SAMPLE MATH 209 FINAL EXAM SOLUTIONS. James D. Lewis. [ ] y sin x

Size: px
Start display at page:

Download "SAMPLE MATH 209 FINAL EXAM SOLUTIONS. James D. Lewis. [ ] y sin x"

Transcription

1 1. Evaluate the integral AMPLE MATH 9 FINAL EXAM OLUTION James D. Lewis 1 1 y sin x x dxdy. olution: The integral in its present form is hard to compute. By graphing the region and reversing the order of integration, we arrive at the simpler integral 1 1 y sin x x dxdy 1 x sin x x dydx 1 [ ] y sin x yx dx x y 1 sin x dx 1 cos 1.. A thin plate D of uniform thickness covers the region enclosed by y x and y x 3. The density at a point in D is the distance to the line x 1. Find the centre of mass. olution: The region D is described by x 3 y x, x 1. For a point P (x, y) D, the density function is given by ρ(x, y) 1 x. We first compute the total mass: M 1 x x 3 (1 x) dydx 1 [ y(1 x) ] yx yx 3 dx 1 (x x 3 + x 4 ) dx Next, M x Finally 1 x M y 1 [ ] y yx y(1 x) dydx (1 x) dx 1 x 3 yx 3 1 [ ] x x 3 x(1 x) dydx (x, y) 1 [ y(x x ) ] yx yx 3 dx ( My M, M ) ( x 1 M, 13 ) (x 4 x 5 x 6 + x 7 ) dx (x 3 x 4 + x 5 ) dx

2 3. Let Ω be the solid bounded above and below by z x + y and on the sides by x + y + z 1. (i) ompute the volume of Ω using spherical coordinates. (ii) ompute the volume of Ω using cylindrical coordinates. [Hint: You may have to express Ω as a union of two solids.] olution: (i) By spherical, we have Vol(Ω) π 3π 4 π 4 1 ρ sin φ dρdφdθ π. 3 (ii) By cylindrical, we have Ω Ω 1 + Ω, where Ω 1 : 1 r z 1 r, 1 r 1, θ π. Ω : r z r, r 1, θ π. This uses the fact that the surfaces z x + y r (double cone with vertex (,, )) and r +z x +y +z 1 (sphere of radius 1 centred at (,, )), meet when r 1/. Thus we have Vol(Ω) Vol(Ω 1 ) + Vol(Ω ). We compute: Vol(Ω 1 ) π 1 1 r 1 1 r rdzdrdθ π 1 r 1 r drdθ π 1 3. Next Vol(Ω ) π 1 r r rdzdrdθ π 1 r drdθ π 3. Finally Vol(Ω) π /3. 4. Let be the path below with given orientation, and P x + y and Q y + x. : (,1) (1,1) (,) yx (i) Evaluate two ways, namely, P dx + Qdy

3 (i.1) Directly from the definition of line integrals. (i.) Using Green s theorem. (ii) Is the vector field given by F P i + Qj conservative? [You must give a reason for your answer.] olution. (i.1) Write as in the diagram below. We have these parametrizations: (,1) (1,1) 3 (,) 1 r(t) (t, t) : [, 1] 1, r(t) (t, 1) : [, 1], r(t) (, t) : [, 1] 3, where j is the the curve j with the opposite orientation. Thus P dx + Qdy 3 P dx + Qdy P dx + Qdy j 1 j1 P dx + Qdy 3 P dx + Qdy 1 (t + t, t + t) (1, 1) dt 1 ( ) (t +, 1 + t) (1, ) dt ( ) (i.) Let D be the region bounded by the curve. By Green s theorem P dx + Qdy D 1 (t, t ) (, 1) dt ( Q x P ) da da Area(D) 1 y D. (ii) The vector field F is clearly not conservative since rot(f) : Q x P y (a) Let be the curve given by r(t) (cos t)i + (sin t)j + (sin t)k with t π. 3

4 Find directly from the definition of line integrals. zdx + xdy + y dz (b) Let f(x, y) xy. ompute the path integral olution: (a) zdx + xdy + y dz π π fds. sin t d(cos t) + cos t d(sin t) + sin t d(sin t) ( sin t + cos t cos t sin t ) dt π. [Note the identities that were used, and that all students should know: sin t 1 ( ) 1 cos t ; cos t 1 ( ) 1 + cos t.] Next (b) r (t) ( sin t)i + (cos t)j + (cos t)k r (t) 1 + cos t. f(r(t)) cos t sin t, and observe that d(1 + cos t) cos t sin t dt. Thus by substitution (or an anti-symmetry argument), we arrive at fds 6. Evaluate the surface integral π cos t sin t 1 + cos t dt. F d, where F xi+yj+3zk, where is the cube with vertices (±1, ±1, ±1), with outward orientation. 4

