Solveeit Logo

Question

Question: Figure shows a glass hemisphere M of $\mu = 3/2$ and radius 10 cm. A point object O is placed at a d...

Figure shows a glass hemisphere M of μ=3/2\mu = 3/2 and radius 10 cm. A point object O is placed at a distance 20 cm behind the flat face which is viewed by an observer from the curved side. Find location of final image after two refractions as seen by observer.

A

10 cm behind the flat face

B

10 cm in front of the flat face

C

30 cm behind the flat face

D

30 cm in front of the flat face

Answer

The final image is formed at a distance of 10 cm behind the flat face.

Explanation

Solution

The problem involves two refractions: first at the flat face and then at the curved face.

Step 1: Refraction at the flat face. The object O is in air (n1=1n_1 = 1) at a distance u1=20u_1 = 20 cm from the flat face. The light enters the glass hemisphere (n2=3/2n_2 = 3/2). For a plane surface, the radius of curvature is infinite (R1=R_1 = \infty). The refraction formula is n2vn1u=n2n1R\frac{n_2}{v} - \frac{n_1}{u} = \frac{n_2 - n_1}{R}. For a plane surface, this simplifies to n2v1=n1u1\frac{n_2}{v_1} = \frac{n_1}{u_1}. Using the sign convention where distances to the right of the surface are positive: u1=+20u_1 = +20 cm. 3/2v1=1+20\frac{3/2}{v_1} = \frac{1}{+20} v1=32×20=+30v_1 = \frac{3}{2} \times 20 = +30 cm. The first image I1I_1 is formed at a distance of 30 cm to the right of the flat face.

Step 2: Refraction at the curved face. The first image I1I_1 acts as the object for the curved surface. This is the interface between glass (n1=3/2n_1 = 3/2) and air (n2=1n_2 = 1). The observer is viewing from the curved side (air). The object distance u2u_2 is the distance of I1I_1 from the pole of the curved surface. Assuming the flat face is at x=0x=0, the curved surface is part of a sphere with its center of curvature at x=R=10x=-R = -10 cm. The pole of the curved surface is at x=0x=0. The object I1I_1 is at x=+30x=+30 cm. Therefore, u2=+30u_2 = +30 cm. The radius of curvature of the curved surface is R2=10R_2 = -10 cm (negative because the center of curvature is on the left of the pole, which is the side of the incident ray). Applying the refraction formula: n2v2n1u2=n2n1R2\frac{n_2}{v_2} - \frac{n_1}{u_2} = \frac{n_2 - n_1}{R_2} 1v23/2+30=13/210\frac{1}{v_2} - \frac{3/2}{+30} = \frac{1 - 3/2}{-10} 1v2120=1/210\frac{1}{v_2} - \frac{1}{20} = \frac{-1/2}{-10} 1v2120=120\frac{1}{v_2} - \frac{1}{20} = \frac{1}{20} 1v2=120+120=220=110\frac{1}{v_2} = \frac{1}{20} + \frac{1}{20} = \frac{2}{20} = \frac{1}{10} v2=+10v_2 = +10 cm.

The final image is formed at a distance of 10 cm to the right (behind) of the flat face.