Numerical simulation of fluid flow and heat transfer of high rotation and density ratio flow in internal cooling channels of turbine blades with smooth walls is the main focus of this study. The flow in these channels is affected by rotation, buoyancy, bends, and boundary conditions. On the basis of comparison between two-equation (k− −ε and k− −ω) and Reynolds-stress (RSM) turbulence models, it is concluded that the two-equation turbulence models cannot predict heat transfer correctly, whereas RSM showed improved prediction. Thus RSM model was validated against available experimental data (which are primarily at low rotation and buoyancy numbers). The model was then used for cases with high rotation numbers (as much as 1.29) and high-density ratios (up to 0.4) not studied previously. Particular attention was given to how Reynolds stresses, turbulence intensity, and transport are affected by coriolis and buoyancy/centrifugal forces caused by high levels of rotation and density ratio. The results obtained are explained in view of physical interpretation of Coriolis and centrifugal forces. It has been concluded that the heat-transfer rate can be enhanced rapidly by increasing rotation number to values that are comparable to the enhancement caused
by introduction of ribs inside internal cooling channels. It is possible to derive linear correlation for the increase in Nusselt number as a function of rotation number. Increasing density ratios at high rotation number does not necessarily cause an increase in Nusselt number. The increasing thermal boundary-layer thickness near walls is the possible reason for this behavior ofNusselt number. Nomenclature a ce = acceleration caused by centrifugal force a co = acceleration caused by Coriolis force D h = hydraulic diameter f ce = centrifugal force f co = Coriolis force N u = local Nusselt number, h D h /k N u 0 = Nusselt number in fully developed turbulent nonrotating tube flow Pr = Prandtl number Pr t = turbulent Prandtl number R = radius from axis of rotation Re = Reynolds number, ρW 0 D h /µ Ro = rotation number, D h /W 0 r = inner radius of bend S = distance in streamwise direction T = local coolant temperature T b = coolant bulk temperature T 0= coolant temperature at inlet T w = wall temperature W 0 = inlet velocity ρ/ρ = density ratio, (T w − T 0 )/T w θ = dimensionless temperature, (T − T 0 )/(T w − T 0 ) µ = dynamic viscosity of coolant ρ = density of air