5 olution: Method #1 (From the definition, and the less favorable method!) Write 6 j1 j, the six sides of the cube, with parametrizations Φ j : [ 1, 1] j, Φ 1 (y, z) (1, y, z) Φ (y, z) ( 1, y, z) Φ 3 (x, y) (x, y, 1) Φ 4 (x, y) (x, y, 1) Φ 5 (x, z) (x, 1, z) Φ 6 (x, z) (x, 1, z) Then correspondingly is the table of calculations: Thus F d n 1 (1,, ) F(Φ 1 ) (1, y, 3z) F n 1 1 n ( 1,, ) F(Φ ) ( 1, y, 3z) F n 1 n 3 (,, 1) F(Φ 3 ) (x, y, 3) F n 3 3 n 4 (,, 1) F(Φ 4 ) (x, y, 3) F n 4 3 n 5 (, 1, ) F(Φ 5 ) (x,, 3z) F n 5 n 6 (, 1, ) F(Φ 6 ) (x,, 3z) F n 6 6 j1 j F d 6 j1 j (F n j )d 1 Area ( [ 1, 1] ) 48. Method # (uperior method!): Use the divergence theorem. Let Ω [ 1, 1] 3 be the cube with boundary. Then div(f) 6, hence F d (F n)d div(f) 6Vol(Ω) Any of the questions below could serve as a question 7: (i) Verify the Divergence Theorem F nd Ω E div(f)dv, where F (xz)i+(yz)j+(3z )k, and E is the solid bounded by the paraboloid z x +y and the plane z 1. olution: div(f) F 8z. Thus E π 1 1 div(f)dv 8 rzdzdrdθ 8π r 3. On the other hand, the boundary of E is of the form 1 +, where 1 is the graph of z x + y over D : {x + y 1}, and 1 is the graph of z 1 over D. Note that the 5

6 unit normal for is k, and that F (x, y, 3) on, and hence F k 3 on. Therefore F d 3 D da 3π. If we put Φ(x, y) (x, y, x + y ) : D 1, then the unit outward on 1 is Further, Thus Φ x Φ y Φ x Φ y (x, y, 1) (x, y, 1). F(Φ(x, y)) (x 3 + xy, yx + y 3, 3(x + y ) ), F (Φ x Φ y ) (x + y ). 1 F d π 1 r 5 drdθ π 3. Finally, we arrive at F d F d + F d π π 8π 3. (ii) Verify tokes Theorem, url(f) d F dr, where F (3y)i + (4z)j + ( 6x)k, and is the part of the paraboloid z 9 x y that lies above the xy-plane, oriented upward. pecial Remark. Note that url(f) d ( url(f) n ) d, where n is the unit normal determined by the orientation on, and ( ) F dr F T ds, where T is the unit tangent determined by the (induced) orientation on. Thus tokes theorem is given by the equivalent statement ( ) ( ) url(f) n d F T ds. olution to (ii): Let D {x + y 9}. The boundary of is easily seen to be the same as the boundary of D, namely {x + y 9}, oriented counterclockwise. Put Φ(x, y) (x, y, 9 x y ) : D. 6

7 Then Φ x Φ y (x, y, 1) (note that this is oriented upward, since the z-component is 1 > ). Put r(t) (3 cos t, 3 sin t, ) : [, π]. Then F(r(t)) (9 sin t,, 18 cos t), and r (t) ( 3 sin t, 3 cos t, ). Thus F r (t) 7 sin t. Thus omputing the other way, we have π F dr 7 sin tdt 7π. url(f) F ( 4, 6, 3) ; url(f) (Φ x Φ y ) 8x + 1y 3. Thus url(f) d π 3 D ( 8x + 1y 3)dA ( 8r cos θ + 1r sin θ 3r)drdθ 7π. (iii) Use tokes theorem to evaluate url(f) d, where F (y z)i + (xz)j + (x y )k, and where is the part of the paraboloid z x + y inside the cylinder x + y 1. olution: If we set D {x + y 1}, then is given by the parametrization: Φ(x, y) (x, y, x + y ) : D. The boundary of D is parametrized by (cos t, sin t), and hence the boundary of is parametrized by r(t) : Φ(cos t, sin t) (cos t, sin t, 1); moreover F(r(t)) (sin t, cos t, cos t sin t) ; r (t) ( sin t, cos t, ). Thus url(f) d π F(r(t)) dr π ( (cos t 1) sin t + cos t ) dt π. ( sin 3 t + cos t)dt (iv) Use the divergence theorem to evaluate the integral: (x + y + z )d, 7

8 where is the sphere x + y + z 1. olution: The unit outward normal on is given by n (x, y, z). [This follows from n F/ F, where F x + y + z 1 describes implicitly.] Now choose F (,, z). Then F n x + y + z, and div(f) 1. Let Ω be the ball of radius 1. Then by the divergence theorem: (x + y + z )d Ω F nd dv Volume(Ω) 4π 3. Ω div(f)dv 8

Fundamental Theorems of Vector Calculus

Fundamental Theorems of Vector Calculus Fundamental Theorems of Vector Calculus We have studied the techniques for evaluating integrals over curves and surfaces. In the case of integrating over an interval on the real line, we were able to use

More information

Solutions - Homework sections 17.7-17.9

Solutions - Homework sections 17.7-17.9 olutions - Homework sections 7.7-7.9 7.7 6. valuate xy d, where is the triangle with vertices (,, ), (,, ), and (,, ). The three points - and therefore the triangle between them - are on the plane x +

More information

Solutions to Practice Problems for Test 4

Solutions to Practice Problems for Test 4 olutions to Practice Problems for Test 4 1. Let be the line segmentfrom the point (, 1, 1) to the point (,, 3). Evaluate the line integral y ds. Answer: First, we parametrize the line segment from (, 1,

More information

Chapter 17. Review. 1. Vector Fields (Section 17.1)

Chapter 17. Review. 1. Vector Fields (Section 17.1) hapter 17 Review 1. Vector Fields (Section 17.1) There isn t much I can say in this section. Most of the material has to do with sketching vector fields. Please provide some explanation to support your

More information

Solutions for Review Problems

Solutions for Review Problems olutions for Review Problems 1. Let be the triangle with vertices A (,, ), B (4,, 1) and C (,, 1). (a) Find the cosine of the angle BAC at vertex A. (b) Find the area of the triangle ABC. (c) Find a vector

More information

This makes sense. t 2 1 + 1/t 2 dt = 1. t t 2 + 1dt = 2 du = 1 3 u3/2 u=5

This makes sense. t 2 1 + 1/t 2 dt = 1. t t 2 + 1dt = 2 du = 1 3 u3/2 u=5 1. (Line integrals Using parametrization. Two types and the flux integral) Formulas: ds = x (t) dt, d x = x (t)dt and d x = T ds since T = x (t)/ x (t). Another one is Nds = T ds ẑ = (dx, dy) ẑ = (dy,

More information

If Σ is an oriented surface bounded by a curve C, then the orientation of Σ induces an orientation for C, based on the Right-Hand-Rule.

