Active filters are frequency-selective circuits that incorporate RC networks and amplii ers
with feedback to produce low-pass, high-pass, bandpass, and bandstop performance.
These i lters can replace standard passive LC i lters in many applications. They offer the
following advantages over standard passive LC filters.
Figure-1.1 Block diagram or schematic symbols for filters.
- Gain. Because active filters use amplifiers, they can be designed to amplify as well as filter, thus offsetting any insertion loss.
- No inductors. Inductors are usually larger, heavier, and more expensive than capacitors and have greater losses. Active filters use only resistors and capacitors.
- Easy to tune. Because selected resistors can be made variable, the filter cutoff frequency, center frequency, gain, Q, and bandwidth are adjustable
- Isolation. The amplifiers provide very high isolation between cascaded circuits because of the amplifier circuitry, thereby decreasing interaction between filter sections.
- Easier impedance matching. Impedance matching is not as critical as with LC filters.
Figure 1.2 Types of active filters. (a) Low-pass. (b) Low-pass. (c) High-pass. (d ) High-pass.
Figure 1.3 Active bandpass and notch filters. (a) Bandpass. (b) Bandpass. (c) High-Q notch.
Two active bandpass filters and a notch filter are shown in Fig.1.3. In Fig.1.3(a),
both RC low-pass and high-pass sections are combined with feedback to give a bandpass result. In Fig.1.3(b), a twin-T RC notch i lter is used with negative feedback
to provide a bandpass result. A notch i lter using a twin-T is illustrated in
Fig. 1.3(c). The feedback makes the response sharper than that with a standard passive twin-T.
Active filters are made with integrated-circuit (IC) op amps and discrete RC networks. They can be designed to have any of the responses discussed earlier, such as
Butterworth and Chebyshev, and they are easily cascaded to provide even greater selectivity. Active filters are also available as complete packaged components. The primary
disadvantage of active i lters is that their upper frequency of operation is limited by the
frequency response of the op amps and the practical sizes of resistors and capacitors.
Most active filters are used at frequencies below 1 MHz, and most active circuits operate
in the audio range and slightly above. However, today op amps with frequency ranges
up to one microwave (.1 GHz) mated with chip resistors and capacitors have made RC
active i lters practical for applications up to the RF range.
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