In this and the following two problems we will use Fermat’s principle to derive laws governing paraxial image formation by spherical mirrors.
Consider an object point O in front of a concave mirror whose center of curvature is at the point C. Consider an arbitrary point Q on the axis of the system and using a method similar to that used in Example 3.3, show that the optical path length Lop(= OS + SQ) is approximately given by
(90)
where the distances x, y and r and the angle θ are defined in Fig. 3.32; θ is assumed to be small. Determine the paraxial image point and show that the result is consistent with the mirror equation
(91)
where u and v are the object and image distance and R is the radius of curvature with the sign convention that all distances to the right of P are positive and to its left negative.
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