Figure below shows a lens of refractive index, $ \mu = 1.4 $. $ C_1 $ and $ C_2 $ are the centres of curvature of the two faces of the lens of radii of curvature 4 cm and 8 cm respectively. The lens behaves as a
The lens is a plano-convex lens, where:
- \( R_1 = 4 \, \text{cm} \) (radius of curvature for the convex face),
- \( R_2 = -8 \, \text{cm} \) (radius of curvature for the concave face, negative because it's opposite in direction).
Using the lens maker's formula: \[ \frac{1}{f} = (\mu - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \] Substitute the given values: \[ \frac{1}{f} = (1.4 - 1) \left( \frac{1}{4} - \frac{1}{-8} \right) \] Simplifying this: \[ \frac{1}{f} = 0.4 \left( \frac{1}{4} + \frac{1}{8} \right) = 0.4 \left( \frac{2}{8} + \frac{1}{8} \right) = 0.4 \times \frac{3}{8} \] \[ \frac{1}{f} = \frac{1.2}{8} = \frac{3}{20} \]
Thus, the focal length \( f = 20 \, \text{cm} \).
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: