The Relativity of Simultaneity — Question 10

Section 37-3 · Physics pages 6090–6091

Question 10 Programmed emission delays can create simultaneity in a chosen frame Two fixed laboratory emitters at xA = 0 and xB = L = 1500 m are programmed to flash simultaneously in a frame moving at v = 0.60c. Set tA = 0. Use ∆t′ = γ(∆t −v∆x/c2), γ = (1 −v2/c2)−1/2; S′ moves at +v along x. Take c = 3.00 × 108 m/s. x A B detector Schematic; labels, not drawing lengths, specify the data. (a) Find the required laboratory delay at B. (b) Find when both flashes reach a detector fixed at x = L/2, and compare their arrival-time difference.
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Question 10 - Solution Programmed emission delays can create simultaneity in a chosen frame x A B detector (a) Method and calculation 0 = γ(tB −vL/c2) ⇒ tB = 3.00 µs . tB′ −tA′ = 0 . (b) Interpretation and further calculation tR,A = L/(2c) = 2.50 µs, tR,B = tB + L/(2c) = 5.50 µs. tR,B −tR,A = 3.00 µs . Physical check The midpoint detector is stationary in the laboratory; equality of emission times in a different frame does not imply equal receptions there.

Question 10

Programmed emission delays can create simultaneity in a chosen frame

Two fixed laboratory emitters at xA=0x_A=0 and xB=L=1500mx_B=L=1500\,\mathrm m are programmed to flash simultaneously in a frame moving at v=0.60cv=0.60c. Set tA=0t_A=0. Use Δt′=γ(Δt−vΔx/c2)\Delta t\prime=\gamma(\Delta t-v\Delta x/c^2), γ=(1−v2/c2)−1/2\gamma=(1-v^2/c^2)^{-1/2}; S′S\prime moves at +v along x. Take c=3.00×108m/sc=3.00\times10^8\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find the required laboratory delay at B.

  2. Find when both flashes reach a detector fixed at x=L/2x=L/2, and compare their arrival-time difference.

Question 10 - Solution

Programmed emission delays can create simultaneity in a chosen frame

Diagram shown in the original SVG worksheet.

(a) Method and calculation

0=γ(tB−vL/c2)⇒tB=3.00μs.0=\gamma(t_B-vL/c^2)\quad\Rightarrow\quad\boxed{t_B=3.00\,\mu\mathrm s}.tB′−tA′=0.\boxed{t_B\prime-t_A\prime=0}.

(b) Interpretation and further calculation

tR,A=L/(2c)=2.50μs,tR,B=tB+L/(2c)=5.50μs.t_{R,A}=L/(2c)=2.50\,\mu\mathrm s,\quad t_{R,B}=t_B+L/(2c)=5.50\,\mu\mathrm s.tR,B−tR,A=3.00μs.\boxed{t_{R,B}-t_{R,A}=3.00\,\mu\mathrm s}.

Physical check

The midpoint detector is stationary in the laboratory; equality of emission times in a different frame does not imply equal receptions there.