# 5.6: Solute Effect - Raoult’s Law


On the other hand, the atmosphere is not very clean either. There are all kinds of dirt and other particles in the atmosphere. Some of these are hydrophilic (i.e., they like water) and water soluble (i.e., they dissolve in water). So let’s see what the effect of soluble CCN might be on the water evaporation rate for a flat water surface. We’ll then put the curvature and the solute effects together.

First, here are some important definitions:

• Solvent: The chemical that another chemical is being dissolved into. For us, the solvent is H2O.
• Solute: The chemical that is being dissolved in the solvent.

The simplest view of this effect is that solute molecules are evenly distributed in the water (solvent). Therefore, some solute molecules occupy surface sites that would otherwise be occupied by water molecules. Thus, the solute prevents water molecules from evaporating from those sites. Adding more solute means that more surface sites would be occupied by solute molecules and water vapor would have even less opportunity to break hydrogen bonds and escape the liquid. The real view is more complicated by the electrostatic interactions between water and solute molecules that cause an attraction between water and solute molecules, but the basic result is the same as the simple view.

Because the evaporation rate is lowered, that means that there will be net condensation until the water vapor flux to the surface matches the water vapor flux leaving the surface. When equilibrium is established between the lower evaporation and condensation, the condensation will be less, which means that the water saturation vapor pressure will be lower. The equilibrium vapor pressure is less than es, which, remember, is the saturation vapor pressure over a flat surface of pure water. As the amount of solute is increased, the equilibrium vapor pressure of the solution will be even less.

We can quantify this equilibrium vapor pressure over a solution with a few simple equations.

The mole fraction is defined as:

$\chi_{s}=\frac{n_{s}}{n_{w}+n_{s}} \approx \frac{n_{s}}{n_{L}}$

if $$n_{w}>n_{s}$$. $$n_w$$ is the number of moles of water in a liter of solution, ns is the number of moles of solute in a liter of solution, and nL is the number of moles per liter of pure water.

As a result, the evaporation rate of the water molecules from the surface decreases. This can be written as Raoult’s Law:

$e_{s o l}=e_{s} \cdot\left(1-\chi_{s}\right)$

We can approximate Raoult’s Law for a reasonably dilute solution by writing:

$\chi_{s} \approx \frac{n_{s}}{n_{L}}=\frac{i N_{s}}{n_{L} V_{d r o p}}=\frac{i N_{s}}{n_{L}\left(4 \pi r_{d}^{3} / 3\right)} \equiv \frac{B i N_{s}}{r_{d}^{3}}, \quad$

where

$B=\frac{3}{4 \pi n_{L}}$

Ns is the total moles of solute. Note that an i was added. This factor is called the Van ’t Hoff factor and it accounts for the splitting of some solutes into components when they dissolve. An example is salt, NaCl, which splits into two ions in solution, $$\ce{Na^{+}}$$ and $$\ce{Cl{-}}$$, which means that $$i = 2$$ in this case.

5.6: Solute Effect - Raoult’s Law is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by William Brune (John A. Dutton: e-Education Institute) via source content that was edited to conform to the style and standards of the LibreTexts platform; a detailed edit history is available upon request.