The Relativity of Velocities — Question 10

Section 37-8 · Physics pages 6190–6191

Question 10 Velocity uncertainty is compressed nonlinearly by a known boost For fixed v = 0.60c, a collinear launch has u′ = 0.50c with small standard uncertainty σu′ = 0.001c. Treat the boost as exactly known. For S′ moving at +v along x, use ux = (ux′ + v)/(1 + vux′/c2) and uy = uy′/[γv(1 + vux′/c2)], with γv = (1 −v2/c2)−1/2. u′ u c Schematic; labels, not drawing lengths, specify the data. (a) Find the laboratory velocity and derivative du/du′. (b) Propagate the uncertainty to first order and explain why simple addition would give a different uncertainty.
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Question 10 - Solution Velocity uncertainty is compressed nonlinearly by a known boost u′ u c (a) Method and calculation u/c = .50 + .60 1 + .60(.50) = 11/13 . du du′ = 1 −v2/c2 (1 + vu′/c2)2 = 64 169 . (b) Interpretation and further calculation σu ≃|du/du′| σu′ = 0.000378698c . uclassical = u′ + v ⇒ σu,classical = 0.001c. Physical check This is a local linear propagation of a small statistical uncertainty, not an exact bound for a broad velocity distribution.

Question 10

Velocity uncertainty is compressed nonlinearly by a known boost

For fixed v=0.60cv=0.60c, a collinear launch has u′=0.50cu\prime=0.50c with small standard uncertainty σu′=0.001c\sigma_{u\prime}=0.001c. Treat the boost as exactly known. For S′S\prime moving at +v along x, use ux=(ux′+v)/(1+vux′/c2)u_x=(u_x\prime+v)/(1+vu_x\prime/c^2) and uy=uy′/[γv(1+vux′/c2)]u_y=u_y\prime/[\gamma_v(1+vu_x\prime/c^2)], with γv=(1−v2/c2)−1/2\gamma_v=(1-v^2/c^2)^{-1/2}.

Diagram shown in the original SVG worksheet.

  1. Find the laboratory velocity and derivative du/du′du/du\prime.

  2. Propagate the uncertainty to first order and explain why simple addition would give a different uncertainty.

Question 10 - Solution

Velocity uncertainty is compressed nonlinearly by a known boost

Diagram shown in the original SVG worksheet.

(a) Method and calculation

u/c=.50+.601+.60(.50)=11/13.\boxed{u/c=\frac{.50+.60}{1+.60(.50)}=11/13}.dudu′=1−v2/c2(1+vu′/c2)2=64169.\boxed{\frac{du}{du\prime}=\frac{1-v^2/c^2}{(1+vu\prime/c^2)^2}=\frac{64}{169}}.

(b) Interpretation and further calculation

σu≃|du/du′|σu′=0.000378698c.\sigma_u\simeq\left|du/du\prime\right|\sigma_{u\prime}=\boxed{0.000378698c}.uclassical=u′+v⇒σu,classical=0.001c.u_{\mathrm{classical}}=u\prime+v\quad\Rightarrow\quad\sigma_{u,\mathrm{classical}}=0.001c.

Physical check

This is a local linear propagation of a small statistical uncertainty, not an exact bound for a broad velocity distribution.