Table 4
Tabulated radii of a pure water sphere using either an adiabatic temperature gradient (RadiusAd) or an isothermal temperature profile (Radiusi.t.) and various surface temperatures.
| Tsurf [K] | RadiusAd [R⊕ ] | Radiusi.t. [R⊕] | δR [%] |
|---|---|---|---|
| Mass = 0.5 M⊕ | |||
| 200.0 | 1.154 | 1.151 | 0.27 |
| 300.0 | 1.170 | 1.157 | 1.10 |
| 500.0 | 1.231 | 1.185 | 3.87 |
| 1000.0 | 2.933 | 1.446 | 102.8 |
| 2000.0 | 27.176 | 2.007 | 1254.1 |
| Mass = 5.0 M⊕ | |||
| 200.0 | 2.148 | 2.143 | 0.22 |
| 300.0 | 2.159 | 2.146 | 0.61 |
| 500.0 | 2.200 | 2.159 | 1.91 |
| 1000.0 | 2.768 | 2.249 | 23.1 |
| 2000.0 | 3.046 | 2.401 | 26.9 |
Notes. The surface pressure was chosen as in Sect. 5.1 of Mazevet et al. (2019), i.e., either along the vapour curve or if the temperature was supercritical fixed at 1 bar.
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