Change of Variables In Multiple Integrals

Similar documents
CHAPTER 8 INTEGRALS. You ll undoubtedly recall that you first learned about integrals by trying to figure out

COMPLETE Chapter 15 Multiple Integrals. Section 15.1 Double Integrals Over Rectangles. Section 15.2 Iterated Integrals

Multivariable Calculus Lecture #13 Notes. in each piece. Then the mass mk. 0 σ = σ = σ

FOCUS ON THEORY. We now consider a general change of variable, where x; y coordinates are related to s; t coordinates by the differentiable functions

Calculus III - Problem Solving Drill 18: Double Integrals in Polar Coordinates and Applications of Double Integrals

Phys 221. Chapter 3. Vectors A. Dzyubenko Brooks/Cole

Chapter 5 Trigonometric Functions of Angles

Use partial integration with respect to y to compute the inner integral (treating x as a constant.)

Fundamentals of Applied Electromagnetics. Chapter 2 - Vector Analysis

SVKM s NMIMS. Mukesh Patel School of Technology Management & Engineering, Vile Parle, Mumbai

Physics 101 Lecture 2 Vectors Dr. Ali ÖVGÜN

Problem Solving 1: Line Integrals and Surface Integrals

CHAPTER 6 VECTOR CALCULUS. We ve spent a lot of time so far just looking at all the different ways you can graph

Vectors for Physics. AP Physics C

The spatial frequency domain

Section 8.5 Parametric Equations

Winter 2017 Ma 1b Analytical Problem Set 2 Solutions

42. Change of Variables: The Jacobian

A. Correct! These are the corresponding rectangular coordinates.

APPENDIX D Rotation and the General Second-Degree Equation

ln e 2s+2t σ(m) = 1 + h 2 x + h 2 yda = dA = 90 da R

Triple Integrals in Cartesian Coordinates. Triple Integrals in Cylindrical Coordinates. Triple Integrals in Spherical Coordinates

MTH 254 Final Exam Technology Free-access Exam. dy dx calculates the area of region(s). dx dy calculates the area of region(s).

Vector Analysis 1.1 VECTOR ANALYSIS. A= Aa A. Aa, A direction of the vector A.

Math Review Night: Work and the Dot Product

CBSE Board Paper Class-XII. Time allowed : 3 hours Maximum Marks : 100

Multivariable Calculus : Change of Variables in Multiple Integrals

QMUL, School of Physics and Astronomy Date: 18/01/2019

Answer sheet: Final exam for Math 2339, Dec 10, 2010

Triple Integrals. y x

Math 2433 Notes Week Triple Integrals. Integration over an arbitrary solid: Applications: 1. Volume of hypersolid = f ( x, y, z ) dxdydz

Double Integrals. Advanced Calculus. Lecture 2 Dr. Lahcen Laayouni. Department of Mathematics and Statistics McGill University.

Math 212-Lecture Integration in cylindrical and spherical coordinates

Integrals in cylindrical, spherical coordinates (Sect. 15.7)

f(p i )Area(T i ) F ( r(u, w) ) (r u r w ) da

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

Math 53 Homework 4 Solutions

ENGI Surface Integrals Page 2.01

APPM 1360 Final Exam Spring 2016

11.4 Polar Coordinates

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

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 3 Solutions [Multiple Integration; Lines of Force]

The branch of mechanics which deals with the motion of object is called dynamics. It is divided into two branches:

9.1 VECTORS. A Geometric View of Vectors LEARNING OBJECTIVES. = a, b

3/31/ Product of Inertia. Sample Problem Sample Problem 10.6 (continue)

The choice of origin, axes, and length is completely arbitrary.

Complex Numbers Class Work. Complex Numbers Homework. Pre-Calc Polar & Complex #s ~1~ NJCTL.org. Simplify using i b 4 3.

CHAPTER 5 VECTOR TRANSFORMATIONS. look at parametric equations. This is because we can always associate a position

we must pay attention to the role of the coordinate system w.r.t. which we perform a tform

27 ft 3 adequately describes the volume of a cube with side 3. ft F adequately describes the temperature of a person.


ENGI 4430 Multiple Integration Cartesian Double Integrals Page 3-01

Exercises. . Evaluate f (, ) xydawhere. 2, 1 x< 3, 0 y< (Answer: 14) 3, 3 x 4, 0 y 2. (Answer: 12) ) f x. ln 2 1 ( ) = (Answer: 1)

CHAPTER SIXTEEN. = 4 x y + 6 x y + 3 x y + 4 x y = 17 x y = 31(0.1)(0.2) = f(x i, y i) x y = 7 x y + 10 x y + 6 x y + 8 x y = 31 x y. x = 0.

