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Oscillatory dou biffusive natural convection in low prandtl number fluid

机译:低普朗特数液中的振动性斗斗自然对流

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The numerical simulations of double-diffusive natural convection were carried out at the Prandtl number Pr=0.01 and the Lewis number Le=100 for two models. One is a two-layer system which consists of a pure liquid (upper layer) and a solution (lower layer) by lateral heating and cooling at an aspect ratio A=4 and a buoyancy ratio N=10. The double-diffusive natural convection was monotonous at the Rayleigh number Ra=10~4 but the double-oscillatory characteristic was found at Ra=10~5. The short periodic oscillation corresponded to the oscillatory flow and the long periodic oscillation corresponded to the migration (collision and rebound) of roll cells. The other model is the case of opposing buoyancy forces near the vertical walls at Ra=10~4. At A=1 the thermal convection was formed at N=1 and 2; the thermal and solutal convections coexisted at N=3; the solutal convection became dominant with the formation of concentration stratified layer at N=5. However the flow at A=2 was oscillatory for N=1 to 10 and the intensity of oscillation became weak at N >= 3. The intensity of flow oscillation at A=2 was generally stronger than that at A=1.
机译:双扩散自然对流的数值模拟在Prandtl号码Pr = 0.01和两个模型的Lewis Number Le = 100处进行。一种是双层系统,其由纯液体(上层)和溶液(下层)组成,通过横向加热和冷却,纵横比a = 4和浮力比n = 10。双扩散天然对流在瑞利率Ra = 10〜4时单调,但在RA = 10〜5时发现双振荡特性。短周期振荡对应于振荡流动和长周期振荡对应于辊子细胞的迁移(碰撞和反弹)。另一种模型是在RA = 10〜4的垂直壁附近相对的浮力力的情况。在a = 1处,在n = 1和2处形成热对流;在n = 3时的热和索径对流共存;随着在n = 5的形成中形成浓度分层层而显着。然而,A = 2的流动是n = 1至10的振荡,并且振荡强度在n> = 3处变弱。a = 2的流动振荡强度通常比a = 1更强。

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