Find the complex Fourier series of the sawtooth wave in Fig. 17.9. Plot the amplitude and the phase spectra.
From Fig. 17.9,f(t) = t, 0 < t < 1 , T = 1 so that ω_{0} = 2π/T = 2 π . Hence,
c_{n} = \frac{1}{T} \int^{T}_{0}{f(t) e^{-jnω_{0}t} dt } = \frac{1}{1} \int^{1}_{0}{te^{-j2nπt} dt} (17.11.1)
But
\int{te^{at} dt} = \frac{e^{at}}{a^{2}} (ax – 1) + C
Applying this to Eq. (17.11.1) gives
\begin{matrix} c_{n} = \frac{e^{-j2nπt}}{(-j2nπ)^{2}}(-j2nπt – 1) \mid^{1}_{0} \\ = \frac{e^{-j2nπ}(-j2nπ – 1) + 1}{-4n^{2}π^{2}}\end{matrix}\quad \quad (17.11.2)
Again,
e^{-j2πn} = \cos 2πn – j \sin 2πn = 1 – j 0 = 1
so that Eq. (17.11.2) becomes
c_{n} = \frac{-j2nπ}{-4n^{2}π^{2}} = \frac{j}{2nπ} (17.11.3)
This does not include the case when n = 0 . When n = 0 ,
c_{0} = \frac{1}{T} \int^{T}_{0}{f(t) dt} = \frac{1}{1} \int^{1}_{0}{t dt } = \frac{t^{2}}{2} \mid^{0}_{1} = 0.5 (17.11.4)
Hence,
f(t) = 0.5 + \sum\limits^{∞}_{\begin{matrix}n = – ∞\\ n≠0\end{matrix}}{\frac{j}{2nπ} e^{j2nπt}} (17.11.5)
and
\left|c_{n}\right| = \begin{cases} \frac{1}{2nπ} , & n ≠ 0 \\ 0.5 , & n = 0 \end{cases} , θ_{n} = 90° , n ≠ 0 (17.11.6)
By plotting \left|c_{n}\right| and θ_{n} for different n, we obtain the amplitude spectrum and the phase spectrum shown in Fig. 17.31.