
Step 1: Image Formation by the Convex Lens
- A parallel beam of light incident on a convex lens converges at the focus of the lens.
- Given focal length of the convex lens: \[ f_L = 10 \text{ cm} \] - Since parallel rays converge at the focal point, the image formed by the convex lens is: \[ I_1 = 10 \text{ cm (to the right of the lens)} \] - This image acts as the object for the concave mirror.
Step 2: Object Distance for the Concave Mirror
- Distance between the lens and the mirror: \[ d = 40 \text{ cm} \] - Distance of the image formed by the lens from the mirror: \[ u_M = 40 - 10 = 30 \text{ cm} \] - Focal length of the concave mirror: \[ f_M = -15 \text{ cm} \quad \text{(negative for concave mirror)} \] Using the mirror formula: \[ \frac{1}{v} + \frac{1}{u} = \frac{1}{f} \] \[ \frac{1}{v} + \frac{1}{30} = \frac{1}{-15} \] \[ \frac{1}{v} = \frac{1}{-15} - \frac{1}{30} \] \[ \frac{1}{v} = -\frac{2}{30} - \frac{1}{30} = -\frac{3}{30} = -\frac{1}{10} \] \[ v = -10 \text{ cm} \]
Step 3: Final Image Position
- The negative sign indicates that the final image is on the same side as the mirror.
- Distance from the mirror: 10 cm.
- Since the mirror is 40 cm from the lens, the final image is: \[ 40 - 10 = 30 \text{ cm from the lens, on the right}. \] - Since the image distance from the lens is greater than the focal length, the final image is real and inverted.
Step 4: Conclusion
- Final image is formed at 10 cm to the right of the lens.
- Thus, the correct answer is: \[ \boxed{(B) \text{ 10 cm, right of lens}} \]
When light travels from an optically denser medium to an optically rarer medium, at the interface it is partly reflected back into the same medium and partly refracted to the second medium. The angle of incidence corresponding to an angle of refraction 90° is called the critical angle (ic) for the given pair of media. This angle is related to the refractive index of medium 1 with respect to medium 2. Refraction of light through a prism involves refraction at two plane interfaces. A relation for the refractive index of the material of the prism can be obtained in terms of the refracting angle of the prism and the angle of minimum deviation. For a thin prism, this relation reduces to a simple equation. Laws of refraction are also valid for refraction of light at a spherical interface. When an object is placed in front of a spherical surface separating two media, its image is formed. A relation between object and image distance, in terms of refractive indices of two media and the radius of curvature of the spherical surface can be obtained. Using this relation for two surfaces of lens, ’lensemaker formula’ is obtained.