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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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