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Table 2.
Variables and distributions used for the Monte Carlo analysis.
Parameter | Variable type | Mean value ±1σ; [bounds] | Note and source |
---|---|---|---|
Final mutual orbit period [h] | Fixed | 52.67 | Mottola et al. (2023) |
Eccentricity | Fixed | 0 | Levison et al. (2024) |
Diameter of Dinkinesh [m] | Gaussian | 719 ± 24 | Levison et al. (2024) |
Diameter of Selam [m] | Gaussian | 282 ± 28 | Levison et al. (2024) |
aeq [m] | Gaussian | 3110 ± 50 | Levison et al. (2024) |
k/Q | Log-Uniform | 10−x; x ∈ (3, 5) | x is uniformly distributed |
Coefficient for YORP | Gaussian | 0 ± 0.0125 ; [−2, Eq. (14)] | Rossi et al. (2009) |
Coefficient for BYORP | Derived | Eq. (11) | Contractive BYORP only |
Density [kg m−3] | Derived | ![]() |
– |
Initial primary spin [rad s−1] | Derived | Eq. (15) | Angular momentum conservation |
Initial semi-major axis [m] | Uniform | (1.5Rp, 2.5Rp) | Roche limit |
Notes. The diameters of Dinkinesh and Selam are volume-equivalent sphere diameters. In the density equation, P is the mutual orbital period.
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