共查询到17条相似文献,搜索用时 187 毫秒
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棒束燃料元件子通道间流体存在搅混与横向二次流,流动及阻力特性相较矩形通道、圆管等简单通道更为复杂。核动力舰船、船舶、小型浮动核电站等会受到海浪影响,经常处于倾斜、摇摆、垂荡等瞬变运动下。目前的相关研究多集中在低压工况的研究领域,高温高压自然循环运动条件下的研究较少。本文采用实验研究方法,对自然循环系统摇摆条件下棒束通道内流动传热特性进行了研究,获得了过冷沸腾和饱和沸腾两种条件下摇摆角度和摇摆周期对棒束壁面温度变化和传热系数的影响,并获得了摇摆周期内棒束通道内的传热系数计算关系式。结果表明,饱和沸腾传热系数变化比过冷沸腾的剧烈;在本文实验工况范围内,棒表面传热系数波动幅值随着摇摆幅度的增大而增大;摇摆条件下棒束通道过冷沸腾和饱和沸腾工况时均传热系数基本不变。 相似文献
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由于海洋条件下反应堆处于非稳态工况,会产生倾斜、摇摆、起伏等运动,这些运动将会在棒束通道中引入额外的惯性力场,对棒束通道中的流场会有额外的影响,因此有必要对摇摆条件下的棒束通道进行研究。本文基于粒子图像测速(PIV)技术开展了摇摆条件下节径比为1.326的棒束通道内流场分布特性研究。对比了相同流量条件下稳态工况与瞬态工况下流场分布差异,分析了同一加速度时棒束通道内不同位置的流场分布特征。实验结果表明:摇摆运动对棒束通道中部的影响较小,对通道两侧的影响较大。通道两侧的速度场呈现周期性波动,波形为反相。在流量较低的情况下会出现倒流现象,但定位格架此时对上游并未造成横向速度影响。研究表明摇摆运动引起的流场变化与脉动流引起的流场变化有较大差异,其中脉动流造成的速度场变化是均匀脉动的,而摇摆引起的速度场是在通道两侧呈现反相波动。 相似文献
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应用非线性kε湍流模式,采用非正交曲线坐标系下求解三维NS方程的非交错网格有限体积方法,数值模拟了充分发展条件下,三角形排列无限棒束间通道内,不同的几何参数(P/D),雷诺数(Re)下的流动和传热问题。给出了不同参数下的速度和温度分布以及湍流二次流动,分析了几何参数、雷诺数及二次流对棒束内流动和传热特性的影响,得到了不同参数下通道的摩擦系数和Nuselt数,并与经验关系式作了比较 相似文献
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建立窄矩形通道在摇摆条件下湍流流动的物理数学模型,应用数值分析方法模拟窄矩形通道的三维非稳态流动的传热过程;考察摇摆条件下通道内流动阻力和换热性能及其随雷诺数Re、摇摆周期T及摇摆幅度max影响的变化规律。结果表明,摇摆状态下窄矩形通道内速度场呈周期性变化;时均摩擦系数favg和时均努塞尔数Nuavg比非摇摆工况下的结果大,Nuavg满足拟合公式0.851 0.4Nu 0.023Re Pr;在相同Re和摇摆周期T下,通道内流体摩擦压降和Nu的变化幅值随max的增大而增大,其变化周期等于T;在相同Re和max下,摩擦压降pf和Nu的变化幅值随T的增大而减小,其变化周期等于T。 相似文献
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The flow and heat transfer characteristic of turbulent flow in typical 4 and 7 rod bundles in ocean environment is investigated theoretically. In ocean environment, the periodic variation of secondary flow in 7 rod bundles is not obvious. Because of the velocity oscillation, there is a periodic heat accumulation on the tube wall. And the restriction of the channel wall on the rolling motion is considerable. In 7 rod bundles, because of the restriction of the channel wall, the effect of the additional force perpendicular to flowing direction is limited, and the turbulent flowing and heat transfer is mainly determined by the axial turbulent intensity and inlet velocity. However, in the 4 rod bundles, the restriction of the channel wall is small. The effect of the additional force perpendicular to flowing direction on the flowing and heat transfer is significant. And the additional force perpendicular to flowing direction can also affect the Reynolds stress. 相似文献
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The flow and heat transfer of turbulent flow in typical 4 rod bundles in rolling motion is investigated with LES and URANS. The effect of rolling motion consists of two parts, the axial additional force which causes velocity oscillation and the radial additional force. The effect of rolling motion on the flowing similarity is considerable. The effect of radial additional force on the flow should not be neglected. In ocean environment, the effect of radial additional force on the flow should not be neglected. The average parameters are determined by the drive force and axial additional force, but the parameter profiles in the cross section are mainly determined by the radial additional force. 相似文献
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The flowing and heat transfer of turbulent flow in typical 4 rod bundles in rolling motion is investigated with LES and URANS. As the rolling period decreases, the average wall shear stress increases, and the frictional resistance increases. The wall shear stress solved by LES is not good enough, while that of URANS is consistent with experiments. The variation of frictional resistance coefficient, Nusselt number and Reynolds stress with rolling amplitude is very weak. In rolling motion, the biggest frictional resistance coefficient is not located in a constant time. 相似文献
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The flow and heat transfer models of laminar flow and turbulent flow in rolling motion are established theoretically and modified with CFD results and experimental data. The correlations of frictional resistance coefficient and Nusselt number in pipes in rolling motion are obtained. The effect of rolling motion on the flow and heat transfer is mainly affected by the Reynolds number, angular acceleration and channel diameter. As the channel diameter is small, the effect of rolling motion on the flow and heat transfer is weak. The modified correlations of frictional resistance coefficient and Nusselt number in rolling motion could predict the flow and heat transfer in pipes in rolling motion correctly. The average discrepancy between theoretical correlations and experimental data is about 15%. 相似文献
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The turbulent flow in 37 rod bundles is investigated with CFD code FLUENT. The calculation results were validated with experimental data at first. Then the effects of diminishing rod-rod gap size on local flow, heat transfer and coherent structure in tight lattice are analyzed. The critical pitch to diameter ratio is next to 1.03. As the pitch to diameter ratio decreases from a high level to 1.03, the coherent structure and flow oscillation increase gradually. However, as the gap size continues decreasing, the coherent structure and flow oscillation decay very quickly. In the very narrow gap, the coherent structure is so weak that it could be neglected. The oscillations of velocity, wall shear stress and wall temperature are also very weak. But the spatial variation of the parameters in this gap is very significant. 相似文献
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The flow in a tight lattice is strongly affected by the quasi-periodic lateral flow pulsations caused by large scale vortices. This kind of large scale vortices is largely responsible for the momentum and heat exchange across the gaps. In rolling motion, the coherent structure and flow oscillation are affected by an additional force. The coherent structure in rolling motion is more significant than that in no rolling motion. The oscillation period in rolling motion is about 10% bigger than that in no rolling motion. The rolling motion can affect the coherent structure. However, the effect of rolling motion on the thermal hydraulic parameters, i.e. wall temperature and bulk temperature, is very limited. The wall temperature and wall shear stress in rolling motion and no rolling motion are nearly the same. The additional force due to rolling motion can change the moving characteristics of coherent structures, but its effect on the turbulent flow and heat transfer is weak. 相似文献