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<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="en"><front><journal-meta><journal-id journal-id-type="publisher-id">blackmet</journal-id><journal-title-group><journal-title xml:lang="en">Izvestiya. Ferrous Metallurgy</journal-title><trans-title-group xml:lang="ru"><trans-title>Известия высших учебных заведений. Черная Металлургия</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">0368-0797</issn><issn pub-type="epub">2410-2091</issn><publisher><publisher-name>National University of Science and Technology "MISIS"</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.17073/0368-0797-2023-5-610-612</article-id><article-id custom-type="elpub" pub-id-type="custom">blackmet-2636</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>PHYSICO-CHEMICAL BASICS OF METALLURGICAL PROCESSES</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>ФИЗИКО-ХИМИЧЕСКИЕ ОСНОВЫ МЕТАЛЛУРГИЧЕСКИХ ПРОЦЕССОВ</subject></subj-group></article-categories><title-group><article-title>Wagner interaction coefficient between nitrogen and cobalt in liquid steel</article-title><trans-title-group xml:lang="ru"><trans-title>Вагнеровский параметр взаимодействия азота с кобальтом в жидкой стали</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Большов</surname><given-names>Л. А.</given-names></name><name name-style="western" xml:lang="en"><surname>Bolʼshov</surname><given-names>L. A.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Леонид Абрамович Большов, д.ф.-м.н., профессор кафедры математики и информатики</p><p>Россия, 160000, Вологда, ул. Ленина, 15</p></bio><bio xml:lang="en"><p>Leonid A. Bolʼshov, Dr. Sci. (Phys.–Math.), Prof. of the Chair of Mathe­matics and Informatics</p><p>15 Lenina Str., Vologda 16000, Russian Federation</p></bio><email xlink:type="simple">labolshov@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Корнейчук</surname><given-names>С. К.</given-names></name><name name-style="western" xml:lang="en"><surname>Korneichuk</surname><given-names>S. K.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Светлана Константиновна Корнейчук, к.ф.-м.н., доцент кафед­ры физики</p><p>Россия, 160000, Вологда, ул. Ленина, 15</p></bio><bio xml:lang="en"><p>Svetlana K. Korneichuk, Cand. Sci. (Phys.–Math.), Assist. Prof. of the Chair of Physics</p><p>15 Lenina Str., Vologda 16000, Russian Federation</p></bio><email xlink:type="simple">korn62@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Большова</surname><given-names>Э. Л.</given-names></name><name name-style="western" xml:lang="en"><surname>Bolʼshova</surname><given-names>E. L.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Элина Леонидовна Большова, доцент кафедры английского языка</p><p>Россия, 160000, Вологда, ул. Ленина, 15</p></bio><bio xml:lang="en"><p>Elina L. Bolʼshova, Assist. Prof. of the Chair of English</p><p>15 Lenina Str., Vologda 16000, Russian Federation</p></bio><email xlink:type="simple">labolshov@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Вологодский государственный университет</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Vologda State University</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2023</year></pub-date><pub-date pub-type="epub"><day>11</day><month>11</month><year>2023</year></pub-date><volume>66</volume><issue>5</issue><fpage>610</fpage><lpage>612</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Bolʼshov L.A., Korneichuk S.K., Bolʼshova E.L., 2023</copyright-statement><copyright-year>2023</copyright-year><copyright-holder xml:lang="ru">Большов Л.А., Корнейчук С.К., Большова Э.Л.</copyright-holder><copyright-holder xml:lang="en">Bolʼshov L.A., Korneichuk S.K., Bolʼshova E.L.</copyright-holder><license license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>This work is licensed under a Creative Commons Attribution 4.0 License.</license-p></license></permissions><self-uri xlink:href="https://fermet.misis.ru/jour/article/view/2636">https://fermet.misis.ru/jour/article/view/2636</self-uri><abstract><p>A simple theory of thermodynamic properties of liquid nitrogen solutions in Fe – Co alloys is proposed. This theory is completely analogous to the theory for liquid nitrogen solutions in alloys of the Fe – Cr system proposed previously by the authors in 2019. The theory is based on lattice model of the Fe – Co solutions. The model assumes FCC lattice. In the sites of this lattice are the atoms of Fe and Co. Nitrogen atoms are located in octahedral interstices. The nitrogen atom interacts only with the metal atoms located in the lattice sites neighboring to it. This interaction is pairwise. It is supposed that the liquid solutions of Fe – Co system are perfect. The initial values for the calculation are the Sieverts law constants for nitrogen solubility in liquid iron and in liquid cobalt. Result of the calculation is value of Wagner interaction coefficient in liquid iron-based alloys at 1873 K \(\varepsilon _{\rm{N}}^{{\rm{Co}}}\) = 1.8. This value is in good agreement with the experimental data obtained by Schenck, Frohberg and Graf, 1958; Maekawa and Nakagawa, 1960.