Legendre s Equation. PHYS Southern Illinois University. October 18, 2016

Similar documents
Legendre s Equation. PHYS Southern Illinois University. October 13, 2016

Power Series Solutions to the Legendre Equation

Power Series Solutions to the Legendre Equation

Function Space and Convergence Types

Solving Differential Equations Using Power Series

Solving Differential Equations Using Power Series

Math Assignment 11

Integer-Valued Polynomials

LEGENDRE POLYNOMIALS AND APPLICATIONS. We construct Legendre polynomials and apply them to solve Dirichlet problems in spherical coordinates.

14 EE 2402 Engineering Mathematics III Solutions to Tutorial 3 1. For n =0; 1; 2; 3; 4; 5 verify that P n (x) is a solution of Legendre's equation wit

Simplifying Rational Expressions and Functions

BMT 2016 Orthogonal Polynomials 12 March Welcome to the power round! This year s topic is the theory of orthogonal polynomials.

Chapter 4. Series Solutions. 4.1 Introduction to Power Series

Additional Practice Lessons 2.02 and 2.03

Section 5.3, Exercise 22

Georgia Department of Education Common Core Georgia Performance Standards Framework CCGPS Advanced Algebra Unit 2

x 9 or x > 10 Name: Class: Date: 1 How many natural numbers are between 1.5 and 4.5 on the number line?

CYK\2010\PH402\Mathematical Physics\Tutorial Find two linearly independent power series solutions of the equation.

Analysis I (Math 121) First Midterm Correction

12d. Regular Singular Points

Chapter 5.3: Series solution near an ordinary point

Background and Definitions...2. Legendre s Equation, Functions and Polynomials...4 Legendre s Associated Equation and Functions...

CSCE 222 Discrete Structures for Computing. Dr. Hyunyoung Lee

Electromagnetism HW 1 math review

A-2. Polynomials and Factoring. Section A-2 1

LEAST SQUARES APPROXIMATION

Introduction to Orthogonal Polynomials: Definition and basic properties

CSE 421 Algorithms. T(n) = at(n/b) + n c. Closest Pair Problem. Divide and Conquer Algorithms. What you really need to know about recurrences

Mathematical Induction Assignments

Chapter 1 Divide and Conquer Algorithm Theory WS 2016/17 Fabian Kuhn

4 Linear Recurrence Relations & the Fibonacci Sequence

Problem Set 5 Solutions

A101 ASSESSMENT Quadratics, Discriminant, Inequalities 1

Notes on Continued Fractions for Math 4400

Sec 4.1 Limits, Informally. When we calculated f (x), we first started with the difference quotient. f(x + h) f(x) h

Outline. We will cover (over the next few weeks) Induction Strong Induction Constructive Induction Structural Induction

Approximation theory

ENGI 9420 Lecture Notes 1 - ODEs Page 1.01

PHYS 404 Lecture 1: Legendre Functions

swapneel/207

ADDITONAL MATHEMATICS

arithmetic properties of weighted catalan numbers

Two special equations: Bessel s and Legendre s equations. p Fourier-Bessel and Fourier-Legendre series. p

Chapter 4: Interpolation and Approximation. October 28, 2005

1 Examples of Weak Induction

MADHAVA MATHEMATICS COMPETITION, December 2015 Solutions and Scheme of Marking

IB Mathematics HL Year 2 Unit 11: Completion of Algebra (Core Topic 1)

PUTNAM PROBLEMS SEQUENCES, SERIES AND RECURRENCES. Notes

Homework 8 Solutions to Selected Problems

EXAMPLES OF PROOFS BY INDUCTION

Bessel s and legendre s equations

Scientific Computing

In Exercises 1 12, list the all of the elements of the given set. 2. The set of all positive integers whose square roots are less than or equal to 3

Generating Functions (Revised Edition)

Power series solutions for 2nd order linear ODE s (not necessarily with constant coefficients) a n z n. n=0

MA2501 Numerical Methods Spring 2015

Chapter 2 notes from powerpoints

Problems in Algebra. 2 4ac. 2a

Chapter 1 Divide and Conquer Polynomial Multiplication Algorithm Theory WS 2015/16 Fabian Kuhn

AP Calculus Chapter 9: Infinite Series

Polynomials. In many problems, it is useful to write polynomials as products. For example, when solving equations: Example:

Review for Exam 2. Review for Exam 2.

