Rja. Janssen et Rawm. Henkes, INFLUENCE OF PRANDTL NUMBER ON INSTABILITY MECHANISMS AND TRANSITION IN A DIFFERENTIALLY HEATED SQUARE CAVITY, Journal of Fluid Mechanics, 290, 1995, pp. 319-344
The transition from laminar to turbulent of the natural-convection how
inside a square, differentially heated cavity with adiabatic horizont
al wails is calculated, using the finite-volume method. The purpose of
this study is firstly to determine the dependence of the laminar-turb
ulent transition on the Prandtl number and secondly to investigate the
physical mechanisms responsible for the bifurcations observed. It is
found that in the square cavity, for Prandtl numbers between 0.25 and
2.0, the transition occurs through periodic and quasi-periodic flow re
gimes. One of the bifurcations is related to an instability occurring
in a jet-like fluid layer exiting from those corners of the cavity whe
re the vertical boundary layers are turned horizontal. This instabilit
y is mainly shear-driven and the visualization of the perturbations sh
ows the occurrence of vorticity concentrations which are very similar
to Kelvin-Helmholtz vortices in a plane jet, suggesting that the insta
bility is a Kelvin-Helmholtz-type instability. The other bifurcation f
or Prandtl numbers between 0.25 and 2.0 occurs in the boundary layers
along the vertical walls. It differs however from the related instabil
ity in the natural-convection boundary layer along an isolated vertica
l plate: the instability in the cavity is shear-driven whereas the ins
tability along the vertical plate is mainly buoyancy-driven. For Prand
tl numbers between 2.5 and 7.0, it is found that there occurs an immed
iate transition from the steady to the chaotic flow regime without int
ermediate regimes. This transition is also caused by instabilities ori
ginating and concentrated in the vertical boundary layers.