A New Look at Momentum — Question 10

Section 37-10 · Physics pages 6230–6231

Question 10 A large momentum uncertainty can correspond to a small speed uncertainty A momentum measurement gives p = (10.0 ± 0.1)mc, where the quoted uncertainty is one standard deviation and m is exactly known. Set w = p/(mc). Use p = γmv, γ = (1 −v2/c2)−1/2, and F = dp/dt. Here m is invariant mass. p v c Schematic; labels, not drawing lengths, specify the data. (a) Derive d(v/c)/dw and evaluate the central speed. (b) Find the first-order speed uncertainty and compare the fractional speed and momentum uncertainties.
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Question 10 - Solution A large momentum uncertainty can correspond to a small speed uncertainty p v c (a) Method and calculation β = w √ 1 + w2 , dβ/dw = (1 + w2)−3/2 . β = 10/ √ 101 ≃0.995037 . (b) Interpretation and further calculation σβ ≃ 0.1 1013/2 = 9.85185 × 10−5 . σv/v ≃0.01 101 = 9.90099 × 10−5 , σp/p = 0.0100. Physical check Near c, increasing momentum changes speed only weakly. The result assumes a narrow distribution for linear uncertainty propagation.

Question 10

A large momentum uncertainty can correspond to a small speed uncertainty

A momentum measurement gives p=(10.0±0.1)mcp=(10.0\pm0.1)mc, where the quoted uncertainty is one standard deviation and m is exactly known. Set w=p/(mc)w=p/(mc). 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. Derive d(v/c)/dwd(v/c)/dw and evaluate the central speed.

  2. Find the first-order speed uncertainty and compare the fractional speed and momentum uncertainties.

Question 10 - Solution

A large momentum uncertainty can correspond to a small speed uncertainty

Diagram shown in the original SVG worksheet.

(a) Method and calculation

β=w1+w2,dβ/dw=(1+w2)−3/2.\beta=\frac w{\sqrt{1+w^2}},\qquad\boxed{d\beta/dw=(1+w^2)^{-3/2}}.β=10/101≃0.995037.\boxed{\beta=10/\sqrt{101}\simeq0.995037}.

(b) Interpretation and further calculation

σβ≃0.11013/2=9.85185×10−5.\boxed{\sigma_\beta\simeq\frac{0.1}{101^{3/2}}=9.85185\times10^{-5}}.σv/v≃0.01101=9.90099×10−5,σp/p=0.0100.\boxed{\sigma_v/v\simeq\frac{0.01}{101}=9.90099\times10^{-5}},\qquad\sigma_p/p=0.0100.

Physical check

Near c, increasing momentum changes speed only weakly. The result assumes a narrow distribution for linear uncertainty propagation.