Issue 
A&A
Volume 661, May 2022



Article Number  A101  
Number of page(s)  18  
Section  Planets and planetary systems  
DOI  https://doi.org/10.1051/00046361/202142781  
Published online  20 May 2022 
Internal structures and magnetic moments of rocky planets
Application to the first exoplanets discovered by TESS
^{1}
Departament d’Astronomia i Astrofísica, Universitat de València,
C. Dr. Moliner 50,
46100
Burjassot, Spain
email: andres.moyabedon@uv.es
^{2}
Electrical Engineering, Electronics, Automation and Applied Physics Department, E.T.S.I.D.I, Polytechnic University of Madrid (UPM),
Madrid
28012,
Spain
Received:
29
November
2021
Accepted:
1
March
2022
Context. For a planet to be considered habitable on its surface, it is an important advantage for it to have a magnetic field that protects its atmosphere from stellar winds as well as cosmic rays. The magnetic protection of potentially habitable planets plays a key role in determining the chances of detecting atmospheric biosignatures. In making an estimate of a planet’s magnetic field, its internal structure must first be known.
Aims. This study proposes to use the Preliminary Reference Earth Model (PREM) internal structure as the base of a numerical model, as it is considered the best available option for estimating the internal structure of rocky exoplanets. With this model, we estimate the magnetic properties of dry and waterrich Earthlike and SuperEarthlike planets and we apply it to the first 176 planets of this kind confirmed by the Transiting Exoplanet Survey Satellite exoplanet mission (TESS).
Methods. Using PREM as a reference, we estimated the internal structure of dry and waterrich rocky planets. This model provides an estimation of the average density and core size of the planet, which are the key ingredients for estimating its magnetic moment, depending on whether it is tidally locked or not. Our model estimates the thermodynamic variables as a function of pressure and including saltwater as a component of waterrich exoplanets. In addition, we did not use the perfect layer differentiation approximation. We validated our model based on the selection of planets and satellites in the Solar System with similar characteristics.
Results. Using our model, we estimated the internal structure and magnetic moment of selected dry and waterrich rocky planets and satellites in the Solar system. The differences with the observed values in the internal structure characteristics, mass, average density, moment of inertia factor, and local Rossby number are remarkably low or even negligible. The estimated magnetic moments are also very similar to the observed ones. We applied the model to the first dry and waterrich rocky planets confirmed by TESS, 176 in total, and we find, from an astrobiological perspective, that TOI700 d and TOI2257 b are the most interesting examples, as they are located in the habitable zone. However, we note that their magnetic moments are only about 0.01 of the Earth’s magnetic moment.
Key words: planets and satellites: fundamental parameters / planets and satellites: interiors / planets and satellites: magnetic fields / planets and satellites: terrestrial planets
© ESO 2022
1 Introduction
For a planet to be considered habitable on its surface, it is generally advantageous for it to have a magnetic field that protects its atmosphere from stellar winds and cosmic rays. The magnetic protection of potentially habitable planets plays a key role in determining their habitability and the chances of detecting biomarkers in its atmosphere (Zuluaga et al. 2013). An Earthlike planet without a magnetic field orbiting an active lowmass star can lose its ozone column drastically over a relatively short time (Tilley et al. 2017). If this happens, highenergy cosmic rays can reach the planet’s surface and significantly alter the development of life.
Planetary dynamos are generally thought to be maintained by thermal and compositional convection mechanisms in electrically conducting fluids located in the planet interiors (Olson & Christensen 2006, OC06). The magnetic field generated by the dynamo of a rocky planet depends mainly on the density and size of the convective core, and the convective buoyancy flux generated in this core. Therefore, for estimating the magnetic field generated by a rocky planet, its internal structure needs to be known first. Unfortunately, the interior structure of an exoplanet is hidden from direct observation. For estimating its internal structure from only the Mass and Radius of the exoplanet, we are limited to indirect methods based on theoretical models (Suissa etal. 2018).
Current technological stateoftheart provides, in the best scenario, planetary masses, radii, and orbital periods with uncertainties usually larger than a 10%. In many other cases, their masses or radii are unknown and we must use models for estimating them (Chen & Kipping 2017). In this uncertain context, our approach to solving this problem of describing the internal structure of an exoplanet is to extrapolate it from the internal structure of known objects at the solar system.
In the case of rocky exoplanets, extrapolation from the solar system to know their internal composition implies that a minimum of three primary constituents must be used: iron, enstatite (Mg SiO_{3}), and water (Valencia et al. 2006). In general, for a given chemical composition, the Equation Of State (EOS) of any material can be expressed as: (1)
where ρ is the density, P the pressure, and T the temperature.
The effect of temperature is secondary compared to the effect of pressure for denser constituents such as iron or enstatite (Valencia et al. 2006). For lighter elements such as water, the effect of temperature cannot be disregarded, but a pressuretemperature relation such as the water melting curve can be included in the models to take it into account (Zeng & Sasselov 2013).
Dry rocky planets are those whose water mass is negligible with respect to the total mass of the planet, and therefore its internal structure can be explained by only two components. Nevertheless, the core may also be affected by eutectic melting, most likely due to sulfur. This would be the case for the inner planets of the solar system such as Mercury, Venus, Earth, and Mars. When there are only two basic constituents, for each mass and radius value of the planet the theoretical models provide a unique solution for its internal structure (Suissa et al. 2018; Zeng & Sasselov 2013).
However, waterrich rocky exoplanets need three basic components to explain their internal structure: iron in the core, enstatite in the mantle, and water usually forming an outer layer of ice. In this case, for each mass and radius value, the theoretical models provide infinite internal structure solutions all compatible with those mass and radius values (Suissa et al. 2018; Zeng & Sasselov 2013).
One of the most used assumptions for modelling these different layers is their complete differentiation. Theoretical models using equations of state of pure components need the layers to be completely differentiated, that is, all the iron on the planet must be in the nucleus and all the silicates in the mantle. This complete differentiation does not occur on the inner planets of the solar system and, most likely, it will be difficult to find completely differentiated exoplanets.
Currently, we have PREM (Dziewonski & Anderson 1981), which, through a broad and extensive seismic field study, has allowed us to determine the physical characteristics of the different constituent layers of our planet. The PREM model provides, apart from many other data, a realistic relationship between density and pressure inside Earth, despite the presence of impurities and partial lack of differentiation.
On the other hand, recent studies on the spectrum of white dwarfs contaminated with the remnants of disintegrated planets show that these remnants are quite similar to the earth’s composition. More than 85% of the mass of these remnants are Fe, Mg, Si, and O. In addition, they have Fe/Si and Mg/Si ratios similar to terrestrial ones, and they are accompanied by poor C content. This leads us to assume that these disintegrated planets had a formation and evolution process similar to the inner planets of the solar system (Jura & Young 2014).
In this paper, we aim to construct an internal structure model for rocky planets. The model is a PREMbased internal structure model that is considered the best available option for estimating the internal structure of these rocky exoplanets, extrapolating the behaviour of density within Earth following PREM and performing only those simplifications that are considered strictly necessary. With regard to waterrich rocky planets, we extrapolated the internal structure of the cases of the waterrich Jupiter’s moons (Europa, Ganymede, and Calixto).
With this estimated internal structure, we analysed the temperature profile and the heat crossing the boundary between the planetary core and mantle. The main idea is to use the planetary dynamo scaling laws (OC06) for estimating the magnetic regime (dipolar or multipolar), moment, and field. In summary, we estimated the planetary magnetic shield protecting its atmosphere from erosion provoked by the stellar wind and cosmic rays (RodríguezMozos & Moya 2019). Finally, we applied this model to all the confirmed rocky planets (dry and waterrich) discovered by TESS (Ricker et al. 2014).
Fig. 1 Section of a rocky planet. R_{p} is the Planet radius, r_{0} the core radius, r_{1} the Mantle radius, D the Outer core thickness, and r_{i} the Inner core radius. 
2 Internal structure of dry rocky planets
We considered a rocky planet with the following known properties: normalised mass of () and normalised radius of (), relative to Earth values. In general, this type of planet will have three layers, as can be seen in the crosssection of Fig. 1. In this figure, we can see the innermost layer or core of the planet, which is primarily made up of Fe, and the mantle’s basic components are silicates and oxides of Si, Mg, and Fe. Finally, an outer layer usually of water ice where liquid internal oceans can also exist. When the ice cap does not exist or its mass is negligible compared to the total mass of the planet, it is considered a dry rocky planet. In this case, the radius of the mantle will be the radius of the planet (r_{1} ≈ R_{p}) and the internal structure of the planet is defined by only two layers whose basic elements will be the normalised radius of the core (r_{0}), the normalised average core density (ρ_{0}), and the normalised average density of the mantle (ρ_{1}). To obtain these values, it would be necessary to determine the planetary density and pressure profiles with the radius.
