The fragility of the terrestrial planets during a giant-planet instability
Many features of the outer Solar system are replicated in numerical simulations if the giant planets undergo an orbital instability that ejects one or more ice giants. During this instability, Jupiter and Saturn's orbits diverge, crossing their 2:1 mean motion resonance (MMR), and this resonanc...
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Veröffentlicht in: | Monthly notices of the Royal Astronomical Society 2016-02, Vol.455 (4), p.3561-3569 |
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description | Many features of the outer Solar system are replicated in numerical simulations if the giant planets undergo an orbital instability that ejects one or more ice giants. During this instability, Jupiter and Saturn's orbits diverge, crossing their 2:1 mean motion resonance (MMR), and this resonance-crossing can excite the terrestrial planet orbits. Using a large ensemble of simulations of this giant-planet instability, we directly model the evolution of the terrestrial planet orbits during this process, paying special attention to systems that reproduce the basic features of the outer planets. In systems that retain four giant planets and finish with Jupiter and Saturn beyond their 2:1 MMR, we find at least an 85 per cent probability that at least one terrestrial planet is lost. Moreover, systems that manage to retain all four terrestrial planets often finish with terrestrial planet eccentricities and inclinations larger than the observed ones. There is less than a ∼5 per cent chance that the terrestrial planet orbits will have a level of excitation comparable to the observed orbits. If we factor in the probability that the outer planetary orbits are well replicated, we find a probability of 1 per cent or less that the orbital architectures of the inner and outer planets are simultaneously reproduced in the same system. These small probabilities raise the prospect that the giant-planet instability occurred before the terrestrial planets had formed. This scenario implies that the giant-planet instability is not the source of the Late Heavy Bombardment and that terrestrial planet formation finished with the giant planets in their modern configuration. |
doi_str_mv | 10.1093/mnras/stv2554 |
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During this instability, Jupiter and Saturn's orbits diverge, crossing their 2:1 mean motion resonance (MMR), and this resonance-crossing can excite the terrestrial planet orbits. Using a large ensemble of simulations of this giant-planet instability, we directly model the evolution of the terrestrial planet orbits during this process, paying special attention to systems that reproduce the basic features of the outer planets. In systems that retain four giant planets and finish with Jupiter and Saturn beyond their 2:1 MMR, we find at least an 85 per cent probability that at least one terrestrial planet is lost. Moreover, systems that manage to retain all four terrestrial planets often finish with terrestrial planet eccentricities and inclinations larger than the observed ones. There is less than a ∼5 per cent chance that the terrestrial planet orbits will have a level of excitation comparable to the observed orbits. If we factor in the probability that the outer planetary orbits are well replicated, we find a probability of 1 per cent or less that the orbital architectures of the inner and outer planets are simultaneously reproduced in the same system. These small probabilities raise the prospect that the giant-planet instability occurred before the terrestrial planets had formed. 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If we factor in the probability that the outer planetary orbits are well replicated, we find a probability of 1 per cent or less that the orbital architectures of the inner and outer planets are simultaneously reproduced in the same system. These small probabilities raise the prospect that the giant-planet instability occurred before the terrestrial planets had formed. This scenario implies that the giant-planet instability is not the source of the Late Heavy Bombardment and that terrestrial planet formation finished with the giant planets in their modern configuration.