Engineering Differential Equations Practice Final Exam Solutions Fall 2011

Similar documents
[1] (20 points) Find the general solutions of y y 2y = sin(t) + e t. Solution: y(t) = y c (t) + y p (t). Complementary Solutions: y

Calculus II Solutions review final problems

(1) Then we could wave our hands over this and it would become:

MA 262, Spring 2018, Final exam Version 01 (Green)

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS

2008 AP Calculus BC Multiple Choice Exam

are given in the table below. t (hours)

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.

The Matrix Exponential

Sec 2.3 Modeling with First Order Equations

The Matrix Exponential

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then

Introduction to Condensed Matter Physics

Exercise 1. Sketch the graph of the following function. (x 2

INTEGRATION BY PARTS

Practice Problems - Week #7 Laplace - Step Functions, DE Solutions Solutions

MATH 1080 Test 2-SOLUTIONS Spring

Where k is either given or determined from the data and c is an arbitrary constant.

Math 34A. Final Review

Engineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12

LESSON 10: THE LAPLACE TRANSFORM

Southern Taiwan University

Calculus II (MAC )

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

Elements of Statistical Thermodynamics

Problem Set 6 Solutions

MATH 319, WEEK 15: The Fundamental Matrix, Non-Homogeneous Systems of Differential Equations

Differential Equations

( ) Differential Equations. Unit-7. Exact Differential Equations: M d x + N d y = 0. Verify the condition

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

VTU NOTES QUESTION PAPERS NEWS RESULTS FORUMS

1 General boundary conditions in diffusion

DIFFERENTIAL EQUATION

6.1 Integration by Parts and Present Value. Copyright Cengage Learning. All rights reserved.

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

Higher order derivatives

First order differential equation Linear equation; Method of integrating factors

2.3 Matrix Formulation

Chapter 10 Time-Domain Analysis and Design of Control Systems

10. The Discrete-Time Fourier Transform (DTFT)

6. The Interaction of Light and Matter

Additional Math (4047) Paper 2 (100 marks) y x. 2 d. d d

MA 266 FINAL EXAM INSTRUCTIONS May 2, 2005

Solution of Assignment #2

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C

MSLC Math 151 WI09 Exam 2 Review Solutions

DISCRETE TIME FOURIER TRANSFORM (DTFT)

nd the particular orthogonal trajectory from the family of orthogonal trajectories passing through point (0; 1).

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Introduction to the Fourier transform. Computer Vision & Digital Image Processing. The Fourier transform (continued) The Fourier transform (continued)

1973 AP Calculus AB: Section I

Integral Calculus What is integral calculus?

2. Laser physics - basics

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

AS 5850 Finite Element Analysis

High Energy Physics. Lecture 5 The Passage of Particles through Matter

Chapter 7: The Laplace Transform Part 1

Laplace Transform of Discontinuous Functions

with Dirichlet boundary conditions on the rectangle Ω = [0, 1] [0, 2]. Here,

Reading assignment: In this chapter we will cover Sections Definition and the Laplace transform of simple functions

4 x 4, and. where x is Town Square

10. Limits involving infinity

A. Limits and Horizontal Asymptotes ( ) f x f x. f x. x "±# ( ).

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

PHA 5127 Answers Homework 2 Fall 2001

BSc Engineering Sciences A. Y. 2017/18 Written exam of the course Mathematical Analysis 2 August 30, x n, ) n 2

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Mathematics 1110H Calculus I: Limits, derivatives, and Integrals Trent University, Summer 2018 Solutions to the Actual Final Examination

Unit 6: Solving Exponential Equations and More

Reading assignment: In this chapter we will cover Sections Definition and the Laplace transform of simple functions

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Chapter 1. Chapter 10. Chapter 2. Chapter 11. Chapter 3. Chapter 12. Chapter 4. Chapter 13. Chapter 5. Chapter 14. Chapter 6. Chapter 7.

