| (a) |
To observe total internal reflection,
light must travel from the denser medium of diamond or glass into the rarer
medium of air. From the Table
of indices of refraction, we see that
n1d
= ndiamond = 2.4, while n1g
= nglass = 1.5. n2
= nair = 1.0.
Using the definition of the critical
angle provided above, we have
θc,diamond/air=
sin-1 (nair/ndiamond)
= sin-1 (0.417) = 24.6o.
θc,glass/air=
sin-1 (nair/nglass)
= sin-1 (0.667) = 41.8o.
|
| (b) |
We can observe the path of laser light as it travels
through the stone. By rotating the stone until TIR is just reached
for the light exiting the stone, we can observe the critical angle.
If the critical angle for light incident on the back face of the stone
is fairly close to 45o (halfway between
face and normal to face so "easy" to reference), the stone is glass.
If, on the other hand, the critical angle for the light incident on the
back face is significantly closer to the normal than halfway, the stone
might actually be a diamond. Of course observing TIR on the back
face of a cut stone might be difficult unless the stone is very large and/or
has few facets. |