Boyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors

Similar documents
Elementary Differential Equations and Boundary Value Problems

Let s look again at the first order linear differential equation we are attempting to solve, in its standard form:

2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues

DE Dr. M. Sakalli

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

EXERCISE - 01 CHECK YOUR GRASP

S.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]

Midterm exam 2, April 7, 2009 (solutions)

Transfer function and the Laplace transformation

Spring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review

CSE 245: Computer Aided Circuit Simulation and Verification

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule

Wave Equation (2 Week)

REPETITION before the exam PART 2, Transform Methods. Laplace transforms: τ dτ. L1. Derive the formulas : L2. Find the Laplace transform F(s) if.

Lecture 4: Laplace Transforms

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

Instructors Solution for Assignment 3 Chapter 3: Time Domain Analysis of LTIC Systems

Copyright 2012 Pearson Education, Inc. Publishing as Prentice Hall.

3.4 Repeated Roots; Reduction of Order

Math 3301 Homework Set 6 Solutions 10 Points. = +. The guess for the particular P ( ) ( ) ( ) ( ) ( ) ( ) ( ) cos 2 t : 4D= 2

Charging of capacitor through inductor and resistor

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018

whereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas

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.

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 )

fiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES MATEMATICAL PHYSICS SOLUTIONS are

On General Solutions of First-Order Nonlinear Matrix and Scalar Ordinary Differential Equations

46. Let y = ln r. Then dy = dr, and so. = [ sin (ln r) cos (ln r)

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline.

Math 266, Practice Midterm Exam 2

EE 350 Signals and Systems Spring 2005 Sample Exam #2 - Solutions

Lecture 2: Current in RC circuit D.K.Pandey

ln 2 1 ln y x c y C x

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument

( ) ( ) + = ( ) + ( )

General Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract

CHAPTER. Linear Systems of Differential Equations. 6.1 Theory of Linear DE Systems. ! Nullcline Sketching. Equilibrium (unstable) at (0, 0)

Chapter 6 Differential Equations and Mathematical Modeling

Math 2214 Solution Test 1B Fall 2017

A THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER

y = (y 1)*(y 3) t

UNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS

5. An object moving along an x-coordinate axis with its scale measured in meters has a velocity of 6t

H is equal to the surface current J S

Lecture 1: Growth and decay of current in RL circuit. Growth of current in LR Circuit. D.K.Pandey

Solutions from Chapter 9.1 and 9.2

Voltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!

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

Control System Engineering (EE301T) Assignment: 2

Chap.3 Laplace Transform

t + t sin t t cos t sin t. t cos t sin t dt t 2 = exp 2 log t log(t cos t sin t) = Multiplying by this factor and then integrating, we conclude that

Boyce/DiPrima/Meade 11 th ed, Ch 6.1: Definition of Laplace Transform

Chapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System

Ministry of Education and Science of Ukraine National Technical University Ukraine "Igor Sikorsky Kiev Polytechnic Institute"

Differential Equations

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

On the Speed of Heat Wave. Mihály Makai

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

ME 391 Mechanical Engineering Analysis

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

Elementary Differential Equations and Boundary Value Problems

Chapter 2. First Order Scalar Equations

Review Lecture 5. The source-free R-C/R-L circuit Step response of an RC/RL circuit. The time constant = RC The final capacitor voltage v( )

Chapter 12 Introduction To The Laplace Transform

Math 36. Rumbos Spring Solutions to Assignment #6. 1. Suppose the growth of a population is governed by the differential equation.

Continous system: differential equations

FIRST-ORDER SYSTEMS OF ORDINARY DIFFERENTIAL EQUATIONS I: Introduction and Linear Systems

Double Slits in Space and Time

MEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control

Logistic equation of Human population growth (generalization to the case of reactive environment).

Chapter 2 The Derivative Business Calculus 99

Chapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

LaPlace Transform in Circuit Analysis

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

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

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT

Note: For all questions, answer (E) NOTA means none of the above answers is correct.

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 11

Some Basic Information about M-S-D Systems

MA Study Guide #1

Why Laplace transforms?

Applied Statistics and Probability for Engineers, 6 th edition October 17, 2016

System of Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations

APPM 2360 Homework Solutions, Due June 10

Chapter 6 Test December 9, 2008 Name

A HAMILTON-JACOBI TREATMENT OF DISSIPATIVE SYSTEMS

MATH 308: Diff Eqs, BDP10 EXAMPLES [Belmonte, 2019] 1 Introduction 1.1 Basic Mathematical Models; Direction Fields

Theory of! Partial Differential Equations!

