
For light to travel along the surface of the cylindrical rod, the angle of incidence \( \theta \) must ensure refraction along the surface. Applying Snell's law at the rod-air interface: \[ n_{\text{air}} \sin \theta = n_{\text{rod}} \sin 90^\circ \] With \( n_{\text{air}} = 1 \) and \( n_{\text{rod}} = \frac{2}{\sqrt{3}} \): \[ \sin \theta = \frac{n_{\text{rod}}}{n_{\text{air}}} = \frac{2}{\sqrt{3}} \] Consequently: \[ \theta = \sin^{-1} \left( \frac{2}{\sqrt{3}} \right) \] The angle \( \theta \) is therefore \( \sin^{-1} \left( \frac{2}{\sqrt{3}} \right) \).

