...
首页> 外文期刊>Nuclear Engineering and Design >Modeling of turbulent transport term of interfacial area concentration in gas-liquid two-phase flow
【24h】

Modeling of turbulent transport term of interfacial area concentration in gas-liquid two-phase flow

机译:气液两相流界面面积浓度湍流输运模型的建立

获取原文
获取原文并翻译 | 示例
           

摘要

A modeling of basic transport equation and constitutive equations of turbulent transport terms of interfacial area concentration was carried out. Based on the local instant formulation, interfacial area concentration was formulated in term of spatial correlation functions of characteristic function (local instant volume fraction) and its directional derivative of each phase. In the basic transport equations, interfacial area concentration is transported by time averaged interfacial velocity. In the previous models, interfacial velocity is roughly approximated by velocity of each phase. In the present model, interfacial velocity is formulated in term of spatial correlation functions of characteristic function and velocity of each phase and their directional derivatives. In this formulation, the time averaged interfacial velocity was shown to be correlation functions of fluctuation of velocity and local instant void fraction and their derivatives which reflect the transport of interfacial area concentration due to interaction between interfacial area and turbulence of each phase. Basic conservation equations of spatial correlation functions of characteristic function and velocity of each phase were also derived based on the conservation equations momentum and its fluctuation of each phase. For practical purpose, further modeling of this turbulent transport terms of interfacial area concentration was carried out. As a result, constitutive equations of turbulent diffusion and lateral migration of interfacial area concentration were obtained which can be applied to various flow regime of two-phase flow.
机译:进行了界面输运过程中界面输运的基本输运方程和本构方程的建模。根据局部瞬时公式,根据特征函数的空间相关函数(局部瞬时体积分数)及其各相的方向导数,来确定界面面积浓度。在基本输运方程中,界面区域浓度是通过时间平均界面速度来传输的。在以前的模型中,界面速度大致由每个相的速度来近似。在本模型中,界面速度用特征函数的空间相关函数和各相速度及其方向导数来表示。在该公式中,时间平均界面速度被证明是速度波动和局部瞬时空隙率及其衍生物的相关函数,它们反映了界面面积和各相之间的相互作用引起的界面面积浓度的传输。基于各相动量及其波动的守恒方程,推导了各相特征函数和速度的空间相关函数的基本守恒方程。出于实际目的,对该界面区域浓度的湍流输运项进行了进一步建模。结果,获得了湍流扩散和界面面积浓度的横向迁移的本构方程,可用于两相流的各种流态。

著录项

  • 来源
    《Nuclear Engineering and Design》 |2012年第12期|322-330|共9页
  • 作者单位

    Department of Mechanical Engineering, Osaka University, Japan;

    Department of Mechanical Engineering, Osaka University, Japan;

    Nuclear Power Engineering Center, Safety Analysis Croup, The Institute of Applied Energy,Japan;

    Nuclear Power Engineering Center, Safety Analysis Croup, The Institute of Applied Energy,Japan;

    Japan Nuclear Energy Safety Organization, Japan;

  • 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

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号