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:
\[ r \approx 2.95 \times 10^{-14}\,\text{m} \]
\(\boxed{2.95 \times 10^{-14}\ \text{m}}\)
For a short dipole placed at origin O, the dipole moment P is along the X-axis, as shown in the figure. If the electric potential and electric field at A are V and E respectively, then the correct combination of the electric potential and electric field, respectively, at point B on the Y-axis is given by:
