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Turbulent Mixing Models and Other Mixing Coefficients in Subchannel Codes-A Review Part A: Single Phase

机译:湍流混合模型和子信道代码中的其他混合系数 - 审查部分A:单相

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摘要

Subchannel code analysis is one of the key thermal-hydraulic approaches for nuclear reactor design and safety analysis. At present, subchannel codes are employed to compute local thermal-hydraulic conditions on the rod bundle fuel assemblies of nuclear reactor cores and to predict the performance of nuclear cores during normal and hypothetical accident conditions. Currently, the subchannel code is still the main tool for thermal-hydraulic analysis in the process of nuclear fuel licensing. For inter-subchannel transfer, the widely accepted key mechanisms are (1) single- and two-phase cross flow, (2) single- and two-phase turbulent mixing, and (3) two-phase void drift. Turbulent mixing has been recognized as a vortex train moving along the gap between rods. As one of the key phenomena, the turbulent mixing model has been embedded in the subchannel code for decades. Originally, the turbulent mixing model was developed based on various adiabatic and diabatic subchannel turbulent mixing tests. Numerous correlations or coefficients have been developed for different codes. For commercial applications, the large-scale rod bundle tests of thermal mixing and critical heat flux (CHF) are the main approaches to obtain a specific model for a particular fuel/spacer design. The turbulent mixing coefficient and other parameters are determined in this process for the specific mixing vane grid design. In this process, various approaches to obtain the turbulent mixing coefficient have been proposed. Conventionally, in the subchannel codes the combined bare rod mixing and spacer grid-enhanced turbulent mixing effects on coolant have been represented by the turbulent mixing coefficient. The lack of a grid-dependent directional cross-flow model has always led to the prediction bias of local condition, especially for the hot channel where CHF generally occurs. However, in recent years, modified grid models with directional diversion cross flow have been developed to improve the prediction of spacer grid performance. In recent years, owing to the very fast improvement and rapid growth of computational resources, computational fluid dynamics (CFD) has gained popularity and advancement in the model development of subchannel codes. To substitute the costly and time consuming tests, instead of a simple turbulent mixing coefficient in the lumped parameter approach, various CFD approaches for turbulent mixing model development in subchannel codes have been proposed. CFD takes great advantage of lower cost, high resolution, and versatility. Though verification and validation are still required, CFD will be a very important tool for developing turbulent mixing models for subchannel codes. In this critical review, the development and application of turbulent mixing models in various subchannel codes for liquid metal-cooled reactor analysis are reviewed and summarized. The codes, models, tests, simulations, and future modifications are reviewed in detail.
机译:子信道代码分析是核反应堆设计和安全性分析的关键热液压方法之一。目前,使用子通道码来计算核反应堆核心杆束燃料组件上的局部热液压条件,并在正常和假设事故条件下预测核核心的性能。目前,子信道代码仍然是核燃料许可过程中热液压分析的主要工具。对于子通道间转移,广泛接受的关键机制是(1)单相和两相交叉流动,(2)单相和两相湍流混合,(3)两相空隙漂移。湍流混合已被认为是沿杆之间的间隙移动的涡流火车。作为关键现象之一,湍流混合模型已嵌入到子信道代码中数十年。最初,基于各种绝热和糖尿病子通道湍流混合试验开发了湍流混合模型。已经为不同的代码开发了许多相关性或系数。对于商业应用,热混合和临界热通量(CHF)的大尺寸杆束试验是获得特定燃料/间隔设计的特定模型的主要方法。在该方法中确定了湍流混合系数和其他参数,用于特定混合叶片网格设计。在该过程中,已经提出了获得湍流混合系数的各种方法。通常,在子通道码中,通过湍流混合系数表示对冷却剂的组合裸杆混合和间隔电网增强的湍流混合效果。缺乏依赖网格依赖的方向横流模型一直导致局部条件的预测偏差,特别是对于通常发生CHF的热通道。然而,近年来,已经开发出具有定向转移横流的改进的网格模型来改善间隔栅格性能的预测。近年来,由于计算资源的快速增长和快速增长,计算流体动力学(CFD)在子信道代码的模型开发中获得了普及和进步。为了替换昂贵和耗时的测试,而不是在集总参数方法中进行简单的湍流混合系数,提出了在子通道码中湍流混合模型开发的各种CFD方法。 CFD具有较低的成本,高分辨率和多功能性的优势。虽然仍然需要验证和验证,但CFD将是开发子信道代码的湍流混合模型的一个非常重要的工具。在这一关键评论中,综述了和总结了液体冷却反应器分析各种子通道码中湍流混合模型的开发和应用。详细审查了代码,模型,测试,模拟和未来修改。

著录项

  • 来源
    《Nuclear Technology》 |2020年第9期|1253-1295|共43页
  • 作者单位

    Delta Energy Group No. 413 Venture Building No. 1 Changjiang Road Economic and Technology Development Zone Jiaozhou Qingdao 266300 Shandong China DEQD Institute for Advanced Research in Multiphase Flow and Energy Transfer No. I Huiying Road Economic and Technology Development Zone Jiaozhou Qingdao 266300 Shandong China;

    Delta Energy Group No. 413 Venture Building No. 1 Changjiang Road Economic and Technology Development Zone Jiaozhou Qingdao 266300 Shandong China DEQD Institute for Advanced Research in Multiphase Flow and Energy Transfer No. I Huiying Road Economic and Technology Development Zone Jiaozhou Qingdao 266300 Shandong China;

    Delta Energy Group No. 413 Venture Building No. 1 Changjiang Road Economic and Technology Development Zone Jiaozhou Qingdao 266300 Shandong China DEQD Institute for Advanced Research in Multiphase Flow and Energy Transfer No. I Huiying Road Economic and Technology Development Zone Jiaozhou Qingdao 266300 Shandong China;

    Xi'an Jiaotong University School of Nuclear Science and Technology Xianning West Road 28 Xi'an 710049 Shaanxi China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Subchannel code; turbulent mixing model; computational fluid dynamics; rod bundle;

    机译:子信道代码;湍流混合模型;计算流体动力学;棒束;

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