Ray Optics
Unit 6 > Physics > Class 12 > Samacheer Kalvi - English Medium
Objectives
• The ray aspect of light. • The phenomenon of reflection and refraction of light. • The determination of speed of light. • The concepts related to mirrors, lenses, prisms etc. • The different phenomena like dispersion and scattering of light
Summary
A ray of light gives the direction of light. Law of reflection is, i = r Paraxial rays are the rays travelling close to the principal axis of the mirror and make small angles with it. The relation between focal length and radius of curvature in spherical mirror is, 2 2 f R R = = (or) f Cartesian sign conventions are to be followed to trace image formed by spherical mirrors. The mirror equation is, 1 1 1 v u f + = The magnification in spherical mirror is, m h h v u = ′ = − , m h h f v f f f u = ′ = − = − Light travels with lesser velocity in optically denser medium. Refractive index is the ratio of speed of light in vacuum to speed of light in medium, n c = v Optical path is the equivalent path travelled in vacuum in the same time light travels through a optically denser medium. d n ′ = d Law of refraction also called as Snell’s law in ratio form is, sin sin i r n n = 2 1 . In product form is, n i n r 1 2 sin s = in The relative refractive index of second medium with respect to first medium is, n n n 21 2 1 = The apparent depth is always lesser than actual depth. The equation for apparent depth is, d′ = d n The critical angle of incidence i c for a ray incident from a denser to rarer medium, is that angle for which the angle of refraction is 90°. For i > i c , total internal reflection occurs. Equations for critical angle incidence is, sini n c = 1 (or) i n c = − sin 1 1 Snell’s window is the restricted area of circular illumination which appears when seen from water due to critical angle incidence. The radius of the circular illumination is, R d n R d n = − = − 1 1 1 2 2 ( ) or Optical fibre makes use of critical angle incidence. The acceptance angle in optical fibre is, . Here, n1 , n2 , n3 are the refractive indices of core, cladding and surrounding medium respectively. Glass slabs produce a lateral displacement on the light falling on it. The equation for lateral shift is, L t i r r = ( ) − ( ) The equation for single spherical surface is, n v u n R − =1 ( ) −1 The focal length of the thin lens is positive for a converging lens and negative for a diverging lens. It is not based on the position of the focal point. The lens makers formula is, 1 1 1 1 1 2 f n R R = − ( ) − The lens equation is, 111 vuf - = The magnification produced by the lens is, m h h v u = =’ , m h h f f u = = + ’ (or) m h h f v f = =’ − The power of a lens is a measure of the degree of convergence (or) divergence of light falling on it. Power and focal length are inverse to each other. P f = 1 The unit of power is diopter (D) when the focal length is taken in meter. The effective focal length of lenses in contact is, 1 1 1 1 2 F f f = + A prism produces deviation on the incident ray. Angle of deviation depends on angle of prism, angle of incidence and refractive index of material of prism given by the equation, d i = +1 2i A − At minimum deviation, i 1 = i 2 , r1 = r2 , and the ray inside the prism is parallel to the base of the prism. The refractive index of prism depends on angle of prism and angle of minimum deviation given by the equation, n A D A = + sin sin 2 2 When white light travels through a medium, different colours travel with different speeds leading to dispersion of light. Red colour travels faster than violet colour in a medium. In vacuum all the colours travel with the same speed. The angle of deviation produced by the small angled prism is, d = − ( ) n A 1 The angular separation between the two extreme colours (violet and red) in the spectrum is called angular dispersion. δV– δR = (nV–nR)A Dispersive power is the measure of ability of the medium to disperse white light. w = ( ) − − n n n V R ( )1 Rainbow is formed by dispersion of light by droplets of water. The scattering of light by particles of size less than wavelength of light is called Rayleigh scattering. The intensity of light produced by Rayleigh scattering is, I µ 1 4 l Non-Rayleigh scattering is by suspended dust particles whose size is greater than the wavelength of light. This scattering is independent of wavelength of light.