Elementary Differential Equations and Boundary Value Problems

Similar documents
Class Notes 1: Introduction. MAE 82 Engineering Mathematics

1 st order ODE Initial Condition

MA Study Guide #1

MA 366 Review - Test # 1

Math 2214 Solution Test 1A Spring 2016

Math 1b. Calculus, Series, and Differential Equations. Final Exam Solutions

Boyce/DiPrima/Meade 11 th ed, Ch 1.1: Basic Mathematical Models; Direction Fields

Math 2214 Solution Test 1B Fall 2017

ME 391 Mechanical Engineering Analysis

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

Boyce/DiPrima 10 th ed, Ch 1.1: Basic Mathematical Models; Direction Fields

Elementary Differential Equations and Boundary Value Problems

Chapter 2. First Order Scalar Equations

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Some Basic Information about M-S-D Systems

ln 2 1 ln y x c y C x

Exam 1 Solutions. 1 Question 1. February 10, Part (A) 1.2 Part (B) To find equilibrium solutions, set P (t) = C = dp

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

Solutions to Assignment 1

EXERCISES FOR SECTION 1.5

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

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page

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

Ordinary Differential Equations

PROBLEMS FOR MATH 162 If a problem is starred, all subproblems are due. If only subproblems are starred, only those are due. SLOPES OF TANGENT LINES

5.2. The Natural Logarithm. Solution

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

3.6 Derivatives as Rates of Change

Math 116 Second Midterm March 21, 2016

and v y . The changes occur, respectively, because of the acceleration components a x and a y

Section 3.8, Mechanical and Electrical Vibrations

KINEMATICS IN ONE DIMENSION

10.6 Parametric Equations

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

8. Basic RL and RC Circuits

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

EEEB113 CIRCUIT ANALYSIS I

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

First Order RC and RL Transient Circuits

ASTR415: Problem Set #5

Math 333 Problem Set #2 Solution 14 February 2003

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance

AP Chemistry--Chapter 12: Chemical Kinetics

6.2 Transforms of Derivatives and Integrals.

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

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

Chapter 3 Boundary Value Problem

Review - Quiz # 1. 1 g(y) dy = f(x) dx. y x. = u, so that y = xu and dy. dx (Sometimes you may want to use the substitution x y

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Ordinary Differential Equations

Vehicle Arrival Models : Headway

Introduction to Physical Oceanography Homework 5 - Solutions

ln y t 2 t c where c is an arbitrary real constant

1.6. Slopes of Tangents and Instantaneous Rate of Change

Differential Equations

Chapter 8 The Complete Response of RL and RC Circuits

IMPROVED HYPERBOLIC FUNCTION METHOD AND EXACT SOLUTIONS FOR VARIABLE COEFFICIENT BENJAMIN-BONA-MAHONY-BURGERS EQUATION

ENGI 9420 Engineering Analysis Assignment 2 Solutions

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x

AP Calculus BC - Parametric equations and vectors Chapter 9- AP Exam Problems solutions

CHAPTER 6: FIRST-ORDER CIRCUITS

Lecture 13 RC/RL Circuits, Time Dependent Op Amp Circuits

INDEX. Transient analysis 1 Initial Conditions 1

Chapter 7 Response of First-order RL and RC Circuits

CSE 3802 / ECE Numerical Methods in Scientific Computation. Jinbo Bi. Department of Computer Science & Engineering

Class Meeting # 10: Introduction to the Wave Equation

System of Linear Differential Equations

Boyce/DiPrima/Meade 11 th ed, Ch 3.1: 2 nd Order Linear Homogeneous Equations-Constant Coefficients

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

DIFFERENTIAL EQUATIONS

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

Second Order Linear Differential Equations

10. State Space Methods

THE SINE INTEGRAL. x dt t

Multiple Choice Solutions 1. E (2003 AB25) () xt t t t 2. A (2008 AB21/BC21) 3. B (2008 AB7) Using Fundamental Theorem of Calculus: 1

Solutions for homework 12

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:

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

Basic Circuit Elements Professor J R Lucas November 2001

CHAPTER 12 DIRECT CURRENT CIRCUITS

Wall. x(t) f(t) x(t = 0) = x 0, t=0. which describes the motion of the mass in absence of any external forcing.

