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Numerical simulation of heat transfer and separation Al_2O_3anofluid flow in concentric annular pipe

机译:同心圆管内传热与分离Al_2O_3 /纳米流的数值模拟

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Predictions are reported for turbulent three-dimensional heat transfer and flow separation of Al_2O_3anofluid in concentric annular cylinders with sudden expansion, in which the outer cylinder of a downstream section is heated at a uniform heat flux whereas the outer cylinder of the upstream section and the whole inner cylinder are adiabatic. The conservation equations are solved using the finite volume method. The numerical simulations are carried out by standard κ-ε turbulence model. Results presented in this paper are for a constant heat flux range of 4000 ≤ q ≤ 16,000 W/m~2, four nanoparticle volumes (Φ = 0.5%, 1%, 1.5%, and 2%), and three expansion ratios (ER = 1.25,1.67, and 2). The Reynolds number is in the range of 20,000 ≤ Re ≤ 50,000. Results reveal that the volume fraction of A1_2O_3 and Reynolds number significantly affect the surface heat transfer coefficient: an increase in surface heat transfer coefficient was noted when both volume fraction of Al_2O_3 and Reynolds number were increased for all cases. It is found that the peak of the heat transfer coefficient occurs after the sudden expansion moved far from the step height with the increase of sudden expansion dimensions due to separation flow in case of both pure water and nanofluid. The size of the recirculation zone increases as the Reynolds number and expansion ratio increase. Increasing the nanoparticle of Al_2O_3anofluid tends to enhance the heat transfer coefficient due to nanoparticle heat transport in the base fluid which raises the convection heat transfer.
机译:据报道,在同心圆环形圆柱中,Al_2O_3 /纳米流体的湍流三维传热和流动分离具有突然膨胀,其中下游部分的外圆柱以均匀的热通量加热,而上游部分的外圆柱和整个内筒都是绝热的。守恒方程采用有限体积法求解。数值模拟是通过标准κ-ε湍流模型进行的。本文给出的结果是在4000≤q≤16,000 W / m〜2的恒定热通量范围,四个纳米颗粒体积(Φ= 0.5%,1%,1.5%和2%)和三个膨胀率(ER = 1.25、1.67和2)。雷诺数在20,000≤Re≤50,000的范围内。结果表明,Al_2O_3的体积分数和雷诺数显着影响表面传热系数:当所有情况下,Al_2O_3的体积分数和雷诺数均增加时,表面传热系数增加。发现在纯水和纳米流体的情况下,由于分离流引起的突然膨胀尺寸的增加,突然膨胀从台阶高度移开之后,传热系数的峰值出现。随着雷诺数和膨胀比的增加,再循环区的大小增加。由于Al_2O_3 /纳米流体的纳米颗粒的增加,由于在基础流体中的纳米颗粒的热传递而导致对流热传递的增加,从而倾向于提高热传递系数。

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