2001
DOI: 10.1006/icar.2001.6589
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Stability of Condensed Hydrocarbons in the Solar Nebula

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Cited by 23 publications
(19 citation statements)
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“…1000 K, the exact temperature depending on the pressure, the thermodynamically preferred states of carbon and oxygen atoms are in the molecules CH 4 and H 2 O rather than CO (see, e.g., Burrows &Sharp 1999 andZolotov &Shock 2001). At a sufficiently low temperature, water and ice droplets form, while CH 4 remains in the gas phase until the temperature drops significantly below 100 K (Boogert et al 1998).…”
Section: Discussionmentioning
confidence: 99%
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“…1000 K, the exact temperature depending on the pressure, the thermodynamically preferred states of carbon and oxygen atoms are in the molecules CH 4 and H 2 O rather than CO (see, e.g., Burrows &Sharp 1999 andZolotov &Shock 2001). At a sufficiently low temperature, water and ice droplets form, while CH 4 remains in the gas phase until the temperature drops significantly below 100 K (Boogert et al 1998).…”
Section: Discussionmentioning
confidence: 99%
“…At a sufficiently low temperature, water and ice droplets form, while CH 4 remains in the gas phase until the temperature drops significantly below 100 K (Boogert et al 1998). The disk's approach to this thermodynamically predicted state in a sufficiently short time can be facilitated by Fischer-Tropsch (FT) catalysis on the surface of iron grains at phases when the material was warmer than 400 K, as has been suggested to explain the presence of carbonaceous material in meteorites (see, e.g., Kress &Tielens 2001 andZolotov &Shock 2001). Alternatively, gas-phase chemistry may be important (Morgan et al 1991).…”
Section: Discussionmentioning
confidence: 99%
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“…equilibrium, and hydrocarbons can coexist with water vapour in a metastable state (Zolotov & Shock 2001). Reactions between hydrocarbons and atomic H occur with significant rates such that all hydrocarbons with more than three carbon atoms are degraded to small hydrocarbons with 1 or 2 carbon atoms, mainly CH 4 and C 2 H 2 , before they disappear at temperatures above ∼1200 K by oxidation to CO.…”
Section: A2 Oxidation Of Sootmentioning
confidence: 99%
“…This radiation-induced lattice damage represents an accumulation of latent energy because atomic displacement defects in solids typically store about 1 eV each (Devanathan et al 1998). Since a Frenkel pair in graphite represents approximately 2.7 eV, or 4.3× 10 −19 J, displacing more than 1% of the atoms in carbonaceous materials (Zolotov and Shock 2001), including nanocrystalline carbon and polyaromatic graphite precursors, can create a stored energy density of approximately 2 MJ kg −1 , while comparable defect densities in oxide and silicate phases can store approximately 0.1 MJ kg −1 (Kurath 1957). If 9P/Tempel-1's interior contains carbonaceous materials (Ewels et al 2003) and grains of oxides or silicates such as enstatite or olivine with high densities of frozen in radiation damage, energy released from shockheated grains or dust could augment the kinetic energy of the Deep Impact probe.…”
Section: Introductionmentioning
confidence: 99%