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS

Finite element discretization of Laplace and Poisson equations

Chapter 10. The singular integral Introducing S(n) and J(n)

SOLUTIONS FOR HOMEWORK SECTION 6.4 AND 6.5

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

3 2x. 3x 2. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Differential Equations

A Quadratic Serendipity Plane Stress Rectangular Element

Stochastic Heating in RF capacitive discharges

1997 AP Calculus AB: Section I, Part A

Search sequence databases 3 10/25/2016

P3-4 (a) Note: This problem can have many solutions as data fitting can be done in many ways. Using Arrhenius Equation For Fire flies: T(in K)

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

UNIT I PARTIAL DIFFERENTIAL EQUATIONS PART B. 3) Form the partial differential equation by eliminating the arbitrary functions

General Notes About 2007 AP Physics Scoring Guidelines

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

1997 AP Calculus AB: Section I, Part A

4. (5a + b) 7 & x 1 = (3x 1)log 10 4 = log (M1) [4] d = 3 [4] T 2 = 5 + = 16 or or 16.

TMA4125 Matematikk 4N Spring 2016

R L R L L sl C L 1 sc

Modeling in the Frequency Domain

Constants and Conversions:

Math 102. Rumbos Spring Solutions to Assignment #8. Solution: The matrix, A, corresponding to the system in (1) is

Calculus Revision A2 Level

LAPLACE TRANSFORM REVIEW SOLUTIONS

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

Basics about radiative transfer

Transcription:

9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr. pt. Firt writ th d.. in tandard form: y y = x x. pt. Th intgrating factor i ρ(x) = /x dx = ln(x) = x. pt. Multiplying both id of th tandard form of th d.. by th intgrating factor, w hav ( x y y = x x) ( x ) pt. x y x y = x d x y = x dx x y = x dx = x + c. pt. y() = 4 (4) = + c c =. pt. Thrfor, x y = x + y = x + x. Problm. (0 pt.) Solv th following initial valu problm: xy x + x {{ M + ln x + y = 0 {{ N xy x + x + ln x + y = 0 with y(5) = 0. Thi d.. i both linar (bcau y and y appar only to th firt powr) and xact (bcau M/ y = N/ x. pt. ( ( x/ x To trat th d.. a linar, firt writ th d.. in tandard form: y + ) ) x + ln(x y = + ) ln(x + ). pt. ( x/ ( x + ) Th intgrating factor i ρ(x) = xp ln(x + ) dx {{ u=ln(x +) ) ) = lnln(x +) = ln (x +. pt. Multiplying both id of th tandard form of th d.. by th intgrating factor, w hav x ln x + y + x y = x pt. d { ln x + y = x + dx ln x + y = x dx = x + c. pt. y(5) = 0 ln 5 + (0) = 5 + c c = 5. pt. Thrfor, ln x + y = x 5.

If you rgard th d.. a an xact quation, th olution of th d.. i f(x, y) = c, whr th function f atifi th condition f x = M = xy f x x and + y = N = ln x +. f x = xy xy x + x f = x + x dx = y ln x + x + g(y) pt. f y = ln x + + g (y). But f y = N = ln x +, o ln x + + g (y) = ln x + g (y) = g(y) = y pt.. Thrfor, f = y ln ( x + ) x y, o th olution of th d.. i y ln ( x + ) x y = c. pt. Th initial condition y(5) = 0 0 ln 5 + 5 (0) = c c = 5 pt.. Thrfor, th olution of th givn IVP i y ln ( x + ) x y = 5 Problm. (5 point) A 000 gallon holding tank that catch runoff from om chmical proc initially ha 600 gallon of watr with Q(0) = ounc of pollutant diolvd in it. Pollutd watr flow into th tank at a rat of gal/hr and contain 5 ounc/gal of pollutant in it. Th wll mixd olution lav th tank at gal/hr a wll. Aftr how many hour will th amount of pollutant in th tank rach 500 ounc? dq = rat in - rat out = (flow rat in)(concntration in) - (flow rat out)(concntration out), dt pt. o dq ( dt = gal ) ( 5 oz ) ( gal ) Q oz. 5 pt. hr gal hr 600 gal (Th volum of liquid in th tank i contant bcau th flow rat in qual th flow rat out.) Thrfor, th d.. modling thi mixing problm i dq dt = 5 Q Thi d.. i both parabl and linar d.. pt. Trating th d.. a a parabl quation, w hav dq dt = 5 Q = (Q 000) dq Q 000 = dt dq dt Q 000 = t ln Q 000 = + c 5 pt. Th initial condition Q(0) = ln 000 = 0 + c c = ln(998) pt. ln Q 000 = t + ln(998) To dtrmin whn th amount of pollutant in th tank rach 500 ounc, t Q = 500 and olv for t: ln 500 000 = t + ln(998) t = (ln(500) ln(998)) 6 hour pt. To trat th d.. a a linar quation, firt put it into tandard form: dq dt + Q = 5. pt. Th intgrating factor i ρ(t) = / dt = t/. pt. Multiplying both id of th tandard form of th d.. by th intgrating factor, w hav dq t/ dt + Q = 5 t/ t/dq dt + t/ Q = 5 t/ d t/ Q = 5 t/ dt t/ Q = 5 t/ dt = 000 t/ + c. pt. Q(0) = 0 () = 000 0 + c = c = 998. pt. Thrfor, t/ Q = 000 t/ 998 Q = 000 998 t/.

