5.5.6 Signal integration
Connected in the configuration shown in Figure 5.15, an
operational amplifier is able to integrate the input signal Vi such
that the output signal V0 is given by:
V0 = -
1/RC
This circuit is used whenever there is a requirement to integrate the output
signal from a transducer.
5.5.7 Voltage follower (pre-amplifier)
The voltage follower, also known as a
pre-amplifier, is a unity gain amplifier circuit with a short circuit in the
feedback path, as shown in Figure 5.16, such that:
V0 = Vi
It has a very high input impedance
and its main application is to reduce the load on the measured system. It also
has a very low output impedance that is very useful in some impedance-matching
applications.
5.5.8 Voltage comparator
The output of a voltage comparator
switches between positive and negative values according to whether the
difference between the two input signals to it is positive or negative. An
operational amplifier connected as shown in Figure 5.17 gives an output that
switches between positive and negative saturation levels according to whether
V1 V2 is greater than or less than zero.
Alternatively, the voltage of a single input
signal can be compared against
positive and negative reference levels with the circuit shown in Figure 5.18.
In practice, operational amplifiers
have drawbacks as voltage comparators for several reasons. These include
non-compatibility between output voltage levels and industry[1]standard logic
circuits, propagation delays and slow recovery. In consequence, various other
special-purpose integrated circuits have been developed for voltage comparison.
In practice, operational amplifiers
have drawbacks as voltage comparators for several reasons. These include
non-compatibility between output voltage levels and industry[1]standard logic
circuits, propagation delays and slow recovery. In consequence, various other
special-purpose integrated circuits have been developed for voltage comparison.
5.5.9 Phase-sensitive detector
One function of a phase-sensitive
detector is to measure the phase difference between two signals that have the
same frequency. For two input signals of amplitude V1 and V2
and frequency f, the output is given by V1V2 cos 0, where 0 is the phase difference between the
signals. In many cases, the phase difference is adjusted to zero (cos 0 = 1) so that the output is a maximum.
A phase-sensitive detector can also be used as
a cross-correlator to enhance the quality of measurement signals that have a
poor signal-to-noise ratio. This ability is also exploited in the use of
phase-sensitive detectors to demodulate amplitude-modulated (AM) signals. For
these roles, the detector requires firstly a clean reference voltage at the
same frequency as the measurement signal and secondly, phase-control circuits
to make the phases of the reference and measurement signals coincide.
Commercial instruments known as lock-in amplifiers (see next section) are
available that combine a phase-sensitive detector with the other components
required to provide the demodu[1]lation function.
Phase-sensitive detectors are known
by several alternative names, two examples of which are synchronous demodulator
and synchronous detector. They can also exist physically in a number of
alternative forms that include both transformer-based and fully electronic
circuits (see Olsen, 1974, pp. 431–435).
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