There is a glass sphere of refractive index \(1.5\), on which a parallel beam of light falls. Find the distance of the final converging point of the emergent rays from the centre of the sphere. Radius of the sphere is \(50\,\text{cm}\).
Show Hint
For optical problems involving spheres:
Always apply refraction formula separately for each surface
Carefully determine the sign of radius and object distance
Final distance is often asked from the centre, not from the surface
Concept:
When a parallel beam of light falls on a transparent spherical object, refraction occurs at both spherical surfaces.
The final image is obtained after applying refraction successively at:
The first spherical surface (air to glass)
The second spherical surface (glass to air)
For refraction at a spherical surface, the formula used is:
\[
\frac{n_2}{v} - \frac{n_1}{u} = \frac{n_2 - n_1}{R}
\]
where
\(n_1, n_2\) = refractive indices,
\(u\) = object distance,
\(v\) = image distance,
\(R\) = radius of curvature.
Step 1: Refraction at the first surface.
Parallel rays imply:
\[
u_1 = \infty
\]
For the first surface:
\[
n_1 = 1,\quad n_2 = 1.5,\quad R_1 = +50\,\text{cm}
\]
Applying the formula:
\[
\frac{1.5}{v_1} - \frac{1}{\infty} = \frac{1.5 - 1}{50}
\]
\[
\frac{1.5}{v_1} = \frac{0.5}{50}
\]
\[
v_1 = \frac{1.5 \times 50}{0.5} = 150\,\text{cm}
\]
Thus, the image formed by the first surface is \(150\,\text{cm}\) inside the glass from the first surface.
Step 2: Locate the object for the second surface.
The thickness of the sphere (diameter):
\[
2R = 100\,\text{cm}
\]
Distance of the image from the second surface:
\[
u_2 = 150 - 100 = 50\,\text{cm}
\]
Since the image lies to the right of the second surface, it acts as a virtual object:
\[
u_2 = +50\,\text{cm}
\]
Step 3: Refraction at the second surface.
For the second surface:
\[
n_1 = 1.5,\quad n_2 = 1,\quad R_2 = -50\,\text{cm}
\]
Apply refraction formula:
\[
\frac{1}{v_2} - \frac{1.5}{50} = \frac{1 - 1.5}{-50}
\]
\[
\frac{1}{v_2} - 0.03 = \frac{-0.5}{-50}
\]
\[
\frac{1}{v_2} - 0.03 = 0.01
\]
\[
\frac{1}{v_2} = 0.04
\Rightarrow v_2 = 25\,\text{cm}
\]
This distance is measured from the second surface.
Step 4: Find distance from the centre of the sphere.
Distance of centre from second surface:
\[
R = 50\,\text{cm}
\]
Hence, distance of final image from centre:
\[
50 + 25 = 75\,\text{cm}
\]
\[
\boxed{\text{Final converging point is } 75\,\text{cm from the centre of the sphere}}
\]
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