<p>The cross second virial coefficients <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10765_2025_3524_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>12</mn> </msub> </math></EquationSource> </InlineEquation> for interactions of molecular nitrogen (N<sub>2</sub>) with molecular hydrogen (H<sub>2</sub>), of molecular oxygen (O<sub>2</sub>) with H<sub>2</sub>, and of carbon dioxide (CO<sub>2</sub>) with H<sub>2</sub> were obtained at temperatures ranging from 36 K to 2000 K for the former two systems and from 100 K to 2000 K for the latter system from new rigid-rotor intermolecular potential energy surfaces (PESs) for the three molecule pairs. Each PES is based on interaction energies calculated for a large number of pair configurations employing high-level quantum-chemical <i>ab initio</i> methods up to coupled cluster with single, double, triple, and perturbative quadruple excitations [CCSDT(Q)]. Core-core and core-valance correlation and relativistic effects were accounted for as well. <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10765_2025_3524_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>12</mn> </msub> </math></EquationSource> </InlineEquation> values were extracted from the PESs classically and semiclassically using the Mayer-sampling Monte Carlo approach. The deficiencies of the semiclassical calculations at the lowest temperatures were partly remedied by a more rigorous treatment of translational quantum effects using the phase-shift method. The results for the N<sub>2</sub>–H<sub>2</sub> and CO<sub>2</sub>–H<sub>2</sub> systems are in excellent agreement with the most accurate experimental data. For the O<sub>2</sub>–H<sub>2</sub> system, there are no experimental <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10765_2025_3524_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>12</mn> </msub> </math></EquationSource> </InlineEquation> data because this mixture is highly explosive. There are, however, previous first-principles results for <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10765_2025_3524_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>12</mn> </msub> </math></EquationSource> </InlineEquation> of this system by Van Tat and Deiters [Chem. Phys. <b>457</b>, 171–179 (2015)], which were obtained at a much lower level of sophistication for both the PES and the method to extract <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10765_2025_3524_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>12</mn> </msub> </math></EquationSource> </InlineEquation> and differ significantly from the present <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10765_2025_3524_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>B</mi> <mn>12</mn> </msub> </math></EquationSource> </InlineEquation> values.</p>

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Cross Second Virial Coefficients of the N2–H2, O2–H2, and CO2–H2 Systems from First Principles

  • Robert Hellmann,
  • Eckard Bich

摘要

The cross second virial coefficients \(B_{12}\) B 12 for interactions of molecular nitrogen (N2) with molecular hydrogen (H2), of molecular oxygen (O2) with H2, and of carbon dioxide (CO2) with H2 were obtained at temperatures ranging from 36 K to 2000 K for the former two systems and from 100 K to 2000 K for the latter system from new rigid-rotor intermolecular potential energy surfaces (PESs) for the three molecule pairs. Each PES is based on interaction energies calculated for a large number of pair configurations employing high-level quantum-chemical ab initio methods up to coupled cluster with single, double, triple, and perturbative quadruple excitations [CCSDT(Q)]. Core-core and core-valance correlation and relativistic effects were accounted for as well. \(B_{12}\) B 12 values were extracted from the PESs classically and semiclassically using the Mayer-sampling Monte Carlo approach. The deficiencies of the semiclassical calculations at the lowest temperatures were partly remedied by a more rigorous treatment of translational quantum effects using the phase-shift method. The results for the N2–H2 and CO2–H2 systems are in excellent agreement with the most accurate experimental data. For the O2–H2 system, there are no experimental \(B_{12}\) B 12 data because this mixture is highly explosive. There are, however, previous first-principles results for \(B_{12}\) B 12 of this system by Van Tat and Deiters [Chem. Phys. 457, 171–179 (2015)], which were obtained at a much lower level of sophistication for both the PES and the method to extract \(B_{12}\) B 12 and differ significantly from the present \(B_{12}\) B 12 values.