Issue 
A&A
Volume 577, May 2015



Article Number  A60  
Number of page(s)  6  
Section  Stellar structure and evolution  
DOI  https://doi.org/10.1051/00046361/201525812  
Published online  05 May 2015 
Stellar models with mixing length and T(τ) relations calibrated on 3D convection simulations
^{1}
Astrophysics Research Institute, Liverpool John Moores
University,
IC2, Liverpool Science Park, 146 Brownlow
Hill,
Liverpool
L3 5RF,
UK
email:
M.Salaris@ljmu.ac.uk
^{2}
INAF−Osservatorio Astronomico di Collurania, via M.
Maggini, 64100
Teramo,
Italy
email:
cassisi@oateramo.inaf.it
Received: 5 February 2015
Accepted: 13 March 2015
The calculation of the thermal stratification in the superadiabatic layers of stellar models with convective envelopes is a longstanding problem of stellar astrophysics, and has a major impact on predicted observational properties such as radius and effective temperature. The mixing length theory, almost universally used to model the superadiabatic convective layers, contains one free parameter to be calibrated (α_{ml}) whose value controls the resulting effective temperature. Here we present the first selfconsistent stellar evolution models calculated by employing the atmospheric temperature stratification, Rosseland opacities, and calibrated variable α_{ml} (dependent on effective temperature and surface gravity) from a recently published large suite of threedimensional radiation hydrodynamics simulations of stellar convective envelopes and atmospheres for solar stellar composition. From our calculations (with the same composition of the radiation hydrodynamics simulations), we find that the effective temperatures of models with the hydrocalibrated variable α_{ml} (that ranges between ~1.6 and ~2.0 in the parameter space covered by the simulations) present only minor differences, by at most ~30–50 K, compared to models calculated at constant solar α_{ml} (equal to 1.76, as obtained from the same simulations). The depth of the convective regions is essentially the same in both cases. We also analyzed the role played by the hydrocalibrated T(τ) relationships in determining the evolution of the model effective temperatures, when compared to alternative T(τ) relationships often used in stellar model computations. The choice of the T(τ) can have a larger impact than the use of a variable α_{ml} compared to a constant solar value. We found that the solar semiempirical T(τ) by Vernazza et al. (1981, ApJS, 45, 635) provides stellar model effective temperatures that agree quite well with the results with the hydrocalibrated relationships.
Key words: convection / stars: evolution / HertzsprungRussell and CM diagrams
© ESO, 2015
1. Introduction
The almost universally adopted method for calculating superadiabatic convective temperature gradients in stellar evolution models is based on the formalism provided by the mixing length theory (MLT; BöhmVitense 1958). This formalism is extremely simple; the gas flow is made of columns of upward and downward moving convective elements with a characteristic size, the same in all dimensions, that cover a fixed mean free path before dissolving. All convective elements have the same physical properties at a given distance from the star centre; upward moving elements release their excess heat into the surrounding gas, and are replaced at their starting point by the downward moving elements that thermalize with the surrounding matter, thus perpetuating the cycle. The MLT is a local theory, and the evaluation of all relevant physical and chemical quantities are based on the local properties of each specific stellar layer, regardless of the extension of the whole convective region.
Both the mean free path and the characteristic size of the convective elements are assumed to be same for all convective bubbles, and are assigned the same value Λ = α_{ml}H_{p}, the mixing length. Here α_{ml} is a free parameter (assumed to be a constant value within the convective regions and along all evolutionary phases), and H_{p} is the local pressure scale height. There are additional free parameters in the MLT that are generally fixed a priori (versions of the MLT with different choices of these additional parameters will be denoted here as different MLT flavours), so that practically the only free parameter to be calibrated is α_{ml}. Stellar evolution calculations for a fixed mass and initial chemical composition but with varying α_{ml} produce evolutionary tracks with different T_{eff} and radius evolution, whereas evolutionary timescales and luminosities are typically unchanged. On the other hand, the prediction of accurate values of T_{eff} and radii by evolutionary models and stellar isochrones is paramount to the study of colour–magnitude diagrams of resolved stellar populations, empirical massradius relations of eclipsing binary systems, and predicting reliable integrated spectra and colours of unresolved stellar systems (extragalactic clusters and galaxies).
