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As shown in the figure, a paraxial ray is incident

at point Q on a concave mirror.

q = angle of incidence = angle of reflection

= Ð CQF = Ð QCF ( by geometry )

So, for D CFQ,

exterior Ð QFP = Ð CQF + Ð QCF = 2q .

For paraxial incident ray and small aperture,

CP' » CP = R and FP' » FP = f.

For small aperture, 2q is very small.

\ from the figure, 2q »

FP

QP

=

f

QP

… ( 1 ) and q =

CP

QP

=

R

QP

… ( 2 )

From equations ( 1 ) and ( 2 ), R = 2f ⇒ f = R / 2

Thus, focal length of a concave mirror is half its radius of curvature.

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