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Bias Circuit

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11.1.1 Voltage Gain of the Noninverting Resistor Feedback Amplifier<br />

In the circuit diagram of Fig. 11.3, an input signal voltage Vs is attached to resistor Rx. By<br />

definition, the output terminal voltage is positive for a plus input. Hence, this is the<br />

noninverting amplifier. Here we obtain the relationship between the amplifier gain, avo = Vo/Vs,<br />

and the open-loop gain (opamp gain), avo = Vo/V , and the circuit resistors.<br />

Figure 11.3. Non-inverting or voltage amplifier (series-shunt). The<br />

input resistance is essentially infinite.<br />

With a signal applied to the plus input terminal, the responding output voltage is fed back to<br />

the resistor Ry. The voltage across Ry, Vf, and Vo (signal) are related by<br />

Equation 11.1<br />

This is just the voltage-divider relation, which applies in this case, as negligible current flows<br />

into the input terminals of the opamp. Variable Vf is used in lieu of VRy to distinguish it from<br />

the dc value of the voltage across Ry. This use is also consistent with the fact that Vf is<br />

technically a signal feedback voltage.<br />

The input signal voltage Vs adds up to<br />

Equation 11.2<br />

where (11.1) is used to eliminate Vf. (The voltage drop across Rx is essentially zero.) This leads<br />

directly to the relation for amplifier gain, which is<br />

Equation 11.3<br />

with (ideal noninverting gain).

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