To find the distance of closest approach when an \( \alpha \)-particle is projected towards a stationary target nucleus, we use the principle of conservation of energy. In this case, the initial kinetic energy (\( KE \)) of the \( \alpha \)-particle is entirely converted into electrostatic potential energy at the point of closest approach.
The formula for the distance of closest approach \( d \) is given by:
d = \frac{k \cdot Z \cdot e^2}{KE}
where:
Substitute the given values into the equation:
d = \frac{(8.99 \times 10^9) \times 79 \times (1.6 \times 10^{-19})^2}{7.9 \times 10^6 \times 1.6 \times 10^{-19}}
Simplifying the expression:
d = \frac{(8.99 \times 10^9) \times 79 \times (1.6 \times 10^{-19})}{7.9 \times 10^6}
On further calculation:
d = \frac{1.803584 \times 10^{-27}}{1.264 \times 10^{-12}}
d = 2.88 \times 10^{-14} \, \text{m}
Thus, the distance of closest approach is \( 2.88 \times 10^{-14} \, \text{m}.
Therefore, the correct answer is: \( 2.88 \times 10^{-14} \)
A small bob A of mass m is attached to a massless rigid rod of length 1 m pivoted at point P and kept at an angle of 60° with vertical. At 1 m below P, bob B is kept on a smooth surface. If bob B just manages to complete the circular path of radius R after being hit elastically by A, then radius R is_______ m :