Some Consequences of the Lorentz Equations — Question 8

Section 37-7 · Physics pages 6166–6167

Question 8 A hyperbolic trajectory has subluminal tangents but no single rest frame A worldline in one spatial dimension is x(t) = √ b2 + c2t2, with b > 0. Consider t ≥0. x ct Spacetime sketch; the vertical coordinate is ct. Labels specify events and worldlines. (a) Find its instantaneous velocity and show its magnitude stays below c. (b) At any event, boost with β = ct/x. Find that event coordinates and explain why this does not make the entire worldline stationary.
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Question 8 - Solution A hyperbolic trajectory has subluminal tangents but no single rest frame x ct (a) Method and calculation v = dx dt = c2t x , β = ct/x < 1 . 1 −β2 = x2 −c2t2 x2 = b2/x2, γ = x/b. (b) Interpretation and further calculation ct′ = γ(ct −βx) = 0 , x′ = γ(x −βct) = b . dβ dt = cb2 (b2 + c2t2)3/2 > 0. Physical check The required boost varies from event to event. A momentarily comoving inertial frame is not a global rest frame for accelerated motion.

Question 8

A hyperbolic trajectory has subluminal tangents but no single rest frame

A worldline in one spatial dimension is x(t)=b2+c2t2x(t)=\sqrt{b^2+c^2t^2}, with b>0b>0. Consider t≥0t\ge0.

Diagram shown in the original SVG worksheet.

  1. Find its instantaneous velocity and show its magnitude stays below c.

  2. At any event, boost with β=ct/x\beta=ct/x. Find that event coordinates and explain why this does not make the entire worldline stationary.

Question 8 - Solution

A hyperbolic trajectory has subluminal tangents but no single rest frame

Diagram shown in the original SVG worksheet.

(a) Method and calculation

v=dxdt=c2tx,β=ct/x<1.v=\frac{dx}{dt}=\frac{c^2t}{x},\quad\boxed{\beta=ct/x<1}.1−β2=x2−c2t2x2=b2/x2,γ=x/b.1-\beta^2=\frac{x^2-c^2t^2}{x^2}=b^2/x^2,\quad\gamma=x/b.

(b) Interpretation and further calculation

ct′=γ(ct−βx)=0,x′=γ(x−βct)=b.ct\prime=\gamma(ct-\beta x)=\boxed{0},\quad x\prime=\gamma(x-\beta ct)=\boxed{b}.dβdt=cb2(b2+c2t2)3/2>0.\frac{d\beta}{dt}=\frac{cb^2}{(b^2+c^2t^2)^{3/2}}>0.

Physical check

The required boost varies from event to event. A momentarily comoving inertial frame is not a global rest frame for accelerated motion.