The modern operational amplifier is a solid state,
high gain, DC voltage amplifier.
Practical feedback circuits employing it are based
on the circuits that were derived in the preceding
section using the
ideal operational amplifier model. Substituting a real for
an
ideal operational
amplifier will result in some predictable variation from ideal operation that is negligibly small in many
applications. This section is intended to acquaint the reader with the characteristics of
the
real devices so that they may be utilized to the fullest possible extent in practical circuits.
In the case of the ideal operational amplifier,
circuit operation was seen to be dependent
entirely on the feedback used.
It is possible
to use the real operational amplifier open loop, but control and stability problems are encountered due to the high open loop gain (X100000 typically at DC). Random noise from the input circuit and noise generated within the operational amplifier
itself plus any variations in amplifier characteristics due to temperature change or
aging components are all multiplied by open loop gain. Slight variations in the manufactured unit become noticeable due to this effect; hence open loop specifications are sometimes given conservative “typical” values.
Open loop operational amplifier specifications have a relatively remote connection to closed loop operation of a circuit since they do not as much define circuit operation as they do limit it. The sheer numbers of useful operational amplifier circuits make it impossible for a manufacturer to
completely
specify closed loop operation. Since each closed loop circuit is, in essence, a
special case, it is necessary to understand both open and closed
loop characteristics before the
intelligent design of circuitry using operational amplifier can begin. Any statements that are to be made about operational amplifier circuits must be qualified by the information “open loop” or “closed loop,” and the character of the feedback should be specified for
“closed loop”
information.
The open loop gain, A, is measured by the slope of the curve so it
can
be seen that
the
operational amplifier only
amplifies between the saturation values of EO.The slope of
the
amplifying portion of the transfer curve is dependent
on the frequency of the
input voltage while the saturation voltages remain constant. This relation between input and output holds regardless of the feedback configuration used as long as the amplifier is not in overload.
The “well behaved” aspect of this operational amplifier is the fact that its transfer curve goes through the origin. In practice, all operational amplifiers exhibit offset, a fault that effectively shifts the transfer
curve from
the
origin.
To
complicate matters further,
this offset value will wander,
producing
drift. Both of
these phenomena are of
the
same order
of
magnitude as the input voltage necessary to drive the open loop amplifier into saturation and a necessary part of circuit design is to minimize their effect.
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