Module

for

Fourier Series

 

Chapter 12  Fourier Series and the Laplace Transform

12.1  Fourier Series

Overview

    In this chapter we show how Fourier Series, the Fourier Transform, and the Laplace Transform are related to the study of complex analysis.  

First, we will introduce the Fourier series for a real-valued function  [Graphics:Images/FourierSeriesComplexMod_gr_1.gif]  of the real variable  [Graphics:Images/FourierSeriesComplexMod_gr_2.gif].  Then we discuss Fourier transforms.  

Finally, we develop the Laplace transform and the complex variable techniques for finding its inverse.

Our goal is to apply these ideas to solving problems, so many of the theorems are stated without proof.

Background

    Let  [Graphics:Images/FourierSeriesComplexMod_gr_3.gif]  be a real-valued function that is periodic with period  [Graphics:Images/FourierSeriesComplexMod_gr_4.gif],  that is

            [Graphics:Images/FourierSeriesComplexMod_gr_5.gif].

One such function is   [Graphics:Images/FourierSeriesComplexMod_gr_6.gif].   

Its graph is obtained by repeating the portion of the graph in any interval of length  [Graphics:Images/FourierSeriesComplexMod_gr_7.gif],  as shown in Figure 12.1.

                    [Graphics:Images/FourierSeriesComplexMod_gr_8.gif]

                                   Figure 12.1.  A function  [Graphics:Images/FourierSeriesComplexMod_gr_9.gif]  with period  [Graphics:Images/FourierSeriesComplexMod_gr_10.gif].

 

    Familiar examples of real functions that have period  [Graphics:Images/FourierSeriesComplexMod_gr_11.gif],  are  [Graphics:Images/FourierSeriesComplexMod_gr_12.gif],  where  n  is an integer.  

These examples raise the question of whether any periodic function can be represented by a sum of terms involving  [Graphics:Images/FourierSeriesComplexMod_gr_13.gif],  

where  [Graphics:Images/FourierSeriesComplexMod_gr_14.gif]  are real constants.  As we soon demonstrate, the answer to this question is often yes.

 

Definition 12.1  (Piecewise Continuous).   The function  [Graphics:Images/FourierSeriesComplexMod_gr_15.gif]  is piecewise continuous on the closed interval  [Graphics:Images/FourierSeriesComplexMod_gr_16.gif],  if there exists values  [Graphics:Images/FourierSeriesComplexMod_gr_17.gif]  

with  [Graphics:Images/FourierSeriesComplexMod_gr_18.gif]  such that  [Graphics:Images/FourierSeriesComplexMod_gr_19.gif]  is continuous in each of the open intervals   [Graphics:Images/FourierSeriesComplexMod_gr_20.gif],   for   [Graphics:Images/FourierSeriesComplexMod_gr_21.gif]  

and has left-hand and right-hand limits at each of the values   [Graphics:Images/FourierSeriesComplexMod_gr_22.gif],   for   [Graphics:Images/FourierSeriesComplexMod_gr_23.gif].  

         We use the symbols  [Graphics:Images/FourierSeriesComplexMod_gr_24.gif]  and  [Graphics:Images/FourierSeriesComplexMod_gr_25.gif]  for the left-hand and right-hand limit, respectively, of a function  [Graphics:Images/FourierSeriesComplexMod_gr_26.gif]  as [Graphics:Images/FourierSeriesComplexMod_gr_27.gif] approaches the point [Graphics:Images/FourierSeriesComplexMod_gr_28.gif].  

The graph of a piecewise continuous function is illustrated in Figure 12.2 below, where the function  [Graphics:Images/FourierSeriesComplexMod_gr_29.gif]  is

                              [Graphics:Images/FourierSeriesComplexMod_gr_30.gif]

                    [Graphics:Images/FourierSeriesComplexMod_gr_31.gif]

                              Figure 12.2.  A piecewise continuous function  [Graphics:Images/FourierSeriesComplexMod_gr_32.gif]  over the interval  [Graphics:Images/FourierSeriesComplexMod_gr_33.gif].

The  left-hand and right-hand limits at [Graphics:Images/FourierSeriesComplexMod_gr_34.gif],  [Graphics:Images/FourierSeriesComplexMod_gr_35.gif],  and  [Graphics:Images/FourierSeriesComplexMod_gr_36.gif]  are easily determined:

            At  [Graphics:Images/FourierSeriesComplexMod_gr_37.gif],  the left-hand limit is   [Graphics:Images/FourierSeriesComplexMod_gr_38.gif],

                        and the right-hand limit is   [Graphics:Images/FourierSeriesComplexMod_gr_39.gif].

