The evolution of scientific thought from Newton to EinsteinD'Abro, A. (Aram)
Science
The evolution of scientific thought from Newton to Einstein
D'Abro, A. (Aram)
Relativity (Physics); Science -- Methodology
Now, without going into mathematical details, let us make an effort to
see why it is that the clock of the travelling twin must necessarily
have suffered retardation. To understand the reason, we must revert
to Einstein’s premises, and in particular to the postulate of the
[Pg 229]
invariant velocity of light. This postulate, as we have explained on
several occasions, states that all Galilean observers situated in their
respective Galilean frames will discover, as a result of measurement
with rigid rods, that waves of light invariably pass through their
frames with the same constant speed of 300,000 kilometres per second.
If this postulate be accepted, we must infer that in every Galilean
frame, time can be measured by the distance in space covered by a
wave of light (the distance being measured with rigid rods at rest in
the frame). As a result the postulate allows us to construct a sort
of optical clock. We may, for example, consider two parallel mirrors
situated at a fixed distance apart of 1.5 kilometres in our Galilean
frame, and we may suppose that a wave of light is reflected back and
forth from one mirror to the other. These oscillations of the ray of
light, covering always the same distance, require equal durations; and
in the present case 100,000 such double oscillations would be seen
to define a duration of one second for that Galilean frame in which
the optical apparatus was situated. We must henceforth consider every
Galilean frame as possessing an optical clock of this kind defining the
passage of time for its own frame.
Let us now analyse the problem of the two twins; and let us suppose
that we as observers are stationed on the earth, say, at
the North Pole. To a high degree of approximation we may consider
ourselves, therefore, as at rest in a non-rotating or Galilean frame.
The moving observer is also situated in a Galilean frame, moving away
from us with a speed which we shall assume to be about four-fifths that
of light. He visits a distant star which we should recognise as being
sixteen light years distant[73] from us, then reverses his velocity and
returns to earth.
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