In stellar evolution calculations the value of α_{ml} is usually calibrated by reproducing the radius of the Sun at the solar age with an evolutionary solar model. This solar calibrated α_{ml} is then kept fixed in all evolutionary calculations of stars of different masses and chemical compositions. The exact numerical value of α_{ml} varies amongst calculations by different authors because variations of input physics and choices of the outer boundary conditions affect the predicted model radii and T_{eff} values, hence require different α_{ml} values to match the Sun. Pedersen et al. (1990) and Salaris & Cassisi (2008) have shown how the various MLT flavours provide the same T_{eff} evolution once α_{ml} is appropriately recalibrated on the Sun.
As discussed by e.g. Vandenberg et al. (1996) and Salaris et al. (2002), metalpoor red giant branch (RGB) models calculated with the solar calibrated value of α_{ml} (hereafter α_{ml, ⊙}) are able to reproduce the T_{eff} of samples of RGB stars in Galactic globular clusters within the error bars on the estimated T_{eff}. On the other hand, several authors find that variations of α_{ml} with respect to α_{ml, ⊙} are necessary to reproduce – to give some examples – the red edge of the RGB in a sample of 38 nearby Galactic disc stars with radii determined from interferometry (Piau et al. 2011); the asteroseismically constrained radii of a sample of main sequence (MS) Kepler targets (Mathur et al. 2012); observations of binary MS stars in the Hyades (Yıldız et al. 2006); and the α Cen system (Yıldız 2007), a lowmass preMS eclipsing binary in Orion (Stassun et al. 2004).
The MLT formalism only provides a very simplified description of convection, and there have been several attempts to introduce nonlocality in the MLT (see e.g. Grossman et al. 1993; Deng et al. 2006, and references therein). These refinements of the MLT are often complex and introduce additional free parameters to be calibrated. The alternative model by Canuto & Mazzitelli (1991, 1992) includes a spectrum of eddy sizes (rather than the onesized convective cells of the MLT) and fixes the scale length of the convective motions to the distance to the closest convective boundary. Recently Pasetto et al. (2014) have presented a new nonlocal and timedependent model based on the solution of the NavierStokes equations for an incompressible perfect fluid that does not contain any free parameters^{1}.
An alternative approach to modelling the superadiabatic layers of convective envelopes is based on the computation of realistic multidimensional radiation hydrodynamics (RHD) simulations of atmospheres and convective envelopes – where convection emerges from first principles – that cover the range of effective temperatures (T_{eff}), surface gravities (g), and compositions typical of stars with surface convection. These simulations have reached a high level of sophistication (see e.g. Nordlund et al. 2009), and for ease of implementation in stellar evolution codes their results can be used to provide an hydrocalibration of an effective α_{ml}, even though RHD simulations do not confirm the basic MLT picture of columns of convective cells. After early attempts using rather crude twodimensional (2D) and threedimensional (3D) simulations (see e.g. Deupree & Varner 1980; Lydon et al. 1992), a first comprehensive RHD calibration of α_{ml} was presented by Ludwig et al. (1999) and Freytag et al. (1999). These authors found from their simulations that the calibrated α_{ml} varies as a function of metallicity, g and T_{eff}. Freytag & Salaris (1999) applied this RHD calibration of α_{ml} (plus T(τ) relations computed from the same RHD models, and Rosseland opacities consistent with the RHD calculations) to metalpoor stellar evolution models for Galactic globular cluster stars, and found that the resulting isochrones for the relevant age range have only small T_{eff} differences along the RGB (of the order of ~50 K) compared to isochrones computed with a solar calibrated value of α_{ml}.
In recent years a number of grids of 3D hydrodynamics simulations of surface convection have been published, and from the point of view of stellar model calculations it is very important to study whether the results by Freytag & Salaris (1999) are confirmed or drastically changed.