To dtrmin whn th amount of pollutant in th tank rach 500 ounc, t Q = 500 and olv for t: 500 = 000 998 t/ t = ln(500/998) 6 hour pt. Problm 4. (0 point) Find th gnral olution to ach of th following diffrntial quation: a. (4 point) y + 6y + 9y = 0 Th charactritic quation i r + 6r + 9 = 0 (r + ) = 0 r = (doubl root). pt. Thrfor, y = c x + c x x. pt. b. (6 point) y () 6y + y = 0 Th charactritic quation i r 6r + r = 0 r r 6r + = 0 r = ( 6) ± ( 6) 4()() () r 6r + = 0. = 6 ± 6 Thu, th root of th charactritic quation ar 0 and ± i. pt. = 6 ± 4i = ± i Thrfor, y = c 0x + c x co(x) + c x in(x) or y = c + c x co(x) + c x in(x). 4 pt. Problm 5. (5 point) Solv th following initial valu problm: y + 4y = 6 x 8x with y(0) = and y (0) = 0. Stp. Find y c by olving th homognou d.. y + 4y = 0. Charactritic quation: r + 4 = 0 r = 4 r = ± 4 = 0 ± i. Thrfor, y c = c 0x co(x) + c 0x in(x) = c co(x) + c in(x). pt. Stp. Find y p uing ithr th Mthod of Undtrmind Cofficint or th Mthod of Variation of Paramtr. Mthod. Undtrmind Cofficint. Sinc th nonhomognou trm in th d.. (6 x 8x ) i th um of an xponntial function and a polynomial of dgr, w gu that y p i th um of an xponntial function and a polynomial of dgr : y p = A x +Bx +Cx+D. No trm in thi gu duplicat a trm in y c, o thr i no nd to modify th gu. pt. y = A x +Bx +Cx+D y = A x +Bx+C y = 4A x +B. Thrfor, th lft id of th d.. i y + 4y = 4A x + B + 4 A x + Bx + Cx + D = 8A x + 4Bx + 4Cx + B + 4D. W want thi to qual th nonhomognou trm 6 x 8x, o 8A = 6, 4B = 8, 4C = 0, and B + 4D = 0 A =, B =, C = 0, and D =. Thrfor, y p = x x +. 6 pt. Mthod. Variation of Paramtr. From y c w obtain two indpndnt olution of th homognou d.: y = co(x) and y y = in(x). Th Wronkian i givn by W(x) = y y y = co(x) in(x) in(x) co(x)