            At  [Graphics:Images/FourierSeriesComplexMod_gr_40.gif],  the left-hand limit is   [Graphics:Images/FourierSeriesComplexMod_gr_41.gif][Graphics:Images/FourierSeriesComplexMod_gr_42.gif],

                        and the right-hand limit is   [Graphics:Images/FourierSeriesComplexMod_gr_43.gif].

            At  [Graphics:Images/FourierSeriesComplexMod_gr_44.gif],  the left-hand limit is   [Graphics:Images/FourierSeriesComplexMod_gr_45.gif][Graphics:Images/FourierSeriesComplexMod_gr_46.gif],

                        and the right-hand limit is   [Graphics:Images/FourierSeriesComplexMod_gr_47.gif].

Exploration.

 

Definition 12.2  (Fourier Series).   If  [Graphics:Images/FourierSeriesComplexMod_gr_103.gif]  is periodic with period  [Graphics:Images/FourierSeriesComplexMod_gr_104.gif]  and is piecewise continuous on  [Graphics:Images/FourierSeriesComplexMod_gr_105.gif],  then the Fourier Series  [Graphics:Images/FourierSeriesComplexMod_gr_106.gif]  for  [Graphics:Images/FourierSeriesComplexMod_gr_107.gif]  is  

(12.1)        [Graphics:Images/FourierSeriesComplexMod_gr_108.gif],  

where the coefficients  [Graphics:Images/FourierSeriesComplexMod_gr_109.gif]  are given by the so-called Euler's formulae:  

(12.2)        [Graphics:Images/FourierSeriesComplexMod_gr_110.gif],  

        and  

(12.3)        [Graphics:Images/FourierSeriesComplexMod_gr_111.gif].  

      We introduced the factor [Graphics:Images/FourierSeriesComplexMod_gr_112.gif] in the constant term  [Graphics:Images/FourierSeriesComplexMod_gr_113.gif]  on the right side of Equation (12.1) for convenience,

so that we can obtain  [Graphics:Images/FourierSeriesComplexMod_gr_114.gif]  from the general formula in Equation (12.1) by setting  [Graphics:Images/FourierSeriesComplexMod_gr_115.gif].  

We explain the reasons for this strategy shortly.  Theorem 12.1 deals with convergence of the Fourier series.

 

Theorem 12.1 (Fourier Expansion).   Assume that  [Graphics:Images/FourierSeriesComplexMod_gr_116.gif]  is the Fourier Series for  [Graphics:Images/FourierSeriesComplexMod_gr_117.gif].  

If  [Graphics:Images/FourierSeriesComplexMod_gr_118.gif]  are piecewise continuous on  [Graphics:Images/FourierSeriesComplexMod_gr_119.gif],  then  [Graphics:Images/FourierSeriesComplexMod_gr_120.gif]  is convergent for all  [Graphics:Images/FourierSeriesComplexMod_gr_121.gif].  

The relation   [Graphics:Images/FourierSeriesComplexMod_gr_122.gif]   holds for all  [Graphics:Images/FourierSeriesComplexMod_gr_123.gif]  where  [Graphics:Images/FourierSeriesComplexMod_gr_124.gif]  is continuous.   

If  [Graphics:Images/FourierSeriesComplexMod_gr_125.gif]  is a point of discontinuity of  [Graphics:Images/FourierSeriesComplexMod_gr_126.gif],  then  

                        [Graphics:Images/FourierSeriesComplexMod_gr_127.gif],  

where [Graphics:Images/FourierSeriesComplexMod_gr_128.gif] denote the left-hand and right-hand limits, respectively.   With this understanding, we have the Fourier Series expansion:

                        [Graphics:Images/FourierSeriesComplexMod_gr_129.gif] .  

Proof.

 

Example 12.1.  The function   [Graphics:Images/FourierSeriesComplexMod_gr_130.gif],   extended periodically by the equation   [Graphics:Images/FourierSeriesComplexMod_gr_131.gif],   

has the Fourier series expansion  

                    [Graphics:Images/FourierSeriesComplexMod_gr_132.gif].  

Solution.

