By Robert E Fischer; Biljana Tadic-Galeb; Paul R Yoder; et al
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8. 2 Manufacture of Spherical Lens Surfaces 38 Chapter 3 Earlier we said that geometrical aberrations are due entirely to the failure of the lens or optical system to form a perfect geometrical image. Maxwell formulated three conditions that have to be met for the lens to form a perfect geometrical image: 1. All the rays from object point O after passing through the lens, must go through the image point O ′. 2. Every segment of the object plane normal to the optical axis that contains the point O must be imaged as a segment of a plane normal to the optical axis, which contains O ′.
As we begin to learn more about image formation, it is important to understand just how light bends or refracts when passing through an air-glass or glass-air interface. As shown in Fig. 9, the refractive index of a material ϭ n, where n is the ratio of the velocity of light in a vacuum to the velocity of light in the denser material such as glass. Since the light or electromagnetic radiation slows down in the denser material, the refractive index is always greater than unity. 85.
Since the light or electromagnetic radiation slows down in the denser material, the refractive index is always greater than unity. 85.