LABORATORY MODULE. EKT 241/4 ELECTROMAGNETIC THEORY Semester 2 (2009/2010) EXPERIMENT # 2

Size: px
Start display at page:

Download "LABORATORY MODULE. EKT 241/4 ELECTROMAGNETIC THEORY Semester 2 (2009/2010) EXPERIMENT # 2"

Transcription

1 LABORATORY MODULE EKT 241/4 ELECTROMAGNETIC THEORY Semester 2 (2009/2010) EXPERIMENT # 2 Vector Analysis: Gradient And Divergence Of A Scalar And Vector Field NAME MATRIK # signature DATE PROGRAMME GROUP School of Computer & Communication Engineering University of Malaysia Perlis - 1 -

2 EXPERIMENT 2 Vector Analysis: Gradient And Divergence Of A Scalar And Vector Field 1. OBJECTIVE: 1.1 To provide you with an introduction to solve the problem manually and applying divergence in SCILAB simulation. In this experiment you will generate 2D space varying, gradient of a scalar field and divergence of a vector field. 2. LECTURE REVIEW We first consider the posit ion vector, r : r = x a + y a + z a x y z where a, a, and a are rectangular unit vectors. Since the unit vectors for x y z rectangular coordinate are constants, the differential distances d x, d y and d z are the components of the differential distance vector d r: dr = dx a + dy a + dz a. x y z The operator, del: is defined to be (in rectangular coordinates) as: This operator operates as a vector. = / x a + / y a + / z a, x y z - 2 -

3 2.1 Gradient: If the del operator, operates on a scalar function, f(x,y,z), we get the gradient : f= ( f/ x) a + ( f/ y) a + ( f/ z) a x y z Gradient is a vector with the magnitude and direction of t he maximum change of the function in space. We can relate the gradient to t he differential change in the function: df = ( f/ x) d x + ( f/ y) d y + ( f/ z) d z = f dr 2.2 Divergence: The divergence of a vector is defined to be: A= [ / x a + / y a + / z a ] [A a + A a + A a ] x y z x x y y z z A= ( A / x) + ( A / y) + ( A / z) x y z Gauss theorem or divergence theorem states that t he total outward flux of a vector field A the closed surface S is the same as the volume integral of the divergence of A: c l o se d su r f ac e A ds = AdV where the vector S is the surface area vector and Ais called divergence of A(div A)

4 3. EXAMPLE 3.1 Gradient of a Scalar Field Using SCILAB simulation to plot a 3-D space varying and gradient of a scalar field for S=x 2 +3(x+y-1) 2 +(x+1) 2 for -2 < x < 2 and -2 < y < Divergence of a Vector Field Using SCILAB simulation to plot a 2-D vector and divergence of a vector field for P= cos xy a - cos y a x y for -2 < x < 2 and -2< y < 2-4 -

5 4. SOLUTION FOR EXAMPLE 4.1 Gradient of a Scalar Field % Gradient of scalar field x=-2:0.2:2; y=-2:0.2:2; [xx,yy]=meshgrid (x,y); //For 3-D space varying S1=xx.^2; S2= 3*(xx+yy-1).^2; S3= (xx+1).^2; S=S1+S2-S3; surf(x,y,s, facecolor, interp )//3D surface plot xlabel('x');ylabel('y');zlabel('s'); title( 3-D space varying scalar field'); // For gradient, first of all, calculate the gradient for the above equation G1=((2*xx)+(6*(xx+yy-1))+(2*(xx+1)));//Enter the equation of the calculated gradient G2=6*(xx+yy-1); scf; champ(x,y,g1,g2,rect=[-0.5,-0.5,2,2]) xlabel('x'); ylabel('y'); title('gradient of the Scalar Field'); Figure D space varying of scalar field - 5 -

6 Figure 2.2 Gradient of the scalar field 4.2 Divergence of a Vector Field % Divergence of a vector field x=-2:0.2:2; y=-2:0.2:2; [xx,yy]=meshgrid (x,y); m=size(xx); Px=cos(xx.*yy); Py=cos(yy.^2); P=Px-Py; scf; champ(x,y,px,py,rect=[-0.5,-0.5,2,2]) xlabel('x'); ylabel('y'); title('2-d vector field'); //For divergence, first of all, calculate the divergence for the above equation D1=(-yy.*(sin(xx.*yy)));//Enter the equation of the calculated divergence D2=sin(yy); scf; D=D1+D2; plot3d(x,y,d)//3d plot of a surface xlabel('x'); ylabel('y'); zlabel('d'); title('divergence of vector field');

7 Figure D vector field Figure 2.4 Divergence of vector field - 7 -

8 5. EXERCISE 5.1 Plot a 3-D space varying and gradient of a scalar field using SCILAB for: A=cos (xy) + 2x + sin (xy) for 0 < x < 3.5 and 0 <y < 3.5 SCILAB result and source code: - 8 -

9 5.2 Plot a 2-D vector and divergence of a vector field using SCILAB for: B= e -2 y (sin 2 x a - cos 2 x a ) for -2 < x < 2 and -2 < y < 2 SCILAB result and source code: x y - 9 -

10 5.3 Find the gradient of a scalar field U= ρ z cos 2ø Calculation: S = x 2 y + xyz Calculation:

11 5.4 Find the divergence f these vector fields Q= x 2 yz a + xz a x z Calculation : P = ρ sin ø aρ + ρ z aø + z cos ø az Calculation :

12 6. DISCUSSION 7. CONCLUSION

Lecture 10 Divergence, Gauss Law in Differential Form

Lecture 10 Divergence, Gauss Law in Differential Form Lecture 10 Divergence, Gauss Law in Differential Form ections: 3.4, 3.5, 3.6 Homework: ee homework file Properties of the Flux Integral: Recap flux is the net normal flow of the vector field F through

More information

Sections minutes. 5 to 10 problems, similar to homework problems. No calculators, no notes, no books, no phones. No green book needed.

