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and Cosmology

Extragalactic Astronomy and Cosmology: An Introduction

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3.3 Spiral Galaxies<br />

luminous galaxies. The specific abundance of globular<br />

clusters in a galaxy is defined as their number, normalized<br />

to a galaxy of absolute magnitude M V =−15.<br />

This can be done by scaling the observed number N t<br />

of globular clusters in a galaxy of visual luminosity<br />

L V or absolute magnitude M V , respectively, to that of<br />

a hypothetical galaxy with M V =−15:<br />

S N = N t<br />

L 15<br />

L V<br />

= N t 10 0.4(M V +15) . (3.13)<br />

If the number of globular clusters were proportional to<br />

the luminosity (<strong>and</strong> thus roughly to the stellar mass) of<br />

a galaxy, then this would imply S N = const. However,<br />

this is not the case: For Sa’s <strong>and</strong> Sb’s we find S N ∼ 1.2,<br />

whereas S N ∼ 0.5 forSc’s.S N is larger for ellipticals<br />

<strong>and</strong> largest for cD galaxies.<br />

3.3.5 Spiral Structure<br />

The spiral arms are the bluest regions in spirals <strong>and</strong> they<br />

contain young stars <strong>and</strong> HII regions. For this reason,<br />

the brightness contrast of spiral arms increases as the<br />

wavelength of the (optical) observation decreases. In<br />

particular, the spiral structure is very prominent in a blue<br />

filter, as is shown impressively in Fig. 3.17.<br />

Naturally, the question arises as to the nature of the<br />

spiral arms. Probably the most obvious answer would be<br />

that they are material structures of stars <strong>and</strong> gas, rotating<br />

around the galaxy’s center together with the rest of the<br />

disk. However, this scenario cannot explain spiral arm<br />

structure since, owing to the differential rotation, they<br />

would wind up much more tightly than observed within<br />

only a few rotation periods.<br />

Rather, it is suspected that spiral arms are a wave<br />

structure, the velocity of which does not coincide with<br />

the physical velocity of the stars. Spiral arms are quasistationary<br />

density waves, regions of higher density (possibly<br />

10–20% higher than the local disk environment).<br />

If the gas, on its orbit around the center of the galaxy,<br />

enters a region of higher density, it is compressed, <strong>and</strong><br />

this compression of molecular clouds results in an enhanced<br />

star-formation rate. This accounts for the blue<br />

color of spiral arms. Since low-mass (thus red) stars live<br />

longer, the brightness contrast of spiral arms is lower in<br />

red light, whereas massive blue stars are born in the spiral<br />

arms <strong>and</strong> soon after explode there as SNe. Indeed,<br />

only few blue stars are found outside spiral arms.<br />

In order to better underst<strong>and</strong> density waves we may<br />

consider, for example, the waves on the surface of a lake.<br />

Peaks at different times consist of different water particles,<br />

<strong>and</strong> the velocity of the waves is by no means the<br />

bulk velocity of the water.<br />

3.3.6 Corona in Spirals?<br />

Hot gas resulting from the evolution of supernova remnants<br />

may exp<strong>and</strong> out of the disk <strong>and</strong> thereby be ejected<br />

to form a gaseous halo of a spiral galaxy. We might<br />

103<br />

Fig. 3.17. The galaxy NGC 1300 in the B<br />

filter (left panel) <strong>and</strong> in the I filter (right<br />

panel). The spiral arms are much more<br />

prominent in the blue than in the red. Also,<br />

the tips of the bar are more pronounced<br />

in the blue – an indicator of an enhanced<br />

star-formation rate

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