A New Look at Momentum — Question 1

Section 37-10 · Physics pages 6212–6213

Question 1 Momentum determines a bounded speed even when p exceeds mc A massive particle has momentum magnitude p = 3mc. Use p = γmv, γ = (1 −v2/c2)−1/2, and F = dp/dt. Here m is invariant mass. p/(mc) v/c 1 Schematic; labels, not drawing lengths, specify the data. (a) Invert the momentum relation to find its speed and Lorentz factor. (b) Compare its momentum with the classical value at that same speed.
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Question 1 - Solution Momentum determines a bounded speed even when p exceeds mc p/(mc) v/c 1 (a) Method and calculation ( p mc )2 = β2 1 −β2 ⇒ β = p/(mc) √ 1 + [p/(mc)]2 . v = 3c/ √ 10 , γ = √ 10 . (b) Interpretation and further calculation pcl = mv = 3mc/ √ 10. p/pcl = √ 10 , v < c. Physical check Momentum has no finite upper bound, but a finite momentum always gives a subluminal speed for nonzero mass.

Question 1

Momentum determines a bounded speed even when p exceeds mc

A massive particle has momentum magnitude p=3mcp=3mc. Use 𝒑=γm𝒗\mathbf p=\gamma m\mathbf v, γ=(1−v2/c2)−1/2\gamma=(1-v^2/c^2)^{-1/2}, and 𝑭=d𝒑/dt\mathbf F=d\mathbf p/dt. Here m is invariant mass.

Diagram shown in the original SVG worksheet.

  1. Invert the momentum relation to find its speed and Lorentz factor.

  2. Compare its momentum with the classical value at that same speed.

Question 1 - Solution

Momentum determines a bounded speed even when p exceeds mc

Diagram shown in the original SVG worksheet.

(a) Method and calculation

(pmc)2=β21−β2⇒β=p/(mc)1+[p/(mc)]2.\left(\frac p{mc}\right)^2=\frac{\beta^2}{1-\beta^2}\quad\Rightarrow\quad\boxed{\beta=\frac{p/(mc)}{\sqrt{1+[p/(mc)]^2}}}.v=3c/10,γ=10.\boxed{v=3c/\sqrt{10}},\qquad\boxed{\gamma=\sqrt{10}}.

(b) Interpretation and further calculation

pcl=mv=3mc/10.p_{\mathrm{cl}}=mv=3mc/\sqrt{10}.p/pcl=10,v<c.\boxed{p/p_{\mathrm{cl}}=\sqrt{10}},\qquad v<c.

Physical check

Momentum has no finite upper bound, but a finite momentum always gives a subluminal speed for nonzero mass.