Cited by 106Astrophysics and Star Formation StudiesAstro and Planetary ScienceStellar, planetary, and galactic studies

Do Proto‐jovian Planets Drive Outflows?

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Quillen, A. C., Trilling, D. E.·1998·The Astrophysical Journal

Abstract

We discuss the possibility that gaseous giant planets drive strong outflows during early phases of their formation. We consider the range of parameters appropriate for magneto-centrifugally driven stellar and disk outflow models and find that, if the proto-Jovian planet or accretion disk had a magnetic field of ≳10 G and moderate mass-inflow accretion rates through the disk of less than ~10 -7 M J yr -1 , it is possible to drive an outflow. Estimates based both on scaling from empirical laws observed in protostellar outflows and the magneto-centrifugal disk and stellar plus disk wind models suggest that winds with mass-outflow rates of order 10 -8 M J yr -1 and velocities of order ~20 km s -1 could be driven from proto-Jovian planets. Prospects for detection and some implications for the formation of the solar system are briefly discussed.

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Crossref · 10.1086/306421

Cites

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  • Martin & Lubow (2011) suggest a tidal truncation limit of ξ ~0.4 and hydrodynamic simulations find ξ ~0.3.

    “Martin & Lubow (2011) suggest a tidal truncation limit of ξ ∼ 0 . 4 and hydrodynamic simulations of planets in circumstellar disks find ξ ∼ 0 . 3 (Quillen & Trilling 1998; Ayliffe & Bate 2009).”

    From Mass and period limits on the ringed companion transiting the young star J1407 (2015) · cites this paper as Quillen & Trilling 1998

    Section 1.3 (page unavailable) estimates a centrifugal radius of about one-third of the Hill radius for material entering through the Lagrange points, a flow pattern it says was seen in simulations. It does not report that hydrodynamic simulations measured a disk truncation limit of ξ ≈ 0.3. The ξ ≈ 0.4 statement is attributed to Martin & Lubow, not to this source. (LLM, conf=0.83)

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  • An important stability criterion for the disc is that it remains stable under gravitational interactions with the host star; to ensure an extended lifetime, R_disc < 0.3 R_Hill.

    “An important stability criterion for the disc is that the disc remains stable under the gravitational interactions with the host star. To ensure an extended lifetime of the disc, R disc &lt; 0 . 3 R Hill , where R Hill is the Hill radius defined by Equation 23 (Quillen &amp; Trilling 1998).”

    From Beyond Circular Eclipsers (BeyonCE) light curve modelling (2024) · cites this paper as Quillen & Trilling 1998

    Section 1.3 (page unavailable) calls the Hill radius a maximum radius for the proto-Jovian disk and estimates a centrifugal radius of about one-third of the Hill radius. It does not present R_disc < 0.3 R_Hill as a stability criterion or say that this limit ensures an extended disk lifetime; the one-third figure describes a centrifugal radius, not a required disk-size limit. (LLM, conf=0.88)

    Experimental — accuracy not yet measured
  • Estimates of the size ratio ξ for circumplanetary disks range from about 0.1 to about 0.4.

    “Based on a centripetal radius argument, Quillen & Trilling (1998) estimated that an accreting circumplanetary disk would have ξ = 1/3.Hydrodynamic simulations of planets embedded in circumstellar disks also can find ξ ∼ 0.3 (Ayliffe & Bate 2009).A tidal truncation argument suggests ξ ∼ 0.4 (Martin & Lubow 2011).Theoretical models for Jupiter's circumplanetary disk accounting for Galilean satellite”
  • Typical values of ξ are expected to be in the range 0.1 < ξ < 0.3.

    “Simulations indicate that ξ &gt; 0 . 4 are unlikely and that typical values are expected to be in the range of 0 . 1 &lt; ξ &lt; 0 . 3 (Quillen &amp; Trilling 1998; Canup &amp; Ward 2002; Magni &amp; Coradini 2004; Ayliffe &amp; Bate 2009; Ward &amp; Canup 2010).”

    From Mass and period limits on the ringed companion transiting the young star J1407 (2015) · cites this paper as Quillen & Trilling 1998

    Section 1.3 estimates a centrifugal radius of about one-third of the Hill radius, but does not identify that ratio as ξ or give typical values of 0.1–0.3. Section 2.3 discusses a different factor, f, for an X-wind model. Searches for ξ, the claimed range, and the simulation threshold found no passage establishing the claim in our copy; page numbers were unavailable. (LLM, conf=0.72)

    Experimental — accuracy not yet measured
  • Simulations indicate that ξ > 0.4 are unlikely.

