Band instability in near-critical fluids subjected to vibration under weightlessness
Author(s) -
T. Lyubimova,
Andrey Ivantsov,
Yves Garrabos,
Carole Lecoutre,
G. Gandikota,
D. Beysens
Publication year - 2017
Publication title -
physical review. e
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.896
H-Index - 304
eISSN - 2470-0053
pISSN - 2470-0045
DOI - 10.1103/physreve.95.013105
Subject(s) - instability , dimensionless quantity , wavelength , physics , viscosity , surface tension , levitation , zero gravity , wavenumber , mechanics , weightlessness , critical point (mathematics) , critical frequency , magnetic levitation , vibration , condensed matter physics , thermodynamics , optics , magnet , quantum mechanics , mathematical analysis , ionosphere , mathematics , astronomy
International audiencePeriodical patterns (bands) developing at the interface of two immiscible fluids under vibration parallel to interface are observed under zero-gravity conditions. Fluids are slightly below their liquid-vapor critical point where they behave in a scaled, universal manner. In addition, liquid and vapor densities are close and surface tension is very low. Linear stability analyses and direct numerical simulation show that this instability, although comparable to the frozen wave instability observed in a gravity field, is nonetheless noticeably different when gravity becomes zero. In particular, the neutral curve minimum corresponds to the long-wave perturbations with k=0 and zero dimensionless vibrational parameter, corresponding to no instability threshold. The pattern wavelength thus corresponds to the wavelength of the perturbations with maximal growth rate. This wavelength differs substantially from the neutral perturbations wavelength at the same vibrational parameter value. The role of viscosity is highlighted in the pattern formation, with a critical wavelength dependence on vibration parameters that strongly depends on viscosity. These results compare well with experimental observations performed in the liquid-vapor phases near the critical point of CO2 (in weightlessness) and H2 (under magnetic levitation)
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