a. Show that these lines intersect by finding the point of intersection. b. Find an equation for the plane containing these lines.

Similar documents
AP Calculus BC Chapter 10 Part 1 AP Exam Problems

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

3, so θ = arccos

Answers to 1 Homework

Math 221: Mathematical Notation

Parametrics and Vectors (BC Only)

15. Vector Valued Functions

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

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

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

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

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

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

(π 3)k. f(t) = 1 π 3 sin(t)

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

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

Roller-Coaster Coordinate System

Applications of the Basic Equations Chapter 3. Paul A. Ullrich

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 Let. 1) k be a vector-valued function. (a) Evaluate f (0). (b) What is the domain of f () t? (c) Is f () t continuous at t = 1?

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs.

1. VELOCITY AND ACCELERATION

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

Math 116 Practice for Exam 2

Trajectory planning in Cartesian space

Kinematics in two dimensions

Traveling Waves. Chapter Introduction

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

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

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

Check in: 1 If m = 2(x + 1) and n = find y when. b y = 2m n 2

Starting from a familiar curve

KINEMATICS IN ONE DIMENSION

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Midterm Exam Review Questions Free Response Non Calculator

Welcome Back to Physics 215!

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3

Applicable Mathematics 2A

Some Basic Information about M-S-D Systems

Chapter 3 Kinematics in Two Dimensions

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

Effects of Coordinate Curvature on Integration

IB Physics Kinematics Worksheet

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

Solutions from Chapter 9.1 and 9.2

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a

AP CALCULUS BC 2016 SCORING GUIDELINES

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

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

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

Vector Calculus. Chapter 2

Ch.1. Group Work Units. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

Chapter 7: Solving Trig Equations

Homework 2: Kinematics and Dynamics of Particles Due Friday Feb 8, 2019

One-Dimensional Kinematics

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

Numerical Dispersion

Math 116 Second Midterm March 21, 2016

Distance Between Two Ellipses in 3D

Echocardiography Project and Finite Fourier Series

Solution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration

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

THE SINE INTEGRAL. x dt t

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

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum

2002 November 14 Exam III Physics 191

AP Calculus BC 2004 Free-Response Questions Form B

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Homework sheet Exercises done during the lecture of March 12, 2014

LAB # 2 - Equilibrium (static)

Displacement ( x) x x x

Mat 267 Engineering Calculus III Updated on 04/30/ x 4y 4z 8x 16y / 4 0. x y z x y. 4x 4y 4z 24x 16y 8z.

Integration Over Manifolds with Variable Coordinate Density

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

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

Constant Acceleration

k 1 k 2 x (1) x 2 = k 1 x 1 = k 2 k 1 +k 2 x (2) x k series x (3) k 2 x 2 = k 1 k 2 = k 1+k 2 = 1 k k 2 k series

Math 2214 Solution Test 1A Spring 2016

SPH3U1 Lesson 03 Kinematics

University Physics with Modern Physics 14th Edition Young TEST BANK

Maxwell s Equations and Electromagnetic Waves

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

BEng (Hons) Telecommunications. Examinations for / Semester 2

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

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should

CHAPTER 2: Mathematics for Microeconomics

Let us start with a two dimensional case. We consider a vector ( x,

MEI STRUCTURED MATHEMATICS 4758

Suggested Practice Problems (set #2) for the Physics Placement Test

DIFFERENTIAL GEOMETRY HW 5

NEWTON S SECOND LAW OF MOTION

Name: Total Points: Multiple choice questions [120 points]

Position, Velocity, and Acceleration

Review Exercises for Chapter 3

Chapter 11. Parametric, Vector, and Polar Functions. aπ for any integer n. Section 11.1 Parametric Functions (pp ) cot

Lecture 10: Wave equation, solution by spherical means

Differential Geometry: Revisiting Curvatures

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

Transcription:

