Transformations of the distribution of nuclei formed in a nucleation pulse: Interface-limited growth
J. Chem. Phys. 131, 164115 (2009); doi:10.1063/1.3254322
Published 29 October 2009
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A typical nucleation-growth process is considered: a system is quenched into a supersaturated state with a small critical radius r
and is allowed to nucleate during a finite time interval tn, after which the supersaturation is abruptly reduced to a fixed value with a larger critical radius r
. The size-distribution of nucleated particles f(r,t) further evolves due to their deterministic growth and decay for r larger or smaller than r
, respectively. A general analytic expressions for f(r,t) is obtained, and it is shown that after a large growth time t this distribution approaches an asymptotic shape determined by two dimensionless parameters,
related to tn, and
=r
/r
. This shape is strongly asymmetric with an exponential and double-exponential cutoffs at small and large sizes, respectively, and with a broad near-flat top in case of a long pulse. Conversely, for a short pulse the distribution acquires a distinct maximum at r=rmax(t) and approaches a universal shape exp[
−e
], with 
r−rmax, independent of the pulse duration. General asymptotic predictions are examined in terms of Zeldovich–Frenkel nucleation model where the entire transient behavior can be described in terms of the Lambert W function. Modifications for the Turnbull–Fisher model are also considered, and analytics is compared with exact numerics. Results are expected to have direct implementations in analysis of two-step annealing crystallization experiments, although other applications might be anticipated due to universality of the nucleation pulse technique.
©2009 American Institute of Physics
related to tn, and
=r
−e
], with 
r−rmax, independent of the pulse duration. General asymptotic predictions are examined in terms of Zeldovich–Frenkel nucleation model where the entire transient behavior can be described in terms of the Lambert W function. Modifications for the Turnbull–Fisher model are also considered, and analytics is compared with exact numerics. Results are expected to have direct implementations in analysis of two-step annealing crystallization experiments, although other applications might be anticipated due to universality of the nucleation pulse technique.
©2009 American Institute of Physics
| History: | Received 18 June 2009; accepted 5 October 2009; published 29 October 2009 |
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http://link.aip.org/link/?JCPSA6/131/164115/1 |
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