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Abstracts - KTH Mechanics

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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).

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