Relativity: The Special and General TheoryEinstein, Albert
Science
Relativity: The Special and General Theory
Einstein, Albert
Relativity (Physics)
Up to now our considerations have been referred to a particular body of
reference, which we have styled a “railway embankment.” We suppose a
very long train travelling along the rails with the constant velocity v
and in the direction indicated in Fig 1. People travelling in this
train will with a vantage view the train as a rigid reference-body
(co-ordinate system); they regard all events in reference to the train.
Then every event which takes place along the line also takes place at a
particular point of the train. Also the definition of simultaneity can
be given relative to the train in exactly the same way as with respect
to the embankment. As a natural consequence, however, the following
question arises:
image001
Are two events (_e.g._ the two strokes of lightning _A_ and _B_) which
are simultaneous _with reference to the railway embankment_ also
simultaneous _relatively to the train?_ We shall show directly that the
answer must be in the negative.
When we say that the lightning strokes _A_ and _B_ are simultaneous
with respect to be embankment, we mean: the rays of light emitted at
the places _A_ and _B_, where the lightning occurs, meet each other at
the mid-point _M_ of the length _A_ → _B_ of the embankment. But the
events _A_ and _B_ also correspond to positions _A_ and _B_ on the
train. Let _M′_ be the mid-point of the distance _A_ → _B_ on the
travelling train. Just when the flashes (as judged from the embankment)
of lightning occur, this point _M′_ naturally coincides with the point
_M_ but it moves towards the right in the diagram with the velocity v
of the train. If an observer sitting in the position _M′_ in the train
did not possess this velocity, then he would remain permanently at M,
and the light rays emitted by the flashes of lightning _A_ and _B_
would reach him simultaneously, _i.e._ they would meet just where he is
situated. Now in reality (considered with reference to the railway
embankment) he is hastening towards the beam of light coming from _B_,
whilst he is riding on ahead of the beam of light coming from _A_.
Hence the observer will see the beam of light emitted from _B_ earlier
than he will see that emitted from _A_. Observers who take the railway
train as their reference-body must therefore come to the conclusion
that the lightning flash _B_ took place earlier than the lightning
flash _A_. We thus arrive at the important result:
Events which are simultaneous with reference to the embankment are not
simultaneous with respect to the train, and _vice versa_ (relativity of
simultaneity). Every reference-body (co-ordinate system) has its own
particular time; unless we are told the reference-body to which the
statement of time refers, there is no meaning in a statement of the
time of an event.
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