Given: Angle of incidence on the glass box: \(45^\circ\) The emergent ray passes along the face AB, indicating that the angle of refraction at the glass-liquid interface is \(90^\circ\). 1. First Surface (Air-Glass Interface): \[ \frac{\sin 45^\circ}{\sin \theta} = \mu \] Given \(\sin 45^\circ = \frac{1}{\sqrt{2}}\): \[ \frac{1}{\sqrt{2}} = \mu \sin \theta \] 2. Second Surface (Glass-Liquid Interface): \[ \frac{\sin(90^\circ - \theta)}{\sin 90^\circ} = \frac{1}{\mu} \] Since \(\sin(90^\circ - \theta) = \cos \theta\) and \(\sin 90^\circ = 1\): \[ \cos \theta = \frac{1}{\mu} \] 3. Combining the Equations: \[ \frac{1}{\sqrt{2} \sin \theta} = \frac{1}{\cos \theta} \] Simplifying: \[ \cos \theta = \sqrt{2} \sin \theta \] \[ \tan \theta = \frac{1}{\sqrt{2}} \] 4. Finding \(\sin \theta\): From the triangle GEF: \[ \sin \theta = \frac{1}{\sqrt{3}} \] 5. Calculating the Refractive Index (\(\mu\)): \[ \mu = \frac{1}{\sqrt{2} \sin \theta} = \frac{1}{\sqrt{2} \times \frac{1}{\sqrt{3}}} = \frac{\sqrt{3}}{\sqrt{2}} = \sqrt{\frac{3}{2}} \] Therefore, the refractive index of the liquid is: \[ \boxed{\sqrt{\frac{3}{2}}} \]
Assertion : Out of Infrared and radio waves, the radio waves show more diffraction effect.
Reason (R): Radio waves have greater frequency than infrared waves.