A ray of light is incident on a parallel slab of thickness (t) and refractive index (n). If the angle of incidence (i) is small, then the lateral displacement of emergent ray will be
A
ti(n−1)n
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B
tin
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C
ti(nn+1)
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D
ti(n+1)n
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Solution
The correct option is Ati(n−1)n Lateral displacement is given by,
S=tcosrsin(i−r)
If i is very small , r is also small, then sini→i,sinr→r and cosr→1.
From snell's law,
sinisinr=n
This can be rewritten as ir=n
Therefore, the expression for lateral displacement takes the form