2016
DOI: 10.1051/0004-6361/201628828
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Planet formation with envelope enrichment: new insights on planetary diversity

Abstract: Aims. We compute, for the first time, self-consistent models of planet growth including the effect of envelope enrichment. The change of envelope metallicity is assumed to be the result of planetesimal disruption or icy pebble sublimation. Methods. We solve internal structure equations taking into account global energy conservation for the envelope to compute in-situ planetary growth. We consider different opacities and equations of state suited for a wide range of metallicities. Results. We find that envelope… Show more

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Cited by 128 publications
(162 citation statements)
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References 51 publications
(113 reference statements)
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“…First works have recently started to study the compositional aspect (Venturini et al 2016;Lozovsky et al 2017), but they do not yet address the consequences for the luminosity. Because of this, it is currently also not clear if, for the core-mass effect to work efficiently, a high total heavy element content today (in the envelope and/or core) is sufficient as implicitly assumed in the argument above.…”
Section: Uncertainties Related To the Core-mass Effectmentioning
confidence: 99%
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“…First works have recently started to study the compositional aspect (Venturini et al 2016;Lozovsky et al 2017), but they do not yet address the consequences for the luminosity. Because of this, it is currently also not clear if, for the core-mass effect to work efficiently, a high total heavy element content today (in the envelope and/or core) is sufficient as implicitly assumed in the argument above.…”
Section: Uncertainties Related To the Core-mass Effectmentioning
confidence: 99%
“…This would then naturally also reduce its impact on L pf . This should be quantified with future work treating self-consistently the thermodynamics and compositional evolution during formation (e.g., Venturini et al 2016). …”
Section: Post-formation Luminosities L Pfmentioning
confidence: 99%
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“…In Model-1, crossover is reached after 0.94 Myr, when M Z =16 M ⊕ , while for Model-2, crossover time is 1.54 Myr and M Z =7.5 M ⊕ . Crossover time is calculated assuming that all the accreted planetesimals reach the core, while the deposition of heavies into the envelope is expected to decrease the time by a factor of a few (Venturini et al 2016). Figure 1 shows Z(m) versus time for the two models up to crossover time.…”
Section: Jupiter's Primordial Internal Structurementioning
confidence: 99%