The problem requires calculating the focal length ($F$) of a combination formed by a plano-convex lens and a plano-concave lens. Both lenses possess a curved surface with radius of curvature $R$. They are constructed from different materials with refractive indices $\mu_1$ and $\mu_2$. The lenses are assumed to be in contact, sharing a common optical axis.
The focal length ($f$) of a single lens is given by the Lens Maker's formula: $ \frac{1}{f} = (\mu - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) $ Here, $\mu$ is the refractive index of the lens material. $R_1$ and $R_2$ are the radii of curvature of the two lens surfaces. We follow the standard sign convention where light travels from left to right, and radii are positive if their center of curvature lies to the right of the lens surface, and negative otherwise.
Note: Based on the provided options and correct answer, we infer that the plano-concave lens corresponds to $\mu_1$ and the plano-convex lens corresponds to $\mu_2$.
For the plano-concave lens with refractive index $\mu_1$: The plane surface has $R_1 = \infty$. The concave surface has a radius $R$, so $R_2 = -R$. Applying the Lens Maker's formula: $ \frac{1}{f_1} = (\mu_1 - 1) \left( \frac{1}{\infty} - \frac{1}{-R} \right) = (\mu_1 - 1) \left( 0 + \frac{1}{R} \right) = \frac{\mu_1 - 1}{R} $
For the plano-convex lens with refractive index $\mu_2$: The plane surface has $R_1 = \infty$. The convex surface has a radius $R$, so $R_2 = R$. Applying the Lens Maker's formula: $ \frac{1}{f_2} = (\mu_2 - 1) \left( \frac{1}{\infty} - \frac{1}{R} \right) = (\mu_2 - 1) \left( 0 - \frac{1}{R} \right) = -\frac{\mu_2 - 1}{R} $
When two thin lenses are placed in contact, the focal length of the combination ($F$) is given by the sum of their individual focal lengths' reciprocals: $ \frac{1}{F} = \frac{1}{f_1} + \frac{1}{f_2} $ Substituting the expressions for $\frac{1}{f_1}$ and $\frac{1}{f_2}$: $ \frac{1}{F} = \frac{\mu_1 - 1}{R} + \left( -\frac{\mu_2 - 1}{R} \right) $ $ \frac{1}{F} = \frac{(\mu_1 - 1) - (\mu_2 - 1)}{R} $ $ \frac{1}{F} = \frac{\mu_1 - 1 - \mu_2 + 1}{R} $ $ \frac{1}{F} = \frac{\mu_1 - \mu_2}{R} $ Taking the reciprocal to find $F$: $ F = \frac{R}{\mu_1 - \mu_2} $ This result matches Option A.
Two points of monochromatic and coherent sources of light of wavelength $\lambda$ each, are placed as shown in figure. The initial phase difference between the sources is zero, ($D \gg d$). Mark the correct statement(s).