A perfect reflecting mirror of mass M mounted on a spring constitudes a spring-mass system of angular frequency Ω such that 4πMΩh=1024 m−2 with h as Planck's constant. N photons of wavelength λ=8π×10−6 m strike the mirror simultaneously at normal incidence such that the mirror gets displaced by 1 μm. If the value of N is
Let momentum of one photon is p and after reflection velocity of the mirror is v conservation of linear momentum
Np^i=−Np^i+mv^i
mv^i=2pN^i
mv=2Np
since v is velocity of mirror (spring mass system) at mean position,
v=AΩ
Where A is maxiflection of mirror from mean position . (A=1 μm) and Ω is angular frequency of mirror spring system,
momentum of 1 photon, p=hλ
mv=2Np
mAΩ=2Nhλ
N=mΩh×λA2
given, mΩh=10244π m−2
λ=8π×10−6 m
N=10244π×8π×10−6×10−62
N=1012=X×1012
Hence X=1