5.4.2 Active analogue filters
In the foregoing discussion on
passive filters, the two main difficulties noted were those of obtaining
resistance-less inductors and achieving proper matching between signal source
and load through the filter sections. A further problem is that the inductors
required by passive filters are bulky and relatively expensive. Active filters
overcome all of these problems and so they are now used more commonly than
passive filters.
The major component in an active
filter is an electronic amplifier. The filter char[1]acteristics
are defined by amplifier input and feedback components that consist of
resistors and capacitors but not inductors. The fact that the necessary
characteristics can be obtained using only resistors and capacitors, without
requiring inductors, is a particular advantage of this class of filters. The
circuits shown in Figure 5.8 produce the four types of filter characteristics
discussed earlier. These are all known as second order filters, because the
input–output relationship across each filter is described by a second order
differential equation.
The characteristics of each filter in
terms of attenuation behaviour in the pass- and stop-bands is determined by the
choice of circuit components in Figure 5.8. A common set of design formulae is
given below, although detailed derivation is not given. Further information on
the derivation of these formulae can be found in specialist texts (e.g.
Stephenson, 1985):
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