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Question: A reflecting surface is represented by the equation \(y = \dfrac{{2L}}{\pi }\sin (\dfrac{{\pi x}}{L}...

A reflecting surface is represented by the equation y=2Lπsin(πxL),0xLy = \dfrac{{2L}}{\pi }\sin (\dfrac{{\pi x}}{L}),0 \leqslant x \leqslant L.
A ray traveling horizontal becomes vertical after reflection. The coordinates of the point(s) on which this ray is incident.
A.(L4:2Lλ)(\dfrac{L}{4}:\dfrac{{\sqrt 2 L}}{\lambda })
B.(L3:3Lπ)(\dfrac{L}{3}:\dfrac{{\sqrt 3 L}}{\pi })
C.(3L4:2Lλ)(\dfrac{{3L}}{4}:\dfrac{{\sqrt 2 L}}{\lambda })
D.(4L3:4Lπ)(\dfrac{{4L}}{3}:\dfrac{{\sqrt 4 L}}{\pi })

Explanation

Solution

We know that the light travels in a straight path unless an obstacle comes along its path. According to the law of reflection, the angle of incidence and angle of reflection are equal. The slope of any line in the x-y plane is defined by the ratio of its vertical and horizontal components.

Complete answer:
The equation of reflecting surface given in the question is below.
y=2Lπsin(πxL),0xLy = \dfrac{{2L}}{\pi }\sin (\dfrac{{\pi x}}{L}),0 \leqslant x \leqslant L
To find the slope let us differentiate the above equation with respect to x.
dydx=2Lπcos(πxL)×πL=2cos(πxL)\dfrac{{dy}}{{dx}} = \dfrac{{2L}}{\pi }\cos \left( {\dfrac{{\pi x}}{L}} \right) \times \dfrac{\pi }{L} = 2\cos \left( {\dfrac{{\pi x}}{L}} \right) ……………….. (1)
Now, according to the question, the incident ray is horizontal which is zero-degree and the reflected ray is vertical which is 90-degree. Hence, we can say that the angle of incident and reflection will be 9090^\circ . So, we conclude that the normal to the point is at 4545^\circ .
Hence, the slope of the point of incidence is given by,
dydx=tan45o=1\dfrac{{dy}}{{dx}} = \tan {45^o} = 1 …………………..(2)
Equating equations (1) and (2) we get the following expression.
2cos(πxL)=12\cos \left( {\dfrac{{\pi x}}{L}} \right) = 1
Let us further simplify it.
cos(πxL)=12\cos \left( {\dfrac{{\pi x}}{L}} \right) = \dfrac{1}{2}
Now, the angle of cosine whose value is π3\dfrac{\pi }{3}.
cos(πxL)=cos(π3)x=L3\cos \left( {\dfrac{{\pi x}}{L}} \right) = \cos \left( {\dfrac{\pi }{3}} \right) \Rightarrow x = \dfrac{L}{3}
Now, to find the value of yy , let us substitute the value of xx in the equation of the reflecting surface.
y=2Lπsin(πL×L3)=2Lπsinπ3y = \dfrac{{2L}}{\pi }\sin \left( {\dfrac{\pi }{L} \times \dfrac{L}{3}} \right) = \dfrac{{2L}}{\pi }\sin \dfrac{\pi }{3}
Let us further simplify it.
y=2Lπ×32=3Lπy = \dfrac{{2L}}{\pi } \times \dfrac{{\sqrt 3 }}{2} = \dfrac{{\sqrt 3 L}}{\pi }
Therefore, the coordinates of the incidence point are (L3,3Lπ)\left( {\dfrac{L}{3},\dfrac{{\sqrt 3 L}}{\pi }} \right).

Hence, the correct option is (B) (L3,3Lπ)\left( {\dfrac{L}{3},\dfrac{{\sqrt 3 L}}{\pi }} \right).

Note:
When light incidents on the interface of any two different optical media, their reflection and transmission are described by the Fresnel equations.
When the light goes from one medium to another then reflection and refraction both can occur. The Fresnel equation gives the ratio of the reflected wave to incident wave and the ratio of the transmitted wave to incident wave.