Le cluster Rayleigh number - Turbulent convection
000037 (2012) | Xiaozhou He [Allemagne] ; Denis Funfschilling [France] ; Eberhard Bodenschatz [Allemagne, États-Unis] ; Guenter Ahlers [Allemagne, États-Unis] | Heat transport by turbulent RayleighBnard convection for Pr0.8 and 41011Ra21014: ultimate-state transition for aspect ratio 1.00 |
000038 (2012) | Guenter Ahlers [États-Unis] ; Xiaozhou He [Allemagne] ; Denis Funfschilling [France] ; Eberhard Bodenschatz [Allemagne, États-Unis] | Heat transport by turbulent RayleighBnard convection for Pr0.8 and 31012Ra1015: aspect ratio 0.50 |
000057 (2009) | Guenter Ahlers [États-Unis] ; Denis Funfschilling [France] ; Eberhard Bodenschatz [Allemagne, États-Unis] | Transitions in heat transport by turbulent convection at Rayleigh numbers up to 1015 |
000045 (2011) | Guenter Ahlers [États-Unis] ; Denis Funfschilling [France] ; Eberhard Bodenschatz [Allemagne, États-Unis] | Heat transport in turbulent Rayleigh-Bénard convection for Pr ≃ 0.8 and Ra ≲ 10 |
000116 (2000) | Bernhard Reiser [Allemagne] | Real processing III. The generalized statement of Helmholtz and Rayleigh and its meaning for process engineering |
000056 (2009) | Guenter Ahlers [États-Unis] ; Eberhard Bodenschatz [Allemagne] ; Denis Funfschilling [France] ; James Hogg [États-Unis] | Turbulent Rayleigh–Bénard convection for a Prandtl number of 0.67 |
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