
Procedure :
- Imagine a point object ‘O’ placed on the principal axis of the thin lens
- Let this lens be placed in a medium of refractive index na and let refractive index of lens be nb.
- Consider a ray, from ‘O’ which is incident on the convex surface of the lens with radius of curvature R1 at A.
- The incident ray refracts at A.
- It forms image at Q, if there were no concave surface. From figure Object distance PO = – u;
Image distance PQ = v = x
Radius of curvature R = R1
n1 = na and n2 = nb .

But the ray that has refracted at A suffers another refraction at B on the concave surface with radius of curvature (R2).
At B the ray is refracted and reaches I.
The image Q of the object due to the convex surface. So I is the image of Q for concave surface.
Object distance u = PQ = + x
Image distance PI = v
Radius of curvature R = – R2
The refraction of the concave surface of lens is medium -1 and surrounding is medium –2.
∴ n1 = nb and n2 = na
Substituting values in \(\frac {n_2}{v} - \frac {n_1}{u}= \frac {(n_2-n_1)}{R} = \frac {n_a}{v}- \frac {n_b}{x} = \frac {(n_b-n_a)}{R_2}\)...(2)
Adding (1) and (2) and dividing both sides by na we have

This is called lens maker's formula.