A precipitation reaction in a supersaturated metastable alloy starts with the formation of stable nuclei, then proceeds to a more or less marked growth regime and finally ends in a coarsening reaction. According to the classical nucleation theory,the nucleation rate J is mainly governed by the work of formation ΔF* of a critical nucleus with radius R* [1]: (1) $$ J\,\infty \,\exp [ - \,\Delta {F^{ * }}/kT]\,and\,\Delta {F^{ * }}\, = \,4\pi \,{R^{{ * 2}}}\bullet \sigma /3 $$ (σ: specific interfacial energy). A nucleated spherical particle of radius R and solute concentration Cp embedded in a supersaturated matrix of mean solute concentration c(t) will grow at a rate [2] (D: diffusion coefficient): (2) $$ \frac{{dR}}{{dt}}\, = \,v(t)\, = \,\frac{{\overline c (t)\, - \,{c_{R}}}}{{{c_{{P\, - \,}}}{c_{R}}}}\,\frac{D}{R} $$
CITATION STYLE
Kampmann, R., & Wagner, R. (1986). Phase Transformations in Fe-Cu-Alloys -SANS-Experiments and Theory (pp. 73–77). https://doi.org/10.1007/978-3-642-71007-0_12
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