Kramers' opacity law describes the opacity of a medium in terms of the ambient density and temperature, assuming that the opacity is dominated by bound-free absorption (the absorption of light during ionization of a bound electron) or free-free absorption (the absorption of light when scattering a free ion, inverse of bremsstrahlung). It is often used to model radiative transfer, particularly in stellar atmospheres. The relation is named after the Dutch physicist Hendrik Kramers, who first derived the form in 1923. The general functional form of the opacity law is κ ¯ ∝ ρ {\displaystyle {\bar {\kappa }}\propto \rho } T − 7 / 2 , {\displaystyle T^{-7/2},} where
κ ¯ {\displaystyle {\bar {\kappa }}} is the resulting average opacity ((kg/m3)−1/m),
ρ {\displaystyle \rho } is the density and
T {\displaystyle T} the temperature of the medium. Often the overall opacity is inferred from observations, and this form of the relation describes how changes in the density or temperature (highly non-linear) will affect the opacity.
Calculation The specific forms for bound-free and free-free absorption are:
Bound-free κ ¯ bf = 4.34 × 10 25 g bf t ⋅ Z ( 1 + X ) ⋅ ρ g / c m 3 ( T K ) − 7 / 2 c m 2 g − 1 , {\displaystyle {\bar {\kappa }}_{\text{bf}}=4.34\times 10^{25}{\frac {g_{\text{bf}}}{t}}\cdot Z(1+X)\cdot {\frac {\rho }{\rm {g/cm^{3}}}}\left({\frac {T}{\rm {K}}}\right)^{-7/2}{\rm {\,cm^{2}\,g^{-1}}},}
Free-free κ ¯ ff = 3.68 × 10 22 g ff ⋅ ( 1 − Z ) ( 1 + X ) ⋅ ρ g / c m 3 ( T K ) − 7 / 2 c m 2 g − 1 . {\displaystyle {\bar {\kappa }}_{\text{ff}}=3.68\times 10^{22}g_{\text{ff}}\cdot (1-Z)(1+X)\cdot {\frac {\rho }{\mathrm {g/cm^{3}} }}\left({\frac {T}{\rm {K}}}\right)^{-7/2}\mathrm {cm^{2}\,g^{-1}} .}
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