Collision of alpha with Be -> C + gamma

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SUMMARY

The discussion centers on the nuclear reaction involving alpha particles and beryllium, specifically the reaction α + 9Be → 13C + γ. Participants calculated the Q value for this reaction and determined the energy of the 13C nucleus when bombarded with 5-MeV alpha particles. The calculations confirmed that neglecting the momentum of the emitted gamma ray simplifies the problem without significantly affecting the accuracy of the results. The mass values used were m(4He) = 4.0026u, m(9Be) = 9.0122u, and m(13C) = 13.0034u.

PREREQUISITES
  • Understanding of nuclear reactions and conservation laws
  • Familiarity with mass-energy equivalence (E=mc²)
  • Knowledge of mass excess calculations in nuclear physics
  • Basic proficiency in performing energy calculations in nuclear reactions
NEXT STEPS
  • Study the derivation of the Q value in nuclear reactions
  • Learn about the implications of momentum conservation in particle physics
  • Explore advanced topics in gamma radiation and its interactions
  • Investigate the role of mass excess in nuclear stability and decay
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This discussion is beneficial for physics students, nuclear physicists, and educators focusing on nuclear reactions and energy calculations in particle physics.

Elvis 123456789
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Homework Statement


Before the discovery of the neutron, it was proposed that the penetrating radiation produced when beryllium was bombarded with alpha particles consisted of high-energy &gamma rays (up to 50 MeV) produced in reactions such as α + 9Be --> 13C + γ

a.) Calculate the Q value for this reaction.

b.) If 5-MeV alpha particles are incident on 9Be, calculate the energy of the 13C nucleus and, hence, determine the energy of gamma radiation assuming it is emitted as a single photon. Hint: You may neglect the momentum of the γ ray relative to the 13C nucleus. Masses: m(4He) = 4.0026u, m(9Be) = 9.0122u, m(13C) = 13.0034u

Homework Equations


m(Z, N) = A*1u +Δ where the Δ stands for the mass excess and A = Z + N

Q = (mc + md - ma - mb)c2

The Attempt at a Solution


My main gripe with this problem is that i don't understand why we can neglect the momentum of the gamma ray when conserving momentum. I did the problem with the assumption but can the problem still be done without it?
 
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Elvis 123456789 said:
I did the problem with the assumption but can the problem still be done without it?
Sure, it just makes the calculation a bit more complex, and it leads to the same answer within the precision you can achieve with the given mass numbers as the assumption is a very good approximation.
 

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