| |  | | Lens Maker's Formula |  | | It is a relation that connects focal length of a lens to radii of curvature of the two surfaces of the lens and refractive index of the material of the lens. | | | | The following assumptions are made for the derivation: | | | The lens is thin, so that distances measured from the poles of its surfaces can be taken as equal to the distances from the optical centre of the lens. | | | The aperture of the lens is small. | | | Point object is considered. | | | Incident and refracted rays make small angles. | | |  | | | | Consider a convex lens (or concave lens) of absolute refractive index m2 to be placed in a rarer medium of absolute refractive index m1. | | | | Considering the refraction of a point object on the surface XP1Y, the image is formed at I1 who is at a distance of V1. | | | | CI1= P1I1 = V1 (as the lens is thin) | | | | CC1 = P1C1 = R1 | | | | CO = P1O = u | | | | It follows from the refraction due to convex spherical surface XP1Y | | |  | | | | The refracted ray from A suffers a second refraction on the surface XP2Y and emerges along BI. Therefore I is the final real image of O. | | | | Here the object distance is | | |  | | | | (Note P1P2 is very small) | | |  | | | | (Final image distance) | | | | Let R2 be radius of curvature of second surface of the lens. | | | | \ It follows from refraction due to concave spherical surface from denser to rarer medium that | | |  | | | | Adding (1) & (2) | | |  | | |  | | |  | | |  | | |  | | source; -google search ....
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