2001
DOI: 10.1070/pu2001v044n10abeh001012
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Natural convection in heat-generating fluids

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Cited by 17 publications
(13 citation statements)
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“…(1). For small Rayleigh numbers, typically Ra ( Ra c1 $ 10 3 , diffusive processes dominate and there is either no motion or very little motion in the system; 26,27 this corresponds to the left-hand region in both the regime diagram Fig. 1 and in Fig.…”
Section: Regime Diagrammentioning
confidence: 95%
“…(1). For small Rayleigh numbers, typically Ra ( Ra c1 $ 10 3 , diffusive processes dominate and there is either no motion or very little motion in the system; 26,27 this corresponds to the left-hand region in both the regime diagram Fig. 1 and in Fig.…”
Section: Regime Diagrammentioning
confidence: 95%
“…For Ra in the range 500 < Ra < 10 6 , Liu et al [3] conducted numerical simulations and identified the transition between stable and explosive behaviour; this explosion boundary is shown in Fig 2. When Ra > 10 6 , natural convection is vigorous and turbulent [19,20]; then the system approximates to the well-mixed (Semenov) case [1]. However, conduction of heat still plays a role in the thin thermal boundary layer adjacent to the reactor wall.…”
Section: Systems With Negligible Consumption Of Reactantmentioning
confidence: 99%
“…For Rayleigh numbers less than a critical value (≈ 10 3 for spheres) (Bol'shov et al 2001), diffusion will be the dominant mechanism for the transfer of heat and mass. When diffusion dominates transport, the temperature and concentration fields are approximately spherically symmetric, with the maximum temperature occurring close to the centre of the reactor.…”
Section: Transport Controlled By Diffusionmentioning
confidence: 99%