If Σ is an oriented surface bounded by a curve C, then the orientation of Σ induces an orientation for C, based on the Right-Hand-Rule. Oriented Surfaces and Flux Integrals Let be a surface that has a tangent plane at each of its nonboundary points. At such a point on the surface two unit normal vectors exist, and they have opposite directions.

More information

Solutions to Homework 10

Solutions to Homework 10 Solutions to Homework 1 Section 7., exercise # 1 (b,d): (b) Compute the value of R f dv, where f(x, y) = y/x and R = [1, 3] [, 4]. Solution: Since f is continuous over R, f is integrable over R. Let x

More information

4.2. LINE INTEGRALS 1. 2 2 ; z = t. ; y = sin

4.2. LINE INTEGRALS 1. 2 2 ; z = t. ; y = sin 4.2. LINE INTEGRALS 1 4.2 Line Integrals MATH 294 FALL 1982 FINAL # 7 294FA82FQ7.tex 4.2.1 Consider the curve given parametrically by x = cos t t ; y = sin 2 2 ; z = t a) Determine the work done by the

More information

F = 0. x ψ = y + z (1) y ψ = x + z (2) z ψ = x + y (3)

F = 0. x ψ = y + z (1) y ψ = x + z (2) z ψ = x + y (3) MATH 255 FINAL NAME: Instructions: You must include all the steps in your derivations/answers. Reduce answers as much as possible, but use exact arithmetic. Write neatly, please, and show all steps. Scientists

More information

AB2.5: Surfaces and Surface Integrals. Divergence Theorem of Gauss

AB2.5: Surfaces and Surface Integrals. Divergence Theorem of Gauss AB2.5: urfaces and urface Integrals. Divergence heorem of Gauss epresentations of surfaces or epresentation of a surface as projections on the xy- and xz-planes, etc. are For example, z = f(x, y), x =

More information

Practice Final Math 122 Spring 12 Instructor: Jeff Lang

Practice Final Math 122 Spring 12 Instructor: Jeff Lang Practice Final Math Spring Instructor: Jeff Lang. Find the limit of the sequence a n = ln (n 5) ln (3n + 8). A) ln ( ) 3 B) ln C) ln ( ) 3 D) does not exist. Find the limit of the sequence a n = (ln n)6

More information

MULTIPLE INTEGRALS. h 2 (y) are continuous functions on [c, d] and let f(x, y) be a function defined on R. Then

MULTIPLE INTEGRALS. h 2 (y) are continuous functions on [c, d] and let f(x, y) be a function defined on R. Then MULTIPLE INTEGALS 1. ouble Integrals Let be a simple region defined by a x b and g 1 (x) y g 2 (x), where g 1 (x) and g 2 (x) are continuous functions on [a, b] and let f(x, y) be a function defined on.

More information

Vector Calculus Solutions to Sample Final Examination #1

Vector Calculus Solutions to Sample Final Examination #1 Vector alculus s to Sample Final Examination #1 1. Let f(x, y) e xy sin(x + y). (a) In what direction, starting at (,π/), is f changing the fastest? (b) In what directions starting at (,π/) is f changing

More information

Line and surface integrals: Solutions

Line and surface integrals: Solutions hapter 5 Line and surface integrals: olutions Example 5.1 Find the work done by the force F(x, y) x 2 i xyj in moving a particle along the curve which runs from (1, ) to (, 1) along the unit circle and

More information

Math 2443, Section 16.3

Math 2443, Section 16.3 Math 44, Section 6. Review These notes will supplement not replace) the lectures based on Section 6. Section 6. i) ouble integrals over general regions: We defined double integrals over rectangles in the

More information

3 Contour integrals and Cauchy s Theorem

3 Contour integrals and Cauchy s Theorem 3 ontour integrals and auchy s Theorem 3. Line integrals of complex functions Our goal here will be to discuss integration of complex functions = u + iv, with particular regard to analytic functions. Of

More information

FINAL EXAM SOLUTIONS Math 21a, Spring 03

FINAL EXAM SOLUTIONS Math 21a, Spring 03 INAL EXAM SOLUIONS Math 21a, Spring 3 Name: Start by printing your name in the above box and check your section in the box to the left. MW1 Ken Chung MW1 Weiyang Qiu MW11 Oliver Knill h1 Mark Lucianovic

More information

vector calculus 2 Learning outcomes

vector calculus 2 Learning outcomes 29 ontents vector calculus 2 1. Line integrals involving vectors 2. Surface and volume integrals 3. Integral vector theorems Learning outcomes In this Workbook you will learn how to integrate functions

More information

Solutions to old Exam 1 problems

Solutions to old Exam 1 problems Solutions to old Exam 1 problems Hi students! I am putting this old version of my review for the first midterm review, place and time to be announced. Check for updates on the web site as to which sections

More information

Exam 1 Practice Problems Solutions

Exam 1 Practice Problems Solutions MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8 Spring 13 Exam 1 Practice Problems Solutions Part I: Short Questions and Concept Questions Problem 1: Spark Plug Pictured at right is a typical

