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Optical Fibers and Optical Fiber Amplifiers
Optical Fibers and Optical FIber Amplifiers 201
Figure 9.8. The angle of aperture of the fiber depends on the ratio of n 2 to n 1 .
In the second case we will evaluate the approximation made above,
taking the index of the cladding to be 1.45:
(n 1 + n 2 ) = 0.01
2
(n 1 – 2n 2 + 2n 2 + n 2 ) = + 2 n 2 = 0.01
–2n 2 ± 4 n 2 + 0 .0 4
2
= = –1.45 + 1.453445 = 0.003444
2
The index difference is less much less the 1%. The accuracy of the ap-
proximation is better than three significant figures.
The propagation of light in an optical fiber is completely and accu-
rately described by Maxwell’s equations. For example, to solve for the
electrical field,
2 2
n
2
E(r, t) + E(r, t) = 0 (9.4)
c 2
An optical fiber has cylindrical symmetry, so an intelligent choice of
coordinates is cylindrical coordinates using r, the radius, the angle
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