The generation of two-dimensional vortices by transverse oscillation of a soap film

1998 ◽  
Vol 10 (2) ◽  
pp. 390-399 ◽  
Author(s):  
V. O. Afenchenko ◽  
A. B. Ezersky ◽  
S. V. Kiyashko ◽  
M. I. Rabinovich ◽  
P. D. Weidman
Keyword(s):  
Soap Film ◽  
Transverse Oscillation ◽  
Two Dimensional

The Generation of Two-Dimensional Vortices by Transverse Oscillation of a Soap Film

1997 ◽  
Vol 9 (9) ◽  
pp. S2-S2 ◽  
Author(s):  
P. D. Weidman ◽  
V. O. Afenchenko ◽  
A. B. Ezersky ◽  
S. V. Kiyashko ◽  
M. I. Rabinovich
Keyword(s):  
Soap Film ◽  
Transverse Oscillation ◽  
Two Dimensional

Two-dimensional soap-film patterns

2017 ◽  
pp. 12-29
Author(s):  
David Lovett ◽  
John Tilley
Keyword(s):  
Soap Film ◽  
Two Dimensional

Influence of the transverse oscillation of the two-dimensional channel on the mass transfer through the wall

2018 ◽  
Vol 2018.54 (0) ◽  
pp. 103
Author(s):  
Takato WATANABE ◽  
Tatsuyoshi OCHIAI ◽  
Orie TAMURA ◽  
Masahide NAKAMURA
Keyword(s):  
Mass Transfer ◽  
Transverse Oscillation ◽  
Two Dimensional

scholarly journals The dynamics of a viscous soap film with soluble surfactant

2001 ◽  
Vol 442 ◽  
pp. 387-409 ◽  
Author(s):  
JEAN-MARC CHOMAZ
Keyword(s):  
Film Thickness ◽  
Elastic Wave ◽  
Surfactant Concentration ◽  
Stokes Equations ◽  
Film Surface ◽  
Soap Film ◽  
Fluid Viscosity ◽  
Two Dimensional ◽  
Leading Order ◽  
Soap Films

Nearly two decades ago, Couder (1981) and Gharib & Derango (1989) used soap films to perform classical hydrodynamics experiments on two-dimensional flows. Recently soap films have received renewed interest and experimental investigations published in the past few years call for a proper analysis of soap film dynamics. In the present paper, we derive the leading-order approximation for the dynamics of a flat soap film under the sole assumption that the typical length scale of the flow parallel to the film surface is large compared to the film thickness. The evolution equations governing the leading-order film thickness, two-dimensional velocities (locally averaged across the film thickness), average surfactant concentration in the interstitial liquid, and surface surfactant concentration are given and compared to similar results from the literature. Then we show that a sufficient condition for the film velocity distribution to comply with the Navier–Stokes equations is that the typical flow velocity be small compared to the Marangoni elastic wave velocity. In that case the thickness variations are slaved to the velocity field in a very specific way that seems consistent with recent experimental observations. When fluid velocities are of the order of the elastic wave speed, we show that the dynamics are generally very specific to a soap film except if the fluid viscosity and the surfactant solubility are neglected. In that case, the compressible Euler equations are recovered and the soap film behaves like a two-dimensional gas with an unusual ratio of specific heat capacities equal to unity.

Soap film flows: Statistics of two-dimensional turbulence

1999 ◽  
Vol 11 (8) ◽  
pp. 2167-2177 ◽  
Author(s):  
P. Vorobieff ◽  
M. Rivera ◽  
R. E. Ecke
Keyword(s):  
Soap Film ◽  
Two Dimensional ◽  
Film Flows
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