Slew-induced distortion, also known as slew-rate distortion or slew-induced nonlinearity, is a phenomenon that occurs in operational amplifier (op-amp) circuits when the input signal changes too quickly for the op-amp to accurately follow the changes.
An operational amplifier has a finite maximum rate at which its output voltage can change in response to a change in the input voltage. This maximum rate of change is called the "slew rate" and is usually specified in volts per microsecond (V/Ξs). The slew rate represents the op-amp's ability to respond to rapid changes in the input signal without introducing distortion.
When the input signal changes too quickly and exceeds the op-amp's slew rate, the op-amp's output voltage will not be able to keep up with the rapid changes in the input voltage. This results in the output signal being "clipped" or distorted, as the op-amp is unable to accurately replicate the input signal's rapid variations. This distortion can lead to harmonics and other undesirable effects in the output signal, effectively degrading the fidelity of the signal being processed.
To mitigate slew-induced distortion, circuit designers may need to choose op-amps with higher slew rates, use external compensation techniques, or implement signal conditioning circuits to limit the rate of change of the input signal. It's important to consider the expected frequency range and amplitude of the input signal to ensure that the chosen op-amp can handle the required slew rate without introducing significant distortion.