</p></abstract><trans-abstract xml:lang="ru"><p>Предложена простая теория термодинамических свойств жидких растворов азота в сплавах системы Fe – Co. Эта теория полностью аналогична теории для жидких растворов азота в сплавах системы Fe –  Cr, предложенной авторами в 2019 г. Теория основана на решеточной модели растворов Fe – Co. Предполагается модельная решетка типа ГЦК. В узлах этой решетки располагаются атомы железа и кобальта. Атомы азота располагаются в октаэдрических междоузлиях. Атом азота взаимодействует с атомами металлов, находящимися в соседних с этим атомом узлах решетки. Это взаимодействие парное. Предполагается, что жидкие растворы системы Fe – Co являются совершенными. В качестве исходных для расчетов взяты значения констант закона Сивертса для растворимости азота в жидком железе и в жидком кобальте. Результатом расчета является значение вагнеровского параметра взаимодействия в жидких сплавах на основе железа при температуре 1873 К \(\varepsilon _{\rm{N}}^{{\rm{Co}}}\) = 1,8. Это хорошо согласуется с экспериментальными данными, полученными Шенк, Фроберг, Граф в 1958 г. и Маекава, Накагава в 1960 г.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>термодинамика</kwd><kwd>растворы</kwd><kwd>азот</kwd><kwd>железо</kwd><kwd>кобальт</kwd><kwd>вагнеровский параметр взаимодействия</kwd><kwd>лангенберговский параметр взаимодействия</kwd><kwd>закон Сивертса</kwd></kwd-group><kwd-group xml:lang="en"><kwd>thermodynamics</kwd><kwd>solutions</kwd><kwd>nitrogen</kwd><kwd>iron</kwd><kwd>cobalt</kwd><kwd>Wagner interaction coefficient</kwd><kwd>Langenberg interaction coefficient</kwd><kwd>Sieverts law</kwd></kwd-group></article-meta></front><body><p>To predict the solubility of nitrogen in liquid steel, understanding the nitrogen solubility in liquid iron is crucial, along with at least obtaining the first order interaction coefficients between nitrogen and alloying elements. Typically, these coefficients are derived from experimental investigations of nitrogen solubility in the melts of binary metal systems like Fe – j, where iron serves as the solvent and j represents the alloying element. Nevertheless, values obtained through this method often encompass experimental uncertainties, occasionally of significant magnitude. This scenario also holds true for the interaction between nitrogen and cobalt.</p><p>Currently, cobalt finds diverse technological applications, including its use in alloying special steels known for their high-speed, magnetic, and heat-resistant properties. The significance of the Wagner interaction coefficient between nitrogen and cobalt in liquid steel lacks consensus. Hence, an intriguing avenue lies in investigating this matter from a theoretical perspective.</p><p>To delve into the thermodynamics of nitrogen solutions in the Fe – Co. system’s liquid alloys, we denote the concentrations of the components in molar fractions as cFe , cCo and cN . Alternatively, expressing these concentrations in mass percentages yields [% Fe], [% Co] and [% N]. Let aN means present the thermodynamic activity of nitrogen in the solution, \({\gamma _{\rm{N}}} = \frac{{{a_{\rm{N}}}}}{{{c_{\rm{N}}}}} - \) the rational coefficient of nitrogen activity in the solution, \({f_{\rm{N}}} = \frac{{{a_{\rm{N}}}}}{{[\% {\rm{ N}}]}} - \) the mass-percentage coefficient of nitrogen activity. The thermodynamic first order interaction coefficients between nitrogen and cobalt in liquid iron-based alloys of the Fe – Co – N systems are determined by the following formulas</p><p> </p><p>\[\begin{array}{c}\varepsilon _{\rm{N}}^{{\rm{Co}}} = \frac{{\partial \ln {\gamma _{\rm{N}}}}}{{\partial {c_{{\rm{Co}}}}}}{\rm{at}}{c_{{\rm{Fe}}}} \to 1;\\e_{\rm{N}}^{{\rm{Co}}} = \frac{{\partial \lg {f_{\rm{N}}}}}{{\partial [\% {\rm{ Co}}]}}{\rm{at}}[\% {\rm{ Fe}}] \to 100,\end{array}\]</p><p> </p><p>where \(\varepsilon _{\rm{N}}^{{\rm{Co}}}\) is the Wagner interaction coefficient, while \(e_{\rm{N}}^{{\rm{Co}}}\) is the Langenberg interaction coefficient. A correlation between these parameters is presented in [<xref ref-type="bibr" rid="cit1">1</xref>]:</p><p> </p><p> </p><p>where AFe and ACo are the atomic masses of the corresponding elements.