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首页> 外文期刊>Experimental Thermal and Fluid Science: International Journal of Experimental Heat Transfer, Thermodynamics, and Fluid Mechanics >Effect of gap width on turbulent mixing of parallel flow in a square channel with a cylindrical rod
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Effect of gap width on turbulent mixing of parallel flow in a square channel with a cylindrical rod

机译:间隙宽度对带有圆柱杆的方形通道中平行流湍流混合的影响

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摘要

The turbulent mixing coefficient is an essential parameter to describe the energy and momentum transports between adjacent subchannels in a nuclear fuel assembly and affect the thermal-hydraulic characteristics in nuclear reactor core. Hence, its estimation is in close connection with the design and performance-prediction of nuclear reactor. In the present experimental study, the effect of gap width on the flow pulsation and turbulent mixing was investigated using PIV (Particle Image Velocimetry). The W/. D (the ratio of distance to wall to rod diameter) covered from 1.03 to 1.14, and the single cylindrical rods with five different diameters were installed in a square channel to adjust the gap width. Among the W/. D cases tested, in the W/. D=1.03, 1.06, 1.08, and 1.10, the flow pulsation, a quasi-periodic oscillating flow motion, appeared at the rod gap center, while it was not observed for W/. D=1.14. As an increase in Reynolds number and/or a decrease in W/. D, the peak frequency and power spectral density of flow pulsation became higher and larger, respectively. On the other hand, the W/. D cases with a flow pulsation exhibited higher RMS (Root-Mean-Square) values of lateral velocity than the case without a flow pulsation. The change in the RMS values of lateral velocity was more sensitive to the W/. D conditions, particularly for the small W/. D cases (i.e., W/. D≤1.10) showing the flow pulsation. This implies that the RMS values of lateral velocity are strongly influenced by the flow pulsation, which in turn, can determine the turbulent mixing between subchannels. To propose the turbulent mixing coefficient for nuclear reactor core application, the W/. D ranges were divided into two groups dominated by (i) the large eddy motion of the flow pulsation, and (ii) the typical fluctuation of the turbulent flow. Finally, the empirical correlations of the turbulent mixing coefficient considering the effects of W/. D and the Reynolds number were proposed using the RMS value of lateral velocity, which were in agreement with previous studies within a reasonable degree of accuracy.
机译:湍流混合系数是描述核燃料组件中相邻子通道之间的能量和动量传输并影响核反应堆堆芯热工水力特性的重要参数。因此,其估算与核反应堆的设计和性能预测密切相关。在本实验研究中,使用PIV(颗粒图像测速)研究了间隙宽度对流动脉动和湍流混合的影响。 W /。 D(壁距与杆直径的比)从1.03到1.14,并且将具有五个不同直径的单个圆柱杆安装在方形通道中以调整间隙宽度。在W /。在W /中测试了D个案例。 D = 1.03、1.06、1.08和1.10,在杆间隙中心出现了流动脉动(准周期振荡流动运动),而未观察到W /。 D = 1.14。随着雷诺数的增加和/或W /的降低。 D,流动脉动的峰值频率和功率谱密度分别变得更高和更大。另一方面,W /。与没有流动脉动的情况相比,具有流动脉动的D情况显示出更高的横向速度RMS(均方根)值。横向速度RMS值的变化对W /更为敏感。 D条件,特别是对于小W /。显示流量脉动的D种情况(即W /。D≤1.10)。这暗示着横向速度的RMS值受到流动脉动的强烈影响,而流动脉动又可以确定子通道之间的湍流混合。提出用于核反应堆堆芯的湍流混合系数W /。 D范围分为两组,分别是(i)流动脉动的大涡流运动和(ii)湍流的典型波动。最后,考虑W /的影响,湍流混合系数的经验相关性。 D和雷诺数是使用横向速度的RMS值提出的,在合理的准确度范围内与先前的研究一致。

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