Some Consequences of the Lorentz Equations — Question 4

Section 37-7 · Physics pages 6158–6159

Question 4 A sweeping light spot can outrun c without carrying a signal along the screen A laser at the origin aims at a screen a perpendicular distance L away. Its emission angle is θ = ωte; the illuminated screen coordinate is x = L tan θ. Light arrives at tR = te + (L/c) sec θ. Ignore material response times. θ L Schematic; labels, not drawing lengths, specify the data. (a) Derive dx/dtR from the parametric equations. (b) At θ = 0 and Lω = 2c, find the spot speed and explain why it is not communication between neighboring screen points.
Show solutionHide solution
Question 4 - Solution A sweeping light spot can outrun c without carrying a signal along the screen θ L (a) Method and calculation dx dte = Lω sec2 θ, dtR dte = 1 + Lω c sec θ tan θ. dx dtR = Lω sec2 θ 1 + (Lω/c) sec θ tan θ . (b) Interpretation and further calculation θ = 0 : dx/dtR = Lω = 2c . Each screen event receives a distinct ray from the laser at speed c. Physical check The spot is a sequence of illumination events. No object or message propagates from one spot position to the next at the sweep speed.

Question 4

A sweeping light spot can outrun c without carrying a signal along the screen

A laser at the origin aims at a screen a perpendicular distance L away. Its emission angle is θ=ωte\theta=\omega t_e; the illuminated screen coordinate is x=Ltan⁡θx=L\tan\theta. Light arrives at tR=te+(L/c)sec⁡θt_R=t_e+(L/c)\sec\theta. Ignore material response times.

Diagram shown in the original SVG worksheet.

  1. Derive dx/dtRdx/dt_R from the parametric equations.

  2. At θ=0\theta=0 and Lω=2cL\omega=2c, find the spot speed and explain why it is not communication between neighboring screen points.

Question 4 - Solution

A sweeping light spot can outrun c without carrying a signal along the screen

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dxdte=Lωsec⁡2θ,dtRdte=1+Lωcsec⁡θtan⁡θ.\frac{dx}{dt_e}=L\omega\sec^2\theta,\qquad\frac{dt_R}{dt_e}=1+\frac{L\omega}{c}\sec\theta\tan\theta.dxdtR=Lωsec⁡2θ1+(Lω/c)sec⁡θtan⁡θ.\boxed{\frac{dx}{dt_R}=\frac{L\omega\sec^2\theta}{1+(L\omega/c)\sec\theta\tan\theta}}.

(b) Interpretation and further calculation

θ=0:dx/dtR=Lω=2c.\theta=0:\quad\boxed{dx/dt_R=L\omega=2c}.Each screen event receives a distinct ray from the laser at speed c.\text{Each screen event receives a distinct ray from the laser at speed }c.

Physical check

The spot is a sequence of illumination events. No object or message propagates from one spot position to the next at the sweep speed.