Frozen wave induced by high frequency horizontal vibrations on a [Formula Presented] liquid-gas interface near the critical point

Physical Review E - Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics

Volumn 59, Issue 5, 1999, Pages 5440-5445

  Wunenburger, R ^a   Evesque, P ^a   Chabot, C ^a   Garrabos, Y ^a   Fauve, S ^b   Beysens, D ^c  

^a CNRS   (France)

^b ECOLE NORMALE SUPÉRIEURE   (France)

^c CEA GRENOBLE   (France)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0000709460     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.59.5440     Document Type: Article

References (13)

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7. The cylindrical geometry of the sample cells is different from the two-dimensional rectangular cell of the model of Ref. 4 (see Fig. 11). When the axes of the cells are parallel to gravity (case I in Fig. 22), all the interfaces have a circular shape of diameter D [see Fig. 33(b)] and the thickness of each fluid layer depends on the volume fraction x. Practically, we can assume that (Formula presented) When the axes of the cells are perpendicular to gravity (case II in Fig. 22), the interfaces have a rectangular shape whose dimension along the vibration direction depends on x (from 0 mm to D). In this case the fluid layer thickness depends on x and is not constant along the vibration direction [see Fig. 33(a)]. Practically, we can still assume that (Formula presented)
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