The Relativity of Length — Question 9

Section 37-5 · Physics pages 6128–6129

Question 9 A measured rotation of a rod determines the boost magnitude A rod makes angle θ0 = 30◦to x in its rest frame and angle θ = 45◦in simultaneous laboratory measurements. Motion is along x; transverse dimensions do not change. Use γ = (1 −v2/c2)−1/2 and c = 3.00 × 108 m/s. x y v Schematic; labels, not drawing lengths, specify the data. (a) Infer γ and |v|/c from the angle change. (b) Find the laboratory-to-proper length ratio.
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Question 9 - Solution A measured rotation of a rod determines the boost magnitude x y v (a) Method and calculation tan θ = γ tan θ0 ⇒ γ = √ 3 . |v|/c = √ 1 −1/γ2 = √ 2/3 . (b) Interpretation and further calculation ( L L0 )2 = cos2 θ0 γ2 + sin2 θ0 = 1 4 + 1 4. L/L0 = 1/ √ 2 . Physical check The angular data determine speed magnitude, not the direction of translation.

Question 9

A measured rotation of a rod determines the boost magnitude

A rod makes angle θ0=30∘\theta_0=30^\circ to x in its rest frame and angle θ=45∘\theta=45^\circ in simultaneous laboratory measurements. Motion is along x; transverse dimensions do not change. 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. Infer γ\gamma and |v|/c|v|/c from the angle change.

  2. Find the laboratory-to-proper length ratio.

Question 9 - Solution

A measured rotation of a rod determines the boost magnitude

Diagram shown in the original SVG worksheet.

(a) Method and calculation

tan⁡θ=γtan⁡θ0⇒γ=3.\tan\theta=\gamma\tan\theta_0\quad\Rightarrow\quad\boxed{\gamma=\sqrt3}.|v|/c=1−1/γ2=2/3.\boxed{|v|/c=\sqrt{1-1/\gamma^2}=\sqrt{2/3}}.

(b) Interpretation and further calculation

(LL0)2=cos⁡2θ0γ2+sin⁡2θ0=14+14.\left(\frac L{L_0}\right)^2=\frac{\cos^2\theta_0}{\gamma^2}+\sin^2\theta_0=\frac14+\frac14.L/L0=1/2.\boxed{L/L_0=1/\sqrt2}.

Physical check

The angular data determine speed magnitude, not the direction of translation.