The problem involves calculating the distance of closest approach of an \( \alpha \)-particle, which is a fundamental problem in electrostatics and nuclear physics. The kinetic energy of the \( \alpha \)-particle is converted entirely into electric potential energy at the distance of closest approach.
Given:
\(U = \dfrac{1}{4\pi\epsilon_0} \cdot \dfrac{qQ}{r}\)
Where:
Thus,
\(7.7 \times 10^6 \times 1.6 \times 10^{-19} = \dfrac{1}{4\pi\epsilon_0} \dfrac{2 \cdot 79 \cdot (1.6 \times 10^{-19})^2}{r}\)
Substituting for \(\dfrac{1}{4\pi\epsilon_0} = 9 \times 10^9 \, \text{Nm}^2/\text{C}^2\), we get:
\(7.7 \times 1.6 \times 10^{-13} = 9 \times 10^9 \times \dfrac{2 \times 79 \times (1.6 \times 10^{-19})^2}{r}\)
\(r = \dfrac{9 \times 10^9 \times 2 \times 79 \times (1.6 \times 10^{-19})^2}{7.7 \times 1.6 \times 10^{-13}}\)
Calculating \(r\):
\(r \approx \dfrac{9 \times 10^9 \times 2 \times 79 \times 2.56 \times 10^{-38}}{1.232 \times 10^{-12}}\)
\(r \approx 2.06 \times 10^{-10} \text{m} = 0.206 \, \text{nm}\)
Rounding to one decimal place, the distance of closest approach is approximately \(0.2 \, \text{nm}\).
Therefore, the correct answer is \( 0.2 \, \text{nm} \).