Photons Have Momentum — Question 10

Section 38-3 · Physics pages 6310–6311

Question 10 Random reflection gives impulse fluctuations even for a fixed photon count A pulse contains exactly N normally incident photons, each of momentum p. Each photon independently reflects with probability R or is absorbed with probability 1 −R. Mirror recoil is negligible. The reflected count K is binomial, with ⟨K⟩= NR and Var K = NR(1 −R). photons detector R Schematic; labels, not drawing lengths, specify the data. (a) Find the mean and variance of the impulse delivered to the surface. (b) For R = 1/2, find the relative standard deviation.
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Question 10 - Solution Random reflection gives impulse fluctuations even for a fixed photon count photons detector R (a) Method and calculation J = 2pK + p(N −K) = p(N + K). ⟨J⟩= Np(1 + R) , Var J = Np2R(1 −R) . (b) Interpretation and further calculation R = 1/2 : ⟨J⟩= 3 2Np, σJ = 1 2p √ N. σJ/⟨J⟩= 1/(3 √ N) . Physical check The incident photon number is fixed here; the fluctuations arise from the random absorption/reflection outcomes, not from Poisson input counts.

Question 10

Random reflection gives impulse fluctuations even for a fixed photon count

A pulse contains exactly N normally incident photons, each of momentum p. Each photon independently reflects with probability R or is absorbed with probability 1−R1-R. Mirror recoil is negligible. The reflected count K is binomial, with ⟨K⟩=NR\langle K\rangle=NR and Var⁡K=NR(1−R)\operatorname{Var}K=NR(1-R).

Diagram shown in the original SVG worksheet.

  1. Find the mean and variance of the impulse delivered to the surface.

  2. For R=1/2R=1/2, find the relative standard deviation.

Question 10 - Solution

Random reflection gives impulse fluctuations even for a fixed photon count

Diagram shown in the original SVG worksheet.

(a) Method and calculation

J=2pK+p(N−K)=p(N+K).J=2pK+p(N-K)=p(N+K).⟨J⟩=Np(1+R),Var⁡J=Np2R(1−R).\boxed{\langle J\rangle=Np(1+R)},\qquad\boxed{\operatorname{Var}J=Np^2R(1-R)}.

(b) Interpretation and further calculation

R=1/2:⟨J⟩=32Np,σJ=12pN.R=1/2:\quad\langle J\rangle=\tfrac32Np,\quad\sigma_J=\tfrac12p\sqrt N.σJ/⟨J⟩=1/(3N).\boxed{\sigma_J/\langle J\rangle=1/(3\sqrt N)}.

Physical check

The incident photon number is fixed here; the fluctuations arise from the random absorption/reflection outcomes, not from Poisson input counts.