1997
DOI: 10.1006/icar.1997.5712
|View full text |Cite
|
Sign up to set email alerts
|

The Origin of Comets in the Solar Nebula: A Unified Model

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

11
382
0
1

Year Published

1998
1998
2013
2013

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 388 publications
(396 citation statements)
references
References 36 publications
11
382
0
1
Order By: Relevance
“…Here we aim to show the general evolution of how water vapor and ice could be distributed in protoplanetary disks by modeling all of the physics that control the evolution of the four species which have the most distinct dynamical behavior. Thus our model is an improvement over the single-size model at a given location of Stepinski and Valageas (1997), but is simpler to evolve than the full size distribution of Weidenschilling (1997) (or other similar studies) and accounts for the diversity of physical behaviors involved. In general, water vapor will be transported by the same processes that transport the rest of the nebular gas (diffusion and advection).…”
Section: Evolution Of the Water Distributionmentioning
confidence: 98%
See 2 more Smart Citations
“…Here we aim to show the general evolution of how water vapor and ice could be distributed in protoplanetary disks by modeling all of the physics that control the evolution of the four species which have the most distinct dynamical behavior. Thus our model is an improvement over the single-size model at a given location of Stepinski and Valageas (1997), but is simpler to evolve than the full size distribution of Weidenschilling (1997) (or other similar studies) and accounts for the diversity of physical behaviors involved. In general, water vapor will be transported by the same processes that transport the rest of the nebular gas (diffusion and advection).…”
Section: Evolution Of the Water Distributionmentioning
confidence: 98%
“…The likelihood of significant particle growth leads us to doubt the reality of the T 2 dependence found by Pollack et al (1994) and assumed by Cassen (1994), which is a tiny-particle property, so we will assume a temperatureindependent opacity per gram of solid material. Results of Weidenschilling (1997Weidenschilling ( , 2000 using detailed particle growth models, tend to find the "dust" regime (microns to tens of centimeters radius) has a mass distribution m(a) with equal mass per bin of width a (equal to the particle radius); that is, then, n (a) a 4 = constant, or n (a) ∝ a −4 . From figure 10 of Miyake and Nakagawa (1993) we see that, very roughly, the opacity of such a distribution, ranging from microns to centimeters, can be approximated by something like Cassen's adopted 5 cm 2 g −1 (because the steep powerlaw emphasizes particles at the small end of the range), over the wavelength range 1-100µm characterizing nebula blackbody radiation.…”
Section: Evolution Of the Nebular Gasmentioning
confidence: 99%
See 1 more Smart Citation
“…For compact spherical particles of size << λ, β = 2, while for Figure 2. A numerical simulation of particle size evolution within a protoplanetary disk (from [11]). The small grains in the disk stick and settle to the mid-plane, which creates a layer of centimeter size particles.…”
Section: Grain Growth Studiesmentioning
confidence: 99%
“…In case of widespread collisional fragmentation, e.g. in the warmer terrestrial planet formation region, up to 80% of the solid material may be bound in small fragments 27,28 , in which case we must implicitly assume an augmentation in solids-to-gas ratio of up to 5.In our self-gravitating model we set ∆v = −0.02c s , but show in the Supplementary Information that gravitationally bound clusters also form for ∆v = −0.05c s , with a factor of two increase in column density threshold. The Supplementary Information also documents that typical boulder collisions happen at speeds below the expected destruction threshold 3 .…”
mentioning
confidence: 99%