The Relativity of Time — Question 10

Section 37-4 · Physics pages 6110–6111

Question 10 Received tick spacing contains a travel-time contribution A receding clock emits two pulses toward a stationary laboratory receiver, separated by proper interval ∆τ = 1.0 µs. Its speed is v = 0.60c. Both emissions occur on the same side of the receiver. Use dτ = dt √ 1 −v2/c2 for an ideal clock, with c = 3.00 × 108 m/s when needed. x ct clock Spacetime sketch; the vertical coordinate is ct. Labels specify events and worldlines. (a) Find the laboratory interval between the emission events. (b) Find the interval between receptions and separate the clock-rate and increasing-distance contributions.
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Question 10 - Solution Received tick spacing contains a travel-time contribution x ct clock (a) Method and calculation ∆temit = γ∆τ = 1.25 µs . ∆x = v∆temit. (b) Interpretation and further calculation ∆tR = ∆temit + ∆x/c = γ(1 + β)∆τ. ∆tR = 2.00 µs = 1.25 µs + 0.75 µs . Physical check Time dilation concerns assigned emission times; the directly observed arrival spacing also contains changing propagation delay.

Question 10

Received tick spacing contains a travel-time contribution

A receding clock emits two pulses toward a stationary laboratory receiver, separated by proper interval Δτ=1.0μs\Delta\tau=1.0\,\mu\mathrm s. Its speed is v=0.60cv=0.60c. Both emissions occur on the same side of the receiver. Use dτ=dt1−v2/c2d\tau=dt\sqrt{1-v^2/c^2} for an ideal clock, with c=3.00×108m/sc=3.00\times10^8\,\mathrm{m/s} when needed.

Diagram shown in the original SVG worksheet.

  1. Find the laboratory interval between the emission events.

  2. Find the interval between receptions and separate the clock-rate and increasing-distance contributions.

Question 10 - Solution

Received tick spacing contains a travel-time contribution

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δtemit=γΔτ=1.25μs.\Delta t_{\mathrm{emit}}=\gamma\Delta\tau=\boxed{1.25\,\mu\mathrm s}.Δx=vΔtemit.\Delta x=v\Delta t_{\mathrm{emit}}.

(b) Interpretation and further calculation

ΔtR=Δtemit+Δx/c=γ(1+β)Δτ.\Delta t_R=\Delta t_{\mathrm{emit}}+\Delta x/c=\gamma(1+\beta)\Delta\tau.ΔtR=2.00μs=1.25μs+0.75μs.\boxed{\Delta t_R=2.00\,\mu\mathrm s=1.25\,\mu\mathrm s+0.75\,\mu\mathrm s}.

Physical check

Time dilation concerns assigned emission times; the directly observed arrival spacing also contains changing propagation delay.