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R = radius of curvature, and k = conic constant as given below: k < 1 Hyperboloid k = 1 Paraboloid 1< k < 0 Ellipsoid k=0 Sphere k>0 Oblate ellipsoid The remaining terms in the preceding equation are the symmetrical deviations from the basic conical form The vertical sag of a spherical surface and an aspheric surface with their basic equations and symmetrical deviation is shown Fig 425: How sag can differentiate between in Figure 425 aspheric and spherical surfaces [49] The manufacture of such aspherics has always been a challenge, especially in infrared window materials and metals Therefore, manufacturers and researchers all over have put in a lot of effort to systematically apply measurement science to the design, manufacture, and the fabrication of highly precise devices to achieve low tolerances, better surface finish and low subsurface damage at a reduced cost The principal use of aspheric lens designs is the reduction or elimination of optical aberrations produced when looking through an ophthalmic lens obliquely We will begin our discussion of aspherics by exploring some of these optical aberrations and their effects For ophthalmic lenses, a lens aberration occurs when rays of light fail to come to a point focus at the ideal image position of the eye (called the far point) as it rotates about its centre Fig 426: Rays of light from an object point strike the lens Astigmatic focusing error, which is obliquely and are focused into two separate focal illustrated in Figure 427, results when lines, instead of a single point focus, results oblique rays of light from an object in the astigmatism [49] periphery strike the lens obliquely Two focal lines are produced from each single object point The dioptric difference between these two focal lines is known as the astigmatic error of the lens Rays of light striking the tangential, or radial, plane of the lens come to a line focus at the tangential focus The resultant focal line is perpendicular to the actual tangential plane Rays striking the sagittal, or the equatorial, plane of the lens come to a line focus at the sagittal focus This focal line is perpendicular to the sagittal plane Both of these planes are shown in Figure 427.



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Fig 427: The sagittal (equatorial) and tangential (radial) planes of a lens [49]

y is the output value. This function is called a dot product, and it is one method of calculating how closely two vectors match. It also has further mathematical significance, not relevant to this discussion.

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Fig. 17-12.





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A coma is a distortion in the image, wherein the focus and the magnification are different for rays passing through various zones of the optical system It usually occurs when the incident rays are not parallel to the optical axis and a ring shaped blurred image is formed In refractive optics, chromatic aberration (lateral and longitudinal) alters the image quality when the optical system has to operate in a wide range of wavelengths This is caused by the phenomenon of dispersion (change of refractive index with wavelength), producing a variation in focal length with wavelength Chromatic aberration increases the size of the blur in the image in direct proportion to the spectral range The aforementioned types of aberrations cannot be eliminated simultaneously Therefore, in optical systems, there is a need to combine several lenses to get a better quality image But, on the other hand, limitations on system weight and overall manufacture costs demand fewer lenses Thus, a parabolic surface on silicon proves to be a better choice for infrared applications Since 1950, the development of optical tools and materials has been dramatic, and their contribution to increased productivity cannot be overemphasized The mass production industries, making ophthalmic lenses and cameras, have undoubtedly provided the large market necessary for such a development Rene Descartes was probably the first man to consider the kind of surface that would give freedom from optical aberrations In 1638, he described the geometrical construction of a lens, which would be free from spherical aberration He expressed the corrective surface required to correct the aberration of a transmittive lens The formation of a parabolic surface was first achieved by Short in 1732, who made a reflecting telescope with parabolic and elliptical surfaces, which was known as the Gregorian telescope after James Gregory who, in 1663, made it clear that conical sections would correct spherical aberrations [50] In 1822, A J Fresnel developed a technique to mould plastic lenses for large magnifiers in industrial use These lenses were also suitable for small aperture lens systems in which inhomogeneity and thermal stability are not important But the main disadvantage of these lenses was that a change in the refractive index might cause a shift in the focal plane [50].

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