Doppler Effect for Light — Question 4

Section 37-9 · Physics pages 6198–6199

Question 4 Transverse Doppler shifts depend on which frame defines transverse A source moves at v = 0.60c. Compare photons emitted at laboratory angle θ = 90◦with photons emitted at source-frame angle θ′ = 90◦. For a source of rest frequency f0 moving at +v, use f = f0/[γ(1 −β cos θ)], where β = v/c and θ is the photon propagation angle from +x in the laboratory. θ = 90◦ θ′ = 90◦ v Schematic; labels, not drawing lengths, specify the data. (a) Find the frequency ratio for laboratory-transverse emission. (b) Using f = γf0(1 + β cos θ′), find the ratio for source-transverse emission and explain the difference.
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Question 4 - Solution Transverse Doppler shifts depend on which frame defines transverse θ = 90◦ θ′ = 90◦ v (a) Method and calculation θ = 90◦: f/f0 = 1/γ = 0.800 . cos θ′ = cos θ −β 1 −β cos θ = −0.600. (b) Interpretation and further calculation θ′ = 90◦: f/f0 = γ = 1.250 . cos θ = cos θ′ + β 1 + β cos θ′ = 0.600. Physical check The two cases refer to different photons and different angles. The red and blue factors are therefore consistent.

Question 4

Transverse Doppler shifts depend on which frame defines transverse

A source moves at v=0.60cv=0.60c. Compare photons emitted at laboratory angle θ=90∘\theta=90^\circ with photons emitted at source-frame angle θ′=90∘\theta\prime=90^\circ. For a source of rest frequency f0f_0 moving at +v, use f=f0/[γ(1−βcos⁡θ)]f=f_0/[\gamma(1-\beta\cos\theta)], where β=v/c\beta=v/c and θ\theta is the photon propagation angle from +x in the laboratory.

Diagram shown in the original SVG worksheet.

  1. Find the frequency ratio for laboratory-transverse emission.

  2. Using f=γf0(1+βcos⁡θ′)f=\gamma f_0(1+\beta\cos\theta\prime), find the ratio for source-transverse emission and explain the difference.

Question 4 - Solution

Transverse Doppler shifts depend on which frame defines transverse

Diagram shown in the original SVG worksheet.

(a) Method and calculation

θ=90∘:f/f0=1/γ=0.800.\theta=90^\circ:\quad\boxed{f/f_0=1/\gamma=0.800}.cos⁡θ′=cos⁡θ−β1−βcos⁡θ=−0.600.\cos\theta\prime=\frac{\cos\theta-\beta}{1-\beta\cos\theta}=-0.600.

(b) Interpretation and further calculation

θ′=90∘:f/f0=γ=1.250.\theta\prime=90^\circ:\quad\boxed{f/f_0=\gamma=1.250}.cos⁡θ=cos⁡θ′+β1+βcos⁡θ′=0.600.\cos\theta=\frac{\cos\theta\prime+\beta}{1+\beta\cos\theta\prime}=0.600.

Physical check

The two cases refer to different photons and different angles. The red and blue factors are therefore consistent.