On Earth, however, the planetary core consists of two distinct areas. On the one hand, the outer core is dominated by liquid Fe, with a few percent of Ni and 5–15% of lighter elements (presented in the following sections) and of a thickness referred to as D. Then there is the inner core, composed of crystalline solid Fe. In general, for a dry rocky exoplanet, of which only M_{p} and R_{p} are known, it would be necessary to use models for the thermal evolution of the planet to determine whether part of the nucleus is in a solidstate and to measure the size of this zone.
2.1 Internal composition of the Earth
As noted above, the Earth’s interior is basically composed of four chemical elements: Fe, Mg, Si, and O. The core consists mainly of Fe and, in a much smaller quantity, of other lighter elements such as S, Si, O, and C (Fischer et al. 2012). Nevertheless, there is no consensus in the literature regarding which elements are on the list of these secondary components and in which percentage.
Above 100 GPa, iron is mostly in phase e with a hexagonal crystalline structure (Zeng & Sasselov 2013). Given that the pressure at the coremantle boundary (CMB) of the Earth reaches up to 135 GPa, the solid Fe contained in the core will be all in phase ϵ.
Regarding the mantle, it primarily consists of Mg, Si, O, and (to a lesser extent) Al, Ca, and Na (Sotin et al. 2007). The most abundant compounds in the Earth’s mantle are magnesium silicates, such as enstatite (Mg Si O_{3}) and olivine ((Fe,Mg)_{2} Si O_{4}), as well as oxides like periclase (Mg O) and silica (Si O_{2}). Magnesium silicates often incorporate impurities of Fe which, in the case of enstatite, can reach up to 12%. As the Mg/Si ratio increases, the relative quantity of olivine and periclase also increases. Above 27 Gpa, the polymorphs of olivine are unstable and then the terrestrial mantle is basically composed of enstatite polymorphs such as perovskite (pv) and postperovskite (ppv), and periclase, with this last element only making up about 7% of the total. Reaching 125 GPa and 2500 K, the pv is transformed into ppv with a density jump of around 1.5%. Around 900 GPa, there is a dissociation of ppv into periclase and compact silicates (Mg Si_{2} O_{5}). Above 2100 Gpa, there is the second dissociation of ppv into periclase and silica (Zeng & Sasselov 2013).
2.2 PREM
Dziewonski & Anderson (1981) presented an internal structure model for the Earth obtained using seismic data (PREM). The velocity of the seismic waves at different points is a reflection of the physical characteristics of the different zones they have traveled by. PREM can be considered to be the best approximation to date of the Earth’s internal structure and it has accurately determined the Earth’s mass and radius, as well as the pressure and density as a function of the Earth’s radius.
According to PREM, it is possible to distinguish five large areas in the terrestrial interior: an ocean layer, with a mean thickness of 3 km, upper mantle (mean thickness of 667 km), lower mantle (mean thickness of 2221 km), outer core (mean thickness of 2258.5 km), and inner core (mean thickness of 1221.5 km). The most important physical characteristics of the Earth arising from PREM are included in Table 1, while in Fig. 2, we can see the variation in the radius of the density, gravity, and pressure provided by this model. The density profile has four different zones: upper mantle, lower mantle, outer core, and inner core, with abrupt changes in density in the upper mantle and between these zones. Concerning gravity, two zones are distinguished: the mantle, where it varies very smoothly from the surface down to the CMB, and the core, where it varies linearly down to zero gravity at the centre of the planet, although the slope in the outer core is slightly lower than the slope in the inner core.
Earth’s physical characteristics according to PREM.
Fig. 2 Density, gravity, and pressure profiles normalised to their higher values for Earth according to PREM.ρ_{max} = 13.1 g cm^{−3}, P_{max} = 364 GPa, and g_{max} = 10.7 ms^{−2}. 
2.3 Internal structure model for dry rocky planets
To determine the internal structure of planets, models based on EOS of minerals and metals obtained either theoretically or experimentally in the laboratory are typically adopted in the literature. Several previous models of solid planets have been built using pure constituents, such as solid Fee in the core and pv and ppv in the mantle, without contemplating the presence of impurities or other elements, and considering a complete differentiation of layers that do not occur on real planets (Zeng & Seager 2008; Zeng & Sasselov 2013). These theoretical models do not properly represent the characteristics of Earth. On the one hand, the Earth’s liquid outer core has a lower density than that corresponding to the solid Fee, and on the other hand, the density of the upper mantle cannot be obtained by extrapolating the density of the lower mantle (Zeng et al. 2016). In addition, a perfect differentiation of the different layers is not realistic.
We begin by defining a model for reproducing the internal structure of the Earth as accurately as possible and then move on to exoplanets. This accurate model for dry rocky planets is constructed under the following assumptions: (1) the planet has spherical symmetry; (2) the ocean layer will not be considered because it is irrelevant from the point of view of the internal structure. On Earth, it accounts for only 0.02% of the total mass; (3) inphase transitions of denser constituents such as iron or enstatite, the effect of temperature will be disregarded compared to the effect of pressure (Valencia et al. 2006); (4) the secondorder BirchMurnaghan EOS will be used to define the density behaviour (Birch 1952), providing a precise description of how the materials are compressed inside Earth. This EOS is defined as follows: (2)
where ρ is the density presented by the material when subjected to the pressure P and K_{i} is the isothermal compressibility, while P_{i} is a reference density. This reference density is determined for each of the four layers defined for the Earth comparing the mean density reported by PREM with that calculated by our model. Following this procedure, we obtained:
Solid core: K_{i} = 255 GPa, and ρ_{i} = 7.848 g cm^{−3},
Liquid core: K_{i} = 201 GPa, and ρ_{i} = 7.055 g cm^{−3},
Lower mantle: K_{i} = 206 GPa, and ρ_{i} = 4.010 g cm^{−3},
Upper mantle: K_{i} = 206 GPa, and ρ_{i} = 3.329 g cm^{−3}.
It is important here to highlight that for this model we have not assumed pure components for a given layer or perfect layer differentiation.
Furthermore, for pressures above 12 000 GPa in the core and 3500 GPa in the mantle, electron degeneration pressure dominates while the crystalline structures become less important (Zeng et al. 2016). From these high pressures onward, we use the ThomasFermiDirac EOS (TFD) modified with energy correlation (Salpeter & Zapolsky 1967). This EOS will provide a lower limit for the density of the material under consideration. The atomic values for the enstatite molecule in the mantle we use are A = 20 and Z = 10, and the corresponding for Fe at the nucleus are A = 55.845 and Z = 26. The use of this representation is validated by the good agreements we find when comparing with PREM, with other massradius models in the literature, and with real masses and radii, as we show in next sections.
We have compared this accurate model with PREM. The density, pressure, and gravity profiles obtained faithfully follow those defined by PREM, and the average errors in the variables are negligible. Therefore, it can be concluded that this model reproduces in a tight way the internal structure of the Earth defined by PREM, as expected.
Our goal is to extend this model to exoplanets. In this case, we don’t know whether the core is solid, liquid, or partially liquid, as it is the case of the Earth. But we know that for masses larger than 2.5 M_{⊕} rocky planets are unable to generate a solid core (Gaidos et al. 2010), and for masses larger than 2 M_{⊕} the core remains liquid until the shutdown of its dynamo (Zuluaga et al. 2013; Driscoll & Olson 2011). Therefore, for exoplanets with masses larger than 2 M_{⊕}, we assume that their cores are liquids with the same behaviour as the liquid part of the Earth’s core. On the other hand, exoplanets with masses lower than 2 M_{⊕} we simplify the model assuming the core as a single layer core defined by its radius and mean density, along with a pressuredensity relation following that of the Earth, described in Eq. (2).
