2004MNRAS.354..971A


Query : 2004MNRAS.354..971A

2004MNRAS.354..971A - Mon. Not. R. Astron. Soc., 354, 971-979 (2004/November-2)

Capture and escape in the elliptic restricted three-body problem.

ASTAKHOV S.A. and FARRELLY D.

Abstract (from CDS):

Several families of irregular moons orbit the giant planets. These moons are thought to have been captured into planetocentric orbits after straying into a region in which the gravitation of the planet dominates solar perturbations (the Hill sphere). This mechanism requires a source of dissipation, such as gas drag, in order to make capture permanent. However, capture by gas drag requires that particles remain inside the Hill sphere long enough for dissipation to be effective. Recently we have proposed that in the circular restricted three-body problem (CRTBP) particles may become caught up in sticky chaotic layers, which tends to prolong their sojourn within the Hill sphere of the planet thereby assisting capture. Here, we show that this mechanism survives perturbations due to the ellipticity of the orbit of the planet. However, Monte Carlo simulations indicate that the ability of the planet to capture moons decreases with increasing orbital eccentricity. At the actual orbital eccentricity of Jupiter, this results in approximately an order of magnitude lower capture probability than estimated in the circular model. Eccentricities of planetary orbits in the Solar system are moderate but this is not necessarily the case for extrasolar planets, which typically have rather eccentric orbits. Therefore, our findings suggest that these extrasolar planets are unlikely to have substantial populations of irregular moons.

Abstract Copyright: 2004 RAS

Journal keyword(s): methods: {em N}-body simulations - celestial mechanics - planets and satellites: formation - planetary systems: formation

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 4203 PM* 00 44 41.2002505536 +20 26 56.138079876       8.2   G6V 154 1
2 * ups And b Pl 01 36 47.8415443907 +41 24 19.651368029           ~ 284 1
3 HD 33636 Pe* 05 11 46.4494089528 +04 24 12.742146936   7.59 6.98 6.6   G0V_CH-0.3 204 1
4 HD 50554 PM* 06 54 42.8261485848 +24 14 44.005690212   7.41 6.84     F8V 219 1
5 HD 73526 PM* 08 37 16.4833548528 -41 19 08.790456324   9.69 9.00     G6V 206 2
6 HD 74156b Pl 08 42 25.1219511432 +04 34 41.145751740           ~ 69 1
7 HD 75289 PM* 08 47 40.3893739728 -41 44 12.455319264 7.04 6.94 6.36     F9VFe+0.3 295 1
8 * rho01 Cnc b Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 267 1
9 HD 82943c Pl 09 34 50.7353072232 -12 07 46.369202196           ~ 88 1
10 HD 108147 PM* 12 25 46.2673666032 -64 01 19.516186956   7.532 6.994     F8/G0V 195 1
11 * tau Boo PM* 13 47 15.7381720026 +17 27 24.809555600 5.02 4.98 4.49 4.09 3.85 F7IV-V 1049 1
12 HD 142415 PM* 15 57 40.7919331560 -60 12 00.922058568   7.94 7.34     G1V 127 1
13 HD 147513 PM* 16 24 01.2911377368 -39 11 34.729913940 6.17 6.02 5.376     G5V 389 1
14 HD 168443b Pl 18 20 03.9332862096 -09 35 44.614653900           ~ 100 1
15 HD 169830c Pl 18 27 49.4849984976 -29 49 00.700831380           ~ 47 1
16 HD 169830 * 18 27 49.4849984976 -29 49 00.700831380   6.406 5.902 7.01   F7V 298 1
17 HD 179949 BY* 19 15 33.2300695008 -24 10 45.671448072   6.772 6.237     F8V 435 1
18 HD 187123 PM* 19 46 58.1122487784 +34 25 10.281404460       7.4   G2V 264 1
19 HD 190228 PM* 20 03 00.7726656864 +28 18 24.687065520   8.094 7.296     G5IV 185 1
20 HD 195019 PM* 20 28 18.6366815627 +18 46 10.180434472 7.730     6.5   G1V 276 1
21 HD 209452 * 22 01 02.2361532744 +66 04 56.927689968   8.38 8.28     B8 12 0
22 HD 210277 PM* 22 09 29.8657847411 -07 32 55.162082226   8.85 8.57 7.36   G8V 366 1
23 * 51 Peg PM* 22 57 27.9804852576 +20 46 07.797040104 6.39 6.16 5.46 4.97 4.61 G2IV 1216 1

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