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Spherical Aberration. For the pasage through the left side of lens, the two optical paths q ℓo = R12 + (so + R1 )2 − 2R1 (so + R1 ) cos φ1 q ℓ1 = R12 + (s1 − R1 + d)2 + 2R1 (s1 − R1 + d) cos φ1 . combine to n1 n2 1 + = ℓo ℓ1 R1 µ ¶ so s1 + d −n1 + n2 . ℓo ℓ1 We set d = 0 and concentrate on h up the lens where we can approximate the small angle φ ≃ h/R. we than expand cos φ ∼ 1 − φ2 /2 in the eqns for 1/ℓo ≃1/so − (so + R)h2 /(2s2o R) 1/ℓ1 ≃1/s1 − (s1 − R)h2 /(2s2o R). The spherical aberration correction to the thin lense formala is " ni n2 1 n1 + = (−n1 + n2 ) + h2 so s1 R1 2so µ 1 1 + so R1 ¶2 + n2 2s1 µ 1 1 − R1 s1 ¶2 # . This extra positive term causes the ray in the lens to bend down passing before the focus, This is called a longitudinal spherical aberration. URL on lens aberrations: ¡ a href=”http://www.photonics.com/EDU/Handbook.aspx?AID=25443”¿Example of lens aberations¡/a¿ (with ways to avoid defects in imagery) ¡ a href=”http://www.edmundoptics.com/technical-resources-center/optics/compar of-optical-aberrations/”¿Edmunds Optical webpage¡/a¿ ¡ a href=”https://en.wikipedia.org/wiki/Optical aberration”¿WikiPedia articles aware of its weakness as first two are not.¡/a¿ ¡ a href=”https://micro.magnet.fsu.edu/primer/java/aberrations/spherical/index.ht microscope optical aberations¡/a¿ Its itemst starts in different order: field curvature. (java tutorials) astigmatism; chromatic aberration; comatic aberration; curvature of field; geometric distortion; spherical aberration; focus depth and spherical aberration; cover glass thickness correction; adjustment of objective correction collars; ¡ a href=”https://micro.magnet.fsu.edu/primer/lightandcolor/opticalaberrations.ht defects in lens systems (aimed at optical microscope with java tutorials¿¡/a¿