If we treat the Earth as an exoplanet and model its core using this simplification, when comparing with PREM we obtain the result that the secondorder BirchMurnaghan EOS coefficients are now K_{i} = 201 GPa, and ρ_{i} = 7.069 g cm^{−3}. In Fig. 3, we show the density, gravity, and pressure profiles as a function of the planet radius obtained for the Earth with this simplified model. In Table 2, we show a comparison of these results with the physical characteristics extracted from PREM. Here, we can see how this simplified model can reproduce accurately the Earth’s internal structure provided by PREM. Only in the core, we can see the absence of two layers in our model, substituted by a mean single layer.
Fig. 3 Density, gravity, and pressure profiles normalised to their higher values for the Earth according our simplified model for exoplanets. Here, ρ_{max} = 12.5 g cm^{−3}, Р_{mах} = 361 GPa, and g_{max} = 10.7 m s^{−2}. 
Comparison between PREM and our simplified model for the Earth, treated as an exoplanet.
2.4 Discussion
We can calculate the fraction of mass that represents the core relative to the total of the planet, namely, the core mass fraction (CMF), expressed as: (3)
In addition, we calculate the fraction of mass of the mantle relative to the total mass of the planet, namely, the mantle mass fraction (MMF) as: (4)
For PREM, the values of which are shown in Table 1, we obtain a CMF = 0.325 and a MMF = 0.675. On any dry rocky planet, where only the core and the mantle are significant in terms of mass, CMF + MMF = 1. Therefore, from Eqs. (3) and (4), we obtain: (5)
with ρ_{p} the average normalised density of the planet.
Another key factor when establishing the internal structure of a planet is the axial moment of inertia factor that imposes the following condition on the internal distribution of mass (Schubert et al. 2004): (6)
with C as the axial moment of inertia. When solving the internal structure of dry rocky planets when only its mass and radius are known, we have three unknown variables (r_{0}, ρ_{0}, and ρ_{1}) and two relations among these variables (Eqs. (5) and (6)). We also have The EOS of the different layers of the mantle and core in the way that, for every r_{0}, we have the mean density of the mantle and the core. We use Eq. (5) for obtaining the value of r_{0} making null the difference between the observed density and that coming from the model. Then we use Eq. (6) for estimating the planetary moment of inertia factor.
Results for dry rocky planets of the Solar System.
Results for lowdensity dry rocky objects of the Solar System.
2.5 Application for other rocky planets in the solar system
As the first test of our model, we verified whether it is capable of reproducing the internal structure of the other rocky planets in the solar system. To do so, the mass and radius, as well as the radius of the nucleus, of Mercury, Venus, and Mars have been introduced as input data in our model. The results obtained can be seen in Table 3, where we can see that the internal structure of Mercury and Venus is reproduced correctly with minimal errors.
However, it is not the same in the case of Mars, where the errors are greater. There are two very different observational data between Mars and Earth. Mars has an average density of 29% lower than Earth while the axial moment of inertia factor is 9% higher. Both data induce the suggestion that the difference in density between the core and the mantle of Mars is much smaller than for the Earth. This might be because during the formation of Mars, which took place farther from the Sun compared to the Earth, lighter materials have been attached to its core, such as S, which can reach up to 16 ± 2% of the mass of the Mars core (Rivoldini et al. 2011). On the other hand, its larger moment of inertia factor suggests a lower differentiation between mantle and core densities in Mars, as compared to the Earth.
To obtain the internal structure of Mars we used the same model, modifying only the parameters making null the difference with the real mean densities at the core and the mantle:
Lowdensity core: K_{i} = 201 GPa, and ρ_{i} = 6.263 g cm^{−3},
Low density mantle: K_{i} = 206 GPa, and ρ_{i} = 3.343 g cm^{−3}.
This modified model of lowdensity exoplanets has been applied to Mars, Io, and the Moon. The obtained results can be seen in Table 4, where it can be verified that the modified model correctly represents the internal structure of these objects. The density, pressure, and gravity obtained for Mars with the modified model as a function of the radius can be seen in Fig. 4. The boundary between what is a lowdensity exoplanet or not is not yet well defined. Mars has a density that is 71% of the Earth and our lowdensity exoplanet model works for Mars. Therefore, this boundary must be between 71 and 99% of the Earth’s density. We used a value of 80% for this boundary, but it must be finetuned based on additional observations.
Fig. 4 Density, pressure, and gravity normalised to their higher values of Mars as a function of the radius obtained with our model. ρ_{max} = 7.28 g cm^{−3}, P_{max} = 40.7 GPa, and g_{max} = 3.7 m s^{−2}. 
3 Internal structure of waterrich rocky planets
Waterrich rocky planets, also called ice planets, are thought to be formed beyond the snowline and they mostly contain water and silicates. Some of these ice planets may migrate into the inner area of the stellar system via interactions with the stellar disk or another planet (Kuchner 2003). If the migration eventually produces an orbit within its stellar HZ, we would have an ocean planet. This does not mean that the entire surface of the planet is covered by water since polar caps could remain covered by ice. The size of the polar ice caps will depend on the effective flux coming from the star. To study the internal structure of the ice planets, we use available objects of this type that are closest to the HZ of Sun, namely, the Galilean’s moons of Jupiter.
3.1 Structure model
In general, a waterrich rocky planet consists of three layers (see Fig. 1). To the structure of a dry rocky planet, we add an ice cap that can also contain an inner ocean. Taking into account the fact that these objects have formed beyond the snowline and are lowdensity objects, we have assumed that the internal structure of these planets is more similar to that of Mars. To this model, we have patched a new layer composed of ice. The EOS representing light elements such as ice cannot ignore the effect of temperature. Therefore, we have implicitly included a wellknown pressuretemperature relation such as the water melting curve (Zeng & Sasselov 2013). In our model, to define the internal structure of ice objects, we used a mantle and core density with a behaviour similar to those of Mars. The water phase diagram is taken from Choukroun & Grasset (2010). This diagram defines the pressures at which ice changes its crystallization system. Regarding the different EOS, for this case we used: for ice Ih, ice III, ice V, and ice VI the EOS defined by Gagnon et al. (1990); for ice VII we applied the EOS proposed by Frank et al. (2004); for ice X we used the EOS obtained by French et al. (2009); for salted water with a 10% wt of MgSiO4 the EOS proposed by Vance et al. (2018). This was done because the Galileo spacecraft has detected the very likely existence of saltwater oceans in Jupiter’s ice moons.
3.2 Discussion
Assuming a waterrich rocky planet with a normalised mass, M_{p}, and a normalised radius, R_{p}, the CMF is still defined by Eq. (3). The MMF is now expressed as follows: (7)
where r_{1} is the normalised radius of the mantle and ρ_{1} its normalised mean density.
The mass fraction of the ice layer, namely, the ice mass fraction (IMF) can be defined as: (8)
where ρ_{2} its normalised mean density of this layer.
Therefore, in this case, these coefficients must verify that CMF + MMF + IMF = 1. After including Eqs. (3), (7), and (8) in this expression, we obtain: (9)
with ρ_{p} as the mean normalised density of the planet. Finally, the axial moment of inertia factor is described as (Schubert et al. 2004): (10)
To solve the internal structure of waterrich rocky planets, we have, in this case, Eqs. (9) and (10) and five unknown variables (r_{0}, r_{1}, ρ_{0}, ρ_{1}, and ρ_{2}). Consequently, additional data are needed. In the case of Jupiter’s ice moons their moment of inertia factor, subsurface conductivity of the planet, and gravitational constants such as C_{22}, as well as the EOS of the core, mantle, and ice layer constituents, help us close the problem.
When analyzing waterrich rocky exoplanets, some of these additional variables, such as the moment of inertia factor, are unknown. In this case, for each mass and radius value, the theoretical models provide infinite solutions for the internal structure (degenerate solution) (Suissa et al. 2018; Zeng & Sasselov 2013). To solve this degeneracy, for this type of exoplanet it is only possible to extrapolate the internal structure of some known ice object from the solar system.
3.3 Ganymede’s internal structure
Ganymede is the biggest satellite in the solar system with a radius of 2632.3 km, greater even than Mercury (Seidelmann et al. 2007). Data from the Galileo spacecraft have provided information about its internal structure. Its moment of inertia factor (0.3115) is the lowest of all known solid objects in the solar system and reveals a complete differentiation of the planet into three layers: the first layer of ice and water, then a rocky mantle, and finally a metal core (Schubert et al. 2004). Its low average density (1.942 g cm^{−3}) suggests an important content in water and ice so a high IMF value is expected. Recent internal structure models of this object suggest a thickness of the ice and water layer around onethird of the planet’s radius, namely, between 800900 km for (Kuskov & Belashchenko 2016) and between 876910 km for (Vance et al. 2018). Galileo spacecraft magnetometer data reveals a relatively strong dipolar magnetic field (0.002 ) that must be generated by the action of a dynamo in a liquid or partially liquid core (Schubert et al. 2004). Calculations have been based on 10 GPa/2000K in the centre of the satellite (Kuskov & Belashchenko 2016), offering a core size between 600 and 800 km and an average density between 6.6 and 7.4 cm^{−3} that would imply a CMF of between 0.04 and 0.10.
