78 OPERATIONAL AMPLIFIER CIRCUITS: ANALYSIS AND DESIGN
where
and
This unwieldy equation can be simplified by letting R
l
=R
2
= R and C
x
= C
2
= C;
hence,
This is of the general form
which is the response of a second-order band pass filter. Notice that A!# which
is the gain at the center frequency, is not equal to as was the case for the
low- and high-frequency gains of the low and high pass filters, respectively.
The damping coefficient a can be shown to be the reciprocal of the Q of
the filter. Therefore, from Equations (5.56) and (5.57) we have
(5.58)
(5.59)
Also,
(5.60)
(5.54)
(5.55)
(5.56)
(5.57)
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