In the laboratory frame

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Special relativity: spacetime and kinematics · Special relativity: spacetime and kinematics

The Geometry of Gravity, Ch Minkowski spacetime and relativistic dynamics, completed

Problem

In the laboratory frame, a detector fires at event AA, at (t,x)=(0,0)(t,x) = (0, 0), and a second detector fires at event BB, at (t,x)=(2.0 μs, 500 m)(t,x) = (2.0\ \mu\mathrm{s},\ 500\ \mathrm{m}), both along the xx-axis. Someone argues: "observers can be boosted arbitrarily close to cc, so a fast enough observer, say at v=0.995cv = 0.995c, will always find some pair of events whose time order is reversed relative to the laboratory, including this one." ((a)) Classify the separation between AA and BB from the sign of the invariant interval. ((b)) Compute the time interval Δt′\Delta t' between the two events as measured by an observer moving at v=0.995cv = 0.995c along xx relative to the laboratory, and use it to show this claim is wrong for this pair. ((c)) State, in one sentence, why no boost below cc can reverse the order of AA and BB.

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