More information

A QUICK GUIDE TO THE FORMULAS OF MULTIVARIABLE CALCULUS

A QUICK GUIDE TO THE FORMULAS OF MULTIVARIABLE CALCULUS A QUIK GUIDE TO THE FOMULAS OF MULTIVAIABLE ALULUS ontents 1. Analytic Geometry 2 1.1. Definition of a Vector 2 1.2. Scalar Product 2 1.3. Properties of the Scalar Product 2 1.4. Length and Unit Vectors

More information

Surface Normals and Tangent Planes

Surface Normals and Tangent Planes Surface Normals and Tangent Planes Normal and Tangent Planes to Level Surfaces Because the equation of a plane requires a point and a normal vector to the plane, nding the equation of a tangent plane to

More information

SOLUTIONS. f x = 6x 2 6xy 24x, f y = 3x 2 6y. To find the critical points, we solve

SOLUTIONS. f x = 6x 2 6xy 24x, f y = 3x 2 6y. To find the critical points, we solve SOLUTIONS Problem. Find the critical points of the function f(x, y = 2x 3 3x 2 y 2x 2 3y 2 and determine their type i.e. local min/local max/saddle point. Are there any global min/max? Partial derivatives

More information

Vector surface area Differentials in an OCS

Vector surface area Differentials in an OCS Calculus and Coordinate systems EE 311 - Lecture 17 1. Calculus and coordinate systems 2. Cartesian system 3. Cylindrical system 4. Spherical system In electromagnetics, we will often need to perform integrals

More information

Review Sheet for Test 1

Review Sheet for Test 1 Review Sheet for Test 1 Math 261-00 2 6 2004 These problems are provided to help you study. The presence of a problem on this handout does not imply that there will be a similar problem on the test. And

More information

Change of Variables in Double Integrals

Change of Variables in Double Integrals Change of Variables in Double Integrals Part : Area of the Image of a egion It is often advantageous to evaluate (x; y) da in a coordinate system other than the xy-coordinate system. In this section, we

More information

Math 241, Exam 1 Information.

Math 241, Exam 1 Information. Math 241, Exam 1 Information. 9/24/12, LC 310, 11:15-12:05. Exam 1 will be based on: Sections 12.1-12.5, 14.1-14.3. The corresponding assigned homework problems (see http://www.math.sc.edu/ boylan/sccourses/241fa12/241.html)

More information

Scalar Valued Functions of Several Variables; the Gradient Vector

Scalar Valued Functions of Several Variables; the Gradient Vector Scalar Valued Functions of Several Variables; the Gradient Vector Scalar Valued Functions vector valued function of n variables: Let us consider a scalar (i.e., numerical, rather than y = φ(x = φ(x 1,

More information

(a) We have x = 3 + 2t, y = 2 t, z = 6 so solving for t we get the symmetric equations. x 3 2. = 2 y, z = 6. t 2 2t + 1 = 0,

(a) We have x = 3 + 2t, y = 2 t, z = 6 so solving for t we get the symmetric equations. x 3 2. = 2 y, z = 6. t 2 2t + 1 = 0, Name: Solutions to Practice Final. Consider the line r(t) = 3 + t, t, 6. (a) Find symmetric equations for this line. (b) Find the point where the first line r(t) intersects the surface z = x + y. (a) We

More information

Math 21a Curl and Divergence Spring, 2009. 1 Define the operator (pronounced del ) by. = i

Math 21a Curl and Divergence Spring, 2009. 1 Define the operator (pronounced del ) by. = i Math 21a url and ivergence Spring, 29 1 efine the operator (pronounced del by = i j y k z Notice that the gradient f (or also grad f is just applied to f (a We define the divergence of a vector field F,

More information

Chapter 4. Electrostatic Fields in Matter

Chapter 4. Electrostatic Fields in Matter Chapter 4. Electrostatic Fields in Matter 4.1. Polarization A neutral atom, placed in an external electric field, will experience no net force. However, even though the atom as a whole is neutral, the

More information

Differential Relations for Fluid Flow. Acceleration field of a fluid. The differential equation of mass conservation

Differential Relations for Fluid Flow. Acceleration field of a fluid. The differential equation of mass conservation Differential Relations for Fluid Flow In this approach, we apply our four basic conservation laws to an infinitesimally small control volume. The differential approach provides point by point details of

More information

Physics 210 Q1 2012 ( PHYSICS210BRIDGE ) My Courses Course Settings

Physics 210 Q1 2012 ( PHYSICS210BRIDGE ) My Courses Course Settings 1 of 11 9/7/2012 1:06 PM Logged in as Julie Alexander, Instructor Help Log Out Physics 210 Q1 2012 ( PHYSICS210BRIDGE ) My Courses Course Settings Course Home Assignments Roster Gradebook Item Library

More information

Math 1B, lecture 5: area and volume

Math 1B, lecture 5: area and volume Math B, lecture 5: area and volume Nathan Pflueger 6 September 2 Introduction This lecture and the next will be concerned with the computation of areas of regions in the plane, and volumes of regions in

More information

M PROOF OF THE DIVERGENCE THEOREM AND STOKES THEOREM

M PROOF OF THE DIVERGENCE THEOREM AND STOKES THEOREM 68 Theor Supplement Section M M POOF OF THE DIEGENE THEOEM ND STOKES THEOEM In this section we give proofs of the Divergence Theorem Stokes Theorem using the definitions in artesian coordinates. Proof

More information

Feb 28 Homework Solutions Math 151, Winter 2012. Chapter 6 Problems (pages 287-291)

Feb 28 Homework Solutions Math 151, Winter 2012. Chapter 6 Problems (pages 287-291) Feb 8 Homework Solutions Math 5, Winter Chapter 6 Problems (pages 87-9) Problem 6 bin of 5 transistors is known to contain that are defective. The transistors are to be tested, one at a time, until the