EXAM 1. OPEN BOOK AND CLOSED NOTES.

4.4 Change of Variable in Integrals: The Jacobian

( ) ( ) ( ) ( ) Calculus III - Problem Drill 24: Stokes and Divergence Theorem

we must pay attention to the role of the coordinate system w.r.t. which we perform a tform

Distance Formula in 3-D Given any two points P 1 (x 1, y 1, z 1 ) and P 2 (x 2, y 2, z 2 ) the distance between them is ( ) ( ) ( )

Marking Scheme (Mathematics XII )

Physics for Scientists and Engineers. Chapter 3 Vectors and Coordinate Systems

Multivariable Calculus Lecture #11 Notes

Phys101 First Major-111 Zero Version Monday, October 17, 2011 Page: 1

Lecture Notes. Math 263 Calculus III. (Part II)

Instructions: No books. No notes. Non-graphing calculators only. You are encouraged, although not required, to show your work.

02. If (x, y) is equidistant from (a + b, b a) and (a b, a + b), then (A) x + y = 0 (B) bx ay = 0 (C) ax by = 0 (D) bx + ay = 0 (E) ax + by =

Lecture 5: 3-D Rotation Matrices.

Exercise Qu. 12. a2 y 2 da = Qu. 18 The domain of integration: from y = x to y = x 1 3 from x = 0 to x = 1. = 1 y4 da.

Lecture 04. Curl and Divergence

MATH 200 WEEK 10 - WEDNESDAY THE JACOBIAN & CHANGE OF VARIABLES

Fixed Point Theorem and Sequences in One or Two Dimensions

18.02 Multivariable Calculus Fall 2007

(b) Let S 1 : f(x, y, z) = (x a) 2 + (y b) 2 + (z c) 2 = 1, this is a level set in 3D, hence

Triple integrals in Cartesian coordinates (Sect. 15.5)

Math 323 Exam 1 Practice Problem Solutions

ANNUAL EXAMINATION - ANSWER KEY II PUC - MATHEMATICS PART - A

Chapter 3: Kinematics in Two Dimensions

STD. XII ISC - BOARD MATHEMATICS - SOLUTIONS

17. Find the moments of inertia I x, I y, I 0 for the lamina of. 4. D x, y 0 x a, 0 y b ; CAS. 20. D is enclosed by the cardioid r 1 cos ; x, y 3

Directional derivatives and gradient vectors (Sect. 14.5). Directional derivative of functions of two variables.

Section A brief on transformations

is a surface above the xy-plane over R.

Vector Calculus. Dr. D. Sukumar

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. C) 2

Introduction to Vector Calculus

Math 212. Practice Problems for the Midterm 3

Physics 101. Vectors. Lecture 2. h0r33fy. EMU Physics Department. Assist. Prof. Dr. Ali ÖVGÜN

Name: SOLUTIONS Date: 11/9/2017. M20550 Calculus III Tutorial Worksheet 8

Name of the Student:

EVALUATING TRIPLE INTEGRALS WITH CYLINDRICAL AND SPHERICAL COORDINATES AND THEIR APPLICATIONS

Math Vector Calculus II

C:\Users\whit\Desktop\Active\304_2012_ver_2\_Notes\4_Torsion\1_torsion.docx 6

University of Bergen. Solutions to Exam in MAT111 - Calculus 1

Engineering Mathematics I

ENGI Multiple Integration Page 8-01

Math 122 Fall Solutions to Homework #5. ( ) 2 " ln x. y = x 2

Module 02: Math Review

36. Double Integration over Non-Rectangular Regions of Type II

CHAPTER 4 VECTORS. Before we go any further, we must talk about vectors. They are such a useful tool for

Mathematics Trigonometry: Unit Circle

Transcription:

Change of Variables In Multiple Integrals

When we convert a double integral from rectangular to polar coordinates, recall the changes that must be made to, and da. = (, r θ = rcosθ θ = (, r θ = rsinθ da = r drdθ r

In the polar coordinate sstem, an element of area is generall a rectangle corresponding to a range of values for r and a range for θ. θ c θ d a r b r

However, in the coordinate sstem, this rectangle usuall takes on a different shape, and the formula for an element of area changes. ΔA r Δr Δθ θ r

his leads to the following formula for the double integral in polar coordinates. θ f (, da = f ( r cos θ, r sin θ r drdθ r

We ll now develop a general method for finding change of variable formulas such as this one. θ f (, da = f ( r cos θ, r sin θ r drdθ r

Suppose we have a rectangle in an st-coordinate sstem and a pair of functions that converts (s,t coordinates into (, coordinates. = st (, t = st (, s

