Step 1: Recall the formula for distance of closest approach.
For a head-on collision between an \( \alpha \)-particle and a nucleus, the distance of closest approach is given by: \[ r = \frac{1}{4\pi\varepsilon_0}\,\frac{Z_1 Z_2 e^2}{E}. \] In nuclear units: \[ \frac{e^2}{4\pi\varepsilon_0} = 1.44\,\text{MeVfm}. \]
Step 2: Substitute known values.
Charge of \( \alpha \)-particle: \[ Z_1 = 2, \] Charge of copper nucleus: \[ Z_2 = 29, \] Energy of \( \alpha \)-particle: \[ E = 8\,\text{MeV}. \]
Step 3: Perform the calculation.
\[ r = \frac{1.44 \times (2 \times 29)}{8} = \frac{1.44 \times 58}{8} = \frac{83.52}{8} = 10.44\,\text{fm}. \]
Step 4: Final conclusion.
The distance of closest approach is approximately: \[ \boxed{10.4\,\text{fm}}. \]
