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Yazar: Albert Einstein

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Thus all our previous conclusions based on general relativity
would appear to be called in question. In reality we must make a
subtle detour in order to be able to apply the postulate of
general relativity exactly. I shall prepare the reader for this
in the following paragraphs.
XXIV.
EUCLIDEAN AND NON-EUCLIDEAN CONTINUUM
The surface of a marble table is spread out in front of me. I can
get from any one point on this table to any other point by
passing continuously from one point to a "neighbouring" one, and
repeating this process a (large) number of times, or, in other
words, by going from point to point without executing "jumps." I
am sure the reader will appreciate with sufficient clearness what
I mean here by "neighbouring" and by "jumps" (if he is not too
pedantic). We express this property of the surface by describing
the latter as a continuum.

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