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Natural Convection in a Rectangular Enclosure with Colliding Boundary Layers

机译:具有碰撞边界层的矩形外壳中的自然对流

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The movement ofthe fluid in natural convection results from the buoyancy forces imposed on thefluid when its density in the proximity of the heat transfer surface isdecreased as a result of the heating process. The objective of this paper isthe computational study of the flow initiated by natural convection. Theproblem being investigated is the colliding boundary layer in a rectangularenclosure. The dimensional governing equations are first transformed tonon-dimensional equations. The purpose of this transformation is to reduce theeffort required to make a study over a range of variables. A non-dimensionalscheme was chosen which led to improved iterative convergence for faster transients.The three dimensional analogue of the stream function-vorticity formulation wasused where the scalar vorticity was replaced by a vector and the scalar streamfunction by a vector potential. The equations were then solved using the methodof variable false transients. The results indicated that the flow region isstratified into three regions; a cold upper region, a hot region in the area ofthe confluence of hot and cold streams and a warm lower region.
机译:流体在自然对流中的运动是由于加热过程导致流体在传热表面附近的密度降低时,施加在流体上的浮力引起的。本文的目的是对自然对流引发的流动进行计算研究。研究的问题是矩形外壳中的碰撞边界层。首先将尺寸控制方程式转换为非尺寸方程式。这种转换的目的是减少对一系列变量进行研究所需的精力。选择了一个无量纲的方案,以提高迭代收敛性,从而实现更快的瞬变。使用了流函数涡度公式的三维类似物,其中标量涡度被矢量取代,标量流函数被矢量势取代。然后使用可变假瞬态方法求解方程。结果表明,流动区域分为三个区域。较冷的上部区域,冷热气流汇合区域中的较热区域和较热的下部区域。

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