MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du.

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

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

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k

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.

Chapter 2. First Order Scalar Equations

Chapter 7: Solving Trig Equations

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

Math 106: Review for Final Exam, Part II. (x x 0 ) 2 = !

Week #13 - Integration by Parts & Numerical Integration Section 7.2

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

MATH 31B: MIDTERM 2 REVIEW. sin 2 x = 1 cos(2x) dx = x 2 sin(2x) 4. + C = x 2. dx = x sin(2x) + C = x sin x cos x

ES.1803 Topic 22 Notes Jeremy Orloff

Solutions to Assignment 1

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

on the interval (x + 1) 0! x < ", where x represents feet from the first fence post. How many square feet of fence had to be painted?

( ) 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+

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

6.003 Homework #8 Solutions

THE SINE INTEGRAL. x dt t

SOLUTIONS TO ECE 3084

Math 333 Problem Set #2 Solution 14 February 2003

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

ENGI 9420 Engineering Analysis Assignment 2 Solutions

10. State Space Methods

Exponential and Logarithmic Functions -- ANSWERS -- Logarithms Practice Diploma ANSWERS 1

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

15. Vector Valued Functions

CHAPTER. Forced Equations and Systems { } ( ) ( ) 8.1 The Laplace Transform and Its Inverse. Transforms from the Definition.

Unit Root Time Series. Univariate random walk

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

Section 7.4 Modeling Changing Amplitude and Midline

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Predator - Prey Model Trajectories and the nonlinear conservation law

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

ln 2 1 ln y x c y C x

Advanced Integration Techniques: Integration by Parts We may differentiate the product of two functions by using the product rule:

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

Math 334 Fall 2011 Homework 11 Solutions

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

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux

Sections 2.2 & 2.3 Limit of a Function and Limit Laws

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

4.6 One Dimensional Kinematics and Integration

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

-e x ( 0!x+1! ) -e x 0!x 2 +1!x+2! e t dt, the following expressions hold. t

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in

Instructor: Barry McQuarrie Page 1 of 5

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

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:

ME 391 Mechanical Engineering Analysis

Logarithms Practice Exam - ANSWERS

Final Spring 2007

Two Coupled Oscillators / Normal Modes

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180

LAPLACE TRANSFORM AND TRANSFER FUNCTION

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

Math 2214 Solution Test 1A Spring 2016

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

Chapter 4 The Fourier Series and Fourier Transform

Short Introduction to Fractional Calculus

THE BERNOULLI NUMBERS. t k. = lim. = lim = 1, d t B 1 = lim. 1+e t te t = lim t 0 (e t 1) 2. = lim = 1 2.

The Fundamental Theorems of Calculus

Mon Apr 9 EP 7.6 Convolutions and Laplace transforms. Announcements: Warm-up Exercise:

ME 452 Fourier Series and Fourier Transform

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

Some Basic Information about M-S-D Systems

Homework 2 Solutions

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

Second Order Linear Differential Equations

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff

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

e t dt e t dt = lim e t dt T (1 e T ) = 1

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016

System of Linear Differential Equations

Chapter 6. Laplace Transforms

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

Math 2214 Solution Test 1B Fall 2017

5.1 - Logarithms and Their Properties

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

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

( ) = 0.43 kj = 430 J. Solutions 9 1. Solutions to Miscellaneous Exercise 9 1. Let W = work done then 0.

Economics 8105 Macroeconomic Theory Recitation 6

Derivatives of Inverse Trig Functions

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

MOMENTUM CONSERVATION LAW

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

Operators related to the Jacobi setting, for all admissible parameter values

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

THE 2-BODY PROBLEM. FIGURE 1. A pair of ellipses sharing a common focus. (c,b) c+a ROBERT J. VANDERBEI

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

INDEX. Transient analysis 1 Initial Conditions 1

From Complex Fourier Series to Fourier Transforms

Undetermined coefficients for local fractional differential equations

Section 4.4 Logarithmic Properties

Continuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0.

