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Eddington Grey Atmosphere

What you are seeing: the textbook temperature profile of a grey stellar atmosphere in radiative equilibrium T(τ)=Teff[3/4(τ+2/3)]1/4T(\tau) = T_\text{eff} [3/4 (\tau + 2/3)]^{1/4}. Three special points are marked: the photosphere at τ=2/3\tau = 2/3 where T=TeffT = T_\text{eff}, the boundary τ=0\tau = 0 where T=Teff/24T = T_\text{eff}/\sqrt[4]{2}, and the deep-interior asymptote TTeff(3τ/4)1/4T \to T_\text{eff} (3\tau/4)^{1/4}.

The right panel shows the linear Eddington limb-darkening law I(μ)/I(1)=0.4+0.6μI(\mu)/I(1) = 0.4 + 0.6\mu (with μ=cosθ\mu = \cos\theta). The center of the solar disk is bright; the limb is dimmer by 60 percent. This is what gives the Sun its visible darkening toward the edge.

Figure 1. Eddington grey atmosphere: T(tau) plus Eddington-Barbier limb darkening.
T_eff (K)5778

WHAT TO TRY

  • Slide T_eff: the whole T(tau) profile scales with it, but the three marked points stay at fixed optical depths. The photosphere is always at tau = 2/3 where T = T_eff.
  • Read the surface boundary: at tau = 0 the temperature is T_eff/2^(1/4), not zero. A real atmosphere has a finite skin temperature set by the inward radiation field.
  • Check the limb-darkening readout: the grey atmosphere predicts a specific center-to-limb intensity ratio, the classic test of the Eddington approximation against real stellar disks.