Combined Natural Convection and Radiation in a Volumetrically Heated Fluid Layer

[+] Author and Article Information
T. C. Chawla, F. B. Cheung, D. H. Cho

Reactor Analysis and Safety Division, Argonne National Laboratory, Argonne, IL 60439

S. H. Chan

Department of Mechanical Engineering, University of Wisconsin-Milwaukee, Milwaukee, Wisc. 53201

J. Heat Transfer 102(1), 81-85 (Feb 01, 1980) (5 pages) doi:10.1115/1.3244253 History: Received May 29, 1979; Online October 20, 2009


The effect of radiation in combination with turbulent natural convection on the rates of heat transfer in volumetrically heated fluid layers characterized by high temperatures has been considered in this study. It is demonstrated that even at high Rayleigh numbers the radiation mode is as effective as the turbulent natural convection mode in removing the heat from the upper surface of the molten pools with adiabatic lower boundary. As a result of this improved heat transfer, it is shown that considerably thicker molten pools with internal heat generation can be supported without boiling inception. The total Nusselt number at a moderate but fixed value of conduction-radiation parameter, can be represented as a function of Rayleigh number in a simple power-law form. As a consequence of this relationship it is shown that maximum nonboiling pool thicknesses vary approximately inversely as the 0.9 power of internal heat generation rate. A comparison between exact analysis using the integral formulation of radiation flux and Rosseland approximation shows that the latter approximation bears out very adequately for optically thick pools with conduction-radiation parameter ≳ 0.4 inspite of the fact that individual components of Nusselt number due to radiation and convection, respectively, are grossly in error. These errors in component heat fluxes are compensating due to the total heat balance constraint. However, the comparison between Rosseland approximation and exact formulation gets poorer as the value of conduction-radiation parameter decreases. This increase in error is principally incurred due to the error in estimating wall temperature differences.

Copyright © 1980 by ASME
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