The Doppler Effect — Question 1

Section 17-8 · Physics pages 2772–2773

Question 1 Equal closing speeds do not imply identical Doppler shifts In still air with c = 340 m/s, a source emits fs = 500 Hz. Compare (A) an observer moving toward a stationary source at 34 m/s and (B) a source moving toward a stationary observer at the same speed. All motion is along the line joining them. S O Two separate experiments exchange which endpoint moves toward the other. (a) Derive and calculate the observed frequency in each case. (b) Explain why equal source-observer closing speed gives different results, and compare their first-order small-speed expansions.
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Question 1 - Solution Equal closing speeds do not imply identical Doppler shifts S O (a) Method and calculation In A, stationary-source wavelength is λ = c/fs, and the observer encounters fronts at speed c + v: fA = fs(1 + v/c) = 550 Hz. In B, successive fronts are separated by (c −v)/fs, so fB = cfs c −v = 555.556 Hz. (b) Interpretation and further calculation The moving observer changes the rate of encountering an existing wave train; the moving source changes the wavefront spacing in the medium. With M = v/c, fA/fs = 1 + M, fB/fs = (1 −M)−1 = 1 + M + M2 + · · · . They agree to first order and differ at higher orders. Acoustic motion is referenced to the medium. Physical check Both approaching configurations raise frequency; both reduce to fs when the speed vanishes.

Question 1

Equal closing speeds do not imply identical Doppler shifts

In still air with c=340m/sc=340\,\mathrm{m/s}, a source emits fs=500Hzf_s=500\,\mathrm{Hz}. Compare (A) an observer moving toward a stationary source at 34m/s34\,\mathrm{m/s} and (B) a source moving toward a stationary observer at the same speed. All motion is along the line joining them.

Diagram shown in the original SVG worksheet.

  1. Derive and calculate the observed frequency in each case.

  2. Explain why equal source-observer closing speed gives different results, and compare their first-order small-speed expansions.

Question 1 - Solution

Equal closing speeds do not imply identical Doppler shifts

Diagram shown in the original SVG worksheet.

(a) Method and calculation

In A, stationary-source wavelength is λ=c/fs\lambda=c/f_s, and the observer encounters fronts at speed c+vc+v:fA=fs(1+v/c)=550Hz.f_A=f_s(1+v/c)=550\,\mathrm{Hz}.In B, successive fronts are separated by (c−v)/fs(c-v)/f_s, sofB=cfsc−v=555.556Hz.f_B=\frac{cf_s}{c-v}=555.556\,\mathrm{Hz}.

(b) Interpretation and further calculation

The moving observer changes the rate of encountering an existing wave train; the moving source changes the wavefront spacing in the medium. With M=v/cM=v/c,fA/fs=1+M,fB/fs=(1−M)−1=1+M+M2+⋯.f_A/f_s=1+M,\qquad f_B/f_s=(1-M)^{-1}=1+M+M^2+\cdots.They agree to first order and differ at higher orders. Acoustic motion is referenced to the medium.

Physical check

Both approaching configurations raise frequency; both reduce to fsf_s when the speed vanishes.