    “Simulations indicate that ξ &gt; 0 . 4 are unlikely and that typical values are expected to be in the range of 0 . 1 &lt; ξ &lt; 0 . 3 (Quillen &amp; Trilling 1998; Canup &amp; Ward 2002; Magni &amp; Coradini 2004; Ayliffe &amp; Bate 2009; Ward &amp; Canup 2010).”

    From Mass and period limits on the ringed companion transiting the young star J1407 (2015) · cites this paper as Quillen & Trilling 1998

    Section 1.3 estimates a centrifugal radius of about one-third of the Hill radius under an assumed accretion path, but does not identify ξ or say simulations make values above 0.4 unlikely. Searches for ξ, the 0.4 threshold, and simulation-based limits found no passage in our copy establishing the attributed claim. (LLM, conf=0.72)

    Experimental — accuracy not yet measured

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Cites

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Research works printed but not linked: 9

  1. [13]13. A., Cerroni, P., Magni, G., & Federico, C. 1989, in Origin and Coradini, Evolution of Planetary and Satellite Atmospheres, ed. S. K. Atreya, J. B. Pollack, & M. S. Matthews (Tucson : University of Arizona Press), 723
  2. [32]32. G. P. 1951, in Astrophysics, ed. J. A. Hynek (New York : McGraw- Kuiper, Hill), 357
  3. [34]34. E. H., Ruzmaikin, A. A., & Ruzmaikina, T. V. 1991, in The Sun in Levy, Time, ed. C. P. Sonnett, M. S. Giampapa, & M. S. Mathews (Tucson : University of Arizona Press), 589
  4. [38]38. G., Spruit, H., & Levy, E. H. 1993, in Protostars and Planets III, MorÐll, ed. E. H. Levy & J. I. Lunine (Tucson : University of Arizona Press), 939
  5. [44]44. M., Hubbard, W. B., & Pollack, J. B. 1993, in Protostars and Podolak, Planets III, ed. E. H. Levy & J. I. Lunine (Tucson : University of Arizona Press), 1109
  6. [46]46. J. B., Lunine, J. I., & Tittemore, W. C. 1990, in Uranus, ed. J. T. Pollack, Bergstrahl, E. D. Miner, & M. S. Matthews (Tucson : University of Arizona Press), 469
  7. [47]47. R. G. 1993, in Protostars and Planets III, ed. E. H. Levy & J. I. Prinn, Lunine (Tucson : University of Arizona Press), 1005
  8. [62]62. D. J., Harris, A. W., & Lunine, J. I. 1986, in Satellites, ed. J. A. Stevenson, Burns & M. S. Matthews (Tucson : The University of Arizona Press), 39
  9. [66]66. S. J., & Cuzzi, J. N. 1993, in Protostars and Planets III, Weidenschilling, ed. E. H. Levy & J. I. Lunine (Tucson : University of Arizona Press), 1031

Cited by

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Authors
Quillen, A. C., & Trilling, D. E.
Affiliations
University of Arizona (US)
Venue
The Astrophysical Journal
Published
1998-12
Volume
508
Issue
2
Pages
707-713
ISSN
  • 0004-637X (ISSN-L)
  • 1538-4357
OpenAlex
W2046128110
Cited by
106
References
65
Citations by year
2026: 7 · 2025: 6 · 2024: 7 · 2023: 2 · 2022: 7 · 2021: 5 · 2020: 4 · 2019: 12 · 2018: 3 · 2017: 5 · 2016: 6 · 2015: 2 · 2014: 6 · 2013: 6 · 2012: 4
FWCI
0.54
Type
journal article
Language
en
Open access
Locations
  • The Astrophysical Journal (publishedVersion)
  • arXiv (Cornell University) (submittedVersion)
  • arXiv (Cornell University)
Funders
  • National Science Foundation (9529190)
  • National Aeronautics and Space Administration
Topics
  • Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Astrophysics and Star Formation Studies
  • Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Astro and Planetary Science
  • Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Stellar, planetary, and galactic studies
Keywords
magnetocentrifugal winds, accretion disks, protostellar outflows, magnetic field, disk accretion rate, planet formation, solar system formation

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