In optics an afocal system (a system without focus) is an optical system that produces no net convergence or divergence of the beam, i.e. has an infinite effective focal length.[1] This type of system can be created with a pair of optical elements where the distance between the elements is equal to the sum of each element's focal length (d = f1+f2). A simple example of an afocal optical system is an optical telescope imaging a star, the light entering the system is at infinity and the image it forms is at infinity (the light is collimated).[2] Although the system does not alter the divergence of a collimated beam, it does alter the width of the beam, increasing magnification. The magnification of such a telescope is given by
\( {\displaystyle M={\frac {f_{2}}{f_{1}}},} \)
Afocal systems are used in laser optics, for instance as beam expanders, Infrared and forward looking infrared systems, camera zoom lenses and telescopic lens attachments such as teleside converters,[3] and photography setups combining cameras and telescopes (Afocal photography).
See also
Lens (optics)
Teleside converter
Galilean telescope, which uses this design
References
Daniel Malacara, Zacarias Malacara, Handbook of optical design. Page 379
Virendra N. Mahajan, Ray geometrical optics, page 38
Rudolf Kingslake, Optics in photography, page 187
Hellenica World - Scientific Library
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