The Doppler Effect — Question 5

Section 17-8 · Physics pages 2780–2781

Question 5 An echo from a moving target has two Doppler transformations A stationary source and receiver transmit fs = 40000 Hz toward a target receding at u = 10.0 m/s in still air with c = 340 m/s. The target reflects backward without changing frequency in its own moving frame. S, R wall u Target moves away; the pulse makes an outward and a reflected return trip. (a) Derive the returned echo frequency. (b) Find the beat rate between the echo and the transmitted reference. Compare with the low-speed approximation 2fsu/c.
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Question 5 - Solution An echo from a moving target has two Doppler transformations S, R wall u (a) Method and calculation The target first acts as a receding observer: fT = fs c −u c . It then acts as a source moving away from the original receiver, emitting backward at fT . Hence fe = fT c c + u = fs c −u c + u = 37714.286 Hz. (b) Interpretation and further calculation The echo-reference difference is fb = fs −fe = 2fsu c + u = 2285.714 Hz. The approximation gives 2(40000)(10)/340 = 2352.941 Hz, about 2.94% above the exact value. It drops the u in the denominator and is appropriate only when u/c ≪1. Physical check A receding target lowers the returned frequency twice. The echo tends to the transmitted tone as u →0.

Question 5

An echo from a moving target has two Doppler transformations

A stationary source and receiver transmit fs=40000Hzf_s=40000\,\mathrm{Hz} toward a target receding at u=10.0m/su=10.0\,\mathrm{m/s} in still air with c=340m/sc=340\,\mathrm{m/s}. The target reflects backward without changing frequency in its own moving frame.

Diagram shown in the original SVG worksheet.

  1. Derive the returned echo frequency.

  2. Find the beat rate between the echo and the transmitted reference. Compare with the low-speed approximation 2fsu/c2f_su/c.

Question 5 - Solution

An echo from a moving target has two Doppler transformations

Diagram shown in the original SVG worksheet.

(a) Method and calculation

The target first acts as a receding observer:fT=fsc−uc.f_T=f_s\frac{c-u}{c}.It then acts as a source moving away from the original receiver, emitting backward at fTf_T. Hencefe=fTcc+u=fsc−uc+u=37714.286Hz.f_e=f_T\frac c{c+u}=f_s\frac{c-u}{c+u}=37714.286\,\mathrm{Hz}.

(b) Interpretation and further calculation

The echo-reference difference isfb=fs−fe=2fsuc+u=2285.714Hz.f_b=f_s-f_e=\frac{2f_su}{c+u}=2285.714\,\mathrm{Hz}.The approximation gives 2(40000)(10)/340=2352.941Hz2(40000)(10)/340=2352.941\,\mathrm{Hz}, about 2.94%2.94\% above the exact value. It drops the uu in the denominator and is appropriate only when u/c≪1u/c\ll1.

Physical check

A receding target lowers the returned frequency twice. The echo tends to the transmitted tone as u→0u\to0.