TY - JOUR
T1 - Role of natural convection in the dissolution of sessile droplets
AU - Dietrich, Erik
AU - Wildeman, Sander
AU - Visser, Claas Willem
AU - Hofhuis, Kevin
AU - Kooij, E. Stefan
AU - Zandvliet, Harold J.W.
AU - Lohse, Detlef
PY - 2016
Y1 - 2016
N2 - The dissolution process of small (initial (equivalent) radius R0 < 1 mm) long-chain alcohol (of various types) sessile droplets in water is studied, disentangling diffusive and convective contributions. The latter can arise for high solubilities of the alcohol, as the density of the alcohol–water mixture is then considerably less than that of pure water, giving rise to buoyancy-driven convection. The convective flow around the droplets is measured, using micro-particle image velocimetry (mPIV) and the schlieren technique. When non-dimensionalizing the system, we find a universal Sh Ra1=4 scaling relation for all alcohols (of different solubilities) and all droplets in the convective regime. Here Sh is the Sherwood number (dimensionless mass flux) and Ra is the Rayleigh number (dimensionless density difference between clean and alcohol-saturated water). This scaling implies the scaling relation c / R5=4 0 of the convective dissolution time c, which is found to agree with experimental data. We show that in the convective regime the plume Reynolds number (the dimensionless velocity) of the detaching alcohol-saturated plume follows Rep Sc
AB - The dissolution process of small (initial (equivalent) radius R0 < 1 mm) long-chain alcohol (of various types) sessile droplets in water is studied, disentangling diffusive and convective contributions. The latter can arise for high solubilities of the alcohol, as the density of the alcohol–water mixture is then considerably less than that of pure water, giving rise to buoyancy-driven convection. The convective flow around the droplets is measured, using micro-particle image velocimetry (mPIV) and the schlieren technique. When non-dimensionalizing the system, we find a universal Sh Ra1=4 scaling relation for all alcohols (of different solubilities) and all droplets in the convective regime. Here Sh is the Sherwood number (dimensionless mass flux) and Ra is the Rayleigh number (dimensionless density difference between clean and alcohol-saturated water). This scaling implies the scaling relation c / R5=4 0 of the convective dissolution time c, which is found to agree with experimental data. We show that in the convective regime the plume Reynolds number (the dimensionless velocity) of the detaching alcohol-saturated plume follows Rep Sc
KW - 2023 OA procedure
U2 - 10.1017/jfm.2016.158
DO - 10.1017/jfm.2016.158
M3 - Article
SN - 0022-1120
VL - 794
SP - 45
EP - 67
JO - Journal of fluid mechanics
JF - Journal of fluid mechanics
ER -