13.26 Under certain circumstances, a nucleus can decay by emitting a particle more massive than an
particle. Consider the following decay processes:
Calculate the Q-values for these decays and determine that both are energetically allowed.
13.26 Under certain circumstances, a nucleus can decay by emitting a particle more massive than an particle. Consider the following decay processes:
Calculate the Q-values for these decays and determine that both are energetically allowed.
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1 Answer
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13.26 For the emission of , the nuclear reaction is:
We know that:
Mass of , = 223.01850 u
Mass of , = 208.98107 u
Mass of , = 14.00324 u
Hence, the Q-value of the reaction is given as:
Q = ( - - )
= (223.01850 - 208.98107 - 14.00324) u
= 0.03419 u
= 0.03419 MeV = 31.848 MeV
Hence, the Q-value of the nuclear reaction is 31.848 MeV, since the value is positive, the reaction is energetically allowed.
For the emission of , the nuclear reaction is:
We know that:
Mass of , = 223.01850 u
Mass of , = 219.00948 u
Mass of , = 4.00260 u
Hence, the Q-value of the reaction is given as:
Q = ( - &n
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Q = [4 *4.0026 – 15.9994] *931.5 MeV
Q = 10.2 MeV
-(1)
for B,
for B,
-(2)
The reaction is X²? → Y¹²? + Z¹²?
Binding energies per nucleon are: X=7.6 MeV, Y=8.5 MeV, Z=8.5 MeV.
Gain in binding energy (Q) = (Binding energy of products) - (Binding energy of reactants)
Q = (120 × 8.5 + 120 × 8.5) - (240 × 7.6) MeV
Q = (2 × 120 × 8.5) - (240 × 7.6) MeV = 2040 - 1824 = 216 MeV.
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