Publication | Closed Access
The effect of cell tilting on turbulent thermal convection in a rectangular cell
44
Citations
39
References
2014
Year
Rectangular CellEngineeringFluid MechanicsTurbulenceConvective Heat TransferTurbulent Thermal ConvectionMixed ConvectionTransport PhenomenaThermodynamicsNatural ConvectionBiophysicsHydrodynamic StabilityCell WidthPhysicsFlow PhysicRayleigh NumberHeat TransferTurbulent Flow Heat TransferPhysiologyTurbulence ModelingThermal Engineering
Abstract In this study the influence of cell tilting on flow dynamics and heat transport is explored experimentally within a rectangular cell (aspect ratios ${\it\Gamma}_{x}=1$ and ${\it\Gamma}_{y}=0.25$ ). The measurements are carried out over a wide range of tilt angles ( $0\leqslant {\it\beta}\leqslant {\rm\pi}/2\ \text{rad}$ ) at a constant Prandtl number ( $\mathit{Pr}\simeq 6.3$ ) and Rayleigh number ( $\mathit{Ra}\simeq 4.42\times 10^{9}$ ). The velocity measurements reveal that the large-scale circulation (LSC) is sensitive to the symmetry of the system. In the level case, the high-velocity band of the LSC concentrates at about a quarter of the cell width from the boundary. As the cell is slightly tilted ( ${\it\beta}\simeq 0.04\ \text{rad}$ ), the position of the high-velocity band quickly moves towards the boundary. With increasing ${\it\beta}$ , the LSC changes gradually from oblique ellipse-like to square-like, and other more complicated patterns. Oscillations have been found in the temperature and velocity fields for almost all ${\it\beta}$ , and are strongest at around ${\it\beta}\simeq 0.48\ \text{rad}$ . As ${\it\beta}$ increases, the Reynolds number ( $\mathit{Re}$ ) initially also increases, until it reaches its maximum at the transition angle ${\it\beta}=0.15\ \text{rad}$ , after which it gradually decreases. The cell tilting causes a pronounced reduction of the Nusselt number ( $\mathit{Nu}$ ). As ${\it\beta}$ increases from 0 to 0.15, 1.05 and ${\rm\pi}/2\ \text{rad}$ , the reduction of $\mathit{Nu}$ is approximately 1.4 %, 5 % and 18 %, respectively. Over the ranges of $0\leqslant {\it\beta}\leqslant 0.15\ \text{rad}$ , $0.15\leqslant {\it\beta}\leqslant 1.05\ \text{rad}$ and $1.05\leqslant {\it\beta}\leqslant {\rm\pi}/2\ \text{rad}$ , the decay slopes are $8.57\times 10^{-2}$ , $3.27\times 10^{-2}$ and $0.24\ \text{rad}^{-1}$ , respectively.
| Year | Citations | |
|---|---|---|
Page 1
Page 1