|
|
|
|
LEADER |
01677 am a22002893u 4500 |
001 |
116239 |
042 |
|
|
|a dc
|
100 |
1 |
0 |
|a Harris, Daniel Martin
|e author
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Mathematics
|e contributor
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Mechanical Engineering
|e contributor
|
100 |
1 |
0 |
|a Harris, Daniel Martin
|e contributor
|
100 |
1 |
0 |
|a Pucci, Giuseppe
|e contributor
|
100 |
1 |
0 |
|a Prost, Victor
|e contributor
|
100 |
1 |
0 |
|a Quintela Casal, Julio
|e contributor
|
100 |
1 |
0 |
|a Bush, John W. M.
|e contributor
|
700 |
1 |
0 |
|a Pucci, Giuseppe
|e author
|
700 |
1 |
0 |
|a Prost, Victor
|e author
|
700 |
1 |
0 |
|a Quintela Casal, Julio
|e author
|
700 |
1 |
0 |
|a Bush, John W. M.
|e author
|
245 |
0 |
0 |
|a Merger of a bubble and a soap film
|
260 |
|
|
|b American Physical Society (APS),
|c 2018-06-12T13:57:47Z.
|
856 |
|
|
|z Get fulltext
|u http://hdl.handle.net/1721.1/116239
|
520 |
|
|
|a The coalescence of a drop into a fluid bath is a subject of continuing interest in fluid dynamics, owing to its dynamical complexity, its accessibility in the laboratory, and its aesthetic appeal. It has been known for some time that a drop gently placed on a static bath of the same fluid may initially combine only partially with the underlying bath, resulting in a daughter droplet of approximately half the diameter of the parent droplet. This process can then repeat, giving rise to the so-called "coalescence cascade" until the final droplet is small enough to be completely absorbed.
|
520 |
|
|
|a National Science Foundation (U.S.) (Grant CMMI-1333242)
|
520 |
|
|
|a MIT-France Program
|
655 |
7 |
|
|a Article
|
773 |
|
|
|t Physical Review Fluids
|