A red dwarf star has surface temperature and radius

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Condensed Matter, Materials & Soft Matter · Origins of quantum theory

Thermal Physics, Ch Photons and phonons: blackbody radiation and the heat capacity of solids

Problem

A red dwarf star has surface temperature 3200 K3200\,\mathrm{K} and radius 0.35 R⊙0.35\,R_\odot, with R⊙=6.96×108 mR_\odot = 6.96\times10^{8}\,\mathrm{m}. A rocky planet orbits it at 0.12 AU0.12\,\mathrm{AU}, where 1 AU=1.496×1011 m1\,\mathrm{AU} = 1.496\times10^{11}\,\mathrm{m}, and has albedo A=0.15A = 0.15. Treat the star as a black radiator, the planet as a bare rotating ball of uniform temperature with no atmosphere, absorbing the fraction 1−A1-A of the starlight and radiating like a black surface, and ignore any internal heat source. You may use ∫0∞x2/(ex−1) dx=2.404\int_0^\infty x^2/(e^x-1)\,\mathrm{d}x = 2.404. ((a)) Find the radiation flux SS at the planet's orbit. ((b)) Find the planet's surface temperature. ((c)) A sealed lava tube of volume 1.0 m31.0\,\mathrm{m^3} sits just below the surface at the planet's temperature. Find the number of photons it holds, and, using the effusion result of Chapter 2 with every photon moving at cc, the rate at which photons would stream out through a 4.0 cm24.0\,\mathrm{cm^2} opening. ((d)) A lump of iron (θD=470 K\theta_D = 470\,\mathrm{K}) from the planet's surface is at 50 K50\,\mathrm{K} on the night side. Using the low-temperature T3T^3 law, estimate its lattice heat capacity per mole, ignoring the electronic contribution.

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