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  • Oreshina, A. V.  (3)
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  • 1
    Online Resource
    Online Resource
    EDP Sciences ; 2022
    In:  Astronomy & Astrophysics Vol. 660 ( 2022-4), p. A125-
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 660 ( 2022-4), p. A125-
    Abstract: Context. The adiabatic exponent Γ 1 is studied as a thermodynamic quantity in the partially ionized plasma of the solar convection zone. Aims. The aim of this study is to understand the impact of heavy elements on the Γ 1 profile. We calculated Γ 1 with the SAHA-S equation of state for different chemical compositions of plasma, and we analyzed contributions of individual elements to Γ 1 . We attempted to determine the mass fractions of the heavy elements using our analysis of the Γ 1 profile. Methods. We studied the decrease in Γ 1 due to the ionization of heavy elements in comparison with the value obtained for a pure hydrogen-helium plasma. These types of differences are denoted as “Z contributions”, and we analyzed them for eight elements (C, N, O, Ne, Mg, S, Si, and Fe) as well as for a mixture of elements corresponding to the solar chemical composition. The contributions of the heavy elements are studied on an adiabat in the lower part of the convection zone, where the influence of hydrogen and helium to the Z contribution is minimal. The Z-contribution profiles are unique for each chemical element. We compared linear combinations of individual Z contributions with the exact Z contribution. Applying a least-squares technique to the decomposition of the full Z contribution to a basis of individual-element contributions, we obtained the mass fractions of the heavy elements. Results. The Z contribution of heavy elements can be described by a linear combination of individual-element Z contributions with a high level of accuracy of 5 × 10 −6 . The inverse problem of estimating the mass fractions of heavy elements from a given Γ 1 profile was considered for the example of solar-type mixtures. In ideal numerical simulations, the mass fractions of the most abundant elements could be determined with a relative accuracy better than a few tenths of a percent. In the presence of random or systematic errors in the Γ 1 profile, abundance estimations become remarkably less accurate, especially due to unknown features of the equations of state. If the amplitude of the errors does not exceed 10 −4 , we can expect a determination of at least the oxygen abundance with a relative error of about 10%. Otherwise, the results of the method would not be reliable.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2022
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
    Location Call Number Limitation Availability
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  • 2
    Online Resource
    Online Resource
    Pleiades Publishing Ltd ; 2017
    In:  Geomagnetism and Aeronomy Vol. 57, No. 7 ( 2017-12), p. 891-895
    In: Geomagnetism and Aeronomy, Pleiades Publishing Ltd, Vol. 57, No. 7 ( 2017-12), p. 891-895
    Type of Medium: Online Resource
    ISSN: 0016-7932 , 1555-645X
    Language: English
    Publisher: Pleiades Publishing Ltd
    Publication Date: 2017
    detail.hit.zdb_id: 2071667-9
    SSG: 16,13
    Location Call Number Limitation Availability
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  • 3
    Online Resource
    Online Resource
    EDP Sciences ; 2019
    In:  Astronomy & Astrophysics Vol. 626 ( 2019-06), p. A108-
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 626 ( 2019-06), p. A108-
    Abstract: Aims . We use Hermite splines to interpolate pressure and its derivatives simultaneously, thereby preserving mathematical relations between the derivatives. The method therefore guarantees that thermodynamic identities are obeyed even between mesh points. In addition, our method enables an estimation of the precision of the interpolation by comparing the Hermite-spline results with those of frequent cubic (B-) spline interpolation. Methods . We have interpolated pressure as a function of temperature and density with quintic Hermite 2D-splines. The Hermite interpolation requires knowledge of pressure and its first and second derivatives at every mesh point. To obtain the partial derivatives at the mesh points, we used tabulated values if given or else thermodynamic equalities, or, if not available, values obtained by differentiating B-splines. Results . The results were obtained with the grid of the SAHA-S equation-of-state (EOS) tables. The maximum lg P difference lies in the range from 10 −9 to 10 −4 , and Γ 1 difference varies from 10 −9 to 10 −3 . Specifically, for the points of a solar model, the maximum differences are one order of magnitude smaller than the aforementioned values. The poorest precision is found in the dissociation and ionization regions, occurring at T  ∼ 1.5 × 10 3 −10 5 K. The best precision is achieved at higher temperatures, T   〉  10 5 K. To discuss the significance of the interpolation errors we compare them with the corresponding difference between two different equation-of-state formalisms, SAHA-S and OPAL 2005. We find that the interpolation errors of the pressure are a few orders of magnitude less than the differences from between the physical formalisms, which is particularly true for the solar-model points.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2019
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
    Location Call Number Limitation Availability
    BibTip Others were also interested in ...
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