Some Consequences of the Lorentz Equations — Question 10

Section 37-7 · Physics pages 6170–6171

Question 10 Density enhancement and lifetime dilation cancel in a local decay rate At corresponding events, a uniform unstable cloud has proper number density n0 and proper mean lifetime τ0. It moves uniformly with Lorentz factor γ. For a small laboratory volume and short interval, ignore depletion and gradients. dV dt dV ′dt′ Schematic; labels, not drawing lengths, specify the data. (a) Combine length contraction and time dilation to find decays per laboratory volume per laboratory time. (b) Check the expected count in a small spacetime cell using the unit Jacobian of a Lorentz boost.
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Question 10 - Solution Density enhancement and lifetime dilation cancel in a local decay rate dV dt dV ′dt′ (a) Method and calculation n = γn0, rper particle = 1/(γτ0). R = n rper particle = n0/τ0 . (b) Interpretation and further calculation dN = R dV dt, dV dt = dV ′ dt′. dN = (n0/τ0) dV ′ dt′ . Physical check The statement is local at corresponding events. It does not claim that densities on different distant simultaneity slices have identical histories.

Question 10

Density enhancement and lifetime dilation cancel in a local decay rate

At corresponding events, a uniform unstable cloud has proper number density n0n_0 and proper mean lifetime τ0\tau_0. It moves uniformly with Lorentz factor γ\gamma. For a small laboratory volume and short interval, ignore depletion and gradients.

Diagram shown in the original SVG worksheet.

  1. Combine length contraction and time dilation to find decays per laboratory volume per laboratory time.

  2. Check the expected count in a small spacetime cell using the unit Jacobian of a Lorentz boost.

Question 10 - Solution

Density enhancement and lifetime dilation cancel in a local decay rate

Diagram shown in the original SVG worksheet.

(a) Method and calculation

n=γn0,rperparticle=1/(γτ0).n=\gamma n_0,\qquad r_{\mathrm{per\ particle}}=1/(\gamma\tau_0).ℛ=nrperparticle=n0/τ0.\boxed{\mathcal R=n\,r_{\mathrm{per\ particle}}=n_0/\tau_0}.

(b) Interpretation and further calculation

dN=ℛdVdt,dVdt=dV′dt′.dN=\mathcal R\,dV\,dt,\qquad dV\,dt=dV\prime\,dt\prime.dN=(n0/τ0)dV′dt′.\boxed{dN=(n_0/\tau_0)\,dV\prime\,dt\prime}.

Physical check

The statement is local at corresponding events. It does not claim that densities on different distant simultaneity slices have identical histories.