Consider a convex lens (or concave lens) of absolute refractive index to be placed in a rarer medium of absolute refractive index. 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=PI1=V1(asthelensisthin)CC1=PC1=R1CO=P1O=u
It follows from the diffraction due to convex spherical surfaceXP1Y
(μ1−u)+(μ2v1)=(μ2−μ1R1)...(1)
the refracted ray from A suffers a second refraction on the surface XP2Y and emerges along BI . Therefore I is the final real image ofO .
Here the object distance is
u=CI1≃P2I1=V
Note that lens thickness is very small. It follows from the refraction due to convex spherical surface XP1Y
CI≃P2I=V(−μ2v1)+(μ2v)=(−μ2−μ1R2)...(2)
1v−1u=1f...(3)
adding equation (1) and (2)
⇒μ1[1v−1u]=μ2−μ1[1R1−1R2]⇒1v−1u=μ2−μ1μ1[1R1−1R2]
⇒1f=μ2−μ1μ1[1R1−1R2](replaced by equation (3))
using μ2μ1=μ
⇒1f=(μ−1)[1R1−1R2] this is called lens maker formula.