A New Look at Momentum — Question 9

Section 37-10 · Physics pages 6228–6229

Question 9 Deflecting momentum through an angle requires a vector impulse A particle moves at 0.80c before and after a scattering event. Its velocity is initially along +x and finally at 60◦above +x. Use p = γmv, γ = (1 −v2/c2)−1/2, and F = dp/dt. Here m is invariant mass. pi pf J Schematic; labels, not drawing lengths, specify the data. (a) Find the x and y components of impulse. (b) Find the impulse magnitude and derive its dependence on a general deflection angle χ.
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Question 9 - Solution Deflecting momentum through an angle requires a vector impulse pi pf J (a) Method and calculation p = γmv = 4 3mc, Jx = p(cos 60◦−1) = −2 3mc . Jy = p sin 60◦= 2 √ 3 3 mc . (b) Interpretation and further calculation |J|2 = p2[(cos χ −1)2 + sin2 χ] = 4p2 sin2(χ/2). |J| = 2p| sin(χ/2)| = 4 3mc (χ = 60◦) . Physical check Unchanged momentum magnitude does not imply unchanged momentum vector. The net impulse is the chord between the initial and final vectors.

Question 9

Deflecting momentum through an angle requires a vector impulse

A particle moves at 0.80c0.80c before and after a scattering event. Its velocity is initially along +x and finally at 60∘60^\circ above +x. 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. Find the x and y components of impulse.

  2. Find the impulse magnitude and derive its dependence on a general deflection angle χ\chi.

Question 9 - Solution

Deflecting momentum through an angle requires a vector impulse

Diagram shown in the original SVG worksheet.

(a) Method and calculation

p=γmv=43mc,Jx=p(cos⁡60∘−1)=−23mc.p=\gamma mv=\frac43mc,\quad J_x=p(\cos60^\circ-1)=\boxed{-\frac23mc}.Jy=psin⁡60∘=233mc.J_y=p\sin60^\circ=\boxed{\frac{2\sqrt3}3mc}.

(b) Interpretation and further calculation

|𝑱|2=p2[(cos⁡χ−1)2+sin⁡2χ]=4p2sin⁡2(χ/2).|\mathbf J|^2=p^2[(\cos\chi-1)^2+\sin^2\chi]=4p^2\sin^2(\chi/2).|𝑱|=2p|sin⁡(χ/2)|=43mc(χ=60∘).\boxed{|\mathbf J|=2p|\sin(\chi/2)|=\frac43mc\quad(\chi=60^\circ)}.

Physical check

Unchanged momentum magnitude does not imply unchanged momentum vector. The net impulse is the chord between the initial and final vectors.