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Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf

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20 2. The X-ray environment of ra<strong>di</strong>o galaxies<br />

-17 00 00<br />

2 4 6 8<br />

-17 00 00<br />

30<br />

30<br />

DECLINATION (J2000)<br />

01 00<br />

30<br />

02 00<br />

DECLINATION (J2000)<br />

01 00<br />

30<br />

02 00<br />

3<br />

2<br />

1<br />

Outer<br />

30<br />

30<br />

03 00<br />

22 14 32 30 28 26 24 22 20<br />

RIGHT ASCENSION (J2000)<br />

03 00<br />

22 14 32 30 28 26 24 22 20 18<br />

RIGHT ASCENSION (J2000)<br />

Figure 2.4: (Left): Overlay of a 5 GHz VLA map (red) of 3C 444 on 0.5 - 5.0 keV Chandra<br />

data (blue) in<strong>di</strong>cating the relationship between the ra<strong>di</strong>o and X-ray structures, inclu<strong>di</strong>ng cavities<br />

coincident with the ra<strong>di</strong>o lobes, and a sharp elliptical surface brightness drop surroun<strong>di</strong>ng the<br />

source. (right): temperature map in keV with 5 GHz contours overlaid. The spectral extraction<br />

regions are numbered. The figure is taken from (Croston et al. 2010).<br />

to shock Mach numbersMof about 8 and 4 respectively (Kraft et al. 2003; Croston et al. 2007).<br />

In both the cases, the total energies stored in the cavities are several times larger than the estimated<br />

PV work.<br />

Weak shocks withM≈1.2−1.7 surroun<strong>di</strong>ng cavities associated with FR I and FR II sources are<br />

observed more frequently (e.g. McNamara et al. 2005; Nulsen et al. 2005a; Croston et al. 2008,<br />

2010). Fig. 2.4 shows the case of the FR II ra<strong>di</strong>o galaxy 3C 444 where the surroun<strong>di</strong>ng intra-cluster<br />

me<strong>di</strong>um is characterized by cavities and a temperature jump of a factor∼1.7, probably caused by<br />

a spheroidal shock (Croston et al. 2010).<br />

The effects of these ra<strong>di</strong>o-galaxy shocks on the magnetic field in the IGM are analysed in<br />

detail in Chapter 5.<br />

20

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