Skip to main navigation Skip to search Skip to main content

Reynolds-averaged Navier-Stokes simulations of opposing flow turbulent mixed convection heat transfer in a vertical tube

  • Kosuke Motegi*
  • , Yasuteru Sibamoto
  • , Takashi Hibiki*
  • *Corresponding author for this work

Research output: Journal Publications and ReviewsRGC 21 - Publication in refereed journalpeer-review

Abstract

This study performed Reynolds-Averaged Navier-Stokes (RANS) simulations of a single-phase turbulent opposing flow mixed convection in a heated vertical circular tube. Previous research has reported that the Launder-Sharma k−ε model (hereafter the LS model), one of the most popular RANS turbulence models, sometimes overestimates experimental data of heat transfer coefficients for opposing flows. Although the RANS models have been widely applied to opposing flows in various engineering problems, the conditions under which the anomaly in the LS model occurs and the underlying mechanisms remain unclear. This study aimed to understand the model characteristics and their applicability under various mixed convection conditions. This study investigated the LS model, the LS model with the Yap correction, and the v2− f model, comparing them with existing experimental data of the Nusselt number and the friction coefficient in fully developed regions. The LS model remarkably over-predicted the Nusselt number and the friction coefficient under highly buoyant conditions. The error for the Nusselt number was >90 % for NB,JF ≈ 3×10−3, where NB,JF is a controlling parameter characterizing the strength of buoyancy influence. The conditions under which the prediction of the LS model failed were linked to those under which reverse flow occurred near the heated wall. We obtained NB,JF ≈ 1.25×10−3 for the reverse flow condition. This condition could be used where the LS model could not be applied. The LS model with Yap correction and v2− f model could predict experimental data successfully from forced convection to mixed convection conditions 10−6 NB,JF  < 10−2. For natural convection-dominant conditions NB,JF  > 10−2, the LS model with the Yap correction was numerically unstable and could not obtain a converged numerical solution; however, the v2−f model stably reproduced the experimental data. By optimizing the model constants included in the Yap correction, the stability and accuracy of the calculations could be improved under highly buoyant opposing flow conditions. © 2024 Elsevier Ltd
Original languageEnglish
Article number126406
JournalInternational Journal of Heat and Mass Transfer
Volume237
Online published16 Nov 2024
DOIs
Publication statusPublished - Feb 2025

Funding

T. Hibiki would like to express his sincere appreciation to the Hong Kong SAR government and Hong Kong Jockey Club for supporting his research under the Global STEM Professorship and JC STEM Lab of Innovative Thermal-fluid Science, respectively

Research Keywords

  • Computational fluid dynamics
  • Friction factor
  • Heat transfer coefficient
  • Opposing flow
  • Turbulence model
  • Turbulent mixed convection

Publisher's Copyright Statement

  • COPYRIGHT TERMS OF DEPOSITED POSTPRINT FILE: © 2024 Elsevier. This manuscript version is made available under the CC-BY-NC-ND 4.0 license https://creativecommons.org/licenses/by-nc-nd/4.0/.

Fingerprint

Dive into the research topics of 'Reynolds-averaged Navier-Stokes simulations of opposing flow turbulent mixed convection heat transfer in a vertical tube'. Together they form a unique fingerprint.

Cite this