Tanner et al. (2013b,a) have presented a grid of simulations employing a 3D Eddington solver in the optically thin layers (Tanner et al. 2012). Their calculations cover four metallicities (from Z = 0.001 to Z = 0.04), but just a few T_{eff} values at constant log(g) = 4.30 for each Z, plus a subset of models at varying He mass fraction for Z = 0.001 and Z = 0.02. These authors studied the properties of convection with varying T_{eff} and chemical composition in these solarlike envelopes. Tanner et al. (2014) extracted metallicitydependent T(τ) relations from these same simulations, and employed them to highlight the critical role these relations play when calibrating α_{ml} with stellar evolution models.
Magic et al. (2013) have published a very large grid of 3D RHD simulations for a range of chemical compositions. Their grid covers a range of T_{eff} from 4000 to 7000 K in steps of 500 K, a range of log(g) from 1.5 to 5.0 in steps of 0.5 dex, and metallicity, [Fe/H], from −4.0 to +0.5 in steps of 0.5 and 1.0 dex. These models have been employed by Magic et al. (2015) to calibrate α_{ml} as function of g, T_{eff}, and [Fe/H]. They found that α_{ml} depends in a complex way on these three parameters, but in general α_{ml} decreases towards higher effective temperature, lower surface gravity, and higher metallicity. So far Magic et al. (2015) have only provided fitting formulae for α_{ml}, but not publicly available prescriptions for the boundary conditions and input physics.
Very recently Trampedach et al. (2013) produced a nonsquare grid of convective atmosphere/envelope 3D RHD simulations for the solar chemical composition. The grid spans a T_{eff} range from 4200 to 6900 K for MS stars around log(g) = 4.5, and from 4300 to 5000 K for red giants with log(g) = 2.2, the lowest surface gravity available. In Trampedach et al. (2014b) the horizontal and temporal averages of the 3D simulations were then matched to 1D hydrostatic equilibrium, spherically symmetric envelope models to calibrate α_{ml} as a function of g and T_{eff} (see Trampedach et al. 2014b, for details about the calibration procedure). Moreover, the same RHD simulations have been employed by Trampedach et al. (2014a) to calculate g and T_{eff}dependent T(τ) relations from temporal and τ (Rosseland optical depth) averaged temperatures of the atmospheric layers. Trampedach et al. (2014b) also provide routines for calculating their g and T_{eff}dependent RHDcalibrated α_{ml} together with their computed T(τ) relations, and Rosseland opacities consistent with the opacities used in the RHD simulations. This enables stellar evolution calculations where boundary conditions, superadiabatic temperature gradients and opacities of the convective envelope are consistent with the RHD simulations. It is particularly important to use both the RHDcalibrated α_{ml} and T(τ) relations because the T_{eff} of the stellar evolution calculations depends on both these inputs (see e.g. Salaris et al. 2002; Tanner et al. 2014, and references therein).
Thanks to this consistency between RHD simulations and publicly available stellar model inputs, we present and discuss in this paper the first stellar evolution calculations where the Trampedach et al. (2014b) 3D RHDcalibration of α_{ml} is selfconsistently included in the evolutionary code. In the same vein as Freytag & Salaris (1999), we focus on the effect of the calibrated variable α_{ml} on the model T_{eff}, compared to the case of calculations with fixed α_{ml, ⊙} (as determined from the same RHD simulations). Selfconsistency of opacity and boundary conditions is paramount in order to assess correctly differential effects, given that the response of models to variations of α_{ml} depends on their T_{eff}, which in turn depends on the absolute value of α_{ml}, opacities, and boundary conditions. We also address the role played by the RHD calibrated T(τ) relations in the determination of the model T_{eff} when compared to other widely used relations.
Section 2 briefly describes the relevant input physics of the models, while Sect. 3 presents and compares the resulting evolutionary tracks. A summary and discussion close the paper.
2. Input physics
All stellar evolution calculations presented here were performed with the BaSTI (BAg of Stellar Tracks and Isochrones) code (Pietrinferni et al. 2004) for a chemical composition with Y = 0.245, Z = 0.018, and the Grevesse & Noels (1993) metal mixture consistent with the chemical composition of the RHD simulations. Atomic diffusion was switched off in these calculations, and convective core overshooting was included when appropriate (see Pietrinferni et al. 2004, for details).
We employed the Rosseland opacities provided by Trampedach et al. (2014b). The low temperature opacities (for log(T) < 4.5) are very close to Ferguson et al. (2005) with the exception of the region with log(T) < 3.5, where the Ferguson et al. (2005) calculations are higher because of the inclusion of the effect of water molecules (see Trampedach et al. 2014a). Opacity Project (Badnell et al. 2005) calculations are used for log(T) ≥ 4.5. Regarding the surface boundary conditions, we employed the T(τ) relations computed by Trampedach et al. (2014a), who provided a routine that calculates, for a given T_{eff} and surface gravity, the appropriate generalized Hopf functions q(τ) related to the T(τ) relation by (1)In our calculations we fixed at τ_{tr} = 2/3 the transition from the T(τ) integration of the atmospheric layers (with τ as independent variable) to the integration of the full system of stellar structure equations. As mentioned by Trampedach et al. (2014a,b), these RHDbased T(τ) relations can also be employed to model the convective layers in the optically thick part of the envelope, together with modified expressions for the temperature gradients in the superadiabatic regions, and an appropriate rescaling of τ (see Trampedach et al. 2014a, for details). In our calculations we compared the radiative (∇_{rad}) and superadiabatic (∇, obtained with the RHD calibrated values of α_{ml}) temperature gradients determined along the upper part of the convective envelopes from the standard stellar structure equations and MLT (down to τ = 100, the upper limit for the routine calculating the Hopf functions), with ∇_{rad} and ∇ calculated according to Eqs. (35) and (36) of Trampedach et al. (2014a), respectively. We have found that in all our models the differences between these two sets of gradients are much less than 1% between τ_{tr} and τ = 100.
We also calculated test models by changing τ_{tr} between 2/3 and 5 (with the appropriate rescaling of τ if convection appears in the atmosphere integration, see Trampedach et al. 2014a), and obtained identical evolutionary tracks in each case.
Regarding the value of α_{ml}, the same routine for the Hopf functions also provides the RHD calibrated value of α_{ml} (for the BöhmVitense 1958, flavour of the MLT) for a given T_{eff} and surface gravity that we employed in our calculations. Uncertainties in the calibrated α_{ml} values are of the order of ± 0.02−0.03 (see Table 1 of Trampedach et al. 2014b)^{2}.
The only difference in terms of input physics between the atmosphere/envelope RHD calculations and our models is the equation of state (EOS). The RHD simulations employed the MHD (Daeppen et al. 1988) EOS, which is not the same EOS used in the BaSTI calculations (see Pietrinferni et al. 2004). To check whether this can cause major differences in the models, we calculated envelope models for the same g − T_{eff} pairs of the RHD simulations, including the RHDcalibrated α_{ml}, T(τ) relations, and RHD opacities. We then compared the resulting depths of the convection zones (d_{CZ}, in units of stellar radius) with the values obtained by Trampedach et al. (2014b) from their RHDcalibrated 1D envelope models, which used the same input physics (including EOS) of the RHD calculations (see Table 1 of Trampedach et al. 2014b). We found random (nonsystematic) differences of d_{CZ} by at most just 2–3% compared to the Trampedach et al. (2014b) results.
Fig. 1
Stellar evolution tracks in the g − T_{eff} diagram for the labelled masses. The region enclosed by the thick black boundary is the g − T_{eff} range covered by the RHD simulations. Thick solid lines denote fully consistent calculations with the RHD calibrated variable α_{ml} and T(τ) relationships. The lower panel displays the evolution of α_{ml} along each track. The dotted portion of each sequence denotes the region where the α_{ml} values are extrapolated. Dashed lines in the upper panel represent tracks calculated with a constant α_{ml} = α_{ml, ⊙} and the RHD T(τ) relationships. 

