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Table 2

Overview of modified Shakura-Sunyaev models for β Lyr A disc.

Assumption Designation κ(ρ, T) Consistency Trγ Figs.
PgPr Kramers 61024ρT72$6 \cdot 10^{24} \rho T^{-\frac{7}{2}}$ Yes −0.75 1,2a,2b,2c,2d
PgPr “Ridge” 107.67ρ0.72T0.1$10^{7.67} \rho^{0.72} T^{-0.1}$ Yes, except for α ≤ 0.01 −1.08 D.1a, D.1b
PgPr High temperatures 1018.6ρ0.77T2.5$10^{18.6} \rho^{0.77} T^{-2.5}$ Yes −0.79 D.2
PgPr Kramers 61024ρT72$6 \cdot 10^{24} \rho T^{-\frac{7}{2}}$ No 1
PgPr “Ridge” 107.67ρ0.72T0.1$10^{7.67} \rho^{0.72} T^{-0.1}$ No D.1a,D.3a, D.3b
PgPr Inverse problem 61023ρ2T1$6 \cdot 10^{23} \rho^{2} T^{-1}$ Only in the inner disc for α = 0. 1 D.4, D.5a, D.5b, D.5c, D.5d
PgPr Kramers 61024ρT72$6 \cdot 10^{24} \rho T^{-\frac{7}{2}}$ No 1
PgPr “Ridge” 107.67ρ0.72T0.1$10^{7.67} \rho^{0.72} T^{-0.1}$ No D.1a
PgPr Extreme temperatures 61023ρ0.5T72$6 \cdot 10^{23} \rho^{0.5} T^{-\frac{7}{2}}$ Only close to α ≈ 1 .0 D.6, D.7a, D.7b, D.7c, D.7d

Notes. The assumption refers to the choice of pressure approximation, the designation to the choice of opacity approximation (i.e. a region of the opacity function Rogers & Iglesias 1992) and κ(ρ, T) is the specific form of the prescription. The consistency reports whether there are any contradictions between the computed profiles and assumptions used in the derivation. The power law is a qualitative description of the computed temperature profile that dominates in the outer part of the disc, where the ‘bending’ term (Eq. (5)) is negligible.

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