© 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; Böhm-Vitense 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_mlH_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 mass-radius 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), metal-poor 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 low-mass pre-MS 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 non-locality 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 one-sized 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 non-local and time-dependent model based on the solution of the Navier-Stokes equations for an incompressible perfect fluid that does not contain any free parameters¹.

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 hydro-calibration 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 two-dimensional (2D) and three-dimensional (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 metal-poor 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 solar-like envelopes. Tanner et al. (2014) extracted metallicity-dependent 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 non-square 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 RHD-calibrated 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 RHD-calibrated 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 RHD-calibration of α_ml is self-consistently 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). Self-consistency 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 RHD-based 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 Böhm-Vitense 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 RHD-calibrated 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 RHD-calibrated 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 (non-systematic) differences of d_CZ by at most just 2–3% compared to the Trampedach et al. (2014b) results.

3. Model comparisons

As mentioned in the introduction, the RHD simulations cover a non-square 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 pre-MS 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 pre-MS 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 pre-MS 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 pre-MS. To this purpose, for the 1.0 M_⊙ models we additionally checked the surface Li abundance that survives the pre-MS 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 pre-MS, models with constant α_{ml, ⊙} display a Li abundance just 9% higher than the reference results.

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 low-mass 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 semi-empirical T(τ) relationships by Krishna-Swamy (KS; Krishna Swamy 1966) and Vernazza et al. (1981) – their Model C for the quiet sun, hereafter VAL_cT(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_cT(τ). The most discrepant relationship is the KS one.

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_cT(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_cT(τ) (coupled to the RHD calibrated α_{ml, ⊙}) gives the closest match to the self-consistent reference calculations. The largest differences appear for the 1.0 M_⊙ along the pre-MS; 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 self-consistent RHD-based 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 pre-MS 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 pre-MS depletion. For all these three T(τ) relations the evolutionary models display a RGB bump luminosity within Δ(L/L_⊙) < 0.01, and a post-dredge 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 pre-MS 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 pre-MS 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_cT(τ), the net effect is to increase the surface Li after the pre-MS 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 self-consistent 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 pre-MS 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, pre-MS, and RGB when the widely used KS T(τ) relation is used, compared to the self-consistent RHD-calibrated calculations. Evolutionary tracks obtained employing the Eddington and VAL_cT(τ) relationships are much less discrepant, and stay within ~50 K of the self-consistent calculations. Even from the point of view of pre-MS Li depletion the VAL_cT(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.

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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. Christensen-Dalsgaard 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 PRIN-INAF2014 (PI: S. Cassisi).

References

All Figures