Spherical aberration in spherical mirrors is a defect that is due to the dependence of focal length ‘f’ on the angle of incidence 'θ' as shown in the figure is given by

where R is radius of curvature of mirror and q is the angle of incidence. The rays that are close to the principal axis are called marginal rays. As a result, different rays focus at different points and the image of a point object is not a point.
If fp and fm represent the focal length of paraxial and marginal rays, respectively, then the correct relationship is:
