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The Stability of Multi-Planet Systems
A system of two small planets orbiting the Sun on low-eccentricity, low-inclination orbits is stable with respect to close encounters if the initial semi-major axis difference, Δ, measured in mutual Hill radii,RH, exceeds[formula], due to conservation of energy and angular momentum. We investigate t...
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Published in: | Icarus (New York, N.Y. 1962) N.Y. 1962), 1996-02, Vol.119 (2), p.261-268 |
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Language: | English |
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container_end_page | 268 |
container_issue | 2 |
container_start_page | 261 |
container_title | Icarus (New York, N.Y. 1962) |
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creator | Chambers, J.E. Wetherill, G.W. Boss, A.P. |
description | A system of two small planets orbiting the Sun on low-eccentricity, low-inclination orbits is stable with respect to close encounters if the initial semi-major axis difference, Δ, measured in mutual Hill radii,RH, exceeds[formula], due to conservation of energy and angular momentum. We investigate the stability of systems of more than two planets using numerical integrations. We find that systems with Δ < 10 are always unstable, with the time,t, of first close encounter given approximately by logt=bΔ +c, wherebandcare constants. It is likely that systems with Δ > 10 are also unstable. The slopebdepends weakly on the number of planets, but is independent of planetary mass,m, if we measure Δ in units that are proportional tom1/4rather than the usualRH∝m1/3. Instability in multi-planet systems arises because energy and angular momentum are no longer conserved within each two-planet subsystem due to perturbations by the additional planet(s). These results suggest that planetary embryos will not become isolated prior to the final stage of terrestrial-planet formation simply due to a failure to achieve close encounters. Other factors leading to isolation cannot be ruled out at this stage. |
doi_str_mv | 10.1006/icar.1996.0019 |
format | article |
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We investigate the stability of systems of more than two planets using numerical integrations. We find that systems with Δ < 10 are always unstable, with the time,t, of first close encounter given approximately by logt=bΔ +c, wherebandcare constants. It is likely that systems with Δ > 10 are also unstable. The slopebdepends weakly on the number of planets, but is independent of planetary mass,m, if we measure Δ in units that are proportional tom1/4rather than the usualRH∝m1/3. Instability in multi-planet systems arises because energy and angular momentum are no longer conserved within each two-planet subsystem due to perturbations by the additional planet(s). These results suggest that planetary embryos will not become isolated prior to the final stage of terrestrial-planet formation simply due to a failure to achieve close encounters. 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We investigate the stability of systems of more than two planets using numerical integrations. We find that systems with Δ < 10 are always unstable, with the time,t, of first close encounter given approximately by logt=bΔ +c, wherebandcare constants. It is likely that systems with Δ > 10 are also unstable. The slopebdepends weakly on the number of planets, but is independent of planetary mass,m, if we measure Δ in units that are proportional tom1/4rather than the usualRH∝m1/3. Instability in multi-planet systems arises because energy and angular momentum are no longer conserved within each two-planet subsystem due to perturbations by the additional planet(s). These results suggest that planetary embryos will not become isolated prior to the final stage of terrestrial-planet formation simply due to a failure to achieve close encounters. 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title | The Stability of Multi-Planet Systems |
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