MA Study Guide #1

Similar documents
MA 366 Review - Test # 1

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

Math 2214 Solution Test 1A Spring 2016

1 st order ODE Initial Condition

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

Math 2214 Solution Test 1B Fall 2017

APPM 2360 Homework Solutions, Due June 10

Math 333 Problem Set #2 Solution 14 February 2003

Math Final Exam Solutions

Solutions to Assignment 1

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

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

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

Elementary Differential Equations and Boundary Value Problems

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

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

Some Basic Information about M-S-D Systems

Math 2214 Solution Test 1 B Spring 2016

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

3.6 Derivatives as Rates of Change

Differential Equations

ln 2 1 ln y x c y C x

EXERCISES FOR SECTION 1.5

AP CALCULUS AB/CALCULUS BC 2016 SCORING GUIDELINES. Question 1. 1 : estimate = = 120 liters/hr

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

Math 115 Final Exam December 14, 2017

Second-Order Differential Equations

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

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

Math 2214 Sol Test 2B Spring 2015

Second Order Linear 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

System of Linear Differential Equations

Section 3.8, Mechanical and Electrical Vibrations

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

Displacement ( x) x x x

KINEMATICS IN ONE DIMENSION

Second Order Linear Differential Equations

4.5 Constant Acceleration

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

Math 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm

Math 116 Second Midterm March 21, 2016

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

IB Physics Kinematics Worksheet

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Chapter 3 Kinematics in Two Dimensions

15. Vector Valued Functions

1.6. Slopes of Tangents and Instantaneous Rate of Change

Chapter 2. First Order Scalar Equations

ENV 6015 Solution to Mixing Problem Set

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

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

ME 391 Mechanical Engineering Analysis

8. Basic RL and RC Circuits

1998 Calculus AB Scoring Guidelines

UCLA: Math 3B Problem set 3 (solutions) Fall, 2018

x(m) t(sec ) Homework #2. Ph 231 Introductory Physics, Sp-03 Page 1 of 4

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

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

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

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.

Phys1112: DC 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.

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

04. Kinetics of a second order reaction

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis

LAPLACE TRANSFORM AND TRANSFER FUNCTION

Ordinary Differential Equations

AP Chemistry--Chapter 12: Chemical Kinetics

1. VELOCITY AND ACCELERATION

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18

Physics 221 Fall 2008 Homework #2 Solutions Ch. 2 Due Tues, Sept 9, 2008

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

University Physics with Modern Physics 14th Edition Young TEST BANK

Announcements: Warm-up Exercise:

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

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

CHEMICAL KINETICS: 1. Rate Order Rate law Rate constant Half-life Temperature Dependence

5.1 - Logarithms and Their Properties

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

Ordinary Differential Equations

Intermediate Differential Equations Review and Basic Ideas

Lecture 23 Damped Motion

MEI STRUCTURED MATHEMATICS 4758

DIFFERENTIAL EQUATIONS

Problem set 6: Solutions Math 207A, Fall x 0 2 x

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

UNIT #4 TEST REVIEW EXPONENTIAL AND LOGARITHMIC FUNCTIONS

) were both constant and we brought them from under the integral.

Basic Circuit Elements Professor J R Lucas November 2001

72 Calculus and Structures

MTH Feburary 2012 Final term PAPER SOLVED TODAY s Paper

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

Problem Set 7-7. dv V ln V = kt + C. 20. Assume that df/dt still equals = F RF. df dr = =

CHAPTER 12 DIRECT CURRENT CIRCUITS

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation

Transcription:

MA 66 Su Guide #1 (1) Special Tpes of Firs Order Equaions I. Firs Order Linear Equaion (FOL): + p() = g() Soluion : = 1 µ() [ ] µ()g() + C, where µ() = e p() II. Separable Equaion (SEP): dx = h(x) g() Soluion : 1 g() = h(x) dx (The soluion is usuall given implicil b he above formula. You ma ge addiional soluions from g() =. You mus check o see if here are exra soluions.) III. Homogeneous Equaion (HOM): dx = f(x, ), where f(x, ) = f(x, ) Soluion : Le v = x Subsiue hese ino dx. Hence = xv and dx = xdv dx + v. = f(x, ) o obain a Separable Equaion. IV. Exac Equaion (EXE): M(x, ) dx + N(x, ) =, where M = N x Soluion : Soluion = ϕ(x) given implicil b ψ(x, ) = C where : ψ x = M(x, ) = ψ = M(x, ) dx + h() ψ ψ = N(x, ) = = ( ) M(x, ) dx + h() = f(, ) has slope f(, ) a he poin (, ). The direcion field (or slope field) of he d.e. indicaes he slope of soluions a () Direcion Fields. A soluion = ϕ() o he d.e.

