Doppler Effect for Light — Question 2

Section 37-9 · Physics pages 6194–6195

Question 2 Opposite emission directions separate source frequency from speed A moving monochromatic source is observed along its forward and backward laboratory directions. The frequencies are f+ = 900 MHz and f−= 100 MHz. f+ f− v Schematic; labels, not drawing lengths, specify the data. (a) Use f± = γ(1 ± β)f0 to infer f0. (b) Find the speed and Lorentz factor from the frequency sum and difference.
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Question 2 - Solution Opposite emission directions separate source frequency from speed f+ f− v (a) Method and calculation f+f−= γ2(1 −β2)f2 0 = f2 0 . f0 = √ f+f−= 300 MHz . (b) Interpretation and further calculation β = f+ −f− f+ + f− = 0.800 . γ = f+ + f− 2f0 = 5/3 . Physical check The geometric mean removes the motion while the normalized difference isolates its direction and speed.

Question 2

Opposite emission directions separate source frequency from speed

A moving monochromatic source is observed along its forward and backward laboratory directions. The frequencies are f+=900MHzf_+=900\,\mathrm{MHz} and f−=100MHzf_-=100\,\mathrm{MHz}.

Diagram shown in the original SVG worksheet.

  1. Use f±=γ(1±β)f0f_\pm=\gamma(1\pm\beta)f_0 to infer f0f_0.

  2. Find the speed and Lorentz factor from the frequency sum and difference.

Question 2 - Solution

Opposite emission directions separate source frequency from speed

Diagram shown in the original SVG worksheet.

(a) Method and calculation

f+f−=γ2(1−β2)f02=f02.f_+f_-=\gamma^2(1-\beta^2)f_0^2=f_0^2.f0=f+f−=300MHz.\boxed{f_0=\sqrt{f_+f_-}=300\,\mathrm{MHz}}.

(b) Interpretation and further calculation

β=f+−f−f++f−=0.800.\boxed{\beta=\frac{f_+-f_-}{f_++f_-}=0.800}.γ=f++f−2f0=5/3.\boxed{\gamma=\frac{f_++f_-}{2f_0}=5/3}.

Physical check

The geometric mean removes the motion while the normalized difference isolates its direction and speed.