Sections minutes. 5 to 10 problems, similar to homework problems. No calculators, no notes, no books, no phones. No green book needed. MTH 34 Review for Exam 4 ections 16.1-16.8. 5 minutes. 5 to 1 problems, similar to homework problems. No calculators, no notes, no books, no phones. No green book needed. Review for Exam 4 (16.1) Line

More information

MAC2313 Final A. (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative.

MAC2313 Final A. (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative. MAC2313 Final A (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative. ii. The vector field F = 5(x 2 + y 2 ) 3/2 x, y is radial. iii. All constant

More information

(a) The points (3, 1, 2) and ( 1, 3, 4) are the endpoints of a diameter of a sphere.

(a) The points (3, 1, 2) and ( 1, 3, 4) are the endpoints of a diameter of a sphere. MATH 4 FINAL EXAM REVIEW QUESTIONS Problem. a) The points,, ) and,, 4) are the endpoints of a diameter of a sphere. i) Determine the center and radius of the sphere. ii) Find an equation for the sphere.

More information

UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH

UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH College of Informatics and Electronics END OF SEMESTER ASSESSMENT PAPER MODULE CODE: MS4613 SEMESTER: Autumn 2002/03 MODULE TITLE: Vector Analysis DURATION OF EXAMINATION:

More information

Department of Mathematics, IIT Bombay End-Semester Examination, MA 105 Autumn-2008

Department of Mathematics, IIT Bombay End-Semester Examination, MA 105 Autumn-2008 Department of Mathematics, IIT Bombay End-Semester Examination, MA 105 Autumn-2008 Code: C-031 Date and time: 17 Nov, 2008, 9:30 A.M. - 12:30 P.M. Maximum Marks: 45 Important Instructions: 1. The question

More information

Created by T. Madas VECTOR OPERATORS. Created by T. Madas

Created by T. Madas VECTOR OPERATORS. Created by T. Madas VECTOR OPERATORS GRADIENT gradϕ ϕ Question 1 A surface S is given by the Cartesian equation x 2 2 + y = 25. a) Draw a sketch of S, and describe it geometrically. b) Determine an equation of the tangent

More information

Fundamental Electromagnetics (Chapter 4: Vector Calculus)

Fundamental Electromagnetics (Chapter 4: Vector Calculus) Fundamental Electromagnetics (Chapter 4: Vector Calculus) Prof. Kwang-Chun Ho kwangho@hansung.ac.kr Tel: 0-760-453 Fax:0-760-4435 Key Point Study differential elements in length, area, and volume useful

More information

EELE 3331 Electromagnetic I Chapter 3. Vector Calculus. Islamic University of Gaza Electrical Engineering Department Dr.

EELE 3331 Electromagnetic I Chapter 3. Vector Calculus. Islamic University of Gaza Electrical Engineering Department Dr. EELE 3331 Electromagnetic I Chapter 3 Vector Calculus Islamic University of Gaza Electrical Engineering Department Dr. Talal Skaik 2012 1 Differential Length, Area, and Volume This chapter deals with integration

More information

Notes 19 Gradient and Laplacian

Notes 19 Gradient and Laplacian ECE 3318 Applied Electricity and Magnetism Spring 218 Prof. David R. Jackson Dept. of ECE Notes 19 Gradient and Laplacian 1 Gradient Φ ( x, y, z) =scalar function Φ Φ Φ grad Φ xˆ + yˆ + zˆ x y z We can

More information

Vector Analysis. Electromagnetic Theory PHYS 401. Fall 2017

Vector Analysis. Electromagnetic Theory PHYS 401. Fall 2017 Vector Analysis Electromagnetic Theory PHYS 401 Fall 2017 1 Vector Analysis Vector analysis is a mathematical formalism with which EM concepts are most conveniently expressed and best comprehended. Many

More information

UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE B.ENG(HONS) ELECTRICAL & ELECTRONIC ENGINEERING SEMESTER ONE EXAMINATION 2015/2016

UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE B.ENG(HONS) ELECTRICAL & ELECTRONIC ENGINEERING SEMESTER ONE EXAMINATION 2015/2016 OCD60 UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE B.ENG(HONS) ELECTRICAL & ELECTRONIC ENGINEERING SEMESTER ONE EXAMINATION 2015/2016 ENGINEERING ELECTROMAGNETISM MODULE NO: EEE6002 Date: Tuesday

