Math 22B, Homework #8 1. y 5y + 6y = 2e t



Similar documents
Solutions to Sample Problems for Test 3

So far, we have looked at homogeneous equations

9. Particular Solutions of Non-homogeneous second order equations Undetermined Coefficients

MECH Statics & Dynamics

HW6 Solutions. MATH 20D Fall 2013 Prof: Sun Hui TA: Zezhou Zhang (David) November 14, Checklist: Section 7.8: 1c, 2, 7, 10, [16]

TRANSFORM AND ITS APPLICATION

The integrating factor method (Sect. 2.1).

MATH 31B: MIDTERM 1 REVIEW. 1. Inverses. yx 3y = 1. x = 1 + 3y y 4( 1) + 32 = 1

Solution of the Heat Equation for transient conduction by LaPlace Transform

HOMEWORK 5 SOLUTIONS. n!f n (1) lim. ln x n! + xn x. 1 = G n 1 (x). (2) k + 1 n. (n 1)!

Student name: Earlham College. Fall 2011 December 15, 2011

Higher Order Equations

v = x t = x 2 x 1 t 2 t 1 The average speed of the particle is absolute value of the average velocity and is given Distance travelled t

ORDINARY DIFFERENTIAL EQUATIONS

The Nonlinear Pendulum

Homework #2 Solutions

Math Assignment 6

Partial Fractions: Undetermined Coefficients

General Theory of Differential Equations Sections 2.8, , 4.1

I. Pointwise convergence

Optical Illusion. Sara Bolouki, Roger Grosse, Honglak Lee, Andrew Ng

A First Course in Elementary Differential Equations. Marcel B. Finan Arkansas Tech University c All Rights Reserved

The Method of Partial Fractions Math 121 Calculus II Spring 2015

Part IB Paper 6: Information Engineering LINEAR SYSTEMS AND CONTROL Dr Glenn Vinnicombe HANDOUT 3. Stability and pole locations.

ECG590I Asset Pricing. Lecture 2: Present Value 1

Integrals of Rational Functions

Second Order Linear Nonhomogeneous Differential Equations; Method of Undetermined Coefficients. y + p(t) y + q(t) y = g(t), g(t) 0.

Homework 2 Solutions

Lecture Notes for Math250: Ordinary Differential Equations

1. (from Stewart, page 586) Solve the initial value problem.

HOMOTOPY PERTURBATION METHOD FOR SOLVING A MODEL FOR HIV INFECTION OF CD4 + T CELLS

Figure 2.1. a. Block diagram representation of a system; b. block diagram representation of an interconnection of subsystems

EASTERN ARIZONA COLLEGE Differential Equations

CITY UNIVERSITY LONDON. BEng Degree in Computer Systems Engineering Part II BSc Degree in Computer Systems Engineering Part III PART 2 EXAMINATION

Homework # 3 Solutions

σ m using Equation 8.1 given that σ

Solutions for Review Problems

12.4 UNDRIVEN, PARALLEL RLC CIRCUIT*

Math Practice exam 2 - solutions

Physics 111. Exam #1. January 24, 2014

PHYSICS 151 Notes for Online Lecture #11

Mixed Method of Model Reduction for Uncertain Systems

Lecture 5 Rational functions and partial fraction expansion

College of the Holy Cross, Spring 2009 Math 373, Partial Differential Equations Midterm 1 Practice Questions

Incline and Friction Examples

Homework #1 Solutions

y cos 3 x dx y cos 2 x cos x dx y 1 sin 2 x cos x dx

LS.6 Solution Matrices

MATH 425, PRACTICE FINAL EXAM SOLUTIONS.

MATH 10550, EXAM 2 SOLUTIONS. x 2 + 2xy y 2 + x = 2

CHAPTER 2. Eigenvalue Problems (EVP s) for ODE s

A note on profit maximization and monotonicity for inbound call centers

Zeros of Polynomial Functions

THE COMPLEX EXPONENTIAL FUNCTION

You may use a scientific calculator (non-graphing, non-programmable) during testing.

