Table 2
Summary of the runs in Cartesian coordinates.
Run | Latitude | Re | Co | Ma |
![]() |
Emer/Ek | Erot/Ek |
|
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cA0 | – | 63 | 0.00 | 0.038 | 1.7 × 10-4 | 0.052 | 0.001 |
cF0 | – | 28 | 0.00 | 0.027 | 2.3 × 10-4 | 0.021 | 0.001 |
cF1 | – | 11 | 0.00 | 0.022 | 2.5 × 10-4 | 0.002 | 0.000 |
|
|||||||
cA1 | 0° | 64 | 0.85 | 0.039 | 2.9 × 10-4 | 0.001 | 0.288 |
cA2 | 7° | 65 | 0.84 | 0.039 | 2.0 × 10-4 | 0.021 | 0.017 |
cA3 | 14° | 65 | 0.84 | 0.039 | 1.8 × 10-4 | 0.014 | 0.007 |
cA4 | 21° | 65 | 0.85 | 0.039 | 1.8 × 10-4 | 0.012 | 0.008 |
|
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cB1 | 0° | 61 | 1.49 | 0.037 | 4.5 × 10-4 | 0.000 | 0.623 |
cB2 | 7° | 70 | 1.30 | 0.042 | 2.4 × 10-4 | 0.023 | 0.012 |
cB3 | 14° | 68 | 1.33 | 0.041 | 2.0 × 10-4 | 0.012 | 0.007 |
cB4 | 21° | 68 | 1.34 | 0.041 | 1.9 × 10-4 | 0.005 | 0.009 |
|
|||||||
cC1 | 0° | 60 | 2.14 | 0.036 | 2.8 × 10-4 | 0.000 | 0.347 |
cC2 | 7° | 76 | 1.68 | 0.046 | 2.5 × 10-4 | 0.029 | 0.031 |
cC3 | 14° | 72 | 1.77 | 0.044 | 2.2 × 10-4 | 0.013 | 0.011 |
cC4 | 21° | 72 | 1.78 | 0.043 | 2.1 × 10-4 | 0.004 | 0.011 |
|
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cD1 | 0° | 69 | 2.38 | 0.042 | 7.5 × 10-4 | 0.000 | 0.584 |
cD2 | 7° | 78 | 2.09 | 0.047 | 2.5 × 10-4 | 0.029 | 0.018 |
cD3 | 14° | 47 | 2.32 | 0.043 | 2.0 × 10-4 | 0.009 | 0.013 |
cD4 | 21° | 70 | 2.36 | 0.042 | 2.1 × 10-4 | 0.003 | 0.005 |
|
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cE1 | 0° | 50 | 3.66 | 0.045 | 1.2 × 10-3 | 0.000 | 0.685 |
cE2 | 7° | 36 | 4.00 | 0.041 | 1.6 × 10-4 | 0.025 | 0.009 |
cE3 | 14° | 34 | 4.24 | 0.039 | 1.5 × 10-4 | 0.005 | 0.005 |
cE4 | 21° | 31 | 4.67 | 0.035 | 1.3 × 10-4 | 0.001 | 0.008 |
Notes. Here, we use a resolution of 64 × 1282 grid points. For the sets of Runs cA–cD, Ra ≈ 3.1 × 106, and for the set of Runs cE, Ra ≈ 1.4 × 106. Thermal energy in all of the cases is . All quantities are computed using the same definitions and normalization factors as in Table 1.
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