The Sommerfeld Polynomial Method: Harmonic Oscillator Example

Fall 2017 Test II review problems

Series Solutions. 8.1 Taylor Polynomials

(2) Dividing both sides of the equation in (1) by the divisor, 3, gives: =

Chapter 5.2: Series solution near an ordinary point

CALCULUS JIA-MING (FRANK) LIOU

SPECTRAL METHODS: ORTHOGONAL POLYNOMIALS

Math221: HW# 7 solutions

10.1 Sequences. Example: A sequence is a function f(n) whose domain is a subset of the integers. Notation: *Note: n = 0 vs. n = 1.

Generating Orthogonal Polynomials and their Derivatives using Vertex Matching-Partitions of Graphs

Roots and Coefficients Polynomials Preliminary Maths Extension 1

Section 5.2 Series Solution Near Ordinary Point

1 Boas, problem p.564,

Generating Functions

2-7 Solving Quadratic Inequalities. ax 2 + bx + c > 0 (a 0)

Some Applications of the Euler-Maclaurin Summation Formula

Methods of Mathematical Physics X1 Homework 3 Solutions

1 Direct Proofs Technique Outlines Example Implication Proofs Technique Outlines Examples...

Chapter 5: The Integers

17.2 Nonhomogeneous Linear Equations. 27 September 2007

Mathematical Induction

5.1 - Polynomials. Ex: Let k(x) = x 2 +2x+1. Find (and completely simplify) the following: (a) k(1) (b) k( 2) (c) k(a)

PHYS 502 Lecture 8: Legendre Functions. Dr. Vasileios Lempesis

5-3 Study Guide and Intervention

Connection to Laplacian in spherical coordinates (Chapter 13)

Modern Algebra Lecture Notes: Rings and fields set 6, revision 2

Lecture Note 3: Polynomial Interpolation. Xiaoqun Zhang Shanghai Jiao Tong University

PUTNAM TRAINING POLYNOMIALS. Exercises 1. Find a polynomial with integral coefficients whose zeros include

OCR Maths FP1. Topic Questions from Papers. Roots of Polynomial Equations

Principle of Mathematical Induction

FFTs in Graphics and Vision. Homogenous Polynomials and Irreducible Representations

Procedure for Graphing Polynomial Functions

Problemen. x = 2X 3 y = 2Y 4

Unit 2 Rational Functionals Exercises MHF 4UI Page 1

Nonlinear Integral Equation Formulation of Orthogonal Polynomials

Recurrence Relations

Ma 530 Power Series II

APPENDIX B GRAM-SCHMIDT PROCEDURE OF ORTHOGONALIZATION. Let V be a finite dimensional inner product space spanned by basis vector functions

Transcription:

Legendre s Equation PHYS 500 - Southern Illinois University October 18, 2016 PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 1 / 11

Legendre s Equation Recall We are trying to find solutions to the equation (1 x 2 )P 2xP + l(l + 1)P = 0. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 2 / 11

Legendre s Equation Recall We are trying to find solutions to the equation (1 x 2 )P 2xP + l(l + 1)P = 0. We have taken P(x) = k=0 a kx k and derived a recursion relation on the coefficients: (k + 1)(k + 2)a k+2 = [(k + 1)k l(l + 1)]a k. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 2 / 11

Legendre s Equation Recall We are trying to find solutions to the equation (1 x 2 )P 2xP + l(l + 1)P = 0. We have taken P(x) = k=0 a kx k and derived a recursion relation on the coefficients: (k + 1)(k + 2)a k+2 = [(k + 1)k l(l + 1)]a k. This leads to two classes of bounded solutions. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 2 / 11