    Using Equation (12.2) and integrating by parts, we obtain  

                    [Graphics:Images/FourierSeriesComplexMod_gr_133.gif],    for    [Graphics:Images/FourierSeriesComplexMod_gr_134.gif].

The coefficient  [Graphics:Images/FourierSeriesComplexMod_gr_135.gif]  is obtained with the separate computation  

                    [Graphics:Images/FourierSeriesComplexMod_gr_136.gif].  

Then using Equation (12.3) we get  

                    [Graphics:Images/FourierSeriesComplexMod_gr_137.gif],    for    [Graphics:Images/FourierSeriesComplexMod_gr_138.gif].

Substituting the coefficients  [Graphics:Images/FourierSeriesComplexMod_gr_139.gif]  and  [Graphics:Images/FourierSeriesComplexMod_gr_140.gif]  into Equation (12.1) produces the required solution  

                    [Graphics:Images/FourierSeriesComplexMod_gr_141.gif].  

        The graphs of   [Graphics:Images/FourierSeriesComplexMod_gr_142.gif]   and the first three partial sums    [Graphics:Images/FourierSeriesComplexMod_gr_143.gif],    [Graphics:Images/FourierSeriesComplexMod_gr_144.gif],    

and    [Graphics:Images/FourierSeriesComplexMod_gr_145.gif]    are shown in Figure 12.3.

                    [Graphics:Images/FourierSeriesComplexMod_gr_146.gif]

               Figure 12.3.  The function  [Graphics:Images/FourierSeriesComplexMod_gr_147.gif],  and the approximations  [Graphics:Images/FourierSeriesComplexMod_gr_148.gif],  [Graphics:Images/FourierSeriesComplexMod_gr_149.gif],  and  [Graphics:Images/FourierSeriesComplexMod_gr_150.gif].  

Explore Solution 12.1.

Solution Details 12.1.

 

Theorem 12.2.   If  [Graphics:Images/FourierSeriesComplexMod_gr_318.gif]  have Fourier series representations, then their sum   [Graphics:Images/FourierSeriesComplexMod_gr_319.gif]   has a Fourier series representation,

and the Fourier coefficients of  [Graphics:Images/FourierSeriesComplexMod_gr_320.gif]  are obtained by adding the corresponding coefficients of  [Graphics:Images/FourierSeriesComplexMod_gr_321.gif].  

Proof.

 

Theorem 12.3 (Fourier Cosine Series).   Assume that  [Graphics:Images/FourierSeriesComplexMod_gr_322.gif]  is an even function and has period  [Graphics:Images/FourierSeriesComplexMod_gr_323.gif].  

Here the Fourier series for   [Graphics:Images/FourierSeriesComplexMod_gr_324.gif]  involves only the cosine terms,  [Graphics:Images/FourierSeriesComplexMod_gr_325.gif],  and we write  

                    [Graphics:Images/FourierSeriesComplexMod_gr_326.gif],    

where   

                    [Graphics:Images/FourierSeriesComplexMod_gr_327.gif].  

Proof.

 

Theorem 12.4 (Fourier Sine Series).   Assume that  [Graphics:Images/FourierSeriesComplexMod_gr_328.gif]  is an odd function and has period  [Graphics:Images/FourierSeriesComplexMod_gr_329.gif].  

Here the Fourier series for   [Graphics:Images/FourierSeriesComplexMod_gr_330.gif]  involves only the sine terms,  [Graphics:Images/FourierSeriesComplexMod_gr_331.gif],  and we write  

                    [Graphics:Images/FourierSeriesComplexMod_gr_332.gif],  

where   

                    [Graphics:Images/FourierSeriesComplexMod_gr_333.gif].  

Proof.

 

Theorem 12.5  (Termwise Integration).   Assume that  [Graphics:Images/FourierSeriesComplexMod_gr_334.gif]  has the Fourier series representation  

                        [Graphics:Images/FourierSeriesComplexMod_gr_335.gif].  

Then the integral  of  [Graphics:Images/FourierSeriesComplexMod_gr_336.gif]  has a Fourier series representation which can be obtained by termwise integration of the Fourier series of  [Graphics:Images/FourierSeriesComplexMod_gr_337.gif],  that is  

                        [Graphics:Images/FourierSeriesComplexMod_gr_338.gif],   

where we have used the expansion    [Graphics:Images/FourierSeriesComplexMod_gr_339.gif].   

Proof.

