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2                                                                 Fiber Optic Communications



                                                                            F 2
                                                                  q 2




                                             r

                                 q 1
                                                     r







                                 Figure 1.1 Force of attraction or repulsion between charges.



            The electric field intensity is defined as the force on a positive unit charge and is given by Eq. (1.4). The
            electric field intensity is a function only of the charge q and the distance between the test charge and q .
                                                                                               1
                                                        1
              For historical reasons, the product of electric field intensity and permittivity is defined as the electric flux
            density D,
                                                          q 1
                                                D = E =    r.                                (1.5)
                                                         4r 2
            The electric flux density is a vector with its direction the same as the electric field intensity. Imagine a sphere
            S of radius r around the charge q as shown in Fig. 1.2. Consider an incremental area ΔS on the sphere. The
                                       1
            electric flux crossing this surface is defined as the product of the normal component of D and the area ΔS.
                                         Flux crossing ΔS =Δ = D ΔS,                         (1.6)
                                                                  n
            where D is the normal component of D. The direction of the electric flux density is normal to the surface of
                   n
                                                                2
            the sphere and therefore, from Eq. (1.5), we obtain D = q ∕4r . If we add the differential contributions to
                                                       n
                                                           1
            the flux from all the incremental surfaces of the sphere, we obtain the total electric flux passing through the
            sphere,
                                               =   d =  D dS.                              (1.7)
                                                  ∫       ∮  n
                                                           S
                                                        D



                                                                      D
                                              q 1

                                                      s
                                                                    Δs
                                              (a)                 (b)

               Figure 1.2 (a) Electric flux density on the surface of the sphere. (b) The incremental surface ΔS on the sphere.
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