The non-inverting gain is easier to scan when the input stays fixed and the feedback ratio changes. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

The non-inverting gain includes the one

With equal feedback and ground resistors, the gain is 2. The 2 volt input becomes 4 volts.

Vout=(1+2 ohm2 ohm)2 V=4 VV_{\text{out}}=\left(1+\frac{2\ \text{ohm}}{2\ \text{ohm}}\right)2\ \text{V}=4\ \text{V}
Non-inverting gain scan rowThe feedback divider forces the minus input to match the plus input.+-op amprails -12 V to 12 VVout 4 VV+ 2 VV- 2 VI+ 0 AI- 0 AVin 2 VRg 2 ohmRf 2 ohmV+ = V-noninverting

A larger feedback resistor raises the gain

The feedback resistor increases to 4 ohms against the same ground resistor. The gain is 3, so the output is 6 volts.

Vout=(1+4 ohm2 ohm)2 V=6 VV_{\text{out}}=\left(1+\frac{4\ \text{ohm}}{2\ \text{ohm}}\right)2\ \text{V}=6\ \text{V}
Non-inverting gain scan rowThe plus-one term remains visible in the formula.+-op amprails -12 V to 12 VVout 6 VV+ 2 VV- 2 VI+ 0 AI- 0 AVin 2 VRg 2 ohmRf 4 ohmV+ = V-noninverting

The third row keeps the same input and divider rule

With feedback resistance 6 ohms, the gain is 4. The same input gives 8 volts.

Vout=(1+6 ohm2 ohm)2 V=8 VV_{\text{out}}=\left(1+\frac{6\ \text{ohm}}{2\ \text{ohm}}\right)2\ \text{V}=8\ \text{V}
Non-inverting gain scan rowThree rows separate the feedback ratio from the input voltage.+-op amprails -12 V to 12 VVout 8 VV+ 2 VV- 2 VI+ 0 AI- 0 AVin 2 VRg 2 ohmRf 6 ohmV+ = V-noninverting