Page 453 - Engineering Electromagnetics, 8th Edition
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CHAPTER 12   Plane Wave Reflection and Dispersion      435






















                                     Figure 12.8 Beam-steering prism for
                                     Example 12.8.

                     as beam-steering prisms, where light within the glass structure totally reflects from
                     glass-air interfaces.


                                                                                           EXAMPLE 12.8
                     A prism is to be used to turn a beam of light by 90 ,as shown in Figure 12.8.
                                                                 ◦
                     Light enters and exits the prism through two antireflective (AR-coated) surfaces.
                     Total reflection is to occur at the back surface, where the incident angle is 45 to the
                                                                                  ◦
                     normal. Determine the minimum required refractive index of the prism material if the
                     surrounding region is air.
                     Solution. Considering the back surface, the medium beyond the interface is air, with
                     n 2 = 1.00. Because θ 1 = 45 , (76) is used to obtain
                                            ◦
                                                  n 2   √
                                            n 1 ≥     =   2 = 1.41
                                                 sin 45
                     Because fused silica glass has refractive index n g = 1.45, it is a suitable material for
                     this application and is in fact widely used.


                         Another important application of total reflection is in optical waveguides. These,
                     in their simplest form, are constructed of three layers of glass, in which the middle
                     layer has a slightly higher refractive index than the outer two. Figure 12.9 shows
                     the basic structure. Light, propagating from left to right, is confined to the middle
                     layer by total reflection at the two interfaces, as shown. Optical fiber waveguides are
                     constructed on this principle, in which a cylindrical glass core region of small radius
                     is surrounded coaxially by a lower-index cladding glass material of larger radius.
                     Basic waveguiding principles as applied to metallic and dielectric structures will be
                     presented in Chapter 13.
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