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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Anomalous Stellar Energy Losses Bounded by Observations 25<br />

medium. M<strong>as</strong>s loss in advanced stages of stellar evolution can take<br />

on the benign <strong>for</strong>m of a “stellar wind,” or it can occur in gigantic<br />

“supernova explosions.” The end state of stellar evolution must be<br />

complete disruption, or a compact object (white dwarf, neutron star, or<br />

black hole), because a normal star, supported by thermal pressure, can<br />

exist only <strong>as</strong> long <strong>as</strong> its nuclear fuel l<strong>as</strong>ts (Sect. 1.2.2). The m<strong>as</strong>ses of<br />

degenerate stars are constrained by their Chandr<strong>as</strong>ekhar limit of about<br />

1.4 M ⊙ <strong>for</strong> white dwarfs, and a similar value <strong>for</strong> neutron stars. Most<br />

m<strong>as</strong>sive stars seem to return enough m<strong>as</strong>s to the interstellar medium<br />

that their typical end states are degenerate stars, not black holes. The<br />

primordial material evolves chemically because it is cycled through one<br />

generation of stars after another.<br />

Today, the continuing birth and death of stars takes place mostly in<br />

the disks of spiral galaxies. Such galaxies also have a population of old<br />

halo stars and of globular clusters, about 150 in our Milky Way, each of<br />

which is a gravitationally bound system of about 10 6 stars (Fig. 2.1).<br />

Most of the globular clusters are in the galactic halo, far away from the<br />

disk. The gravitational escape velocity <strong>for</strong> stars or g<strong>as</strong> from a cluster<br />

is rather small, about 10 km s −1 . A supernova explosion, on the other<br />

hand, ejects its material with typical velocities of several 10 3 km s −1 .<br />

A single supernova is enough to sweep a globular cluster clean of all<br />

Fig. 2.1. Globular cluster M3. (Image courtesy of Palomar/Caltech.)

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