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13.3 Sine and Cosine Series 441
⎧
⎧
⎨ cos(x) for −2 ≤ x < 0 ⎪−2 for −4 ≤ x ≤−2
⎨
16. f (x) = 19. f (x) = 1 + x 2
⎩sin(x) for 0 ≤ x ≤ 2 for −2 < x ≤ 2
⎪
0 for 2 < x ≤ 4
⎩
−1 for −4 ≤ x < 0
17. f (x) = 20. Using Problem 14, write the Fourier series of the
1 for 0 ≤ x ≤ 4 function and plot some partial sums, pointing out the
occurrence of the Gibbs phenomenon at the points of
⎧
⎪0for −1 ≤ x < 1/2 discontinuity of the function.
⎨
18. f (x) = 1for 1/2 ≤ x ≤ 3/4
21. Carry out the program of Problem 20 for the function
⎪
2for 3/4 < x ≤ 1 of Problem 16.
⎩
13.3 Sine and Cosine Series
If f is piecewise continuous on [−L, L], we can represent f (x) at all but possibly finitely many
points of [−L, L] by its Fourier series. This series may contain just sine terms, just cosine terms,
or both sine and cosine terms. We have no control over this.
If f is defined on the half interval [0, L], we can write a Fourier cosine series (containing
just cosine terms) and a Fourier sine series (containing just sine terms) for f on [0, L].
13.3.1 Cosine Series
Suppose f (x) is defined for 0 ≤ x ≤ L. To get a pure cosine series on this interval, imagine
reflecting the graph of f across the vertical axis to obtain an even function g defined on [−L, L]
(see Figure 13.13).
Because g is even, its Fourier series on [−L, L] has only cosine terms and perhaps the
constant term. But g(x) = f (x) for 0 ≤ x ≤ L, so this gives a cosine series for f on [0, L].
Furthermore, because g is even, the coefficients in the Fourier series of g on [−L, L] are
1 L
a n = g(x)cos(nπx/L)dx
L −L
2 L
= g(x)cos(nπx/L)dx
L 0
2 L
= f (x)cos(nπx/L)dx.
L 0
y
x
FIGURE 13.13 Even extension of a
function defined on [0, L].
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October 14, 2010 14:57 THM/NEIL Page-441 27410_13_ch13_p425-464