The optical power of the system of two thin lenses placed in air is given as,
`Phi = Phi_(1) + Phi_(2) - d Phi_(1)Phi_(2)`
or, `(1)/(f) = (1)/(f_(1)) + (1)/(f_(2)) - (d)/(f_(1)f_(2))`, where `f` is the equivalent focal length
So, `(1)/(f) = (f_(2) + f_(1) - d)/(f_(1)f_(2))`
or, `f = (f_(1)f_(2))/(f_(1) + f_(2) - d)......... (1)`
This equivalent focal length of the system of two lenses is measured from the primary principle plane.
As clear from the figure, the distance of the primary principle plane from the optical centre of the first is
`O_(1)H = x =+ (n//Phi) (d//n') Phi_(1)`
`= (d Phi_(1))/(Phi)`, as `n = n' = 1`, for air.
`= (df)/(f_(1))`
`= ((d)/(f_(1))) ((f_(1)f_(2))/(f_(1) + f_(2) - d))`
`= (df_(2))/(f_(1) + f_(2) - d)`
Now, if we place the equivalent lens at the primary principle plane of the lens system, it will provide the same transverse magnification as the system. So, the distance of equivalent lens from the vertex of the first lens is,
`x = (df_(2))/(f_(1) + f_(2) - d)`