More information

Notes 3 Review of Vector Calculus

Notes 3 Review of Vector Calculus ECE 3317 Applied Electromagnetic Waves Prof. David R. Jackson Fall 2018 A ˆ Notes 3 Review of Vector Calculus y ya ˆ y x xa V = x y ˆ x Adapted from notes by Prof. Stuart A. Long 1 Overview Here we present

More information

Mathematical Notes for E&M Gradient, Divergence, and Curl

Mathematical Notes for E&M Gradient, Divergence, and Curl Mathematical Notes for E&M Gradient, Divergence, and Curl In these notes I explain the differential operators gradient, divergence, and curl (also known as rotor), the relations between them, the integral

More information

ENERGY IN ELECTROSTATICS

ENERGY IN ELECTROSTATICS ENERGY IN ELECTROSTATICS We now turn to the question of energy in electrostatics. The first question to consider is whether or not the force is conservative. You will recall from last semester that a conservative

More information

Multiple Integrals and Vector Calculus (Oxford Physics) Synopsis and Problem Sets; Hilary 2015

Multiple Integrals and Vector Calculus (Oxford Physics) Synopsis and Problem Sets; Hilary 2015 Multiple Integrals and Vector Calculus (Oxford Physics) Ramin Golestanian Synopsis and Problem Sets; Hilary 215 The outline of the material, which will be covered in 14 lectures, is as follows: 1. Introduction

More information

Math 23b Practice Final Summer 2011

Math 23b Practice Final Summer 2011 Math 2b Practice Final Summer 211 1. (1 points) Sketch or describe the region of integration for 1 x y and interchange the order to dy dx dz. f(x, y, z) dz dy dx Solution. 1 1 x z z f(x, y, z) dy dx dz

More information

Chapter 3 - Vector Calculus

Chapter 3 - Vector Calculus Chapter 3 - Vector Calculus Gradient in Cartesian coordinate system f ( x, y, z,...) dr ( dx, dy, dz,...) Then, f f f f,,,... x y z f f f df dx dy dz... f dr x y z df 0 (constant f contour) f dr 0 or f

More information

ES.182A Topic 45 Notes Jeremy Orloff

ES.182A Topic 45 Notes Jeremy Orloff E.8A Topic 45 Notes Jeremy Orloff 45 More surface integrals; divergence theorem Note: Much of these notes are taken directly from the upplementary Notes V0 by Arthur Mattuck. 45. Closed urfaces A closed

More information

Method of Lagrange Multipliers

Method of Lagrange Multipliers Method of Lagrange Multipliers A. Salih Department of Aerospace Engineering Indian Institute of Space Science and Technology, Thiruvananthapuram September 2013 Lagrange multiplier method is a technique

More information

Physics 6303 Lecture 2 August 22, 2018

Physics 6303 Lecture 2 August 22, 2018 Physics 6303 Lecture 2 August 22, 2018 LAST TIME: Coordinate system construction, covariant and contravariant vector components, basics vector review, gradient, divergence, curl, and Laplacian operators

More information

UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH

UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH Faculty of Science and Engineering Department of Mathematics and Statistics END OF SEMESTER ASSESSMENT PAPER MODULE CODE: MA4006 SEMESTER: Spring 2011 MODULE TITLE:

More information

16.2. Line Integrals

16.2. Line Integrals 16. Line Integrals Review of line integrals: Work integral Rules: Fdr F d r = Mdx Ndy Pdz FT r'( t) ds r t since d '(s) and hence d ds '( ) r T r r ds T = Fr '( t) dt since r r'( ) dr d dt t dt dt does

More information

MATHS 267 Answers to Stokes Practice Dr. Jones

MATHS 267 Answers to Stokes Practice Dr. Jones MATH 267 Answers to tokes Practice Dr. Jones 1. Calculate the flux F d where is the hemisphere x2 + y 2 + z 2 1, z > and F (xz + e y2, yz, z 2 + 1). Note: the surface is open (doesn t include any of the

More information

1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is

1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is 1. The value of the double integral (a) 15 26 (b) 15 8 (c) 75 (d) 105 26 5 4 0 1 1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is 2. What is the value of the double integral interchange the order

More information

12. Stresses and Strains

12. Stresses and Strains 12. Stresses and Strains Finite Element Method Differential Equation Weak Formulation Approximating Functions Weighted Residuals FEM - Formulation Classification of Problems Scalar Vector 1-D T(x) u(x)

More information

Problem Solving 1: Line Integrals and Surface Integrals

Problem Solving 1: Line Integrals and Surface Integrals A. Line Integrals MASSACHUSETTS INSTITUTE OF TECHNOLOY Department of Physics Problem Solving 1: Line Integrals and Surface Integrals The line integral of a scalar function f ( xyz),, along a path C is

More information

Vector Calculus. Dr. D. Sukumar. February 1, 2016

Vector Calculus. Dr. D. Sukumar. February 1, 2016 Vector Calculus Dr. D. Sukumar February 1, 2016 Green s Theorem Tangent form or Ciculation-Curl form c Mdx + Ndy = R ( N x M ) da y Green s Theorem Tangent form or Ciculation-Curl form Stoke s Theorem

More information

UNIT 1. INTRODUCTION

UNIT 1. INTRODUCTION UNIT 1. INTRODUCTION Objective: The aim of this chapter is to gain knowledge on Basics of electromagnetic fields Scalar and vector quantities, vector calculus Various co-ordinate systems namely Cartesian,

