2016A&A...591A.100F


Query : 2016A&A...591A.100F

2016A&A...591A.100F - Astronomy and Astrophysics, volume 591A100-100 (2016/7-1)

Formation of H2-He substellar bodies in cold conditions. Gravitational stability of binary mixtures in a phase transition.

FUGLISTALER A. and PFENNIGER D.

Abstract (from CDS):

Context. Molecular clouds typically consist of 3/4 H2, 1/4 He and traces of heavier elements. In an earlier work we showed that at very low temperatures and high densities, H2 can be in a phase transition leading to the formation of ice clumps as large as comets or even planets. However, He has very different chemical properties and no phase transition is expected before H2 in dense interstellar medium conditions. The gravitational stability of fluid mixtures has been studied before, but these studies did not include a phase transition.
Aims. We study the gravitational stability of binary fluid mixtures with special emphasis on when one component is in a phase transition. The numerical results are aimed at applications in molecular cloud conditions, but the theoretical results are more general.
Methods. First, we study the gravitational stability of van der Waals fluid mixtures using linearized analysis and examine virial equilibrium conditions using the Lennard-Jones intermolecular potential. Then, combining the Lennard-Jones and gravitational potentials, the non-linear dynamics of fluid mixtures are studied via computer simulations using the molecular dynamics code LAMMPS.
Results. Along with the classical, ideal-gas Jeans instability criterion, a fluid mixture is always gravitationally unstable if it is in a phase transition because compression does not increase pressure. However, the condensed phase fraction increases. In unstable situations the species can separate: in some conditions He precipitates faster than H2, while in other conditions the converse occurs. Also, for an initial gas phase collapse the geometry is essential. Contrary to spherical or filamentary collapses, sheet-like collapses starting below 15 K easily reach H2 condensation conditions because then they are fastest and both the increase of heating and opacity are limited.
Conclusions. Depending on density, temperature and mass, either rocky H2 planetoids, or gaseous He planetoids form. H2 planetoids are favoured by high density, low temperature and low mass, while He planetoids need more mass and can form at temperature well above the critical value.

Abstract Copyright: © ESO, 2016

Journal keyword(s): instabilities - ISM: clouds - ISM: kinematics and dynamics - ISM: molecules - methods: numerical - methods: analytical

Simbad objects: 1

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Number of rows : 1
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 NGC 7293 PN 22 29 38.5454047152 -20 50 13.747242408 11.894 13.158 13.524 13.689 13.898 DAO.5 983 1

Query : 2016A&A...591A.100F

Basic data :
NGC 7293 -- Planetary Nebula
Other object types:
otypes_help
* (CSI,GCRV,...), Rad (GLEAM,NVSS,...), PN (2013MNRAS,PK,...), blu (2019A&A,PHL), X (2E,2RXP,...), IR (IRAS,[RHK93]), WD* (WD), WD? (2021MNRAS), HS? (2019A&A), G (ESO), NIR (2MASS)
ICRS coord. (ep=J2000) :
22 29 38.5454047152 -20 50 13.747242408 (Optical) [ 0.0409 0.0335 90 ] A 2020yCat.1350....0G
FK4 coord. (ep=B1950 eq=1950) :
22 26 54.6585789314 -21 05 36.749197852 [ 0.0409 0.0335 90 ]
Gal coord. (ep=J2000) :
036.1613363573655 -57.1183735402488 [ 0.0409 0.0335 90 ]
Proper motions mas/yr :
38.790 -3.347 [0.048 0.040 90] A 2020yCat.1350....0G
Radial velocity / Redshift / cz :
V(km/s) -15.0 [10] / z(~) -0.000050 [0.000033] / cz -15.00 [10.00]
   E 1953GCRV..C......0W
Parallaxes (mas):
5.0124 [0.0437] A 2020yCat.1350....0G
Spectral type:
DAO.5 C 2011ApJ...743..138G
Angular size (arcmin):
13.400 13.400 90 (Rad) D 2008ApJ...689..194S
Fluxes (9) :
U 11.894 [~] D 2007AJ....133..768L
B 13.158 [~] D 2007AJ....133..768L
V 13.524 [~] D 2007AJ....133..768L
R 13.689 [~] D 2007AJ....133..768L
G 13.458613 [0.002878] C 2020yCat.1350....0G
I 13.898 [~] D 2007AJ....133..768L
J 14.332 [0.024] C 2003yCat.2246....0C
H 14.49 [0.04] C 2003yCat.2246....0C
K 14.55 [0.08] C 2003yCat.2246....0C
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Identifiers (39) :
An access of full data is available using the icon Vizier near the identifier of the catalogue

NGC 7293 IRAS X2226-210 PLX 5437 WD 2226-210
CSI-21-22270 2MASS J22293854-2050136 PLX 5437.00 WEB 19878
2E 4615 NAME HELICAL NEB PN G036.1-57.1 WISH B2226.9-2105
2E 2226.9-2105 NAME Helix Nebula PN ARO 17 2XMM J222938.5-205014
ESO 602-22 NVSS J222941-205025 PN VV' 563 [HBC92] 222654.7-210537
GCRV 14134 PHL 287 PN VV 275 [LFO93] 2226-21
GJ 9785 PK 036-57 2RXP J222938.8-205015 [RHK93] 18755
GLEAM J222942-205017 PK 036-57 1 TIC 69813909 Gaia DR2 6628874205642084224
GSC2 S32303301945 PKS 2226-211 USNO 271 Gaia DR3 6628874205642084224
IRAS 22267-2102 PKS J2229-2050 uvby98 610160287

References (983 between 1850 and 2026) (Total 983)
Simbad bibliographic survey began in 1850 for stars (at least bright stars) and in 1983 for all other objects (outside the solar system).
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Collections of Measurements Description of Measurements

Velocities : 2    Distance : 5    Fe/H : 2    Plx : 6    PM : 4    SpT : 1   

   

Observing logs
Herschel : 13    ISO : 21    IUE : 35    XMM : 1   

   


External archives :

Archive data at HEASARC - High-Energy Astrophysics Science Archive Research Center

Data at NED - NASA/IPAC Extragalactic Database : NGC 7293

Link by name to the catalogue in VizieR :

NGC 7293 2E 4615 GJ 9785 IRAS 22267-2102 IRAS X2226-210
2MASS J22293854-2050136 NVSS J222941-205025 PHL 287 PKS 2226-211 PKS J2229-2050
PLX 5437 PN G036.1-57.1 uvby98 610160287 WD 2226-210 WISH B2226.9-2105
Gaia DR2 6628874205642084224 Gaia DR3 6628874205642084224

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