2007
DOI: 10.1103/physreve.75.026210
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Hexagons and spiral defect chaos in non-Boussinesq convection at low Prandtl numbers

Abstract: We study the stability and dynamics of non-Boussinesq convection in pure gases ͑CO 2 and SF 6 ͒ with Prandtl numbers near PrӍ 1 and in a H 2 -Xe mixture with Pr= 0.17. Focusing on the strongly nonlinear regime we employ Galerkin stability analyses and direct numerical simulations of the Navier-Stokes equations. For Pr Ӎ 1 and intermediate non-Boussinesq effects we find reentrance of stable hexagons as the Rayleigh number is increased. For stronger non-Boussinesq effects the usual, transverse side-band instabil… Show more

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Cited by 13 publications
(14 citation statements)
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“…Similar results exist for other spatially periodic patterns such as hexagons, see e.g. [33]. We have seen that in the present problem the coefficients a 1 , a 2 may render the Eckhaus-stable region highly asymmetrical with respect to k → −k and may reduce dramatically its extent, perhaps eliminating it altogether (see e.g.…”
Section: Discussionsupporting
confidence: 83%
“…Similar results exist for other spatially periodic patterns such as hexagons, see e.g. [33]. We have seen that in the present problem the coefficients a 1 , a 2 may render the Eckhaus-stable region highly asymmetrical with respect to k → −k and may reduce dramatically its extent, perhaps eliminating it altogether (see e.g.…”
Section: Discussionsupporting
confidence: 83%
“…For small Prandtl numbers the signature of the long filaments and of the target patterns disappears and instead a much broader spectrum of smaller, more compact components arises. In a separate investigation 45 we find that the number of small compact components strongly increases when the fluid properties depend significantly on the temperature, i.e., when non-Boussinesq effects become important. They introduce a resonant triad interaction between the stripe modes that enhances the tendency towards hexagonal ͑cellular͒ patterns.…”
Section: Discussionmentioning
confidence: 99%
“…The dependence of NOB effects, especially in numerical simulations, is usually characterized by the coefficients (Madruga et al 2006;Madruga & Riecke 2007a) is equal to 0.015, 0.040, 0.010 and 0.009 for E-I, E-II, E-III and E-IV, respectively, for 6 3.0. The temperature difference T is increased in each experiment from onset at a constantT to reach values for which SDC is fully developed.…”
Section: Methodsmentioning
confidence: 99%