More information

Lecture: Wave-induced Momentum Fluxes: Radiation Stresses

Lecture: Wave-induced Momentum Fluxes: Radiation Stresses Chapter 4 Lecture: Wave-induced Momentum Fluxes: Radiation Stresses Here we derive the wave-induced depth-integrated momentum fluxes, otherwise known as the radiation stress tensor S. These are the 2nd-order

More information

G G. G. x = u cos v, y = f(u), z = u sin v. H. x = u + v, y = v, z = u v. 1 + g 2 x + g 2 y du dv

G G. G. x = u cos v, y = f(u), z = u sin v. H. x = u + v, y = v, z = u v. 1 + g 2 x + g 2 y du dv 1. Matching. Fill in the appropriate letter. 1. ds for a surface z = g(x, y) A. r u r v du dv 2. ds for a surface r(u, v) B. r u r v du dv 3. ds for any surface C. G x G z, G y G z, 1 4. Unit normal N

More information

SOLUTIONS TO THE FINAL EXAM. December 14, 2010, 9:00am-12:00 (3 hours)

SOLUTIONS TO THE FINAL EXAM. December 14, 2010, 9:00am-12:00 (3 hours) SOLUTIONS TO THE 18.02 FINAL EXAM BJORN POONEN December 14, 2010, 9:00am-12:00 (3 hours) 1) For each of (a)-(e) below: If the statement is true, write TRUE. If the statement is false, write FALSE. (Please

More information

Directional Derivative and the Gradient Operator

Directional Derivative and the Gradient Operator Chapter 4 Directional Derivative and the Gradient Operator The equation z = f(x, y) defines a surface in 3 dimensions. We can write this as z f(x, y) = 0, or g(x, y, z) = 0, where g(x, y, z) = z f(x, y).

More information

MATH 311 Topics in Applied Mathematics I Lecture 36: Surface integrals (continued). Gauss theorem. Stokes theorem.

MATH 311 Topics in Applied Mathematics I Lecture 36: Surface integrals (continued). Gauss theorem. Stokes theorem. MATH 311 Topics in Applied Mathematics I Lecture 36: Surface integrals (continued). Gauss theorem. Stokes theorem. Surface integrals Let X : R 3 be a smooth parametrized surface, where R 2 is a bounded

More information

PRACTICE PROBLEMS. Please let me know if you find any mistakes in the text so that i can fix them. 1. Mixed partial derivatives.

PRACTICE PROBLEMS. Please let me know if you find any mistakes in the text so that i can fix them. 1. Mixed partial derivatives. PRACTICE PROBLEMS Please let me know if you find any mistakes in the text so that i can fix them. 1.1. Let Show that f is C 1 and yet How is that possible? 1. Mixed partial derivatives f(x, y) = {xy x

More information

DO NOT BEGIN THIS TEST UNTIL INSTRUCTED TO START

DO NOT BEGIN THIS TEST UNTIL INSTRUCTED TO START Math 265 Student name: KEY Final Exam Fall 23 Instructor & Section: This test is closed book and closed notes. A (graphing) calculator is allowed for this test but cannot also be a communication device

More information

Vector Calculus, Maths II

Vector Calculus, Maths II Section A Vector Calculus, Maths II REVISION (VECTORS) 1. Position vector of a point P(x, y, z) is given as + y and its magnitude by 2. The scalar components of a vector are its direction ratios, and represent

More information

Multiple Integrals and Vector Calculus: Synopsis

Multiple Integrals and Vector Calculus: Synopsis Multiple Integrals and Vector Calculus: Synopsis Hilary Term 28: 14 lectures. Steve Rawlings. 1. Vectors - recap of basic principles. Things which are (and are not) vectors. Differentiation and integration

More information

Introduction to Vector Calculus (29) SOLVED EXAMPLES. (d) B. C A. (f) a unit vector perpendicular to both B. = ˆ 2k = = 8 = = 8

Introduction to Vector Calculus (29) SOLVED EXAMPLES. (d) B. C A. (f) a unit vector perpendicular to both B. = ˆ 2k = = 8 = = 8 Introduction to Vector Calculus (9) SOLVED EXAMPLES Q. If vector A i ˆ ˆj k, ˆ B i ˆ ˆj, C i ˆ 3j ˆ kˆ (a) A B (e) A B C (g) Solution: (b) A B (c) A. B C (d) B. C A then find (f) a unit vector perpendicular

More information

Math 234 Final Exam (with answers) Spring 2017

Math 234 Final Exam (with answers) Spring 2017 Math 234 Final Exam (with answers) pring 217 1. onsider the points A = (1, 2, 3), B = (1, 2, 2), and = (2, 1, 4). (a) [6 points] Find the area of the triangle formed by A, B, and. olution: One way to solve

More information

Directional Derivatives in the Plane

Directional Derivatives in the Plane Directional Derivatives in the Plane P. Sam Johnson April 10, 2017 P. Sam Johnson (NIT Karnataka) Directional Derivatives in the Plane April 10, 2017 1 / 30 Directional Derivatives in the Plane Let z =

