The Postulates — Question 9

Section 37-1 · Physics pages 6048–6049

Question 9 A rotating receiver is outside the global inertial-frame assumption In an inertial laboratory, two light pulses circulate in opposite directions along an ideal circular vacuum guide of circumference C at speed c. A receiver moves along the guide at constant tangential speed v. At t = 0 both pulses leave it; neglect all material optical effects. v C Schematic; labels, not drawing lengths, specify the data. (a) Find the first return times for the pulse chasing the receiver and the counter-propagating pulse. (b) Find their laboratory time difference and its small-v limit.
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Question 9 - Solution A rotating receiver is outside the global inertial-frame assumption v C (a) Method and calculation (c −v)t+ = C, (c + v)t−= C ⇒ t± = C c ∓v. t+ > t− (v > 0). (b) Interpretation and further calculation ∆t = 2Cv c2 −v2 . v ≪c : ∆t ≃2Cv/c2 . Physical check The receiver changes direction continuously. This laboratory calculation does not assign a single global inertial rest frame to the rotating receiver.

Question 9

A rotating receiver is outside the global inertial-frame assumption

In an inertial laboratory, two light pulses circulate in opposite directions along an ideal circular vacuum guide of circumference C at speed c. A receiver moves along the guide at constant tangential speed v. At t=0t=0 both pulses leave it; neglect all material optical effects.

Diagram shown in the original SVG worksheet.

  1. Find the first return times for the pulse chasing the receiver and the counter-propagating pulse.

  2. Find their laboratory time difference and its small-v limit.

Question 9 - Solution

A rotating receiver is outside the global inertial-frame assumption

Diagram shown in the original SVG worksheet.

(a) Method and calculation

(c−v)t+=C,(c+v)t−=C⇒t±=Cc∓v.(c-v)t_+=C,\quad(c+v)t_-=C\quad\Rightarrow\quad t_\pm=\frac{C}{c\mp v}.t+>t−(v>0).t_+>t_-\quad(v>0).

(b) Interpretation and further calculation

Δt=2Cvc2−v2.\boxed{\Delta t=\frac{2Cv}{c^2-v^2}}.v≪c:Δt≃2Cv/c2.v\ll c:\quad\boxed{\Delta t\simeq2Cv/c^2}.

Physical check

The receiver changes direction continuously. This laboratory calculation does not assign a single global inertial rest frame to the rotating receiver.