Prandtl number scaling of unsteady natural convection boundary layers for Pr>1 fluids under isothermal heating

Wenxian Lin, S. W. Armfield, J. C. Patterson, and Chengwang Lei
Phys. Rev. E 79, 066313 – Published 24 June 2009

Abstract

In this paper, the scalings incorporating the Prandtl number (Pr) dependence have been obtained by a scaling analysis for the unsteady natural convection boundary layer of an initially quiescent isothermal Newtonian fluid of Pr>1 produced by the sudden imposition of a higher temperature on a vertical plate. It is shown that the transient flow behavior of the resulting boundary layer can be described by a three-region structure and at the start-up stage the boundary layer development is one dimensional and independent of height due to the dominance of pure conduction; however, at steady state it becomes two dimensional and height dependent as the flow becomes dominated by convection. Numerical results demonstrate that the scalings representing the thermal boundary layer development accurately represent their Pr dependence over the whole stage of flow development. The scalings representing the viscous boundary layer development are generally in good agreement with the numerical results with the Pr variation over the whole stage of flow development, although there are small deviations from the numerical results with the Pr variation that are within acceptable limits for scaling.

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  • Received 7 October 2008

DOI:https://doi.org/10.1103/PhysRevE.79.066313

©2009 American Physical Society

Authors & Affiliations

Wenxian Lin1,2,*, S. W. Armfield3, J. C. Patterson1, and Chengwang Lei1

  • 1School of Engineering, James Cook University, Townsville, Queensland 4811, Australia
  • 2Solar Energy Research Institute, Yunnan Normal University, Kunming, Yunnan 650092, People’s Republic of China
  • 3School of Aerospace, Mechanical and Mechatronic Engineering, University of Sydney, New South Wales 2006, Australia

  • *FAX: 61-7-4781-6788; wenxian.lin@jcu.edu.au

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Issue

Vol. 79, Iss. 6 — June 2009

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