INTEGRATING FACTOR METHOD

1 Lecture: Integration of rational functions by decomposition

Solving DEs by Separation of Variables.

19.6. Finding a Particular Integral. Introduction. Prerequisites. Learning Outcomes. Learning Style

Linear energy-preserving integrators for Poisson systems

Math Practice Exam 2 with Some Solutions

COWLEY COLLEGE & Area Vocational Technical School

Math 55: Discrete Mathematics

Solution to Problem Set 1

where x is check for normality T

Solutions to Linear First Order ODE s

Class Meeting # 1: Introduction to PDEs

y cos 3 x dx y cos 2 x cos x dx y 1 sin 2 x cos x dx y 1 u 2 du u 1 3u 3 C

Intermediate Value Theorem, Rolle s Theorem and Mean Value Theorem

Nonhomogeneous Linear Equations

Solutions to Homework 5

RAJALAKSHMI ENGINEERING COLLEGE MA 2161 UNIT I - ORDINARY DIFFERENTIAL EQUATIONS PART A

Separable First Order Differential Equations

Integral Calculus - Exercises

A new continuous dependence result for impulsive retarded functional differential equations

AB2.5: Surfaces and Surface Integrals. Divergence Theorem of Gauss

AP Calculus AB 2007 Scoring Guidelines Form B

Core Maths C3. Revision Notes

Methods of Solution of Selected Differential Equations Carol A. Edwards Chandler-Gilbert Community College

36 CHAPTER 1. LIMITS AND CONTINUITY. Figure 1.17: At which points is f not continuous?

PRACTICE FINAL. Problem 1. Find the dimensions of the isosceles triangle with largest area that can be inscribed in a circle of radius 10cm.

The two dimensional heat equation

Differential Equations and Linear Algebra Lecture Notes. Simon J.A. Malham. Department of Mathematics, Heriot-Watt University

Laplace Transform. f(t)e st dt,

Derivation of the Laplace equation

Transient turbulent flow in a pipe

Lecture 14: Transformers. Ideal Transformers

Inner Product Spaces

AP Calculus AB 2004 Scoring Guidelines

AP Calculus AB 2005 Scoring Guidelines Form B

Rotation of an Object About a Fixed Axis

Coffeyville Community College #MATH 202 COURSE SYLLABUS FOR DIFFERENTIAL EQUATIONS. Ryan Willis Instructor

19.7. Applications of Differential Equations. Introduction. Prerequisites. Learning Outcomes. Learning Style

Review Solutions MAT V (a) If u = 4 x, then du = dx. Hence, substitution implies 1. dx = du = 2 u + C = 2 4 x + C.

Linear and quadratic Taylor polynomials for functions of several variables.

Math 115 Spring 2011 Written Homework 5 Solutions

Transcription:

Math 22B, Homework #8 3.7 Problem # We find a particular olution of the ODE y 5y + 6y 2e t uing the method of variation of parameter and then verify the olution uing the method of undetermined coefficient. VOP Firt we olve the homogeneou equation uing the characteritic equation r 2 5r + 6 which ha root r 3, 2. a fundamental et of olution for the homogeneou equation i y e 3t and y 2 e 2t we aume that a particular olution ha the form differentiating we get that y p (t) u (t)e 3t + u 2 (t)e 2t y p 3u e 3t + 2u 2 e 2t y p 3(u + 3u )e 3t + 2(u 2 + 2u 2 )e 2t The form of y p come from the contituent equation u e 3t + u 2e 2t () Plugging y p and it derivative back into the ODE we get a econd equation 3u e 3t + 2u 2e 2t 2e t (2) Putting equation () and (2) together we get the ytem [ [ [ e 3t e 2t u 3e 3t 2e 2t u 2 2e t Solving the ytem we obtain [ u u 2 [ 2e 2t 2e t after integrating we get: u e 2t and u 2 2e t Returning to the original form we get y p (t) u (t)e 3t + u 2 (t)e 2t e 2t e 3t + 2e t e 2t e t

