Page 116 - The Indian Optician Digital Edition March-April 2021
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and the thickness of the second element at P is

                                                                                     2
                                                                              2
                                                                 t  = t  - Ay (x  + ⅓y ).
                                                                                    2
                                                                           2
                                                                  P2
                                                                      C
                                                              Substituting  y - d for y  and  y + d for y , leads to
                                                                                     1
                                                                                                    2
                                                                                            2
                                                                                  2
                                                                 t  = t  + A(y - d)(x  + ⅓(y - d) )
                                                                      C
                                                                  P1
                                                                                                  2
                                                                 and t  = t  - A(y + d)(x2 + ⅓(y + d) ).
                                                                      P2
                                                                           C
                                                                 Adding these to obtain the combined
                                                              thickness variation at P, gives:
                       Figgure 8.  Alvareez lens elements        ୿t = A {-⅔d   - 2d (x  + y )}
                                                                                        2
                                                                                   2
                                                                            3
                                            n
                                                                 Now the term in d 3 is independent of x and y
                                                              and represents the same increment in thickness
                                                              at every point on the combination. It can,
                                                              therefore, be ignored, giving
                                                                                 2
                                                                            2
                                                                 ୿t = - 2Ad (x  + y ).
                                                                 It was shown earlier that the variation in
                                                              thickness can be expressed in terms of the
                                                              spherical and cylindrical components of the
                                                              lens as:
                                                                         2
                                                                                              2
                                                              ୿t = - (x  + y )S - (x sin ת + y cos ת) C / 2000(n - 1)
                                                                     2
                  Figure 9.  Thickness of aan Alvarez componeent
                                            m
                                                                 Hence,
                                                                       2
                                                                 2Ad (x  + y ) = (x  + y )S + (x sin ת + y cos ת) C /
                                                                           2
                                                                                                          2
                                                                                 2
                                                                                     2
                                                              2000(n - 1)
             The value of the coefficient A will
                                                                 and since in Figure 11, to form a spherical
          emerge later.
                                                              element,  x = 0,
             The total thickness variation at P,
                                                                                     2
                                                                 2Ad y  = y  (S + C cos  ת) / 2000(n - 1)
                                                                       2
                                                                           2
             ୿t = z  + z
                  X   Y                                          Dividing through by y2, the resulting sphere
                        3
             = Ayx  + Ay /3                                   power, S, for a movement, d, is found from
                  2
                                                                                            2
                         2
             = Ay(x  + ⅓y )                                      S  =   4000(n - 1) A d  - C cos  ת
                   2
             and the total thickness at P is                     When the Alvarez elements are displaced
                                                              along both the x and y-axes they will generate
                               2
                         2
             t  = t  + Ay(x  + ⅓y ).
                  C
              P
                                                              a sphero-cylinder. When displaced only along
             In the zero position, the elements form          the y-axis, the cylinder is zero. If a cylinder is
          a parallel slab and their centres coincide at       generated its axis will lie along the 45 meridian,
          O. Suppose each element is then slid in the         so ת = 45 and
          opposite direction along the y-axis through the
                                                                 S = 4000(n - 1) A d - C / 2.
          distance, d, (Figure 10).
                                                                 The value of A is determined by the required
             Point P now lies at a distance, y, from O, y   1
          from O  and y  from O .                             power range, k.S, in either the plus or minus
                 1
                                2
                        2
                                                              direction and the movement, d, here expressed
             The thickness of the first element at P is        in millimetres per dioptre of change.
                                2
             t  = t  + Ay (x  + ⅓y )                             A = k.S / 4000(n - 1)
                          2
                       1
                                1
                  C
              P1
           |  MAR-APR 2021  |  112  LENS TALK
   Mar-Apr 2021 SK.indd   60                                                                                 26-04-2021   13:32
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