More information

Lecture 04. Curl and Divergence

Lecture 04. Curl and Divergence Lecture 04 Curl and Divergence UCF Curl of Vector Field (1) F c d l F C Curl (or rotor) of a vector field a n curlf F d l lim c s s 0 F s a n C a n : normal direction of s follow right-hand rule UCF Curl

More information

Vector Calculus - GATE Study Material in PDF

Vector Calculus - GATE Study Material in PDF Vector Calculus - GATE Study Material in PDF In previous articles, we have already seen the basics of Calculus Differentiation and Integration and applications. In GATE 2018 Study Notes, we will be introduced

More information

Solutions to Sample Questions for Final Exam

Solutions to Sample Questions for Final Exam olutions to ample Questions for Final Exam Find the points on the surface xy z 3 that are closest to the origin. We use the method of Lagrange Multipliers, with f(x, y, z) x + y + z for the square of the

More information

MAT 211 Final Exam. Spring Jennings. Show your work!

MAT 211 Final Exam. Spring Jennings. Show your work! MAT 211 Final Exam. pring 215. Jennings. how your work! Hessian D = f xx f yy (f xy ) 2 (for optimization). Polar coordinates x = r cos(θ), y = r sin(θ), da = r dr dθ. ylindrical coordinates x = r cos(θ),

More information

Page Points Score Total: 210. No more than 200 points may be earned on the exam.

Page Points Score Total: 210. No more than 200 points may be earned on the exam. Name: PID: Section: Recitation Instructor: DO NOT WRITE BELOW THIS LINE. GO ON TO THE NEXT PAGE. Page Points Score 3 18 4 18 5 18 6 18 7 18 8 18 9 18 10 21 11 21 12 21 13 21 Total: 210 No more than 200

More information

Practice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr.

Practice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr. 1. Let F(x, y) xyi+(y 3x)j, and let be the curve r(t) ti+(3t t 2 )j for t 2. ompute F dr. Solution. F dr b a 2 2 F(r(t)) r (t) dt t(3t t 2 ), 3t t 2 3t 1, 3 2t dt t 3 dt 1 2 4 t4 4. 2. Evaluate the line

More information

Chain Rule. MATH 311, Calculus III. J. Robert Buchanan. Spring Department of Mathematics

Chain Rule. MATH 311, Calculus III. J. Robert Buchanan. Spring Department of Mathematics 3.33pt Chain Rule MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Spring 2019 Single Variable Chain Rule Suppose y = g(x) and z = f (y) then dz dx = d (f (g(x))) dx = f (g(x))g (x)

More information

Jim Lambers MAT 280 Summer Semester Practice Final Exam Solution. dy + xz dz = x(t)y(t) dt. t 3 (4t 3 ) + e t2 (2t) + t 7 (3t 2 ) dt

Jim Lambers MAT 280 Summer Semester Practice Final Exam Solution. dy + xz dz = x(t)y(t) dt. t 3 (4t 3 ) + e t2 (2t) + t 7 (3t 2 ) dt Jim Lambers MAT 28 ummer emester 212-1 Practice Final Exam olution 1. Evaluate the line integral xy dx + e y dy + xz dz, where is given by r(t) t 4, t 2, t, t 1. olution From r (t) 4t, 2t, t 2, we obtain

More information

free space (vacuum) permittivity [ F/m]

free space (vacuum) permittivity [ F/m] Electrostatic Fields Electrostatic fields are static (time-invariant) electric fields produced by static (stationary) charge distributions. The mathematical definition of the electrostatic field is derived

More information

Exercises for Multivariable Differential Calculus XM521

Exercises for Multivariable Differential Calculus XM521 This document lists all the exercises for XM521. The Type I (True/False) exercises will be given, and should be answered, online immediately following each lecture. The Type III exercises are to be done

More information

Stokes s Theorem 17.2

Stokes s Theorem 17.2 Stokes s Theorem 17.2 6 December 213 Stokes s Theorem is the generalization of Green s Theorem to surfaces not just flat surfaces (regions in R 2 ). Relate a double integral over a surface with a line

More information

Created by T. Madas LINE INTEGRALS. Created by T. Madas

Created by T. Madas LINE INTEGRALS. Created by T. Madas LINE INTEGRALS LINE INTEGRALS IN 2 DIMENSIONAL CARTESIAN COORDINATES Question 1 Evaluate the integral ( x + 2y) dx, C where C is the path along the curve with equation y 2 = x + 1, from ( ) 0,1 to ( )

More information

Chapter 1. Vector Algebra and Vector Space

Chapter 1. Vector Algebra and Vector Space 1. Vector Algebra 1.1. Scalars and vectors Chapter 1. Vector Algebra and Vector Space The simplest kind of physical quantity is one that can be completely specified by its magnitude, a single number, together

More information

Math 3435 Homework Set 11 Solutions 10 Points. x= 1,, is in the disk of radius 1 centered at origin

Math 3435 Homework Set 11 Solutions 10 Points. x= 1,, is in the disk of radius 1 centered at origin Math 45 Homework et olutions Points. ( pts) The integral is, x + z y d = x + + z da 8 6 6 where is = x + z 8 x + z = 4 o, is the disk of radius centered on the origin. onverting to polar coordinates then

More information

One side of each sheet is blank and may be used as scratch paper.

