One can make an estimation. Consider the first part, liquid and its vapour in equilibrium. Let the vapour concentration be $n_0$ and temperature $T$ such that vapour can be treated as an ideal gas (that is there isn't much vapour).
Then the flow of molecules flying from vapour to liquid is
$$F(n_0) = \frac{1}{4} n_0 \langle v\rangle = \frac{1}{4} n_0 \sqrt{\frac{8kT}{\pi m}}$$
There is an equal but opposite flux from liquid to vapour. One may assume that this flux will remain the same if the vapour was removed.
Let $n(t)$ be the constantly increasing vapour concentration after the removing. Then it's behaviour is governed by the differential equation
$$V \frac{dn}{dt} = \left(F(n_0)-F(n) \right) S $$
where $V$ is the volume available for the vapour and $S$ is the surface area of evaporation. This equation implies that the already evaporated vapour is in equilibrium, which I guess shouldn’t be very wrong in the case in hand.
Once again, the argument is not applicable near the critical point since there vapour is almost like liquid.