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Volumn 53, Issue 6 SUPPL. A, 1996, Pages 5982-5992

Nonlinear analysis of the coupling between interface deflection and hexagonal patterns in Rayleigh-Bénard-Marangoni convection

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EID: 0000832960     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/physreve.53.5982     Document Type: Article
Times cited : (9)

References (19)
  • 4
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    • M. J. Block, Nature 178, 650 (1956).
    • (1956) Nature , vol.178 , pp. 650
    • Block, M.J.1
  • 12
    • 0642275225 scopus 로고
    • L. Hadji, J. Safar, and M. Schell, J. Non-Equilib. Thermodyn. 16, 343 (1991). The derivation of an expression for the heat transfer coefficient β′ that appears in Eq. (2.21) is described in the Appendix. The derivation makes use of the experimental fact that the air layer is bounded from above by a plate. Note the following correction: H should be the plate's thickness, and D the depth of the air layer.
    • (1991) J. Non-Equilib. Thermodyn. , vol.16 , pp. 343
    • Hadji, L.1    Safar, J.2    Schell, M.3
  • 17
    • 0025446297 scopus 로고
    • The physical properties of Silicone Oil are displayed in Table I on p. 573
    • E. L. Koschmeider and S. A. Prahl, J. Fluid Mech. 215, 571 (1990). The physical properties of Silicone Oil are displayed in Table I on p. 573.
    • (1990) J. Fluid Mech. , vol.215 , pp. 571
    • Koschmeider, E.L.1    Prahl, S.A.2
  • 18
    • 5344258742 scopus 로고    scopus 로고
    • M. Assenheimer and V. Steinberg [Phys. Rev. Lett. 76, 736 (1996)] describe a method for varying the Prandtl number in a Rayleigh-Bénard convection experiment without changing the working fluid. These authors report observing domains of down-hexagons coexisting with domains of up-flow hexagons. The present analysis predicts boundaries in the parameter space of RBM convection that separate up-flow hexagons from down-hexagons. The possibility of coexistence is theoretically ruled out. From an experimental point of view, however, coexistence is plausible. For instance, for the experimental situation that is described by Eq. (3.32a), up-flow hexagons are predicted to occur for ĜĈP̂<1 and down-hexagons for ĜĈP̂>1. During the testing of this case, spatial nonuniformities in the physical parameters may divide the fluid cell into regions consisting of up-flow hexagons (ĜĈP̂>1) coexisting with regions of down-hexagons (ĜĈP̂<1).
    • (1996) Phys. Rev. Lett. , vol.76 , pp. 736
    • Assenheimer, M.1    Steinberg, V.2
  • 19
    • 5344275089 scopus 로고
    • The experimental setup that is appropriate to our present analysis is that of a fluid layer overlying a layer of air, and bounded below by a plate whose thermal conductance is low compared to that of the fluid. In this case the critical wave number is small but not zero. The resulting convection flow is therefore not homogeneous but cellular. Consequently, the present analysis can be tested by making use of an experimental apparatus analogous to the one used by P. Le Gal, A. Pocheau, and V. Croquette [Phys. Rev. Lett. 54, 2501 (1985)].
    • (1985) Phys. Rev. Lett. , vol.54 , pp. 2501
    • Le Gal, P.1    Pocheau, A.2    Croquette, V.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.