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Direct numerical simulation of turbulent flow and heat transfer over a heated cube placed in a matrix of unheated cubes

机译:在加热立方体矩阵中的加热立方体中湍流和热传递的直接数值模拟

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Direct numerical simulation (DNS) of turbulent flow and heat transfer has been performed over a heated wall-mounted cube positioned in a non-heated cube matrix by applying periodic boundary conditions in both streamwise (X) and spanwise (Y) directions. Three different channel heights namely, 3.4H, 2.0H, 1.5H corresponding to blockage ratio (BR) of 0.0735, 0.125 and 0.167 with H as the size of the cube are employed. The Reynolds number defined for the present simulation is kept at 3,854 (based on the cube height and average streamwise velocity) while the Prandtl number is chosen to be 0.712. A second-order spatial and temporal discretization has been used to solve the Navier-Stokes and energy equations. The flow structures and the associated heat transfer have been compared and discussed at different BRs based on the results of instantaneous snapshots and statistical quantities of flow variables. The turbulent states for each BR has been compared using an anisotropic invariant map in the horseshoe vortex regime, top surface regime and in the wake regime. The total heat flux and turbulent heat flux quantities are compared near the cube's surface to determine the contribution of both heat transfer by the thermal gradients, and due to the fluctuation induced heat flux. The overall Nusselt number is found to increase significantly with an increase in BR from 0.0735 to 0.125. However, at BR- 0.167. no considerable augmentation in heat transfer has been observed as compared to BR = 0.125. On the other hand, the friction factor increases monotonically but significantly with BR.
机译:通过在流动(x)和跨越跨越(y)方向上施加周期性边界条件,在位于非加热立方体矩阵中定位的加热壁挂式立方体上进行了湍流和传热的直接数值模拟(DNS)。三种不同的通道高度即3.4h,2.0h​​,1.5h,对应于Hy为0.0735,0.125和0.167的封闭率(Br),因为采用H尺寸。为本模拟定义的雷诺数保持在3,854(基于立方体高度和平均流速),而PRANDTL编号选择为0.712。二阶空间和时间离散化已被用于解决Navier-Stokes和能量方程。已经基于瞬时快照和统计量的流量变量的结果比较了流动结构和相关的传热在不同的BRS中讨论并讨论。使用马蹄涡流制度,顶部表面制度和唤醒制度的各向异性不变地图进行了对每个BR的动荡状态。在立方体表面附近比较总热通量和湍流热量量,以确定热梯度的热传递的贡献,并且由于波动引起的热通量。发现整个营养数量显着增加,增加了0.0735至0.125的BR。但是,在BR-0.167。与BR = 0.125相比,没有观察到热传递中的相当大的增强。另一方面,摩擦因子单调而显着增加。

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