More information

Name Class. Date Section. Test Form A Chapter 11. Chapter 11 Test Bank 155

Name Class. Date Section. Test Form A Chapter 11. Chapter 11 Test Bank 155 Chapter Test Bank 55 Test Form A Chapter Name Class Date Section. Find a unit vector in the direction of v if v is the vector from P,, 3 to Q,, 0. (a) 3i 3j 3k (b) i j k 3 i 3 j 3 k 3 i 3 j 3 k. Calculate

More information

CBE 6333, R. Levicky 1 Differential Balance Equations

CBE 6333, R. Levicky 1 Differential Balance Equations CBE 6333, R. Levicky 1 Differential Balance Equations We have previously derived integral balances for mass, momentum, and energy for a control volume. The control volume was assumed to be some large object,

More information

Statistics 100A Homework 7 Solutions

Statistics 100A Homework 7 Solutions Chapter 6 Statistics A Homework 7 Solutions Ryan Rosario. A television store owner figures that 45 percent of the customers entering his store will purchase an ordinary television set, 5 percent will purchase

More information

Math 432 HW 2.5 Solutions

Math 432 HW 2.5 Solutions Math 432 HW 2.5 Solutions Assigned: 1-10, 12, 13, and 14. Selected for Grading: 1 (for five points), 6 (also for five), 9, 12 Solutions: 1. (2y 3 + 2y 2 ) dx + (3y 2 x + 2xy) dy = 0. M/ y = 6y 2 + 4y N/

More information

The Math Circle, Spring 2004

The Math Circle, Spring 2004 The Math Circle, Spring 2004 (Talks by Gordon Ritter) What is Non-Euclidean Geometry? Most geometries on the plane R 2 are non-euclidean. Let s denote arc length. Then Euclidean geometry arises from the

More information

Differentiation of vectors

Differentiation of vectors Chapter 4 Differentiation of vectors 4.1 Vector-valued functions In the previous chapters we have considered real functions of several (usually two) variables f : D R, where D is a subset of R n, where

More information

MATH 121 FINAL EXAM FALL 2010-2011. December 6, 2010

MATH 121 FINAL EXAM FALL 2010-2011. December 6, 2010 MATH 11 FINAL EXAM FALL 010-011 December 6, 010 NAME: SECTION: Instructions: Show all work and mark your answers clearly to receive full credit. This is a closed notes, closed book exam. No electronic

More information

Problem 1 (25 points)

Problem 1 (25 points) MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2012 Exam Three Solutions Problem 1 (25 points) Question 1 (5 points) Consider two circular rings of radius R, each perpendicular

More information

L 2 : x = s + 1, y = s, z = 4s + 4. 3. Suppose that C has coordinates (x, y, z). Then from the vector equality AC = BD, one has

L 2 : x = s + 1, y = s, z = 4s + 4. 3. Suppose that C has coordinates (x, y, z). Then from the vector equality AC = BD, one has The line L through the points A and B is parallel to the vector AB = 3, 2, and has parametric equations x = 3t + 2, y = 2t +, z = t Therefore, the intersection point of the line with the plane should satisfy:

More information

CHAPTER 24 GAUSS S LAW

CHAPTER 24 GAUSS S LAW CHAPTER 4 GAUSS S LAW 4. The net charge shown in Fig. 4-40 is Q. Identify each of the charges A, B, C shown. A B C FIGURE 4-40 4. From the direction of the lines of force (away from positive and toward

More information

www.mathsbox.org.uk Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x

www.mathsbox.org.uk Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x Mechanics 2 : Revision Notes 1. Kinematics and variable acceleration Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx differentiate a = dv = d2 x dt dt dt 2 Acceleration Velocity

More information

Section 11.1: Vectors in the Plane. Suggested Problems: 1, 5, 9, 17, 23, 25-37, 40, 42, 44, 45, 47, 50

Section 11.1: Vectors in the Plane. Suggested Problems: 1, 5, 9, 17, 23, 25-37, 40, 42, 44, 45, 47, 50 Section 11.1: Vectors in the Plane Page 779 Suggested Problems: 1, 5, 9, 17, 3, 5-37, 40, 4, 44, 45, 47, 50 Determine whether the following vectors a and b are perpendicular. 5) a = 6, 0, b = 0, 7 Recall

More information

Section 12.6: Directional Derivatives and the Gradient Vector

Section 12.6: Directional Derivatives and the Gradient Vector Section 26: Directional Derivatives and the Gradient Vector Recall that if f is a differentiable function of x and y and z = f(x, y), then the partial derivatives f x (x, y) and f y (x, y) give the rate

More information

PROBLEM SET. Practice Problems for Exam #1. Math 1352, Fall 2004. Oct. 1, 2004 ANSWERS

PROBLEM SET. Practice Problems for Exam #1. Math 1352, Fall 2004. Oct. 1, 2004 ANSWERS PROBLEM SET Practice Problems for Exam # Math 352, Fall 24 Oct., 24 ANSWERS i Problem. vlet R be the region bounded by the curves x = y 2 and y = x. A. Find the volume of the solid generated by revolving

More information

Review B: Coordinate Systems

Review B: Coordinate Systems MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of hysics 8.02 Review B: Coordinate Systems B.1 Cartesian Coordinates... B-2 B.1.1 Infinitesimal Line Element... B-4 B.1.2 Infinitesimal Area Element...