A response induced to Jupiter’s magnetic field has also been detected, requiring the existence of a conductive layer compatible with a saltwater ocean (Kivelson et al. 2002). The Galileo spacecraft has also provided a relatively low value for the gravitational constant C_{22} measuring Ganymede’s tidal response, which may mean that tidal warming is negligible (Bland & McKinnon 2015). This may show that the salty ocean would not have to be very close to the surface.
Introducing in our model all the above observational data and iterating until a null mean density difference with the observed value is reached, we obtain a r_{0} = 770 km, a D_{ice} = R_{p} – r_{1} = 901 km, and a D_{ocean} = 130 km. The complete results can be seen in Table 5 and the density profile obtained for Ganymede is presented in Fig. 5.
Results for ice satellites of the Solar System.
Fig. 5 Density, pressure, and gravity normalised to their higher values of Ganymede as a function of the radius obtained with our model. ρ_{max} = 6.6 g cm^{−3}, P_{max} = 10.3 GPa, and g_{max} = 1.8 m s^{−2}. 
3.4 The internal structure of Europa and Callisto
Europa is a much smaller ice object than Ganymede, with a radius of 1562.1 km (Seidelmann et al. 2007), but with a much higher mean density 2.989 g cm^{3} (Schubert et al. 2004), suggesting an ice layer that is not too deep. The observed moment of inertia factor (0.346) requires a concentration of mass in the centre of the object and a differentiation in layers with a metal core of Fe, a mantle of silicates, and an outer ice and water layer (Schubert et al. 2004). The Galileo spacecraft has detected electrical conductivity within the first 200 km deep in Europa, indicating the presence of an ocean of saltwater (Schubert et al. 2004). In addition, it observed a value for the gravitational constant of C_{22}, which is compatible with an ocean of thickness around 130 km, suggesting significant tidal warming that may have turned much of the Ih ice cap into a liquid ocean.
Kuskov & Kronrod (2005) propose a core size for Europa between 470 and 640 km, whereas Kuskov & Belashchenko (2016) estimate a range for the core densities between 6.3 and 7 g cm^{−3}. For a concentration of S in the range of 3.5 and 10% wt in its liquid core, and a pressure of 5 GPa and a temperature of 2000 K at its centre, the CMF ranges between 0.05 and 0.13. In Table 5, we show the results for Europa obtained introducing all this observational data in our model.
Callisto is a satellite similar in size to Ganymede, with a radius of 2409.3 km (Seidelmann et al. 2007), but with a density that is even lower, at 1.8344 g cm^{3} (Schubert et al. 2004), suggesting an important thickness of the ice layer. Since the Galileo spacecraft only performed equatorial flights over Callisto, the moment of inertia factor has been obtained using the (Gao & Stevenson 2013) correction. Its value of 0.32 suggests a mass distribution similar to Ganymede, that is, welldifferentiated layers with a large ice layer, a rocky mantle, and a metallic core. Callisto can have also an inner ocean (Zimmer et al. 2000).
Applying our model together with the previous observational data, the results included in Table 5 have been obtained. Therefore, our model for ice planets produces consistent results with the data observed for these two objects.
Fig. 6 IMF vs. CMF for the three ice moons of Jupiter analysed: Ganymede, Europa, and Callisto. The black line represent the linear regression of these three points, to guide the eye. 
3.5 IMFCMF relation
In the light of the results we obtained for the ice moons of Jupiter: Ganymede, Europa, and Callisto, we found a possible relationship between their IMF and CMF: when the IMF increases, the CMF decreases. This can be seen in Fig. 6. These three observational points lie in a line. We have also plotted the regression line of these three points to guide the eye. Of course, with only three points, it is impossible to assess a physical event, but we can use this property for breaking the degeneracy of our model for these objects. If we impose this condition to the model of waterrich exoplanets, for a given M_{p} and R_{p} we would have a unique solution compatible with the internal structure of these moons.
4 Massradius grid
After extrapolating the three internal structure models described above for Earth, Mars, and Ganymede we constructed a new grid of exoplanets characteristics, which are shown in Table B.1. Thus, by entering the mass and radius of an exoplanet in the grid, we can quickly identify whether it is a dry or waterrich rocky exoplanet, as well as its CMF or its IMF. For lowdensity dry rocky planets, the internal structure model of Mars has only been used when the mean density of the planet is less than 0.8 times the mean density of the Earth.
We assumed that for a given value of a planet mass, it is a dry rocky planet when its radius is less than or equal to the radius corresponding to a composition made up 100% of rock (CMF = 0). If the radius of the planet is greater than this value, its internal structure cannot be explained with only two layers and there must be additional lighter components, such as ice.
The grid has been made for planetary masses from 0.1 up to 48 M_{⊕}. When extrapolating the model for dry rocky planets with masses greater than 32 M_{⊕}, pressures are so intense that the most widely used EOS is the modified TFD, that is, when electron degeneration pressure dominates. Nevertheless, this EOS must be taken with caution since it can introduce elevated errors. Something similar happens for waterrich planets and masses larger than 48 M_{⊕}, where the electron degeneration pressure dominates, especially for IMF < 0.5. When applying our model, we must take into account that all the reference objects have masses lower than Earth. That means that for exoplanets with masses larger than 1 M_{⊕}, it can be extrapolated to reflect the Earth’s internal structure somehow. When the mass increases, the thermal conductivity and energy flow are the most impactful factors. In this case, we use the most updated models for describing them as a function of the mass. We think this is the best approximation available currently, although we recognise that the extrapolation of PREM models to objects more massive than the Earth induces significant uncertainty.
5 Magnetic properties of exoplanets
The main goal of our study is to estimate the magnetic properties of exoplanets using the most common known characteristics such as exoplanetary mass, radius, and orbital period. In this section, we describe how we obtain these estimations assuming we have a model of its internal structure as shown in the previous sections.
5.1 Magnetic moment
Most planetary dynamo is thought to be maintained by thermal and compositional convection mechanisms in electrically conductive fluids inside planets (OC06). The scaling laws of OC06 make it possible to determine the regime (dipolar or multipolar) and the magnetic moment of a planetary dynamo once the Rayleigh number is known. From this value, applying these laws, along with the Rossby number, the Reynolds magnetic number, and the dipole field Lorentz number, it is possible to determine the magnetic behaviour of the planet.
The Rayleigh number (Ra_{Q}) can be defined as: (11)
where r* is the ratio between the core radii (r* = r_{0}/r_{i}), D is the core convective zone thickness (D = r_{0} − r_{i}), Ω the planet’s rotational frequency, and F the mean buoyancy convective flux that can be obtained following: (12)
with α, g, ρ, and C_{p} as the thermal expansion coefficient, gravity, density, and the specific heat capacity at constant pressure at the planet core, respectively, whereas q_{conv} is the convective heat flux generated by the core (OC06 and Driscoll & Olson 2011).
Another fundamental parameter to define the magnetic regime of the planet is the Rossby number: (13)
with u as the speed of the fluid that generates the planetary dynamo. Similarly, the local Rossby number is defined based on the order of the spherical harmonics when spherical symmetry is assumed for the planet, that is: (14)
where ℓ_{u} is the spherical harmonic degree ℓ of the velocity vector u. Two completely differentiated regimes (dipolar and multipolar) have been found in the action of planetary dynamos. On the one hand, in the dipolar regime, the planet’s magnetic field is strong and is dominated by the dipolar component. It corresponds to low values of the local Rossby number. On other hand, the multipolar regime corresponds to high values of the local Rossby number. In this case, the magnetic field is dominated by multipoles and its value decreases drastically.
In the case of baseheated dynamos, as is the case on Earth, the transition from the dipolar regime to the multipolar regime occurs at a very narrow interval around a value of the local Rossby number of 0.12 (OC06). Values larger than 0.12 indicate a multipolar regime whereas lower values involve a dipolar regime. When the value of the local Rossby number is in a range close to and below 0.12, the planet is in an area with a dipole magnetic field with reversible polarity.