Math 22B, Homework #8 2 UC Now we can check the anwer above by the following: Aume that y p where A i a contant. Then we get Ae t A and y p e t Ae t 5Ae t + 6Ae t 2e t 2A 2 Problem #5 We ue Variation of Parameter to olve the ODE y + y tan t < t < π 2 y h (t) The characteritic equation i r 2 + which ha root r ±i. the general olution to the homogeneou equation i VOP We aume that y h A co t + B in t y p (t) u (t) co t + u 2 (t) in t Then the derivative of y p have the form y p u in t + u 2 co t y p (u 2 u ) co t (u + u 2 ) in t The form of y p come from the contituent equation u co t + u 2 in t () Plugging y p and it derivative back into the ODE we get another equation u in t + u 2 co t tan t (2) Putting equation () and (2) together we get the ytem [ [ [ co t in t u in t co t u 2 tan t Which after olving yield [ u u 2 [ ec t + co t in t u (t) Now we have u (t) ec t + co t thu u (t) ( ec t + co t)dt ec tdt + co tdt The econd integral i eay, but to do the firt we write ec t co t co t co t co t co t in 2 t

Math 22B, Homework #8 3 So ( ec tdt Now, let u in t and du co tdt, then ( ) co t du in 2 dt t u [ 2 2 co t in 2 t ) dt du + u + du u 2 ln + u u So finally we get ( ) co t ec tdt in 2 dt t 2 ln + in t in t u (t) in t 2 ln + in t in t u 2 (t) Thankfully, the expreion for u 2 i much eaier. We have u 2 in t thu u 2 (t) co t y p (t) Now we aumed that y p (t) u (t) co t + u 2 (t) in t So [ y p (t) in t 2 ln + in t in t co t + [ co t in t y p (t) 2 ln + in t in t co t y(t) Now for the general olution y(t) y h (t) + y p (t), thu y(t) A co t + B in t 2 ln + in t in t co t Problem #6 Given that y e t and y 2 t form a fundamental et of olution for ( t)y + ty y we find a particular olution for Aume that Then the derivative of y p become with the contituent equation ( t)y + ty y 2(t ) 2 e t y p (t) u e t + u 2 t y p u e t + u 2 y p (u + u )e t + u 2 u e t + u 2t ()

Math 22B, Homework #8 4 Plugging y p and it derivative into the ODE we get Putting () and (2) together we have [ e t t [ u e t u 2 u e t + u 2 2( t)e t (2) [ 2( t)e t Inverting give [ u u 2, after integrating, we get [ 2te 2t 2e t u (t) te 2t + 2 e 2t and u 2 (t) 2e t y p (t) u e t + u 2 t (te 2t + 2 e 2t ) e t + ( 2e t )t 2 e t te t Problem #2 Let y(t) be any olution to the IVP L[y y + p(t)y + q(t)y g(t) ; y(t ) y ; y (t ) y By Theorem 3.2. there exit a unique function u(t) which i a olution to the IVP L[u u + p(t)u + q(t)u ; u(t ) y ; u (t ) y Then let v(t) y(t) u(t). We have L[v L[y u L[y L[u g(t) g(t) and v(t ) y(t ) u(t ) y y ; v (t ) y (t ) u (t ) y y y(t) v(t) + u(t) i a olution to the original IVP. 6. Problem #5 (a) Find L[t L[t te t dt [ te t 2 e t 2 (b) Find L[t 2 L[t 2 t 2 e t dt [ t2 e t 2 2 e t 2 3 e t 2 3

