Examples of the Fourier Theorem (Sect. 10.3). The Fourier Theorem: Continuous case.

Similar documents
More on Fourier Series

Physics 250 Green s functions for ordinary differential equations

3 rd class Mech. Eng. Dept. hamdiahmed.weebly.com Fourier Series

Overview of Fourier Series (Sect. 6.2). Origins of the Fourier Series.

22. Periodic Functions and Fourier Series

Fourier Integral. Dr Mansoor Alshehri. King Saud University. MATH204-Differential Equations Center of Excellence in Learning and Teaching 1 / 22

Review: Power series define functions. Functions define power series. Taylor series of a function. Taylor polynomials of a function.

Solving the Heat Equation (Sect. 10.5).

Power Series Solutions We use power series to solve second order differential equations

Time-Frequency Analysis

Find the Fourier series of the odd-periodic extension of the function f (x) = 1 for x ( 1, 0). Solution: The Fourier series is.

Computer Problems for Fourier Series and Transforms

Ma 221 Eigenvalues and Fourier Series

Math 121A: Homework 6 solutions

Fourier and Partial Differential Equations

14 Fourier analysis. Read: Boas Ch. 7.

Chapter 4 Sequences and Series

Fourier Series. Department of Mathematical and Statistical Sciences University of Alberta

Ma 530 Power Series II

MAT137 Calculus! Lecture 5

f (x) = k=0 f (0) = k=0 k=0 a k k(0) k 1 = a 1 a 1 = f (0). a k k(k 1)x k 2, k=2 a k k(k 1)(0) k 2 = 2a 2 a 2 = f (0) 2 a k k(k 1)(k 2)x k 3, k=3

Functions based on sin ( π. and cos

f (t) K(t, u) d t. f (t) K 1 (t, u) d u. Integral Transform Inverse Fourier Transform

Tangent Lines Sec. 2.1, 2.7, & 2.8 (continued)

Math 3150 HW 3 Solutions

Lecture 5: Function Approximation: Taylor Series

Math Exam II Review

(c) Find the equation of the degree 3 polynomial that has the same y-value, slope, curvature, and third derivative as ln(x + 1) at x = 0.

Periodic functions: simple harmonic oscillator

The Fourier series for a 2π-periodic function

MAT137 Calculus! Lecture 6

Chapter 7: Techniques of Integration

JUST THE MATHS UNIT NUMBER DIFFERENTIATION APPLICATIONS 5 (Maclaurin s and Taylor s series) A.J.Hobson

1 + lim. n n+1. f(x) = x + 1, x 1. and we check that f is increasing, instead. Using the quotient rule, we easily find that. 1 (x + 1) 1 x (x + 1) 2 =

Taylor and Maclaurin Series

Emily Jennings. Georgia Institute of Technology. Nebraska Conference for Undergraduate Women in Mathematics, 2012

Fourier Series and the Discrete Fourier Expansion

Taylor Series. Math114. March 1, Department of Mathematics, University of Kentucky. Math114 Lecture 18 1/ 13

Math Numerical Analysis

Weighted SS(E) = w 2 1( y 1 y1) y n. w n. Wy W y 2 = Wy WAx 2. WAx = Wy. (WA) T WAx = (WA) T b

Math Review for Exam Answer each of the following questions as either True or False. Circle the correct answer.

8.5 Taylor Polynomials and Taylor Series

11.10a Taylor and Maclaurin Series

Notes on Fourier Series and Integrals Fourier Series

Math 489AB A Very Brief Intro to Fourier Series Fall 2008

X b n sin nπx L. n=1 Fourier Sine Series Expansion. a n cos nπx L 2 + X. n=1 Fourier Cosine Series Expansion ³ L. n=1 Fourier Series Expansion

Section 5.8. Taylor Series

The First Derivative and Second Derivative Test

Next, we ll use all of the tools we ve covered in our study of trigonometry to solve some equations.

7: FOURIER SERIES STEVEN HEILMAN

The First Derivative and Second Derivative Test

Study # 1 11, 15, 19

Math Assignment 14

swapneel/207

SET 1. (1) Solve for x: (a) e 2x = 5 3x

General Inner Product and The Fourier Series

`an cos nπx. n 1. L `b

Chapter 2: Functions, Limits and Continuity

THE UNIVERSITY OF WESTERN ONTARIO. Applied Mathematics 375a Instructor: Matt Davison. Final Examination December 14, :00 12:00 a.m.

MATH 162. Midterm Exam 1 - Solutions February 22, 2007

Mathematical Methods and its Applications (Solution of assignment-12) Solution 1 From the definition of Fourier transforms, we have.

