Table 4.
Change in the orbital elements.
| Model | ȧ/a | (ȧ/a)DK16 | ė/e | (ė/e)DK16 | (ė/e)tides |
|---|---|---|---|---|---|
| – | yr−1 | yr−1 | yr−1 | yr−1 | yr−1 |
| Q2e0 | −8.43 × 10−7 | 5.20 × 10−6 | – | – | – |
| Q2e02 | 8.28 × 10−7 | 5.77 × 10−6 | −1.18 × 10−6 | −2.40 × 10−6 | −1.10 × 10−4 |
| Q2e04 | 2.77 × 10−6 | 6.22 × 10−6 | −9.58 × 10−7 | −1.53 × 10−6 | −1.91 × 10−5 |
| Q2e06 | 4.56 × 10−6 | 6.49 × 10−6 | −5.37 × 10−7 | −8.67 × 10−7 | −4.41 × 10−6 |
| Q2e08 | 6.15 × 10−6 | 6.81 × 10−6 | −2.16 × 10−7 | −3.33 × 10−7 | −9.22 × 10−7 |
| Q2e06v1 | −1.58 × 10−6 | 4.15 × 10−6 | −1.66 × 10−6 | −1.97 × 10−6 | −4.41 × 10−6 |
| MMe05 | −6.88 × 10−6 | −3.18 × 10−6 | 6.41 × 10−6 | −3.91 × 10−6 | −5.10 × 10−6 |
Notes. ȧ/a and ė/e correspond to the changes in semi-major axis and eccentricity, respectively, as measured dynamically from the simulations. The values of ȧ/a and ė/e with the subscript DK16 correspond to the analytical values for these quantities as derived from Eqs. (81) and (82) in Dosopoulou & Kalogera (2016). (ė/e)tides is the expected change in the eccentricity due to tidal interaction, as derived from Eq. (12).
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