various poins (, ). The direcion field ma be used o give qualiaive informaion abou he behavior of soluions as (or, or, ec). Direcion fields ma also be used o approximae he inerval where a soluion hrough a poin (, ) is defined. (3) Applicaions of 1s Order Equaions. (A1) Mixing Problems : Q() = amoun of subsance in soluion a ime dq = Rae In Rae Ou = r ic i r o c o (A) Exponenial Growh/Deca : Q() = quani presen a ime dq = r Q (A3) Newon s Law of Cooling : T () = emperaure a ime dt = k (T T a) (T a = ambien emperaure) (A4) Falling & Rising Objecs : You should be able o se up and solve simple problems using Newon s nd Law: F = m dv. Near he surface of he Earh, he force due o gravi is he weigh of he objec F g = mg. Le F d = magniude of drag force. (a) For falling objecs, we usuall le he posiive direcion be he downward direcion so m dv = mg F d. (b) For rising objecs, le he posiive direcion be upward. For he upward porion of he fligh, m dv = mg F d ; while for he downward porion of he fligh, m dv = mg + F d. (a) Falling Bo (b) Rising Bo 11 1 1 F d m F = mg g + direcion F = mg g 11 1 1 m F d (i) rising par + direcion F = mg g 11 1 1 F d m (ii) falling par

(4) Exisence and Uniqueness Theorems for 1 s Order Equaions. (a) THEOREM (Firs Order Linear). If p() and g() are coninuous on an inerval { α < < β conaining, hen he IVP + p() = g() has a unique soluion ( ) = = ϕ() on he inerval α < < β, for an. Noe: The larges such open inerval conaining is where he soluion = ϕ() is guaraneed o exis. (b) THEOREM (Firs Order Nonlinear). If f(, ) and f are coninuous in some recangle R: { α < < β, and γ < < δ and (, ) lies inside he recangle R, hen he IVP = f(, ) has a unique soluion on he inerval ( ) = h < < + h, for some number h >. Noe: The number h is no eas o find. The inerval conaining where soluion exiss can be esimaed b looking a he direcion field of he differenial equaion. To deermine he exac inerval, ou mus solve he IVP explicil for. (5) Auonomous Equaions: Equaions of he form = F () ( ) are said o be auonomous since does no depend on he independen variable. Such equaions can have consan soluions (i.e., = K) which are called equilibrium soluions. These soluions are found b solving F () =. (These are also called criical poins.) You should be able o find all equilibrium soluions o he auonomous d.e. ( ) and skech nonequilibrium soluions using he phase line of he differenial equaion ( ). You should also be able o classif he sabili of he equilibrium soluions as follows: (a) Asmpoicall Sable - Soluions which sar near = K will alwas approach = K as : = K (b) Asmpoicall Unsable - Soluions which sar near = K does no alwas approach = K as : = K

(c) Semisable - This is a special pe of unsable soluion. In his case soluions on one side of = K will approach = K as, while soluions on he oher side of = K will approach somehing else: = K Remark. To skech non-equilibrium soluions of ( ), ou do no necessaril need direcion fields, ou can use ordinar calculus. Since = F (), he graph of F () vs will deermine where he soluion = ϕ() is increasing (F () > ) or decreasing (F () < ). B he Chain d df () Rule, = F (), hence a graph of df F will deermine where he soluion = ϕ() is concave up (F F > ) or concave down (F F < ). = f(, ) (6) Euler (Tangen Line) Mehod. Approximae acual soluion ϕ() o ( ) = using he Euler (Tangen Line) Mehod : n = n 1 + h f( n 1, n 1 ) where h = sep size. A each ieraion, k ϕ( k ), where k = + hk. (7) Second Order Linear Homogeneous wih Equaions Consan Coefficiens. The differenial equaion a + b + c = has Characerisic Equaion ar + br + c =. Call he roos r 1 and r. The general soluion o a + b + c = is as follows: (a) If r 1, r are real and disinc = C 1 e r 1 + C e r (b) If r 1 = λ + iµ (hence r = λ iµ) = C 1 e λ cos µ + C e λ sin µ (c) If r 1 = r (repeaed roos) = C 1 e r 1 + C e r 1 (8) Theor of nd Linear Order Equaions. The Wronskian is defined as 1 () W ( 1, )() = 1() () () (a) The funcions 1 () and () are linearl independen over a < < b if W ( 1, ) for a leas one poin in he inerval. (b) THEOREM (Exisence & Uniqueness) If p(), q() and g() are coninuous in an + p() + q() = g() open inerval a < < b conaining, hen he IVP ( ) = ( ) = 1 has a unique soluion = ϕ() defined in he open inerval a < < b..