Using the scaling laws described at OC06, the local Rossby number can be estimated using the following equation: (15)
where ν is the kinematic viscosity and λ_{m} and λ_{t} are respectively the diffusivities magnetic and thermal of the fluid. Therefore, depending on the value of Ro_{ℓ} with respect to the critical value of 0.12, we can estimate the magnetic regime of the exoplanet. Thus, this value depends mainly on the Rayleigh number, Ω, and D, and weakly on the core thermodynamic properties.
The scaling laws of OC06 also allow us to obtain the global Rossby number that for dynamo heated by the base can be calculated by the following equation: (16)
with β ≈ 0.85 (OC06). In this way, by applying Eq. (13) the velocity of the fluid generated by the dynamo can be determined. The third parameter that defines a planetary dynamo is the magnetic Reynolds number, which is determined as: (17)
For a planet to have a dynamo, it is necessary to have a layer of electric conductor fluid, and a Reynolds magnetic number (R_{m}) larger than 40 (Gaidos et al. 2010). Below that critical value, the magnetic moment is null. In this study, a prior check of the magnetic Reynolds number will always be carried out to ensure that the action of the dynamo has begun.
The fourth parameter that defines planetary dynamo is the dipole field Lorentz number: (18)
where μ_{0} is the magnetic vacuum permeability and M the magnetic moment. The scaling laws of OC06 make it easy to determine the Lorentz number from the Rayleigh number, using the following relation: (19)
where γ_{d} is the dipolar saturation constant that, for fast rotators dynamos it is assumed to have a value of 0.2 (Driscoll & Olson 2011). Equations (18) and (19) allows us to obtain an estimation of the magnetic moment as: (20)
If we analyse how the dipole moment varies with the Rayleigh number (see Fig. 4 of OC06), it can be observed that there are four different zones. In the first zone, for low values of RaQ, the magnetic moment is null due either to the lack of convection or because the action of the dynamo has not begun. This zone corresponds to Reynolds magnetic number values less than 40. Once the critical value of the Reynolds number is exceeded, the dipole magnetic moment dominates. After an initial and rapid rise, a zone occurs with a linear increment of the magnetic moment relative to the Rayleigh number. In this zone, the magnetic moment can be determined by Eq. (20). It is important to note that, in this zone, it does not present an explicit dependence on the angular velocity of the planet. If we continue increasing the Rayleigh number, the magnetic moment begins to be of reversible polarity, in a relatively narrow area and before reaching the critical local Rossby number of 0.12. Here is where a maximum value of the magnetic moment () is produced, and it can be calculated imposing the condition Ro_{ℓ} = 0.12, resulting: (21)
At the fourth and last zone, with values of the Rayleigh number above the critical value of 0.12, the magnetic moment suffers a fast decrease changing from dipolar to multipolar. In the cases studied by OC06, this reduction of the magnetic moment is very important, as it is on the order of 0.05 times the maximum value of the magnetic moment. Some other authors work with a dipole moment reduction coefficient of 0.15 (Grießmeier et al. 2009). In this work, it has been verified that the reducing coefficient in the solar system is about 0.06 that comes to ratify the value determined by OC06. Therefore, the magnetic moment in this zone can be determined in relation to the maximum dipole moment as: (22)
5.2 Application in the case of exoplanets
If we want to extrapolate this model to rocky exoplanets, several previous considerations must be made. First of all, we know that for masses greater than 2 M_{⊕} the core remains completely liquid, at least, until the shutdown of its dynamo (Zuluaga et al. 2013; Driscoll & Olson 2011). In this case, the thickness of the convective zone shall be considered to be equal to the radius of the core (D = r_{0}).
One of the main ingredients of these equations is the exoplanet angular velocity. Unfortunately, this variable cannot be observed yet, and we need other considerations for estimating its value. More common observational data are the orbital period and eccentricity and the hosting star mass. With these values we can estimate whether the planet is tidally coupled to the star (Grießmeier et al. 2009), using it for estimating this angular velocity as follows: (1) If the planet is tidally coupled, we can estimate the most probable spinorbit resonance following Dobrovolskis (2007) and then its angular velocity. (2) If the planet is not tidally coupled, we assume free rotation leading to a dipolar magnetic moment, as for all the objects of the solar system with this characteristic. In this case, we use Eq. (20) for estimating .
Other important ingredients for estimating for exoplanet are the thermal and magnetic diffusivities at the exoplanetary core, λ_{t} and λ_{m}, respectively, and their evolution with the pressure. For our model, we initially obtained the values for the thermal and electric conductivities (к and σ, respectively) in the case of the Earth (see Table 6) and then we estimated their variation with pressure using Pozzo et al. (2012). A more detailed description of this process can be found in the appendix. Finally, we obtain the thermal and magnetic diffusivities as:
A key factor for defining the exoplanets thermal model is the core thermal conductivity. There are different values for this conductivity in the literature. For example, Gaidos et al. (2010) propose a core thermal conductivity of 35 W/m/K, Zuluaga et al. (2013) a value of 40 W/m/K, Labrosse (2003) a value in the range 5060 W/m/K, and Pozzo et al. (2012) a value of 100 W/m/K. We used our model, with the details explained in the appendix, to the Earth, Venus, Mercury, Mars, and Ganymede and we have found that the value for the core thermal conductivity better fitting the observed magnetic moment and local Rossby number is 60 W/m/K, confirming the estimations of Labrosse (2003). With this value, the characteristics of the core and the magnetic moment can be calculated for these five objects. These values are summarised in Table B.2. In this table, we can see how our model describes properly the observed values.
Thermodynamic parameters of the Earth.
5.3 Magnetic field
With the magnetic moment, it is possible to estimate the intensity of the dipolar magnetic field B_{0dip} at r_{0}. It follows the relation: (25)
and this value can be extrapolated to the planet surface (B_{sdip}) using (Gaidos et al. 2010; Driscoll & Olson 2011): (26)
6 Application to the first set of exoplanets discovered by TESS
To test how our model works on real data, we applied our method in order to calculate the composition and magnetic moment of dry and waterrich rocky planets found at the first 176 planets confirmed by the Transiting Exoplanet Survey Satellite space mission (TESS). For doing that we used the exoplanet’s data available at TESS database on January 2022^{1}. In general, this study will considers four types of exoplanets: dry rocky, waterrich rocky, ice giants, and gas giants.
Dry rocky exoplanets are exoplanets that, for a given mass, have a radius equal to or less than the radius producing a CMF = 0 (see Table B.1). They are mainly iron and silicate worlds where the presence of water is residual, as in the case of Earth.
Waterrich rocky exoplanets are those exoplanets that, for a given mass, have a radius greater than the radius producing a CMF = 0 and equal to or lower to the radius corresponding to an IMF = 1. That is to say that from the radius corresponding to CMF = 0, the decrease in density cannot be justified with an increase in the presence of silicates and a lighter element such as water is necessary. If an exoplanet of this type is in the HZ, we call it an ‘ocean planet’.
Ice giants. They are worlds of ice and silicates in the core, and a gas envelope in the outer zone made mainly of hydrogen and helium, where the planetary core predominates. They are those planets that, for a given mass, have a radius greater than that, making IMF = 1 and lower to or equal to the radius corresponding to a mixture of 50% of HHe. That is to say, from the radius corresponding to IMF = 1, the decrease in density cannot be justified with an increase in the presence of water and, thus, lighter elements such as hydrogen and helium are necessary.
Gas giants are worlds of ice and silicates in the nucleus, and a gas envelope in the outer area of hydrogen and helium, where the core’s envelope predominates. They are planets that, for a given mass, have a radius greater than the corresponding to 50% of HHe.
From a statistical point of view, dry rocky planets do not usually have a radius greater than 2 R_{⊕}, while waterrich rocky planets are rare beyond 2.8 R_{⊕}. Ice giants range from 2.3 to 7 R_{⊕}, while Gas giants typically have more than 7 R_{⊕}.
