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| Combination |  | Ai |  | ||||
|  |  | g1 | g2 |  | (deg/yr) | (deg) | (deg) | 
| 0 | 0 | 0 | 0 | 1 | 19.8207 | 68.444 | -144.426 | 
| 0 | 0 | -1 | 1 | 0 | 0.8698 | 13.400 | 136.931 | 
| 0 | 0 | 1 | -1 | 1 | 18.9509 | 8.606 | 168.643 | 
| 0 | 0 | -1 | 1 | 1 | 20.6905 | 8.094 | 82.505 | 
| 0 | 0 | -2 | 2 | 0 | 1.7396 | 2.165 | -176.138 | 
| 0 | 0 | -2 | 2 | 1 | 21.5603 | 0.622 | -50.564 | 
| 0 | 0 | 0 | 0 | 3 | 59.4621 | 0.540 | -73.279 | 
| 1 | -1 | 0 | 0 | -1 | 172.5756 | 0.506 | 7.504 | 
| 1 | -1 | 0 | 0 | 0 | 192.3963 | 0.501 | -46.923 | 
| 0 | 0 | -3 | 3 | 0 | 2.6093 | 0.416 | -129.207 | 
| 0 | 0 | 2 | -2 | 1 | 18.0811 | 0.420 | 121.712 | 
| 1 | -1 | 0 | 0 | 1 | 212.2170 | 0.416 | 78.651 | 
| 0 | 1 | -1 | 0 | 0 | 384.7926 | 0.451 | 176.155 | 
| 1 | -1 | 0 | 0 | -2 | 152.7549 | 0.424 | -118.070 | 
| 0 | 1 | -1 | 0 | -1 | 364.9719 | 0.341 | 50.581 | 
| 0 | 1 | -1 | 0 | 1 | 404.6133 | 0.274 | 121.729 | 
| 0 | 0 | 1 | -1 | 3 | 58.5923 | 0.212 | -120.210 | 
| 1 | -1 | 0 | 0 | 2 | 232.0377 | 0.201 | 24.225 | 
| 0 | 0 | -1 | 1 | 3 | 60.3319 | 0.211 | 153.652 | 
| 1 | 0 | -1 | 0 | -1 | 557.3682 | 0.182 | -86.342 | 
| We have  ,
where   the amplitude and phases Ai,  are given in degree, and the   frequencies  in degree/year. We only give the first 20 terms, ordered by  decreasing amplitude. All terms are identified as  integer combinations   of the fundamental frequencies given in   Table 3. The fact that we are able to express all the main frequencies of  in terms of exact combinations of the fundamental frequencies g1, g2 and  is a signature of a very regular motion. | 
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  for an integration  over 100 kyr of the orbital solution in
  Table
for an integration  over 100 kyr of the orbital solution in
  Table