Abstract
In this work, we present a numerical study of mixed convection coupled with radiation in an inclined channel with an aspect ratio B = L′/H′=10, and locally heated from one side. Convective, radiative and total Nusselt numbers, evaluated on the cold surface and at the exit of the channel, are presented for different combinations of the governing parameters namely, the surface emissivity (0 ≤ ε ≤ 1), the Reynolds number (10 ≤ Re ≤ 50), the inclination of the channel with respect to the horizontal surface (0° ≤ θ ≤ 90°) and the Rayleigh number (Ra = 105). The ratio, R = QC/QE, of the heat quantities, leaving the channel through the cold wall, QC, and through the exit, QE, is presented to identify the most favorable issue to the heat transfer in the studied configuration. The results obtained show that the flow structure is significantly altered by radiation which contributes to reduce or to enhance the number of the solutions obtained.
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Abbreviations
- B:
-
aspect ratio of the channel, B = L′/H′
- cv:
-
convection
- Fij:
-
view factor between Si and Sj elements
- g:
-
acceleration due to the gravity, m/s2
- H′:
-
height of the channel, m
- Ii:
-
dimensionless irradiation, \(I_{\text{i}} = {{I{\prime}_{\text{i}} } \mathord{\left/ {\vphantom {{I{\prime}_{\text{i}} } {\sigma T{\prime}_{\text{C}}^4 }}} \right. \kern-\nulldelimiterspace} {\sigma T{\prime}_{\text{C}}^4 }}\)
- Ji:
-
dimensionless radiosity, \(J_{\text{i}} = {{J{\prime}_{\text{i}} } \mathord{\left/ {\vphantom {{J{\prime}_{\text{i}} } {\sigma T{\prime}_{\text{C}}^4 }}} \right. \kern-\nulldelimiterspace} {\sigma T{\prime}_{\text{C}}^4 }}\)
- L′:
-
length of the channel, m
- Nr:
-
convection-radiation interaction parameter, \(N_{\text{r}} = {{\sigma T{\prime}_{\text{C}}^4 H{\prime}} \mathord{\left/ {\vphantom {{\sigma T{\prime}_{\text{C}}^4 H{\prime}} {\lambda \left( {T{\prime}_{\text{H}} - T{\prime}_{\text{C}} } \right)}}} \right. \kern-\nulldelimiterspace} {\lambda \left( {T'_{\text{H}} - T'_{\text{C}} } \right)}}\)
- Nu:
-
average Nusselt number
- Pr:
-
Prandtl number, Pr = ν /α
- Qr:
-
dimensionless radiative heat flux, \(Q_{\text{r}} = {{Q{\prime}_{{\text{ r}}} } \mathord{\left/ {\vphantom {{Q{\prime}_{{\text{ r}}} } {\sigma T{\prime}_{\text{C}}^4 }}} \right. \kern-\nulldelimiterspace} {\sigma T{\prime}_{\text{C}}^4 }}\)
- R:
-
ratio of the heat quantities evacuated through the cold wall and the exit, R = QC/QE
- Ra:
-
Rayleigh number, Ra = g β (T′H − T′C) H′3/α ν
- rd:
-
radiation
- Re:
-
Reynolds number, Re = u′o H′/ν
- t:
-
dimensionless time, t = t′ u′o/H′
- T:
-
dimensionless fluid temperature, T = (T′ − T′C)/(T′H − T′C)
- T′C:
-
temperature of the cold plate, K
- T′H:
-
temperature of the heated elements, K
- To:
-
dimentionless reference temperature, To = T′C/(T′H − T′C)
- u′o:
-
velocity of the imposed flow, m/s
- (u, v):
-
dimensionless horizontal and vertical velocities, (u, v) = (u′, v′)/u′o
- (x, y):
-
dimensionless coordinates, (x, y) = (x′, y′)/H′
- α:
-
thermal diffusivity of fluid, m2/s
- β:
-
thermal expansion coefficient of fluid, 1/K
- ε:
-
emissivity of the walls
- λ:
-
thermal conductivity of fluid, W/(K m)
- ν:
-
kinematic viscosity of fluid, m2/s
- Ω:
-
dimensionless vorticity, Ω = Ω′ H′/u′o
- Ψ:
-
dimensionless stream function, Ψ = Ψ′/u′o H′
- σ:
-
Stéfan-Boltzman constant, σ = 5669×10−8 W/(m2 K4)
- θ:
-
inclination of the channel, (in degree)
- C:
-
cold surface
- CR:
-
critical parameter
- E:
-
exit of the channel
- H:
-
heated surface
- I:
-
inlet of the channel
- ′:
-
dimensional variable
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Bahlaoui, A., Raji, A. & Hasnaoui, M. Multiple Steady State Solutions Resulting From Coupling Between Mixed Convection And Radiation In An Inclined Channel. Heat Mass Transfer 41, 899–908 (2005). https://doi.org/10.1007/s00231-004-0590-9
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DOI: https://doi.org/10.1007/s00231-004-0590-9