Table A.4.
Number of volume elements per colatitude for Nθ = 20.
| Parl | θ | Num | Parl | θ | Num |
|---|---|---|---|---|---|
| 1 | 7.179 | 80 | 11 | 50.769 | 155 |
| 2 | 11.538 | 80 | 12 | 55.128 | 164 |
| 3 | 15.897 | 80 | 13 | 59.487 | 172 |
| 4 | 20.256 | 80 | 14 | 63.846 | 180 |
| 5 | 24.615 | 83 | 15 | 68.205 | 186 |
| 6 | 28.974 | 97 | 16 | 72.564 | 191 |
| 7 | 33.333 | 110 | 17 | 76.923 | 195 |
| 8 | 37.692 | 122 | 18 | 81.282 | 198 |
| 9 | 42.051 | 134 | 19 | 85.641 | 199 |
| 10 | 46.410 | 145 | 20 | 90.000 | 200 |
Notes. Columns 1 and 4: the identifying number of the parallel, with 20 corresponding to the equator; Cols. 2 and 5: value of the corresponding colatitude midpoint in degrees; Cols. 3 and 6: number of elements in the corresponding parallel. Calculation was performed for colatitudes in the range 5−90°. The total number of volume elements for all layers in a Nr = 10 run is 28510 (one hemisphere) and this is the number of equations of motion that are solved simultaneously with the orbital motion.
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