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Fourier Series and Partial Differential Equations Lecture Notes

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Chapter 2. <strong>Fourier</strong> series 12<br />

<strong>Notes</strong>. If f, f1 are odd functions <strong>and</strong> g, g1 are even functions then:<br />

1. f(0) = 0 because f(0) = −f(−0) = −f(0);<br />

y<br />

2. for any α ∈ R, α<br />

f(x)dx = 0; (2.17)<br />

−α<br />

3. for any α ∈ R, α α<br />

g(x)dx = 2 g(x)dx; (2.18)<br />

−α 0<br />

4. the functions h(x) = f(x)g(x), h1(x) = f(x)f1(x) <strong>and</strong> h2(x) = g(x)g1(x) are odd,<br />

even <strong>and</strong> even, respectively.<br />

2.2 <strong>Fourier</strong> series for functions of period 2π<br />

Let f be a function of period 2π. We would like to get an expansion for f of the form<br />

f(x) = 1<br />

2 a0 +<br />

∞<br />

[ancos(nx)+bnsin(nx)], (2.19)<br />

n=1<br />

where the an <strong>and</strong> bn are constants. Remember that sin(nx) <strong>and</strong> cos(nx) are periodic with<br />

period 2π. We have two questions to answer.<br />

Question 1: if equation (2.19) is true, can we find the an <strong>and</strong> bn in terms of f?<br />

Question 2: with these an, bn, when, if ever, is equation (2.19) true?<br />

2.2.1 Question 1<br />

Suppose equation (2.19) is true <strong>and</strong> that we can integrate it term by term, i.e.<br />

π<br />

−π<br />

f(x)dx = 1<br />

2 a0<br />

π<br />

−π<br />

Since π<br />

−π<br />

dx = 2π,<br />

dx+<br />

∞<br />

<br />

n=1<br />

an<br />

π π<br />

cos(nx)dx+bn<br />

−π<br />

π<br />

cos(nx)dx = 0,<br />

−π<br />

−π<br />

x<br />

<br />

sin(nx)dx . (2.20)<br />

π<br />

sin(nx)dx = 0, (2.21)<br />

−π

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