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and Cosmology

Extragalactic Astronomy and Cosmology: An Introduction

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3. The World of Galaxies<br />

140<br />

by no means isolated systems: their mass continuously<br />

changes through accretion <strong>and</strong> merging processes. In<br />

addition, the kinetic energy transferred to the ISM by<br />

supernova explosions causes an outflow of the ISM,<br />

in particular in low-mass galaxies where the gas is<br />

not strongly gravitationally bound. Therefore, the observed<br />

deviations from relation (3.72) allow us to draw<br />

conclusions about these processes.<br />

Also, from observations in our Milky Way we find<br />

indications that the model of the chemical evolution<br />

sketched above is too simplified. This is known as the<br />

G-dwarf problem. The model described above predicts<br />

that about half of the F- <strong>and</strong> G-main-sequence stars<br />

should have a metallicity of less than a quarter of the<br />

Solar value. These stars have a long lifetime on the<br />

main sequence, so that many of those observed today<br />

should have been formed in the early stages of the Galaxy.<br />

Thus, in accordance with our model they should<br />

have very low metallicity. However, a low metallicity<br />

is in fact observed in only very few of these stars. The<br />

discrepancy is far too large to be explained by selection<br />

effects. Rather, observations show that the chemical<br />

evolution of our Galaxy must have been substantially<br />

more complicated than described by our simple model.

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