Consider an object O placed at a distance u from a convex lens as shown in figure. Let its image I after two refractions from spherical surfaces of radii R1 (positive) and R2 (negative) be formed at a distance v from the lens. Let v1 be the distance of image formed by refraction from the refracting surface of radius R1 . This image acts as an object for the second surface. Using,
This expression relates the image distance v of the image formed by a thin lens to the object distance u and to the thin lens properties (index of refraction and radii of curvature). It is valid only for paraxial rays and only when the lens thickness is much less then R1 and R2 . The focal length f of a thin lens is the image distance that corresponds to an object at infinity. So, putting u = ∞ and v = f in the above equation, we have
If the refractive index of the material of the lens is µ and it is placed in air, µ2 = µ and µ1 = 1 so that Eq. (iv) becomes
This is called the lens maker’s formula because it can be used to determine the values of R1 and R2 that are needed for a given refractive index and a desired focal length f.
Combining Eqs. (iii) and (v), we get