DIFFERENTIAL EQUATIONS

3.6 Derivatives as Rates of Change

6.2 Transforms of Derivatives and Integrals.

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

Transcription:

MATH 3B: MIDTERM REVIEW JOE HUGHES. Inegraion by Pars. Evaluae 3 e. Soluion: Firs make he subsiuion u =. Then =, hence 3 e = e = ue u Now inegrae by pars o ge ue u = ue u e u + C and subsiue he definiion of u in o obain 3 e = [ e e ] + C. Evaluae ln(). Soluion: Inegrae by pars wih u() = ln() and v () =. Then ln() = ln() ln() = ln() ln Inegrae by pars a second ime, now wih u() = ln and v () =, o obain ln = ln + C ln() = ln() ln + + C 3. Evaluae sin( ). Soluion: Le u =. Then =, or = u. Thus sin( ) = u sin(u)

JOE HUGHES Now inegrae by pars wice o ge u sin(u) = u cos(u) + 4 u cos(u) = u cos(u) + 4u sin(u) 4 sin(u) = u cos(u) + 4u sin(u) + 4 cos(u) + C and plug back in u = o obain sin( ) = cos( ) + 4 sin( ) + 4 cos( ) + C. Evaluae sin 4 cos 3.. Trigonomeric Inegrals Soluion: The key idea for evaluaing rig inegrals wih odd powers of sine or cosine is o use he ideniy sin +cos = o ry o se up a subsiuion. In his case, we ge sin 4 cos 3 = sin 4 cos cos = sin 4 ( sin ) cos Now he inegral is wrien in a way ha makes a u-subsiuion possible. Le u = sin, so = cos. Then he inegral becomes u 4 ( u ) = u 4 u 6 = u5 5 u7 7 + C = sin5 sin7 + C 5 7. Evaluae an sec 4. Soluion: This inegral can also be solved wih a u-subsiuion. In his case he ideniy o remember is sec = + an, as well as he fac ha d an = sec. So an sec 4 = an sec sec = an ( + an ) sec Now le u = an, so = sec. Then he inegral becomes u( + u ) = u + u 3 = u + u4 4 + C = an + an4 + C 4. Evaluae 9. 3. Trig Subsiuions Soluion: Make he subsiuion = 3 sin θ, so ha = 3 cos θ dθ. Then 9 sin = θ 3 cos θ dθ = 9 sin θ dθ 9 3 cos θ = 9 [θ sin θ cos θ] + C

cos θ = MATH 3B: MIDTERM REVIEW 3 using a rigonomeric inegral (I hink you will be given he answer o inegrals like hese on he eam). Now θ = sin 3, sin θ = 3, and 9 3, so 9 = 9. Evaluae. [ sin 3 3 9 3 ] + C = 9 sin 3 9 + C Soluion: A firs glance, i doesn look like we can do a rig subsiuion. Bu observe ha ( 6) = + 36 hence = 36 ( 6) by aking u = 6. = = 36 ( 6) 36 u Now we can do a rig subsiuion: le u = 6 sin θ. Then = 6 cos θ dθ, hence 6 cos θ = 36 u 6 cos θ dθ = θ + C = u sin 6 + C = 6 sin + C 6. Evaluae ( ) ( 3). 4. Parial Fracions Soluion: The numeraor has degree less han he denominaor, so we can use parial fracions. Wrie ( ) ( 3) = A + A ( ) + B 3 Afer clearing denominaors, we ge = A ( )( 3) + A ( 3) + B( ) Now plug in = o obain = A, so A =. Similarly, if we plug in = 3 hen we ge = B. To deermine A, le s look a he coefficien of on boh sides. On he lef-hand side, his coefficien is zero, while on he righ-hand side he coefficien is A + B. A = B =. So our inegral becomes ( ) = ( 3) ( ) + = ln 3 ln + + C 3

