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Table 2

Key parameters for all evaluated models consisting of H–He, water, rock, and potentially iron.

Model name Tc (K) S0Sc (erg K−1 g−1) ra→ na MXY (M) MFe (M) w:r ratio ρc (kg m−3)
model 1 CC 27 854 8.601−7.339 0.559 0.12 10.24 3.96 0.22 2.6 11 523
model 2 CC 20 182 8.605−7.275 0.626 0.14 13.07 0.63 0.70 20.7 14358
model 3 CC 12 740 8.595−7.201 0.753 0.48 12.78 0.87 0.40 14.7 11 701

model 1 PV 7457 8.598−7.334 0.837 1.25 11.60 1.68 0 6.9 6035
model 2 PV 9822 8.599−7.505 0.822 0.81 12.88 0.84 0 15.3 4893
model 3 PV 10 600 8.598−7.489 0.826 0.96 12.33 1.25 0 9.9 5159
model 4 PV 9773 8.596−7.496 0.801 0.66 12.97 0.91 0 14.2 4964
model 5 PV 9135 8.596−7.419 0.812 0.92 12.24 1.38 0 8.9 5546

model 1 PH 17 130 8.596−7.466 0.742 0.27 12.26 2.00 0 6.1 6070
model 3 PH 11 938 8.603−7.466 0.760 0.77 11.57 2.20 0 5.3 5672
model 4 PH 11 948 8.600−7.479 0.759 0.75 11.50 2.28 0 5.0 5556

Notes. The models are separated into three groups: The first group consists of models with a high central density (see Fig. 1). The second group uses the slower rotation period of Uranus (PV) to calculate its structure. The third group uses the faster rotation period (PH) instead. MXY, , and MFe are the total bulk abundances of H–He, water, rock and iron, respectively. Finally, w:r is the water-to-rock ratio. Note that compared to pure rock models (Table 1) these models tend to have lower central temperatures and higher bulk heavy-element abundances.

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