Given:
\[ R = R_0 A^{1/3} \]
We know that:
\[ R^3 \propto A \]
For the first nucleus:
\[ \frac{4.8^3}{A} = \frac{4^3}{64} \]
Rearranging and simplifying:
\[ \frac{64}{A} = \left(\frac{4}{4.8}\right)^3 \]
Calculating:
\[ \frac{64}{A} = (1.2)^3 \]
\[ \frac{64}{A} = 1.44 \times 1.2 \]
Next, equating for the second nucleus:
\[ \frac{1000}{x} = 64 \times 1.44 \times 12 \]
Calculating:
\[ x = 27 \]
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: