Doppler Effect for Light — Question 6

Section 37-9 · Physics pages 6202–6203

Question 6 Reflection from a receding mirror produces two Doppler factors A plane mirror recedes along +x at v = 0.20c. A laboratory wave of frequency f = 10.0 GHz propagates along +x, reflects backward, and returns. The mirror is massive enough that recoil is negligible; reflection preserves frequency in its rest frame. f fR v Schematic; labels, not drawing lengths, specify the data. (a) Transform to the mirror frame and back to derive the returned frequency ratio. (b) Find the return frequency and compare the fractional shift with the small-speed approximation −2β.
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Question 6 - Solution Reflection from a receding mirror produces two Doppler factors f fR v (a) Method and calculation fM = γ(1 −β)f, fR = γ(1 −β)fM. fR/f = γ2(1 −β)2 = 1 −β 1 + β . (b) Interpretation and further calculation fR = (2/3)(10.0) = 6.66667 GHz . (fR −f)/f = −1/3 , −2β = −0.400. Physical check The two factors correspond to incident and reflected propagation. A one-way shift would underestimate the reflection effect.

Question 6

Reflection from a receding mirror produces two Doppler factors

A plane mirror recedes along +x at v=0.20cv=0.20c. A laboratory wave of frequency f=10.0GHzf=10.0\,\mathrm{GHz} propagates along +x, reflects backward, and returns. The mirror is massive enough that recoil is negligible; reflection preserves frequency in its rest frame.

Diagram shown in the original SVG worksheet.

  1. Transform to the mirror frame and back to derive the returned frequency ratio.

  2. Find the return frequency and compare the fractional shift with the small-speed approximation −2β-2\beta.

Question 6 - Solution

Reflection from a receding mirror produces two Doppler factors

Diagram shown in the original SVG worksheet.

(a) Method and calculation

fM=γ(1−β)f,fR=γ(1−β)fM.f_M=\gamma(1-\beta)f,\qquad f_R=\gamma(1-\beta)f_M.fR/f=γ2(1−β)2=1−β1+β.\boxed{f_R/f=\gamma^2(1-\beta)^2=\frac{1-\beta}{1+\beta}}.

(b) Interpretation and further calculation

fR=(2/3)(10.0)=6.66667GHz.\boxed{f_R=(2/3)(10.0)=6.66667\,\mathrm{GHz}}.(fR−f)/f=−1/3,−2β=−0.400.\boxed{(f_R-f)/f=-1/3},\qquad-2\beta=-0.400.

Physical check

The two factors correspond to incident and reflected propagation. A one-way shift would underestimate the reflection effect.