4.7 Article

Mixed Convection in a Horizontal Channel-Cavity Arrangement with Different Heat Source Locations

Journal

MATHEMATICS
Volume 11, Issue 6, Pages -

Publisher

MDPI
DOI: 10.3390/math11061428

Keywords

mixed heat transfer; heated sources; Nusselt number; horizontal channel; enclosure

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This article uses COMSOL-Multiphysics to study laminar coupled mixed convection heat transfer in a horizontal channel-cavity architecture. The effect of heat source location on isotherms, velocity distribution, pressure, temperature, Nusselt numbers, and air density is investigated. The results show that the highest heat transfer occurs when the heat source is near the contact surface between the channel and the cavity. Changing the position of the heated source does not affect the velocity distribution or pressure distribution. Air density profiles differ around y = 0.035 m, with the third case having a higher density than the second case, which in turn has a higher density than the first case. The contact surface (y = 0) has the highest Nusselt number and exhibits the highest heat transfer.
Several researchers are very interested in mixed convection heat transfer because of how widely it is used, particularly for solar thermal collectors, cooling electronic equipment, and chemical process instruments. Using COMSOL-Multiphysics, this article establishes laminar coupled mixed convection heat transfer characteristics across a horizontal channel-cavity architecture. Investigations are conducted into the effect of heat source location on isotherms, velocity distribution, pressure, temperature, average and local Nusselt numbers, and air density. The intake airflow Reynolds number is assumed constant on 2.8814. The enclosure with an isothermally heated right wall in the shape of a < as a heat source in three configurations (heat source in the base (1st case), in the upper step (2nd case), and the below step (3rd case). The obtained numerical results present that the higher heat transfer is performed in case two because the heat source is near the contact surface between the channel and the cavity. With the hot sources' locations being altered, the velocity distribution seems to be unchanged. The increase in the positive y axis has no impact on the pressure distribution throughout the channel. Changing the position of the heated source does not seem to have any impact on the pressure distribution. Air density profiles start to diverge across cases around y = 0.035 m; the third example has a larger value than the second case, and the latter case has a larger value in the density distribution than the former. The contact between the enclosure and the channel (y = 0), where the greatest Nusselt number also occurs, exhibits the highest heat transfer. The maximal Nusselt number falls as y's absolute value rises.

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