<p>Thermophysical properties such as density (<i>ρ</i>), and viscosity (<i>η</i>) of pure components and binary mixtures of pyridine (PY) with 2-alcohols viz., 2-propanol (2-PPL), 2-butanol (2-BTL), and 2-pentanol (2-PTL) were measured over the entire range of composition of pyridine at varying temperatures <i>T</i>&#xa0;=&#xa0;(298.15, 303.15 and 308.15) K and at pressure 0.1&#xa0;MPa. Using measured data, excess molar volume (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\({V}_\text{m}^\text{E}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>V</mi> <mtext>m</mtext> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation>), and viscosity variation (∆<i>η</i>) were derived and correlated to the Redlich–Kister (R–K) polynomial equation. Further, the apparent molar volumes (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\({V}_{\text m,\varnothing ,1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mrow> <mtext>m</mtext> <mo>,</mo> <mi>∅</mi> <mo>,</mo> <mn>1</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\({V}_{\text m,\varnothing ,2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mrow> <mtext>m</mtext> <mo>,</mo> <mi>∅</mi> <mo>,</mo> <mn>2</mn> </mrow> </msub> </math></EquationSource> </InlineEquation>), partial molar volumes (<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq4.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\({\overline{V} }_{\text m,1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi>V</mi> <mo>¯</mo> </mover> <mrow> <mtext>m</mtext> <mo>,</mo> <mn>1</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq5.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\({\overline{V} }_{\text m,2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi>V</mi> <mo>¯</mo> </mover> <mrow> <mtext>m</mtext> <mo>,</mo> <mn>2</mn> </mrow> </msub> </math></EquationSource> </InlineEquation>), and excess partial molar volumes (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq6.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\({\overline{V} }_{\text m,1}^{\text E}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mover> <mi>V</mi> <mo>¯</mo> </mover> <mrow> <mtext>m</mtext> <mo>,</mo> <mn>1</mn> </mrow> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq7.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\({\overline{V} }_{\text m,2}^{\text E}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mover> <mi>V</mi> <mo>¯</mo> </mover> <mrow> <mtext>m</mtext> <mo>,</mo> <mn>2</mn> </mrow> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation>) values were also derived. These characteristics are employed to explain the emergence of new intermolecular interactions (H-bonding, packing efficiency, and OH–π interaction) between dissimilar molecules. Over the whole range of pyridine composition, the <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1473_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\({V}_\text{m}^\text{E}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>V</mi> <mtext>m</mtext> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation> values showed a negative trend, while the ∆<i>η</i> values showed a positive trend. Furthermore, using thermodynamic results, discuss about how temperature affects molecular interactions between molecules.</p>

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Thermodynamic Properties of Binary Liquid Systems of Pyridine and 2-Alcohols at Varying Temperatures

  • Razia Shamshad Begum,
  • Donthula Sumalatha,
  • Kasturi Srinivas,
  • Jagadeesh Kumar Ega

摘要

Thermophysical properties such as density (ρ), and viscosity (η) of pure components and binary mixtures of pyridine (PY) with 2-alcohols viz., 2-propanol (2-PPL), 2-butanol (2-BTL), and 2-pentanol (2-PTL) were measured over the entire range of composition of pyridine at varying temperatures T = (298.15, 303.15 and 308.15) K and at pressure 0.1 MPa. Using measured data, excess molar volume ( \({V}_\text{m}^\text{E}\) V m E ), and viscosity variation (∆η) were derived and correlated to the Redlich–Kister (R–K) polynomial equation. Further, the apparent molar volumes ( \({V}_{\text m,\varnothing ,1}\) V m , , 1 and \({V}_{\text m,\varnothing ,2}\) V m , , 2 ), partial molar volumes ( \({\overline{V} }_{\text m,1}\) V ¯ m , 1 and \({\overline{V} }_{\text m,2}\) V ¯ m , 2 ), and excess partial molar volumes ( \({\overline{V} }_{\text m,1}^{\text E}\) V ¯ m , 1 E and \({\overline{V} }_{\text m,2}^{\text E}\) V ¯ m , 2 E ) values were also derived. These characteristics are employed to explain the emergence of new intermolecular interactions (H-bonding, packing efficiency, and OH–π interaction) between dissimilar molecules. Over the whole range of pyridine composition, the \({V}_\text{m}^\text{E}\) V m E values showed a negative trend, while the ∆η values showed a positive trend. Furthermore, using thermodynamic results, discuss about how temperature affects molecular interactions between molecules.