Table 1
Parameters used in the experiments discussed here.
| Experiment | b (cm) | η | Γ | max(Re1) | max(Re2) | min(RΩ) | max(RΩ) |
|
|
|||||||
| Wendt (1933) | 14.7 | 0.68 | 10.64 | 8.47 × 104 | 1.24 × 105 | –0.71 | 0.47 |
| Wendt (1933) | 14.7 | 0.85 | 22.93 | 4.95 × 104 | 5.83 × 104 | –0.80 | 0.18 |
| Wendt (1933) | 14.7 | 0.935 | 52.63 | 2.35 × 104 | 2.52 × 104 | –0.42 | 0.11 |
| Taylor (1936) | 4.055 | 0.79–0.973 | 100–768 | 0 | 1.08 × 105 | 0.03 | 0.27 |
| Richard (2001) | 5.00 | 0.72 | 27.18 | 9.50 × 104 | 1.30 × 105 | –1.43 | –0.94 |
| Richard (2001) | 5.00 | 0.72 | 27.18 | 9.50 × 104 | 1.30 × 105 | 0.38 | 0.58 |
| Ji et al. (2006) | 20.3 | 0.35 | 2.1 | 1.20 × 106 | 4.50 × 105 | –1.67 | –1.08 |
| Maryland | 22.09 | 0.725 | 11.47 | 3.70 × 106 | 1.50 × 106 | –2.04 | 1.46 |
| Twente | 27.9 | 0.716 | 11.68 | 2.00 × 106 | 1.40 × 106 | –0.74 | 0.17 |
Notes. The geometry of each apparatus is given by the outer cylinder radius b, the radius ratio η = a/b and the aspect ratio Γ = L/(b − a). The range of turbulence intensities are governed by the inner and outer cylinder Reynolds numbers Re1 and Re2. The effects of rotation are parameterized by the rotation number RΩ introduced by Dubrulle et al. (2005).
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