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Chapter II Solution Growth….<br />

pressure of the liquid phase at the same temperature known as equilibrium<br />

pressure P*, the vapor is described as under-saturated, saturated or<br />

supersaturated, respectively with respect to the liquid phase. The under-<br />

saturated state and saturated state are thermodynamically stable. The<br />

supersaturated vapor in contact with the bulk liquid phase will condense into<br />

the liquid until saturation is obtained.<br />

In a supersaturated vapor, not only monomers A1 are present but also<br />

embryos, which are clusters of molecules bound together by their<br />

intermolecular interactions. The mechanisms of formation of such embryos is<br />

the simple collision process consisting of a single molecules A1 with a cluster<br />

Ai-1 consisting of (i-1) molecules and hence giving rise to a cluster Ai as follows<br />

A1 + Ai-1 → Ai<br />

The cluster Ai may also form by the evaporation of a molecule from some<br />

cluster Ai+1 as follows,<br />

Ai+1 → Ai + A1<br />

The phase change takes place by single molecule attached to<br />

embryos of various sizes, this process predominant slightly over the reverse<br />

process in which the different embryos lose single molecules. The size<br />

distribution of embryos changes with time, the numbers of the larger ones<br />

increasing. There is a critical size which is unstable equilibrium with the<br />

supersaturated vapor and this critical nucleus forms the bottleneck of the<br />

phase change. Once embryos achieve this critical size, there is a high<br />

probability that they will grow, relatively unhindered, to microscopic size.<br />

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