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3. Model comparisons
As mentioned in the introduction, the RHD simulations cover a nonsquare region in the g − T_{eff} diagram, as shown in Fig. 1 (the region enclosed by thick solid lines), ranging from 4200 to 6900 K on the MS, and from 4300 to 5000 K for RGB stars with log(g) = 2.2. The MLT calibration results in an α_{ml} varying from 1.6 for the warmest dwarfs, with a thin convective envelope, up to 2.05 for the coolest dwarfs in the grid. In between there is a triangular plateau of α_{ml} ~ 1.76, where the Sun is located. The RHD simulation for the Sun provides α_{ml} ~ 1.76 ± 0.03. The top panel of Fig. 1 shows the results of our evolutionary model calculations in the g − T_{eff} diagram (from the preMS to the lower RGB), for masses M = 0.75, 1.0, 1.4, 2.0, and 3.0 M_{⊙} that cover the full domain of the RHD simulations.
The thick solid lines denote the reference set of models, calculated with the varying α_{ml} calibration, and the run of α_{ml} along each individual track is shown in the lower panel. The dotted part of each sequence in this panel denotes the α_{ml} values extrapolated by the calibration routine, when the models are outside the region covered by the simulations but still retain a convective region. This happens along the preMS evolution of the M = 0.75 M_{⊙} track, and for the 2.0 and 3.0 M_{⊙} calculations along the subgiant phase. Apart from the preMS stages of the two lowest mass models, the evolution of α_{ml} spans a narrow range of values, between ~1.6 and ~1.8.
To study the significance of the variation of α_{ml} for the model T_{eff}, we calculated evolutionary models for the same masses, this time keeping α_{ml} = α_{ml, ⊙} = 1.76 along the whole evolution. The results are also shown in Fig. 1.
A comparison of the two sets of tracks clearly shows that the effect of a varying α_{ml} is almost negligible. The largest differences are of only ~30 K along the RGB phase of the 3.0 M_{⊙} track (solar tracks being hotter because of a higher α_{ml} value compared to the calibration) and ~50 K at the bottom of the Hayashi track of the 1.0 M_{⊙} track (solar α_{ml} tracks being cooler because of a lower α_{ml}). In all other cases differences are smaller, often almost zero.
For all stellar masses we found that the mass fraction of He dredged to the surface by the first dredge up, which depends on the maximum depth of the convective envelope at the beginning of the RGB phase, is the same within 0.001 between constant α_{ml, ⊙} and variable α_{ml} models. We then compared the luminosity of the RGB bump, which also depends on the maximum depth of the convective envelope at the first dredge up (see e.g. Cassisi & Salaris 1997, 2013, and references therein), for the 0.75 and 1.0 M_{⊙} models. We found that the luminosity is unchanged between models with constant and variable α_{ml}. This reflect the fact that the depth of the convective envelope is the same between the two sets of models throughout the MS phase to the RGB until the end of the calculations. Small differences appear only during the preMS. To this purpose, for the 1.0 M_{⊙} models we additionally checked the surface Li abundance that survives the preMS depletion. This provides information about the evolution of the lower boundary of the convective envelope during this phase, where according to Fig. 1, α_{ml} shows the largest difference from α_{ml, ⊙}. We found that, after the preMS, models with constant α_{ml, ⊙} display a Li abundance just 9% higher than the reference results.
Fig. 2
Comparison of the ratio T/T_{eff} as a function of the optical depth τ as predicted by different T(τ) relationships. The thick solid and dotted lines represent the RHDcalibrated relationships for T_{eff} = 4500 K and 6000 K (log(g) = 3.5 in both cases), respectively. The thin solid, dashdotted, and dashed lines show the ratios obtained from the Eddington, KS, and VAL_{c}T(τ) relationships, respectively. 

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We then analyzed the role played by the T(τ) relationships computed from the RHD calculations in determining the model T_{eff} (the role played by the boundary conditions in determining the T_{eff} of stellar models is especially crucial for very lowmass stars, see e.g. Allard et al. 1997; Brocato et al. 1998). Figure 2 shows the ratio T/T_{eff} as a function of τ as predicted by the calibrated relationships for atmospheres/envelopes with T_{eff} = 4500 K and 6000 K (log(g) = 3.5). The RHD calibrated T(τ) relationships contain values for the Hopf function that vary with τ and T_{eff} (also with g, but to a lesser degree). The variation with T_{eff} is obvious from the figure. For these two temperatures the largest differences appear at the layers with τ between ~0.1 and ~−1, where stellar model calculations usually fix the transition from the atmosphere to the interior. Figure 2 also shows the results of the traditional Eddington approximation to the grey atmosphere, and the solar semiempirical T(τ) relationships by KrishnaSwamy (KS; Krishna Swamy 1966) and Vernazza et al. (1981) – their Model C for the quiet sun, hereafter VAL_{c}T(τ). In these cases the ratio T/T_{eff} does not depend on T_{eff}. It is easy to notice that around the photospheric layers the RHD relationships are in between the Eddington grey and VAL_{c}T(τ). The most discrepant relationship is the KS one.
