Abstract
Studies on mixed convective fluid flow and heat transfer are much more scarce compared to the large volume of literature available on either forced or natural convection. This is primarily because it was thought that applications of comparable forced and natural convection simultaneously are rather limited. However, the recent advent of high heat flux computing and LASER equipment and the need for their cooling has made mixed convection more relevant. The present review traces the development of studies in mixed convection over the last half a century. The most tricky and complex question in this respect may be that of the onset of turbulent flow in mixed convection. A clear and acceptable criterion for the transition of laminar flow to turbulent in this regime is still evasive. Hence, the review has culminated into a relook into the studies dedicated to these transition characteristics.
The article is dedicated to the memory of Prof. Brian Spalding with whom the corresponding author spent an exciting week at St. Petersburg, Russia during a conference organized by Prof. D. Leontiev. Prof. Spalding’s (along with Prof. Launder) work in turbulent mixed convection is the inspiration behind this review.
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Abbreviations
- \(Re\) :
-
Reynolds number (\(\rho VD/\mu\))
- \(Ri\) :
-
Richardson number (\(Gr/Re^{2}\))
- \(Pr\) :
-
Prandtl number (\(\mu C_{p} /k\))
- \(Ra\) :
-
Rayleigh number (\(Gr.Pr\))
- \(Nu\) :
-
Nusselt number (\(hD/k\))
- \(Kn\) :
-
Knudsen number (\(\lambda /L\)); ‘\(\lambda\)’ is mean free path
- \(Ha\) :
-
Hartman number
- \(\overline{Nu}\) :
-
Average Nusselt number
- \(Nu_{T}\) :
-
Nusselt number for forced turbulent convection
- \(Gr\) :
-
Grashof number
- \(Gr_{q}\) :
-
Grashof number based on heat flux (\(g\beta D^{4} \dot{q}/\nu^{2} k\))
- \(Gr_{D}\) :
-
Grashof number based on diameter (\(g\beta D^{3} {\Delta }T/\nu^{2}\))
- \(Gr_{L}\) :
-
Grashof number based on constant wall temperature (\(g\beta L^{3} {\Delta }T/\nu^{2}\))
- \(Gr_{T}\) :
-
Thermal Grashof number (\(g\beta D^{3} {\Delta }T/\nu^{2}\))
- \(Gr_{M}\) :
-
Solutal Grashof number (\(g\beta_{M} D^{3} {\Delta \omega }/\nu^{2}\))
- \(\overline{Ra}\) :
-
Average Rayleigh number
- \(\overline{Re}\) :
-
Average Reynolds number
- \(\widehat{Nu}\) :
-
Weighted average Nusselt number
- \(Gz\) :
-
Graetz number \(\left( {\frac{D}{L}Re.Pr} \right)\)
- \(Re_{cr}\) :
-
Critical Reynolds number
- \(Re_{\theta }\) :
-
Transition momentum thickness Reynolds number
- \(Re_{qt}\) :
-
Reynolds value at the start of quasi-turbulent flow regime
- \(Re_{x}\) :
-
Local Reynolds number
- \(Bo\) :
-
Buoyancy parameter (\(Gr_{q} /Re^{m} Pr^{n}\))
- \(Bo_{2}\) :
-
Buoyancy parameter (\(Gr_{q} /Re^{2.5} Pr\))
- \(K\) :
-
Buoyancy parameter (\(Gr/Re^{2.5}\))
- \(ER\) :
-
Expansion ratio (outlet to inlet height ratio)
- E :
-
Enhancement ratio (ratio of heat input with porosity and without porosity)
- ACFD:
-
Asymptotic Computational Fluid Dynamics
- AWF:
-
Analytical Wall Functions
- CFD:
-
Computational Fluid Dynamics
- CMM:
-
Compound Matrix Method
- CMSIP:
-
Coupled Modified Strongly Implicit Procedure
- DNS:
-
Direct Numerical Simulation
- FCD:
-
Forced Convection Developing
- FD:
-
Fully Developed
- LBM:
-
Lattice Boltzmann Method
- LES:
-
Large Eddy Simulation
- MCD:
-
Mixed Convection Developing
- OpenFOAM:
-
Open source Field Operation And Manipulation
- PIV:
-
Particle Image Velocimetry
- RANS:
-
Reynolds Averaged Navier-Stokes
- RNG:
-
Renormalization Group Method
- SST:
-
Shear Stress Transport
- UHF:
-
Uniform Heat Flux
- UWT:
-
Uniform Wall Temperature
- \(\varepsilon\) :
-
Rate of dissipation of turbulence energy
- \(\omega\) :
-
Specific rate of dissipation
- \(\varphi_{v}\) :
-
Viscosity ratio (\(\mu_{b} /\mu_{w}\))
- \(\mu_{b}\) :
-
Dynamic viscosity at bulk temperature (Pa s)
- \(\mu_{w}\) :
-
Dynamic viscosity at the wall temperature (Pa s)
- \(\lambda\) :
-
Buoyancy parameter (\(Gr/Re^{2}\))
- \(\emptyset\) :
-
Volume fraction
- \(\varphi\) :
-
Angle (degree or radian)
- \(\theta\) :
-
Dimensionless temperature
- \(\rho\) :
-
Density (kg/m3)
- \(\gamma\) :
-
Intermittency in \(\gamma - Re_{\theta }\) transition model
- \(\beta\) :
-
Thermal expansion coefficient (K−1)
- k:
-
Thermal conductivity (W/m K)
- \(k\) :
-
Turbulence kinetic energy (J)
- Sp. Gr.:
-
Specific gravity
- g :
-
Acceleration due to gravity (m/s2)
- a, b, c :
- \(L\) :
-
Length (m)
- \(D\) :
-
Diameter (m)
- \(D_{h}\) :
-
Hydraulic diameter (m)
- \(d_{e}\) :
-
Equivalent diameter of a channel (m) (\(2hb/\left( {h + b} \right);\) \(h,b\) are channel height and width)
- \(A\) :
-
Aspect ratio (–)
- Q:
-
Heat rate (W)
- \(\dot{q}\) :
-
Heat flux (W/m2)
- \(q_{1}\) :
-
Cold wall heat flux (W/m2)
- \(q_{2}\) :
-
Hot wall heat flux (W/m2)
- \(x, y\) :
-
Axial and transverse coordinates (m)
- \(u, v\) :
-
Axial and transverse velocities (m/s)
- \(X, Y\) :
-
Dimensionless axial and transverse coordinates
- \(U, V\) :
-
Dimensionless axial and transverse velocity
- \(x\) :
-
Distance from the initial point of heating (m)
- \(C_{p}\) :
-
Specific heat at constant pressure (J/kg K)
- \(C_{f}\) :
-
Skin friction coefficient (–)
- ̴:
-
Approximately
- ©:
-
Copyright
- lam, l:
-
Laminar
- b :
-
Properties of fluid at bulk temperature
- q :
-
Based on heat flux
- M :
-
Mixed convection in Eq. 7
- trans:
-
Transition
- \(c, cr\) :
-
Critical value
- \(lc\) :
-
Laminar flow at critical Reynolds number
- \(cr_{2}\) :
-
Critical value at second wall
- \(x\) :
-
Local value
- t :
-
Turbulent
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Gorai, S., Das, S.K. (2020). Studies on Mixed Convection and Its Transition to Turbulence—A Review. In: Runchal, A. (eds) 50 Years of CFD in Engineering Sciences. Springer, Singapore. https://doi.org/10.1007/978-981-15-2670-1_10
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