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We derive an updated, analytic formula for the gravitational radius, r g , of an irradiated, thin disk. For such a disk, the region outside the gravitational radius will produce a thermal wind, while the region interior to the gravitational radius will be stable. We find that r g ≈ 1.4 ( M * / M ⊙ )/( T 0 /10 4 K) AU. The value of 1.4 AU is approximately one fifth of currently used values. The analysis uses the adiabatic approximation. We argue that the same formula applies for the non-adiabatic, isothermal case.
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Kurt Liffman (2003) studied this question.
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