Chapter 3a Topics in differentiation. Problems in differentiation. Problems in differentiation. LC Abueg: mathematical economics

Advanced Mathematics Unit 2 Limits and Continuity

Advanced Mathematics Unit 2 Limits and Continuity

Vectors in Function Spaces

1 A complete Fourier series solution

Dr. Sophie Marques. MAM1020S Tutorial 8 August Divide. 1. 6x 2 + x 15 by 3x + 5. Solution: Do a long division show your work.

Solutions. MATH 1060 Exam 3 Fall (10 points) For 2 sin(3x π) + 1 give the. amplitude. period. phase shift. vertical shift.

Differentiation and Integration of Fourier Series

What will you learn?

PHYS 502 Lecture 3: Fourier Series

Fourier Sin and Cos Series and Least Squares Convergence

3.1 Day 1: The Derivative of a Function

Math 4263 Homework Set 1

Concavity and Lines. By Ng Tze Beng

Convergence of Fourier Series

MATH 251 Final Examination May 3, 2017 FORM A. Name: Student Number: Section:

MATH 31B: MIDTERM 2 REVIEW. sin 2 x = 1 cos(2x) dx = x 2 sin(2x) 4. + C = x 2. dx = x sin(2x) + C = x sin x cos x

Learning Objectives for Math 165

Math 5 Trigonometry Chapter 4 Test Fall 08 Name Show work for credit. Write all responses on separate paper. Do not use a calculator.

The moral of the story regarding discontinuities: They affect the rate of convergence of Fourier series

Math 1431 Final Exam Review

Chapter 17. Fourier series

MA 201: Differentiation and Integration of Fourier Series Applications of Fourier Series Lecture - 10

Bessel s Equation. MATH 365 Ordinary Differential Equations. J. Robert Buchanan. Fall Department of Mathematics

Mathematics for Engineers II. lectures. Power series, Fourier series

Fourier Transform in Image Processing. CS/BIOEN 6640 U of Utah Guido Gerig (slides modified from Marcel Prastawa 2012)

Chapter 10: Partial Differential Equations

Fourier Series. Fourier Transform

Advanced Calculus Math 127B, Winter 2005 Solutions: Final. nx2 1 + n 2 x, g n(x) = n2 x

Notes for the Physics-Based Calculus workshop

Practice Problems: Integration by Parts

Lecture 16: Bessel s Inequality, Parseval s Theorem, Energy convergence

0 3 x < x < 5. By continuing in this fashion, and drawing a graph, it can be seen that T = 2.

8.8 Applications of Taylor Polynomials

McGill University Math 354: Honors Analysis 3

Math 180, Final Exam, Fall 2012 Problem 1 Solution

David A. Stephens Department of Mathematics and Statistics McGill University. October 28, 2006

Calculus II Practice Test 1 Problems: , 6.5, Page 1 of 10

Cotangent and the Herglotz trick

Transcription:

s of the Fourier Theorem (Sect. 1.3. The Fourier Theorem: Continuous case. : Using the Fourier Theorem. The Fourier Theorem: Piecewise continuous case. : Using the Fourier Theorem. The Fourier Theorem: Continuous case. Theorem (Fourier Series If the function f : [, R R is continuous, then f can be expressed as an infinite series f (x = a + [ ( x a n cos with the constants a n and b n given by a n = 1 b n = 1 ( x f (x cos ( x f (x sin ( x + b n sin dx, n, dx, n 1. Furthermore, the Fourier series in Eq. (?? provides a -periodic extension of f from the domain [, R to R. (1

The Fourier Theorem: Continuous case. Sketch of the Proof: Define the partial sum functions f N (x = a N [ ( x + a n cos with a n and b n given by a n = 1 ( x f (x cos b n = 1 ( x f (x sin ( x + b n sin dx, n, dx, n 1. Express f N as a convolution of Sine, Cosine, functions and the original function f. Use the convolution properties to show that lim f N(x = f (x, N x [,. s of the Fourier Theorem (Sect. 1.3. The Fourier Theorem: Continuous case. : Using the Fourier Theorem. The Fourier Theorem: Piecewise continuous case. : Using the Fourier Theorem.

: Using the Fourier Theorem. f (x = 1 + x x [,, 1 x x [, 1. Solution: In this case = 1. The Fourier series expansion is f (x = a + [ an cos(x + b n sin(x, where the a n, b n are given in the Theorem. We start with a, a = f (x dx = (1 + x dx + (1 x dx. a = (x + x ( + x x 1 (1 = 1 + ( 1 1 We obtain: a = 1. : Using the Fourier Theorem. f (x = 1 + x x [,, 1 x x [, 1. Solution: Recall: a = 1. Similarly, the rest of the a n are given by, a n = Recall the integrals a n = (1 + x cos(x dx + f (x cos(x dx cos(x dx = 1 (1 x cos(x dx. sin(x, and x cos(x dx = x sin(x + 1 n π cos(x.