More information

27.3. Introduction. Prerequisites. Learning Outcomes

27.3. Introduction. Prerequisites. Learning Outcomes olume Integrals 27. Introduction In the previous two sections, surface integrals (or double integrals) were introduced i.e. functions were integrated with respect to one variable and then with respect

More information

MATH 132: CALCULUS II SYLLABUS

MATH 132: CALCULUS II SYLLABUS MATH 32: CALCULUS II SYLLABUS Prerequisites: Successful completion of Math 3 (or its equivalent elsewhere). Math 27 is normally not a sufficient prerequisite for Math 32. Required Text: Calculus: Early

More information

Exam 1 Sample Question SOLUTIONS. y = 2x

Exam 1 Sample Question SOLUTIONS. y = 2x Exam Sample Question SOLUTIONS. Eliminate the parameter to find a Cartesian equation for the curve: x e t, y e t. SOLUTION: You might look at the coordinates and notice that If you don t see it, we can

More information

Chapter 22: Electric Flux and Gauss s Law

Chapter 22: Electric Flux and Gauss s Law 22.1 ntroduction We have seen in chapter 21 that determining the electric field of a continuous charge distribution can become very complicated for some charge distributions. t would be desirable if we

More information

Gauss Formulation of the gravitational forces

Gauss Formulation of the gravitational forces Chapter 1 Gauss Formulation of the gravitational forces 1.1 ome theoretical background We have seen in class the Newton s formulation of the gravitational law. Often it is interesting to describe a conservative

More information

Arrangements And Duality

Arrangements And Duality Arrangements And Duality 3.1 Introduction 3 Point configurations are tbe most basic structure we study in computational geometry. But what about configurations of more complicated shapes? For example,

More information

Derive 5: The Easiest... Just Got Better!

Derive 5: The Easiest... Just Got Better! Liverpool John Moores University, 1-15 July 000 Derive 5: The Easiest... Just Got Better! Michel Beaudin École de Technologie Supérieure, Canada Email; mbeaudin@seg.etsmtl.ca 1. Introduction Engineering

More information

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid.

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid. Fluid Statics When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid. Consider a small wedge of fluid at rest of size Δx, Δz, Δs

More information

ALPERTON COMMUNITY SCHOOL MATHS FACULTY ACHIEVING GRADE A/A* EXAM PRACTICE BY TOPIC

ALPERTON COMMUNITY SCHOOL MATHS FACULTY ACHIEVING GRADE A/A* EXAM PRACTICE BY TOPIC ALPERTON COMMUNITY SCHOOL MATHS FACULTY ACHIEVING GRADE A/A* EXAM PRACTICE BY TOPIC WEEK Calculator paper Each set of questions is followed by solutions so you can check & mark your own work CONTENTS TOPIC

More information

4 More Applications of Definite Integrals: Volumes, arclength and other matters

4 More Applications of Definite Integrals: Volumes, arclength and other matters 4 More Applications of Definite Integrals: Volumes, arclength and other matters Volumes of surfaces of revolution 4. Find the volume of a cone whose height h is equal to its base radius r, by using the

More information

Stack Contents. Pressure Vessels: 1. A Vertical Cut Plane. Pressure Filled Cylinder

Stack Contents. Pressure Vessels: 1. A Vertical Cut Plane. Pressure Filled Cylinder Pressure Vessels: 1 Stack Contents Longitudinal Stress in Cylinders Hoop Stress in Cylinders Hoop Stress in Spheres Vanishingly Small Element Radial Stress End Conditions 1 2 Pressure Filled Cylinder A

More information

x 2 + y 2 = 1 y 1 = x 2 + 2x y = x 2 + 2x + 1

x 2 + y 2 = 1 y 1 = x 2 + 2x y = x 2 + 2x + 1 Implicit Functions Defining Implicit Functions Up until now in this course, we have only talked about functions, which assign to every real number x in their domain exactly one real number f(x). The graphs

More information

The Fourth International DERIVE-TI92/89 Conference Liverpool, U.K., 12-15 July 2000. Derive 5: The Easiest... Just Got Better!

The Fourth International DERIVE-TI92/89 Conference Liverpool, U.K., 12-15 July 2000. Derive 5: The Easiest... Just Got Better! The Fourth International DERIVE-TI9/89 Conference Liverpool, U.K., -5 July 000 Derive 5: The Easiest... Just Got Better! Michel Beaudin École de technologie supérieure 00, rue Notre-Dame Ouest Montréal

More information

Physics of the Atmosphere I

Physics of the Atmosphere I Physics of the Atmosphere I WS 2008/09 Ulrich Platt Institut f. Umweltphysik R. 424 Ulrich.Platt@iup.uni-heidelberg.de heidelberg.de Last week The conservation of mass implies the continuity equation:

More information

Triple Integrals in Cylindrical or Spherical Coordinates

Triple Integrals in Cylindrical or Spherical Coordinates Triple Integrals in Clindrical or Spherical Coordinates. Find the volume of the solid ball 2 + 2 + 2. Solution. Let be the ball. We know b #a of the worksheet Triple Integrals that the volume of is given

More information

CHAPTER 29 VOLUMES AND SURFACE AREAS OF COMMON SOLIDS

CHAPTER 29 VOLUMES AND SURFACE AREAS OF COMMON SOLIDS CHAPTER 9 VOLUMES AND SURFACE AREAS OF COMMON EXERCISE 14 Page 9 SOLIDS 1. Change a volume of 1 00 000 cm to cubic metres. 1m = 10 cm or 1cm = 10 6m 6 Hence, 1 00 000 cm = 1 00 000 10 6m = 1. m. Change

More information

RARITAN VALLEY COMMUNITY COLLEGE ACADEMIC COURSE OUTLINE MATH 251 CALCULUS III

RARITAN VALLEY COMMUNITY COLLEGE ACADEMIC COURSE OUTLINE MATH 251 CALCULUS III RARITAN VALLEY COMMUNITY COLLEGE ACADEMIC COURSE OUTLINE MATH 251 CALCULUS III I. Basic Course Information A. Course Number and Title: MATH 251 Calculus III B. New or Modified Course: Modified Course C.

