Spherical Coordinates

Σχετικά έγγραφα
Integrals in cylindrical, spherical coordinates (Sect. 15.7)

Answer sheet: Third Midterm for Math 2339

Homework 8 Model Solution Section

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r(t) = 3cost, 4t, 3sint

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

CYLINDRICAL & SPHERICAL COORDINATES

Areas and Lengths in Polar Coordinates

Parametrized Surfaces

Areas and Lengths in Polar Coordinates

Appendix A. Curvilinear coordinates. A.1 Lamé coefficients. Consider set of equations. ξ i = ξ i (x 1,x 2,x 3 ), i = 1,2,3

Problem 3.1 Vector A starts at point (1, 1, 3) and ends at point (2, 1,0). Find a unit vector in the direction of A. Solution: A = 1+9 = 3.

Section 8.2 Graphs of Polar Equations

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

Double Integrals, Iterated Integrals, Cross-sections

CURVILINEAR COORDINATES

CHAPTER 70 DOUBLE AND TRIPLE INTEGRALS. 2 is integrated with respect to x between x = 2 and x = 4, with y regarded as a constant

D Alembert s Solution to the Wave Equation

Equations. BSU Math 275 sec 002,003 Fall 2018 (Ultman) Final Exam Notes 1. du dv. FTLI : f (B) f (A) = f dr. F dr = Green s Theorem : y da

Problem 3.16 Given B = ˆx(z 3y) +ŷ(2x 3z) ẑ(x+y), find a unit vector parallel. Solution: At P = (1,0, 1), ˆb = B

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

11.4 Graphing in Polar Coordinates Polar Symmetries

Approximation of distance between locations on earth given by latitude and longitude

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

28.3. Orthogonal Curvilinear Coordinates. Introduction. Prerequisites. Learning Outcomes

Solutions to Exercise Sheet 5

Reminders: linear functions

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Geodesic Equations for the Wormhole Metric

ECE 468: Digital Image Processing. Lecture 8

28.3. Orthogonal Curvilinear Coordinates. Introduction. Prerequisites. Learning Outcomes

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

Laplace s Equation on a Sphere

10/3/ revolution = 360 = 2 π radians = = x. 2π = x = 360 = : Measures of Angles and Rotations

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2

Section 9.2 Polar Equations and Graphs

AREAS AND LENGTHS IN POLAR COORDINATES. 25. Find the area inside the larger loop and outside the smaller loop

3.5 - Boundary Conditions for Potential Flow

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

Section 8.3 Trigonometric Equations

SPECIAL FUNCTIONS and POLYNOMIALS

16 MULTIPLE INTEGRALS ET 15

Tutorial Note - Week 09 - Solution

CHAPTER (2) Electric Charges, Electric Charge Densities and Electric Field Intensity

Trigonometry 1.TRIGONOMETRIC RATIOS

Matrices and Determinants

Written Examination. Antennas and Propagation (AA ) April 26, 2017.

Exercise 1.1. Verify that if we apply GS to the coordinate basis Gauss form ds 2 = E(u, v)du 2 + 2F (u, v)dudv + G(u, v)dv 2

Solution to Review Problems for Midterm III

Partial Differential Equations in Biology The boundary element method. March 26, 2013

Dr. D. Dinev, Department of Structural Mechanics, UACEG

derivation of the Laplacian from rectangular to spherical coordinates

Variational Wavefunction for the Helium Atom

Differentiation exercise show differential equation

ST5224: Advanced Statistical Theory II

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Trigonometric Formula Sheet

physicsandmathstutor.com Paper Reference Core Mathematics C4 Advanced Level Tuesday 23 January 2007 Afternoon Time: 1 hour 30 minutes

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

Laplace s Equation in Spherical Polar Coördinates

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Orbital angular momentum and the spherical harmonics

On a four-dimensional hyperbolic manifold with finite volume

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

CRASH COURSE IN PRECALCULUS

EE512: Error Control Coding

Rectangular Polar Parametric

Parallel transport and geodesics

PARTIAL NOTES for 6.1 Trigonometric Identities

(As on April 16, 2002 no changes since Dec 24.)

Second Order Partial Differential Equations

Other Test Constructions: Likelihood Ratio & Bayes Tests

Math221: HW# 1 solutions

Lecture 26: Circular domains

2 Composition. Invertible Mappings

Chapter 7 Transformations of Stress and Strain

If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2

Homework 3 Solutions

If we restrict the domain of y = sin x to [ π 2, π 2

Strain gauge and rosettes

Topic 4. Linear Wire and Small Circular Loop Antennas. Tamer Abuelfadl

r t te 2t i t Find the derivative of the vector function. 19. r t e t cos t i e t sin t j ln t k Evaluate the integral.

