(x 1 ) = γ 1,, y(x n 1 ) = γ n 1. (6.1.3) 35

36CHAPTER 6. THEORY OF HIGHER-ORDER LINEAR DIFFERENTIAL EQUATIONS Def 6.2. Let f 1,, f n be any n functions that are (n 1) times differentiable. The function W [f 1,, f n ] = f 1 f 2 f n f 1 f 2 f n. f (n 1) 1 f (n 1).. 2 f n (n 1) is called the Wronskian of f 1,, f n. (What is determinant?) Theorem 6.3 (Solutions for Homogeneous Case). Given n solutions y 1,, y n to y (n) (x) + p 1 (x)y (n 1) (x) + + p n (x)y(x) = 0 where p 1,, p n are continuous on (a, b). If for some points x 0 (a, b) there is W [y 1,, y n ](x 0 ) 0, then every solution of the above homogeneous equation on (a, b) can be expressed by y(x) = C 1 y 1 (x) + + C n y n (x). n functions f 1,, f n are linearly dependent on an interval I if one of them can be expressed as a linear combination of the others. Equivalently, if there exists constants c 1,, c n such that c 1 f 1 (x) + + c n f n (x) 0 for all x on I. Otherwise, they are linearly independent on I. Ex. (ex2, p346) Ex. (ex3, p346) For solutions y 1,, y n of the above homogeneous equation, the linear dependence can be checked by its Wronskian at on point. Theorem 6.4. If y 1,, y n are solutions to y (n) (x)+p 1 (x)y (n 1) (x)+ + p n (x)y(x) = 0 on (a, b) with p 1,, p n continuous on (a, b), then y 1,, y n are linearly dependent on (a, b) if and only if W [y 1,, y n ](x 0 ) = 0 for some x 0 on (a, b).

6.2. HOMOGENEOUS LINEAR EQUATIONS WITH CONSTANT COEFFICIENTS37 Theorem 6.5 (Solutions for Nonhomogeneous Case). If y p (x) is a particular solution to the nonhomogeneous equation y (n) (x) + p 1 (x)y (n 1) (x) + + p n (x)y(x) = g(x) (6.1.4) on (a, b) with p 1,, p n continuous on (a, b), and {y 1,, y n } is a fundamental solution set of the corresponding homogeneous equation y (n) (x) + p 1 (x)y (n 1) (x) + + p n (x)y(x) = 0 then the general solution of (6.1.4) is of the form Ex. (ex4, p349) y(x) = y p (x) + C 1 y 1 (x) + C 2 y 2 (x) + + C n y n (x). Homework 6.1 (p349-351): 1, 3, 5, 7, 9, 11, 13, 15, 17, 19, 21, 23 6.2 Homogeneous Linear Equations with Constant Coefficients The solutions to a homogeneous linear equation with constant coefficients a n y (n) + + a 1 y + a 0 y = 0 (6.2.1) depends on the roots of the characteristic equation P (r) := a n r n + + a 1 r + a 0 = 0 (6.2.2) Let D be the operator such that D(y) = y. Then P (D) = a n D n + +a 1 D+ a 0 is an operator. The homogeneous equation (6.2.1) becomes P (D)(y) = 0. If P (r) has distinct roots r 1,, r m where r i repeats d i times (d i = 1, 2,, d 1 + + d m = n), then P (D)(y) = (D r 1 ) d1 (D r m ) dm (y) = 0 Clearly, if y is a solution to (D r i ) d i (y) = 0 for some i, then y is a solution to P (D)(y) = 0. One can verify by induction that: A set of fundamental solutions to the differential equation (D r i ) d i (y) = 0 is {e r it, te r it,, t d i 1 e r it }. So P (D)(y) = 0 has the following solutions:

