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NATURAL CONVECTION IN A RECTAGULAR ENCLOSURE WITH TWO HEATED SECTIONS ON THE LOWER SURFACE AND COOLED SIDE WALLS

机译:矩形外壳中的自然对流,下表面上有两个加热部分和冷却的侧壁

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The development of unsteady free convective flow in a rectangular enclosure has been numerically studied. The enclosure considered has rectangular horizontal lower and upper surfaces and vertical side surfaces. The horizontal width of enclosure is twice the vertical height of the enclosure while the longitudinal length of the enclosure is equal to the vertical height of the enclosure. There are two square, symmetrically placed isothermal heated sections on the lower surface, the rest of this surface being adiabatic. The vertical side-walls of the enclosure are kept at a uniform low temperature and the horizontal rectangular upper surface is adiabatic. The solution has been obtained by numerically solving the unsteady form of the governing equations. The unsteady, three-dimensional governing equations written in dimensionless form, have been solved using a iterative, semi-implicit finite-difference method. The solution was continued in dimensionless time until the time-averaged values of the flow variables ceased to change with time. The solution has the following parameters: the Rayleigh number, Ra, the Prandtl number, Pr, the dimensionless size, w_H, of the square heated sections and the dimensionless distance between the heated sections on the lower surface, w_S. Results have been obtained for a Prandtl number of 0.7. The conditions under which unsteady flow develops and the nature of the unsteady flow have been investigated and the variation of mean average Nusselt number with Rayleigh number and the effect of unsteadiness in the flow on this variation have been extensively explored.
机译:不稳定自由对流的矩形外壳中的发展已数值研究。考虑的外壳具有矩形水平下表面和上表面和垂直侧面上。外壳的水平宽度是所述外壳的所述垂直高度的两倍,而外壳的纵向长度等于所述外壳的所述垂直高度。有两种方,对称地放置的下表面等温加热区段上,该表面是绝热的其余部分。所述外壳的所述垂直侧壁被保持在均匀的低温和水平矩形上表面是绝热的。该解决方案已通过数值求解的控制方程的不稳定形式而获得。写在无量纲形式的非稳态,三维控制方程,已使用迭代的,半隐式有限差分法求解。该解决方案继续在无量纲时间,直到不再随时间变化的流量变量的时间平均值。该解决方案具有以下参数:该瑞利数中,Ra,普朗特数,PR,无量纲大小,W_H,广场加热部和所述下表面上的加热部分之间的无量纲的距离,w_S。结果已经获得了0.7的普朗特数。根据该非定常流开发的条件和非定常流的性质进行了研究并与瑞利数值平均Nusselt数和的不稳定在该变型中的流动的影响的变化已被广泛探索。

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