SLOA332A July 2023 – September 2024 LMV821-N , LMV831 , OPA2991 , OPA345 , OPA376 , OPA376-Q1 , OPA377 , OPA377-Q1 , OPA4991 , OPA991 , TL074 , TLV376 , TLV9001 , TLV9002 , TS321
Figure 3-2 has two schematics that produce a 1V output step. In the left circuit, the 1V is amplified by a noise gain of 1. In the right circuit, 10mV is amplified by a noise gain of 100. In these non-inverting circuits, signal gain and noise gain are equivalent.
Figure 5-1 is the resulting simulation waveform from the Figure 5-1 schematics. The unity gain (black curve) rises at 2V/µs, which is the same as the data sheet specification. The 100 gain (red curve) has a slower slew rate that continues to decrease as the voltage rises. The initial slew rate for a 10mV input step, following the Figure 3-1 output, is 14% of the natural slew maximum of 0.5V/µs, which is 70mV/µs. By the time the waveform rises half way, the VID has dropped to 5mV. Now, the SR is the Figure 3-1 output 7% (of 0.5V/µs), which is 35mV/µs.
Even if the TLV9002 device did not have slew boost, the unity gain slew rate (0.5V/µs natural) is much faster than a G=100 curve. Slew boost or not, a smaller input signal with higher gain must always have a slower observed slew rate than a larger input signal with lower gain.