Kazys said:
My intention was to illustrate that some common and very familiar
phenomena are still not completely understood.
Saying that we do not know the exact way in which water molecules cluster, or the distribution of kinetic energy of the molecules, is not the same as saying we do not know how water can evaporate. Nothing that you are saying in any way invalidates the simple explanation: water evaporates because some water molecules have sufficient kinetic energy to escape.
In fact, that simple explanation is
not precisely correct--but not for any reason that you gave. Consider: if some water molecules in the liquid have a high enough kinetic energy to escape, then some water molecules in the vapor should also have
low enough kinetic energy to be captured. So what is actually going on is a dynamic process, with water molecules escaping from the liquid and being captured from the gas. In equilibrium, the rates of both processes will be the same, and macroscopically you have a stable state with a given number of molecules of liquid and a given number of molecules of vapor. Out of equilibrium, the rates are not the same: for example, when water boils, the rate of molecules going from liquid to gas is higher than the rate of molecules going from gas to liquid. When water vapor condenses, the opposite is true.
You could object, of course, that the processes involved in my more elaborate explanation are not completely understood either. But by the criterion you appear to be using, nothing is completely understood. All of our current theories are incomplete. All of them have elements that we have not derived from first principles but just assumed. So saying that a particular explanation is not complete is just repeating a commonplace fact about all scientific explanations.
Kazys said:
until the actual distribution is known the precise mechanism used by an escaping molecule cannot be determined.
This is false. We can know that a molecule of sufficient kinetic energy will escape, without knowing exactly which molecules have that amount of kinetic energy at a given instant. The mechanism of escape is obvious: the kinetic energy of the molecule is greater than the binding energy between it and neighboring molecules.
Kazys said:
Re. the Maxwellian distribution - it provides a good approximation for the distribution of kinetic energy of water molecules in the vapor phase, by assumption it has often been applied also to the liquid phase, that is not correct.
Can you give any examples of a mainstream reference assuming that the liquid phase has a Maxwellian distribution? And can you give mainstream references that show why that assumption is not correct?
Kazys said:
The "by definition" comment refers
to the conditions that Maxwell used to derive a distribution of kinetic energy for a statistically large number of interacting entities.
These are: interaction occurs between 2 entities at a time, these collisions are elastic, scattering is isotropic. None of
these conditions apply for liquid water.
This is true; but it does not show that the distribution of kinetic energies in a liquid is not Maxwellian. It only shows that Maxwell's derivation of that result cannot be applied to a liquid, at least not in the way it applies to a gas.