One side of each sheet is blank and may be used as scratch paper. Math 244 Spring 2017 (Practice) Final 5/11/2017 Time Limit: 2 hours Name: No calculators or notes are allowed. One side of each sheet is blank and may be used as scratch paper. heck your answers whenever

More information

Review Sheet for the Final

Review Sheet for the Final Review Sheet for the Final Math 6-4 4 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 the absence

More information

Tangent Planes, Linear Approximations and Differentiability

Tangent Planes, Linear Approximations and Differentiability Jim Lambers MAT 80 Spring Semester 009-10 Lecture 5 Notes These notes correspond to Section 114 in Stewart and Section 3 in Marsden and Tromba Tangent Planes, Linear Approximations and Differentiability

More information

Today in Physics 217: electric potential

Today in Physics 217: electric potential Today in Physics 17: electric potential Finish Friday s discussion of the field from a uniformly-charged sphere, and the gravitational analogue of Gauss Law. Electric potential Example: a field and its

More information

In addition to the problems below, here are appropriate study problems from the Miscellaneous Exercises for Chapter 6, page 410: Problems

In addition to the problems below, here are appropriate study problems from the Miscellaneous Exercises for Chapter 6, page 410: Problems 22M:28 Spring 05 J. Simon Ch. 6 Study Guide for Final Exam page 1 of 9 22M:28 Spring 05 J. Simon Study Guide for Final Exam Chapter 6 Portion How to use this guide: I am not going to list a lot of problems

More information

7a3 2. (c) πa 3 (d) πa 3 (e) πa3

7a3 2. (c) πa 3 (d) πa 3 (e) πa3 1.(6pts) Find the integral x, y, z d S where H is the part of the upper hemisphere of H x 2 + y 2 + z 2 = a 2 above the plane z = a and the normal points up. ( 2 π ) Useful Facts: cos = 1 and ds = ±a sin

More information

Review for the Final Test

Review for the Final Test Math 7 Review for the Final Test () Decide if the limit exists and if it exists, evaluate it. lim (x,y,z) (0,0,0) xz. x +y +z () Use implicit differentiation to find z if x + y z = 9 () Find the unit tangent

More information

x + ye z2 + ze y2, y + xe z2 + ze x2, z and where T is the

x + ye z2 + ze y2, y + xe z2 + ze x2, z and where T is the 1.(8pts) Find F ds where F = x + ye z + ze y, y + xe z + ze x, z and where T is the T surface in the pictures. (The two pictures are two views of the same surface.) The boundary of T is the unit circle

More information

52. The Del Operator: Divergence and Curl

52. The Del Operator: Divergence and Curl 52. The Del Operator: Divergence and Curl Let F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z) be a vector field in R 3. The del operator is represented by the symbol, and is written = x, y, z, or = x,

More information

S12.1 SOLUTIONS TO PROBLEMS 12 (ODD NUMBERS)

S12.1 SOLUTIONS TO PROBLEMS 12 (ODD NUMBERS) OLUTION TO PROBLEM 2 (ODD NUMBER) 2. The electric field is E = φ = 2xi + 2y j and at (2, ) E = 4i + 2j. Thus E = 2 5 and its direction is 2i + j. At ( 3, 2), φ = 6i + 4 j. Thus the direction of most rapid

More information

Ma 1c Practical - Solutions to Homework Set 7

Ma 1c Practical - Solutions to Homework Set 7 Ma 1c Practical - olutions to omework et 7 All exercises are from the Vector Calculus text, Marsden and Tromba (Fifth Edition) Exercise 7.4.. Find the area of the portion of the unit sphere that is cut

More information

Disclaimer: This Final Exam Study Guide is meant to help you start studying. It is not necessarily a complete list of everything you need to know.

Disclaimer: This Final Exam Study Guide is meant to help you start studying. It is not necessarily a complete list of everything you need to know. Disclaimer: This is meant to help you start studying. It is not necessarily a complete list of everything you need to know. The MTH 234 final exam mainly consists of standard response questions where students

More information

EKC314: TRANSPORT PHENOMENA Core Course for B.Eng.(Chemical Engineering) Semester II (2008/2009)

EKC314: TRANSPORT PHENOMENA Core Course for B.Eng.(Chemical Engineering) Semester II (2008/2009) EKC314: TRANSPORT PHENOMENA Core Course for B.Eng.(Chemical Engineering) Semester II (2008/2009) Dr. Mohamad Hekarl Uzir-chhekarl@eng.usm.my School of Chemical Engineering Engineering Campus, Universiti

More information

18.02 Multivariable Calculus Fall 2007

18.02 Multivariable Calculus Fall 2007 MIT OpenCourseWare http://ocw.mit.edu 18.02 Multivariable Calculus Fall 2007 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. V9. Surface Integrals Surface

More information

No calculators, cell phones or any other electronic devices can be used on this exam. Clear your desk of everything excepts pens, pencils and erasers.

