The problem involves finding the distance of closest approach of an alpha particle to a gold nucleus. This is solved using energy conservation in electrostatics.
At the point of closest approach, the entire kinetic energy of the alpha particle is converted into electrostatic potential energy.
At closest approach,
\[ E_{\text{kinetic}} = \frac{1}{4\pi\varepsilon_0}\,\frac{(2e)(Ze)}{r} \]
Solving for \(r\):
\[ r = \frac{1}{4\pi\varepsilon_0}\,\frac{2Ze^2}{E_{\text{kinetic}}} \]
Convert energy from MeV to joules:
\[ 7.7\,\text{MeV} = 7.7 \times 1.6 \times 10^{-13} = 1.232 \times 10^{-12}\,\text{J} \]
Substitute values:
\[ r = \frac{9 \times 10^9 \times 2 \times 79 \times (1.6 \times 10^{-19})^2} {1.232 \times 10^{-12}} \]
Evaluating:
\[ r \approx 2.95 \times 10^{-14}\,\text{m} \]
\(\boxed{2.95 \times 10^{-14}\ \text{m}}\)
Two short dipoles \( (A, B) \), \( A \) having charges \( \pm 2\,\mu\text{C} \) and length \( 1\,\text{cm} \) and \( B \) having charges \( \pm 4\,\mu\text{C} \) and length \( 1\,\text{cm} \) are placed with their centres \( 80\,\text{cm} \) apart as shown in the figure. The electric field at a point \( P \), equidistant from the centres of both dipoles is \underline{\hspace{2cm}} N/C.