= co(x) ( co(x)) ( in(x)) in(x) = co (x) + in (x) =. pt. ( y f(x) in(x) 6 x 8x ) u = dx = dx = 4x in(x) dx 8 x in(x) dx W(x) For th firt intgral, u ubtitution with u = x and u ntri 40 (with n = ) and 9 from th Tabl of Intgral: 4x in(x) dx = u in(u) du = u co(u) + u co(u) du = u co(u) + (co(u) + u in(u)) = x co(x) + co(x) + x in(x) For th cond intgral in th formula for u, u ntry 49 from th Tabl of Intgral with a = and b = : 8 x x in(x) dx = 8 + in(x) co(x) = x in(x) + x co(x) Thrfor, u = x co(x) + co(x) + x in(x) 4 x in(x) + 4 x co(x) pt. ( y f(x) co(x) 6 x u = W(x) dx = 8x ) dx = 8 x co(x) dx 4x co(x) dx For th firt intgral, u ntry 50 from th Tabl of Intgral with a = and b = : 8 x x co(x) dx = 8 + co(x) + in(x) = x co(x) + x in(x) For th cond intgral in th formula for u, u ubtitution with u = x and u ntri 4 (with n = ) and 8 from th Tabl of Intgral: 4x co(x) dx = u co(u) du = u in(u) u in(u) du = u in(u) (in(u) u co(u)) = x in(x) + in(x) x co(x) Thrfor, u = x co(x) + x in(x) x in(x) + in(x) x co(x) pt. and y p = u y + u y = x co(x) + co(x) + x in(x) x in(x) + x co(x) co(x) + x co(x) + x in(x) x in(x) + in(x) x co(x) in(x) = x co (x) + co (x) + x in(x) co(x) x in(x) co(x) + x co (x) + x co(x) inx) + x in (x) x in (x) + in (x) x co(x) in(x) = x co (x) + in (x) + co (x) + in (x) + x co (x) + in (x) = x + + x pt. Stp. y = y c + y p, o y = c co(x) + c in(x) + x x +. pt. Stp 4. U th initial condition to find c and c. y = c co(x) + c in(x) + x x + y = c in(x) + c co(x) + 4 x 4x y(0) = = c co(0) + c in(0) + 0 (0) + = c + c = 0 pt. y (0) = 0 0 = c in(0) + c co(0) + 4 0 4(0) = c + 4 c = pt. Thrfor, y = in(x) + x x +.

Problm 6. (5 point) Conidr a dampd, forcd ma/pring ytm. Lt t dnot tim (in cond) and lt x(t) dnot th poition (in mtr) of th ma at tim t, with x = 0 corrponding to th quilibrium poition. Suppo th ma m = kg, th damping contant c = N /m, th pring contant k = N/m, th xtrnal forc i F(t) = 0 co(t), th initial poition x(0) = m, and th initial vlocity x (0) = m/. a. ( point) Find th poition function x(t). Th d.. modling thi ytm i mx + cx + kx = F(t), or x + x + x = 0 co(t). pt. Stp. Find x c by olving th homognou d.. x + x + x = 0. Charactritic quation: r + r + = 0 (r + )(r + ) = 0 r = or r = x c = c t + c t. pt. Stp. Find x p uing ithr th Mthod of Undtrmind Cofficint or th Mthod of Variation of Paramtr. Mthod. Undtrmind Cofficint. Sinc th nonhomognou trm in th d.. (0 co(t)) i a coin, w gu that x p i th um of a coin and in with th am frquncy: x p = A co(t) + B in(t). No trm in thi gu duplicat a trm in x c, o thr i no nd to modify th gu. pt. x = A co(t) + B in(t) x = A in(t) + B co(t) x = 4A co(t) 4B in(t). Thrfor, th lft id of th d.. i x +x +x = 4A co(t) 4B in(t)+ A in(t) + B co(t)+ A co(t) + B in(t) = A + 6B co(t) + 6A Bin(t). W want thi to qual th nonhomognou trm 0 co(t), o A + 6B = 0 and 6A B = 0 A = and B =. Thrfor, x p = co(t) + in(t). 4 pt. Mthod. Variation of Paramtr. From x c w obtain two indpndnt olution of th homognou d.: x = t and x = t x. Th Wronkian i givn by W = x x x = t t t t ( = t t) ( t) t = t. pt. x F(t) t (0 co(t)) u = dt = W t dt = 0 t co(t) dt t = 0 + co(t) + in(t) = 5 t co(t) 5 t in(t) pt. whr w hav ud ntry 50 from th Tabl of Intgral. x F(t) t u = W dt = (0 co(t)) t dt = 0 t co(t) dt t = 0 + co(t) + in(t) = 4 t co(t) + 8 t in(t) pt. whr again w hav ud ntry 50 from th Tabl of Intgral. x p = u x + u x = 5 t co(t) 5 t in(t) t + 4 t co(t) + 8 t in(t) t = co(t) + in(t) pt. Stp. x = x c + x p, o x = c t + c t co(t) + in(t). pt. Stp 4. U th initial condition to find c and c. x = c t + c t co(t) + in(t) x = c t c t + in(t) + 6 co(t) x(0) = = c 0 + c 0 co(0) + in(0) = c + c c + c = x (0) = = c 0 c 0 + in(0) + 6 co(0) = c c + 6 c c = 4 c + c =, c c = 4 c =, c = 0. pt. Thrfor, x = t co(t) + in(t).