Mah A Final Eam Problems for onsideraion. Show all work for credi. Be sure o show wha you know. Given poins A(,,, B(,,, (,, 4 and (,,, find he volume of he parallelepiped wih adjacen edges AB, A, and A. Hin: The volume of he parallelepiped deermined by vecors abc,, is he riple produc, a ( b c.. onsider he lines r ( = +,+ 4,5+ 6 and r ( = 4 5,+,+ 7. a. Show ha hese lines inersec by finding he poin of inersecion. b. Find an equaion for he plane conaining hese lines. = =. Give an approimae formula for he small change Δz ha resuls from small ln. Le z y ( e y changes Δ and Δ y in he values of and y. Use his o approimae he value of.99.. 4. The figure a righ is he conour plo of a funcion of wo variables, f ( y,, for and y ranging from o. The scale is uni = 5 cm; spacing beween conour levels is. a. Use he conour plo o deermine wheher f and f y are >, =, or < a (,.5 and (.,.6. b. The funcion ploed on he figure is f ( y, = y + y 4 +. alculae he acual values of he parial derivaives a (,.5 and (.,.6. c. In he diagram, here are hree places where he angen plane is horizonal. Find he eac coordinaes of each of hese and characerize each as a ma, a min or neiher. / 5. onsider he curve r( = cos,sin, a. Find he lengh of he curve from b. Find he curvaure as a funcion of. c. Find he angenial and normal componens of he acceleraion. 6. onsider (,, g y z = + yz a. Find a uni vecor in he direcion from (,, in which g decreases mos rapidly. b. Find a parameerizaion of he line from ha poin in he direcion of mos rapid decrease. 7. Le f ( y, = y + + yand g(, y y minimum and maimum values, if hey eis, of f ( y, subjec o he consrain =. Use he mehod of Lagrange mulipliers o find he g, y = wih >. In he case ha hey do eis, idenify all of he poins (, y a which hese values are aained. 8. Find he area of he par of he saddle z = y ha lies inside he cylinder + y = 4.

9. Le f ( y, y y = +, and be y =, beween (, and (,, direced upwards. a. alculae F = f. b. alculae he inegral F dr hree differen ways: i. direcly; ii. by using pah-independence o replace by a simpler pah. iii. by using he Fundamenal Theorem for line inegrals.. Verify Green s heorem in he normal form, i.e. F nds ˆ = div (, sides and showing hey are equal if and (,. F =, y. Verify Sokes heorem for he paraboloid z = 6 y for z and he vecor field F = y,4 z, 6. You may find i convenien o use polar coordinaes o evaluae he surface inegral of he curl. F y da, by calculaing boh and is he square wih opposie verices a (,. Use he divergence heorem o calculae dv where V is he region bounded by he cone z y How abou F =,, = + and he plane z =. To do his, you will need a simple field whose divergence is `.? Hin: You can parameerize he cone by r, θ = cos θ, sin θ,.. The posiion of a paricle moving in he plane a is given by r( =, + + a. Find he velociy of he paricle a ime. b. Find he speed of he paricle a ime. c. Wha is he paricle s highes speed and when does ha occur?. 4. Find equaions of he normal plane and he osculaing plane for he curve r( =,, a (,, θ θ R = cos d, sin d a. Show ha he arc lengh along he curve from R o R( θ is θ. b. Find he curvaure a θ. 5. onsider he curve ( θ

yz 6. Find he direcion in which f ( yz,, = e increases mos rapidly a he poin Wha is he maimum rae of increase? 7. Find he minimum value of f ( y, / e ( y f fyy fy > o verify his.,,. = + and use he second derivaive es: 8. escribe and skech a graph for he solid whose volume is given by he following inegral: ρ sinφdρdφdθ and evaluae he inegral. 5 /6 9. Using cylindrical coordinaes, se up an inegral for he volume under he paraboloid z above he disc r cosθ.. Find he work done by he force field F( y z r( = sin,cos, for.,, = y, z, F, y, z =, y, z. Verify Soke s heorem for he vecor field paraboloid = above he y-plane. z y F, y, z zan y, z ln, z. Le = ( + paraboloid = r and in moving a paricle along he heli where S is he par of he. Find he flu of F across he par of he z = + y ha lies below he plane z = and is oriened upwards.

Mah A Final EamSoluions Fall. Given poins A(,,, B(,,, (,, 4 and (,,, find he volume of he parallelepiped wih adjacen edges AB, A, and A. Hin: The volume of he parallelepiped deermined by vecors abc,, is he riple produc, a ( b c. SOLN: Take a = AB=,,, b = A =,, and c = A=,, so ha a ( b c =,, 8,, 5 = 8 + 5 = 6. onsider he lines r ( = +,+ 4,5+ 6 and r ( = 4 5,+,+ 7. a. Show ha hese lines inersec by finding he poin of inersecion. SOLN: r( = r =,7, b. Find an equaion for he plane conaining hese lines. SOLN: Take one vecor along r ; r r( = 5,,7,7, =,4,6 =,, and anoher along r : r r = 7,,,7, = 4,,, whence a normal o he plane is given by 4,,,, = 5,,5 = 5,,, so ha he equaion of he plane is y+ z = = =. Give an approimae formula for he small change Δz ha resuls from small changes Δ and Δ y in he values of and y. Use his o approimae he value of.99.. yln z y yln y SOLN: z = e, so e y z = = and = yln y ( ln e = ln. Thus, near a poin y y y (, y, wih Δ = and Δ y = y y we have Δz y Δ + ln Δ y. Thus.99. = +Δz 8 + (. + 8ln (. = 8. +.6ln 7.999. To be sure, his esimae is slighly above he TI86 approimaion.99 7.9898 ln. Le z y ( e y 4. The figure a righ is he conour plo of a funcion of wo variables, f ( y,, for and y ranging from o. The scale is uni = 5 cm; spacing beween conour levels is. a. Use he conour plo o deermine wheher f and f y are >, =, or < a (,.5 and (.,.6.,.5 f,.5 < whereas SOLN: f < and y f (.,.6 < and f y (.,.6 = b. The funcion is f y, = y + y 4 +. alculae he acual values of he parial derivaives a (,.5 and (.,.6. SOLN: f ( y, = y + y 8+ and f y ( y, y f (,.5 =.5 + 8 + =.5, f y (,.5 = + = f (.,.6 = 4..6 +.6 9.6 + =., = + whence f.,.6 =.44 +.44 = c. In he diagram, here are hree places where he angen plane is horizonal. Find he eac coordinaes of each of hese and characerize each as a ma, a min or neiher. y

