<p>Thermophysical properties such as density, and speed of sound of binary liquid systems of benzyl acetate (BZA) with 1-alkanols (1-propanol (PPL), 1-butanol (BTL), 1-pentanol (PTL), 1-hexanol (HXL), and 1-heptanol (HPL) at <i>T</i> = (298.15 to 308.15) K under atmospheric pressure, were reported complete composition of benzyl acetate. Using experimental data, thermodynamic properties like molar volume (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\({V}_{\text{m}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mtext>m</mtext> </msub> </math></EquationSource> </InlineEquation>), excess molar volume (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq2.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> <mrow> <mtext>m</mtext> </mrow> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation>), apparent molar volumes (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq3.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="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq4.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>), acoustic impedance (<i>Z</i>), isentropic compressibility (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\({k}_{\text{s}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>k</mi> <mtext>s</mtext> </msub> </math></EquationSource> </InlineEquation>), intermolecular free length (<i>L</i><sub>f</sub>), excess isentropic compressibility (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({k}_{\text{s}}^{\text{E}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>k</mi> <mrow> <mtext>s</mtext> </mrow> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation>), and excess intermolecular free length (<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq7.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\({L}_{\text{f}}^{\text{E}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>L</mi> <mrow> <mtext>f</mtext> </mrow> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation>) were considered. Using these data, we may forecast the formation of new molecular interactions between dissimilar components, as well as explain how temperature influences those interactions. Further, the <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10953_2025_1463_Article_IEq8.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> <mrow> <mtext>m</mtext> </mrow> <mtext>E</mtext> </msubsup> </math></EquationSource> </InlineEquation>, and <i>∆κ</i><sub>s</sub> variables were fitted using the Redlich–Kister (R–K) equation. Furthermore, the geometrical structure of the monomer and all conceivable H-bonded (molecular interaction) dimers is fully optimized using density functional theory with the Lee–Yang–Parr correlation function (B3LYP) and the 6-311++G(d, p) basis set. An extensive examination of the computational results is carried out to confirm the complex formation through H-bonding.</p>

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Thermodynamic and Computational Studies of Binary Liquid Systems of Benzyl Acetate with 1-Alcohols at Varying Temperatures

  • Ramachandra Rao Panem,
  • Sreenu Dharavath,
  • Kavitha Siddoju,
  • Satheesh Bolloju,
  • Savitha Jyostna Tangeda

摘要

Thermophysical properties such as density, and speed of sound of binary liquid systems of benzyl acetate (BZA) with 1-alkanols (1-propanol (PPL), 1-butanol (BTL), 1-pentanol (PTL), 1-hexanol (HXL), and 1-heptanol (HPL) at T = (298.15 to 308.15) K under atmospheric pressure, were reported complete composition of benzyl acetate. Using experimental data, thermodynamic properties like molar volume ( \({V}_{\text{m}}\) V m ), excess molar volume ( \({V}_{\text{m}}^\text{E}\) V m E ), apparent molar volumes ( \({V}_{\text{m},\varnothing ,1}\) V m , , 1 and \({V}_{\text{m},\varnothing ,2}\) V m , , 2 ), acoustic impedance (Z), isentropic compressibility ( \({k}_{\text{s}}\) k s ), intermolecular free length (Lf), excess isentropic compressibility ( \({k}_{\text{s}}^{\text{E}}\) k s E ), and excess intermolecular free length ( \({L}_{\text{f}}^{\text{E}}\) L f E ) were considered. Using these data, we may forecast the formation of new molecular interactions between dissimilar components, as well as explain how temperature influences those interactions. Further, the \({V}_{\text{m}}^{\text{E}}\) V m E , and ∆κs variables were fitted using the Redlich–Kister (R–K) equation. Furthermore, the geometrical structure of the monomer and all conceivable H-bonded (molecular interaction) dimers is fully optimized using density functional theory with the Lee–Yang–Parr correlation function (B3LYP) and the 6-311++G(d, p) basis set. An extensive examination of the computational results is carried out to confirm the complex formation through H-bonding.