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Onset of secondary flow and enhancement of heat transfer in horizontal convergent and divergent channels heated from below

机译:从下方加热的水平会聚和发散通道中二次流的产生和传热的增强

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Experiments for the onset and development of the buoyancy driven secondary air flow and enhancement of heat transfer in a horizontal convergent and a divergent channel have been carried out. The bottom wall of the channel is horizontal and heated uniformly, while the top wall is insulated and inclined with respect to the horizontal plane so as to create a convergence angle of 3° for the convergent channel, or a divergence angle of 3° for the divergent channel. The aspect ratio (width to height) and the ratio of channel length to height at the entrance of the channel is 6.67 and 15, respectively. The Reynolds number ranges from 200 to 2000, the buoyancy parameter, GrIRe{sup}2, from 2.5 to 907 and Pr of the air flow is 0.7. Flow structure inside the channel is visualized by injecting smoke at the inlet flowing along the bottom wall. The onset of secondary flow appearing as transverse instability wave and onset of initial protrusion of the bottom heated layer are identified. Secondary flow structures observed are somewhat different from the case in the parallel-plate channel. This is attributed to the destabilization effect of the deceleration in the divergent channel which results in a much earlier initiation of secondary flow and more pronounced enhancement in the heat transfer, and the stabilization effect of the acceleration in the convergent channel which results in a much later initiation of the secondary flow and less pronounced enhancement in the heat transfer. However, the deceleration flow in the divergent channel and the acceleration in the convergent make the average Nusselt numbers approach the results of the parallel-plate channel. Correlation results for the onset of the secondary flow and enhancement of the heat transfer will be presented and discussed.
机译:已经进行了用于浮力驱动的二次气流的发生和发展以及在水平会聚和发散通道中增强传热的实验。通道的底壁是水平的并且被均匀地加热,而顶壁是隔热的并且相对于水平面倾斜,从而对于会聚的通道产生3°的会聚角,或者对于会聚的通道产生3°的发散角。分歧渠道。通道入口的纵横比(宽度与高度)和通道长度与高度之比分别为6.67和15。雷诺数范围为200至2000,浮力参数GrIRe {sup} 2为2.5至907,气流的Pr为0.7。通过在沿底壁流动的进口处注入烟气,可以看到通道内部的流动结构。确定了以横向不稳定性波出现的二次流的开始以及底部加热层的初始突出的开始。观察到的二次流结构与平行板通道中的情况有些不同。这归因于发散通道中的减速的去稳定作用,这导致更早地开始次级流动和传热的更明显的增强,以及会聚通道中的加速的稳定作用,这导致了更晚的发散。二次流的开始和传热的增强不明显。但是,发散通道中的减速流和收敛中的加速度使平均Nusselt数接近平行板通道的结果。将介绍和讨论二次流的开始和传热增强的相关结果。

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