No calculators, cell phones or any other electronic devices can be used on this exam. Clear your desk of everything excepts pens, pencils and erasers. Name: Section: Recitation Instructor: READ THE FOLLOWING INSTRUCTIONS. Do not open your exam until told to do so. No calculators, cell phones or any other electronic devices can be used on this exam. Clear

More information

Solutions for the Practice Final - Math 23B, 2016

Solutions for the Practice Final - Math 23B, 2016 olutions for the Practice Final - Math B, 6 a. True. The area of a surface is given by the expression d, and since we have a parametrization φ x, y x, y, f x, y with φ, this expands as d T x T y da xy

More information

APPM 2350 Final Exam points Monday December 17, 7:30am 10am, 2018

APPM 2350 Final Exam points Monday December 17, 7:30am 10am, 2018 APPM 2 Final Exam 28 points Monday December 7, 7:am am, 28 ON THE FONT OF YOU BLUEBOOK write: () your name, (2) your student ID number, () lecture section/time (4) your instructor s name, and () a grading

More information

A Brief Revision of Vector Calculus and Maxwell s Equations

A Brief Revision of Vector Calculus and Maxwell s Equations A Brief Revision of Vector Calculus and Maxwell s Equations Debapratim Ghosh Electronic Systems Group Department of Electrical Engineering Indian Institute of Technology Bombay e-mail: dghosh@ee.iitb.ac.in

More information

25. Chain Rule. Now, f is a function of t only. Expand by multiplication:

25. Chain Rule. Now, f is a function of t only. Expand by multiplication: 25. Chain Rule The Chain Rule is present in all differentiation. If z = f(x, y) represents a two-variable function, then it is plausible to consider the cases when x and y may be functions of other variable(s).

More information

Math 31CH - Spring Final Exam

Math 31CH - Spring Final Exam Math 3H - Spring 24 - Final Exam Problem. The parabolic cylinder y = x 2 (aligned along the z-axis) is cut by the planes y =, z = and z = y. Find the volume of the solid thus obtained. Solution:We calculate

More information

Final Exam Review Sheet : Comments and Selected Solutions

Final Exam Review Sheet : Comments and Selected Solutions MATH 55 Applied Honors alculus III Winter Final xam Review heet : omments and elected olutions Note: The final exam will cover % among topics in chain rule, linear approximation, maximum and minimum values,

More information

16.2 Line Integrals. Lukas Geyer. M273, Fall Montana State University. Lukas Geyer (MSU) 16.2 Line Integrals M273, Fall / 21

16.2 Line Integrals. Lukas Geyer. M273, Fall Montana State University. Lukas Geyer (MSU) 16.2 Line Integrals M273, Fall / 21 16.2 Line Integrals Lukas Geyer Montana State University M273, Fall 211 Lukas Geyer (MSU) 16.2 Line Integrals M273, Fall 211 1 / 21 Scalar Line Integrals Definition f (x) ds = lim { s i } N f (P i ) s

More information

Lecture 2 : Curvilinear Coordinates

Lecture 2 : Curvilinear Coordinates Lecture 2 : Curvilinear Coordinates Fu-Jiun Jiang October, 200 I. INTRODUCTION A. Definition and Notations In 3-dimension Euclidean space, a vector V can be written as V = e x V x + e y V y + e z V z with

More information

Let F be a field defined on an open region D in space, and suppose that the (work) integral A

Let F be a field defined on an open region D in space, and suppose that the (work) integral A 16.3 1 16.3 Path Independence and Conservative Fields Definition. Path Independence Let F be a field defined on an open region D in space, and suppose B that the work) integral A F dr is the same for all

More information

Page Problem Score Max Score a 8 12b a b 10 14c 6 6

Page Problem Score Max Score a 8 12b a b 10 14c 6 6 Fall 14 MTH 34 FINAL EXAM December 8, 14 Name: PID: Section: Instructor: DO NOT WRITE BELOW THIS LINE. Go to the next page. Page Problem Score Max Score 1 5 5 1 3 5 4 5 5 5 6 5 7 5 8 5 9 5 1 5 11 1 3 1a

More information

Final Review Worksheet

Final Review Worksheet Score: Name: Final Review Worksheet Math 2110Q Fall 2014 Professor Hohn Answers (in no particular order): f(x, y) = e y + xe xy + C; 2; 3; e y cos z, e z cos x, e x cos y, e x sin y e y sin z e z sin x;

More information

In this section, mathematical description of the motion of fluid elements moving in a flow field is

In this section, mathematical description of the motion of fluid elements moving in a flow field is Jun. 05, 015 Chapter 6. Differential Analysis of Fluid Flow 6.1 Fluid Element Kinematics In this section, mathematical description of the motion of fluid elements moving in a flow field is given. A small

More information

MP204 Electricity and Magnetism

MP204 Electricity and Magnetism MATHEMATICAL PHYSICS SEMESTER 2, REPEAT 2016 2017 MP204 Electricity and Magnetism Prof. S. J. Hands, Dr. M. Haque and Dr. J.-I. Skullerud Time allowed: 1 1 2 hours Answer ALL questions MP204, 2016 2017,

More information

MATH H53 : Final exam

MATH H53 : Final exam MATH H53 : Final exam 11 May, 18 Name: You have 18 minutes to answer the questions. Use of calculators or any electronic items is not permitted. Answer the questions in the space provided. If you run out

