DIOPTRICS OF THE EYE. 



303 



its refractive power, as measured by the refractive index of the 

 material of which it is composed. Parallel rays are given theo- 

 retically by a source of light at an infinite distance in front of the 

 lens, but practically objects not nearer than about twenty feet 

 give rays so little divergent that they may be considered as par- 



Fig. 124. — Diagrams to illustrate the refraction of light by a convex lens : a., Kefrac- 

 tion of parallel rays ; b., refraction of divergent rays ; c, refraction of divergent rays from 

 a luminous point nearer than the principal focal distance. 



allel, so far as the optical apparatus of the eye is concerned. On 

 the other hand, if a luminous object is placed at F the rays from 

 it that strike upon the lens will emerge from the other surface 

 as parallel rays of light. If a luminous point (/, Fig. 124) is 

 placed in front of such a lens at a distance greater than the prin- 

 cipal focal distance, but not so far as to give practically parallel 

 rays, the cone of diverging rays from it that impinges upon the 

 surface of the lens will be brought to a focus (/') further away 

 than the principal focus. Conversely, the rays from a lumin- 

 ous point at /' will be brought to a focus at /. These points, 

 / and/', are, therefore, spoken of as conjugate foci. All luminous 

 points within the limits specified will have their corresponding 

 conjugate foci, at which their images will be formed by the lens. 

 Lastly, if a luminous point is placed at v, Fig. 124, nearer to the 

 lens than the principal focal distance, the cone of strongly di- 

 vergent rays that falls upon the lens, although refracted, is still 



