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Lenses are transparent optical components that use refraction to focus or collimate electromagnetic radiation.
Lenses are characterized by their focal length. The focal length is given by the lens maker's formula:
1/f() = [n() - 1][1/R1 - 1/R2]
where f is the focal length, n is refractive index, and R1 and R2 are the radii of curvature of the two surfaces of the lens.
Illustration of lens properties:
Focus spot size of light from infinity:
spot diameter = * f / * D
where is wavelength, f is focal length, and D is diameter of the incoming beam.
The position of an image can be determined by tracing three lines in a diagram:
Finding an image by ray tracing
The position of an image can be found from the ray trace or from:
1/f = 1/xo + 1/xi
where f is the lens focal length, xo is distance of the object from the lens, and xi is the distance of the image from the lens.
Magnification, M, is the ratio of the image size to the object size, and is equal to:
M = xi / xo
where xi and xo are the distances of the image and object from the lens, respectively.
The light collection efficiency is the solid angle that an optic makes with an object. The f-number describes this angle:
f-number: f/# = l/d
where l is distance and d is diameter of lens.
The solid angle that a lens collects is approximately:
= d2 / 4 l2
The fraction of light that an optic collects is this solid angle divided by the total 4 steradians:
fraction collected = /4 = d2 / 16 l2 = 1 / 16 (f/#)2.
Lenses (and curved mirrors) do not focus light perfectly. Chromatic and spherical aberations occur on-axis and coma and astigmitism occur off-axis.
Chromatic aberration occurs due to the variation of refractive index with wavelength for a lens material (there is no chromatic aberation in curved mirrors). This wavelength dependence results in slightly different focal lengths for different wavelengths of light. Compound lenses, called achromats, can reduce or eliminate chromatic aberation because the components are chosen such that the variation in refractive index as a function of wavelength cancels out.
Spherical aberation results because the actual focal point of a light ray depends on its distance from the optic axis.
Coma is caused by the distortion of a wavefront as it encounters an optic asymmetrically. The result for collimated incoming light is a circle instead of a point image. The light rays farther from the optic axis have more severe aberation and the resulting image looks like a comet-shaped series of circles.
The projection of an optic off-axis looks squashed in one direction. The squashed direction focuses light to a greater extent than the normal dimension. The result is two line images.
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