Doppler Effect for Light — Question 9

Section 37-9 · Physics pages 6208–6209

Question 9 Opposite sightlines provide a consistency test for Doppler data A source with known rest frequency f0 = 500 MHz is reportedly observed at f1 = 800 MHz and f2 = 400 MHz along opposite laboratory directions θ and π −θ. 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. f1 f2 v Schematic; labels, not drawing lengths, specify the data. (a) Eliminate the unknown angle to infer γ. (b) Decide whether any physical speed and angle can produce the data under this model.
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Question 9 - Solution Opposite sightlines provide a consistency test for Doppler data f1 f2 v (a) Method and calculation 1 f1 = γ f0 (1 −β cos θ), 1 f2 = γ f0 (1 + β cos θ). γ = f0 2 ( 1 f1 + 1 f2 ) . (b) Interpretation and further calculation γ = 250 ( 1 800 + 1 400 ) = 0.9375 . γ ≥1 ⇒ no physical solution . Physical check An algebraic fit that demands gamma below one fails the physical admissibility test; at least one measurement or model assumption is inconsistent.

Question 9

Opposite sightlines provide a consistency test for Doppler data

A source with known rest frequency f0=500MHzf_0=500\,\mathrm{MHz} is reportedly observed at f1=800MHzf_1=800\,\mathrm{MHz} and f2=400MHzf_2=400\,\mathrm{MHz} along opposite laboratory directions θ\theta and π−θ\pi-\theta. 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. Eliminate the unknown angle to infer γ\gamma.

  2. Decide whether any physical speed and angle can produce the data under this model.

Question 9 - Solution

Opposite sightlines provide a consistency test for Doppler data

Diagram shown in the original SVG worksheet.

(a) Method and calculation

1f1=γf0(1−βcos⁡θ),1f2=γf0(1+βcos⁡θ).\frac1{f_1}=\frac\gamma{f_0}(1-\beta\cos\theta),\quad\frac1{f_2}=\frac\gamma{f_0}(1+\beta\cos\theta).γ=f02(1f1+1f2).\boxed{\gamma=\frac{f_0}2\left(\frac1{f_1}+\frac1{f_2}\right)}.

(b) Interpretation and further calculation

γ=250(1800+1400)=0.9375.\gamma=250\left(\frac1{800}+\frac1{400}\right)=\boxed{0.9375}.γ≥1⇒no physical solution.\gamma\ge1\quad\Rightarrow\quad\boxed{\text{no physical solution}}.

Physical check

An algebraic fit that demands gamma below one fails the physical admissibility test; at least one measurement or model assumption is inconsistent.