b. ( point) What part of th olution you found in part a i th tranint part of th olution, x tr? Th tranint part of th olution i th part that approach 0 a t, o x tr = t c. ( point) What part of th olution you found in part a i th tady-tat (tady priodic) part of th olution, x p? Th tady-tat part of th olution i th part that do not approach 0 a t, o x p = co(t) + in(t) Problm 7. (0 point) Find L {F() whr a. F() = 6 U a partial fraction dcompoition: 6 = ( )( + ) = A + B Multiplying both id of th quation ( )( + ) = A + B by th dnominator ( )(+), w obtain = A( + ) + B( ) = A + A + B B = (A + B) + A B A + B =, A B = 0 A = 9/5, B = 6/5. pt. Thrfor, L { 6 { { { = L 9/5 + 6/5 = 9 5 L + 6 5 L + = 9 5 t + 6 5 t uing th Laplac Tranform tabl ntry L { a b. F() = 8 4 + ( + 4) = at pt. U a partial fraction dcompoition: 8 4 + ( = A + 4) + B + C + 4 Multiplying both id of thi quation by th dnominator + 4 w obtain 8 4 + = A + 4 + (B + C) = (A + B) + C + 4A A + B = 8, C = 4, and 4A = A =, B = 5, and C = 4. pt. Thrfor, { 8 L { 4 + ( = L + 4) + 5 4 { { { = L + 5L + 4 L + 4 = + 4 + 5 co(t) in(t) uing th Laplac Tranform tabl ntri { { { L =, L + k = co(kt), and L k + k = in(kt) pt. Problm 8. (5 point) a. Find L{h(t) whr h(t) i th picwi-dfind function givn by { if 0 t < 0 h(t) = 0 if t 0. h(t) = u(t 0) pt. o L {h(t) = L { u(t 0) = L { L {u(t 0) ( 0 = = ) 0 pt.

b. Suppo y(t) i th iz of a population of fih (maurd in ton) t day aftr th tart of th fihing aon, with a % individual growth rat. Suppo that y(0) = 00 and that w harvt h(t) ton pr day whr h(t) i th picwi-dfind function givn in part a (i.., w allow a 0 day harvt bfor impoing a ban on harvting). Th balanc law for population growth thu giv y (t) = 0.0y(t) h(t), y(0) = 00 Solv thi initial valu problm for y uing Laplac Tranform. Solution to thi IVP not uing th Laplac tranform mthod will not rciv any crdit. y (t) = 0.0y(t) h(t) y 0.0y = h(t) L { y 0.0y = L { h(t) L { y 0.0L{y = L {h(t) pt. L{y y(0) 0.0L{y = 0 pt. L{y 00 0.0L{y = + 0 ( 0.0)L{y = 00 + 0 L{y = 00 0.0 ( 0.0) + 0 ( 0.0) pt. { 00 y = L 0.0 ( 0.0) + 0 { L { 00 y = L 0.0 ( 0.0) { = 00 0.0t f(t) + u(t 0)f(t 0) whr f(t) = L (W ud th Laplac Tranform tabl ntry L { a ( 0.0) + L { 0 ( 0.0) pt. ( 0.0) = at with a = 0.0.) To find f(t) w u a partial fraction dcompoition: ( 0.0) = A + B 0.0 A = + B ( 0.0) = A ( 0.0) + B 0.0 = A 0.0A + B = (A + B) 0.0A A + B = 0, { 0.0A = A = 00, B = 00 00 f(t) = L + 00 { { = 00L + 00L = 00() + 00 0.0t 0.0 0.0 { { (W ud th Laplac Tranform tabl ntri L = at with a = 0.0 and L =.) a Thrfor, y = 00 0.0t 00 + 00 0.0t + u(t 0) y = 00 0.0t + 00u(t 0) 0.0(t 0) pt. 00 + 00 0.0(t 0)