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/content/aip/journal/jcp/132/4/10.1063/1.3299320
1.
1.V. A. Shneidman, J. Chem. Phys. 132, 047101 (2010).
2.
2.V. Holten and M. E. H. van Dongen, J. Chem. Phys. 130, 014102 (2009).
http://dx.doi.org/10.1063/1.3054634
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3.V. A. Shneidman, personal communication (2009).
4.
4.V. A. Shneidman, J. Chem. Phys. 115, 8141 (2001).
http://dx.doi.org/10.1063/1.1409366
http://aip.metastore.ingenta.com/content/aip/journal/jcp/132/4/10.1063/1.3299320
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/content/aip/journal/jcp/132/4/10.1063/1.3299320
2010-01-26
2016-10-01

Abstract

The analytical results presented in the comment of Shneidman for the droplet size distribution, the thickness of the distribution front, and the location of the stationary source are compared to our earlier numerical results. The agreement is very good in the case of the size distribution and the source location, but the analytical result for the thickness of the front deviates from the numerical result at high supersaturations.

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