SOLN: Firs find criical poins where f (, y = and y y+ = = or = y. Now = means ha means ha criical poins: f, y =. For he laer, f, y = y = and = y also 6 ± 56 8 ± 4 f y, y = 5y 6y+ = y = =. Thus here are hree 5 8± 4 8± 4, and, 5. I is eviden from he level curves plo ha 8 4 8 4 8+ 4 8+ 4, 5 is a local ma and, 5 is a saddle. The poin (, on he y- ais is no so obvious so we look a he discriminan: f ( y, = 6+ y 8, f yy ( y, = and f fy f y ( y, = y+ so ha a (,, = = < his is also a saddle. I fy fyy hough i d be. / 5. onsider he curve r( = cos,sin, a. Find he lengh of he curve from / 6 6 = + + = + = + = 7 7 SOLN: r '( d 4sin 4cos 9d 4 9d ( 4 9

b. Find he curvaure as a funcion of. dtˆ dtˆ / d r' r'' κ ( = = = ds ds / d r' SOLN: = = ( ( ( sin(,cos(, 4cos(, 4sin(, + / ( 4+ 9 / ( 4+ 9 ( 4+ 9 / / sin,cos, / / / / cos sin, sin cos,8 = = 9 + 64 + 44 44 + 64 + 9 / / c. Find he angenial and normal componens of he acceleraion. r' ( r'' ( 44 + 64+ 9 SOLN: an = =, / / r' 4+ 9 a T ( ( ( ( 4+ 9 ( sin(,cos(, 4cos(, 4sin(, r' r'' = = / r = ( + / ' 4 9 / 6. onsider (,, / / / g y z = + yz a. Find a uni vecor in he direcion from (,, in which g decreases mos rapidly. 4,, SOLN: g(,, =, z, y = 4,, uˆ =. (,, b. Find a parameerizaion of he line from ha poin in he direcion of mos rapid decrease. SOLN: r( =,, + 4,, = 4,,+ 7. Le f ( y, = y + + yand g(, y y minimum and maimum values, if hey eis, of f ( y, subjec o he consrain =. Use he mehod of Lagrange mulipliers o find he g, y = wih >. In he case ha hey do eis, idenify all of he poins (, y a which hese values are aained. SOLN: A he opimal poin we require ha he normals are parallel: f ( y, = λ g( y, y +,y+ = λ y, Also, he consrain mus be me. Thus we have hree equaions in hree unknowns: y + = λ y y+ = λ y = From he las equaion we subsiue y = ino he second equaion and ge λ = 4 whence y = λ/4 λ λ 6 4 and subsiuing ino he firs equaion yields + = λ =± =± so ha y =± 4 4

and, correspondingly, =±. f, = is a ma and f, = is a min. 8. Find he area of he par of he saddle z = y ha lies inside he cylinder + y = 4. SOLN: ( y 4 S ds = + z + z da = + + y da so ha A = / / 7 ds = r + 4r drdθ = r ( + 4r dr = ( 4r 7 + = 8 6 6 9. Le f ( y, y y = +, and be y =, beween (, and (,, direced upwards. a. alculae F = f. SOLN: F = f = y, + y b. alculae he inegral F dr hree differen ways: 5 6 6 7 i. direcly; F dr =,, d 7 d 4 + = + = + = ii. by using pah-independence o replace by a simpler pah. SOLN: The simpler pah would be r( =, as goes from o. F dr,, = d d 4 + = + = + = iii. by using he Fundamenal Theorem for line inegrals. f, f, = = 4 SOLN:. Verify Green s heorem in he normal form, i.e. F nds ˆ = div (, sides and showing hey are equal if F =, y F y da, by calculaing boh and is he square wih opposie verices a (, and (,. Paramerize he four edges like so:. r( =, ; r( =, ; r( =, ; r4( =, whence r ' ( =, ; r ' ( =, ; r ' ( =, ; r 4' ( =, and he normal componens for hese are n =, ; n =,; n =,; n =, ( ( ( ( 4 SOLN: F nˆ ds = d + d ( d d + + = + = = ddy = div F, y da

