A transparent cylinder has its right half polished so as to act as a mirror. A paraxial light ray incident from left, that is parallel to the pricipal axis, exits parallel to the incident ray as shown. The refractive index n of the material of the cylinder is
From above figure,
u=−∞; v=+2R
[∵ Light ray is intersecting at 2R from pole of spherical surface]
Using the formula of refraction through curved surface,
μ2v−μ1u=μ2−μ1R
⇒n+2R−1(−∞)=n−1R
(∵μ2=n,μ1=μair=1)
⇒n2R=n−1R
⇒2n−2=n
∴n=2
Hence, option (d) is the correct answer.
Why this question? Tip: After first refraction a real image is formed at distance 2R from spherical surface when u→−∞ . |