: Using the Fourier Theorem. f (x = 1 + x x [,, 1 x x [, 1. Solution: It is not difficult to see that a n = 1 sin(x + [ x sin(x + 1 n π cos(x + 1 sin(x 1 [ x sin(x + 1 n π cos(x 1 a n = [ 1 n π 1 [ 1 n π cos( n π cos( 1 n π. We then conclude that a n = n π [ 1 cos(. : Using the Fourier Theorem. f (x = 1 + x x [,, 1 x x [, 1. Solution: Recall: a = 1, and a n = n π [ 1 cos(. Finally, we must find the coefficients b n. A similar calculation shows that b n =. Then, the Fourier series of f is given by f (x = 1 + n π [ 1 cos( cos(x.

: Using the Fourier Theorem. f (x = 1 + x x [,, 1 x x [, 1. Solution: Recall: f (x = 1 + n π [ 1 cos( cos(x. We can obtain a simpler expression for the Fourier coefficients a n. Recall the relations cos( = ( n, then f (x = 1 + f (x = 1 + n π [ 1 ( n cos(x. n π [ 1 + ( n+1 cos(x. : Using the Fourier Theorem. f (x = 1 + x x [,, 1 x x [, 1. Solution: Recall: f (x = 1 + n π [ 1 + ( n+1 cos(x. If n = k, so n is even, so n + 1 = k + 1 is odd, then a k = (k π (1 1 a k =. If n = k 1, so n is odd, so n + 1 = k is even, then a k = (k 1 π (1 + 1 a 4 k = (k 1 π.

: Using the Fourier Theorem. f (x = 1 + x x [,, 1 x x [, 1. Solution: Recall: f (x = 1 + n π [ 1 + ( n+1 cos(x, and a k =, a k = 4 (k 1 π. We conclude: f (x = 1 + k=1 4 (k 1 cos((k 1πx. π s of the Fourier Theorem (Sect. 1.3. The Fourier Theorem: Continuous case. : Using the Fourier Theorem. The Fourier Theorem: Piecewise continuous case. : Using the Fourier Theorem.

The Fourier Theorem: Piecewise continuous case. Recall: Definition A function f : [a, b R is called piecewise continuous iff holds, (a [a, b can be partitioned in a finite number of sub-intervals such that f is continuous on the interior of these sub-intervals. (b f has finite limits at the endpoints of all sub-intervals. The Fourier Theorem: Piecewise continuous case. Theorem (Fourier Series If f : [, R R is piecewise continuous, then the function f F (x = a + [ ( x ( x a n cos + b n sin where a n and b n given by a n = 1 ( x f (x cos b n = 1 ( x f (x sin satisfies that: dx, n, dx, n 1. (a f F (x = f (x for all x where f is continuous; (b f F (x = 1 lim [ x x + discontinuous. f (x + lim x x f (x for all x where f is

s of the Fourier Theorem (Sect. 1.3. The Fourier Theorem: Continuous case. : Using the Fourier Theorem. The Fourier Theorem: Piecewise continuous case. : Using the Fourier Theorem. : Using the Fourier Theorem. Find the Fourier series of f (x = and periodic with period T =. 1 x [,, 1 x [, 1. Solution: We start computing the Fourier coefficients b n ; b n = 1 ( x f (x sin dx, = 1, b n = b n = ( ( sin ( x dx + [ cos(x + 1 (1 sin ( x dx, [ cos(x b n = ( [ 1 [ + cos( + cos( + 1. 1,

: Using the Fourier Theorem. Find the Fourier series of f (x = and periodic with period T =. 1 x [,, 1 x [, 1. Solution: b n = ( [ 1 [ + cos( + cos( + 1. b n = 1 [ [ 1 cos( cos( + 1 = 1 cos(, We obtain: b n = [ 1 ( n. If n = k, then b k = kπ If n = k 1, then b k = hence b k = 4 (k 1π. [ 1 ( k, hence b k =. [ 1 ( k, (k 1π : Using the Fourier Theorem. Find the Fourier series of f (x = and periodic with period T =. Solution: Recall: b k =, and b k = a n = a n = 1 a n = ( ( x f (x cos ( cos ( x dx + [ sin(x 1 x [,, 1 x [, 1. 4 (k 1π. dx, = 1, + 1 (1 cos ( x dx, [ sin(x a n = ( [ 1 [ sin( + sin( 1, a n =.

: Using the Fourier Theorem. Find the Fourier series of f (x = and periodic with period T =. Solution: Recall: b k =, b k = Therefore, we conclude that 1 x [,, 1 x [, 1. 4 (k 1π, and a n =. f F (x = 4 π k=1 1 (k 1 sin( (k 1π x.