The Relativity of Length — Question 5

Section 37-5 · Physics pages 6120–6121

Question 5 A longitudinal light clock reconciles unequal laboratory legs A rod of proper length L0 = 300 m moves at v = 0.60c. A pulse leaves its rear, reflects immediately at its front, and returns to its rear. Both endpoints move with the rod. Use γ = (1 −v2/c2)−1/2 and c = 3.00 × 108 m/s. x ct Spacetime sketch; the vertical coordinate is ct. Labels specify events and worldlines. (a) Find the laboratory outward and return travel times. (b) Find the elapsed proper time on the rear clock and compare with 2L0/c.
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Question 5 - Solution A longitudinal light clock reconciles unequal laboratory legs x ct (a) Method and calculation L = L0/γ = 240 m, t+ = L/(c −v) = 2.00 µs . t−= L/(c + v) = 0.500 µs . (b) Interpretation and further calculation T = t+ + t−= 2.50 µs, τ = T/γ. τ = 2.00 µs = 2L0/c . Physical check The moving rear meets the returning pulse, so its return distance is shorter in the laboratory. A fixed-source mirror problem has different endpoints.

Question 5

A longitudinal light clock reconciles unequal laboratory legs

A rod of proper length L0=300mL_0=300\,\mathrm m moves at v=0.60cv=0.60c. A pulse leaves its rear, reflects immediately at its front, and returns to its rear. Both endpoints move with the rod. Use γ=(1−v2/c2)−1/2\gamma=(1-v^2/c^2)^{-1/2} and c=3.00×108m/sc=3.00\times10^8\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find the laboratory outward and return travel times.

  2. Find the elapsed proper time on the rear clock and compare with 2L0/c2L_0/c.

Question 5 - Solution

A longitudinal light clock reconciles unequal laboratory legs

Diagram shown in the original SVG worksheet.

(a) Method and calculation

L=L0/γ=240m,t+=L/(c−v)=2.00μs.L=L_0/\gamma=240\,\mathrm m,\quad t_+=L/(c-v)=\boxed{2.00\,\mu\mathrm s}.t−=L/(c+v)=0.500μs.t_-=L/(c+v)=\boxed{0.500\,\mu\mathrm s}.

(b) Interpretation and further calculation

T=t++t−=2.50μs,τ=T/γ.T=t_++t_-=2.50\,\mu\mathrm s,\quad\tau=T/\gamma.τ=2.00μs=2L0/c.\boxed{\tau=2.00\,\mu\mathrm s=2L_0/c}.

Physical check

The moving rear meets the returning pulse, so its return distance is shorter in the laboratory. A fixed-source mirror problem has different endpoints.