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Question: A ray of light strikes a plane mirror at an angle of incidence \(45^\circ \)as shown in fig. 1.364. ...

A ray of light strikes a plane mirror at an angle of incidence 4545^\circ as shown in fig. 1.364. After reflection, the ray passes through a prism of reflection index 1.51.5 whose apex angle is44^\circ . If the mirror is rotated by xx^\circ then the total deviation of the ray becomes 9090^\circ . Find xx

Explanation

Solution

When there are many optical instruments involved then the total angle of deviation will be the sum of the angle of deviation of every optical instrument. The angle of the prism and apex angle represent the same thing which is the topmost angle of the prism.
Formula used:
For mirror
δ=1802i\delta = 180^\circ - 2i
For prism with small apex angle
δ=A(n1)\delta = A(n - 1)
Where δ\delta is the angle of deviation, AAis the apex angle,ii is the angle of incidence, andnn is the refractive index of prism.

Complete step-by-step answer:
For the initial case when the angle of incidence on mirror is 4545^\circ (before rotation)
We know that,
For mirror
δ=1802i\delta = 180^\circ - 2i
For prism with small apex angle
δ=A(n1)\delta = A(n - 1)
Where δ\delta is the angle of deviation, AAis the apex angle,ii is the angle of incidence, andnn is the refractive index of prism.
Hence
The angle of deviation of ray due to mirror be δ1{\delta _1}
δ1=1802(45)\Rightarrow {\delta _1} = 180^\circ - 2(45^\circ )
δ1=90\Rightarrow {\delta _1} = 90^\circ
The angle of deviation of ray due to prism be δ2{\delta _2}
It is given that the apex angle is44^\circ and the refractive index of the prism is 1.51.5
δ2=4(1.51)\Rightarrow {\delta _2} = 4(1.5 - 1)
δ2=2\Rightarrow {\delta _2} = 2^\circ
Let the total angle of deviation be δ3{\delta _3}
We know that the total angle of deviation from the given setup will be δ1+δ2{\delta _1} + {\delta _2}
δ3=δ1+δ2\Rightarrow {\delta _3} = {\delta _1} + {\delta _2}
δ3=90+2\Rightarrow {\delta _3} = 90^\circ + 2^\circ
δ3=92\Rightarrow {\delta _3} = 92^\circ
Now solving for the second case
For the second case when the mirror is rotated by xx^\circ (let’s assume that we have turned the mirror in an anticlockwise direction) hence angle of incidence upon the mirror is (45+x)(45 + x)^\circ
We know that,
For mirror
δ=1802i\delta = 180^\circ - 2i
For prism with small apex angle
δ=A(n1)\delta = A(n - 1)
Where δ\delta is the angle of deviation, AAis the apex angle,ii is the angle of incidence, andnn is the refractive index of prism.
Hence
The angle of deviation of ray due to mirror be δ1{\delta _1}
δ1=1802((45+x))\Rightarrow {\delta _1} = 180^\circ - 2((45 + x)^\circ )
δ1=(902x)\Rightarrow {\delta _1} = (90 - 2x)^\circ
The angle of deviation of ray due to prism be δ2{\delta _2}
It is given that the apex angle is44^\circ and the refractive index of the prism is 1.51.5
δ2=4(1.51)\Rightarrow {\delta _2} = 4(1.5 - 1)
δ2=2\Rightarrow {\delta _2} = 2^\circ
Let the total angle of deviation be δ3{\delta _3} and it’s given that in this case δ3=90{\delta _3} = 90^\circ
We know that the total angle of deviation from the given setup will be δ1+δ2{\delta _1} + {\delta _2}
δ3=δ1+δ2\Rightarrow {\delta _3} = {\delta _1} + {\delta _2}
δ3=(902x)+2\Rightarrow {\delta _3} = (90 - 2x)^\circ + 2^\circ
90=(922x)\Rightarrow 90^\circ = (92 - 2x)^\circ
2x=2\Rightarrow 2x = 2
x=1\Rightarrow x = 1^\circ
As the value of xxis positive our assumption of anticlockwise rotation was correct.

Therefore the correct answer to the above question is 11^\circ in an anticlockwise direction.

Note:
When the apex angle of the prism is small then we can use the trigonometric approximation which is sinθθ\sin \theta \approx \theta . Due to this, the formula derived for the angle of deviation of the prism is independent of the angle of incidence which made our solution simpler.