The Cosmic Background Radiation — Question 4

Section 44-11 · Physics pages 7498–7499

Question 4 A photon gas has a calculable mean energy and particle density Use nγ = 20.29T 3 cm−3 and ⟨E⟩= 2.701kBT. Let T=2.725 K and kB = 8.617 × 10−5 eV/K. V = 1 m3 Schematic; labels, not drawing lengths, specify the data. (a) Find photon density and mean photon energy. (b) Calculate total photon energy in one cubic meter, using 1 eV = 1.602 × 10−19 J.
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Question 4 - Solution A photon gas has a calculable mean energy and particle density V = 1 m3 (a) Method and calculation nγ = 20.29(2.725)3 ≃410.6 cm−3 = 4.106 × 108 m−3 . ⟨E⟩= 2.701(8.617 × 10−5)(2.725) ≃6.343 × 10−4 eV . (b) Interpretation and further calculation U = nγV ⟨E⟩. U(1 m3) ≃4.17 × 10−14 J . Physical check The mean photon energy is not the energy at either spectral peak. The result agrees with the independent blackbody energy-density law to rounding.

Question 4

A photon gas has a calculable mean energy and particle density

Use nγ=20.29T3n_\gamma=20.29T^3 cm−3^{-3} and ⟨E⟩=2.701kBT\langle E\rangle=2.701k_BT. Let T=2.725 K and kB=8.617×10−5k_B=8.617\times10^{-5} eV/K.

Diagram shown in the original SVG worksheet.

  1. Find photon density and mean photon energy.

  2. Calculate total photon energy in one cubic meter, using 1eV=1.602×10−191\ {\mathrm{eV}}=1.602\times10^{-19} J.

Question 4 - Solution

A photon gas has a calculable mean energy and particle density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

nγ=20.29(2.725)3≃410.6cm−3=4.106×108m−3.\boxed{n_\gamma=20.29(2.725)^3\simeq410.6\ {\mathrm{cm^{-3}}}=4.106\times10^8\ {\mathrm{m^{-3}}}}.⟨E⟩=2.701(8.617×10−5)(2.725)≃6.343×10−4eV.\boxed{\langle E\rangle=2.701(8.617\times10^{-5})(2.725)\simeq6.343\times10^{-4}\ {\mathrm{eV}}}.

(b) Interpretation and further calculation

U=nγV⟨E⟩.U=n_\gamma V\langle E\rangle.U(1m3)≃4.17×10−14J.\boxed{U(1\ {\mathrm{m^3}})\simeq4.17\times10^{-14}\ {\mathrm{J}}}.

Physical check

The mean photon energy is not the energy at either spectral peak. The result agrees with the independent blackbody energy-density law to rounding.