Calculate the voltage gain of the following circuit.
The analysis is similar to that used in earlier examples. First we note that, as in earlier circuits, the negative feedback forces V_{-} to equal V_{+} , and therefore
V_{-} = V_{+}Since no current flows into the inputs of the op-amp, V_{-} and V_{+} are determined by the potential dividers formed by the resistors.
V_{-} is easy to calculate and is given by
V_{-} = V_{0} \frac{10 KΩ}{10 KΩ + 20 KΩ} = \frac{V_{0}}{3}V_{+} is slightly more complicated to compute, since it is determined by the two input voltages. However, applying the principle of superposition, we know that the voltage on V_{+} will be equal to the sum of the voltages that would be generated if each input voltage were applied separately.
If V_{1} is applied while V_{2} is set to zero, then the resistor connected to V_{2} effectively goes to ground and is in parallel with the existing 10 kΩ resistor that goes from V_{+} to ground. Therefore,
V_{+} = V_{1} \frac{10 KΩ//10 KΩ}{10 KΩ//10 KΩ + 10 KΩ} = V_{1}\frac{5 KΩ}{5 KΩ + 10 KΩ} =\frac{V_{1}}{3}If now V_{2} is applied while V_{1} is set to zero, we have a directly equivalent situation and clearly, because of the symmetry of the circuit,
V_{+} = V_{2} \frac{10 KΩ//10 KΩ}{10 KΩ//10 KΩ + 10 KΩ} = V_{2}\frac{5 KΩ}{5 KΩ + 10 KΩ} =\frac{V_{2}}{3}Therefore if both inputs are applied simultaneously we have
V_{+} = \frac{V_{1}}{3} + \frac{V_{2}}{3}Now since
V_{-} = V_{+}we have
\frac{V_{0}}{3} = \frac{V_{1}}{3} + \frac{V_{2}}{3}and
V_{o} = V_{1} + V_{2}Thus the circuit is a non-inverting adder. This circuit can be extended to have any number of inputs (see Appendix C).