Boek · Relativity
Pagina 52 van 212
Auteur: Albert Einstein
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In Section VI we derived the theorem of the addition of
velocities in one direction in the form which also results from
the hypotheses of classical mechanics. This theorem can also be
deduced readily from the Galilei transformation (Section XI). In
place of the man walking inside the carriage, we introduce a
point moving relatively to the co-ordinate system K′ in
accordance with the equation
x′ = wt′
By means of the first and fourth equations of the Galilei
transformation we can express x′ and t′ in terms of x and t, and
we then obtain
x = (v + w)t
This equation expresses nothing else than the law of motion of
the point with reference to the system K (of the man with
reference to the embankment). We denote this velocity by the
symbol W, and we then obtain, as in Section VI,
W = v + w . . . . . . . (A).
But we can carry out this consideration just as well on the basis
of the theory of relativity. In the equation
x′ = wt′
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