Let O be a point object in the rarer medium of refractiive index μ1 and lying on the principal axis. The image of this object. O is formed by refraction at the convex spherical surface of radius at the point I into the medium B of refractive index μ2 of curvature as shown in the fig. The convex surface has a small aperture and the angles of incidence z and refraction r are small. Let ∠AOP = α, ∠AIP = β and ∠ACP = γ
From A, draw AN perpendicular to principal axis. For refraction at the point A, by Snell’s law, we have

\(\frac{sinr}{sinr}=\frac{\mu_2}{\mu_1}\)
Since i and r are small, sin i = i and sin r = r
∴ \(\frac{i}{r}\) = \(\frac {\mu_2}{\mu_1}\)
μ1i = μ2r
Now, in ΔAOC, we have
i = α + γ
and in ΔIAC, γ = r + β
r = γ - β
Substituting the value of i and r from (ii) and (iii) into (i) , we have
μ1(α + γ) = μ2 (γ - β)
Since α, β and γ are small, they can be replaced by their tangents

Due to small aperture, the point N lies close to P, also applying sign convention, we get
NO ~ PO = -u, NC ~ PC = R, NI ~ PI = v
Putting these values in (iv), we get
