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Max Planck Institute for Astronomy - Annual Report 2005

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not only causes a diffusion of the smallest dust particles,<br />

it also creates relative velocities between rock-sized bodies<br />

that are not coupled to the gas any longer. On the one<br />

hand more collisions will occur, on the other hand a local<br />

concentration of the rocks will develop. So <strong>for</strong> instance,<br />

boulders up to several meters across can be captured this<br />

way in vortices. Such vortices can <strong>for</strong>m in the so-called<br />

magnetorotational turbulence (MRI turbulence).<br />

MRI turbulence is an interplay of shear flows and<br />

magnetic fields that can be visualized more or less the<br />

following way. Shear flows can cause turbulence. This is<br />

known, e.g., from fast sports cars where the circumfluent<br />

air can become turbulent. The skill of car designers is to<br />

shape the car in such a way that the turbulence is minimized<br />

since the developing vortices increase the drag.<br />

Spoilers and streamlining help to shift the occurrence of<br />

turbulence as far behind the sports car as possible.<br />

Such a shear flow also occurs in gaseous disks surrounding<br />

young stars. Close to the star the gas flows faster<br />

than further out. Experiments and analytical studies<br />

have shown that the flow in disks does not easily become<br />

turbulent since the circumstellar disk rotates very fast.<br />

The related angular momentum stabilizes the shear flow,<br />

acting like a spoiler on a sports car.<br />

Now the effect of the magnetic fields is added. The gas<br />

surrounding the young star is probably is ionized, and the<br />

charge carriers couple to the magnetic field lines. These<br />

lines pass through the disk like elastic bands, trying to<br />

prevent the shear. So the inner region of the disk is slowed<br />

down and the outer part is sped up. However, this<br />

destabilizes the flow in the disk to such an extent that it<br />

becomes turbulent, <strong>for</strong>ming vortices. The magnetic fields<br />

thus act like a <strong>for</strong>est of antennas screwed onto one’s<br />

sports car: the drag is increased enormously as the flow<br />

around the car becomes turbulent – despite all spoilers.<br />

Theorists at MPIA simulated numerically the phenomenon<br />

of MRI turbulence in the disks around young<br />

stars. Two million particles represented rocks moving in<br />

a gas. Friction could be varied by a parameter. Then the<br />

MRI turbulence of the gas was included in the simulation<br />

in order to study the effect of this phenomenon on the<br />

max (n)<br />

700<br />

600<br />

500<br />

400<br />

300<br />

200<br />

100<br />

� 0 � f = 0.1<br />

� 0 � f = 10.0<br />

0<br />

0 20 40 60<br />

t [25/� 0 ]<br />

II. 4. Plantesimal Formation by Gravitational Instability 27<br />

motion of macroscopic bodies. Since a complete threedimensional<br />

treatment of the entire disk is far beyond the<br />

computing power of present-day computers the simulation<br />

had to be limited to a volume within the disk. Values<br />

<strong>for</strong> a radial density gradient and a pressure gradient were<br />

each varied over a range expected <strong>for</strong> protoplanetary<br />

disks. The sizes of the rocks was assumed to be ten centimeters<br />

as well as one and ten meters.<br />

The simulations per<strong>for</strong>med with various parameters<br />

showed surprising results. The MRI turbulence produces<br />

vortices in the gas that have a slightly higher density<br />

and a marginally higher pressure than their environment.<br />

These condensations survive in the disks <strong>for</strong> some orbital<br />

periods, corresponding to some ten or – in the outer regions<br />

of the disk – even hundred years. Then they disperse,<br />

but might <strong>for</strong>m again somewhere else.<br />

The vortices rotate in different directions and can be<br />

distinguished, as in the earth’s atmosphere, into cyclones<br />

and anticyclones according to their sense of rotation.<br />

Interestingly the solid bodies move towards the anticyclones,<br />

remaining captured there. Cyclones, on the other<br />

hand, disperse the particles. This effect even increases<br />

with the size of the particles, reaching a maximum <strong>for</strong><br />

meter-sized bodies: Here the local concentration of the<br />

bodies is a hundred times higher than on average while<br />

the effect is much lower <strong>for</strong> the small grains and <strong>for</strong><br />

larger objects (Fig. II.4.1 and Fig. II.4.2). The motion of<br />

the particles towards the anticyclone regions is caused<br />

by the pressure gradient existing there. These accumulations<br />

of large bodies survive <strong>for</strong> a while even when<br />

the gas vortices that had created them already have<br />

dispersed.<br />

A second interesting result was that the MRI turbulence<br />

slows down the drift of the rocks towards the central<br />

star mentioned above. Compared to a laminar disk<br />

this velocity is reduced by up to 40 percent (Fig. II.4.3).<br />

Fig. II.4.2: Like Fig. II.4.1, but <strong>for</strong> particles 10 cm (lower curve)<br />

and 10 m across. Clearly evident is the higher-than-average<br />

concentration of the large boulders.<br />

80<br />

60<br />

40<br />

20<br />

0<br />

80 100<br />

max (n)/n 0

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