Abstract <p>Babingtonite, Ca<sub>2.0</sub>(<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11476_2025_11752_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="72" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{Fe}}_{{0.6}}^{{2 + }}{\text{Mn}}_{{0.2}}^{{2 + }}\)</EquationSource> <!--GeoChem2460204Gritsenko-m1--> </InlineEquation>Mg<sub>0.2</sub>)<sub>∑10.</sub><InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11476_2025_11752_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{Fe}}_{{1.0}}^{{3 + }}\)</EquationSource> <!--GeoChem2460204Gritsenko-m2--> </InlineEquation>Si<sub>5</sub>O<sub>14</sub>(OH)<sub>1.0</sub> from Herborn (Hessen, Germany) was comprehensively studied using powder X-ray diffraction, electron probe microanalysis, and IR absorption, Raman, and Mössbauer spectroscopies. The enthalpy of babingtonite formation from the elements was determined for the first time by high-temperature solution calorimetry on a Calvet microcalorimeter in 2PbO · B<sub>2</sub>O<sub>3</sub> melt at <i>T</i> = 973 K as –6911.6 ± 10.2 kJ/mol. Its standard entropy was estimated as 338.8 ± 2.0 J/(mol K), and the standard entropy and Gibbs energy of formation were calculated: –1501.3 ± 2.0 J/(mol K) and –6464.0 ± 10.2 kJ/mol, respectively. The thermodynamic constants of the end-members of the babingtonite Ca<sub>2</sub>Fe<sup>2+</sup>Fe<sup>3+</sup>Si<sub>5</sub>O<sub>14</sub>(OH)–manganbabingtonite Ca<sub>2</sub>Mn<sup>2+</sup>Fe<sup>3+</sup>Si<sub>5</sub>O<sub>14</sub>(OH) isomorphous series were estimated: <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11476_2025_11752_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\Delta }_{f}}H_{{{\text{el}}}}^{^\circ }\)</EquationSource> <!--GeoChem2460204Gritsenko-m3--> </InlineEquation>(298.15 K) = –6868.0 ± 10.4 and –6876.9 ± 9.9 kJ/mol, <i>S</i>°(298.15 K) = 341.2 ± 1.8 and 343.9 ± 2.6 J/(mol K), <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11476_2025_11752_Article_IEq4.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\Delta }_{f}}S_{{{\text{el}}}}^{^\circ }\)</EquationSource> <!--GeoChem2460204Gritsenko-m4--> </InlineEquation>(298.15 K) = –1496.8 ± 1.8 and –1499.0 ± 2.6 J/(mol K), and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11476_2025_11752_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\Delta }_{f}}G_{{{\text{el}}}}^{^\circ }\)</EquationSource> <!--GeoChem2460204Gritsenko-m5--> </InlineEquation>(298.15 K) = ‒6422.0 ± 10.4 and –6430.0 ± 9.9 kJ/mol, respectively. The stability fields of babingtonite in the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11476_2025_11752_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\({{P}_{{{{{\text{H}}}_{{\text{2}}}}{\text{O}}}}}\)</EquationSource> <!--GeoChem2460204Gritsenko-m6--> </InlineEquation>–<i>T</i> coordinates were calculated for the redox conditions controlled by the quartz–fayalite–magnetite and magnetite–hematite buffers, and mineral associations of babingtonite characteristic of low-grade metamorphism and late skarn assemblages were determined in the <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11476_2025_11752_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="127" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{log}}{\kern 1pt} {{P}_{{{\text{C}}{{{\text{O}}}_{{\text{2}}}}}}}{\kern 1pt} - {\kern 1pt} {\text{log}}{\kern 1pt} {{P}_{{{{{\text{O}}}_{{\text{2}}}}}}}\)</EquationSource> <!--GeoChem2460204Gritsenko-m7--> </InlineEquation> plane.</p>

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Physicochemical Characteristics and Thermodynamic Properties of Babingtonite

  • Yu. D. Gritsenko,
  • L. P. Ogorodova,
  • M. F. Vigasina,
  • S. K. Dedushenko,
  • A. Yu. Bychkov,
  • D. A. Ksenofontov,
  • L. V. Mel’chakova

摘要

Abstract

Babingtonite, Ca2.0( \({\text{Fe}}_{{0.6}}^{{2 + }}{\text{Mn}}_{{0.2}}^{{2 + }}\) Mg0.2)∑10. \({\text{Fe}}_{{1.0}}^{{3 + }}\) Si5O14(OH)1.0 from Herborn (Hessen, Germany) was comprehensively studied using powder X-ray diffraction, electron probe microanalysis, and IR absorption, Raman, and Mössbauer spectroscopies. The enthalpy of babingtonite formation from the elements was determined for the first time by high-temperature solution calorimetry on a Calvet microcalorimeter in 2PbO · B2O3 melt at T = 973 K as –6911.6 ± 10.2 kJ/mol. Its standard entropy was estimated as 338.8 ± 2.0 J/(mol K), and the standard entropy and Gibbs energy of formation were calculated: –1501.3 ± 2.0 J/(mol K) and –6464.0 ± 10.2 kJ/mol, respectively. The thermodynamic constants of the end-members of the babingtonite Ca2Fe2+Fe3+Si5O14(OH)–manganbabingtonite Ca2Mn2+Fe3+Si5O14(OH) isomorphous series were estimated: \({{\Delta }_{f}}H_{{{\text{el}}}}^{^\circ }\) (298.15 K) = –6868.0 ± 10.4 and –6876.9 ± 9.9 kJ/mol, S°(298.15 K) = 341.2 ± 1.8 and 343.9 ± 2.6 J/(mol K), \({{\Delta }_{f}}S_{{{\text{el}}}}^{^\circ }\) (298.15 K) = –1496.8 ± 1.8 and –1499.0 ± 2.6 J/(mol K), and \({{\Delta }_{f}}G_{{{\text{el}}}}^{^\circ }\) (298.15 K) = ‒6422.0 ± 10.4 and –6430.0 ± 9.9 kJ/mol, respectively. The stability fields of babingtonite in the \({{P}_{{{{{\text{H}}}_{{\text{2}}}}{\text{O}}}}}\) T coordinates were calculated for the redox conditions controlled by the quartz–fayalite–magnetite and magnetite–hematite buffers, and mineral associations of babingtonite characteristic of low-grade metamorphism and late skarn assemblages were determined in the \({\text{log}}{\kern 1pt} {{P}_{{{\text{C}}{{{\text{O}}}_{{\text{2}}}}}}}{\kern 1pt} - {\kern 1pt} {\text{log}}{\kern 1pt} {{P}_{{{{{\text{O}}}_{{\text{2}}}}}}}\) plane.