The focal length of a lens is determined by the curvature of its optical surfaces and the refractive index of the material. It is independent of the lens's size or aperture, provided the light rays interact with the relevant curved surfaces.
Consider a symmetrical biconvex lens with radii of curvature \(R\) and \(-R\), and focal length \(f\). The lens maker's formula gives:
\(\frac{1}{f} = (\mu - 1) \left( \frac{1}{R} - \frac{1}{-R} \right) = \frac{2(\mu-1)}{R}\)
When this lens is cut into two identical halves along its principal axis, each half becomes a plano-convex lens. This plano-convex lens has one flat surface (radius of curvature \(\infty\)) and one curved surface (radius of curvature \(R\)). Its focal length, \(f_{half}\), is given by:
\(\frac{1}{f_{half}} = (\mu - 1) \left( \frac{1}{R} - \frac{1}{\infty} \right) = \frac{\mu-1}{R}\)
Comparing the two equations:
\(\frac{1}{f_{half}} = \frac{1}{2} \left( \frac{2(\mu-1)}{R} \right) = \frac{1}{2} \left( \frac{1}{f} \right)\)
Therefore, the focal length of each half-lens is:
\(f_{half} = 2f\)
The original lens is cut into four identical pieces along *and* perpendicular to its principal axis. This means the two halves (obtained by cutting along the axis) are further cut perpendicular to the axis, passing through the center.
Thus, the focal length of each of the four identical pieces remains \(2f\).
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