Chris Ormel
Hubble fellow
University of California, Berkeley
Chris OrmelHubble fellow
University of California, Berkeley
Protoplanet growth is
complex. There are a multitude of physical processes -- for instance,
planetesimal fragmentation, radial drift, turbulent diffusion, gas drag
-- that determine its efficiency. Catching all these mechanisms in one
self-consistent
model is virtually impossible. Let alone to perform a statistically
viable parameter study.Here, a toy model serves as a useful tool to quickly explore the parameter
space. We construct a toy model for the protoplanet growth, emphasizing simplicity and versatilty....
Coagulation
will affect he dust size distribution in dense molecular clouds.
This, in turn, affects the dust opacity -- a critical quantity required
for any
interpretation of observational data sets. Following previous work previous work where we computed the
dust size distribution as function of time, we
now present the corresponding mass-weighted opacities for infra-red
wavelengths.
The figure shows that the opacities change on timescales of ~Myr (or
less if the cloud's density is higher than the assumed n=105
cm-3). At visible and near-IR wavelengths the opacitiy
decreases,
but at longer wavelengths it will increase with time. We have
quantified this evolutionary trend in terms of the strength in the
9.7μm silicate feature vs near-IRcolor excess and in terms of the
sub-mm slope β.
Protoplanets
can sweep-up particles effectively due to their gravitational focusing
effect which allows particles to be accreted with a collision cross
section much
larger than the geometrical cross section of the protoplanets.
The amount of
focusing depends to a large degree on the velocity at which the bodies
approach, with the largest focusing being achieved at low relative
velocities. This effects is well described in the literature;
however the effects of gas drag --a force that becomes especially
important for small particles-- on this process are less clear.
In this project we determined how gas drag affects the gravitational
focusing of particles.
The figure shows some examples of particle trajectories under the
influence of varying levels of gas drag. The protoplanet is in
the center of the coordinate system.
[More...] [ADS]
[ArXiv] [A&A
Highlights]
When bodies are large enough to attract
each other gravitationally the effective cross section for
collisions becomes larger than the geometrical cross section.
This enhancement factor is called the gravitational
focusing
factor (GFF) and is approximately given by the square of the ratio of
the escape velocity of
the protoplanet and the relative velocity at wich the bodies
approach. The nature of this phenomenon is such that the largest
bodies grow faster than other bodies, a situation referred as runaway growth (RG).
RG indicates a
positive feedback effect: due to the growth, the gravitational focusing
increases. RG or, generally, a large GFF is required in order to
grow protoplanets in a sufficiently short time span.
When
bodies reach km-sizes
(planetesimals), their collisional and dynamical evolution becomes
dominated by gravity. Ideally, one would model the collisional
evolution by an N-body methods; hower the shear number of planetesimals
limit these attempts in practise. However, to model the (runaway
and oligarchic) growth correctly, its discrete nature must be taken
into account. For this reason we have extended our Monte Carlo
/superparticle code to treat dynamical interactions. [More...] [ADS] [ArXiv] [Movie]