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Optical Fibers



                                                                              Optical Fibers  51




























                      Figure 4.4. Variations in the material composition of
                      the core and cladding yield different fiber types.
                      (a) Simple profiles define step- and graded-index
                      fibers; (b) complex cladding-index profiles tailor the
                      signal dispersion characteristics of a fiber.

                      TABLE 4.1. Typical Core, Cladding, and Buffer Coating Sizes of Optical Fibers
                                                   Cladding outer   Buffer outer
                      Fiber type  Core diameter, µm  diameter, µm  diameter, µm  Application
                      Single-mode       7–10          125         250 or 500  Telecommunications
                      Multimode        50.0           125         250 or 500  LAN or MAN
                      Multimode        62.5           125         250 or 500  LAN
                      Multimode        85             125         250 or 500  Older LAN fiber
                      Multimode       100             140         250 or 500  Older fiber type


                        The critical angle also defines a parameter called the  numerical aperture
                      (NA), which is used to describe the light acceptance or gathering capability of
                      fibers that have a core size much larger than a wavelength. This parameter
                      defines the size of the acceptance cone shown in Fig. 4.2. The numerical aper-
                      ture is a dimensionless quantity which is less than unity, with values ranging
                      from 0.14 to 0.50.

                        Numerical Aperture The critical angle condition on the entrance angle defines the
                        numerical aperture (NA) of a step-index fiber. This is given by
                                                                    1/2
                                       NA n sin θ 0,max  n 1 sin θ c   n 1  n 2  ≈n 1  2 ∆
                                                                  2
                                                               2
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