38CHAPTER 6. THEORY OF HIGHER-ORDER LINEAR DIFFERENTIAL EQUATIONS Theorem 6.6. A fundamental solution set {y 1,, y n } of the homogeneous constant coefficient equation a n y (n) + + a 1 y + a 0 y = 0 consists of e r it, te r it,, t d i 1 e r it where r i is a root repeated d i times (d i equation a n r n + + a 1 r + a 0 = 0. = 1, 2, ) in the characteristic Ex. (ex1, p353, distinct roots) Ex. (ex3, p356, repeated roots) If the characteristic equation P (r) = 0 has complex conjugated roots α + iβ and α iβ, each repeated d times, then the solution functions {e (α+iβ)t,, t d 1 e (α+iβ)t, e (α iβ)t,, t d 1 e (α iβ)t } can be replaced by real functions {e αt cos(βt),, t d 1 e αt cos(βt), e αt sin(βt),, t d 1 e αt sin(βt)}. Ex. (ex2, p354) Ex. (ex4, p356) Ex. (hw18, p356) Homework 6.2 (p356-358): 1, 2, 3, 9, 11, 14, 15, 17, 19, 21

6.3. UNDETERMINED COEFFICIENTS AND THE ANNIHILATOR METHOD39 6.3 Undetermined Coefficients and the Annihilator Method We have used undetermined coefficient method to solve the linear differential equation (ad 2 + bd + c)[y] = f(x), where f(x) is of the form Ct m e rt, Ct m e αt cos(βt), or Ct m e αt sin(βt), or a summand of such terms by superposition principle. The method of undetermined coefficients can be generalized to solve P (D)[y] = f(x) where f(x) is of the above forms. This can be justified by the annihilator method below. To solve P (D)[y] = f(x), suppose f(x) is a solution to Q(D)[f] = 0 for some polynomial Q(r) (so Q(r) is said to annihilate f), then In other words, Q(D)P (D)[y] = Q(D)[f](x) = 0. y is a solution to P (D)[y] = f(x) = y is a solution to Q(D)P (D)[y] = 0. The latter one is homogeneous and we know how to solve it. Thus we may choose y from a general solution of Q(D)P (D)[y] = 0, then apply the method of undetermined coefficients to get the coefficients. Lemma 6.7. The following rules are useful to determine annihilators of certain functions: 1. f(x) = e rx satisfies (D r)[f] = 0. (i.e. (D r) annihilates e rx ) 2. f(x) = x k e rx satisfies (D r) m [f] = 0 for k = 0, 1,, m 1. 3. f(x) = cos βx or sin βx satisfies (D 2 + β 2 )[f] = 0. 4. f(x) = x k e αx cos(βx) or x k e αx sin(βx) satisfies [(D α) 2 +β 2 ] m [f] = 0 for k = 0, 1,, m 1. 5. If Q i (D) is an annihilator of f i (x) for i = 1,, p, then the least common multipler lcm(q 1 (D),, Q p (D)) and the product Q 1 (D) Q p (D) are both annihilators of f 1 (x) + f 2 (x) + + f p (x). (proof) Ex. (ex1, p359) Find a differential operator that annihilates 6xe 4x + 5e x sin(2x).

40CHAPTER 6. THEORY OF HIGHER-ORDER LINEAR DIFFERENTIAL EQUATIONS Ex. (ex2, p360) Use both method of undetermined coefficient and method of annihilators to find a general solution to y y = xe x + sin x. Ex. (ex3, p361) Use the annihilator method to find a general solution to y 3y + 4y = xe 2x. Theorem 6.8 (Method of Undetermined Coefficients). Let L = P (D) be a constant coefficient polynomial differential operator. 1. To find a particular solution to L[y] = Cx m e rx, use the form y p (x) = x s [A m x m + + A 1 x + A 0 ]e rx where s {0, 1, 2, } is the multiplicity of r in the associated characteristic equation P (z) = 0. 2. To find a particular solution to L[y] = Cx m e αx cos(βx) or L[y] = Cx m e αx sin(βx), use the form y p (x) = x s [A m x m + +A 1 x+a 0 ]e αx cos(βx)+x s [B m x m + +B 1 x+b 0 ]e αx sin(βx) where s {0, 1, 2, } is the multiplicity of α + iβ in the associated characteristic equation P (z) = 0. Homework 6.3 (p362-363): 1, 3, 5, 7, 9, 11, 13, 15, 23, 25, 27, 31, 33