2001
DOI: 10.1016/s0017-9310(00)00188-5
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Transitions of natural convection in a horizontal annulus

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Cited by 58 publications
(48 citation statements)
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“…He observed dual steady solutions at Ra > Ra c ≈ 3800 for wide gap annuli (R = 2) by the vorticity-streamfunction method. Similar results were provided later by Mizushima et al, 20,21 xin et al 22 and Mercader et al 23 Petrone et al 24 performed a stability analysis of numerical steady-state solutions, and provided a detail of the bifurcation diagram near the imperfect bifurcation for different radius ratio R = 1.2, 1.4 and 2 at Pr = 0.7. Angeli et al 25 provided a critical review of buoyancy-induced flow transitions in horizontal annuli.…”
Section: Introductionsupporting
confidence: 68%
“…He observed dual steady solutions at Ra > Ra c ≈ 3800 for wide gap annuli (R = 2) by the vorticity-streamfunction method. Similar results were provided later by Mizushima et al, 20,21 xin et al 22 and Mercader et al 23 Petrone et al 24 performed a stability analysis of numerical steady-state solutions, and provided a detail of the bifurcation diagram near the imperfect bifurcation for different radius ratio R = 1.2, 1.4 and 2 at Pr = 0.7. Angeli et al 25 provided a critical review of buoyancy-induced flow transitions in horizontal annuli.…”
Section: Introductionsupporting
confidence: 68%
“…In the light of the previous observations, what should be expected for large A is a consistent convective flow, with a fairly articulated streamline structure, as noticed in [9][10][11][12], associated with a consistent average Nusselt number, strongly depending on A, as noticed in [6]. All these properties occur even for very small Rayleigh numbers, so small that one would observe the fluid almost at rest if A were also small.…”
supporting
confidence: 59%
“…In (14), and can be either scalar-, vector-or tensor-valued functions and the dot between and denotes multiplication for scalar functions or the corresponding scalar product in case of vectors or tensors, respectively. Next, the norm of the difference between the gradients of solutions to problems (3)(4)(5) and (10)(11)(12), namely, the quantity ∇(v − w) 2 + ∇(τ − τ 0 ) 2 , is taken as a measure of the absolute error. Finally, an upper bound for the absolute error is found; such a bound essentially depends on Pr −1 (Ra/b) 2 .…”
Section: Mathematical Modelmentioning
confidence: 99%
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“…[10] studied natural convection flow in a horizontal annulus enclosure with a transversely oscillating inner cylinder. [11] investigated transition of natural convection in an annulus between horizontal concentric cylinders theoretically by assuming two-dimensional and incompressible flow fields.…”
mentioning
confidence: 99%