Fourier transform of a triangular pulse

Solution 1:

Sinc function is tricky, because there are two of them. It seems your book uses the convention $$\operatorname{sinc} x = \frac{\sin (\pi x)}{\pi x}$$ The desired answer is $$X(\tau) = \tau\frac{\sin^2 (\omega \tau/2)}{(\omega \tau/2)^2} = \frac{4}{\omega^2 \tau }\sin^2 (\omega \tau/2) =\frac{2}{\omega^2 \tau }(1-\cos \omega \tau) $$ Which is what you have, since $e^{j\omega\tau}+e^{-j\omega\tau}=2\cos \omega\tau$.

Solution 2:

Continue from what you have got: $$\frac{2-(e^{j\omega \tau} + e^{-j\omega \tau)}}{\omega^2 \tau} = \frac{2-2\cos(\omega \tau)}{\omega^2 \tau} = \frac{2(1-\cos(\omega \tau))}{\omega^2 \tau} $$ Recall that $$1-\cos(\omega \tau) = 2 \sin^2 (\frac{\omega \tau}{2})$$ Thus $$\frac{2(1-\cos(\omega \tau))}{\omega^2 \tau} = \frac{4\sin^2 (\frac{\omega \tau}{2})}{\omega^2 \tau}$$ Rearrange by multiplying the numerator and the denominator by $\frac{\tau}{4}$

$$\frac{4\sin^2 (\frac{\omega \tau}{2})}{\omega^2 \tau} \cdot \frac{\frac{\tau}{4}}{\frac{\tau}{4}} = \tau \left[\frac{\sin (\frac{\omega \tau}{2})}{\frac{\omega \tau}{2}}\right]^2$$

And recall that $$\mathrm{sinc}(\frac{\omega \tau}{2}) = \frac{\sin (\frac{\omega \tau}{2})}{\frac{\omega \tau}{2}}$$

Therefore, $$\mathfrak{F}[\mathrm{tri}(\frac{t}{\tau}] = \tau \mathrm{sinc}^2(\frac{\omega \tau}{2})$$

Solution 3:

A simpler way to arrive at the expression involving the cosine term is to consider the symmetry of the triangular pulse. Since it is an even function, multiplication by exp(-jwt) is equivalent to multiplying by coswt, since the sine term will go to zero. Then we get lesser number of integrals to evaluate and the same expression involving [1-cos(omega.tau)]can be obtained much more easily.

Hope this helps.