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Q. Light enters at an angle of incidence in a transparent rod of refractive index of the material of the rod the light once entered into it will not leave it through its lateral face whatsoever be the value of angle of incidence?

AFMCAFMC 2006Ray Optics and Optical Instruments

Solution:

The first idea is that for no refraction at its lateral face, angle of incidence should be greater than critical angle.
Let a light ray enters at $A$ and refracted beam is $A B$.
At the lateral face, the angle of incidence is
$\theta$. For no refraction at this face, $\theta>C$.
i.e., $ \sin \theta>\sin C$
but $ \theta+r=90^{\circ} $
$\Rightarrow \theta=90^{\circ}-r$
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The second idea is that in $E q$. (i),
the substitution for $\cos r$ can be found from Snell's law.
Now, from Snell's law, $n=\frac{\sin i}{\sin r}$
$\Rightarrow \sin r=\frac{\sin i}{n} $
$\therefore \cos r=\sqrt{1-\sin ^{2} r}=\sqrt{\left(1-\frac{\sin ^{2} i}{n^{2}}\right)}$
$\therefore $ Eq. (i) gives,
$\sqrt{1-\frac{\sin ^{2} i}{n^{2}}}>\sin C$
Also $ \sin C=\frac{1}{n}$
$\therefore 1-\frac{\sin ^{2} i}{n^{2}}>\frac{1}{n^{2}}$
or $ n^{2}>\sin ^{2} i+1$
The maximum value of $\sin i$ is $1 .$
So, $ n^{2} >2 $
or $ n > \sqrt{2} $