To solve the problem, we need to calculate the focal length of a double concave lens placed in air using the lens maker’s formula. The radii of curvature are given as \( R_1 = 20 \, \text{cm} \) and \( R_2 = 40 \, \text{cm} \), and the refractive index \( n = \frac{5}{3} \).
1. Lens Maker’s Formula:
The lens maker’s formula for a lens in air is:
\( \frac{1}{f} = (n - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \)
2. Sign Convention:
For a double concave lens:
- The first surface is convex from the side of the incident light, so \( R_1 = -20 \, \text{cm} \)
- The second surface is concave from the side of the incident light, so \( R_2 = 40 \, \text{cm} \)
(Note: R₁ is negative and R₂ is positive for a double concave lens)
3. Substituting Values:
\( \frac{1}{f} = \left( \frac{5}{3} - 1 \right) \left( \frac{1}{-20} - \frac{1}{40} \right) \)
\( \frac{1}{f} = \frac{2}{3} \left( \frac{-2 - 1}{40} \right) = \frac{2}{3} \times \left( \frac{-3}{40} \right) = \frac{-6}{120} = \frac{-1}{20} \)
4. Final Calculation:
\( f = -20 \, \text{cm} \)
Final Answer:
The focal length of the lens is \({-20 \, \text{cm}} \).
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = 4/3 \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \frac{n_2}{2n_1} \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is cm. 