Legendre s Equation Even Solutions { 0 for odd k a k = k 1 j=1 [(2j + 1)2j l(l + 1)] a 0 (2k)! for even k. For a finite solution l = 2n for some non-negative integer n. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 3 / 11

Legendre s Equation Even Solutions { 0 for odd k a k = k 1 j=1 [(2j + 1)2j l(l + 1)] a 0 (2k)! for even k. For a finite solution l = 2n for some non-negative integer n. Odd Solutions a k = { 0 for even k k j=1 [2j(2j 1) l(l + 1)] a 1 (2k+1)! for odd k. For a finite solution l = 2n 1 for some positive integer n. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 3 / 11

Legendre s Equation Even Solutions : P n (x) = Odd Solutions : P n (x) = a k x k = a k x k = a 2k x 2k k=0 even k a k x k = a k x k = k=0 k=0 odd k k=0 a 2k+1 x 2k+1. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 4 / 11

Legendre s Equation Even Solutions : P n (x) = Odd Solutions : P n (x) = a k x k = a k x k = a 2k x 2k k=0 even k a k x k = a k x k = k=0 k=0 odd k k=0 Consider again the recurrence relation (k + 1)(k + 2)a k+2 = [(k + 1)k l(l + 1)]a k. a 2k+1 x 2k+1. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 4 / 11

Legendre s Equation Even Solutions : P n (x) = Odd Solutions : P n (x) = a k x k = a k x k = a 2k x 2k k=0 even k a k x k = a k x k = k=0 k=0 odd k k=0 Consider again the recurrence relation (k + 1)(k + 2)a k+2 = [(k + 1)k l(l + 1)]a k. a 2k+1 x 2k+1. l = n : (k + 1)(k + 2)a k+2 = [(k + 1)k n(n + 1)]a k. a k+2 = 0 for k > n. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 4 / 11

Legendre s Equation Therefore, we just focus on k < n. Let k = n 2j. Then (n 2j + 1)(n 2j + 2) a n 2j = (n 2j + 1)(n 2j) n(n + 1) a n 2j+2, = (n 2j + 1)(n 2j + 2) a n 2j+2, j = 1, 2,, n (2j)(2n 2j + 1) 2. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 5 / 11

Legendre Polynomials (n 1)(n) a n 2 = (2)(2n 1) a n (n 3)(n 2) a n 4 = (4)(2n 3) a n 2 2 (n 3)(n 2) (n 1)(n) = ( 1) (4)(2n 3) (2)(2n 1) a n a n 2j = ( 1)j 2 j j! n(n 1)(n 2) (n 2j + 1) (2n 1)(2n 3) (2n 2j + 1) a n j = 1, 2,, n 2. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 6 / 11

Legendre Polynomials Therefore P n (x) := n 2 j=0 ( 1) j 2 j j! n(n 1)(n 2) (n 2j + 1) (2n 1)(2n 3) (2n 2j + 1) a nx n 2j. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 7 / 11

Legendre Polynomials Therefore P n (x) := n 2 j=0 ( 1) j 2 j j! n(n 1)(n 2) (n 2j + 1) (2n 1)(2n 3) (2n 2j + 1) a nx n 2j. The polynomials P n are called the Legendre Polynomials. The factor a n is customarily chosen so that P n (1) = 1. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 7 / 11

Legendre Polynomials Therefore P n (x) := n 2 j=0 ( 1) j 2 j j! n(n 1)(n 2) (n 2j + 1) (2n 1)(2n 3) (2n 2j + 1) a nx n 2j. The polynomials P n are called the Legendre Polynomials. The factor a n is customarily chosen so that P n (1) = 1. The n th Legendre Polynomial P n (x) is the only bounded polynomial solution to Legendre s Equation (1 x 2 )P 2xP + n(n + 1)P = 0 that satisfies P n (1) = 1. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 7 / 11

Rodrigues Formula Theorem. The Legendre Polynomials are equivalently given by the formula d n P n (x) = 1 2 n n! dx n (x 2 1) n. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 8 / 11

Rodrigues Formula Theorem. The Legendre Polynomials are equivalently given by the formula d n P n (x) = 1 2 n n! dx n (x 2 1) n. Proof Idea: Let y = (x 2 1) n. Show that y (n) satisfies Legendre s Equation (1 x 2 )P 2xP + n(n + 1)P = 0. We will also need to use the following Lemma, which is a higher-order form of the product rule. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 8 / 11

Rodrigues Formula Theorem. The Legendre Polynomials are equivalently given by the formula d n P n (x) = 1 2 n n! dx n (x 2 1) n. Proof Idea: Let y = (x 2 1) n. Show that y (n) satisfies Legendre s Equation (1 x 2 )P 2xP + n(n + 1)P = 0. We will also need to use the following Lemma, which is a higher-order form of the product rule. Lemma. For any functions a(x) and b(x) and any integer k, d k dx k [ab] = k ( ) k a (l) b (k l). l l=0 PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 8 / 11

Rodrigues Formula Proof of Lemma Prove by induction and use the relations ( ( k l 1) + k ) ( l = k+1 ) l, ( k ( k) = ( k+1), and k ) ( 0 = k+1 ) 0. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 9 / 11

Rodrigues Formula Proof of Lemma Prove by induction and use the relations ( ( k l 1) + k ) ( l = k+1 ) l, ( k ( k) = ( k+1), and k ) ( 0 = k+1 ) 0. Proof of Rodrigues Formula First note the equality (x 2 1)y = 2nxy. Then differentiate both sides n + 1 times. This gives us (1 x 2 )[y (n) ] 2x[y (n) ] + n(n + 1)y (n) = 0. PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 9 / 11

Rodrigues Formula Proof of Lemma Prove by induction and use the relations ( ( k l 1) + k ) ( l = k+1 ) l, ( k ( k) = ( k+1), and k ) ( 0 = k+1 ) 0. Proof of Rodrigues Formula First note the equality (x 2 1)y = 2nxy. Then differentiate both sides n + 1 times. This gives us (1 x 2 )[y (n) ] 2x[y (n) ] + n(n + 1)y (n) = 0. 1 The last step is to verify that 2 n n! y (n) (1) = 1. Since P n (x) is the only bounded polynomial solution to Legendre s equation with P n (1) = 1, we have that P n (x) = 1 2 n n! y (n) (x) = 1 d n 2 n n! dx (x 2 1) n. n PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 9 / 11

Legendre Polynomials We have the equality P n (x) = n 2 j=0 ( 1) j 2 j j! d n = 1 2 n n! dx n (x 2 1) n. n(n 1)(n 2) (n 2j + 1) (2n 1)(2n 3) (2n 2j + 1) a nx n 2j PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 10 / 11

Legendre Polynomials We have the equality P n (x) = n 2 j=0 ( 1) j 2 j j! d n = 1 2 n n! dx n (x 2 1) n. n(n 1)(n 2) (n 2j + 1) (2n 1)(2n 3) (2n 2j + 1) a nx n 2j Use this to find the constant a n. Compare the coefficients of x n : d n a n = 1 2 n n! dx n x 2n = 1 2 n n! (2n)!. n! PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 10 / 11

Legendre Polynomials We have the equality P n (x) = n 2 j=0 ( 1) j 2 j j! d n = 1 2 n n! dx n (x 2 1) n. n(n 1)(n 2) (n 2j + 1) (2n 1)(2n 3) (2n 2j + 1) a nx n 2j Use this to find the constant a n. Compare the coefficients of x n : d n a n = 1 2 n n! dx n x 2n = 1 2 n n! a n = (2n)! 2 n (n!) 2. (2n)!. n! PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 10 / 11

Legendre Polynomials P 0 (x) = 1 P 1 (x) = x P 2 (x) = 1 2 (3x 2 1) P 3 (x) = 1 2 (5x 3 3x) P 4 (x) = 1 8 (35x 4 30x 2 + 3) PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 11 / 11