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If you need an amplifier to boost an audio signal by exactly negative ten, you might think you can just hook up any two resistors that give a 10-to-1 ratio. But if you choose 10ฮฉ and 100ฮฉ, your signal source will crash, and if you choose 10Mฮฉ and 100Mฮฉ, your circuit will drown in background noise.
Designing an inverting amplifier requires balancing voltage gain, input impedance, and the practical reality of standard resistor series.
How do these two resistors actually set the gain and input resistance? Let's trace the signal through the circuit.
The Inverting Topology
In 1941, Bell Labs engineer Karl Swartzel designed the first operational amplifier summing circuit to perform real-time math for anti-aircraft gun directors during World War II.
An inverting amplifier connects the input signal through an input resistor Rinโ to the inverting input (โ), while a feedback resistor Rfโ connects that same node to the output.
๐Interactive diagram
Because negative feedback drives the difference between inputs to zero and the non-inverting input is grounded, the inverting terminal is held at a virtual ground (0V).
Since an ideal op-amp draws zero input current (Iโโ=0), all current through Rinโ must flow entirely through Rfโ:
RinโVinโโ0โ=Rfโ0โVoutโโโนAvโ=VinโVoutโโ=โRinโRfโโ
The input impedance (Zinโ)โthe effective resistance seen by the signal sourceโis simply equal to Rinโ, because the other side of Rinโ sits at 0V.
Now that we have the gain equation Avโ=โRfโ/Rinโ, what boundaries decide whether a resistor value is safe or dangerous to use?