$4.2$
Step 1: The nuclear radius is given by the empirical formula: \[ R = R_0 A^{1/3} \] where $A$ is the mass number and $R_0$ is a proportionality constant.
Step 2: Using the ratio of nuclear radii: \[ \frac{R_2}{R_1} = \left( \frac{A_2}{A_1} \right)^{1/3} \] Given $R_1 = 6$ fermi for $A_1 = 125$ and $A_2 = 27$, we compute: \[ R_2 = 6 \times \left( \frac{27}{125} \right)^{1/3} \]
Step 3: Approximating the cube root: \[ \left( \frac{27}{125} \right)^{1/3} = \frac{3}{5} = 0.6 \]
Step 4: \[ R_2 = 6 \times 0.6 = 3.6 { fermi} \]
Step 5: Therefore, the correct answer is (A).
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: