Table 1.
Example of a configuration and the main output data obtained with a prolate core and an oblate envelope.
| Config. A | DROP | Full NSFoE | First-order |
|---|---|---|---|
| ε12 | −0.00979 | ← − 0.01 | ← − 0.01 |
| ε22 | ←0.01 | ←0.01 | ←0.01 |
| q | 0.70007 | ←0.70 | ←0.70 |
| α | ←1.25 | ←1.25 | ←1.25 |
| −c | 1.685 × 10−2 | 1.700 × 10−2 | 1.700 × 10−2 |
| ε2, lim2 | 7.439 × 10−3 | ||
| qlim | −1.00000 | ||
| b1/a2 | ←NSFoE | 0.70349 | 0.70349 |
 |
4.585 × 10−4 | 4.596 × 10−4 | 4.585 × 10−4 |
 |
3.411 × 10−3 | 3.420 × 10−3 | 3.406 × 10−3 |
| Δ | ←NSFoE | 3.666 × 10−1 | 3.669 × 10−1 |
| M/(ρ2a23) | 4.52913 | 4.52877 | 4.52883 |
| pc/(πGρ22a22) | 8.963 × 10−1 | 8.963 × 10−1 | 8.962 × 10−1 |
| |VP/W| | 7 × 10−7 | 4 × 10−6 | 3 × 10−3 |
Notes. pc is the central pressure and M is the mass; ‘←’ indicates input data. The second column contains the results from the numerical solution obtained with the DROP code (Basillais & Huré 2021). The third column contains the results from the full NSFoE theory (Huré 2022) and the fourth the results obtained with the first-order approximation of ε2 used in this work.
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