4 JOE HUGHES. Evaluae 5 (+)( +). Soluion: When we do parial fracions wih an irrecible quadraic facor like +, he corresponding erm in he epansion should have a linear polynomial in he numeraor. So wrie 5 ( + )( + ) = A + + B + C + Now clear he denominaors o ge Ne, plug in = : or A =. 5 = A( + ) + (B + C)( + ) 5( ) = A(4 + ) To find B, look a he coefficien of. On he lef-hand side his coefficien is zero, while on he righ hand side i is A + B. B = A =. Finally, o find C we look a he consan coefficien on boh sides o ge = A + C, so C = A =. 5 ( + )( = + ) 3. Evaluae sec θ an θ dθ. + + + = + + + = ln + + ln( + ) + an () + C + + + Soluion: One migh be emped o ry o use he rig ideniy sec θ = + an θ, bu I don hink ha helps here. So insead le s sar wih a subsiuion: le u = an θ, so ha = sec θ dθ. Then sec θ an θ dθ = u = Now we can proceed using parial fracions. Wrie (u )(u + ) = A u + B u + and clear denominaors o obain = A(u + ) + B(u ) (u )(u + ) Plugging in u = gives = A, so A =. Similarly, plugging in u = gives B =. (u )(u + ) = u u + = ln u ln u + + C and plugging in u = an θ gives sec θ an θ dθ = ln an θ ln an θ + + C

4. Evaluae 3. MATH 3B: MIDTERM REVIEW 5 Soluion: Parial fracions won work on his inegral (a leas no righ away) because he degree of he numeraor is greaer han ha of he denominaor. So we need o sar wih long division. The easies approach is o noice ha boh he numeraor and denominaor are divisible by. 3 = ( )( + + ) = + + ( + ) + = = + ( )( + ) + + + and 3 = So we ended up no needing parial fracions a all. + = + ln + + C + 5. Improper Inegrals. Deermine wheher 7 8 converges, and if so, evaluae i: Soluion: The funcion 7 8 has an infinie disconinuiy a =, so his is an improper inegral. We can evaluae i using he limi definiion: [ ] = lim = lim 8 8 = lim 8 8a 8 = 8 a + a + a a + 7 8 7 8 a he inegral converges, and he value of he inegral is 8.. Deermine wheher e ln() converges, and if so, evaluae i. Soluion: u-subsiuions are valid for improper inegrals, so ake u = ln() o obain e ln() = lim R e ln() = lim [ ln(r) u = lim ln(r) u = lim = since ln(r) as R. he inegral converges, and is equal o. 3. Deermine wheher + ln(r) + ] converges or diverges. Soluion: for, hence + 3 and + 3 Using he limi definiion of improper inegrals, 3 = [ 3 lim ln() ] R 4 = 3 lim ln(r) = for.

6 JOE HUGHES 3 diverges, hence by he comparison es also diverges. 4. Deermine wheher converges or diverges. + e (+ ) Soluion: This inegral is improper no only because one of he limis is infinie, bu also because he inegrand has an infinie disconinuiy a zero. In a siuaion like his one, he firs sep should be o spli he inegral ino wo pieces: e (+ ) d = e (+ ) d d + e (+ ) For he second inegral, we can use he comparison es: for, and ( + ), so e (+ ) e and Since e d = lim e (+ ) R converges, he comparison es implies ha converges as well. e d e d = lim e R + e = e e (+ ) For he firs inegral, I hink i s easies o sar wih a subsiuion. If u =, hen = d, which can be rewrien as u = d. e (+ ) d = lim r + e (+ ) r r lim r + d e (u+u ) u d = lim r + e (u+u ) r u

Now as r +, R = r MATH 3B: MIDTERM REVIEW 7 ends o. So we can rewrie his as R lim e (u+u ) e (u+u ) = u u and we ve already shown ha his inegral converges. boh inegrals converge, so converges. 5. Deermine wheher π sin e (+ ) d converges or diverges. Soluion: Since sin() for all, he epression inside he absolue values is always negaive. since sin. Hence and since sin = (sin ) = sin sin π diverges by he p-inegral es, i follows from he comparison es ha also diverges. π sin