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We have simulated different formation scenarios of Varuna by varying the accretion time, accretion rate, and a fraction of impact kinetic energy converted into heat.
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More advanced model of Robuchon et al. (2010) further reduces the range of possible time of accretion and indicates that special Burgess rheology is necessary.
This layer would have a fabric anisotropy associated with plate motion at the time of accretion and so could also be electrically anisotropic by shearing.
VPI-2 and VSP-2 seem to have assembled over time by accretion of smaller units, which we call islets.
Time-dependent accretion during the infall phase may account for the low luminosity of Taurus-Auriga protostars; this hypothesis requires more tests.
(2) In addition, we point out that iron lines from time-dependent accretion disks in their "quiescent" states should be narrow even if the cold accretion disk extends to the last stable orbit.
Onset-time of accretion, magnitude and overall behaviour are in excellent agreement, despite the chaotic nature of the turbulent flow.
Also the onset-time of accretion and the saturation values differ significantly between the (N_{theta}=64) run and its high-resolution counterparts.
Due to the high temperature of the gas, the time-averaged accretion rate onto the protostar is of order (1mbox { M}_{odot} mbox { yr}^{-1}), eventually resulting in the formation of a super-massive star.
Up to a mass of about 10 M⊙, the accretion time (t_{mathrm{acc}}=M_/dot{M}_), where (M_) is the mass of the protostar, is smaller than the Kelvin-Helmholtz time (t_{mathrm{KH}}=GM_^{2}/ (R_L_ )), where (L_) is the luminosity of the protostar.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com