TY - JOUR
T1 - Dynamics of droplet-film collision
AU - Pan, K. L.
AU - Law, Chung King
N1 - Funding Information:
The work was supported by the Air Force Office of Scientific Research under the technical monitoring of Dr M. Birkan. We thank Professor S. H. Lam for stimulating discussions and Mr D. L. Zhu for his help with the experimentation.
PY - 2007/9/25
Y1 - 2007/9/25
N2 - The head-on collision of a droplet onto a liquid layer of the same material, backed bya solid surface, was experimentally and computationally investigated, with emphasis on the transition from bouncing of the droplet to its absorption by the film for given dropletWeber number, We, and the film thickness scaled by the droplet radius, Hf. Experimental results show that while absorption is favoured with increasing We, there exists a range around Hf ≈ 1 over which this tendency is moderated. This local moderation in turn corresponds to a regime, 11 ∼ We ∼ 14, over which increasing Hf from a small value leads to a triple reversalbehaviour of absorption, bouncing, absorption again, and bouncing again. The collision dynamics including evolution of the surface contours of the droplet and film, as well as the energy budgets, were then simulated by using a front-tracking technique. For collisionsleading to absorption and partial absorption, for which part of the absorbed droplet is subsequently ejected from the film, rupture and hence merging of the interfaces were manually imposed at an instant that leads to agreement between the subsequent calculated and experimental images. The simulation satisfactorily identified the different factors influencing the observed non-monotonic response of the collision event.
AB - The head-on collision of a droplet onto a liquid layer of the same material, backed bya solid surface, was experimentally and computationally investigated, with emphasis on the transition from bouncing of the droplet to its absorption by the film for given dropletWeber number, We, and the film thickness scaled by the droplet radius, Hf. Experimental results show that while absorption is favoured with increasing We, there exists a range around Hf ≈ 1 over which this tendency is moderated. This local moderation in turn corresponds to a regime, 11 ∼ We ∼ 14, over which increasing Hf from a small value leads to a triple reversalbehaviour of absorption, bouncing, absorption again, and bouncing again. The collision dynamics including evolution of the surface contours of the droplet and film, as well as the energy budgets, were then simulated by using a front-tracking technique. For collisionsleading to absorption and partial absorption, for which part of the absorbed droplet is subsequently ejected from the film, rupture and hence merging of the interfaces were manually imposed at an instant that leads to agreement between the subsequent calculated and experimental images. The simulation satisfactorily identified the different factors influencing the observed non-monotonic response of the collision event.
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U2 - 10.1017/S002211200700657X
DO - 10.1017/S002211200700657X
M3 - Article
AN - SCOPUS:37749023084
SN - 0022-1120
VL - 587
SP - 1
EP - 22
JO - Journal of Fluid Mechanics
JF - Journal of Fluid Mechanics
ER -