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106<br />
Turbulent thermal convection over grooved surfaces: effect of<br />
the finite thermal conductivity of the plates.<br />
G.Stringano ∗ , G.Pascazio ∗ and R.Verzicco ∗<br />
The effects of the finite thermal conductivity of the plates in turbulent thermal<br />
convection over grooved surfaces are investigated by direct numerical simulations of<br />
the Navier-Stokes equations with the Boussinesq approximation. The simulations are<br />
performed in a cylindrical cell of aspect ratio, diameter over cell height, Γ = 1/2 at<br />
Prandtl number Pr =0.7. The cell is heated from below and cooled from above<br />
with an adiabatic sidewall. The plate geometry presents five axisymmetric V shaped<br />
grooves with the height of the tip over height of the cell, H/h =0.025 and vertex<br />
angle equal to 90 o . The presence of grooves forces the formation of plumes over<br />
the tips, with a dynamics very similar to the ’wedge effect’ in electrical problems 1<br />
2 . This effect, combined with a finite thermal conductivity of the plates, leads to a<br />
non isothermal fluid–plate interface and therefore to weaker wall normal temperature<br />
gradients thus reducing the overall heat flux. A comparison with ideal plates with<br />
infinite thermal conductivity, shows a decrease of the heat transfer, when the ratio<br />
between plates and fluid thermal resistance is smaller than a threshold value. This<br />
behaviour can be explained in terms of thermal energy balance: if the plates thermal<br />
conductivity is too low, the supplied heat flux can not balance the heat taken away<br />
by thermal plumes and the plate cools down below a developing plume. The different<br />
balance between the heat needed by an ascending plume and that supplied by the<br />
plate can alter the plume dynamics and consequently modify the heat transfer. Since<br />
regardless of the particular shape every non flat surface will have cusps and throats<br />
the main conclusion is that the tips of the rough elements represent a critical region<br />
for heat transfer. A detailed analysis of the plume dynamics and their role in the heat<br />
transfer will be presented at the conference.<br />
∗DIMeG & CEMEC Politecnico di Bari, Via Redavid 200, 70125 Bari, Italy.<br />
1G.Stringano, G.Pascazio and R.Verzicco, Turbulent thermal convection over grooved plates, J.<br />
Fluid Mech. 2005 in press.<br />
2Y.-B.Du and P.Tong, Turbulent thermal convection in a cell with ordered rough boundaries, J.<br />
Fluid Mech. 2000, vol. 407, pp 57-84.<br />
Figure 1: Temperature field at Ra =2· 10 10 and Pr =0.7 (closeup of the hot plate).