Lecture 21: Scattering and FGR

Space Physics (I) [AP-3044] Lecture 1 by Ling-Hsiao Lyu Oct Lecture 1. Dipole Magnetic Field and Equations of Magnetic Field Lines

1 String with massive end-points

Lifting Entry (continued)

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS

2x 2 y x 4 +y 2 J (x, y) (0, 0) 0 J (x, y) = (0, 0) I ϕ(t) = (t, at), ψ(t) = (t, t 2 ), a ÑL<ÝÉ b, ½-? A? 2t 2 at t 4 +a 2 t 2 = lim

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Jackson 2.25 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

1. Consider the three dimensional space with the line element. Determine the surface area of the sphere that corresponds to r = R.

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Lifting Entry 2. Basic planar dynamics of motion, again Yet another equilibrium glide Hypersonic phugoid motion MARYLAND U N I V E R S I T Y O F

Statistical Inference I Locally most powerful tests

Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Lecture 15 - Root System Axiomatics

New bounds for spherical two-distance sets and equiangular lines

Transcript:

Spherical Coordinates MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Fall 2011

Spherical Coordinates Another means of locating points in three-dimensional space is known as the spherical coordinate system. z 0,0,z y x,y,z Φ Θ Ρ x,y,0 x

Coordinate Definitions If the point P has Cartesian coordinates (x, y, z), the points spherical coordinates (ρ, φ, θ) are as follows: ρ: the distance from the origin O to P. ρ = x 2 + y 2 + z 2 0 φ: the angle between vector x, y, z and the positive z-axis. ( ) 0 φ = cos 1 z π x 2 + y 2 + z 2 θ: the angle between vector x, y, 0 and the positive x-axis. ( ) θ = cos 1 x x 2 + y 2

Converting from Spherical to Cartesian Coordinates Given the spherical coordinates (ρ, φ, θ), x = ρ sin φ cos θ y = ρ sin φ sin θ z = ρ cos φ.

Converting from Spherical to Cylindrical Coordinates Given the spherical coordinates (ρ, φ, θ), r = ρ sin φ θ = θ z = ρ cos φ.

Example (1 of 6) If point P has spherical coordinates (ρ, φ, θ) = (2, π/4, π/3), find the coordinates of P in 1 Cartesian coordinates. 2 Cylindrical coordinates.

Example (2 of 6) 1 Cartesian coordinates: x = ρ sin φ cos θ = 2 sin π 4 cos π 3 = 1 2 y = ρ sin φ sin θ = 2 sin π 4 sin π 3 = 3 2 z = ρ cos φ = 2 cos π 4 = 2 2 Cylindrical coordinates: r = ρ sin φ = 2 sin π 4 = 2 θ = θ = π 3 z = ρ cos φ = 2 cos π 4 = 2

Example (3 of 6) If point P has Cartesian coordinates (x, y, z) = (0, 2 3, 2), find the coordinates of P in 1 Spherical coordinates. 2 Cylindrical coordinates.

Example (4 of 6) 1 Spherical coordinates: ρ = x 2 + y 2 + z 2 = 0 2 + (2 3) 2 + ( 2) 2 = 4 ( ) ( φ = cos 1 z = cos 1 2 ) = 2π x 2 + y 2 + z 2 4 3 ( ) θ = cos 1 x = cos 1 (0) = π x 2 + y 2 2 2 Cylindrical coordinates: r = x 2 + y 2 = 0 2 + (2 3) 2 = 2 3 ( ) θ = cos 1 x = cos 1 (0) = π x 2 + y 2 2 z = z = 2

Example (5 of 6) Find the equation in spherical coordinates of the hyperboloid of 2 sheets: x 2 y 2 z 2 = 1.

Example (5 of 6) Find the equation in spherical coordinates of the hyperboloid of 2 sheets: x 2 y 2 z 2 = 1. 1 = x 2 y 2 z 2 = ρ 2 sin 2 φ cos 2 θ ρ 2 sin 2 φ sin 2 θ ρ 2 cos 2 ( φ ) = ρ 2 sin 2 φ cos 2 θ sin 2 φ sin 2 θ cos 2 φ ( [ ] ) = ρ 2 sin 2 φ cos 2 θ sin 2 θ cos 2 φ ( ) = ρ 2 sin 2 φ cos 2θ cos 2 φ

Example (6 of 6) Find the equation in Cartesian coordinates of the surface whose equation in spherical coordinates is ρ = sin φ sin θ.

