MATH 312 Section 8.3: Non-homogeneous Systems

Similar documents
MATH 312 Section 4.5: Undetermined Coefficients

MATH 312 Section 4.3: Homogeneous Linear Equations with Constant Coefficients

MATH 312 Section 2.4: Exact Differential Equations

MATH 312 Section 1.2: Initial Value Problems

MATH 312 Section 6.2: Series Solutions about Singular Points

MATH 312 Section 7.1: Definition of a Laplace Transform

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

Chapter 3: Theory Review: Solutions Math 308 F Spring 2015

MATH 312 Section 3.1: Linear Models

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

MATH 2250 Final Exam Solutions

Math 240 Calculus III

Math Ordinary Differential Equations

Math 2142 Homework 5 Part 1 Solutions

= AΦ, Φ(0) = I, = k! tk A k = I + ta t2 A t3 A t4 A 4 +, (3) e ta 1

MAT 1332: CALCULUS FOR LIFE SCIENCES. Contents. 1. Review: Linear Algebra II Vectors and matrices Definition. 1.2.

2.2 Separable Equations

Math 115 HW #10 Solutions

Solutions to Math 53 Math 53 Practice Final

Homogeneous Linear Systems of Differential Equations with Constant Coefficients

Lecture Notes for Math 251: ODE and PDE. Lecture 30: 10.1 Two-Point Boundary Value Problems

Elementary Matrices. MATH 322, Linear Algebra I. J. Robert Buchanan. Spring Department of Mathematics

Math 322. Spring 2015 Review Problems for Midterm 2

June 2011 PURDUE UNIVERSITY Study Guide for the Credit Exam in (MA 262) Linear Algebra and Differential Equations

Math 60. Rumbos Spring Solutions to Assignment #17

Math Boot Camp Functions and Algebra

MATH 23 Exam 2 Review Solutions

Applied Math Qualifying Exam 11 October Instructions: Work 2 out of 3 problems in each of the 3 parts for a total of 6 problems.

Math 1B Final Exam, Solution. Prof. Mina Aganagic Lecture 2, Spring (6 points) Use substitution and integration by parts to find:

First Order ODEs, Part I

1. The accumulated net change function or area-so-far function

Inverse Kinematics. Mike Bailey.

Stokes and the Surveyor s Shoelaces

Lecture 8: Ordinary Differential Equations

MATH 215/255 Solutions to Additional Practice Problems April dy dt

Math 266: Phase Plane Portrait

Inverse Kinematics. Mike Bailey. Oregon State University. Inverse Kinematics

Test #2 Math 2250 Summer 2003

Math 2a Prac Lectures on Differential Equations

Copyright c 2008 Kevin Long

Review For the Final: Problem 1 Find the general solutions of the following DEs. a) x 2 y xy y 2 = 0 solution: = 0 : homogeneous equation.

4. Higher Order Linear DEs

Differential Equations 2280 Sample Midterm Exam 3 with Solutions Exam Date: 24 April 2015 at 12:50pm

Calculus and Differential Equations II

MATH 320 INHOMOGENEOUS LINEAR SYSTEMS OF DIFFERENTIAL EQUATIONS

Math 127C, Spring 2006 Final Exam Solutions. x 2 ), g(y 1, y 2 ) = ( y 1 y 2, y1 2 + y2) 2. (g f) (0) = g (f(0))f (0).

4.5 Linearization Calculus 4.5 LINEARIZATION. Notecards from Section 4.5: Linearization; Differentials. Linearization

Math 250B Final Exam Review Session Spring 2015 SOLUTIONS

Systems of differential equations Handout

Spring 2015 Sample Final Exam

Old Math 330 Exams. David M. McClendon. Department of Mathematics Ferris State University

Math 2Z03 - Tutorial # 6. Oct. 26th, 27th, 28th, 2015

MA 262, Spring 2018, Midterm 1 Version 01 (Green)

AP Calculus AB 2015 Free-Response Questions

Solutions to Math 53 First Exam April 20, 2010

Prelim 1 Solutions V2 Math 1120

Section 5.5 More Integration Formula (The Substitution Method) 2 Lectures. Dr. Abdulla Eid. College of Science. MATHS 101: Calculus I

DIFFERENTIAL EQUATIONS

17.2 Nonhomogeneous Linear Equations. 27 September 2007

MATH 2203 Exam 3 Version 2 Solutions Instructions mathematical correctness clarity of presentation complete sentences

Finite difference method for solving Advection-Diffusion Problem in 1D

Math 212-Lecture 8. The chain rule with one independent variable

STUDENT NAME: STUDENT SIGNATURE: STUDENT ID NUMBER: SECTION NUMBER RECITATION INSTRUCTOR:

( ) be the particular solution to the differential equation passing through the point (2, 1). Write an

A Concise Introduction to Ordinary Differential Equations. David Protas

MA 1128: Lecture 19 4/20/2018. Quadratic Formula Solving Equations with Graphs

MATH 213 Linear Algebra and Ordinary Differential Equations Spring 2015 Study Sheet for Final Exam. Topics

Applied Calculus. Review Problems for the Final Exam

MA 262 Spring 1993 FINAL EXAM INSTRUCTIONS. 1. You must use a #2 pencil on the mark sense sheet (answer sheet).