Fig. 3
As the upper panel of Fig. 1 but for evolutionary tracks with masses equal to 1.0 and 1.4 M_{⊙}, respectively. Thick solid lines denote fully consistent calculations with the RHD calibrated variable α_{ml} and T(τ) relationships. Dotted, dashdotted, and dashed lines display tracks calculated with constant α_{ml, ⊙} and the Eddington, KS, and VAL_{c}T(τ), respectively. 

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Figure 3 shows the results of evolutionary calculations with this set of T(τ) relationships. We compare here the reference set of models for 1.0 and 1.4 M_{⊙} and varying α_{ml}, with constant α_{ml, ⊙} models calculated using the Eddington, KS, and VAL_{c}T(τ) relationships (τ_{tr} = 2/3 also for these calculations).
The differences between these new sets of models at constant α_{ml, ⊙} and the reference calculations are larger than the case of Fig. 1 because of the differences with the RHD T(τ) relationships. On the whole, the VAL_{c}T(τ) (coupled to the RHD calibrated α_{ml, ⊙}) gives the closest match to the selfconsistent reference calculations. The largest differences appear for the 1.0 M_{⊙} along the preMS; models calculated with the VAL_{c} relation are ~50 K cooler, approximately the same as the case of α_{ml, ⊙} and the RHD T(τ). For the same 1.0 M_{⊙} track the T_{eff} differences along the RGB are at most 10 K, and at most ~40 K along the MS. Differences for the 1.4 M_{⊙} track are smaller.
Regarding the Eddington T(τ), the resulting tracks are generally hotter than the selfconsistent RHDbased calculations. The largest differences amount to ~40–50 K along MS and RGB of the two tracks. Comparisons with Fig. 1 show that, from the point of view of the resulting model T_{eff}, the Eddington T(τ) differs more – although not by much – than the VAL_{c} one from the RHD relations.
The worse agreement is found with the KS T(τ). For both masses the RGB is systematically cooler by ~70 K, and the preMS by ~80–100 K, whilst the MS of the 1.0 M_{⊙} calculations is cooler by ~120 K, a difference reduced to ~50 K along the MS of the 1.4 M_{⊙} track.
In case of the 1.0 M_{⊙} models we rechecked the luminosity level of the RGB bump, the surface He mass fraction after the first dredge up, and the amount of surface Li after the preMS depletion. For all these three T(τ) relations the evolutionary models display a RGB bump luminosity within Δ(L/L_{⊙}) < 0.01, and a postdredge up He abundance within 0.001 of the fully consistent result. In all these calculations the convective envelope has the same depth throughout the MS phase and along the RGB. Differences along the preMS are highlighted by the amount of Li depletion during this phase. We found that models calculated with the Eddington T(τ) have 9% less Li after the preMS than the reference calculations. Comparing this number with just the effect of a constant α_{ml, ⊙} discussed above, we derive that the use of this T(τ) decreases the surface Li abundance by ~20% compared to the use of the Hopf functions determined from the RHD simulations. In the case of the VAL_{c}T(τ), the net effect is to increase the surface Li after the preMS by ~10% compared to the RHD T(τ), and the KS relation causes a similar increase by ~11%.