</p><p>The solubility of nitrogen in liquid alloys of the Fe – Co system, expressed in mass percentage, is denoted as [% N]\(^*\). At a partial pressure of nitrogen in the liquid phase PN2 approaching zero PN2 → 0, the square root law, also known as Sieverts law, applies:</p><p> </p><p>\[{[\% {\rm{ N}}]^*} = K'\sqrt {\frac{{{P_{{{\rm{N}}_2}}}}}{{{P_0}}}} ,\]</p><p> </p><p>where P0 is the standard pressure (P0 = 1 atm ≈ 0.101 MPa); K′ is the Sieverts law constant. Let K′ = K′(Fe) at cFe = 1 and K′ = K′(Co) at cCo = 1.</p><p>Following the proposed simple theory regarding the thermodynamic properties of liquid nitrogen solutions in Fe – Co alloy systems, an alignment is observed with the theoretical framework governing nitrogen solutions in Fe – Cr and Ni – Cr alloy systems [<xref ref-type="bibr" rid="cit2">2</xref>]. The abstract of this paper outlines the theoretical model. Utilizing the findings from [<xref ref-type="bibr" rid="cit2">2</xref>], we arrive at the model presented below:</p><p> </p><p> </p><p>At a temperature of T = 1873 K K′(Fe) = 0.044 wt. % [<xref ref-type="bibr" rid="cit3">3</xref>] and K′(Co) = 0.0047 wt. % [<xref ref-type="bibr" rid="cit4">4</xref>]. With AFe = 55.847 and ACo = 58.9332 applying formula (2) yields the theoretical Wagner interaction coefficient between nitrogen and cobalt in liquid steel at T = 1873 K as \(\varepsilon _{\rm{N}}^{{\rm{Co}}}\) = 1.8. Subsequently, equation (1) provides the corresponding value of the Langenberg interaction coefficient  \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.0076.</p><p>Consideration of experimental values of the \(e_{\rm{N}}^{{\rm{Co}}}\) coefficient in liquid steel at T = 1873 K reveals various findings. In [<xref ref-type="bibr" rid="cit5">5</xref>], nitrogen solubility in Fe – Co alloys was studied by quenching samples to a concentration of [% Co] = 24 wt. %, resulting in an estimated \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.0072. Continuation of this study in [<xref ref-type="bibr" rid="cit6">6</xref>] up to [% Co] = 100 wt. % produced an estimate for nitrogen solubility in liquid cobalt K′(Co) = 0.0044 wt. %, which closely aligns with the value used in this paper K′(Co) = 0.0047 wt. %.</p><p>In [<xref ref-type="bibr" rid="cit7">7</xref>], an experimental value of \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.007 was reported.</p><p>Additionally, [<xref ref-type="bibr" rid="cit8">8</xref>] investigated the nitrogen solubility in melts of the Fe – Co system using the Sieverts method, determining an experimental estimate of the interaction coefficient at 1873 K as \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.011.</p><p>Comparing these estimates of the Langenberg interaction coefficient at T = 1873 K: \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.0072 [<xref ref-type="bibr" rid="cit5">5</xref>] and \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.007 [<xref ref-type="bibr" rid="cit7">7</xref>] are closer to the theoretical estimate \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.0076 than the experimental one \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.011 [<xref ref-type="bibr" rid="cit8">8</xref>]. Consequently, based on the theory presented in this paper, the estimates from [<xref ref-type="bibr" rid="cit5">5</xref>] and [<xref ref-type="bibr" rid="cit7">7</xref>] appear more plausible than the one described in [<xref ref-type="bibr" rid="cit8">8</xref>].</p><p> </p><p>Conclusions</p><p>Theoretical estimates for the thermodynamic first-order interaction coefficients between nitrogen and cobalt in liquid steel at T = 1873 K: \(\varepsilon _{\rm{N}}^{{\rm{Co}}}\) = 1.8; \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.0076.</p><p>The experimental estimates of the Langenberg interaction coefficient \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.0072 [<xref ref-type="bibr" rid="cit5">5</xref>] and \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.007 [<xref ref-type="bibr" rid="cit7">7</xref>] appear more credible or reliable compared to the estimate \(e_{\rm{N}}^{{\rm{Co}}}\) = 0.011 [<xref ref-type="bibr" rid="cit8">8</xref>].</p><p> </p></body><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Lupis C.H.P., Elliott J.F. 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