If the primed frame moves at speed in the positive direction relative to the unprimed frame, the one-dimensional Lorentz transformation is
For a trajectory with velocity , differentiating these expressions gives . Solving for , when the particle has primed-frame speed , proves the relativistic velocity-addition formula
For the train problem the sign of the frame velocity reverses: the train frame moves at relative to the station frame . Put . The transformation appropriate to the subsequent parts is therefore

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