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Main Approximations of the LSW Approach

2) The mean-field approximation is applied, that is, the supersaturation of the parent phase A = (C — in the vicinity of any precipitate is taken as one and the same, common for the whole system without considering correlations between the size and local supersaturation. [Pg.136]

3) The steady state approximation is employed. This means that the Laplace equation V C S 0 is solved rather than the diffusion equation (second Pick s [Pg.136]

Here a for the case of precipitation of an almost pure element B from a diluted solution of B in A equals [Pg.137]

Taking into account the steady state and Gibbs-Thomson conditions, the growth (or dissolution) rate for a spherical precipitate is determined by the following balance equation at the moving spherical boimdary  [Pg.137]

The critical radius increases with time (as supersaturation diminishes), catching up with the growing particles one by one, which then start dissolving (ultimately, the only one must remain in a finite system, yet this falls beyond the statistical theory). [Pg.137]


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