Page 176 - Modern Optical Engineering The Design of Optical Systems
P. 176

Characteristics of the Human Eye  159

        fact, a reasonable simulation of the optics of the eye can be made by
        considering the eye as a single refracting surface of water
        (n D   1.333, V   55).
          The following table lists typical values for the radii, thicknesses, and
        indices of the optical surfaces of the eye. These, of course, vary from
        individual to individual.

         R (air to cornea)   7.8 mm  t (cornea) 0.6  n 1.376        v 57
          1                          1                1              1
         R (cornea to aqueous)   6.4 mm  t (aqueous) 3.0  n 1.336   v 61
          2                          2                2              2
         R (aqueous to lens)   10.1 mm  t (lens) 4.0  n 1.386–1.406  v 48
          3                          3                3              3
         R (lens to vitreous)  6.1 mm  t (vitreous) 16.9  n 1.337   v 61
          4                          4                4              4
         R (vitreous to retina) – 13.4 mm
          5
          The principal points are located 1.5 and 1.8 mm behind the cornea,
        and the nodal points are 7.1 and 7.4 mm behind the cornea. The first
        focal point is 15.6 mm outside the eye; the second is, of course, at the
        retina. The distance from the second nodal point to the retina is 17.1
        mm; thus the retinal size of an image can be found by multiplying the
        angular subtense of the object (from the first nodal point) by this dis-
        tance. When the eye accommodates (focuses), the lens becomes nearly
        equiconvex with radii of about 5.3 mm, and the nodal points move a
        few millimeters toward the retina. The center of rotation of the eyeball
        is 13 to 16 mm behind the cornea.
          An often overlooked fact is that the commonly accepted eye data
        tabulated above do not give an adequate picture of the quality of the
        visual system. First, the surfaces of the eye are not spherical. Some sur-
        faces, especially those of the lens, depart significantly from true
        spheres. In general, the surface curvature tends to be weaker toward
        the margin of the surface. Second, the index of the lens is not uniform,
        but is higher in the central part of the lens. This sort of index gradient
        produces convergent refracting power in and of itself; it also reduces
        the surface refracting power at the margin of the lens. Note that both the
        gradient index and the surface asphericities introduce overcorrected
        spherical aberration, which offsets the undercorrected spherical of the
        outer surface of the cornea.
          The retina contains blood vessels, nerve fibers, the light-sensitive rod
        and cone cells, and a pigment layer, in that order in the direction that
        the light travels. The optic nerve and the associated blind spot are
        located where the nerve fibers leave the eyeball and proceed to the brain.
        Slightly (about 5°) to the temporal (outer) side of the optical axis of the
        eye is the macula; the center of the macula is the fovea. At the fovea, the
        structure of the retina thins out and, in the central 0.3-mm diameter,
        only cones are present. The fovea is the center of sharp vision. Outside
        this area rods begin to appear; further away only rods are present.
   171   172   173   174   175   176   177   178   179   180   181