Closed-loop gain 2026-10-20
The closed-loop gain is the input-to-output transfer after closing the feedback connection. In the elementary noninverting voltage model it tends to for large stable loop gain, rather than retaining the uncertain open-loop gain . A frequency-dependent transfer must be checked for stability before that approximation is used.
Inverting two-pole band-pass filter Created 2026-10-20 Updated 2026-11-05
An ideal inverting operational amplifier with series input and parallel feedback has the displayed transfer function, where and . Its peak is at with voltage gain . A wide input-high-pass/feedback-low-pass separation produces a broad plateau, not a narrow resonance. Validity requires stable negative feedback, sufficient loop gain and linear output operation.
Loop gain 2026-10-20
The loop gain is the product of the forward amplifier response and the return-network fraction, with the summing-junction minus sign kept explicit. Closed-loop poles are determined by in this convention. Large low-frequency magnitude controls gain error, while frequency-dependent phase affects stability.
Noise gain of an operational amplifier Created 2026-10-20 Updated 2026-11-05
The closed-loop gain from an equivalent differential input-voltage disturbance to the output is the noise gain. For an ideal-input inverting amplifier, and , although the voltage gain is . A dominant-pole amplifier has approximate closed-loop bandwidth when loop gain is large at low frequency and the circuit is stable.
Non-inverting operational amplifier Created 2026-10-20 Updated 2026-11-05
A non-inverting operational amplifier applies the signal to its non-inverting input and returns part of the output to its inverting input through negative feedback. Connect resistor from the output to the inverting input, and resistor from that input to a reference circuit node at electric potential .
In stable, unsaturated ideal operation, the inputs draw no electric current and their electric potentials are equal. Writing the signal as , Kirchhoff's current law at the inverting input givessoFor a grounded reference circuit node, the voltage gain is . For example, and give gain three. The equal-input-potential approximation requires sufficiently large loop gain; amplifier saturation or unstable feedback invalidates it.[ref]
Operational-amplifier negative feedback 2026-10-20
Return a fraction of the output to the inverting input so that it opposes the input difference. Large stable loop gain makes the closed-loop gain depend mainly on the external feedback ratio rather than the uncertain open-loop gain. Frequency-dependent phase lag can destabilize the loop; saturation and finite slew rate also limit the approximation.[ref]
In an operational-amplifier negative feedback loop, an operational amplifier has large open-loop gain , with . Feeding a fraction back to the inverting input opposes an output increase. For a non-inverting signal input,Its sensitivity to open-loop gain changes is reduced by . Thus resistor ratios can set a reproducible gain despite device variation; feedback also suppresses internal distortion and reduces output impedance. Gain is traded for usable bandwidth, subject to the amplifier's frequency response.
For the non-inverting connection, place between output and inverting input and between that input and ground. Then , giving gain . For an inverting connection, ground the non-inverting input, inject the signal through and return from output to the inverting node. Small differential input and negligible input current then give gain . The near-zero node is a virtual ground, not a physical ground connection.
The feedback must remain stable at the frequencies where loop gain matters. Extra phase lag can turn the intended opposition into oscillation; adequate phase margin, supply headroom, input common-mode range, output-current capability and slew rate are required. Feedback neither prevents clipping nor removes all input noise.[ref]