Feedback in the Inverting Amplifier Electronics Help

To investigate the effect of open-loop gain A and feedback ratio f3 on the closedloop gain of the inverting amplifier. let us recall equations 13-6 and 13-7 from Section 13-1:

Once again we see that the closed-loop gain reduces to the ideal amplifier value. -RlR” when A = 00. Notice that the denominator of (13-28) is the same as that of (13-21). the equation for the closed-loop gain of the noninvcrting amplifier. Furthermore. the quantity RI/(UI + R,) is also the feedback ratio f3 for the inverting amplifier. This (act is illustrated in Figure 13-10. which shows the feedback paths of both configurations when their signal inputs are grounded. Think of the amplifier output as a source that generates the feedback signal. By the superposition principle.

We can analyze the contribution of the feedback source by grounding all other signal sources. When this is done, as shown in Figure 13-10, we see that the feedback \ <‘II age in both configurations is developed across the R1-Rf voltage divider. and fJ .. R,/(RI + I?f} ill both cases. In view of this fact, we can write (13-X)

Toward developing a feedback model for the inverting amplifier, consider the block diagram shown in Figure 13-11. This diagram is quite similar to Figure I3-X(b) for the noninverting amplifier, except that we now denote the open loop gain by A. Note also that the summing junction now adds its two inputs. Since v” is inverted, so is the feedback voltage, and adding a negative voltage to v is the same as subtracting a positive one from it. In other words, we still have a negativefeedback situation. Notice that we use v to represent an arbitrary input voltage, rather than Vii” because we will have to make some adjustments in this model before it can truly represent the inverting amplifier.

Comparing (13-31) with the equation we have already developed for the inverting nrnpliflcr (equation 13-29), we see that they differ slightly. We must therefore adjust the model so that it produces the same result as (13-29). Equation 13-3\ for the model can be written

Equation D-.B shows that multiplication of the model equation by the constant R/(RI + Rf) gives liS exactly the same result (equation D-29 with V 1/, = 11) that we obtain for the inverting amplifier. Therefore, we modify the block-diagram model in Figure 13-11 by adding a block that multiplies the input by /(/(NI + R,). The complete feed hack model is shown in Figure 13-12.

As can be seen in Figure 13-12, the loop gain for the inverting amplifier is 1\{3, the same as that for the lioninverting amplifier. From equation D-2lJ, it is apparent that the greater the loop gain, the closer the closed-loop gain is to its value in the deal inverting amplifier. – R/R,. II can he shown that the input resistance seen by till’ signal source driving the inverting amplifier

This equation confirms that the input resistance is HI for the ideal inverting amplifier. where ;\ = co , II also shows thai the input resistance decreases with increasing values of A.
As with the noninvcrting amplifier. the output resistance of the inverting amplifier is decreased by negative feedback. In Iact, the relationship between output resistance and loop gain is the same for both:

The amplifier shown in Figure 13-13 has open-loop gain equal to 2500 and openloop output resistance I()O n. rind
I. the magnitude of till: loop gain
2. the closed-loop gain:
3. the input resistance seen
4. the closed-loop output resistance

Use SPICE to find the closed-loop voltage gain. the input resistance seen by VII/. SPICE and the output resistance of the inverting amplifier in Example 13-5.

Solution. Figure 13-14 shows how we can use a voltage-controlled voltage source (EOP) to model an operational amplifier in SPICE. Notice that the inverting property of the amplifier is realized by connecting the positive terminal (N +) of EOP to ground (node 0). The voltage source is controlled by the voltage between nodes 2 and 0 (NC+ and NC-. respectively). Thus. node 2 corresponds to the inverting input of the amplifier in Figure 13-13. Notice that till! simulated amplifier has infinite input impedance. since there is ,HI open circuit between nodes 2 and O.

Since VIN = I V. the output voltage at node 4. V(4), is nurncricnlly equal to the dosed-loop voltage gain. The results of a program run reveal that V(4) = -96.11, in close agreement with till! gain calculated in Example 13-5. SPICE computes the magnitude of I(VIN) to he n.MI 1111\. so the input resistance.

To find the output resistance of the amplifier, we must compute the current that flows through a short circuit connected to the output, since 1′” = Vt.(open circuit)/h(short circuit). A zero-valued dummy voltage source, VDUM, connected between nodes 4 and 0 effectively shorts the output to ground. The current in VDUM is then the short-circuit output current. SPIC~ computes this value to be I{VDUM) = 24.7 A. Thus,

Posted on November 19, 2015 in Operational Ampiifier Theory

Share the Story

Back to Top
Share This