| n0 sin θ0max = (n12 - n22)1/2 = NA. |
| (a) | From the Table
of indices of refraction, we see that n0
= nair = 1.0003. The numerical
aperture is therefore
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| (b) | The index of refraction of the
cladding can be found from the numerical aperture:
n22 = n12 - NA2 = (1.425)2 - (0.1479)2 = 2.0088 n2 = 1.417. |
| (c) | From the Table,
we see that the n0
= nwater = 1.33. Since
the numerical aperture is a property of the fiber and only depends upon
n1
and n2, it will not change when
the medium outside the fiber changes. The cut-off angle, however,
will have to change if the numerical aperture is to be unaffected by a
change in n0:
sin θ0max = NA/n0 θ0max = sin-1(NA/n0) = sin-1(0.1479/1.33) = = sin-1(0.1112) = 6.38o. |
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