</description><subject>Astronomy</subject><subject>Computer simulation</subject><subject>Extrasolar planets</subject><subject>Finishes</subject><subject>Instability</subject><subject>Orbitals</subject><subject>Orbits</subject><subject>Planet formation</subject><subject>Simulation</subject><subject>Stability</subject><subject>Star & galaxy formation</subject><subject>Terrestrial planets</subject><issn>0035-8711</issn><issn>1365-2966</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqNkc1LAzEQxYMoWKtH7wEvXtZOks3XUYqfFLzU85LtZmvKdndNskL_e9NuQfCip4HHbx5v5iF0TeCOgGazbetNmIX4RTnPT9CEMMEzqoU4RRMAxjMlCTlHFyFsACBnVEzQ6_LD4tqbtWtc3OGuxjEJ0XpvQ_TONLhvTGtjwNXgXbvGBq-daWM2yti1IZrysHyJzmrTBHt1nFP0_viwnD9ni7enl_n9IlvlQseMqkpXXCpTakWVlrlhhHFhATi16QyuoZZgONW0NGXO2F6BShEjK0poyabodvTtffc5pJjF1oWVbfaBuiEURCpBhAQl_4EKmuzTuxJ68wvddINv0yGJ4hI4KK4SlY3UyncheFsXvXdb43cFgWJfQnEooTiW8BOgG_o_0G_oHIfj</recordid><startdate>20160201</startdate><enddate>20160201</enddate><creator>Kaib, Nathan A.</creator><creator>Chambers, John E.</creator><general>Oxford University Press</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7TG</scope><scope>KL.</scope></search><sort><creationdate>20160201</creationdate><title>The fragility of the terrestrial planets during a giant-planet instability</title><author>Kaib, Nathan A. ; Chambers, John E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c469t-28d9d578ab9828974a31356e0052e093590f70a5292bab43335900d81a7d212b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Astronomy</topic><topic>Computer simulation</topic><topic>Extrasolar planets</topic><topic>Finishes</topic><topic>Instability</topic><topic>Orbitals</topic><topic>Orbits</topic><topic>Planet formation</topic><topic>Simulation</topic><topic>Stability</topic><topic>Star & galaxy formation</topic><topic>Terrestrial planets</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kaib, Nathan A.</creatorcontrib><creatorcontrib>Chambers, John E.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><jtitle>Monthly notices of the Royal Astronomical Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Kaib, Nathan A.</au><au>Chambers, John E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The fragility of the terrestrial planets during a giant-planet instability</atitle><jtitle>Monthly notices of the Royal Astronomical Society</jtitle><date>2016-02-01</date><risdate>2016</risdate><volume>455</volume><issue>4</issue><spage>3561</spage><epage>3569</epage><pages>3561-3569</pages><issn>0035-8711</issn><eissn>1365-2966</eissn><abstract>Many features of the outer Solar system are replicated in numerical simulations if the giant planets undergo an orbital instability that ejects one or more ice giants. During this instability, Jupiter and Saturn's orbits diverge, crossing their 2:1 mean motion resonance (MMR), and this resonance-crossing can excite the terrestrial planet orbits. Using a large ensemble of simulations of this giant-planet instability, we directly model the evolution of the terrestrial planet orbits during this process, paying special attention to systems that reproduce the basic features of the outer planets. In systems that retain four giant planets and finish with Jupiter and Saturn beyond their 2:1 MMR, we find at least an 85 per cent probability that at least one terrestrial planet is lost. Moreover, systems that manage to retain all four terrestrial planets often finish with terrestrial planet eccentricities and inclinations larger than the observed ones. There is less than a ∼5 per cent chance that the terrestrial planet orbits will have a level of excitation comparable to the observed orbits. If we factor in the probability that the outer planetary orbits are well replicated, we find a probability of 1 per cent or less that the orbital architectures of the inner and outer planets are simultaneously reproduced in the same system. These small probabilities raise the prospect that the giant-planet instability occurred before the terrestrial planets had formed. This scenario implies that the giant-planet instability is not the source of the Late Heavy Bombardment and that terrestrial planet formation finished with the giant planets in their modern configuration.</abstract><cop>London</cop><pub>Oxford University Press</pub><doi>10.1093/mnras/stv2554</doi><tpages>9</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Astronomy Computer simulation Extrasolar planets Finishes Instability Orbitals Orbits Planet formation Simulation Stability Star & galaxy formation Terrestrial planets |
title | The fragility of the terrestrial planets during a giant-planet instability |
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