To solve this problem, we need to understand the concept of the closest approach in Rutherford scattering experiments. The closest approach r_0 is the minimum distance between a projectile (charged particle) and a target nucleus during a scattering event. It can be understood using the principles of conservation of energy.
The total energy of the system before scattering is essentially kinetic energy, due to the incoming projectile, and potential energy at the closest approach. The formula for electrostatic potential energy U at the distance of closest approach is given by:
U = \dfrac{k \cdot Z_1 \cdot Z_2 \cdot e^2}{r_0}
Where:
The energy of the projectile is primarily kinetic and therefore at the point of closest approach, it is completely converted into potential energy. Thus, the initial kinetic energy K of the projectile is equal to U, so:
K = \dfrac{k \cdot Z_1 \cdot Z_2 \cdot e^2}{r_0}
This shows that the kinetic energy is directly proportional to the product Z_1 Z_2.
Analyzing the given options:
Therefore, the correct answer is that the energy of the projectile is directly proportional to Z_1 Z_2.