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: \[ \boxed{10.4\,\text{fm}}. \]
A substance 'X' (1.5 g) dissolved in 150 g of a solvent 'Y' (molar mass = 300 g mol$^{-1}$) led to an elevation of the boiling point by 0.5 K. The relative lowering in the vapour pressure of the solvent 'Y' is $____________ \(\times 10^{-2}\). (nearest integer)
[Given : $K_{b}$ of the solvent = 5.0 K kg mol$^{-1}$]
Assume the solution to be dilute and no association or dissociation of X takes place in solution.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]