 

Theorem 12.6  (Termwise Differentiation).   Assume that both  [Graphics:Images/FourierSeriesComplexMod_gr_340.gif]  have Fourier series representation and that  

                    [Graphics:Images/FourierSeriesComplexMod_gr_341.gif].  

Then  [Graphics:Images/FourierSeriesComplexMod_gr_342.gif]  can be obtained by termwise differentiation of  [Graphics:Images/FourierSeriesComplexMod_gr_343.gif],  that is  

                    [Graphics:Images/FourierSeriesComplexMod_gr_344.gif].  

Proof.

 

Example 12.2.  The function   [Graphics:Images/FourierSeriesComplexMod_gr_345.gif],   extended periodically by the equation   [Graphics:Images/FourierSeriesComplexMod_gr_346.gif],   

has the Fourier series expansion  

                    [Graphics:Images/FourierSeriesComplexMod_gr_347.gif],  

which can be written in the alternative form  

                    [Graphics:Images/FourierSeriesComplexMod_gr_348.gif].  

Solution.

    The function  [Graphics:Images/FourierSeriesComplexMod_gr_349.gif]  is an even function;  hence we can use Theorem 11.3 to conclude that  [Graphics:Images/FourierSeriesComplexMod_gr_350.gif]  for all  [Graphics:Images/FourierSeriesComplexMod_gr_351.gif]  and that  

                    [Graphics:Images/FourierSeriesComplexMod_gr_352.gif],    for    [Graphics:Images/FourierSeriesComplexMod_gr_353.gif].  
    
The coefficient  [Graphics:Images/FourierSeriesComplexMod_gr_354.gif]  is obtained with the separate computation  

                    [Graphics:Images/FourierSeriesComplexMod_gr_355.gif].

Using the  [Graphics:Images/FourierSeriesComplexMod_gr_356.gif]  and Theorem 12.3 produces the required solution.

Therefore, we have the found the Fourier series expansion  

                    [Graphics:Images/FourierSeriesComplexMod_gr_357.gif].  

It is easy to see that  [Graphics:Images/FourierSeriesComplexMod_gr_358.gif]  for all  [Graphics:Images/FourierSeriesComplexMod_gr_359.gif],  and we can express  [Graphics:Images/FourierSeriesComplexMod_gr_360.gif]  in the form   

                    [Graphics:Images/FourierSeriesComplexMod_gr_361.gif].  

Therefore,  

                    [Graphics:Images/FourierSeriesComplexMod_gr_362.gif].  

The graphs of   [Graphics:Images/FourierSeriesComplexMod_gr_363.gif]   and the first two partial sums   [Graphics:Images/FourierSeriesComplexMod_gr_364.gif],   and   [Graphics:Images/FourierSeriesComplexMod_gr_365.gif]   are shown below.

                         [Graphics:Images/FourierSeriesComplexMod_gr_366.gif]

                    Figure 12.2.a.  The function  [Graphics:Images/FourierSeriesComplexMod_gr_367.gif],  and the approximations  [Graphics:Images/FourierSeriesComplexMod_gr_368.gif],  and  [Graphics:Images/FourierSeriesComplexMod_gr_369.gif].

Explore Solution 12.2.

Solution Details 12.2.

 

Extra Example 1.   Given   [Graphics:Images/FourierSeriesComplexMod_gr_562.gif]  extended periodically by the equation   [Graphics:Images/FourierSeriesComplexMod_gr_563.gif],  

find the Fourier series expansion.     

                              [Graphics:Images/FourierSeriesComplexMod_gr_564.gif]

Extra Solution 1.

 

Extra Example 2.   Given  [Graphics:Images/FourierSeriesComplexMod_gr_703.gif],   extended periodically by the equation   [Graphics:Images/FourierSeriesComplexMod_gr_704.gif],  

find the Fourier series expansion.     

                              [Graphics:Images/FourierSeriesComplexMod_gr_705.gif]

Extra Solution 2.

 

Exercises for Section 12.1.  Fourier Series Representation

 

Library Research Experience for Undergraduates

Fourier Series

Fourier Series and Transform

Dirichlet Problem

Laplace Transform

 

 

 

 

The Next Module is

Dirichlet Problem for the Disk

 

 

 Return to the Complex Analysis Modules

 

 

Return to the Complex Analysis Project

 

 

 

 

  

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

This material is coordinated with our book Complex Analysis for Mathematics and Engineering.

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

(c) 2012 John H. Mathews, Russell W. Howell