The giant planets have not been analysed here as they are not the target of this study. For the rest of the planets, we apply the following procedure. We assumed a Gaussian distribution for the observational uncertainties and we generated a set of 30 000 sampling values of the planet mass, radius, and rotational period following the observed values. For these 30000 sampling points, we evaluated the probability for this planet to be included among the different types. When we did not know the exoplanet mass, it was estimated following (Chen & Kipping 2017). In the TESS database, some planets are shown with a mass without uncertainties. If when using this mass as input in our massradius diagram the planet appears above the composition of 100% of Fe, we assume that this mass has no physical sense and we follow the procedure of the absence of known planetary mass. To distinguish whether the exoplanet is tidally locked, we used the equations of Grießmeier et al. (2009). For tidally locked exoplanets, from the orbital eccentricity, we estimated the spinorbit most likely relation following (Dobrovolskis 2007). To determine the mean effective flux of energy that a planet receives from its star, the eccentricity of the orbit has been taken into account (Kopparapu et al. 2013). The HZ of each star was determined following (Kopparapu et al. 2013). The displacement of the inner edge of the HZ for synchronised rotating planets around lowmass stars was also taken into account according to Kopparapu et al. (2016), as well as the effect of the planet mass on the HZ (Kopparapu et al. 2014). The boundaries of the HZ (D_{2} for the inner boundary and D_{3} for the outer boundary) were obtained as the mean values of the 30 000 samples. Finally, we assumed that all planetary dynamos are active since the TESS database does not include the ages of stars.
The results we obtained are summarised in Table B.3 for dry rocky planets and Table B.4 for waterrich planets. In these tables, we can see the situation of the planets with respect to the HZ (D_{2} and D_{3}), the probability of it being this specific type of planet (Prob.), its composition (core mass fraction, mantle mass fraction, and ice mass fraction), and the magnetic properties (local Rossby number, regime, and normalised magnetic moment).
For dry rocky planets, it is remarkable to note that all the confirmed planets are found to be tidally locked since the orbital periods are very small and their spinorbit resonance is 1:1, except for the case of LHS 1678 b and TOI2285 b, which have a spinorbit resonance of 3:2. All these planets, except TOI700d, are in the hot zone of their star receiving a flow of energy making it impossible for water to be in the liquid phase. Approximately onehalf of these planets have an Earthlike composition (CMF = 0.325 ± 20%). Regarding the magnetic moment, half of these planets may have a powerful dipole magnetic moment, but they are in orbits so close to their star that they can hardly protect the planet from possible violent events from their star. This result, exemplified mainly by Mercurylike planets, may be an observational bias because the first discovered TESS exoplanets (i.e. those we analyse in this work) present short orbital periods.
The most interesting dry rocky planet so far, according to our analysis, is TOI700d, which is the only one of this class that is included on the list at the HZ and which may contain liquid water on its surface. However, it has a slow rotation (37.42 days) and its magnetic moment is weak (0.01 M_{⊕}), albeit ten times greater than that of Mercury. Therefore, it is very exposed to the action of erosion from stellar winds. If it has been able to maintain its atmosphere  taking into account the fact that it rotates in synchronous rotation with its star and the flow of energy is not much less than that received by the Earth from the Sun (0.87 S_{eff⊕})  at the equator of the day face of the planet there could be an ocean of liquid water, although the polar ice caps could be larger than the terrestrial ones.
When looking at the waterrich rocky planets (Table B.4), the only notable remark is that they are all tidally locked and in the hot zone of their star, except TOI2257 b. According to our model, this is an ocean planet located in the HZ of its star with a small core that could generate a magnetic field four times larger than that of Ganymede. Due to the absence of an observed mass for this planet, we have estimated it from models, following the procedure described above.
7 Conclusions
In this work, we determine an internal structure model for rocky planets. We propose three reference models: Earth’s internal structure defined by PREM to be used for mediumhigh density dry rocky exoplanets; Mars assuming an Earthlike mantle composition for lowdensity dry rocky exoplanets; and Ganymede for waterrich rocky exoplanets. The main idea of our work is to extrapolate, in each case, the internal structure of one of the reference models to estimations of the internal characteristics of both dry and waterrich rocky exoplanets as well as similar objects in the solar system, with the latter applied in testing the performance of our model.
The internal structure model we propose has some differences with previous proposals in the literature, which can be summarised as:
The solid part of the core is not discarded. In the case of Earth, it means an error in mass larger than a 2%.
We take into account the possible existence of inner liquid oceans in waterrich exoplanets. We have also included the option of a presence of saltwater.
To calculate the internal structure of waterrich planets, it is imperative to use the moment of inertia factor. It allows for the accurate determination of the beginning and depth of these liquid oceans, and, together with the imposed null error for the total mass and the corresponding EOS, allows for the determination of the thicknesses of the ice, mantle, and core layers.
We also modeled the key thermodynamic variables as a function of the internal pressure.
With this internal structure model, a new massradio diagram has been constructed based on extrapolating the three reference models.
The magnetic moment is a fundamental factor protecting the atmosphere of an exoplanet, and therefore its potential life on its surface, based on the erosion of stellar winds and cosmic rays (RodríguezMozos & Moya 2019). To determine the magnetic moment of an exoplanet and whether it is dipolar or multipolar, we used the scaling laws of planetary dynamos of Olson & Christensen (2006). For extrapolating these scaling laws to exoplanets more massive than Earth that are both dry and waterrich, different approaches have been used to obtain the variation with the pressure of the thermodynamic parameters involved in these planetary dynamos.
Finally, the proposed procedure has been applied to the first 176 exoplanets confirmed by TESS. To our knowledge, this is the first time that a massive estimation of the magnetic properties of exoplanets has been undertaken. We present the situation of these exoplanets in the HZ of their hosting stars. For all those rocky planets in the list, we obtained their composition and magnetic properties based on the assumption that that this dynamo is still active. We find that the most interesting objects, from an astrobiological point of view, are TOI700 d and TOI2257 b.
Acknowledgements
The authors want to thank the referee, Peter Olson, and the editor for their very constructive comments that have certainly improved this manuscript. A.M. acknowledges funding support from Grant PID2019107061GBC65 funded by MCIN/AEI/10.13039/501100011033, and from Generalitat Valenciana in the frame of the GenT Project CIDEGENT/2020/036.
Appendix A Thermal model
A key element in determining a planet’s magnetic moment is the buoyancy convective flux that is related to the heat flow generated by the core. To estimate both variables it is necessary to have a thermal model. The model we have constructed is described below.
In this study, we follow the thermal models made for the Earth by of (Labrosse 2003), (Gaidos et al. 2010), and (Zuluaga et al. 2013). Afterwards, we extrapolate the results to rocky exoplanets that, in general, are more massive and have higher interior temperatures and pressures. For example, the pressure at the CMB of the Earth reaches up to 135 GPa, but in rocky exoplanets, this pressure can reach up to the level of TPa. This has a large impact on the interior heat transport models, and thermal properties such as thermal expansivity, specific heat, or viscosity must be modeled at extreme pressure conditions (Stamenkovic et al. 2011).
In doing so, we start by estimating the temperature gradient of the exoplanets. With this gradient, we can describe the heat extracted from the core.
A.1 Temperature gradient
Assuming a steadystate for the exoplanet, if we know the adiabatic gradient of temperatures, we can estimate the temperature at any position at the mantle. This can be done using (Labrosse 2003): (A.1)
where T_{m} is the temperature in the outermost part of the Upper Mantle and D_{m} is the temperature high scale of the mantle that can be calculated as (Labrosse 2003): (A.2)
with γ as the Gruneisen parameter and G the gravitational constant. In this equation, C_{p}, α, and ρ are those at the bottom of the mantle, at the boundary with the CMB. Using these two equations, the temperature at this bottom limit of the mantle (T_{ℓ}) can be estimated.
For calculating the temperature at the beginning of the core (T_{c}) we can assume that the temperature gradient in this zone (ΔT_{CMB}) is proportional to the temperature increment produced at the mantle (Zuluaga et al. 2013), that is: (A.3)
where ϵ_{ad} is the adiabatic factor of the CMB. Zuluaga et al. (2013) estimated that the value for this adiabatic factor better reproducing the Earth is ϵ_{ad} = 0.7. Therefore, we have: (A.4)
In the core we can also assume an adiabatic gradient of temperatures: (A.5)
where D_{c} is the temperature high scale of the core that can be calculated as (Labrosse 2003): (A.6)
The only difference betwen this equation and Equation A.2 is the absence of the Gruneisen parameter. Finally, the temperature at the planet centre (Tcc) is estimated using Equation A.5 at r = 0.
To fix the temperature profile of the planet, it is necessary to know the average temperature of the mantle, T_{mm}, which can be calculated using the following equation (Gaidos et al. 2010): (A.7)
with θ the potential temperature of the mantle, which we take as equal to 1700 K (Zuluaga et al. 2013).
