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Annual Report 2011 Max Planck Institute for Astronomy

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42 III. Selected Research Areas<br />

low <strong>for</strong> direct falsifiability with future observations is a<br />

strength of the method. Besides that, the predictions are<br />

also useful to estimate the yield of future instruments<br />

and surveys.<br />

Planet <strong>for</strong>mation models<br />

On the observational side, usually only the initial conditions<br />

(the protoplanetary disks) and the final outcomes<br />

(the planets) are accessible to observations. With theoretical<br />

<strong>for</strong>mation models, it is possible to bridge this gap<br />

at least on the theoretical side. The global, numerical<br />

models of planet <strong>for</strong>mation used in population synthesis<br />

calculations try to cover the largest possible extent<br />

of important mechanisms. The various mechanisms like<br />

accretion or migration must be treated in an interlinked<br />

way, since they happen on similar timescales and feed<br />

back on each other. Ideally, the models would start with<br />

a protoplanetary disk at a very early stage when the<br />

solids are in the <strong>for</strong>m of micrometer-sized dust grains,<br />

and yield as an output full-blown planetary systems at<br />

an age of several billions of years. This means that also<br />

the evolution of the planets over long timescales must<br />

be modeled, since we essentially observe planets a long<br />

time after they have <strong>for</strong>med. It is clear that these glob-<br />

Fig. III.1.3: Theoretical planetary <strong>for</strong>mation tracks which show<br />

how planetary seeds (initial mass 0.6 Earth masses) concurrently<br />

grow and migrate. The colors indicate the different types<br />

of orbital migration. The position of the planet at the moment<br />

Mass [M Earth ]<br />

10 4<br />

10 3<br />

10 2<br />

10<br />

1<br />

0,1 1<br />

Semimajor axis [AU]<br />

al models of planet <strong>for</strong>mation and evolution involve<br />

important simplifications of the actual processes, and<br />

cannot describe all physical effects at the same level<br />

of detail as models dedicated to one single process. On<br />

the other hand, only combined models allow to see the<br />

interaction between different processes, and only they<br />

allow <strong>for</strong> direct comparisons with many observational<br />

constraints.<br />

The global planet <strong>for</strong>mation and evolution models<br />

used in population synthesis calculations are based on<br />

the so called core-accretion paradigm which states that<br />

first, solid cores are <strong>for</strong>med, some of which later accrete<br />

massive gaseous envelopes to become giant planets<br />

(bottom-up process), while the remaining cores collide<br />

to <strong>for</strong>m both ice giants and terrestrial planets. The<br />

models address the following processes in a number of<br />

coupled computational modules:<br />

1. A structure and evolution model <strong>for</strong> a gaseous protoplanetary<br />

disk. The gaseous disk model yields the<br />

ambient properties in which the planets <strong>for</strong>m. The<br />

ambient pressure and temperature serve as outer<br />

boundary conditions <strong>for</strong> the calculation of the structure<br />

of the gaseous envelope of the planets. The<br />

structure of the disk is also very important <strong>for</strong> the<br />

orbital migration of the protoplanets, since the di-<br />

in time that is shown (4.9 Myrs) is indicated by black symbols.<br />

Some planets have reached the inner border of the computational<br />

domain at 0.1 AU.<br />

10<br />

t 4.9 Myr<br />

Credit: C. Mordasini

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