Ok, so I was thinking about your problem, Fledarmus.
If you have equimolar amounts of two compounds in a reaction flask, but one is a solid which has settled to the bottom, what are the odds that any molecule of the compound in solution will be next to a molecule of the undissolved material?
So, I attempted to do a basic model of this. One difficulty was: How do I represent the probability of a collision? What I decided to do was use the surface area of a sphere to represent the odds of one molecule's probability to be collided with. I assumed both different molecules (my solvated and non-solvated molecules, respectively), were of equal radius, and the radius is 1. I also assumed the solid has zero solubility in the solution. These assumptions may turn out to be unnecessary, but we'll see.
So, I am dealing with molecules that are perfect spheres with a radius 1. If I have a million "solid" molecules, the sum of the surface area of each molecule is:
[4*PI*r^2]*1000000 = 12.57 x 10^6 sq. units.
This number would correspond to their square area if the solid were completely solvated. Then, for equal amounts of two reactants, there would be a 50% chance of collision.
Now, if the solid has zero solubility, it exists only as a solid. I took two extremes. If the particles are evenly divided on the floor of the glass, with spacing between each particle, then we could say that only the top half of the molecules are available to reaction. In this case, their surface area is simply divided by two. Their "ability" to collide or react with another molecule is halved, so there is a 25% chance of collision.
In the other extreme, the molecules all aggregate together at the bottom of the glass. In this case, I decided to assume the form of a hemisphere on the bottom. On an atomic scale, the edge of this hemisphere is jagged and not smooth. This would increase the effective surface area, but given that orientation also plays a role in a reaction, this may increase or decrease reactivity. I decided to exclude jaggedness. I'm not even sure yet how to model it if I had the information necessary.
A million perfect spheres of radius 1 have a volume of
4/3*PI*1^3*1000000 = 4.19 x 10^6 cu. units.
This is the volume of the hemisphere. The equation for the volume of a hemisphere is one half times the equation for the volume of a sphere. ie:
(4/3)/2*PI*r^3=2/3*PI*r^3
The radius of this hemisphere is therefore:
[(4.19 x 10^6 cu. units)*(3/2)/(PI)]^(1/3)= 126 units.
The surface area of a hemisphere of radius 126 units is:
2*PI*(126)^2=9.97 x 10^4 sq. units.
Taking the ratio of this surface area, representing the availability for collision, with the maximum surface area available when solvated, I get:
(9.97 x 10^4)/(12.57 x 10^6) *100% = 0.8 %.
So, an unsolvated solid phase molecule is 99.2% less available than a fully solvated one. But this final calculation is a little meaningless because in a solid there are lattice energies which I think should raise the activation energy of a reaction.
A lot of this is dependent on the radius of the molecules involved. This could likely change the results by an order of magnitude or more. Also orientation requirements could have a massive effect. Furthermore, the collision velocity is halved, since only one molecule is moving and the solid phase molecule is at rest. If the lattice energy raises the activation energy, but the molecules have half the velocity (quarter the kinetic energy), the reaction is probably even less likely to occur. I think the energy required for the reaction and orientation make up the greatest amount of error in the model assumed, both of which should decrease the likelihood of a reaction occuring. The model is more or less an "at best" scenario. "At best," the K value is altered by 0.8%, which is really small. I guess we can conclude that the contribution really is pretty much nothing.
EDITOk, I made a mistake. It turns out that, the more molecules you have, the greater this difference becomes. I took one mole of particles, 6.022 x 10^23, performed the same calculation, and the 0.8% became 9.4 x 10^-7 %. One million particles was just too small, unless you are dealing with a femtomolar concentration. Considering lattice energies and kinetic energy of the collision, I think really that the result is even more infinitesimal than I had thought. Even considering a solubility % of the solid is probably unnecessary. The difference would still likely remain very small.
Assuming that you can get perfect mixing of your heterogeneous solution and every single particle of your undissolved solid is equidistant from every other particle, how small would the particles have to be to make even a 0.1% statistical contribution to collisions with the dissolved component?
I'm not really sure how to model this. My understanding was that if all of the particles are equidistant from one another in a solution, then, that is the definition of being solvated?