Therefore, for estimating the temperature profile of an exoplanet, in general more massive than Earth, we need to know how C_{p}, α, γ, and ρ change with pressure. The density profile is provided by our internal structure model, and the other three variables are taken from (Stamenkovic et al. 2011).
In waterrich exoplanets, the temperature gradient can be known from the water melt curve of the different crystallization systems via the EOS described in Section 3.1. With this information, we can estimate the pressure and temperature at the boundary ice layermantle and use the equations here described to obtain the temperature for the rest of the exoplanet.
A.2 Heat extracted from the core
The CMB is a relatively narrow zone. (Driscoll & Olson 2011) estimated that it can have a thickness up to 286 km with a temperature gradient of 5.5 K/km. On the other hand, (Okuda et al. 2020) estimated a thickness of 200 km and a temperature gradient of 7 K/km. The planetary dynamo activity is related to the heat transport and the temperature gradient at CMB (Gaidos et al. 2010). Heat transport in the Earth’s interior occurs predominantly by convection. However, heat transport in the CMB occurs only by conduction (Okuda et al. 2020).
The total heat released by the core (Q_{c}) can be obtained using the approximation shown in (Ricard et al. 2009): (A.8)
where κ_{m} is the thermal conductivity of the lower mantle and Nu_{c} is the Nusselt number at the core and it is defined as (A.9)
with Ra_{*} as the critical Rayleigh number and Ra_{c} as this number at the CMB. For our model, we adopted the values proposed by (Gaidos et al. 2010), that is, Ra_{*} = 1100 and δ = 0.3. Ra_{c} can be calculated assuming a CMB that is heated from below and using the equation (Ricard et al. 2009): (A.10)
where η_{c} is the dynamic viscosity at the CMB.
Manga (2001) showed that the temperature gradients at the CMB are produced at two narrow zones of this layers close to the core and mantle boundaries respectively. Throughout the rest of the CMB, the temperature remains almost constant. This constant value (TCMB) can be estimated as a value between the upper core temperature and the bottom mantle temperature, that is: (A.11)
where θ_{c} is inversely proportional to the ratio between the lower mantle and core viscosities, that is, its value must be lower than 0.5 (Manga 2001). For our model, we used the value proposed by (Zuluaga et al. 2013) for Earth of θ_{c} = 0.4.
Another variable we must estimate is the dynamical viscosity at the CMB (η_{c}). The dynamical viscosity of a mineral at large pressures and temperatures can be obtained using the NavarroHerring model (Yamazaki & Karato 2002) with the following expression: (A.12)
with R_{g} as the ideal gas constant in mols, d the grain size, m the grain growth rate, D_{0} the preexponential diffusion coefficient, A the viscosity preexponential coefficient, m_{mol} the molar weight, ξ the homologous constant, and T_{melt} the melting temperature of the constituent. For our model, we used the values displayed in Table 1 of (Stamenkovic et al. 2011) (see Table 6). For T_{melt} a good approximation is using the following fifthorder polynomial: (A.13)
With the following coefficients: (a_{0}, a_{1}, a_{2}, a_{3}, a_{4}, a_{5}) = (2752.41, 22.817, 0.013104, 8.8756·10^{−6}, −3.02732·10^{−9}, 3.9362 10^{−13}), (Stamenkovic et al. 2011) found an inaccuracy in this approximation that is lower than a 1.5% above 25 GPa.
The last ingredient to determine the heat released by the core is the thermal conductivity of the lower mantle (κ_{m}) which is one of the most important properties to understand the thermal dynamics in the CMB. Recent observations of thermal conductivity of Fe_{x} Mg_{1−x} O show an important reduction of its value due to the presence of Fe impurities (Ohta et al. 2017). As we noted earlier in this work, pv transform into ppv at a pressure of 125 GPa and a temperature of 2500 K. These reduction impacts mainly on ppv and not on pv (Okuda et al. 2020). To determine the variation of thermal conductivity with the pressure at ambient temperature (300 K), the measures for pv have been used (Ohta et al. 2017), while for pressures larger than 125 Gpa we used a mix of ppv with a 3% of Fe (Okuda et al. 2020) and impurities of Fex Mg_{1−x} O.
This thermal conductivity at ambient temperature, which we will call κ_{m}0, can be extrapolated to the pressure and temperatures conditions at the CMB, using the densitytemperature model described by (Okuda et al. 2020): (A.14)
In this expression, T_{0} = 300 K, ρ_{0} = 5470 kg/m^{3}, and the exponents are presented in Okuda et al. (2020), with values e_{1} = 6 ± 0.3 and e_{2} = 0.65 ± 0.04. The results for κ_{m} at the pressure and temperature conditions of the CMB we obtain are very similar to those presented by (Gaidos et al. 2010) and (Zuluaga et al. 2013) of κ_{m} = 6 W/m/K. These results have been recently confirmed by thermal conductivity measurements of ppv+Fe_{x} Mg_{1−x} O at 124 GPa and temperatures between 2000 and 3000 K, with a value of 5.9 W/m/K (Geballe et al. 2020).
In the case of waterrich rocky planets, for the same mass and similar core size, Q_{c} is lower thanks to lower pressure and temperature conditions at the CMB compared with the case of a dry rocky planet.
Appendix B Long tables
Grid massradius for rocky exoplanets.
Core characteristics and magnetic properties of planets and satellites of the Solar System.
Results for dry rocky planets observed by TESS after 30,000 runs (Monte Carlo method).
Results for waterrich rocky planets observed by TESS after 30,000 runs (Monte Carlo method).
References
 Birch, F. 1952, J. Geophys. Res., 57, 227 [NASA ADS] [CrossRef] [Google Scholar]
 Bland, M. T., & McKinnon, W. B. 2015, Lunar and Planetary Science Conference [Google Scholar]
 Choukroun, M., & Grasset, O. 2010, J. Chem. Phys., 133, 144502 [NASA ADS] [CrossRef] [Google Scholar]
 Chen, J., & Kipping, D. 2017, ApJ, 834, 17 [Google Scholar]
 Dobrovolskis, A. R. 2007, Icarus, 192, 1 [NASA ADS] [CrossRef] [Google Scholar]
 Driscoll, P., & Olson, P. 2011, Icarus, 213, 12 [NASA ADS] [CrossRef] [Google Scholar]
 Dumoulin, C., Tobie, G., Verhoeven, O., et al. 2017, AGU Fall Meeting Abstracts, #P13A2552 [Google Scholar]
 Dziewonski, A. M., & Anderson, D. L. 1981, Phys. Earth Planet. Inter., 25, 297 [CrossRef] [Google Scholar]
 Fischer, R. A., Campbell, A. J., Caracas, R., et al. 2012, Earth Planet. Sci. Lett., 357, 268 [CrossRef] [Google Scholar]
 Frank, M. R., Fei, Y., & Hu, J. 2004, Geochim. Cosmochim. Acta, 68, 2781 [NASA ADS] [CrossRef] [Google Scholar]
 French, M., Mattsson, T. R., Nettelmann, N., et al. 2009, Phys. Rev. B, 79, 054107 [NASA ADS] [CrossRef] [Google Scholar]
 Gagnon, R. E., Kiefte, H., Clouter, M. J., et al. 1990, J. Chem. Phys., 92, 1909 [NASA ADS] [CrossRef] [Google Scholar]