(c) Superposiion Principle If 1 () and () are soluions o he nd order linear homogeneous equaion P () + Q() + R() = over he inerval a < < b, hen = C 1 1 () + C () is also a soluion for an consans C 1 and C. (d) THEOREM (Homogeneous) If 1 () and () are soluions o he linear homogeneous equaion P () + Q() + R() = in some inerval I and W ( 1, ) for some 1 in I, hen he general soluion is c () = C 1 1 () + C (). This is usuall called he complemenar soluion and we sa ha 1 (), () form a Fundamenal Se of Soluions (FSS) o he differenial equaion. (e) THEOREM (Nonhomogeneous) The general soluion o he nonhomogeneous equaion P () + Q() + R() = G() is () = c () + p (), where c () = C 1 1 () + C () is he general soluion o he corresponding homogeneous equaion P () +Q() +R() = and p () is a paricular soluion o he nonhomogeneous equaion P () + Q() + R() = G(). (f) Useful Remark : If p1 () is a paricular soluion of P () + Q() + R() = G 1 () and if p () is a paricular soluion of P () + Q() + R() = G (), hen p () = p1 () + p () is a paricular soluion of P () + Q() + R() = [G 1 () + G ()]. Pracice Problems 1. Deermine he order of each of hese differenial equaions; also sae wheher he equaion is linear or nonlinear: (a) + x = 1 (b) x + = 1 (c) ( ) 3 + = 1 (d) + = 1. (a) Which of he funcions 1 () = and () = is/are soluions of he IVP =, () =? (b) Which of he funcions 1 () = and () = are is/soluions of he IVP =, (1) = 1? 3. For wha value(s) of r is = e rx a soluion of 5 + 6 =? 4. (a) Show ha = x 3 is a soluion of he iniial value problem = 3 /3, () =. (b) Find a differen soluion of he iniial value problem. 5. Find an explici soluion of he iniial value problem x =, (1) = 1. Indicae he inerval in which he soluion is valid. 6. (a) Find an implici soluion of he iniial value problem = x, () =. + 1 (b) Find an explici soluion of he iniial value problem = x, () =. + 1 7. For wha value(s) of a is he soluion of he IVP + e =, () = a bounded on he inerval? 8. Deermine wheher each of he following differenial equaions is linear, separable, homogeneous, and/or exac or none of hese. (a) x + + (x + 3) dx = (b) x + 3 + (x + ) dx =

(c) (x + 3 + 1)dx + (x + + 1) = (e) ( + 1) + (x + 1)dx = (d) x + 1 + (x + 1) dx = 9. Find implici soluions o (a) x + x = (b) (1 + ) dx x = (c) x + + x = 1. Find an implici form of he general soluion of he differenial equaion dx = x +. x 11. Find an implici soluion of he IVP x + 1 + (x + ) =, (1) = 1. dx 1. If x + (x + 1) = xe x and (1) =, hen () =? 13. Use he given direcion field o skech he soluion of he corresponding iniial value problem = f(, ), ( ) = for he indicaed iniial value (, ) : (a) (, ) (b) (, ) (c) ( 1, 3) (d) (, 4) 14. For each of he iniial value problems deermine he larges inerval for which a unique soluion is guaraneed : (a) = 1, (1) = (b) + (an ) = sec, () = (c) + x x 9 = 1 x, () = 1 (d) (x + 4) x = 1 x, ( ) = 1 15. For each of he iniial value problems deermine all iniial poins (, ) for which a unique soluion is guaraneed in some inerval h < < + h: (a) = +, ( ) = (b) = /, ( ) = (c) = +, ( ) = 1 (d) = 1/3 + 1/3, ( ) = (e) =, ( ) = 16. Find he explici soluion of he iniial value problem = 1, () =. Where is his soluion defined?

