Table C.1.
Frequencies and non-toroidicity of the n = 0 equatorial Rossby modes under uniform rotation.
| m | Compressible | Compr. - | Compr. - | Γ |
|---|---|---|---|---|
| ω/2π (nHz) | Anelastic | Boussinesq | ||
| 1 | −455.9944 | 0.0056 | 0.0056 | 0.0000 |
| 2 | −303.9977 | 0.0018 | 0.0020 | 0.0009 |
| 3 | −227.9918 | 0.0008 | 0.0023 | 0.0019 |
| 4 | −182.3657 | 0.0004 | 0.0061 | 0.0031 |
| 5 | −151.9042 | 0.0002 | 0.0175 | 0.0045 |
| 6 | −130.0859 | 0.0001 | 0.0388 | 0.0060 |
| 7 | −113.6626 | 0.0001 | 0.0661 | 0.0076 |
| 8 | −100.8461 | 0.0001 | 0.0907 | 0.0090 |
| 9 | −90.5729 | 0.0001 | 0.1043 | 0.0103 |
| 10 | −82.1683 | 0.0000 | 0.1026 | 0.0113 |
| 11 | −75.1793 | 0.0000 | 0.0855 | 0.0120 |
| 12 | −69.2873 | 0.0000 | 0.0562 | 0.0125 |
| 13 | −64.2603 | 0.0000 | 0.0198 | 0.0127 |
| 14 | −59.9249 | 0.0000 | −0.0192 | 0.0128 |
| 15 | −56.1494 | 0.0000 | −0.0569 | 0.0127 |
| 16 | −52.8323 | 0.0000 | −0.0911 | 0.0125 |
Notes. The first column denotes the azimuthal order m. The second column reports the frequency (ω) of the modes in the Carrington frame as computed using the compressible model. The third and fourth columns report the differences in the frequencies (in nHz) for the anelastic and the Boussinesq models, respectively, relative to the compressible model. The fifth column denotes the non-toroidicity Γ as computed for the modes from the compressible model using Eq. (22).
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