Suppose also that these functions are differentiable and that the transformation from the st-coordinates to -coordinates is one-to-one. = st (, t = st (, s

hen because of differentiabilit, local linearit will be present and a small rectangle in the st sstem will be mapped onto approimatel a parallelogram in the -coordinate sstem. t = = st (, st (, s

If we add some coordinates, then it looks like this. t ( st, +Δt = = ( st, ( s+δs, t st (, s st (, ( ( s, t+ Δ t, ( s, t+δt b a ( ( s, t, ( s, t ( ( s+δ s, t, ( s+δs, t

An element of area in our -coordinate sstem is represented b a parallelogram. t ( st, +Δt = = ( st, ( s+δs, t st (, s st (, ( ( s, t+ Δ t, ( s, t+δt b a ( ( s, t, ( s, t ( ( s+δ s, t, ( s+δs, t

he area of this parallelogram is given b the norm of a cross product. Area = a b ( ( s, t+ Δ t, ( s, t+δt b a ( ( s, t, ( s, t ( ( s+δ s, t, ( s+δs, t

a = s+δs t s t i + s+δs t st ˆj Notice that, ( ( (,, ˆ ( (, (, ˆ Δ si + Δs ˆj s s b= st+δt st i+ st+δt st ˆj ( (, (, ˆ (, (, ˆ Δ ti + Δt ˆj t t ( ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t

Hence, iˆ ˆj kˆ a b Δs Δ s 0 = s t s t kˆ Δ Δ Δ Δ s s s t s t Δt Δt 0 t t ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t

And, a b Δs Δt Δs Δ t = ΔsΔt s t s t s t s t ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t

he epression inside the last absolute value sign is called the Jacobian, and it is usuall written as follows: (, s t = = (, s t s t s t s t ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t

herefore, (, (, Area =Δ A = a b ΔsΔ t = ΔsΔt s t s t s t ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t

And as a result of local linearit, this approimation improves as the changes in s and t become smaller. (, (, Area =Δ A = a b ΔsΔ t = ΔsΔt s t s t s t ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t

And finall, f(, da= lim f(, ΔA ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t ΔA 0 (, ( st, = lim f((,, s t (, s t ΔsΔt Δs, Δt 0 (, ( st, = f ( st (,, ( s, t dsdt

Now let s verif that this formula works for polar coordinates. f(, da= lim f(, ΔA ΔA 0 ( ( st ( ( st,, = lim f (, ΔsΔ t = f (, dsdt Δs, Δt 0,, ( ( st, +Δ t, ( st, +Δt b a ( ( st,, ( st, ( ( s+δ s, t, ( s+δs, t

(, ( r, θ f (, da = f ( st (,, ( st, drdθ = rcosθ = rsinθ (, r θ cosθ r sinθ = = (, r θ sinθ rcosθ r θ ( 2 2 2 2 = rcos θ + rsin θ = r cos θ + sin θ = r (, (, r θ = = r = r

herefore, (, ( r, θ f (, da= f ( rcos θ, rsin θ drdθ = f( rcos θ, rsin θ rdrdθ

Let s tr one more eample! Consider the equation below for an ellipse. a 2 2 + = b 2 2 1

he following substitution will change it into an equation for a unit circle. = a s = b t 2 2 2 2 ( a s ( b t 2 2 + = 1 + = 1 s + t = 1 2 2 2 2 a b a b

Now find the absolute value of the Jacobian. = a s = b t (, s t a 0 = = = (, st 0 b s t ab (, (, st = ab

We can now easil find the area of the ellipse. Area of ellipse= da = ab dsdt ellipse unit circle = ab dsdt = ab π = π ab unit circle

We can now easil find the area of the ellipse. Area of ellipse= da = ab dsdt ellipse unit circle = ab dsdt = ab π = π ab unit circle B the wa, another wa to arrive at the same result is to notice that: = a s d= ads dd = ab dsdt = b t d = bdt

If we have a function of three variables, then our Jacobian looks like this. s t u (, z, = (,, stu s t u z z z s t u

Find the volume of the ellipsoid. 2 2 2 + + = 1 2 2 2 z a b c

he coordinate change below transforms the ellipsoid into a unit sphere. = a s = b t z = c u 2 2 2 + + = 1 2 2 2 z a b c s t u a 0 0 ( z,, = = 0 b 0 = (,, stu s t u 0 0 c z z z s t u abc

2 2 2 + + = 1 2 2 2 z a b c ( z,, Volume= dv = dsdtdu V (,, stu = abc dsdtdu = abc dsdtdu π 4 4 = abc = 3 3 π abc

An Questions?