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Fourier Series and Partial Differential Equations Lecture Notes

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Chapter 2. <strong>Fourier</strong> series 17<br />

(a) s0 (b) s1 (c) s2<br />

(d) s5 (e) s10 (f) s50<br />

Figure 2.1: Convergence of the <strong>Fourier</strong> series for the function of Section 2.2.3.<br />

2.3 Convergence of <strong>Fourier</strong> series<br />

For the previous example it does appear that except at points of discontinuity the partial<br />

sums do converge to f(x). At points of discontinuity they converge to zero. A similar<br />

result is true also for most functions which appear in applications. To present this result<br />

we first need to discuss one-sided limits.<br />

Definition We say that the right-h<strong>and</strong> limit of f at c is<br />

f(c+) = lim f(c+h), (2.51)<br />

h→0<br />

h>0<br />

if this exists. Similarly, the left-h<strong>and</strong> limit of f at c is<br />

if this exists.<br />

f(c−) = lim f(c−h), (2.52)<br />

h→0<br />

h>0<br />

The existence part is important since, for example, f(x) = sin(1/x) does not have these<br />

limits at zero.<br />

Definition The function f is piecewise continuous on an interval (a,b) if we can divide<br />

(a,b) into a finite number of sub-intervals, on each of which f is defined <strong>and</strong> continuous,<br />

<strong>and</strong> the left- <strong>and</strong> right-h<strong>and</strong> limits at the endpoints of each sub-interval exist.

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