p+r = 90
i.e r = 90
Now according to snell's lae
refractive index = sini/sinr
= sinp/sin(90-p)
= sinp/cosp
=tanp
Therefore refractive index of material is equal to tangent of polarizing angle.
Malus law
The intensity of the light coming out from analyzer will be directly proportional to the square of cosine of angle between polarizer and analyzer.
Now, if a be the amplitude of the light used and (theta) be the angle between analyzer and polarizer then acos(theta) will be the component of a along analyzer and asin(theta) will be that along perpendicular direction. Therefore intensity of light which pass through analyzer is
I = (acos(theta))^2
since a is constant
I α cos^2(theta)
Calcite crystal
It is a cuboid made up of six 119m having angle 109 and 71. There will be two corners in which all parallepgram will meet at obtuse angle are called blunt corners. The axis of crystal. The light incident on optical axis will pass without splitting. In actual practice light incident parallel to potical axis will pass without splitting. SO that optical axis is not just a line, it is a direction
Principal section
Principal section is a plane which contains optical axis and perpendicular to opposite faces
Quarter wave plate
A special type of crystal which introduces a path difference of λ/4(i.e quarter of wavelength) between two emergent light is called quarter wave plate
optical path for o-ray = Uot
optical path for e-ray = Uet
In case of clacite crystal Ue
In case of quarts crystal Ue>Uo
Uet - Uot = λ/4
Half wave plate
A special type of crystal which introduces path diference of λ/2(i.e) half of wave length) between two emergent light is called half wave plate
In case of clacite crystal Ue
In case of quarts crystal Ue>Uo
Uet - Uot = λ/2
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