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Question: What is polarization of light? Explain polarization of light with the suitable diagram and hence der...

What is polarization of light? Explain polarization of light with the suitable diagram and hence derive Brewster’s law.

Explanation

Solution

Brewster’s law states that when light from a medium enters a medium of another medium such that the refractive index one is different from another, it gets polarized. This results in production of two rays i.e. refracted ray and reflected ray which are perpendicular to each other. This occurs when angle of incidence has a certain value called the Brewster’s angle.

Complete step by step solution:

In this figure, it can be seen that an incident unpolarized ray of light breaks down into a refracted ray of light and a reflected ray of light.
Let the refractive index of medium 1 is n1{n_1} and that of medium 2 is n2{n_2} . Using Snell’s law,
nisinθi=nrsinθr.........(1){n_i}\sin {\theta _i} = {n_r}\sin {\theta _r}.........(1) where θi&θr{\theta _i}\& {\theta _r} are the angle of incidence and angle of refraction respectively.
Brewster’s angle is denoted by θB{\theta _B} and angle of reflection by θr{\theta _r} .
We know θi=θrefl{\theta _i} = {\theta _{refl}}
\therefore (1)(1) becomes n1sinθB=n2sinθr{n_1}\sin {\theta _B} = {n_2}\sin {\theta _r}
sinθr=n1n2sinθB.............(2)\Rightarrow \sin {\theta _r} = \dfrac{{{n_1}}}{{{n_2}}}\sin {\theta _B}.............(2)
Consider the figure,
θref+900+θr=180o\Rightarrow{\theta _{ref}} + {90^0} + {\theta _r} = {180^o} (Angle of straight line)
θr=900θref............(3)\Rightarrow {\theta _r} = {90^0} - {\theta _{ref}}............(3)
(3)(3) can be written as θr=900θB{\theta _r} = {90^0} - {\theta _B}............(4)(4)
because θi=θrefl{\theta _i} = {\theta _{refl}}
Using (2)&(4)(2)\& (4) ,
sin(900θB)=n1n2sinθB\Rightarrow \sin ({90^0} - {\theta _B}) = \dfrac{{{n_1}}}{{{n_2}}}\sin {\theta _B}
cosθB=n1n2sinθB\therefore \cos {\theta _B} = \dfrac{{{n_1}}}{{{n_2}}}\sin {\theta _B} as sin(900θ)=cosθ\sin ({90^0} - \theta ) = \cos \theta
n2n1=sinθBcosθB=tanθB\therefore \dfrac{{{n_2}}}{{{n_1}}} = \dfrac{{\sin {\theta _B}}}{{\cos {\theta _B}}} = \tan {\theta _B} as sinθcosθ=tanθ\dfrac{{\sin \theta }}{{\cos \theta }} = \tan \theta
n21=tanθB\therefore {n_{21}} = \tan {\theta _B} where n21{{{n}}_{21}} is refractive index of medium 22 with respect to medium 11

Note: Refractive index of a medium with respect to another one depends on both the medium and hence when one medium is replaced by another, the Brewster’s angle also changes.
Using inverse trigonometry, we can directly evaluate the Brewster’s angle as
θB=tan1(n21){\theta _B} = {\tan ^{ - 1}}({n_{21}})