Tuesday 3 November 2015

discrete signals - Zero Padding of FFT


There are many question related to the zero padding a time domain signal to get more frequency bins after performing Fourier transform. As I understand this process is equivalent to trigonometric interpolation in the frequency domain. However, I am not certain of this fact. Can anyone verify this correct or incorrect mathematically?



Answer




It's true that zero-padding in the time domain corresponds to interpolation in the frequency domain. If you have a length $N$ signal $x[n]$, its discrete Fourier transform (DFT) is given by


$$X[k]=\sum_{n=0}^{N-1}x[n]e^{-j2\pi nk/N}\tag{1}$$


The signal $x[n]$ can be expressed in terms of its DFT coefficients $X[k]$ by the inverse DFT


$$x[n]=\frac{1}{N}\sum_{k=0}^{N-1}X[k]e^{j2\pi nk/N}\tag{2}$$


Since the coefficients $X[k]$ contain the same information as the signal $x[n]$, anything that can be computed from $x[n]$ can also be computed from $X[k]$.


Let $\tilde{X}(\omega)$ denote the discrete-time Fourier transform (DTFT) of $x[n]$:


$$\tilde{X}(\omega)=\sum_{n=0}^{N-1}x[n]e^{-jn\omega}\tag{3}$$


Note that $\omega$ is a continuous variable. Comparing (1) and (3) shows that the DFT is simply a sampled version of the DTFT:


$$X[k]=\tilde{X}(2\pi k/N),\quad k=0,\ldots,N-1\tag{4}$$


Furthermore, a length $L$ DFT ($L>N$) of $x[n]$ simply corresponds to a more densely sampled version of $\tilde{X}(\omega)$:



$$X_L[l]=\sum_{n=0}^{N-1}x[n]e^{-j2\pi nl/L}=\tilde{X}(2\pi l/L),\quad l=0,\ldots,L-1\tag{5}$$


Now let's express $\tilde{X}(\omega)$ in terms of the length $N$ DFT of $x[n]$. Rewriting (3) using (2) gives


$$\begin{align}\tilde{X}(\omega)&=\sum_{n=0}^{N-1}\frac{1}{N}\sum_{k=0}^{N-1}X[k]e^{j2\pi nk/N}e^{-jn\omega}\\ &=\sum_{k=0}^{N-1}X[k]\underbrace{\frac{1}{N}\sum_{n=0}^{N-1}e^{-jn(\omega-2\pi k/N)}}_{G(\omega-2\pi k/N)} \end{align}\tag{6}$$


where $G(\omega)$ is an interpolation function which can be expressed by


$$G(\omega)=\frac{1}{N}\sum_{n=0}^{N-1}e^{-jn\omega}=\frac{e^{-j\omega(N-1)/2}}{N}\frac{\sin(N\omega/2)}{\sin(\omega/2)}\tag{7}$$


By setting $\omega=2\pi l/L$ in (6) and using (5) you can see that the length $L$ zero-padded DFT of $x[n]$ can be computed from the length $N$ DFT using the interpolation function given by (7):


$$X_L(l)=\tilde{X}(2\pi l/L)=\sum_{k=0}^{N-1}X[k]G(2\pi l/L-2\pi k/N)\tag{8}$$


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