In optics, the Herschel's condition is a condition for an optical system to produce sharp images for objects over an extended axial range, i.e. for objects displaced along the optical axis. It was formulated by John Herschel.
Mathematical formulation The Herschel's condition in mathematical form is
1 − cos α o 1 − cos α i = 1 − cos β o 1 − cos β i = n i 2 n o 2 | M T | 2 {\displaystyle {\frac {1-\cos \alpha _{\mathrm {o} }}{1-\cos \alpha _{\mathrm {i} }}}={\frac {1-\cos \beta _{\mathrm {o} }}{1-\cos \beta _{\mathrm {i} }}}={\frac {n_{i}^{2}}{n_{o}^{2}}}|M_{T}|^{2}}
where α o , β o {\displaystyle \alpha _{o},\beta _{o}} are the object side ray angles, α i , β i {\displaystyle \alpha _{i},\beta _{i}} are the image side ray angle. n o , n i {\displaystyle n_{o},n_{i}} are the object and image side refractive index, and M T {\displaystyle M_{T}} is the transverse magnification. This condition can be derived by the Fermat's principle. This condition can also be expressed as
M L = n o sin 2 ( α o / 2 ) n i sin 2 ( α i / 2 ) = n o ( 1 − cos α o ) n i ( 1 − cos α i ) and M T = n o sin ( α o / 2 ) n i sin ( α i / 2 ) {\displaystyle M_{L}={\frac {n_{o}\sin ^{2}(\alpha _{\mathrm {o} }/2)}{n_{i}\sin ^{2}(\alpha _{\mathrm {i} }/2)}}={\frac {n_{o}(1-\cos \alpha _{\mathrm {o} })}{n_{i}(1-\cos \alpha _{\mathrm {i} })}}{\text{ and }}M_{T}={\frac {n_{o}\sin(\alpha _{\mathrm {o} }/2)}{n_{i}\sin(\alpha _{\mathrm {i} }/2)}}}
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