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Bias Circuit

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Equation 11.4<br />

AvNI is the limiting form of the noninverting amplifier gain for avo . This is consistent with<br />

the fact that in the limit, V 0 and Vs = VRy. Thus, the output and input voltages are simply<br />

related by the voltage-divider relation. The result, (11.3), indicates that for avo>>AvNI, the<br />

voltage gain can simply be expressed in terms of the resistors and therefore is very<br />

predictable. If we make, for example, Rf = 10Ry, AvNI = 11, and (11.3) gives Av = 10.998, with<br />

avo = 40,000. The value for the opamp gain is typical for our project opamp. Note that due to<br />

the high resistance at the opamp input terminals, Rx has no influence on the gain.<br />

The noninverting amplifier has a very high input resistance and a low output resistance, as<br />

discussed in Unit 11.4. The amplifier technically falls into the category of a series – shunt<br />

feedback configuration or a voltage amplifier.<br />

11.1.2 Voltage Gain of the Inverting Resistor Feedback Amplifier<br />

To obtain the inverting amplifier, the signal is applied to the negative or inverting terminal as<br />

shown in Fig. 11.4. A positive signal results in a negative output voltage. The gain expression<br />

can be obtained with the loop equation from output to input:<br />

Equation 11.5<br />

Figure 11.4. Inverting or transresistance amplifier (shunt – shunt).<br />

The input resistance is equal to the signal-source resistance, Ry.<br />

and the loop equation at the input (voltage drop across Rx is zero)<br />

Equation 11.6<br />

Eliminating Is between (11.5) and (11.6) gives<br />

Equation 11.7

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