3.1. The standard solar model
We close our analysis by discussing the implications of the RHD results and the choice of the T(τ) relation, on the calibration of the standard solar model. As is well known, in stellar evolution it is customary to fix the value of α_{ml, ⊙} (and the initial solar He and metal mass fractions) by calculating a 1 M_{⊙} stellar model that matches the solar bolometric luminosity and radius at the age of the Sun, with the additional constraint of reproducing the present metal to hydrogen mass fraction Z/X ratio (see e.g. Pietrinferni et al. 2004, for details). The accuracy of the derived solar model can then be tested against helioseismic estimates of the depth of the convective envelope and the surface He mass fraction. It is also well established that solar models without microscopic diffusion cannot properly account for some helioseismic constraints, hence solar models are routinely calculated by including microscopic diffusion of He and metals (see e.g. Pietrinferni et al. 2004, for a discussion and references).
We first calculated a standard solar model (with the same input physics and solar metal distribution of the calculations discussed above) employing both the variable α_{ml} and the T(τ) relations from the RHD results. Given that microscopic diffusion decreases the surface chemical abundances of the model with time, the initial solar Z (and Y) need to be higher than the present level. This means that we also had to employ the RHD results for chemical compositions that were not exactly the same as the composition of the RHD simulations.
We found that it is necessary to rescale the RHD α_{ml} calibration by a factor of just 1.034 to reproduce the solar radius. This implies α_{ml, ⊙} = 1.82, extremely close, within the error, to the RHD value α_{ml, ⊙} = 1.76 ± 0.01(range) ±0.03(calibration uncertainty) obtained by Trampedach et al. (2014b). Given our previous results, it is also obvious that a solar model calibration with fixed α_{ml} and the RHD T(τ) relations provides the same α_{ml, ⊙} = 1.82.
Solar calibrations with the KS, VAL_{c}, and Eddington T(τ) relations have provided α_{ml, ⊙} = 2.11, 1.90, and 1.69, respectively.
In all these calibrated solar models the initial solar He mass fraction (Y_{ini, ⊙} ~ 0.274) and metallicity ((Z_{ini, ⊙} ~ 0.0199) are essentially the same, as expected. In addition, the model values for the present He mass fraction in the envelope (Y_{⊙} = 0.244) and the depth of the convection zone (d_{CZ} = 0.286R_{⊙}) are the same for all calibrations and are in agreement with the helioseismic values (see e.g. Dziembowski et al. 1995; Basu & Antia 1997).
If we take α_{ml, ⊙} obtained with the RHD T(τ) as a reference, the lower value obtained with the Eddington T(τ) and the larger values obtained with both the VAL_{c} and KS relations (in increasing order) are fully consistent with the results of Fig. 3. In that figure VAL_{c} and KS T(τ) MS models are increasingly cooler than the reference RHD calculations (hence increasingly larger α_{ml} values are required to match the reference MS) whereas the use of the Eddington T(τ) produces models hotter than the reference MS (hence lower α_{ml} value are needed to match the reference MS).
4. Summary and discussion
We presented the first selfconsistent stellar evolution calculations that employ the variable α_{ml} and T(τ) by Trampedach et al. (2014b), based on their 3D RHD simulations. Our set of evolutionary tracks for different masses and the same chemical composition (plus consistent Rosseland opacities) of the RHD simulations, cover approximately the entire g − T_{eff} parameter space of the 3D atmosphere/envelope calculations.
We found that, from the point of view of the predicted T_{eff} (plus the depth of the convective envelopes and amount of preMS Li depletion), models calculated with constant RHD calibrated α_{ml, ⊙} = 1.76 are very close to, and often indistinguishable from, the models with variable α_{ml}. The maximum differences are at most ~30–50 K. This result is similar to the conclusions by Freytag & Salaris (1999), based on 2D RHD simulations at low metallicities.
At first sight this may appear surprising, given that the full range of α_{ml} spanned by the RHD calibration is between ~1.6 and ~2.0. However, one has to take into account the following points:

1.
The derivative ΔT_{eff}/ Δα_{ml} for stellar evolution models depends on theabsolute value of α_{ml}, and decreases when α_{ml} increases.

2.
The variation of ΔT_{eff} for a given Δα_{ml} also depends on the mass extension of the convective and superadiabatic regions.
It is therefore clear that the decrease of α_{ml} with increasing T_{eff} cannot have a major effect because of the thin convective (and superadiabatic) layers of models crossing this region of the g − T_{eff} diagram. The large variations Δα_{ml} ~ 0.2 (see lower panel of Fig. 1) along the lower Hayashi track of the 1.0 M_{⊙} model is also not very significant (~50 K) because of the decreased extension of the surface convection and the reduced ΔT_{eff}/ Δα_{ml} at higher α_{ml}.
