In Young's double slit experiment, the intensity of light passing through a slit is directly proportional to the width of the slit.
Let the widths of the two slits be \( w_1 \) and \( w_2 \). Given that the width of one slit is half the width of the other slit, let \( w_1 = w \) and \( w_2 = 2w \).
The intensities of light from the two slits are proportional to their widths. Let the intensities be \( I_1 \) and \( I_2 \). \[ I_1 \propto w_1 = w \implies I_1 = I_0 \] \[ I_2 \propto w_2 = 2w \implies I_2 = 2I_0 \] The maximum intensity \( I_{max} \) in the interference pattern occurs when the waves from the two slits interfere constructively, and is given by: \[ I_{max} = (\sqrt{I_1} + \sqrt{I_2})^2 \] Substituting the values of \( I_1 \) and \( I_2 \): \[ I_{max} = (\sqrt{I_0} + \sqrt{2I_0})^2 = (\sqrt{I_0} (1 + \sqrt{2}))^2 = I_0 (1 + \sqrt{2})^2 = I_0 (1 + 2 + 2\sqrt{2}) = I_0 (3 + 2\sqrt{2}) \] The minimum intensity \( I_{min} \) in the interference pattern occurs when the waves from the two slits interfere destructively, and is given by: \[ I_{min} = (\sqrt{I_1} - \sqrt{I_2})^2 \] Substituting the values of \( I_1 \) and \( I_2 \): \[ I_{min} = (\sqrt{I_0} - \sqrt{2I_0})^2 = (\sqrt{I_0} (1 - \sqrt{2}))^2 = I_0 (1 - \sqrt{2})^2 = I_0 (1 + 2 - 2\sqrt{2}) = I_0 (3 - 2\sqrt{2}) \] The ratio of the maximum to the minimum intensity is: \[ \frac{I_{max}}{I_{min}} = \frac{I_0 (3 + 2\sqrt{2})}{I_0 (3 - 2\sqrt{2})} = \frac{3 + 2\sqrt{2}}{3 - 2\sqrt{2}} \] So, the ratio \( I_{max} : I_{min} \) is \( (3 + 2\sqrt{2}) : (3 - 2\sqrt{2}) \).
Consider the sound wave travelling in ideal gases of $\mathrm{He}, \mathrm{CH}_{4}$, and $\mathrm{CO}_{2}$. All the gases have the same ratio $\frac{\mathrm{P}}{\rho}$, where P is the pressure and $\rho$ is the density. The ratio of the speed of sound through the gases $\mathrm{v}_{\mathrm{He}}: \mathrm{v}_{\mathrm{CH}_{4}}: \mathrm{v}_{\mathrm{CO}_{2}}$ is given by
Match List-I with List-II: List-I