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections

15. Vector Valued Functions

Chapter 1 Fundamental Concepts

Elementary Linear Algebra

Morning Time: 1 hour 30 minutes Additional materials (enclosed):

Math Final Exam Solutions

Math 10B: Mock Mid II. April 13, 2016

10.1 EXERCISES. y 2 t 2. y 1 t y t 3. y e

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Fractional Method of Characteristics for Fractional Partial Differential Equations

3, so θ = arccos

Chapter 13 Homework Answers

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

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

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

EE 301 Lab 2 Convolution

ECE 2100 Circuit Analysis

Theory of! Partial Differential Equations!

( ) 2. Review Exercise 2. cos θ 2 3 = = 2 tan. cos. 2 x = = x a. Since π π, = 2. sin = = 2+ = = cotx. 2 sin θ 2+

Transcription:

Elemenar Differenial Equaions and Boundar Value Problems Boce. & DiPrima 9 h Ediion Chaper 1: Inroducion 1006003 คณ ตศาสตร ว ศวกรรม 3 สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา 1/2555 ผศ.ดร.อร ญญา ผศ.ดร.สมศ กด วล ยร ชต 1

Topics Some Basic Mahemaical Models; Direcion Fields Soluions of Some Differenial Equaions Classificaion of Differenial Equaions 2

1.1 Basic Mahemaical Models; Direcion Fields Elemenar Differenial Equaions and Boundar Value Problems 9 h ediion b William E. Boce and Richard C. DiPrima 2009 b John Wile & Sons Inc. Differenial equaions are equaions conaining derivaives. The following are examples of phsical phenomena involving raes of change: Moion of fluids Moion of mechanical ssems Flow of curren in elecrical circuis Dissipaion of hea in solid objecs Seismic waves Populaion dnamics A differenial equaion ha describes a phsical process is ofen called a mahemaical model. 3

Some Applicaions of Differenial Equaion 4

Example 1: Free Fall Formulae a differenial equaion describing moion of an objec falling in he amosphere near sea level. Variables: ime veloci v Newon s 2 nd Law: F ma m(dv/d) ne force Force of gravi: F mg downward force Force of air resisance: F γ v upward force Then m dv d mg γ v Taking g 9.8 m/sec 2 m 10 kg γ 2 kg/sec we obain dv d 9.8 0.2v 5

v 9.8 0. 2v Example 2: Skeching Direcion Field (1 of 3) Using differenial equaion and able plo slopes (esimaes) on axes below. The resuling graph is called a direcion field. (Noe ha values of v do no depend on.) v v' 0 9.8 5 8.8 10 7.8 15 6.8 20 5.8 25 4.8 30 3.8 35 2.8 40 1.8 45 0.8 50-0.2 55-1.2 60-2.2 6

Example 2: Direcion Field Using Maple (2 of 3) v 9.8 0. 2v Sample Maple commands for graphing a direcion field: wih(deools): DEplo(diff(v())9.8-v()/5v() 0..10v0..80sepsize.1colorblue); When graphing direcion fields be sure o use an appropriae window in order o displa all equilibrium soluions and relevan soluion behavior. 7

v 9.8 0. 2v Example 2: Direcion Field & Equilibrium Soluion (3 of 3) Arrows give angen lines o soluion curves and indicae where soln is increasing & decreasing (and b how much). Horizonal soluion curves are called equilibrium soluions. Use he graph below o solve for equilibrium soluion and hen deermine analicall b seing v' 0. Se v 0 : 9.8 0.2v 9.8 v 0.2 v 49 0 8

Equilibrium Soluions In general for a differenial equaion of he form a b find equilibrium soluions b seing ' 0 and solving for : ( ) b a Example: Find he equilibrium soluions of he following. 2 5 + 3 ( + 2) 9

Example 3: Mice and Owls (1 of 2) Consider a mouse populaion ha reproduces a a rae proporional o he curren populaion wih a rae consan equal o 0.5 mice/monh (assuming no owls presen). When owls are presen he ea he mice. Suppose ha he owls ea 15 per da (average). Wrie a differenial equaion describing mouse populaion in he presence of owls. (Assume ha here are 30 das in a monh.) Soluion: dp d 0.5 p 450 10

