The Relativity of Velocities — Question 6

Section 37-8 · Physics pages 6182–6183

Question 6 A backward-hemisphere photon can enter the forward hemisphere In S′ a photon propagates at θ′ = 120◦from +x. The frame moves at v = 0.80c relative to S. 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. x u′ u Schematic; labels, not drawing lengths, specify the data. (a) Find the laboratory propagation angle. (b) Derive the condition on θ′ for the laboratory x component to be positive.
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Question 6 - Solution A backward-hemisphere photon can enter the forward hemisphere x u′ u (a) Method and calculation cos θ = cos θ′ + β 1 + β cos θ′ = −.5 + .8 1 −.4 = .5 . θ = 60◦, uy/c = √ 3/2 (5/3)(.6) = √ 3/2. (b) Interpretation and further calculation 1 + β cos θ′ > 0 (|β| < 1). ux > 0 ⇐⇒cos θ′ > −β . Physical check Backward and forward hemispheres are frame dependent; the photon still propagates at c in each frame.

Question 6

A backward-hemisphere photon can enter the forward hemisphere

In S′S\prime a photon propagates at θ′=120∘\theta\prime=120^\circ from +x. The frame moves at v=0.80cv=0.80c relative to S. 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 propagation angle.

  2. Derive the condition on θ′\theta\prime for the laboratory x component to be positive.

Question 6 - Solution

A backward-hemisphere photon can enter the forward hemisphere

Diagram shown in the original SVG worksheet.

(a) Method and calculation

cos⁡θ=cos⁡θ′+β1+βcos⁡θ′=−.5+.81−.4=.5.\cos\theta=\frac{\cos\theta\prime+\beta}{1+\beta\cos\theta\prime}=\frac{-.5+.8}{1-.4}=\boxed{.5}.θ=60∘,uy/c=3/2(5/3)(.6)=3/2.\boxed{\theta=60^\circ},\qquad u_y/c=\frac{\sqrt3/2}{(5/3)(.6)}=\sqrt3/2.

(b) Interpretation and further calculation

1+βcos⁡θ′>0(|β|<1).1+\beta\cos\theta\prime>0\quad(|\beta|<1).ux>0⇔cos⁡θ′>−β.\boxed{u_x>0\ \Longleftrightarrow\ \cos\theta\prime>-\beta}.

Physical check

Backward and forward hemispheres are frame dependent; the photon still propagates at c in each frame.