Table A.2
Parameter values with conversion factors to the definition in the present study from the same studies as in Table A.1.
| Study | Pr | PrSGS | PrM | Pe | Re | ReM | Co | ||||||
|
|
|||||||||||||
| Present work | 18...72 | 0.25...5 | 0.5...5 | 4...134 | 17...134 | 5...151 | 1.4...15.9 | ||||||
|
|
|||||||||||||
| Nelson et al. (2013), (ASH) | ν/κr | ν/κ | ν/η | PrRe′/ (2π) | Re′/ (2π) | Rm′/ (2π) |
|
||||||
| Cases D3[a, b, pm1, pm2] |
|
0.25 | 0.5...2 | 4...11 | 16...43 | 8...22 | 4.5...5.5 | ||||||
|
|
|||||||||||||
| Nelson et al. (2013), | ν S /κ r | ν S /κ S | ν S /η S | PrRe′/ (2π) | Re′/ (2π) | Rm′/ (2π) |
|
||||||
| Case S3 |
|
0.25 | 0.5 | 229 | 915 | 458 | 5.8 | ||||||
|
|
|||||||||||||
| Ghizaru et al. (2010) | – | – | – | – | – | – | – | ||||||
| (EULAG) | ? | ≈ 1 | ≈ 1 | 5...10 | 5...10 | 5...10 | 30 | ||||||
|
|
|||||||||||||
| Hotta et al. (2016) | ν/κ r | ν/κ | ν/η | PrRe / (2π) | Re / (2π) | PmRe / (2π) | – | ||||||
| Low |
|
0.05 | 1 | 2.5 | 51 | 51 | 1.4 | ||||||
|
|
|||||||||||||
| Hotta et al. (2016) | ν SL/κ r | ν SL/κ | ν SL/η SL | PrRe / (2π) | Re / (2π) | PmRe / (2π) | – | ||||||
| Medium, High, High-S |
|
0.04...2 × 10-3 | 1.03...1.71 | 2.5 | 61...1129 | 63...1930 | 1.4 | ||||||
Notes. The values for Pe, Re, and ReM for the study of Ghizaru et al. (2010) are based on values stated in Passos & Charbonneau (2014) divided by 2π. The Coriolis numbers for the simulations of Ghizaru et al. (2010) and Hotta et al. (2016) were calculated using our definition, Eq. (22), and simulation data for the volume-averaged rms-value of velocity fluctuations provided by P. Charbonneau and H. Hotta, respectively. The Prandtl number Pr is not described in Ghizaru et al. (2010) and thus denoted by a question mark here. In the last row, νSL and ηSL are the viscosity and magnetic diffusivity estimated from the slope-limited diffusion scheme of Hotta et al. (2016; see text).
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