The "distance of closest approach" refers to the minimum distance between the incident particle (in this case, a proton) and the nucleus due to electrostatic repulsion. This occurs when the kinetic energy of the proton is entirely converted into potential energy at the closest point.
We use the concept of energy conservation here:
\[ \text{Initial kinetic energy} = \text{Final potential energy} \]
The potential energy \( U \) at the closest distance \( r \) is given by the Coulomb force formula:
\[ U = \frac{1}{4 \pi \epsilon_0} \frac{Z e^2}{r} \]
Where:
Now, equate the initial kinetic energy to the final potential energy:
\[ K.E. = U \]
The kinetic energy \( K.E. \) is given by:
\[ K.E. = \text{Energy of the proton} = 3.95 \, \text{MeV} = 3.95 \times 10^6 \times 1.6 \times 10^{-13} \, \text{J} \]
Equating the two energies:
\[ 3.95 \times 10^6 \times 1.6 \times 10^{-13} = \frac{1}{4 \pi \epsilon_0} \frac{Z e^2}{r} \]
Substituting the known values and solving for \( r \):
\[ r = \frac{1}{4 \pi \epsilon_0} \frac{Z e^2}{K.E.} \]
After substituting values:
\[ r = \frac{(9 \times 10^9) \times (79) \times (1.6 \times 10^{-19})^2}{3.95 \times 10^6 \times 1.6 \times 10^{-13}} \, \text{m} \]
Solving for \( r \), we get:
\[ r = 28.8 \times 10^{-15} \, \text{m} = 28.8 \, \text{fm} \]
Thus, the distance of closest approach is \( 28.8 \times 10^{-15} \, \text{m} \).
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: