For a circular aperture, the radius of the first dark ring in the Fraunhofer diffraction pattern, often referred to as the Airy disk radius \( r_1 \), is given by: \[ r_1 = 1.22 \frac{\lambda f}{D}, \] where \( D \) is the diameter of the aperture. Given that the radius \( a = 0.05 \, \text{cm} \), the diameter \( D = 2a = 0.1 \, \text{cm} \). Substituting the given values: \[ r_1 = 1.22 \times \frac{5 \times 10^{-5} \, \text{cm} \times 20 \, \text{cm}}{0.1 \, \text{cm}} = 1.22 \times 10^{-2} \, \text{cm} = 12.20 \times 10^{-3} \, \text{cm}. \] This calculation confirms that the radius of the first dark ring matches option (b).
In the diagram given below, there are three lenses formed. Considering negligible thickness of each of them as compared to \( R_1 \) and \( R_2 \), i.e., the radii of curvature for upper and lower surfaces of the glass lens, the power of the combination is: