A sharp change in lapse rate will (absent sharp changes in optical thickness per unit distance, which occurs at TOA and at the surface even in wavelength bands dominated by well - mixed gases) tend to differ from radiative equilibrium — the inflection point may correspond to a maximum deviation from radiative equilibrium if the radiative equilibrium profile has some intermediate lapse rate in that vicinity.
When optical thickness is large, the net flux will tend to be small, but the flux will vary with lapse rate (according to the corresponding Planck function «lapse rate») and a sufficiently
sharp change in that lapse rate could lead to some significant flux convergence or divergence at that level (net radiant heating or cooling).