 Gaidos, E., Conrad, C. P., Manga, M., et al. 2010, ApJ, 718, 596 [NASA ADS] [CrossRef] [Google Scholar]
 Gallet, F., Charbonnel, C., Amard, L., et al. 2017, A&A, 597, A14 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
 Gao, P., & Stevenson, D. J. 2013, Icarus, 226, 1185 [NASA ADS] [CrossRef] [Google Scholar]
 Geballe, Z. M., Sime, N., Badro, J., et al. 2020, Earth Planet. Sci. Lett., 536, 116161 [CrossRef] [Google Scholar]
 Grießmeier, J.M., Stadelmann, A., Grenfell, J. L., et al. 2009, Icarus, 199, 526 [CrossRef] [Google Scholar]
 Jura, M., & Young, E. D. 2014, Ann. Rev. Earth Planet. Sci., 42, 45 [CrossRef] [Google Scholar]
 Khurana, K. K., Kivelson, M. G., Russell, C. T., et al. 1997, Nature, 387, 262 [NASA ADS] [CrossRef] [Google Scholar]
 Kivelson, M. G., Khurana, K. K., & Volwerk, M. 2002, Icarus, 157, 507 [CrossRef] [Google Scholar]
 Konopliv, A. S., Asmar, S. W., Folkner, W. M., et al. 2011, Icarus, 211, 401 [NASA ADS] [CrossRef] [Google Scholar]
 Kronrod, V. A., & Kuskov, O. L. 2011, Izvestiya Phys. Solid Earth, 47, 711 [CrossRef] [Google Scholar]
 Kopparapu, R. K., Ramirez, R., Kasting, J. F., et al. 2013, ApJ, 765, 131 [NASA ADS] [CrossRef] [Google Scholar]
 Kopparapu, R. K., Ramirez, R. M., SchottelKotte, J., et al. 2014, ApJ, 787, L29 [Google Scholar]
 Kopparapu, R. Kumar, Wolf, E.T., HaqqMisra, J., et al. 2016, ApJ, 819, 84 [Google Scholar]
 Kuchner, M. J. 2003, ApJ, 596, L105 [Google Scholar]
 Kuskov, O. L., & Belashchenko, D. K. 2016, Sol. Syst. Res., 50, 165 [NASA ADS] [CrossRef] [Google Scholar]
 Kuskov, O. L., & Kronrod, V. A. 2001, Icarus, 151, 204 [NASA ADS] [CrossRef] [Google Scholar]
 Kuskov, O. L., & Kronrod, V. A. 2005, Icarus, 177, 550 [NASA ADS] [CrossRef] [Google Scholar]
 Labrosse, S. 2003, Phys. Earth Planet. Inter., 140, 127 [NASA ADS] [CrossRef] [Google Scholar]
 Manga, M. 2001, Geophys. Res. Lett., 28, 2133 [NASA ADS] [CrossRef] [Google Scholar]
 Okuda, Y., Ohta, K., Hasegawa, A., et al. 2020, Earth Planet. Sci. Lett., 547, 116466 [CrossRef] [Google Scholar]
 Olson, P., & Christensen, U. R. 2006, Earth Planet. Sci. Lett., 250, 561 [CrossRef] [Google Scholar]
 Ohta, K., Yagi, T., Hirose, K., et al. 2017, Earth Planet. Sci. Lett., 465, 29 [CrossRef] [Google Scholar]
 Pozzo, M., Davies, C., Gubbins, D., Alfè, D. 2012, Nature, 485, 355 [NASA ADS] [CrossRef] [Google Scholar]
 Ricard, Y., Srámek, O., & Dubuffet, F. 2009, Earth Planet. Sci. Lett., 284, 144 [CrossRef] [Google Scholar]
 Ricker, G. R., Winn, J. N., Vanderspek, R., et al. 2014, Proc. SPIE, 9143, 914320 [Google Scholar]
 Rivoldini, A., & Van Hoolst, T. 2013, Earth Planet. Sci. Lett., 377, 62 [CrossRef] [Google Scholar]
 Rivoldini, A., Van Hoolst, T., Verhoeven, O., et al. 2011, Icarus, 213, 451 [NASA ADS] [CrossRef] [Google Scholar]
 RodríguezMozos, J. M., & Moya, A. 2017, MNRAS, 471, 4628 [CrossRef] [Google Scholar]
 RodríguezMozos, J. M., & Moya, A. 2019, A&A, 630, A52 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
 Salpeter, E. E., & Zapolsky, H. S. 1967, Phys. Rev., 158, 876 [NASA ADS] [CrossRef] [Google Scholar]
 Schilling, N., Khurana, K. K., & Kivelson, M. 2003, EGS  AGU  EUG Joint Assembly conference, 9285 [Google Scholar]
 Schubert, G., Anderson, J. D., Spohn, T., et al. 2004, Jupiter. The Planet, Satellites and Magnetosphere (Cambridge: Cambridge University Press), 281 [Google Scholar]
 Seidelmann, P. K., Archinal, B. A., A’Hearn, M.F., et al. 2007, Celest. Mech. Dyn. Astron., 98, 155 [NASA ADS] [CrossRef] [Google Scholar]
 Selsis, F., Kaltenegger, L., & Paillet, J. 2008, Phys. Scr. T, 130, 014032 [NASA ADS] [CrossRef] [Google Scholar]
 Smith, D. E., Zuber, M. T., Phillips, R. J., et al. 2012, Science, 336, 214 [NASA ADS] [CrossRef] [Google Scholar]
 Sotin, C., Grasset, O., & Mocquet, A. 2007, Icarus, 191, 337 [Google Scholar]
 Stamenković, V., Breuer, D., & Spohn, T. 2011, Icarus, 216, 572 [Google Scholar]
 Suissa, G., Chen, J., & Kipping, D. 2018, MNRAS, 476, 2613 [Google Scholar]
 Tilley, M. A., Segura, A., Meadows, V. S., et al. 2017, Astrobiology, V19, 1 [Google Scholar]
 Valencia, D., O’Connell, R.J., & Sasselov, D. 2006, Icarus, 181, 545 [NASA ADS] [CrossRef] [Google Scholar]
 Vance, S. D., Panning, M. P., Stähler, S., et al. 2018, J. Geophys. Res. Planets, 123, 180 [NASA ADS] [CrossRef] [Google Scholar]
 Williams, J. G., Konopliv, A. S., Boggs, D. H., et al. 2014, J. Geophys. Res. Planets, 119, 1546 [NASA ADS] [CrossRef] [Google Scholar]
 Yamazaki, D., and Karato, S. 2002, Phys. Earth Planet. Inter., 131, 251 [CrossRef] [Google Scholar]
 Zimmer, C., Khurana, K. K., & Kivelson, M. G. 2000, Icarus, 147, 329 [NASA ADS] [CrossRef] [Google Scholar]
 Zeng, L., & Seager, S. 2008, PASP, 120, 983 [CrossRef] [Google Scholar]
 Zeng, L., & Sasselov, D. 2013, PASP, 125, 227 [Google Scholar]
 Zeng, L., Sasselov, D. D., & Jacobsen, S. B. 2016, ApJ, 819, 127 [Google Scholar]
 Zeng, L., Jacobsen, S. B., Sasselov, D. D., et al. 2019, Proc. Natl. Acad. Sci., 116, 9723 [Google Scholar]
 Zuluaga, J. I., & Bustamante, S. 2018, Planet. Space Sci., 152, 55 [Google Scholar]
 Zuluaga, J. I., Bustamante, S., Cuartas, P. A., et al. 2013, ApJ, 770, 23 [NASA ADS] [CrossRef] [Google Scholar]
All Tables
Comparison between PREM and our simplified model for the Earth, treated as an exoplanet.
Core characteristics and magnetic properties of planets and satellites of the Solar System.
Results for dry rocky planets observed by TESS after 30,000 runs (Monte Carlo method).
Results for waterrich rocky planets observed by TESS after 30,000 runs (Monte Carlo method).
All Figures
Fig. 1 Section of a rocky planet. R_{p} is the Planet radius, r_{0} the core radius, r_{1} the Mantle radius, D the Outer core thickness, and r_{i} the Inner core radius. 

In the text 
Fig. 2 Density, gravity, and pressure profiles normalised to their higher values for Earth according to PREM.ρ_{max} = 13.1 g cm^{−3}, P_{max} = 364 GPa, and g_{max} = 10.7 ms^{−2}. 

In the text 
Fig. 3 Density, gravity, and pressure profiles normalised to their higher values for the Earth according our simplified model for exoplanets. Here, ρ_{max} = 12.5 g cm^{−3}, Р_{mах} = 361 GPa, and g_{max} = 10.7 m s^{−2}. 

In the text 
Fig. 4 Density, pressure, and gravity normalised to their higher values of Mars as a function of the radius obtained with our model. ρ_{max} = 7.28 g cm^{−3}, P_{max} = 40.7 GPa, and g_{max} = 3.7 m s^{−2}. 

In the text 
Fig. 5 Density, pressure, and gravity normalised to their higher values of Ganymede as a function of the radius obtained with our model. ρ_{max} = 6.6 g cm^{−3}, P_{max} = 10.3 GPa, and g_{max} = 1.8 m s^{−2}. 

In the text 
Fig. 6 IMF vs. CMF for the three ice moons of Jupiter analysed: Ganymede, Europa, and Callisto. The black line represent the linear regression of these three points, to guide the eye. 

In the text 
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