EEEB113 CIRCUIT ANALYSIS I

Final Exam : Solutions

Chapter 7 Response of First-order RL and RC Circuits

( ) 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+

Institute of Actuaries of India

Part I: Short Answer [50 points] For each of the following, give a short answer (2-3 sentences, or a formula). [5 points each]

20. Applications of the Genetic-Drift Model

Circuits and Systems I

Transcription:

Boc/DiPrima 9 h d, Ch.: Linar Equaions; Mhod of Ingraing Facors Elmnar Diffrnial Equaions and Boundar Valu Problms, 9 h diion, b William E. Boc and Richard C. DiPrima, 009 b John Wil & Sons, Inc. A linar firs ordr ODE has h gnral form d d f, whr f is linar in. Exampls includ quaions wih consan cofficins, such as hos in Chapr, a b or quaions wih variabl cofficins: d d p g

Consan Cofficin Cas For a firs ordr linar quaion wih consan cofficins, a b, rcall ha w can us mhods of calculus o solv: d / d a b / a d b / a ln b / a a C b / a k a a d, k ± C

Variabl Cofficin Cas: Mhod of Ingraing Facors W nx considr linar firs ordr ODEs wih variabl cofficins: d d p g Th mhod of ingraing facors involvs mulipling his quaion b a funcion, chosn so ha h rsuling quaion is asil ingrad.

Exampl : Ingraing Facor of Considr h following quaion: /3 Mulipling boh sids b, w obain W will choos so ha lf sid is drivaiv of known quani. Considr h following, and rcall produc rul: Choos so ha d d d d d d d d [ ] / /3

Exampl : Gnral Soluion of Wih /, w solv h original quaion as follows: [ ] gnral soluion : / /3 / 6 5 / / 6 5 / / 6 5 / / /3 5 3 5 3 C C d d d d 3 4 5 6-3 HL / /3 5 3 Sampl Soluions : C

Mhod of Ingraing Facors: Variabl Righ Sid In gnral, for variabl righ sid g, h soluion can b found as follows: a g a d d a d d [ ] a d d a a a g a a a a g g d a g g d C a

Exampl : Gnral Soluion of W can solv h following quaion using h formula drivd on h prvious slid: Ingraing b pars, Thus 4 a a a g d C 4 d 7 4 4 d 4 7 4 /5 C 7 4 d C C d d

4 Exampl : Graphs of Soluions of Th graph shows h dircion fild along wih svral ingral curvs. If w s C 0, h xponnial rm drops ou and ou should noic how h soluion in ha cas, hrough h poin 0, -7/4, sparas h soluions ino hos ha grow xponniall in h posiiv dircion from hos ha grow xponniall in h ngaiv dircion.. 7 4 0 C 0.5.0.5.0 - HL - -3-4

Mhod of Ingraing Facors for Gnral Firs Ordr Linar Equaion Nx, w considr h gnral firs ordr linar quaion p g Mulipling boh sids b, w obain d p g d Nx, w wan such ha ' p, from which i will follow ha d d d d [ ] p

Ingraing Facor for Gnral Firs Ordr Linar Equaion Thus w wan o choos such ha ' p. Assuming > 0, i follows ha d p d p d ln k Choosing k 0, w hn hav p d, and no > 0 as dsird.

Soluion for Gnral Firs Ordr Linar Equaion Thus w hav h following: Thn d p g p d d g p whr, [ ] d p c d g c d g g d d whr,

Exampl 3: Gnral Soluion of To solv h iniial valu problm firs pu ino sandard form: Thn and hnc 4, 4, for, 0 p d d ln ln g d C 4 d C [ ] 3 C 4 d C

Exampl 3: Paricular Soluion of Using h iniial condiion and gnral soluion C, C C i follows ha Th graphs blow show soluion curvs for h diffrnial quaion, including a paricular soluion whos graph conains h iniial poin,. Noic ha whn C0, w g h parabolic soluion shown and ha soluion sparas h soluions ino hos ha ar asmpoic o h posiiv vrsus ngaiv -axis. 4, 4 3, - - - - 5, C

Exampl 4: A Soluion in Ingral Form of To solv h iniial valu problm firs pu ino sandard form: Thn and hnc 0,, d p d s ds C 0 0 s 4 ds C

Exampl 4: A Soluion in Ingral Form of Noic ha his soluion mus b lf in h form of an ingral, sinc hr is no closd form for h ingral. 0 s Using sofwar such as Mahmaica or Mapl, w can approxima h soluion for h givn iniial condiions as HL wll as for ohr iniial 3 condiions. Svral soluion curvs ar shown. 3 4 5 6 ds C - - -3 0,, 0 s ds C