Particles, Particles, Particles — Question 6

Section 44-1 · Physics pages 7302–7303

Question 6 Momentum resolution limits mass identification near the speed of light Infer mass from m = p √ 1 −β2/(βc). Momentum and speed errors are independent. At β = .900, let σp/p = .0100 and σβ = .00200. β σm/m Schematic; labels, not drawing lengths, specify the data. (a) Derive the leading fractional standard uncertainty in mass. (b) Evaluate it and identify the dominant contribution.
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Question 6 - Solution Momentum resolution limits mass identification near the speed of light β σm/m (a) Method and calculation d ln m = d ln p − dβ β(1 −β2). (σm m )2 = (σp p )2 + [ σβ β(1 −β2) ]2 . (b) Interpretation and further calculation σm/m = √ .01002 + [.00200/(.900 · .190)]2 = .0153881 . speed term = .0116959 > momentum term = .0100 . Physical check The speed sensitivity diverges as beta approaches one. This is linear uncertainty propagation and assumes errors small enough for local derivatives to apply.

Question 6

Momentum resolution limits mass identification near the speed of light

Infer mass from m=p1−β2/(βc)m=p\sqrt{1-\beta^2}/(\beta c). Momentum and speed errors are independent. At β=.900\beta=.900, let σp/p=.0100\sigma_p/p=.0100 and σβ=.00200\sigma_\beta=.00200.

Diagram shown in the original SVG worksheet.

  1. Derive the leading fractional standard uncertainty in mass.

  2. Evaluate it and identify the dominant contribution.

Question 6 - Solution

Momentum resolution limits mass identification near the speed of light

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dln⁡m=dln⁡p−dββ(1−β2).d\ln m=d\ln p-\frac{d\beta}{\beta(1-\beta^2)}.(σmm)2=(σpp)2+[σββ(1−β2)]2.\boxed{\left(\frac{\sigma_m}{m}\right)^2=\left(\frac{\sigma_p}{p}\right)^2+\left[\frac{\sigma_\beta}{\beta(1-\beta^2)}\right]^2}.

(b) Interpretation and further calculation

σm/m=.01002+[.00200/(.900⋅.190)]2=.0153881.\boxed{\sigma_m/m=\sqrt{.0100^2+[.00200/(.900\cdot.190)]^2}=.0153881}.speed term=.0116959>momentum term=.0100.\boxed{\text{speed term}=.0116959>\text{momentum term}=.0100}.

Physical check

The speed sensitivity diverges as beta approaches one. This is linear uncertainty propagation and assumes errors small enough for local derivatives to apply.