Example 5: Direcion Field (2 of 2) Discuss soluion curve behavior and find equilibrium soln. p 0.5 p 450 11

Seps in Consrucing Mahemaical Models Using Differenial Equaions 1. Idenif independen and dependen variables and assign leers o represen hem. 2. Choose he unis of measure for each variable. 3. Ariculae he basic principle ha underlies or governs he problem ou are invesigaing. This requires our being familiar wih he field in which he problem originaes. 4. Express he principle or law in he previous sep in erms of he variables idenified a he sar. This ma involve he use of inermediae variables relaed o he primar variables. 5. Make sure each erm of our equaion has he same phsical unis. 6. The resul ma involve one or more differenial equaions. 12

1.2 Soluions of Some Differenial Equaions Elemenar Differenial Equaions and Boundar Value Problems 9 h ediion b William E. Boce and Richard C. DiPrima 2009 b John Wile & Sons Inc. Recall he free fall and owl/mice differenial equaions: v 9.8 0.2v p 0.5 p 450 These equaions have he general form ' a - b We can use mehods of calculus o solve differenial equaions of his form. 13

Example 1: Mice and Owls (1 of 3) To solve he differenial equaion p 0.5 p 450 we use mehods of calculus as follows. dp d 0.5 ( p 900) dp / d p 900 0.5 p dp 900 0.5d ln p 900 0.5 + C p 900 e 0.5+ C p 900 ± e 0.5 e C p 900 + ke 0.5 k ± e C Thus he soluion is p 900 + ke 0.5 where k is a consan. 14

p 900 + ke 0.5 15

Example 1: Inegral Curves (2 of 3) Thus we have infiniel man soluions o our equaion p 0.5 p 450 p 900 + since k is an arbirar consan. 0.5 ke Graphs of soluions (inegral curves) for several values of k and direcion field for differenial equaion are given below. Choosing k 0 we obain he equilibrium soluion while for k 0 he soluions diverge from equilibrium soluion. 16

Example 1: Iniial Condiions (3 of 3) A differenial equaion ofen has infiniel man soluions. If a poin on he soluion curve is known such as an iniial condiion hen his deermines a unique soluion. In he mice/owl differenial equaion suppose we know ha he mice populaion sars ou a 850. Then p(0) 850 and p( ) 900 + ke 0.5 p(0) 850 900 + ke 0 50 k Soluion : p( ) 900 50e 0.5 17

Soluion o General Equaion To solve he general equaion a b we use mehods of calculus as follows. d d a ln b a b / a b / a ± e a + C Thus he general soluion is a e b a + ke a where k is a consan. C d / d b / a a b / a b / a + ke a d b / a e a+ C k ± e C a d 18

Iniial Value Problem Nex we solve he iniial value problem a b (0) From previous slide he soluion o differenial equaion is b + a a ke Using he iniial condiion o solve for k we obain b 0 b (0) 0 + ke k 0 a a and hence he soluion o he iniial value problem is 0 b a + 0 b e a a 19

Equilibrium Soluion To find he equilibrium soluion se ' 0 & solve for : se b a b 0 ( ) a From he previous slide our soluion o he iniial value problem is: b + a Noe he following soluion behavior: 0 If 0 b/a hen is consan wih () b/a If 0 > b/a and a > 0 hen increases exponeniall wihou bound If 0 > b/a and a < 0 hen decas exponeniall o b/a If 0 < b/a and a > 0 hen decreases exponeniall wihou bound If 0 < b/a and a < 0 hen increases asmpoicall o b/a b a a e 20

Example 2: Free Fall Equaion (1 of 3) อ างจาก slide5 Recall equaion modeling free fall descen of 10 kg objec assuming an air resisance coefficien γ 2 kg/sec: dv / d 9.8 0. 2v Suppose objec is dropped from 300 m. above ground. (a) Find veloci a an ime. (b) How long unil i his ground and how fas will i be moving hen? For par (a) we need o solve he iniial value problem v 9.8 0.2v v(0) 0 Using resul from previous slide we have b a + b a.2 ( e ) a 9.8 9.8.2 0 e v + 0 e v 49 1 0.2 0.2 21

