自然对流的微观尺度

V. Arpaci
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引用次数: 0

摘要

一个通用的无量纲数ΠN ~ NN1+Pr-1,Pr是通常的普朗特数,NN是Pr→∞的极限ΠN,被引入到所有自然对流过程中。对于NN=Ra,Ra为通常的瑞利数,ΠN描述浮力驱动的自然对流。对于NN=Ma,Ma是通常的Marangoni数,ΠN描述了热毛细管驱动的自然对流。对于NN=TaPr,Ta为通常的泰勒数,ΠN描述离心驱动的自然对流。根据ΠN,相对于积分尺度的热Kolmogorov尺度,ηθ r ~ ΠN-1/3引入了自然对流,包括浮力、热毛细和离心驱动的流动。与这些流动相关的传热用Nu ~ ΠN1/3来模拟,Nu是通常的努塞尔数。与该模型相关的各种湍流自然对流现象也被展示出来。
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Microscales of Natural Convection
A universal dimensionless number, ΠN∼NN1+Pr-1 ,Pr being the usual Prandtl number and NN the limit of ΠN for Pr → ∞, is introduced for all natural convection processes. For NN=Ra ,Ra being the usual Rayleigh number, ΠN describes buoyancy-driven natural convection. For NN=Ma ,Ma being the usual Marangoni number, ΠN describes thermocapillary-driven natural convection. For NN=TaPr ,Ta being the usual Taylor number, ΠN describes centrifugally-driven natural convection. In terms of ΠN, a thermal Kolmogorov scale relative to an integral scale, ηθℓ∼ΠN-1/3 is introduced for natural convection including buoyancy, thermocapillary and centrifugally-driven flows. Heat transfer associated with these flows is modeled byNu∼ΠN1/3 ,Nu being the usual Nusselt number. A variety of turbulent natural convection phenomena are shown correlating the model.
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