Table 5.
Time-averaged, dimensionless, turbulent stresses for cases without irradiation: sg-mhd-noirrad-10 (τcΩ0 = 10, first line) and sg-mhd-noirrad-20, (τcΩ0 = 20, second line).
| αr | αg | αm | α | rsp | |
|---|---|---|---|---|---|
| sg-mhd- | |||||
| noirrad-20 | 0.0065 | 0.0072 | 0.0102 | 0.0239 | 0.3231 |
| SGMRI-20 | 0.0056 | 0.012 | 0.0028 | 0.020 | 0.28 |
| sg-mhd- | |||||
| noirrad-10 | 0.0126 | 0.0197 | 0.0111 | 0.0434 | 0.3578 |
| SGMRI-10 | 0.011 | 0.017 | 0.012 | 0.04 | 0.34 |
Notes. In both cases, the time average starts at tΩ0 = 1100 and covers an interval of 
. The corresponding cases in Riols & Latter (2018a), SGMRI-10 and SGMRI-20, are shown in the second and fourth lines, respectively. The magnetic stress-to-pressure ratio is rsp = ⟨⟨−BxBy⟩/⟨B2/2⟩⟩t.
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