Fundamental characteristics of secondary drops produced by early splash during single-drop impingement onto a thick liquid film

Author(s):  
Tomio Okawa ◽  
Katsuyuki Kawai ◽  
Kohei Kubo ◽  
Sota Kitabayashi
Keyword(s):  
2021 ◽  
Vol 121 ◽  
pp. 110279
Author(s):  
Tomio Okawa ◽  
Kohei Kubo ◽  
Katsuyuki Kawai ◽  
Sota Kitabayashi

2015 ◽  
Vol 92 (1) ◽  
Author(s):  
Nils Paul van Hinsberg ◽  
Marie Charbonneau-Grandmaison
Keyword(s):  

2004 ◽  
Vol 45 (9) ◽  
pp. 1009-1023 ◽  
Author(s):  
Heng Xie ◽  
Seiichi Koshizuka ◽  
Yoshiaki Oka

2016 ◽  
Vol 69 (6) ◽  
pp. 575-582 ◽  
Author(s):  
Gangtao Liang ◽  
Xingsen Mu ◽  
Yali Guo ◽  
Shengqiang Shen

1999 ◽  
Vol 385 ◽  
pp. 229-254 ◽  
Author(s):  
DANIEL A. WEISS ◽  
ALEXANDER L. YARIN

Single drop impact onto liquid films is simulated numerically. Surface tension and gravity are taken into account, whereas viscosity and compressibility are neglected. This permits recourse to a boundary-integral method, based on an integral equation for a scalar velocity potential. Calculations are performed for normal impacts resulting in axisymmetric flows.For times that are small compared to the characteristic time of impact 2R/w0 (R being the drop radius, w0 its initial velocity towards the liquid film), it is found that a disk-like jet forms at the neck between the drop and the pre-existing liquid film, if the impact Weber number is high enough. This jet can pinch off a torus-shaped liquid volume at its tip or reconnect with the pre-existing liquid film, thus entraining a torus- shaped bubble. In reality, both the torus-shaped bubble and liquid torus will decay according to Rayleigh's capillary instability, thus breaking the cylindrical symmetry. This mechanism of bubble entrainment differs from those described in literature.For times that are comparable to or larger than the characteristic time of impact, capillary waves on the film, or the well-known crowns, are obtained again according to whether the impact Weber number is low or high enough.


2002 ◽  
Vol 472 ◽  
pp. 373-397 ◽  
Author(s):  
I. V. ROISMAN ◽  
C. TROPEA

The impact of a drop onto a liquid film with a relatively high impact velocity, leading to the formation of a crown-like ejection, is studied theoretically. The motion of a kinematic discontinuity in the liquid film on the wall due to the drop impact, the formation of the upward jet at this kinematic discontinuity and its elevation are analysed. Four main regions of the drop and film are considered: the perturbed liquid film on the wall inside the crown, the unperturbed liquid film on the wall outside the crown, the upward jet forming a crown, and the free rim bounding this jet. The theory of Yarin & Weiss (1995) for the propagation of the kinematic discontinuity is generalized here for the case of arbitrary velocity vectors in the inner and outer liquid films on the wall. Next, the mass, momentum balance and Bernoulli equations at the base of the crown are considered in order to obtain the velocity and the thickness of the jet on the wall. Furthermore, the dynamic equations of motion of the crown are developed in the Lagrangian form. An analytical solution for the crown shape is obtained in the asymptotic case of such high impact velocities that the surface tension and the viscosity effects can be neglected in comparison to inertial effects. The edge of the crown is described by the motion of a rim, formed due to the surface tension.Three different cases of impact are considered: normal axisymmetric impact of a single drop, oblique impact of a single drop, and impact and interaction of two drops. The theoretical predictions of the height of the crown in the axisymmetric case are compared with experiments. The agreement is quite good in spite of the fact that no adjustable parameters are used.


2021 ◽  
Vol 127 (8) ◽  
Author(s):  
M. Y. Lanzerotti ◽  
K. Brakke ◽  
K. Allen ◽  
W. Blackmon ◽  
J. Hartke ◽  
...  

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