2001
DOI: 10.1016/s0017-9310(00)00219-2
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On the transition from conduction to convection regime in a cubical enclosure with a partially heated wall

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Cited by 48 publications
(47 citation statements)
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“…The results in steady-state regime obtained in the present study are close to those of Frederick et al [22] who looked at the case of a discrete isothermal square source, with a side s, disposed on the vertical wall of a right cavity (a = 0°), the rest of the plate being adiabatic as well as the channel of the enclosure. The cold wall is facing the hot one as in the cavity under consideration here.…”
Section: Convective Exchangesupporting
confidence: 89%
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“…The results in steady-state regime obtained in the present study are close to those of Frederick et al [22] who looked at the case of a discrete isothermal square source, with a side s, disposed on the vertical wall of a right cavity (a = 0°), the rest of the plate being adiabatic as well as the channel of the enclosure. The cold wall is facing the hot one as in the cavity under consideration here.…”
Section: Convective Exchangesupporting
confidence: 89%
“…Its extrapolation to Ra = 1.07 Â 10 7 leads to Nu ¼ 14:12. The difference with the values of the present study is 6.2%, which reduces further if the results in [22] are extrapolated for values of s/H > 0.7 that are closer to our values. With a still equals 0, the comparison is now conducted with the work of Tou et al [23], which considers a geometry close to the one treated in the present study but with 3 Â 3 active elements on the hot wall.…”
Section: Convective Exchangecontrasting
confidence: 70%
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“…This has been observed in other studies for particular thermal and geometric configurations. Frederick et al [26] showed for example that 3D effects can significantly influence the flows since, for some combinations, the peak value of the w component can exceed the 61% of the peak value of u and more than a 37% of the peak value of the v component.…”
Section: Velocity and Thermal Mapsmentioning
confidence: 99%