Page 395 - Schaum's Outline of Theory and Problems of Applied Physics
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380                                      LIGHT                                   [CHAP. 30



                  Now medium 1 is water and medium 2 is air. Hence
                                                       1.33
                                               n 1             ◦
                                         sinr =  sin i =   sin 40 = 0.855
                                               n 2     1.00
                                           r = 59 ◦
              The angle of refraction is greater than the angle of incidence because n 2 < n 1 .

        SOLVED PROBLEM 30.15

                                                                      ◦
              A beam of light strikes a pane of glass at an angle of incidence of 50 . If the angle of refraction is 30 ,
                                                                                               ◦
              find the index of refraction of the glass.
                  According to Snell’s law, n 1 sin i = n 2 sin r. Here air is medium 1, so n 1 = 1.00 and

                                               sin i         sin 50 ◦
                                      n 2 = (n 1 )   = (1.00)      = 1.53
                                               sinr          sin 30 ◦
        SOLVED PROBLEM 30.16
                                                                                       ◦
              A ray of light enters a glass plate whose index of refraction is 1.5 at an angle of incidence of 50 (Fig. 30-9).
              At what angle does the ray leave the other side of the plate?



                                                 i 1

                                                                          Air
                                                                        Glass

                                                    r 1
                                                         i 2

                                                                        Glass
                                                                          Air

                                                             r 2



                                                    Fig. 30-9

                  We start by finding the angle of refraction r 1 at the first side of the plate:

                                             n air         1.0
                                                                    ◦
                                     sinr 1 =     (sin i 1 ) =  (sin 50 )
                                             n glass       1.5
                                                  1.0
                                       r 1 = sin −1  sin 50 ◦  = sin −1  0.51 = 30.7 ◦
                                                 1.5
              The angle of incidence i 2 at the other side of the plate is equal to r 1 . Hence

                                        n glass       n glass       1.5       ◦
                                sinr 2 =     (sin i 2 ) =  (sinr 1 ) =  (sin 30.7 )
                                        n air         n air         1.0
                                             1.5
                                  r 2 = sin −1  sin 30.7 ◦  = 50 ◦
                                            1.0
              The ray leaves the glass plate parallel to its original direction but shifted to one side. This result would be true
              regardless of the index of refraction of the glass.
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