More information

88 CHAPTER 2. VECTOR FUNCTIONS. . First, we need to compute T (s). a By definition, r (s) T (s) = 1 a sin s a. sin s a, cos s a

88 CHAPTER 2. VECTOR FUNCTIONS. . First, we need to compute T (s). a By definition, r (s) T (s) = 1 a sin s a. sin s a, cos s a 88 CHAPTER. VECTOR FUNCTIONS.4 Curvature.4.1 Definitions and Examples The notion of curvature measures how sharply a curve bends. We would expect the curvature to be 0 for a straight line, to be very small

More information

RADIUS OF CURVATURE AND EVOLUTE OF THE FUNCTION y=f(x)

RADIUS OF CURVATURE AND EVOLUTE OF THE FUNCTION y=f(x) RADIUS OF CURVATURE AND EVOLUTE OF THE FUNCTION y=f( In introductory calculus one learns about the curvature of a function y=f( also about the path (evolute that the center of curvature traces out as x

More information

3.1 MAXIMUM, MINIMUM AND INFLECTION POINT & SKETCHING THE GRAPH. In Isaac Newton's day, one of the biggest problems was poor navigation at sea.

3.1 MAXIMUM, MINIMUM AND INFLECTION POINT & SKETCHING THE GRAPH. In Isaac Newton's day, one of the biggest problems was poor navigation at sea. BA01 ENGINEERING MATHEMATICS 01 CHAPTER 3 APPLICATION OF DIFFERENTIATION 3.1 MAXIMUM, MINIMUM AND INFLECTION POINT & SKETCHING THE GRAPH Introduction to Applications of Differentiation In Isaac Newton's

More information

Exam 2 Practice Problems Part 1 Solutions

Exam 2 Practice Problems Part 1 Solutions MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Exam Practice Problems Part 1 Solutions Problem 1 Electric Field and Charge Distributions from Electric Potential An electric potential V ( z

More information

1. First-order Ordinary Differential Equations

1. First-order Ordinary Differential Equations Advanced Engineering Mathematics 1. First-order ODEs 1 1. First-order Ordinary Differential Equations 1.1 Basic concept and ideas 1.2 Geometrical meaning of direction fields 1.3 Separable differential

More information

Mechanics 1: Conservation of Energy and Momentum

Mechanics 1: Conservation of Energy and Momentum Mechanics : Conservation of Energy and Momentum If a certain quantity associated with a system does not change in time. We say that it is conserved, and the system possesses a conservation law. Conservation

More information

Lecture L6 - Intrinsic Coordinates

Lecture L6 - Intrinsic Coordinates S. Widnall, J. Peraire 16.07 Dynamics Fall 2009 Version 2.0 Lecture L6 - Intrinsic Coordinates In lecture L4, we introduced the position, velocity and acceleration vectors and referred them to a fixed

More information

MATH 425, PRACTICE FINAL EXAM SOLUTIONS.

MATH 425, PRACTICE FINAL EXAM SOLUTIONS. MATH 45, PRACTICE FINAL EXAM SOLUTIONS. Exercise. a Is the operator L defined on smooth functions of x, y by L u := u xx + cosu linear? b Does the answer change if we replace the operator L by the operator

More information

Notes on Elastic and Inelastic Collisions

Notes on Elastic and Inelastic Collisions Notes on Elastic and Inelastic Collisions In any collision of 2 bodies, their net momentus conserved. That is, the net momentum vector of the bodies just after the collision is the same as it was just

More information

1 3 4 = 8i + 20j 13k. x + w. y + w

1 3 4 = 8i + 20j 13k. x + w. y + w ) Find the point of intersection of the lines x = t +, y = 3t + 4, z = 4t + 5, and x = 6s + 3, y = 5s +, z = 4s + 9, and then find the plane containing these two lines. Solution. Solve the system of equations

More information

MATH 2433-12631. http://www.math.uh.edu/ ajajoo/math2433

MATH 2433-12631. http://www.math.uh.edu/ ajajoo/math2433 MATH 2433-12631 Aarti Jajoo ajajoo@math.uh.edu Office : PGH 606 Lecture : MoWeFre 10-11am in SR 116 Office hours : MW 11:30-12:30pm and BY APPOINTMENT http://www.math.uh.edu/ ajajoo/math2433 A. Jajoo,

More information

FLUID FORCES ON CURVED SURFACES; BUOYANCY

FLUID FORCES ON CURVED SURFACES; BUOYANCY FLUID FORCES ON CURVED SURFCES; BUOYNCY The principles applicable to analysis of pressure-induced forces on planar surfaces are directly applicable to curved surfaces. s before, the total force on the

More information

MATH 10550, EXAM 2 SOLUTIONS. x 2 + 2xy y 2 + x = 2

MATH 10550, EXAM 2 SOLUTIONS. x 2 + 2xy y 2 + x = 2 MATH 10550, EXAM SOLUTIONS (1) Find an equation for the tangent line to at the point (1, ). + y y + = Solution: The equation of a line requires a point and a slope. The problem gives us the point so we

More information

Lecture 5. Electric Flux and Flux Density, Gauss Law in Integral Form

Lecture 5. Electric Flux and Flux Density, Gauss Law in Integral Form Lecture 5 Electric Flux and Flux ensity, Gauss Law in Integral Form ections: 3.1, 3., 3.3 Homework: ee homework file LECTURE 5 slide 1 Faraday s Experiment (1837), Flux charge transfer from inner to outer

More information

Elasticity Theory Basics

Elasticity Theory Basics G22.3033-002: Topics in Computer Graphics: Lecture #7 Geometric Modeling New York University Elasticity Theory Basics Lecture #7: 20 October 2003 Lecturer: Denis Zorin Scribe: Adrian Secord, Yotam Gingold

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Sometimes functions are given not in the form y = f(x) but in a more complicated form in which it is difficult or impossible to express y explicitly in terms of x. Such functions

More information

EXAMPLE 6 Find the gradient vector field of f x, y x 2 y y 3. Plot the gradient vector field together with a contour map of f. How are they related?

