AIAA-44356-943.pdf

  1. 1、本文档共10页,可阅读全部内容。
  2. 2、有哪些信誉好的足球投注网站(book118)网站文档一经付费(服务费),不意味着购买了该文档的版权,仅供个人/单位学习、研究之用,不得用于商业用途,未经授权,严禁复制、发行、汇编、翻译或者网络传播等,侵权必究。
  3. 3、本站所有内容均由合作方或网友上传,本站不对文档的完整性、权威性及其观点立场正确性做任何保证或承诺!文档内容仅供研究参考,付费前请自行鉴别。如您付费,意味着您自己接受本站规则且自行承担风险,本站不退款、不进行额外附加服务;查看《如何避免下载的几个坑》。如果您已付费下载过本站文档,您可以点击 这里二次下载
  4. 4、如文档侵犯商业秘密、侵犯著作权、侵犯人身权等,请点击“版权申诉”(推荐),也可以打举报电话:400-050-0827(电话支持时间:9:00-18:30)。
查看更多
AIAA-44356-943

Turbulence Modeling Applied to Flow Through a Staggered Tube Bundle You Qin Wang? and Peter L. Jackson? University of Northern British Columbia, Prince George, British Columbia V2N 4Z9, Canada DOI: 10.2514/1.44356 Both two-dimensional and three-dimensional numerical simulations of the turbulent flow through a staggered tube bundle are presented. The primary aim of the present study is to search for a turbulentmodel that could serve as an engineering design tool at a relatively low computational cost. In the present study, the performances of the Spalart–Allmaras model, the k- model, and large eddy simulation are evaluated by comparing their simulation results against experimental measurements. The turbulence models are assessed mainly based on their ability to resolve time-dependent features of the flow related to vortex shedding. Simulations are performed at a Reynolds number of 9300. Overall, the predicted streamwise mean velocity and transverse mean velocity in the present study are in good agreement with measurements, and the results show that the simple one-equation Spalart–Allmaras model could be a verypromising tool for numerical simulation of complex turbulentflows, since the Strouhal number obtained by it agrees well with measurements available in the literature for similar tube geometries. Nomenclature Cd = streamwise drag coefficient, 2Fd=U 21dLz d = tube diameter, m Fd = streamwise drag force, N k = turbulent kinetic energy, m2=s3 Lz = computational domain in the z direction, m Re = Reynolds number, U1d= SL = longitudinal pitch, m ST = transverse pitch, m T = temperature, K t = physical time step, s t = nondimensional time step, tU1=d U = x-direction mean velocity component, m=s U1 = inlet velocity, m=s uiuj = Reynolds stress, m=s2 u = friction velocity, m=s V = y-direction mean velocity component, m=s W = z-direction mean velocity component, m=s x = streamwise coordinate, m y = transverse coordinate, m z = spanwise coordinate, m y = distance fr

您可能关注的文档

文档评论(0)

l215322 + 关注
实名认证
内容提供者

该用户很懒,什么也没介绍

1亿VIP精品文档

相关文档