The cell size or the wave numbers of supercritical hexagonal convection cells in primarily surface tension driven convection on a uniformly heated plate was studied experimentally in thermal equilibrium in thin layers of silicone oil of large aspect ratio. It was found that the cell size decreases with increased temperature difference in the slightly supercritical range, and that the cell size is unique within the experimental error. It was also observed that the cell size reaches a minimum and begins to increase at larger temperature differences. This reversal of the rate of change of the wave number with temperature difference is attributed to influences of buoyancy on the fluid motion. The consequences of buoyancy were tested with three ...
International audienceWe study the nonlinear dynamics of hydrothermal waves produced by a surface-te...
The stability of a liquid layer with an undeformable interface open to the atmosphere, subjected to ...
Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/76679/1/AIAA-232-799.pd
Marangoni-Benard convection which is mainly driven by the thermocapillary (Marangoni) effect occurs ...
Under certain conditions, such as in thin liquid films or microgravity, surface tension variations a...
Surface-tension-driven convection in a planar fluid layer is studied by numerical simulation of the ...
High resolution laboratory experiments with large aspect ratio are being conducted for thin fluid la...
Marangoni-Benard convection in evaporating liquid thin layers has been investigated through flow vis...
International audienceWaves appear in a liquid layer with a free surface if a sufficiently high hori...
Numerical simulation studies are reported for the convection of a supercritical fluid, He-3, in a Ra...
Laboratory and numerical experiments are underway to generate, and subsequently suppress, oscillator...
Thermal and fingering convection in a horizontal porous layer underlying a fluid layer was studied u...
The convective instabilities in two or more superposed layers heated from below were studied extensi...
AbstractIn this paper, numerical results of convective instabilities in a horizontal liquid layer, w...
©2004 The American Physical Society. The research of J. Oh and G. Ahlers was supported by U.S. Natio...
International audienceWe study the nonlinear dynamics of hydrothermal waves produced by a surface-te...
The stability of a liquid layer with an undeformable interface open to the atmosphere, subjected to ...
Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/76679/1/AIAA-232-799.pd
Marangoni-Benard convection which is mainly driven by the thermocapillary (Marangoni) effect occurs ...
Under certain conditions, such as in thin liquid films or microgravity, surface tension variations a...
Surface-tension-driven convection in a planar fluid layer is studied by numerical simulation of the ...
High resolution laboratory experiments with large aspect ratio are being conducted for thin fluid la...
Marangoni-Benard convection in evaporating liquid thin layers has been investigated through flow vis...
International audienceWaves appear in a liquid layer with a free surface if a sufficiently high hori...
Numerical simulation studies are reported for the convection of a supercritical fluid, He-3, in a Ra...
Laboratory and numerical experiments are underway to generate, and subsequently suppress, oscillator...
Thermal and fingering convection in a horizontal porous layer underlying a fluid layer was studied u...
The convective instabilities in two or more superposed layers heated from below were studied extensi...
AbstractIn this paper, numerical results of convective instabilities in a horizontal liquid layer, w...
©2004 The American Physical Society. The research of J. Oh and G. Ahlers was supported by U.S. Natio...
International audienceWe study the nonlinear dynamics of hydrothermal waves produced by a surface-te...
The stability of a liquid layer with an undeformable interface open to the atmosphere, subjected to ...
Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/76679/1/AIAA-232-799.pd