EXAMPLE 6 Find the gradient vector field of f x, y x 2 y y 3. Plot the gradient vector field together with a contour map of f. How are they related? 9 HAPTER 3 VETOR ALULU 4 _4 4 _4 FIGURE 5 EXAMPLE 6 Find the gradient vector field of f, 3. Plot the gradient vector field together with a contour map of f. How are the related? OLUTION The gradient vector

More information

a b c d e You have two hours to do this exam. Please write your name on this page, and at the top of page three. GOOD LUCK! 3. a b c d e 12.

a b c d e You have two hours to do this exam. Please write your name on this page, and at the top of page three. GOOD LUCK! 3. a b c d e 12. MA123 Elem. Calculus Fall 2015 Exam 2 2015-10-22 Name: Sec.: Do not remove this answer page you will turn in the entire exam. No books or notes may be used. You may use an ACT-approved calculator during

More information

Gradient, Divergence and Curl in Curvilinear Coordinates

Gradient, Divergence and Curl in Curvilinear Coordinates Gradient, Divergence and Curl in Curvilinear Coordinates Although cartesian orthogonal coordinates are very intuitive and easy to use, it is often found more convenient to work with other coordinate systems.

More information

Consumer Theory. The consumer s problem

Consumer Theory. The consumer s problem Consumer Theory The consumer s problem 1 The Marginal Rate of Substitution (MRS) We define the MRS(x,y) as the absolute value of the slope of the line tangent to the indifference curve at point point (x,y).

More information

11.1. Objectives. Component Form of a Vector. Component Form of a Vector. Component Form of a Vector. Vectors and the Geometry of Space

11.1. Objectives. Component Form of a Vector. Component Form of a Vector. Component Form of a Vector. Vectors and the Geometry of Space 11 Vectors and the Geometry of Space 11.1 Vectors in the Plane Copyright Cengage Learning. All rights reserved. Copyright Cengage Learning. All rights reserved. 2 Objectives! Write the component form of

More information

1.(6pts) Find symmetric equations of the line L passing through the point (2, 5, 1) and perpendicular to the plane x + 3y z = 9.

1.(6pts) Find symmetric equations of the line L passing through the point (2, 5, 1) and perpendicular to the plane x + 3y z = 9. .(6pts Find symmetric equations of the line L passing through the point (, 5, and perpendicular to the plane x + 3y z = 9. (a x = y + 5 3 = z (b x (c (x = ( 5(y 3 = z + (d x (e (x + 3(y 3 (z = 9 = y 3

More information

Unified Lecture # 4 Vectors

Unified Lecture # 4 Vectors Fall 2005 Unified Lecture # 4 Vectors These notes were written by J. Peraire as a review of vectors for Dynamics 16.07. They have been adapted for Unified Engineering by R. Radovitzky. References [1] Feynmann,

More information

1 if 1 x 0 1 if 0 x 1

1 if 1 x 0 1 if 0 x 1 Chapter 3 Continuity In this chapter we begin by defining the fundamental notion of continuity for real valued functions of a single real variable. When trying to decide whether a given function is or

More information

LECTURE 6: Fluid Sheets

LECTURE 6: Fluid Sheets LECTURE 6: Fluid Sheets The dynamics of high-speed fluid sheets was first considered by Savart after his early work on electromagnetism with Biot, and was subsequently examined in a series of papers by

More information

Analysis of Stresses and Strains

Analysis of Stresses and Strains Chapter 7 Analysis of Stresses and Strains 7.1 Introduction axial load = P / A torsional load in circular shaft = T / I p bending moment and shear force in beam = M y / I = V Q / I b in this chapter, we

More information

10 Polar Coordinates, Parametric Equations

10 Polar Coordinates, Parametric Equations Polar Coordinates, Parametric Equations ½¼º½ ÈÓÐ Ö ÓÓÖ Ò Ø Coordinate systems are tools that let us use algebraic methods to understand geometry While the rectangular (also called Cartesian) coordinates

More information

A Resource for Free-standing Mathematics Qualifications

A Resource for Free-standing Mathematics Qualifications To find a maximum or minimum: Find an expression for the quantity you are trying to maximise/minimise (y say) in terms of one other variable (x). dy Find an expression for and put it equal to 0. Solve

More information

SURFACE TENSION. Definition

SURFACE TENSION. Definition SURFACE TENSION Definition In the fall a fisherman s boat is often surrounded by fallen leaves that are lying on the water. The boat floats, because it is partially immersed in the water and the resulting

More information

Chapter 22: The Electric Field. Read Chapter 22 Do Ch. 22 Questions 3, 5, 7, 9 Do Ch. 22 Problems 5, 19, 24

Chapter 22: The Electric Field. Read Chapter 22 Do Ch. 22 Questions 3, 5, 7, 9 Do Ch. 22 Problems 5, 19, 24 Chapter : The Electric Field Read Chapter Do Ch. Questions 3, 5, 7, 9 Do Ch. Problems 5, 19, 4 The Electric Field Replaces action-at-a-distance Instead of Q 1 exerting a force directly on Q at a distance,

More information