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Auteur: Albert Einstein

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[22] First observed by Eddington and others in 1919. (Cf.
Appendix III).
[23] Established by Adams in 1924. (Cf. p. 132)
PART III: CONSIDERATIONS ON THE UNIVERSE AS A WHOLE
XXX.
COSMOLOGICAL DIFFICULTIES OF NEWTON'S THEORY
Part from the difficulty discussed in Section XXI, there is a
second fundamental difficulty attending classical celestial
mechanics, which, to the best of my knowledge, was first
discussed in detail by the astronomer Seeliger. If we ponder over
the question as to how the universe, considered as a whole, is to
be regarded, the first answer that suggests itself to us is
surely this: As regards space (and time) the universe is
infinite. There are stars everywhere, so that the density of
matter, although very variable in detail, is nevertheless on the
average everywhere the same. In other words: However far we might
travel through space, we should find everywhere an attenuated
swarm of fixed stars of approrimately the same kind and density.

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