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4. Structure of Dark Matter halos Obviously, we cannot observe the ...

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6-4-10see http://www.strw.leidenuniv.nl/˜ franx/college/galaxies10 10-c04-15<br />

In our own Milky Way, <strong>the</strong> number <strong>of</strong> satellites appears<br />

much smaller than predicted by <strong>the</strong> models:<br />

The solution for this problem is not clear. Are <strong>we</strong> missing<br />

a lot <strong>of</strong> satellites ? Or do <strong>we</strong> underestimate <strong>the</strong>ir<br />

mass ? Or is <strong>the</strong> dark matter model wrong ?<br />

Problem sets<br />

1) Derive <strong>the</strong> enclosed mass M(< r) for <strong>the</strong> NFW<br />

pr<strong>of</strong>ile ρ(r) = ρs/[(r/rs)(1 + r/r2) 2 ]. Use r/(1 + r) 2<br />

= 1/(r + 1) − 1/(1 + r) 2<br />

2) Derive <strong>the</strong> circular velocity as a function <strong>of</strong> radius<br />

6-4-10see http://www.strw.leidenuniv.nl/˜ franx/college/galaxies10 10-c04-16<br />

for <strong>the</strong> NFW pr<strong>of</strong>ile<br />

3) Approximate <strong>the</strong> rotation curve <strong>of</strong> UGC 4325 by a<br />

straight line, through (0 arcsec, 0 km/s) and (60 arcsec,<br />

110 km/s). What is <strong>the</strong> best fitting NFW model ?<br />

This would be <strong>the</strong> model for which<br />

χ 2 = � (Vobs − Vmodel) 2 dr is minimized.<br />

What is <strong>the</strong> average rms residual ? [(Vobs − Vmodel)] ?<br />

4) We can see from <strong>the</strong> figure from Springel et al. that<br />

about 30-40 % <strong>of</strong> <strong>the</strong> mass <strong>of</strong> a halo is in sub<strong>halos</strong>.<br />

This appears quite different from <strong>the</strong> situation in clusters,<br />

where <strong>the</strong> light is dominated by <strong>the</strong> ensemble <strong>of</strong><br />

regular cluster galaxies, and NOT by <strong>the</strong> brightest cluster<br />

galaxy. Can you think <strong>of</strong> an explanation ?

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