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442 CHAPTER 13 Fourier Series
for n = 0,1,2,···. Notice that we can compute a n strictly in terms of f on [0, L]. The construc-
tion of g showed us how to obtain this cosine series for f , but we do not need g to compute the
coefficients of this series.
Based on these ideas, define the Fourier cosine coefficients of f on [0, L] to be the numbers
2 L
a n = f (x)cos(nπx/L)dx (13.10)
L 0
for n = 0,1,2,···.The Fourier cosine series for f on [0, L] is the series
∞
1
a 0 + a n cos(nπx/L) (13.11)
2
n=1
in which the a s are the Fourier cosine coefficients of f on [0, L].
n
By applying Theorem 13.1 to g, we obtain the following convergence theorem for cosine
series on [0, L].
THEOREM 13.2 Convergence of Fourier Cosine Series
Let f be piecewise smooth on [0, L]. Then
1. If 0 < x < L, the Fourier cosine series for f on [0, L] converges to
1
( f (x+) + f (x−)).
2
2. At 0 this cosine series converges to f (0+).
3. At L this cosine series converges to f (L−).
EXAMPLE 13.9
2x
Let f (x) = e for 0 ≤ x ≤ 1. We will write the cosine expansion of f on [0,1]. The coefficients
are
1
2
2x
a 0 = 2 e dx = e − 1
0
and for n = 1,2,···,
1
2x
a n = 2 e cos(nπx)dx
0
1
4e cos(nπx) + 2nπe sin(nπx)
2x 2x
=
4 + n π 2
2
0
n
2
e (−1) − 1
= 4 .
2
4 + n π 2
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October 14, 2010 14:57 THM/NEIL Page-442 27410_13_ch13_p425-464