Example 2: Graphs for Par (a) (2 of 3) The graph of he soluion found in par (a) along wih he direcion field for he differenial equaion is given below. v 9.8 0.2v v 49 1 (.2 e ) v(0) 0 22

Example 2 Par (b): Time and Speed of Impac (3 of 3) Nex given ha he objec is dropped from 300 m. above ground how long will i ake o hi ground and how fas will i be moving a impac? Soluion: Le s() disance objec has fallen a ime. I follows from our soluion v() ha s ( ) s(0) v( ) 0 49 49e C 245.2 s( ) s( ) Le T be he ime of impac. Then s( T ) 49T + 245e.2T 245 300 49 49 Using a solver T 10.51 sec hence 0.2(10.51) v(10.51) 49 1 e 43.01 ( ) f/sec + 245e + 245e.2.2 + C 245 23

1.3: Classificaion of Differenial Equaions Elemenar Differenial Equaions and Boundar Value Problems 9 h ediion b William E. Boce and Richard C. DiPrima 2009 b John Wile & Sons Inc. The main purpose of his course is o discuss properies of soluions of differenial equaions and o presen mehods of finding soluions or approximaing hem. To provide a framework for his discussion in his secion we give several was of classifing differenial equaions. 24

Ordinar Differenial Equaions When he unknown funcion depends on a single independen variable onl ordinar derivaives appear in he equaion. In his case he equaion is said o be an ordinar differenial equaions (ODE). The equaions discussed in he preceding wo secions are ordinar differenial equaions. For example dv d dp 9.8 0.2v 0.5 p 450 d 25

Parial Differenial Equaions When he unknown funcion depends on several independen variables parial derivaives appear in he equaion. In his case he equaion is said o be a parial differenial equaion (PDE). Examples: (wave equaion) ) ( ) ( (hea equaion) ) ( ) ( 2 2 2 2 2 2 2 2 2 x u x x u a x u x x u α 26

Ssems of Differenial Equaions Anoher classificaion of differenial equaions depends on he number of unknown funcions ha are involved. If here is a single unknown funcion o be found hen one equaion is sufficien. If here are wo or more unknown funcions hen a ssem of equaions is required. For example predaor-pre equaions have he form du / d a u α uv dv / d cv + γ uv where u() and v() are he respecive populaions of pre and predaor species. The consans a c α γ depend on he paricular species being sudied. Ssems of equaions are discussed in Chaper 7. 27

Order of Differenial Equaions The order of a differenial equaion is he order of he highes derivaive ha appears in he equaion. Examples: + 3 0 + 3 2 4 2 d d + 1 e 4 2 d d u + u sin xx 0 We will be suding differenial equaions for which he highes derivaive can be isolaed: ( n) ( ) f 2 ( ( n 1) ) 28

Linear & Nonlinear Differenial Equaions An ordinar differenial equaion ( n) F is linear if F is linear in he variables ( n) Thus he general linear ODE has he form Example: Deermine wheher he equaions below are linear or nonlinear. (1) + 3 0 4 2 d d (4) 4 2 d d ( ) 0 ( n) ( n 1) a0( ) + a1( ) + + a ( ) g( ) + 1 2 (2) (5) + 3e u xx + uu 2 n sin 0 (3) (6) + 3 2 u xx 2 + sin( u) u 0 cos 29

Soluions o Differenial Equaions A soluion φ() o an ordinar differenial equaion saisfies he equaion: Example: Verif he following soluions of he ODE sin 2 ) ( cos ) ( sin ) ( ; 0 3 2 1 + ( ) 1) ( ) ( ) ( n n f ( ) 1) ( ) ( ) ( n n f φ φ φ φ φ 30

Soluions o Differenial Equaions Three imporan quesions in he sud of differenial equaions: Is here a soluion? (Exisence) If here is a soluion is i unique? (Uniqueness) If here is a soluion how do we find i? (Analical Soluion Numerical Approximaion ec) 31