The Traveling Electromagnetic Wave, Qualitatively — Question 8

Section 33-2 · Physics pages 5406–5407

Question 8 A moving sampler crosses fewer wave crests when it follows the wave A laboratory wave has phase ϕ = kx −ωt with omega=ck. A sampler moves along x=ut, where |u| < c. Its readings are indexed by laboratory time t, not by its own proper time. x E c sampler u Schematic; labels, not drawing lengths, specify the data. (a) Find the angular oscillation frequency in the recorded laboratory-time trace. (b) Compare the observed cycle rates for u=+c/4 and u=-c/4. Explain why this is not the full relativistic Doppler formula.
Show solutionHide solution
Question 8 - Solution A moving sampler crosses fewer wave crests when it follows the wave x E c sampler u (a) Method and calculation ϕ(t) = (ku −ω)t = −ω(1 −u/c)t. ωtrace = ω(1 −u/c) (|u| < c). (b) Interpretation and further calculation ω+ = 3ω/4, ω−= 5ω/4, ω−/ω+ = 5/3 . Proper-time rate = γωtrace, γ = (1 −u2/c2)−1/2. Physical check The defined laboratory clock avoids confusing crest-crossing kinematics with the time read by a moving observer.

Question 8

A moving sampler crosses fewer wave crests when it follows the wave

A laboratory wave has phase ϕ=kx−ωt\phi=kx-\omega t with omega=ck. A sampler moves along x=ut, where |u|<c|u|<c. Its readings are indexed by laboratory time t, not by its own proper time.

Diagram shown in the original SVG worksheet.

  1. Find the angular oscillation frequency in the recorded laboratory-time trace.

  2. Compare the observed cycle rates for u=+c/4 and u=-c/4. Explain why this is not the full relativistic Doppler formula.

Question 8 - Solution

A moving sampler crosses fewer wave crests when it follows the wave

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ϕ(t)=(ku−ω)t=−ω(1−u/c)t.\phi(t)=(ku-\omega)t=-\omega(1-u/c)t.ωtrace=ω(1−u/c)(|u|<c).\boxed{\omega_{\mathrm{trace}}=\omega(1-u/c)}\quad(|u|<c).

(b) Interpretation and further calculation

ω+=3ω/4,ω−=5ω/4,ω−/ω+=5/3.\boxed{\omega_+=3\omega/4,\quad\omega_-=5\omega/4,\quad\omega_-/\omega_+=5/3}.Proper-time rate=γωtrace,γ=(1−u2/c2)−1/2.\text{Proper-time rate}=\gamma\omega_{\mathrm{trace}},\quad\gamma=(1-u^2/c^2)^{-1/2}.

Physical check

The defined laboratory clock avoids confusing crest-crossing kinematics with the time read by a moving observer.