To determine the atomic mass number \( A \) of the original nucleus, we need to consider the effect of losing two alpha particles on the original nucleus. Each alpha particle consists of 2 protons and 2 neutrons, which means it has an atomic mass number of 4.
Thus, when a nucleus loses two alpha particles, the decrease in the atomic mass number is:
\( 2 \times 4 = 8 \)
Let's denote the atomic mass number of the original nucleus as \( A \). After losing two alpha particles, the new atomic mass number becomes \( A - 8 \).
The problem states that the volume of the new nucleus is 60 times that of an alpha particle. Since the volume of a nucleus is proportional to its atomic mass number, we can express this relationship as:
\( A - 8 = 60 \times 4 \)
Solving for \( A \):
\( A - 8 = 240 \)
\( A = 240 + 8 = 248 \)
Thus, the atomic mass number \( A \) of the original nucleus is 248.
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: