Mass Defect and Energy Released in the Fission of \( ^{235}_{92}\text{U} \)
When a neutron collides with \( ^{235}_{92}\text{U} \), the nucleus gives \( ^{140}_{54}\text{Xe} \) and \( ^{94}_{38}\text{Sr} \) as fission products, and two neutrons are ejected. Calculate the mass defect and the energy released (in MeV) in the process.
Given:
The total mass changes during this fission process. The mass defect \( \Delta m \) is the difference between the initial mass and the mass of the fission products.
\[ \Delta m = m(\text{Initial mass}) - m(\text{Final mass}) \]
The initial mass comprises the \( ^{235}_{92}\text{U} \) nucleus and a neutron:
\[ m_{\text{initial}} = m(^{235}_{92}\text{U}) + m(^{1}_0n) \]
Using the provided values:
\[ m_{\text{initial}} = 235.04393 + 1.00866 = 236.05259 \, \text{u} \]
The final mass consists of the \( ^{140}_{54}\text{Xe} \) and \( ^{94}_{38}\text{Sr} \) nuclei along with two neutrons:
\[ m_{\text{final}} = m(^{140}_{54}\text{Xe}) + m(^{94}_{38}\text{Sr}) + 2 \times m(^{1}_0n) \]
Substituting the given values:
\[ m_{\text{final}} = 139.92164 + 93.91536 + 2 \times 1.00866 = 235.85432 \, \text{u} \]
The mass defect is calculated as:
\[ \Delta m = 236.05259 - 235.85432 = 0.19827 \, \text{u} \]
The energy released is determined using the mass-energy equivalence \( E = \Delta m \times 931 \, \text{MeV}/c^2 \):
\[ E = 0.19827 \times 931 = 184.59 \, \text{MeV} \]
The energy released in this process is \( \boxed{184.59} \, \text{MeV} \).
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