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Oscillatory dou biffusive natural convection in low prandtl number fluid

机译:低普朗特数流体的振荡双扩散自然对流

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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:对两个模型在Prandtl数Pr = 0.01和Lewis数Le = 100时进行了双扩散自然对流的数值模拟。一种是由纯液体(上层)和溶液(下层)通过纵横加热和冷却以纵横比A = 4和浮力比N = 10组成的两层系统。在瑞利数Ra = 10〜4时,双扩散自然对流是单调的,但在Ra = 10〜5时发现了双振荡的特性。短周期振荡对应于振荡流,长周期振荡对应于滚动单元的迁移(碰撞和回弹)。另一种模型是在Ra = 10〜4处垂直壁附近有相反的浮力的情况。在A = 1时,在N = 1和2时形成热对流;在A = 1时,热对流形成。在N = 3时,热对流和溶液对流同时存在。随着N = 5浓度分层层的形成,溶液对流占主导地位。但是,对于N = 1到10,在A = 2处的流动是振荡的,并且在N> = 3时,振荡的强度变弱。通常,在A = 2处的流动的振荡强度要强于在A = 1时的流动。

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