One-Pole
Fig.B.3 gives the signal flow graph for the general one-pole filter. The road to the frequency response goes as follows:
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The one-pole filter has a transfer function (hence frequency response) which is the reciprocal of that of a one-zero. The analysis is thus quite analogous. The frequency response in polar form is given by
![\begin{eqnarray*}
G(\omega) &=& \frac{\vert b_0\vert}{\sqrt{[1 + a_1 \cos(\omega...
... + a_1 \cos(\omega T)}\right], & b_0<0 \\
\end{array} \right..
\end{eqnarray*}](http://www.dsprelated.com/josimages_new/filters/img1351.png)
A plot of the frequency response in polar form for and
various values of
is given in Fig.B.4.
The filter has a pole at , in the
plane (and a zero at
= 0). Notice that the one-pole exhibits
either a lowpass or a highpass frequency response, like the
one-zero. The lowpass character occurs when the pole is near the point
(dc), which happens when
approaches
. Conversely,
the highpass nature occurs when
is positive.
The one-pole filter section can achieve much more drastic differences
between the gain at high frequencies and the gain at low frequencies
than can the one-zero filter. This difference is achieved in the
one-pole by gain boost in the passband rather than
attenuation in the stopband; thus it is usually desirable when
using a one-pole filter to set to a small value, such as
, so that the peak gain is 1 or so. When the peak gain is 1,
the filter is unlikely to overflow.B.1
Finally, note that the one-pole filter is stable if and only if
.
Next Section:
Two-Pole
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One-Zero