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.
Step 1: For a ray parallel to the principal axis, reflection occurs such that angle of incidence equals angle of reflection.
Step 2: Geometry of the concave mirror gives focal shift due to oblique incidence.
Step 3: Using mirror geometry:
\[
PQ = R\left(1-\cos 30^\circ\right)
\]
Step 4: Substitute \(\cos 30^\circ = \frac{\sqrt{3}}{2}\):
\[
PQ = R\left(1-\frac{\sqrt{3}}{2}\right) = R\left(1-\frac{1}{\sqrt{3}}\right)
\]