scholarly journals Drop impact entrapment of bubble rings

2013 ◽  
Vol 724 ◽  
pp. 234-258 ◽  
Author(s):  
M.-J. Thoraval ◽  
K. Takehara ◽  
T. G. Etoh ◽  
S. T. Thoroddsen

AbstractWe use ultra-high-speed video imaging to look at the initial contact of a drop impacting on a liquid layer. We observe experimentally the vortex street and the bubble-ring entrapments predicted numerically, for high impact velocities, by Thoraval et al. (Phys. Rev. Lett., vol. 108, 2012, article 264506). These dynamics mainly occur within $50~\mathrm{\mu} \mathrm{s} $ after the first contact, requiring imaging at 1 million f.p.s. For a water drop impacting on a thin layer of water, the entrapment of isolated bubbles starts through azimuthal instability, which forms at low impact velocities, in the neck connecting the drop and pool. For Reynolds number $Re$ above ${\sim }12\hspace{0.167em} 000$, up to 10 partial bubble rings have been observed at the base of the ejecta, starting when the contact is ${\sim }20\hspace{0.167em} \% $ of the drop size. More regular bubble rings are observed for a pool of ethanol or methanol. The video imaging shows rotation around some of these air cylinders, which can temporarily delay their breakup into micro-bubbles. The different refractive index in the pool liquid reveals the destabilization of the vortices and the formation of streamwise vortices and intricate vortex tangles. Fine-scale axisymmetry is thereby destroyed. We show also that the shape of the drop has a strong influence on these dynamics.

2015 ◽  
Vol 785 ◽  
Author(s):  
E. Q. Li ◽  
I. U. Vakarelski ◽  
S. T. Thoroddsen

When a drop impacts onto a solid surface, the lubrication pressure in the air deforms its bottom into a dimple. This makes the initial contact with the substrate occur not at a point but along a ring, thereby entrapping a central disc of air. We use ultra-high-speed imaging, with 200 ns time resolution, to observe the structure of this first contact between the liquid and a smooth solid surface. For a water drop impacting onto regular glass we observe a ring of microbubbles, due to multiple initial contacts just before the formation of the fully wetted outer section. These contacts are spaced by a few microns and quickly grow in size until they meet, thereby leaving behind a ring of microbubbles marking the original air-disc diameter. On the other hand, no microbubbles are left behind when the drop impacts onto molecularly smooth mica sheets. We thereby conclude that the localized contacts are due to nanometric roughness of the glass surface, and the presence of the microbubbles can therefore distinguish between glass with 10 nm roughness and perfectly smooth glass. We contrast this entrapment topology with the initial contact of a drop impacting onto a film of extremely viscous immiscible liquid, where the initial contact appears to be continuous along the ring. Here, an azimuthal instability occurs during the rapid contraction at the triple line, also leaving behind microbubbles. For low impact velocities the nature of the initial contact changes to one initiated by ruptures of a thin lubricating air film.


2020 ◽  
Vol 13 (3) ◽  
Author(s):  
Arash Sayyah ◽  
Mohammad Mirzadeh ◽  
Yi Jiang ◽  
Warren V. Gleason ◽  
William C. Rice ◽  
...  

2009 ◽  
Vol 32 (2) ◽  
pp. 101631 ◽  
Author(s):  
L. D. Suits ◽  
T. C. Sheahan ◽  
L. N. Y. Wong ◽  
H. H. Einstein

Soft Matter ◽  
2021 ◽  
Author(s):  
Payman Jalali ◽  
Yuchen Zhao ◽  
Joshua E. S. Socolar

A spherical intruder embedded in a confined granular column is extracted by pulling it upward by an attached string. At a certain pulling force (measured), the failure of granular column occurs characterized by high-speed video imaging.


Langmuir ◽  
2010 ◽  
Vol 26 (11) ◽  
pp. 7865-7874 ◽  
Author(s):  
Seher Ata ◽  
Elizabeth S. Davis ◽  
Damien Dupin ◽  
Steven P. Armes ◽  
Erica J. Wanless

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