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Fourier transform of a sinusoid

We can use the phase shift formula above to find the Fourier transform of any complex sinusoid ${Z^n}$ with frequency $\alpha $, simply by setting $X[n]=1$ in the formula and using the Fourier transform for DC:

\begin{displaymath}
{\cal FT} \left \{ {Z^n} \right \} (k) =
{\cal FT} \left \{ 1 \right \}(k - {{\alpha } \over {\omega}})
\end{displaymath}


\begin{displaymath}
= \left [ \cos(\Phi(k) + i \sin(\Phi(k))\right ]
{D_N}(k - {{\alpha } \over {\omega}})
\end{displaymath}

where ${D_N}$ is the Dirichlet kernel and $\Phi$ is an ugly phase term:

\begin{displaymath}
\Phi(k) = \pi \cdot (k - {{\alpha } \over {\omega}}) \cdot (N-1)/N)
\end{displaymath}

Figure 9.3: Fourier transforms of complex sinusoids, with $N$ = 100: (a) with frequency $2\omega $ ; (b) with frequency $1.5\omega $. (The effect of the phase winding term is not shown.)
\begin{figure}\psfig{file=figs/fig09.03.ps}\end{figure}

If the sinusoid's frequency $\alpha $ is an integer multiple of the fundamental frequency $\omega $, the Dirichlet kernel is shifted to the left or right by an integer. In this case the zero crossings of the Dirichlet kernel line up with integer values of $k$, so that only one partial is nonzero. This is pictured in Figure 9.3 (part a).

Figure 9.4: A complex sinusoid with frequency $\alpha =1.5\omega =3\pi /N$, forced to repeat every $N$ samples. ($N$ was arbitrarily set to 100; only the real part is shown.)
\begin{figure}\psfig{file=figs/fig09.04.ps}\end{figure}

Part (b) shows the result when the frequency $\alpha $ falls halfway between two integers. The partials have amplitudes falling off roughly as $1/k$ in both directions, measured from the actual frequency $\alpha $. That the energy should be spread over many partials, when after all we started with a single sinusoid, might seem surprising at first. However, as shown in Figure 9.4, the signal repeats at a period $N$ which disagrees with the frequency of the sinusoid. As a result there is a discontinuity at the beginning of each period, and energy is flung over a wide range of frequencies.


next up previous contents index
Next: Fourier analysis of non-periodic Up: Properties of Fourier transforms Previous: Shifts and phase changes   Contents   Index
Miller Puckette 2006-09-24