17. Suppose is proporional o, () = 4, and () =. Se up and solve an iniial value problem ha gives in erms of. For wha value of does () = 3? 18. A hermomeer reads 36 when i is moved ino a 7 room. Five minues laer he hermomeer reads 5. Se up and solve an iniial value problem ha gives he hermomeer reading minues afer i is moved ino he room. Wha will i read en minues afer i is moved ino he room? 19. A ime = a 5 gallon ank conains 4 pounds of sal mixed in 1 gallons of waer. A soluion ha conains 3 lb of sal per gallon of soluion is hen pumped ino he ank a a consan rae of 5 gal/min. The well-sirred mixure flows ou of he ank a he rae of 3 gal/min. Se up and solve an iniial value problem ha gives he amoun of sal in he ank afer minues. Wha is he concenraion of sal in he ank a he ime he ank becomes full?. A huge 3 gallon radiaor is full of a 6% anifreeze soluion. Pure waer is poured in a a rae of 5 gal/min and he sirred mixure is drained a he same rae. How long do we pour waer ino he radiaor o ge a 5% anifreeze soluion? 1. Se up and solve an iniial value problem ha gives he verical veloci of a 18-lb parachuis seconds afer she jumps from an airplane ha is fling horizonall a an aliude of 5 fee. Assume ha air resisance is eigh imes he speed and ignore horizonal moion and downward direcion is posiive.. Consider he differenial equaion (a) Wha are he equilibrium soluions? = ( ). (b) Which equilibrium soluions are sable/unsable? (c) Skech he graph of he soluion of he differenial equaion for wih each of he iniial values () = /3, () =, () = /3, () = 4/3, () =, () = 8/3. (d) Find he explici soluion of he iniial value problem = ( ), () =. (e) For wha values of is he soluion in (d) valid? 3. Consider he differenial equaion = F (), w w = F ( ) 1 1 3 where he graph of F () is indicaed below. (a) Wha are he equlibrium soluions? (b) Which equilibrium soluions are sable? (c) Skech some soluions o = F (). 4. Esimae he soluion a = 1.5 o he IVP = 5, (1) = using he Euler Mehod wih h =.5. Wha is he rue soluion a = 1.5? 5. Find he general soluion o (a) 4 + 4 = (b) + 4 + 5 =. = 6. For wha value of α will he soluion o he IVP () = α saisf as? () = 7. Find he larges open inerval guaraneed b he Exisence and Uniqueness Theorem for which he iniial value problem 3x + + 1 x = 1 x 3, (1) = 3, (1) =, has a unique soluion.

Answers (1) (a) 1 s order nonlinear (b) 1 s order linear (c) 1 s order nonlinear (d) 3 rd order linear () (a) 1 and (b) 1 onl (3) r =, r = 3 (4) (a) = 3x = 3(x 3 ) /3 = 3 /3 ; = 3() /3 (b) (5) = x x + 1, x > 1 (6) (a) + = x (b) = 1 + 4x + 1 HOME (7) a = 1 (8) (a) HOME and EXE (b) (c) none of hese pes (d) FOL and EXE (e) SEP and EXE (9) (a) (HOME) ln 1 ( x ) = ln x + C and = x and = x (b) (SEP) + 1 = Cx (c) (EXE) x + x = C (1) 1 ( ) = ln x + C (11) x + x + = 1 x (1) () = 3 e (13) See below : (14) (a) > (b) π < < π (c) 3 < x < (d) 4 < x < (15) (a) all (, ) (b) all (, ) wih (c) all (, ) (, ) (d) all (, ) wih (e) all (, ) where 1 < < 1 and (16) = 1 + 3ex 1 3e, soluion defined for 1 ln 3 < x <. x (17) (18) (19) = k () = 4 () = T = k(t 7) T () = 36 T (5) = 5 Q = 15 Q() = 4 ; = 4e (ln.5)/, = 3Q 1 + ln.75 ln.5.83 ; T = 7 34e (ln(1/17))/5, T (1) 58. ; Q = 3(1+) 6, (1+) 3/, Q() 5.95 lbs/gal

() If Q() = # gals of anifreeze, hen Q = Q, Q() = 18 and so Q() = 18e 6. newline 6 Hence = 6 ln 5 1.94 minues 6 4 dv = 18 8v (1) ; v = 16(1 e ) v() = () (a) = and = (b) = is sable, = is unsable (c) See below (d) = (e) The soluion is valid for all if ( )e. If > or <, he soluion is valid onl for < < 1 ( ) ln. (3) (a) = 1 and = 3 (b) onl = 1 is sable (c) See below (4) =.375, rue soluion ϕ(1.5) = 1 5 (13 58 e.5 ).396 (c) 1 3 (c) 3 1 1 (5) (a) = C 1 e + C e (b) = C 1 e cos + C e sin (6) α = (7) < x <