@article {1526,
title = {Coarsening and solidification via solvent-annealing in thin liquid films},
journal = {J. Fluid Mech.},
volume = {723},
year = {2013},
month = {2013/5/25},
pages = {69-90},
publisher = {Cambridge University Press},
abstract = {We examine solidification in thin liquid films produced by annealing amorphous \${\mathrm{Alq} }_{3} \$ (tris-(8-hydroxyquinoline) aluminium)
in methanol vapour. Micrographs acquired during annealing capture the
evolution of the film: the initially-uniform film breaks up into drops
that coarsen, and single crystals of \${\mathrm{Alq} }_{3} \$ nucleate
randomly on the substrate and grow as slender . The growth of these
needles appears to follow power-law behaviour, where the growth exponent,
\$\gamma \$, depends on the thickness of the deposited \${\mathrm{Alq}
}_{3} \$ film. The evolution of the thin film is modelled by a lubrication
equation, and an advection{\textendash}diffusion equation captures the transport of
\${\mathrm{Alq} }_{3} \$ and methanol within the film. We define a
dimensionless transport parameter, \$\alpha \$, which is analogous to an
inverse Sherwood number and quantifies the relative effects of diffusion-
and coarsening-driven advection. For large \$\alpha \$-values, the model
recovers the theory of one-dimensional, diffusion-driven solidification,
such that \$\gamma \rightarrow 1/ 2\$. For low \$\alpha \$-values, the
collapse of drops, i.e. coarsening, drives flow and regulates the growth
of needles. Within this regime, we identify two relevant limits: needles
that are small compared to the typical drop size, and those that are
large. Both scaling analysis and simulations of the full model reveal that
\$\gamma \rightarrow 2/ 5\$ for small needles and \$\gamma \rightarrow 0.
29\$ for large needles.
},
keywords = {2013, 2013 and earlier, interfacial flows (free surface), low-Reynolds-number flows, lubrication theory},
isbn = {0022-1120},
doi = {10.1017/jfm.2013.115},
author = {Yu, Tony S and Vladimir Bulovi{\'c} and Hosoi, A E}
}