The mass defect \( \Delta m \) for a deuteron is the difference between the mass of the deuteron and the sum of the masses of its constituent nucleons (proton and neutron): \[ \Delta m = (m_p + m_n) - m_{\text{deuteron}} \] Substitute the given values: \[ \Delta m = (1.007277 + 1.008665) - 2.01355 = 0.002392 \, \text{u} \] The energy equivalent of the mass defect is: \[ E = \Delta m \cdot 931.5 \, \text{MeV/c}^2 = 0.002392 \times 931.5 = 2.23 \, \text{MeV} \] Thus, the mass defect is \( 0.002392 \, \text{u} \), and the energy equivalence is \( 2.23 \, \text{MeV} \).
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: