Sign in

username:

password:



Not a member?

Search Online Books



Search tips

Free Online Books

Ads

Chapters

Chapter Contents:

Search Mathematics of the DFT

  

Book Index | Global Index


Would you like to be notified by email when Julius Orion Smith III publishes a new entry into his blog?

  

Filters and Convolution

A reason for the importance of convolution (defined in §7.2.4) is that every linear time-invariant system8.4can be represented by a convolution. Thus, in the convolution equation

$\displaystyle y = h\ast x \protect$ (8.1)

we may interpret $ x$ as the input signal to a filter, $ y$ as the output signal, and $ h$ as the digital filter, as shown in Fig.8.12.

Figure 8.12: The filter interpretation of convolution.
\includegraphics[scale=0.8]{eps/filterbox}

The impulse or ``unit pulse'' signal is defined by

$\displaystyle \delta(n) \isdef \left\{\begin{array}{ll}
1, & n=0 \\ [5pt]
0, & n\neq 0. \\
\end{array}\right.
$

For example, for sequences of length $ N=4$, $ \delta = [1,0,0,0]$.

The impulse signal is the identity element under convolution, since

$\displaystyle (x\ast \delta)_n \isdef \sum_{m=0}^{N-1}x(m) \delta(n-m) = x(n).
$

If we set $ x=\delta$ in Eq.$ \,$(8.1) above, we get

$\displaystyle y = h\ast \delta = h.
$

Thus, $ h$, which we introduced as the convolution representation of a filter, has been shown to be more specifically the impulse response of the filter.

It turns out in general that every linear time-invariant (LTI) system (filter) is completely described by its impulse response [65]. No matter what the LTI system is, we can feed it an impulse, record what comes out, call it $ h(n)$, and implement the system by convolving the input signal $ x$ with the impulse response $ h$. In other words, every LTI system has a convolution representation in terms of its impulse response.



Subsections

Order a Hardcopy of Mathematics of the DFT

Previous: Spectrogram of Speech
Next: Frequency Response

written by Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See http://ccrma.stanford.edu/~jos/ for details.


Comments


No comments yet for this page


Add a Comment
You need to login before you can post a comment (best way to prevent spam). ( Not a member? )