More information

M273Q Multivariable Calculus Spring 2017 Review Problems for Exam 3

M273Q Multivariable Calculus Spring 2017 Review Problems for Exam 3 M7Q Multivariable alculus Spring 7 Review Problems for Exam Exam covers material from Sections 5.-5.4 and 6.-6. and 7.. As you prepare, note well that the Fall 6 Exam posted online did not cover exactly

More information

Tangent Plane. Linear Approximation. The Gradient

Tangent Plane. Linear Approximation. The Gradient Calculus 3 Lia Vas Tangent Plane. Linear Approximation. The Gradient The tangent plane. Let z = f(x, y) be a function of two variables with continuous partial derivatives. Recall that the vectors 1, 0,

More information

Math 212-Lecture 8. The chain rule with one independent variable

Math 212-Lecture 8. The chain rule with one independent variable Math 212-Lecture 8 137: The multivariable chain rule The chain rule with one independent variable w = f(x, y) If the particle is moving along a curve x = x(t), y = y(t), then the values that the particle

More information

MATH 228: Calculus III (FALL 2016) Sample Problems for FINAL EXAM SOLUTIONS

MATH 228: Calculus III (FALL 2016) Sample Problems for FINAL EXAM SOLUTIONS MATH 228: Calculus III (FALL 216) Sample Problems for FINAL EXAM SOLUTIONS MATH 228 Page 2 Problem 1. (2pts) Evaluate the line integral C xy dx + (x + y) dy along the parabola y x2 from ( 1, 1) to (2,

More information

Introduction and Vectors Lecture 1

Introduction and Vectors Lecture 1 1 Introduction Introduction and Vectors Lecture 1 This is a course on classical Electromagnetism. It is the foundation for more advanced courses in modern physics. All physics of the modern era, from quantum

More information

Past Exam Problems in Integrals, Solutions

Past Exam Problems in Integrals, Solutions Past Exam Problems in Integrals, olutions Prof. Qiao Zhang ourse 11.22 December 7, 24 Note: These problems do not imply, in any sense, my taste or preference for our own exam. ome of the problems here

More information

Mathematical Analysis II, 2018/19 First semester

Mathematical Analysis II, 2018/19 First semester Mathematical Analysis II, 208/9 First semester Yoh Tanimoto Dipartimento di Matematica, Università di Roma Tor Vergata Via della Ricerca Scientifica, I-0033 Roma, Italy email: hoyt@mat.uniroma2.it We basically

More information

Unit 6 Line and Surface Integrals

Unit 6 Line and Surface Integrals Unit 6 Line and Surface Integrals In this unit, we consider line integrals and surface integrals and the relationships between them. We also discuss the three theorems Green s theorem, the divergence theorem

More information

2.20 Fall 2018 Math Review

2.20 Fall 2018 Math Review 2.20 Fall 2018 Math Review September 10, 2018 These notes are to help you through the math used in this class. This is just a refresher, so if you never learned one of these topics you should look more

More information

Without fully opening the exam, check that you have pages 1 through 12.

Without fully opening the exam, check that you have pages 1 through 12. Name: Section: Recitation Instructor: INSTRUCTIONS Fill in your name, etc. on this first page. Without fully opening the exam, check that you have pages 1 through 12. Show all your work on the standard

More information

MATH2000 Flux integrals and Gauss divergence theorem (solutions)

MATH2000 Flux integrals and Gauss divergence theorem (solutions) DEPARTMENT O MATHEMATIC MATH lux integrals and Gauss divergence theorem (solutions ( The hemisphere can be represented as We have by direct calculation in terms of spherical coordinates. = {(r, θ, φ r,

More information

Introduction to Differentials

Introduction to Differentials Introduction to Differentials David G Radcliffe 13 March 2007 1 Increments Let y be a function of x, say y = f(x). The symbol x denotes a change or increment in the value of x. Note that a change in the

More information

Module 2: Governing Equations and Hypersonic Relations

Module 2: Governing Equations and Hypersonic Relations Module 2: Governing Equations and Hypersonic Relations Lecture -2: Mass Conservation Equation 2.1 The Differential Equation for mass conservation: Let consider an infinitely small elemental control volume

More information

Maxwell s Equations in Differential Form, and Uniform Plane Waves in Free Space

Maxwell s Equations in Differential Form, and Uniform Plane Waves in Free Space C H A P T E R 3 Maxwell s Equations in Differential Form, and Uniform Plane Waves in Free Space In Chapter 2, we introduced Maxwell s equations in integral form. We learned that the quantities involved

More information

Multivariable Calculus and Matrix Algebra-Summer 2017

Multivariable Calculus and Matrix Algebra-Summer 2017 Multivariable Calculus and Matrix Algebra-Summer 017 Homework 4 Solutions Note that the solutions below are for the latest version of the problems posted. For those of you who worked on an earlier version

More information

Here are some solutions to the sample problems assigned for Chapter 4. Solution: Consider a function of 3 (independent) variables. treating as real.

Here are some solutions to the sample problems assigned for Chapter 4. Solution: Consider a function of 3 (independent) variables. treating as real. Lecture 11 Appendix B: Some sample problems from Boas Here are some solutions to the sample problems assigned for Chapter 4. 4.1: 3 Solution: Consider a function of 3 (independent) variables,, ln z u v

More information