Estudio numérico y experimental de flujo Rayleigh-Bénard en cavidades cúbicas para régimen transitorio y turbulento

Identificador:  TDX:328

Handle: https://hdl.handle.net/20.500.11797/TDX328

Autors:  Valencia Merizalde, Leonardo

Resum:
In the first part of this study, the effects of a non-Boussinesq fluid are numerically studied and discussed for Rayleigh-Bénard convection in a cubical cavity with perfectly conducting sidewalls at low and high Rayleigh numbers using water as a convecting fluid (Pr=5.9). Numerical simulations at all Rayleigh numbers considered were carried out for two different cases. In the first case a Boussinesq fluid was considered (Boussinesq Fluid Simulation-BFS) and in the second case, the dependence of viscosity and thermal conductivity of water on temperature was adopted in the simulations (Non-Boussinesq Fluid Simulation-NBFS). At the low Rayleigh numbers used in this study (Ra=104 and Ra=5x104) the flow is laminar and steady and at the high Rayleigh number considered (Ra=107) the flow is turbulent. At Ra=104 and Ra=5x104 we focus our analysis on the effect of variation of the fluid viscosity with temperature on the more stable flow structures from the set of seven different topologies reported in previous studies. At Ra=107 and Pr=5.9 the non-Boussinesq effects on the turbulent flow are analysed in detail and the flow structures and heat transfer rates compared with those available in the literature at Pr=0.71. Previous works recommend that temperature difference should be less than 4.5ºC in order to obtain less than 10% of variation in the viscosity. Non-Boussinesq simulations in the present work were calculated with a viscosity variation of 40% between cold and hot plates. The numerical simulations at high and low Rayleigh numbers were conducted with a second order finite volume code without any turbulence model because the time-steps and grid sizes used are adequate for the time and spatial resolution requirements reported in previous direct numerical simulations of Rayleigh-Bénard flows. The structure of the flow topologies at Ra=104 and Ra=5x104 are not significantly affected by the effects of the variation of viscosity and thermal conductivity with temperature. However, results obtained with a NBFS show an increase of the ascending flow velocities compared with those obtained with the Boussinesq approximation according to the decrease of viscosity with increasing temperature. At Ra=107 the instantaneous flow shows large deviations with respect to the time-average flow field that consists in two counter rotating vortex rings located near the horizontal plates. The temperature gradients and, thus the viscosity variation are located close to the walls within the thermal boundary layers. This causes that the time-averaged flow field topologies corresponding to BFS and NBFS are not greatly affected by the effects of the variation of viscosity and thermal conductivity with temperature.<br/>In the second part, experimental measurements and numerical simulations of natural convection in a cubical cavity heated from below and cooled from above are reported at turbulent Rayleigh numbers using water as a convective fluid (Pr=6.0). The numerical simulations were carried out, in the range 107&#8804;Ra&#8804;108, with a second order finite volume code without any turbulence model because the time-steps and grid sizes used are adequate for the time and spatial resolution requirements reported in previous direct numerical simulations of Rayleigh-Bénard flows. The Boussinesq approximation was considered in the simulations according to the thermal conditions and the dimensions of the cavities used in the experiments. The Particle Image Velocimetry technique was used to measure the two velocity components parallel to a vertical mid-plane of the cavity at Ra=107, Ra=7×107 and Ra=108. Both experiments and simulations show that at Ra=107 the time averaged flow structure consists in two horizontal counter-rotating vortex rings located near the horizontal walls of the cavity. At the higher Rayleigh numbers considered, the simulations predict an unsteady single roll motion in which the direction of the axis of rotation rotates in the horizontal plane with very low frequencies. This rotation produces a time averaged flow structure similar to that found at Ra=107. There is a general agreement between the predicted time averaged local<br/>velocities and those experimentally measured if the heat conduction through the sidewalls occurring in the experiments is considered in the simulations.