Photons Have Momentum — Question 3

Section 38-3 · Physics pages 6296–6297

Question 3 Oblique reflection introduces separate momentum and projected-area factors A beam of intensity I measured per area perpendicular to the beam strikes a perfect stationary mirror at angle θ from the surface normal. A mirror patch has area A. Reflection is specular. θ Schematic; labels, not drawing lengths, specify the data. (a) Derive the normal force and pressure on the patch. (b) Evaluate their factors relative to normal incidence at θ = 60◦.
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Question 3 - Solution Oblique reflection introduces separate momentum and projected-area factors θ (a) Method and calculation Phit = IA cos θ, ∆pn = 2(Eγ/c) cos θ. Fn = 2IA cos2 θ/c , Pn = 2I cos2 θ/c . (b) Interpretation and further calculation Fn(60◦)/Fn(0) = cos2 60◦= 1/4 . Pn(60◦) = I/(2c) . Physical check One cosine comes from photon momentum normal to the mirror; the other comes from the illuminated projected area.

Question 3

Oblique reflection introduces separate momentum and projected-area factors

A beam of intensity ℐ\mathcal I measured per area perpendicular to the beam strikes a perfect stationary mirror at angle θ\theta from the surface normal. A mirror patch has area A. Reflection is specular.

Diagram shown in the original SVG worksheet.

  1. Derive the normal force and pressure on the patch.

  2. Evaluate their factors relative to normal incidence at θ=60∘\theta=60^\circ.

Question 3 - Solution

Oblique reflection introduces separate momentum and projected-area factors

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Phit=ℐAcos⁡θ,Δpn=2(Eγ/c)cos⁡θ.P_{\mathrm{hit}}=\mathcal I A\cos\theta,\qquad\Delta p_n=2(E_\gamma/c)\cos\theta.Fn=2ℐAcos⁡2θ/c,𝒫n=2ℐcos⁡2θ/c.\boxed{F_n=2\mathcal I A\cos^2\theta/c},\qquad\boxed{\mathcal P_n=2\mathcal I\cos^2\theta/c}.

(b) Interpretation and further calculation

Fn(60∘)/Fn(0)=cos⁡260∘=1/4.\boxed{F_n(60^\circ)/F_n(0)=\cos^260^\circ=1/4}.𝒫n(60∘)=ℐ/(2c).\boxed{\mathcal P_n(60^\circ)=\mathcal I/(2c)}.

Physical check

One cosine comes from photon momentum normal to the mirror; the other comes from the illuminated projected area.