Radiation Pressure — Question 9

Section 33-5 · Physics pages 5468–5469

Question 9 An isotropic radiation field has pressure one third of energy density A cavity contains isotropic radiation with total energy density u. Its energy density per solid angle is u divided by 4 pi. The wall perfectly reflects. A ray at angle theta from the wall normal has incident energy flux c cos(theta) times its directional energy density. reflecting wall Schematic; labels, not drawing lengths, specify the data. (a) Write the angular integral of normal momentum transfer at the wall. (b) Evaluate it and compare with a single normally incident beam having energy density u.
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Question 9 - Solution An isotropic radiation field has pressure one third of energy density reflecting wall (a) Method and calculation dp = 2 cos θ c (uc cos θ 4π dΩ ) . p = u 2π ∫2π 0 dϕ ∫π/2 0 cos2 θ sin θ dθ. (b) Interpretation and further calculation ∫π/2 0 cos2 θ sin θ dθ = 1/3 ⇒p = u/3 . pbeam = 2I/c = 2u ⇒p/pbeam = 1/6 . Physical check The cavity u includes all directions, including rays moving away from this wall; the comparison beam u is entirely incident normally.

Question 9

An isotropic radiation field has pressure one third of energy density

A cavity contains isotropic radiation with total energy density u. Its energy density per solid angle is u divided by 4 pi. The wall perfectly reflects. A ray at angle theta from the wall normal has incident energy flux c cos(theta) times its directional energy density.

Diagram shown in the original SVG worksheet.

  1. Write the angular integral of normal momentum transfer at the wall.

  2. Evaluate it and compare with a single normally incident beam having energy density u.

Question 9 - Solution

An isotropic radiation field has pressure one third of energy density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dp=2cos⁡θc(uccos⁡θ4πdΩ).dp=\frac{2\cos\theta}{c}\left(\frac{uc\cos\theta}{4\pi}d\Omega\right).p=u2π∫02πdϕ∫0π/2cos⁡2θsin⁡θdθ.p=\frac{u}{2\pi}\int_0^{2\pi}d\phi\int_0^{\pi/2}\cos^2\theta\sin\theta\,d\theta.

(b) Interpretation and further calculation

∫0π/2cos⁡2θsin⁡θdθ=1/3⇒p=u/3.\int_0^{\pi/2}\cos^2\theta\sin\theta\,d\theta=1/3\Rightarrow\boxed{p=u/3}.pbeam=2I/c=2u⇒p/pbeam=1/6.p_{\mathrm{beam}}=2I/c=2u\Rightarrow\boxed{p/p_{\mathrm{beam}}=1/6}.

Physical check

The cavity u includes all directions, including rays moving away from this wall; the comparison beam u is entirely incident normally.