In the fig SR || PQ and OM is the reflected ray Hence r1=r2
Let μ be the refractive index of the glass slab.
Then, according to Snell's law,
Then, according to Snell's law,
\(\frac{sin\,\,i}{sin\,\, r_1}\) = μ .....(i)
and
\(\frac{sin\,\,r_2}{sin\,\, e}\) = \(\frac{1}{μ}\) .... .....(ii)
But r1=r2
Putting (iii) in (i), we get
\(\frac{sin\,\,i}{sin\,\, r_2}\) = μ .....(iv)
Multiplying (ii) and (iv), we have
\(\frac{sin\,\,i}{sin\,\, r_2}\) x \(\frac{sin\,\,r_2}{sin\,\, e}\) = μ x \(\frac{1}{μ}\)
∴ \(\frac{sin\,\,i}{sin\,\, e}\) = 1
∴ i = e proved