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著者: Albert Einstein

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Place a metre-rod in the x′-axis of K′ in such a manner that one
end (the beginning) coincides with the point x′ = 0 whilst the
other end (the end of the rod) coincides with the point x′ = 1.
What is the length of the metre-rod relatively to the system K?
In order to learn this, we need only ask where the beginning of
the rod and the end of the rod lie with respect to K at a
particular time t of the system K. By means of the first equation
of the Lorentz transformation the values of these two points at
the time t = 0 can be shown to be
image006
the distance between the points being
image007
But the metre-rod is moving with the velocity v relative to K. It
therefore follows that the length of a rigid metre-rod moving in
the direction of its length with a velocity v is
image008
of a metre. The rigid rod is thus shorter when in motion than
when at rest, and the more quickly it is moving, the shorter is
the rod. For the velocity v = c we should have
image009

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