Eigenvalues and eigenvectors

Properties of Linear Transformations from R n to R m

MATH The Chain Rule Fall 2016 A vector function of a vector variable is a function F: R n R m. In practice, if x 1, x n is the input,

4.2 Homogeneous Linear Equations

Exam 2 Study Guide: MATH 2080: Summer I 2016

Math 4377/6308 Advanced Linear Algebra

Exam 3 MATH Calculus I

V 1 V 2. r 3. r 6 r 4. Math 2250 Lab 12 Due Date : 4/25/2017 at 6:00pm

Limits and Continuity/Partial Derivatives

Math 240: Spring-mass Systems

Ordinary Differential Equations

Math 3313: Differential Equations Second-order ordinary differential equations

Euler-Cauchy Using Undetermined Coefficients

CALCULUS EXAM II Spring 2003

The Change-of-Variables Formula for Double Integrals

Ex. 1. Find the general solution for each of the following differential equations:

VANDERBILT UNIVERSITY. MATH 2300 MULTIVARIABLE CALCULUS Practice Test 1 Solutions

The Cayley-Hamilton Theorem and Minimal Polynomials

MA 262, Fall 2017, Final Version 01(Green)

Review Problems for Exam 2

Spring 2011 solutions. We solve this via integration by parts with u = x 2 du = 2xdx. This is another integration by parts with u = x du = dx and

EXAMPLES OF PROOFS BY INDUCTION

Arc Length and Surface Area in Parametric Equations

Math 265H: Calculus III Practice Midterm II: Fall 2014

Antiderivatives and Indefinite Integrals

Math221: HW# 7 solutions

Math 215 HW #11 Solutions

MA22S3 Summary Sheet: Ordinary Differential Equations

6 Linear Equation. 6.1 Equation with constant coefficients

ES.1803 Topic 19 Notes Jeremy Orloff. 19 Variation of parameters; exponential inputs; Euler s method

Math 240 Calculus III

Transcription:

MATH 32 Section 8.3: Non-homogeneous Systems Prof. Jonathan Duncan Walla Walla College Spring Quarter, 2007

Outline Undetermined Coefficients 2 Variation of Parameter 3 Conclusions

Undetermined Coefficients In section 4.4, which we skipped, the method of undetermined coefficients was introduced without annihilators. Form of a Particular Solution To determine the form of a particular solution to the non-homogeneous differential equation d n y dx n + a n (x) d n y dx n + + a n (x) dy dx + a n(x)y = g(x) we examine the form of g(x). Determine the form of a particular solution y p (x) to the differential equation above if g(x) is 5x + 7 2 cos 4x 3 x 2 e 5x

Applications to Matrices If we apply this procedure to a system of differential equations in matrix form, we see much the same phenomena. Form of a Particular Solution To determine the form of a particular solution to the non-homogeneous system of equations X = A X + F (t) we examine the form of F (t). Determine the general form of a particular solution X p if F (t) is 2 7 [ 2 ] e t + 0 t + 5 7

Solution Method With this guessing technique we can now wolve non-homogeneous systems using the following method. Solution Method To solve a non-homogeneous system by undetermined coefficients Solve the associated homogeneous system to find X c. Determine the form of X p with undetermined coefficients. Find X p by plugging the form above into X = A X + F. The solution is then X = X c + X p Solve the initial value problem below subject to X (0) = X = 2 3 4 3 X + 3 3 5

Another We finish this section looking at another example. Find the general solution to the differential equation dx = 5x +9y + 2t+ dt dy dt = x+y + 6 Solve the system of differential equations X = 0 2 3 X + e 4t 0 0 5 2

Variation of Parameter While the method of undetermined coefficients is straight-forward, it does have some limits. Limitations of Undetermined Coefficients Undetermined coefficients is not an appropriate method when More complicated F (t) s are much harder to deal with. When the complementary solution has eigenvalues with multiplicity, this method may not work. In section 4.6 we developed the method of variation of parameter for solving a single DE based on the assumption that for some u (x) and u 2 (x). y p = u (x)y (x) + u 2 (x)y 2 (x)

The Fundamental Matrix To see how this method would generalize to a system of differential equations, consider the following. Fundamental Matrix If X, X 2,..., X n form a fundamental set of solutions to the homogeneous system X = AX on some interval I, then the general solution can be expressed as x x n x x 2 x n c x 2 X = c.. + + c x 2n n.. = x 2 x 22 x 2n c 2........... = ϕ(t) C x n x nn x n x n2 x nn c n

Deriving the Formula We assume then that the form of the particular solution is X p = ϕ(t) U(t) for some U(t). Properties of ϕ(t) Note that ϕ(t) has two important properties. ϕ(t) is non-singular and thus invertible. ϕ (t) = Aϕ(t). Formula for X p Using the properties and assumptions above, show that X p = ϕ(t) ϕ (t) F (t) dt

s We now apply the variation of parameter formula to solve the following examples. Solve the system of equations dx = 2y +2 dt dy = 3y x + e 3t dt X = ϕ(t) C + ϕ(t) ϕ (t) F (t) dt X = c e 2t 2 + c 2 [ ] e t + 0 3 20 3

Initial Value s The variation of parameter formula can be used to solve initial value problems with a slight adjustment. Initial Value Formula Using the fundamental theorem of calculus, show that the solution to the initial value problem X = A X + F (t) subject to X (t 0 ) = ϕ(t 0 ) C = X 0 is t X = ϕ(t)ϕ (t 0 ) X 0 + ϕ(t) ϕ (s) F (s) ds t 0 Solve the initial value problem below subject to X (0) = X = 3 X + 3 4e 2t 4e 4t.

Important Concepts Things to Remember from Section 8.3 Using undetermined coefficients with matrix equations. 2 Solving non-homogeneous systems using undetermined coefficients. 3 Finding the fundamental matrix for a non-homogeneous system. 4 Using variation of parameters to solve a non-homogeneous system.