A ray parallel to the principal axis is incident at \(30^\circ\) from the normal on a concave mirror having radius of curvature \(R\). The point on the principal axis where rays are focused is \(O\) such that \(PQ\) is:
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For oblique incidence on spherical mirrors, focal length depends on angle:
\[
f_{\theta} = \frac{R}{2}\cos\theta
\]
Use geometry instead of paraxial approximation.