The Relativity of Velocities — Question 4

Section 37-8 · Physics pages 6178–6179

Question 4 A transverse launch acquires longitudinal motion and a reduced transverse component A probe is launched with ux′ = 0 and uy′ = 0.80c from a spacecraft moving at v = 0.60c. 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. ux uy u Schematic; labels, not drawing lengths, specify the data. (a) Find both laboratory velocity components and the total speed. (b) Find the total Lorentz factor and check it against the product of the spacecraft and launch factors.
Show solutionHide solution
Question 4 - Solution A transverse launch acquires longitudinal motion and a reduced transverse component ux uy u (a) Method and calculation ux = 0.60c , uy = 0.80c/1.25 = 0.64c . |u|/c = √ .602 + .642 = √ 481/25 ≃0.877268 . (b) Interpretation and further calculation γu = (1 −481/625)−1/2 = 25/12 . γvγu′ = (5/4)(5/3) = 25/12 . Physical check Transverse velocity does not stay unchanged because elapsed time transforms even when the transverse coordinate does not.

Question 4

A transverse launch acquires longitudinal motion and a reduced transverse component

A probe is launched with ux′=0u_x\prime=0 and uy′=0.80cu_y\prime=0.80c from a spacecraft moving at v=0.60cv=0.60c. 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 both laboratory velocity components and the total speed.

  2. Find the total Lorentz factor and check it against the product of the spacecraft and launch factors.

Question 4 - Solution

A transverse launch acquires longitudinal motion and a reduced transverse component

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ux=0.60c,uy=0.80c/1.25=0.64c.\boxed{u_x=0.60c},\qquad\boxed{u_y=0.80c/1.25=0.64c}.|𝒖|/c=.602+.642=481/25≃0.877268.\boxed{|\mathbf u|/c=\sqrt{.60^2+.64^2}=\sqrt{481}/25\simeq0.877268}.

(b) Interpretation and further calculation

γu=(1−481/625)−1/2=25/12.\gamma_u=(1-481/625)^{-1/2}=\boxed{25/12}.γvγu′=(5/4)(5/3)=25/12.\gamma_v\gamma_{u\prime}=(5/4)(5/3)=\boxed{25/12}.

Physical check

Transverse velocity does not stay unchanged because elapsed time transforms even when the transverse coordinate does not.