Nuclear Fission: The Basic Process โ€” Question 9

Section 43-1 ยท Physics pages 7168โ€“7169

Question 9 Missing momentum reveals why two fragments need not be back to back In a compound-nucleus rest frame, measured fragment momenta are p1 = (100, 0) MeV/c and p2 = (โˆ’96, 3) MeV/c. Assume the only unobserved momentum is carried by one neutron with mnc2 = 939 MeV. p1 p2 pn Schematic; labels, not drawing lengths, specify the data. (a) Find the neutron momentum vector and direction relative to the positive x axis. (b) Estimate its kinetic energy and check the validity of the nonrelativistic formula.
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Question 9 - Solution Missing momentum reveals why two fragments need not be back to back p1 p2 pn (a) Method and calculation pn = โˆ’(p1 + p2) = (โˆ’4, โˆ’3) MeV/c . |pn| = 5 MeV/c, ฮธ = 180โ—ฆ+ tanโˆ’1(3/4) = 216.87โ—ฆ. (b) Interpretation and further calculation Kn โ‰ƒ(pnc)2 2mnc2 = 25 1878 = .01331 MeV . pn/(mnc) = 5/939 = .005325 โ‰ช1 . Physical check This is an ideal missing-momentum exercise. Additional photons or neutrons would prevent assigning the entire momentum de๏ฌcit to a single neutron.

Question 9

Missing momentum reveals why two fragments need not be back to back

In a compound-nucleus rest frame, measured fragment momenta are ๐’‘1=(100,0)\mathbf p_1=(100,0) MeV/c and ๐’‘2=(โˆ’96,3)\mathbf p_2=(-96,3) MeV/c. Assume the only unobserved momentum is carried by one neutron with mnc2=939m_nc^2=939 MeV.

Diagram shown in the original SVG worksheet.

  1. Find the neutron momentum vector and direction relative to the positive x axis.

  2. Estimate its kinetic energy and check the validity of the nonrelativistic formula.

Question 9 - Solution

Missing momentum reveals why two fragments need not be back to back

Diagram shown in the original SVG worksheet.

(a) Method and calculation

๐’‘n=โˆ’(๐’‘1+๐’‘2)=(โˆ’4,โˆ’3)MeV/c.\boxed{\mathbf p_n=-(\mathbf p_1+\mathbf p_2)=(-4,-3)\,\mathrm{MeV}/c}.|๐’‘n|=5MeV/c,ฮธ=180โˆ˜+tan⁡โˆ’1(3/4)=216.87โˆ˜.|\mathbf p_n|=5\,\mathrm{MeV}/c,\quad\boxed{\theta=180^\circ+\tan^{-1}(3/4)=216.87^\circ}.

(b) Interpretation and further calculation

Knโ‰ƒ(pnc)22mnc2=251878=.01331MeV.\boxed{K_n\simeq\frac{(p_nc)^2}{2m_nc^2}=\frac{25}{1878}=.01331\,\mathrm{MeV}}.pn/(mnc)=5/939=.005325โ‰ช1.\boxed{p_n/(m_nc)=5/939=.005325\ll1}.

Physical check

This is an ideal missing-momentum exercise. Additional photons or neutrons would prevent assigning the entire momentum deficit to a single neutron.