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Appendix C C-55<br />
PROJECT<br />
Fourier Series<br />
In the project at the end of Section 8.2,* we discussed square waves, sawtooth<br />
waves, and triangular waves. In this project we use the idea of superposition of<br />
waves to find a “trigonometric” way to describe a square wave.<br />
We start with the square wave given by y f(x) where<br />
f(x) b 1, 0 x 1<br />
1, 1 x 0<br />
f(x) 0 for all integers x and f(x 2) f(x)<br />
This square wave is shown in Figure A.<br />
y<br />
1<br />
-4<br />
-3<br />
-2<br />
-1<br />
1 2 3 4<br />
x<br />
-1<br />
Figure A<br />
A graph of f(x) b 1, 0 x 1 ,<br />
1, 1 x 0<br />
f(x) 0 for integer x, and f(x 2) f(x).<br />
Now, f is an odd function, periodic with period 2, and has domain all real<br />
numbers. That f is periodic suggests it might be related to more familiar periodic<br />
waves, for example, sine waves and cosine waves. Since f is an odd function<br />
we might be able to describe f by using only sine waves. And since the<br />
domain of f is all real numbers, our description of f using sine waves should<br />
coincide with f for most, if not all, real numbers.<br />
It turns out that f can be expressed by adding together infinitely many sine<br />
waves. In fact, using methods from calculus, it can be shown that<br />
f(x) 4 4<br />
4<br />
4<br />
sin px sin 3px sin 5px sin 7px p (1)<br />
p 3p 5p 7p<br />
for all real numbers x. The symbol “ p ” means there are infinitely many more<br />
terms that in this case follow the given pattern. So we are expressing f(x) as an<br />
infinite series, a sum of infinitely many terms. (While we will study some<br />
infinite series of numbers in Chapter 14,* it should be noted that the right-hand<br />
side of equation (1) is an infinite series of functions.) The particular infinite<br />
series on the right-hand side of equation (1) is called the Fourier series for the<br />
function f. Notice that the Fourier series for f consists of sine waves of different<br />
periods, but that 2, the period of the given square wave, is an integer multiple<br />
of each period. When we superimpose or add up the waves, we obtain the<br />
function f of period 2.<br />
Figure B shows the graphs of the first three partial sums of the Fourier series<br />
for f on the closed interval [3, 3] along with the graph of the square wave.<br />
*Precalculus: A Problems-Oriented Approach, 7th edition