. Verify Sokes heorem for he paraboloid z = 6 y for z and he vecor field F = y,4 z, 6. You may find i convenien o use polar coordinaes o evaluae he surface inegral of he curl. SOLN: If z =, hen we have r = 4, which can be parameerized by r( = 4cos,4sin, so ha F dr = sin,, 4cos 4sin,4cos, d S sin 48 sin d 48 48 4 = = = On he oher side, F ds = r θ r θ rdrdθ = r θ r θ rdrdθ 4 4 4, 6, cos, sin, sin 8 cos 4 8 5 = 4r sinθ r cosθ r dθ = 56sinθ cosθ 4dθ 5 = 56 cosθ sinθ 4θ = 48. Use he divergence heorem o calculae dv where V is he region bounded by he cone z y How abou F =,,? Hin: You can parameerize he cone by r(, θ = cos θ, sin θ,. SOLN: dv = is he volume of he cone. To apply Guass heorem, compue F ds =,, ds =,, ds +,, ds = + and he plane z =. To do his, you will need a simple field whose divergence is `. where S is he fla op of he cone and S S S S S is he curved surface of he cone. Now since he normal o fla par of he surface is perpendicular o he field lines, he firs inegral is zero. For he second, we have he normal o he surface, r rθ = cos θ,sin θ, sin θ, cos θ, = cos θ, sin θ, which poins upwards when we wan somehing poining ouwards. So we negae i and inegrae,, ds = cos θ,, cos θ, sin θ, ddθ cos θdθ d = = S. The posiion of a paricle moving in he plane a is given by r( =, + + a. Find he velociy of he paricle a ime. + + SOLN: r' ( =, =, + + + + b. Find he speed of he paricle a ime. SOLN: r' ( + = = + ( + / / / / / /.

c. Wha is he paricle s highes speed and when does ha occur? The speed is maimum of when =. 4. Find equaions of he normal plane and he osculaing plane for he curve r( =,, 4 SOLN: r' ( =,, and r'' ( =,,6 so Tˆ =,, / + 4 + 9 and a (,, 4 9 + 9 6 + Tˆ ' = 4 /, 4 /, so a (,, he angen vecor is parallel 4 / + 4 + 9 + 4 + 9 + 4 + 9 o T ˆ = k,, and he normal vecor is parallel o N ˆ = k,8,9 so ha he binormal is Bˆ = kk,,,8,9 = 6kk, 7, 5 whence he normal plane is + y + z = 6 and he osculaing plane is 8y 9z = 6. θ θ R θ = cos d, sin d as a funcion of he 5. Epress he curvaure of he pah direced disance s measured from (,. ( θ θ u u θ s = R ' u du = cos + sin du = du = θ so ha he curvaure is dtˆ dtˆ d θ θ θ θ κ = = = cos d, sin d cos, sin ds dθ dθ = = yz 6. Find he direcion in which f ( yz,, = e increases mos rapidly a he poin Wha is he maimum rae of increase? SOLN: The gradien vecor is f = e, ze, ye yz yz yz 7. Find he minimum value of f ( y, / e ( y f fyy fy > o verify his. SOLN: / / e e which a (,, is,,.,,. = + and use he second derivaive es: / / f = + y + e = + y + = + y + = fy = ye = y = so he e e f fyy fy = + y + 4 y e = y + 4, which is f, = > which means f (, = is a local minimum. e e criical poin is (-,, and since e >, we noe ha

8. escribe and skech a graph for he solid whose volume is given by he following inegral: 5 /6 ρ sinφdρdφdθ and evaluae he inegral. SOLN: This is he inersecion of a cone whose op is a he origin and which opens downwards wih an angle of / wih a spherical shell. Two views of his volume are shown below: 9. Using cylindrical coordinaes, se up an inegral for he volume under he paraboloid z = r and above he disc r cosθ. SOLN: / cosθ / rdrdθ. Find he work done by he force field F( y z,, = y, z, in moving a paricle along he heli r( = sin,cos, for. / / SOLN: F dr = cos,,sin cos, sin, d = cos + ( sin d = joules? 4

. Verify Soke s heorem for he vecor field F(, y, z =, y, z paraboloid z = y above he y-plane. SOLN: Sokes heorem saes ha F dr = F ds where S is he par of he cos + sin F dr = cos,sin, sin, cos, d = sin cos + sin cosd = = iˆ ˆj kˆ This is consisen wih F = = y z y z F, y, z zan y, z ln, z. Le = ( +. Find he flu of F across he par of he paraboloid z = + y ha lies below he plane z = and is oriened upwards. SOLN: The divergence heorem is helpful here. The ouwards surface inegral is y r F ds = FdV = dzdyd = rdzdrdθ = r r dr S E = = 4