It is however very important to remark here that the detailed structure of the superadiabatic convective regions is not suitably reproduced either by α_{ml, ⊙} or by a variable α_{ml}, and that the full results from RHD models need to be employed whenever a detailed description of the properties of these layers is needed.
To some degree the role played by the RHD T(τ) is more significant. Constant α_{ml, ⊙} = 1.76 stellar evolution models become systematically cooler by up to ~100 K along the MS, preMS, and RGB when the widely used KS T(τ) relation is used, compared to the selfconsistent RHDcalibrated calculations. Evolutionary tracks obtained employing the Eddington and VAL_{c}T(τ) relationships are much less discrepant, and stay within ~50 K of the selfconsistent calculations. Even from the point of view of preMS Li depletion the VAL_{c}T(τ) causes only minor differences, of the order of 10%. A similar difference is found with the KS relation, whilst a larger effect of ~20% is found with the Eddington T(τ).
An extension of the Trampedach et al. (2013) simulations to different metallicities is necessary to extend this study and test the significance of the α_{ml} variability (and Hopf functions) over a larger parameter space. The 3D RHD simulations by Magic et al. (2013) and the α_{ml} calibration by Magic et al. (2015) cover a large metallicity range, and predict an increase of α_{ml} with decreasing metal content, but at the moment it is not possible to properly include this calibration in stellar evolution calculations, for the lack of available T(τ) relations and input physics consistent with the RHD simulations. At solar metallicity the general behaviour of α_{ml} with g and T_{eff} seems to be qualitatively similar to Trampedach et al. (2014b) calibration. However, the range of α_{ml} is shifted to higher values compared to Trampedach et al. (2014b) results, probably owing to different input physics and the different adopted solar chemical composition.
We did not include any turbulent pressure in the convective envelope, as the α_{ml} RHD calibration was performed in a way that works for standard stellar evolution models without this extra contribution to the pressure (Trampedach, priv. comm.; see also Sect. 4 in Trampedach et al. 2014b).
Acknowledgments
We are grateful to R. Trampedach for clarifications about his results, and for making available the routine to calculate Rosseland opacities. We also thank J. ChristensenDalsgaard for interesting discussions on this topic, and the anonymous referee for comments that have improved the presentation of our results. S.C. gratefully acknowledges financial support from PRININAF2014 (PI: S. Cassisi).
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All Figures
Fig. 1
Stellar evolution tracks in the g − T_{eff} diagram for the labelled masses. The region enclosed by the thick black boundary is the g − T_{eff} range covered by the RHD simulations. Thick solid lines denote fully consistent calculations with the RHD calibrated variable α_{ml} and T(τ) relationships. The lower panel displays the evolution of α_{ml} along each track. The dotted portion of each sequence denotes the region where the α_{ml} values are extrapolated. Dashed lines in the upper panel represent tracks calculated with a constant α_{ml} = α_{ml, ⊙} and the RHD T(τ) relationships. 

Open with DEXTER  
In the text 
Fig. 2
Comparison of the ratio T/T_{eff} as a function of the optical depth τ as predicted by different T(τ) relationships. The thick solid and dotted lines represent the RHDcalibrated relationships for T_{eff} = 4500 K and 6000 K (log(g) = 3.5 in both cases), respectively. The thin solid, dashdotted, and dashed lines show the ratios obtained from the Eddington, KS, and VAL_{c}T(τ) relationships, respectively. 

Open with DEXTER  
In the text 
Fig. 3
As the upper panel of Fig. 1 but for evolutionary tracks with masses equal to 1.0 and 1.4 M_{⊙}, respectively. Thick solid lines denote fully consistent calculations with the RHD calibrated variable α_{ml} and T(τ) relationships. Dotted, dashdotted, and dashed lines display tracks calculated with constant α_{ml, ⊙} and the Eddington, KS, and VAL_{c}T(τ), respectively. 

Open with DEXTER  
In the text 
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