The effects of interfacial energy on nucleation can be evaluated using a sphere as the form of the new phase.
Figure 05. Spherical Nucleus Gibbs Energy vs. Radius. Click on the image to see a larger version with a more detailed explanation.
When calculating the Gibbs energy change to grow the nucleus, the volume term will become more important as the radius increases.
In Figure 05, example values of interfacial Gibbs energy per nm2 (σA) and reaction Gibbs energy per nm3 (ΔGV) are used to calculate the total Gibbs energy change (ΔGT) for a nucleus of radius R. A graph of the total Gibbs energy change as a function of radius in Figure 05 shows that ΔGT begins to decline when the radius of a spherical nucleus reaches a critical value (the maximum of ΔGT on the graph). It is at this radius that the Gibbs energy decreases with nucleus growth. Declining ΔGT with growth of the product phase is necessary for the reaction to proceed spontaneously.
Thus, if the size of the nucleus of a new phase produced by a reaction is large enough, the phase will grow and the reaction will proceed. However, if the new phase is too small, interfacial energy will prevent it from growing further. Every nucleus must begin very small. What circumstances will lead to the appearance of a nucleus that is large enough to grow spontaneously?