Calculate the Fourier series for the function in Fig. 17.17 .
The function in Fig. 17.17 is half-wave odd symmetric, so that a_{0} = 0 = a_{n} . It is described over half the period as
f(t) = t, -1 < t < 1
T = 4, ω_{0} = 2π/T = π/2. Hence,
b_{n} = \frac{4}{T} \int^{T/2}_{0}{f(t) \sin n ω_{0} t dt}
Instead of integrating f(t) from 0 to 2, it is more convenient to integrate from -1 to 1. Applying Eq. (17.15d),
\int{ t \sin at dt} = \frac{1}{a^{2}} \sin at – \frac{1}{a} t \cos at (17.15d)
b_{n} = \frac{4}{4} \int^{1}_{-1}{t \sin \frac{nπ t}{2} dt} = [ \frac{\sin nπt/2}{n^{2} π^{2}/4} – \frac{t \cos n π t /2}{n π /2}] \mid^{1}_{-1}
= \frac{4}{n^{2} π^{2}} [ \sin \frac{nπ}{2} – \sin(- \frac{nπ}{2})] – \frac{2}{nπ} [ \cos \frac{nπ}{2} – \cos (-\frac{nπ}{2}) ]
= \frac{8}{n^{2}π^{2}} \sin \frac{nπ}{2}
since \sin (-x) = – \sin x is an odd function, while \cos(-x) = \cos x is an even function. Using the identities for \sin nπ /2 in Table 17.1,
b_{n} = \frac{8}{n^{2}π^{2}} (-1)^{(n – 1)/2} , n = odd = 1 , 3 , 5 , . . .
Thus,
f(t) = \sum \limits_{n = 1, 3 , 5}^{∞}{b_{n} \sin \frac{nπ}{2} t }
where b_{n} is given above.
TABLE 17.1 | |
Values of cosine, sine, and exponential functions for integral multiples of π. | |
\cos 2n π | 1 |
\sin 2nπ | 0 |
\cos n π | (-1)^{n} |
\sin nπ | 0 |
\cos \frac{nπ }{2} | \begin{cases}(-1)^{n/2} ,& n = even \\ 0 , & n = odd \end{cases} |
\sin \frac{nπ }{2} | \begin{cases}(-1)^{(n-1)/2} ,& n = odd \\ 0 , & n = even \end{cases} |
e^{j2nπ} | 1 |
e^{jnπ} | (-1)^{n} |
e^{jnπ/2} | \begin{cases}(-1)^{n/2} ,& n = even \\ j(-1)^{(n -1)/2} , & n = odd \end{cases} |