Math 22B, Homework #8 5 (c) Find L[t n. L[t n t n e t dt n! n+ The reaon i that all the term in the integral are of the form t k e t for the lat term. The coefficient of the lat term i n!. n+ k except Problem #9 Find L[e at coh bt ( ) e L[e at coh bt L [e at bt + e bt 2 2 (L[e(a+b)t + L[e (a b)t ) 2 (L[e(a+b)t + L[e (a b)t ) [ 2 (a + b) + a (a b) ( a) 2 b 2 L[e at a coh bt ( a) 2 b 2 Problem #3 Find L[e at in bt L[e at in bt [ L[e (a+ib)t L[e (a ib)t [ 2i 2i (a + ib) (a ib) Problem #8 Find L[t n e at 6.2 Let S a. Then Problem # Solve the IVP L[t n e at uing a Laplace tranform. t n e (a )t dt L[e at in bt t n e at e t dt L[t n e at y y 6y ; b ( a) 2 + b 2 t n e (a )t dt t n e St dt n! S n+ n! ( a) n+ n! ( a) n+ y() ; y () L[y y 6y ( 2 Y () y() y ()) (Y () y()) 6Y () Y () 2 2 6 5 y(t) 5 e3t + 4 5 e 2t 3 + 4 5 + 2 b ( a) 2 + b 2

Math 22B, Homework #8 6 Problem #4 Solve the IVP y 4y + 4y ; y() ; y () uing a Laplace tranform. L[y 4y + 4y ( 2 Y () y() y ()) 4(Y () y()) + 4Y () Y () 3 ( 2) 2 2 ( 2) 2 ( 2) 2 Y () 2 ( 2) 2 y(t) e 2t te 2t ( t)e 2t Problem #6 Solve the IVP y + 2y + 5y ; y() 2 ; y () uing a Laplace tranform. L[y + 2y + 5y ( 2 Y y() y ()) + 2(Y y()) + 5Y Y () 2 + 3 2 + 2 + 5 Problem #8 Solve the IVP (2 + 2) + ( 2 + 2 + ) + 4 2 + ( + ) 2 + 4 + 2 2 ( + ) 2 + 4 y(t) 2e t co 2t + 2 e t in 2t y iv y ; y() ; y () ; y () ; y () uing a Laplace tranform. L[y iv y ( 4 Y 3 y() 2 y () y () y ()) Y Y () 3 + 4 y(t) coh t 2 Problem #2 Solve the IVP uing a Laplace tranform. y 2y + 2y co t ; y() ; y () L[y 2y + 2y ( 2 Y y() y ()) 2(Y y()) + 2Y 2 + L[co t

Math 22B, Homework #8 7 ( ) ( ) 2 Y () + 2 2 + 2 ( } {{ } 2 + ) ( 2 2 + 2) } {{ } () (2) We can deal with the two part () and (2) eperately ince L i a linear operator. Furthermore () correpond to the homogeneou equation and (2) to a particular olution to the given ODE. () We have Y h () 2 2 2 + 2 2 ( ) 2 + ( ) 2 + ( ) 2 + y h (t) e t co t e t in t (2) Here we have Now we aume that Y p () ( 2 + ) ( 2 2 + 2) ( 2 + ) ( 2 2 + 2) A + B 2 2 + 2 + C + D 2 + Solving thi we get A 5 ; B 4 5 ; C 5 ; D 2 5. Y p () [ + 4 5 2 2 + 2 + 2 [ ( ) 3 2 + 5 ( ) 2 + + 2 + 2 2 + And finally Y p (t) 5 ( ) ( ) 2 + + 3 5 ( ) 2 + + 5 2 + 2 5 2 + Hence y p (t) 5 et co t + 3 5 et in t + 5 co t 2 5 in t Finally if we put () and (2) together we get y(t) y h (t) + y p (t) 4 5 et co t 2 5 et in t + 5 co t 2 5 in t Proble #23 Solve the IVP y + 2y + y 4e t ; y() 2 ; y () uing a Laplace tranform. L[y + 2y + y ( 2 Y y() y ()) + 2(Y y()) + Y 4 + L[4e 4t

Math 22B, Homework #8 8 And finally Y () 2 + 3 2 + 2 + + 4 ( + )( 2 + 2 + ) Y () + + ( + ) + 2 2 2 ( + ) 3 y(t) 2e t + te t + 2t 2 e t 2( + ) + 4 + ( + ) 2 ( + ) 3