Class 12 Physics Notes
Complete, exam-ready notes on ray optics and optical instruments: reflection, refraction and Snell's law, spherical mirrors, lenses and the lens maker formula, total internal reflection, prisms, and the microscope and telescope — written for CBSE boards, JEE and NEET revision.
Written byDeep Narayan· Science & Mathematics EducatorReviewed byPushpanjali
Snell's law relates the angles of incidence and refraction to the refractive indices of two media: n₁ sinθ₁ = n₂ sinθ₂, where n = c/v is the refractive index.
For a spherical mirror of focal length f = R/2, object distance u and image distance v. Magnification . Sign convention: distances to the left of the mirror are negative.
The refractive index of a medium is n = c/v. When light travels from a rarer to a denser medium it bends toward the normal; from denser to rarer it bends away.
Total internal reflection
When light travels from a denser to a rarer medium at an angle beyond the critical angle , it is totally reflected back. This powers optical fibres and produces mirages.
Relates the focal length of a thin lens to its refractive index n and the radii of curvature of its two surfaces. A converging (convex) lens has positive f; a diverging (concave) lens has negative f.
The angle of deviation δ depends on the angle of incidence and the prism angle A. At minimum deviation the ray travels symmetrically: .
Example: A convex lens has focal length . Find its power.
Solution: .
Revision
Memorise these before attempting numericals — most exam questions hinge on one of them.
Snell's law
Mirror formula
Lens maker formula
Power of lens
Critical angle
Telescope magnification
Exam tips
Where this topic appears in CBSE, JEE Main and NEET papers.
FAQ
When a ray travelling from a denser to a rarer medium strikes the interface at an angle greater than the critical angle, it is fully reflected back. Optical fibres rely on it.
A concave mirror converges light and can form real, inverted images; a convex mirror diverges light and always forms virtual, erect, diminished images (used as rear-view mirrors).
The focal length of a thin lens from its refractive index and the radii of curvature of its surfaces: 1/f = (n−1)(1/R₁ − 1/R₂).
The objective forms a real, magnified image, and the eyepiece further magnifies it — the total magnification is the product of the two.
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