
Buoyancy-assisted flow reversal and combined mixed convection–radiation heat transfer in symmetrically heated vertical parallel plates: Influence of two radiative parameters
Author(s) -
Farzad Bazdidi–Tehrani,
Hadi Nazaripoor
Publication year - 2011
Publication title -
scientia iranica
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.299
H-Index - 51
eISSN - 2345-3605
pISSN - 1026-3098
DOI - 10.1016/j.scient.2011.07.008
Subject(s) - radiative transfer , emissivity , thermal radiation , mechanics , laminar flow , heat transfer , buoyancy , heat transfer coefficient , molar absorptivity , thermodynamics , churchill–bernstein equation , materials science , physics , nusselt number , optics , turbulence , reynolds number
The present article encompasses the laminar ascending flow and combined mixed (free and forced) convective-radiative heat transfer within symmetrically heated vertical parallel plates. Radiative heat transfer between two opposite walls is considered and the gas is assumed as gray, absorbing, emitting and scattering. Elliptic governing equations for the case of buoyancy assisted flow are solved numerically employing a home-made CFD code based on the finite volume method. The radiative transfer equation is solved using the discrete ordinates method, adopting its S6 quadrature scheme. The influence of two important radiative parameters, namely, wall emissivity and scattering albedo, while the extinction coefficient is either constant or not, on the occurrence of flow reversal, fanning friction coefficient, flow and thermal fields, is investigated. Present results show that the occurrence of reversed flow enhances both heat transfer and the fanning friction coefficient, and the radiation mode amplifies heat transfer, while reducing the fanning friction coefficient. As wall emissivity increases from 0 to 1, effects of radiation on flow and thermal fields rise. However, there is no linear relationship for the whole range of ε. As scattering albedo varies between 0 and 0.75, radiation effects on flow and thermal fields for the constant and variable extinction coefficient are entirely opposite