When complex
networks are put into the feedback loop, the circuits get harder to
analyze because the simple gain equations cannot be used. The usual
technique is to write and solve node or loop equations. There is only
one input voltage, so superposition is not of any use, but Thevenin’s
theorem can be used as is shown in the example problem given below.
Sometimes it is desirable to have a low resistance path to ground in
the feedback loop. Standard inverting op amps can not do this when
the driving circuit sets the input resistor value, and the gain
specification sets the feedback resistor value. Inserting a T network
in the feedback loop (FIgure 3–7) yields a degree of freedom that
enables both specifications to be met with a low dc resistance path
in the feedback loop.
Figure 3–7. T
Network in Feedback Loop
Break the circuit at
point X–Y, stand on the terminals looking into R4, and calculate
the Thevenin equivalent voltage as shown in Equation 3–15. The
Thevenin equivalent impedance is calculated in Equation 3–16.
Replace the output
circuit with the Thevenin equivalent circuit as shown in Figure 5–8,
and calculate the gain with the aid of the inverting gain equation as
shown in Equation 3–17.
Figure 3–8.
Thevenin’s Theorem Applied to T Network
Substituting the
Thevenin equivalents into Equation 3–17 yields Equation 3–18.
Algebraic
manipulation yields Equation 3–19.
Specifications for
the circuit you are required to build are an inverting amplifier with
an input resistance of 10 k (RG = 10 k), a gain of 100, and a
feedback resistance of 20 K or less. The inverting op amp circuit can
not meet these specifications because RF must equal 1000 k. Inserting
a T network with R2 = R4 = 10 k and R3 = 485 k approximately meets
the specifications.
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