IMPACT OF DROPS ON SOLID-SURFACES - SELF-SIMILAR CAPILLARY WAVES, ANDSPLASHING AS A NEW-TYPE OF KINEMATIC DISCONTINUITY

Authors
Citation
Al. Yarin et Da. Weiss, IMPACT OF DROPS ON SOLID-SURFACES - SELF-SIMILAR CAPILLARY WAVES, ANDSPLASHING AS A NEW-TYPE OF KINEMATIC DISCONTINUITY, Journal of Fluid Mechanics, 283, 1995, pp. 141-173
Citations number
49
Categorie Soggetti
Mechanics,"Phsycs, Fluid & Plasmas
Journal title
ISSN journal
00221120
Volume
283
Year of publication
1995
Pages
141 - 173
Database
ISI
SICI code
0022-1120(1995)283:<141:IODOS->2.0.ZU;2-F
Abstract
The impact of drops impinging one by one on a solid surface is studied experimentally and theoretically. The impact process is observed by m eans of a charge-coupled-device camera, its pictures processed by comp uter. Low-velocity impact results in spreading and in propagation of c apillary waves, whereas at higher velocities splashing (i.e. the emerg ence of a cloud of small secondary droplets, absent in the former case ) sets in. Capillary waves are studied in some detail in separate expe riments. The dynamics of the extension of liquid lamellae produced by an impact in the case of splashing is recorded. The secondary-droplet size distributions and the total volume of these droplets are measured , and the splashing threshold is found as a function of the impact par ameters. The pattern of the capillary waves is predicted to be self-si milar. The calculated wave profile agrees well with the experimental d ata. It is shown theoretically that the splashing threshold correspond s to the onset of a velocity discontinuity propagating over the liquid layer on the wall. This discontinuity shows several aspects of a shoc k. In an incompressible liquid such a discontinuity can only exist in the presence of a sink at its front. The latter results in the emergen ce of a circular crown-like sheet virtually normal to the wall and pro pagating with the discontinuity. It is predicted theoretically and rec orded in the experiment. The crown is unstable owing to the formation of cusps at the free rim at its top edge, which results in the splashi ng effect. The onset velocity of splashing and the rate of propagation of the kinematic discontinuity are calculated and the theoretical res ults agree fairly well with the experimental data. The structure of th e discontinuity is shown to match the outer solution.