Example (6 of 6) Find the equation in Cartesian coordinates of the surface whose equation in spherical coordinates is ρ = sin φ sin θ. ρ = sin φ sin θ ρ 2 = ρ sin φ sin θ x 2 + y 2 + z 2 = y ( x 2 + y 1 ) 2 + z 2 = 1 2 4

Spherical Coordinate Equations (1 of 3) Sphere: ρ = c > 0, a constant y z x x 2 + y 2 + z 2 = c 2

Spherical Coordinate Equations (2 of 3) Plane: θ = θ 0, with 0 θ 0 2π z y x

Spherical Coordinate Equations (3 of 3) Cone: φ = φ 0, with 0 < φ 0 < π z y x

Volume Element in Spherical Coordinates 2.0 1.5 1.0 0.5 2.0 0.0 1.5 1.0 0.5 0.0 0.0 0.5 1.0 1.5 2.0 V (ρ sin φ θ)(ρ φ)( ρ) = ρ 2 sin φ ρ φ θ dv = ρ 2 sin φ dρ dφ dθ

Iterated Integrals in Spherical Coordinates The triple integral of f (ρ, φ, θ) over the solid region Q = {(ρ, φ, θ) g 1 (φ, θ) ρ g 2 (φ, θ), h 1 (θ) φ h 2 (θ), α θ β} is Q f (ρ, φ, θ) dv = β h2 (θ) g2 (φ,θ) α h 1 (θ) g 1 (φ,θ) f (ρ, φ, θ)ρ 2 sin φ dρ dφ dθ.

Examples (1 of 9) Evaluate the triple integral below by converting to spherical coordinates. e (x 2 +y 2 +z 2 ) 3/2 dv where Q = {(x, y, z) x 2 + y 2 + z 2 1}. Q

Examples (2 of 9) Q e (x 2 +y 2 +z 2 ) 3/2 dv = = 2π = 2π 2π π 1 0 0 0 π 1 0 π 0 1 e (ρ2 ) 3/2 ρ 2 sin φ dρ dφ dθ ρ 2 e ρ3 sin φ dρ dφ 1 0 3 eρ3 0 π sin φ dφ = 2π 1 (e 1) sin φ dφ 0 3 = 2(e 1)π ( cos φ) π 0 3 = 4(e 1)π 3

Examples (3 of 9) Find the volume of the solid that lies above the cone z 2 = x 2 + y 2 and below the sphere x 2 + y 2 + z 2 = z. y 0.0 0.5 1.0 0.5 z 0.5 0.0 0.5 0.0 x 0.5

Example (4 of 9) In spherical coordinates the equations of the cone and the sphere are Cone: φ = π 4 Sphere: ρ = cos φ.

Example (5 of 9) V = = 2π = 2π = 2π 3 = 2π 3 1 dv = Q 0 π/4 cos φ 0 π/4 0 1 0 3 ρ3 0 π/4 0 1/ 2 = π 1 6 u4 1/ = π 2 8 1 2π π/4 cos φ 0 0 ρ 2 sin φ dρ dφ cos φ sin φ dφ cos 3 φ sin φ dφ u 3 du = 2π 3 1 1/ 2 (1)ρ 2 sin φ dρ dφ dθ u 3 du

Examples (6 of 9) Find the mass and center of mass of the solid hemisphere of radius a if the density at any point in the solid is proportional to its distance from the base. z y J. Robert Buchanan x Spherical Coordinates

Examples (7 of 9) The distance of a point in the hemisphere from the base is the z-coordinate of the point. In spherical coordinates z = ρ cos φ. Without loss of generality, we may choose the proportionality constant to be 1. m = M yz = M xz = M xy = Q Q Q Q z dv x z dv y z dv z 2 dv

Examples (8 of 9) m = M xy = = 2π 2π π/2 a = πa4 2 = 2π 0 0 0 π/2 a 0 0 π/2 0 2π π/2 a = 2πa5 5 0 0 0 π/2 a = 2πa5 5 0 0 π/2 0 0 (ρ cos φ)ρ 2 sin φ dρ dφ dθ ρ 3 cos φ sin φ dρ dφ cos φ sin φ dφ = πa4 2 1 (ρ cos φ) 2 ρ 2 sin φ dρ dφ dθ ρ 4 cos 2 φ sin φ dρ dφ cos 2 φ sin φ dφ u 2 du = 2πa5 5 1 1 0 0 u du = πa4 4 u 2 du = 2πa5 15

Examples (9 of 9) M yz = = M xz = = = 0 = 0 2π π/2 a 0 0 0 a π/2 2π 0 0 0 2π π/2 a 0 0 0 a π/2 2π 0 0 0 (ρ sin φ cos θ)ρ 2 sin φ dρ dφ dθ ρ 3 sin 2 φ cos θ dθ dφ dρ (ρ sin φ sin θ)ρ 2 sin φ dρ dφ dθ ρ 3 sin 2 φ sin θ dθ dφ dρ Thus (x, y, z) = ( Myz m, M xz m, M ) ( xy = 0, 0, 8a ). m 15

Homework Read Section 13.7. Exercises: 1 57 odd