Derive the relationship between the focal length and radius of curvature of spherical mirror.
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Solution
MPN= Concave spherical mirror P=Pole F= Principle focus C=Centre of curvature PC=Principle axis f= Focal length of mirror R= Radius of curvature of mirror AD= incident ray EF=reflected ray DC= Normal at point D Angle of incidence=∠ADC Angle of reflection=∠CDF ∠ADC=∠ CDF=θ(let)(By second law of reflection) ∠ADC=∠DCF=θ(alternate angles) In ΔDCF, ∠CDF=∠DCF ΔDCF is a isocsleles triangle ∴DF=PC⎡⎢⎣sidesopp.toequal.anglesinatriangleareequal⎤⎥⎦ If the aperture of mirror is very small i.e., point D is very near to point P then. DF=PF(approx) Hence, PF=FC PE+PF=PF+FC 2PF=PC ...(i) Applying sign convention, PF=−f,PF=R Put in eq. (1) 2(−f)=−R
R=2f
OR
f=R2
Hence, focal length of concave mirror is half of its radius of curvature. For convex mirror: Let, MPN=convex spherical mirror P=Pole F= Principle focus C= Centure of curvature PC= Principle axis f= Focal length of mirror R= Radius of curvature of mirror AD= Incident ray DB=Reflected ray CE= Normal at point D Angle of incidence=∠ADE Angle of reflection=∠EDB ∠ADE=∠EDB=θ(let) (By 2nd law of reflection) ∠EDB=∠ FDC=θ(vertically opposite angles) ∠ADE=∠FCD=θ(corresponding angles) ΔDCF is a isosceles triangle ∴DF=FC⎡⎢⎣Sidesopp.toequalanglesinatriangleareequal⎤⎥⎦ If the aperture of mirror is very small i.e., point D is very near to point P then. DF=PF Hence, PF=FC PF+PF=PF+FC .......(1) Applying sign convetion, $ PF=+f,PC=+R Put in eq.(1)
R=2f
OR
f=R2
Hence focal length of concave mirror is half of its radius of curvature