Thermoacoustic, volumetric, and viscometric investigations in the binary mixtures of 1,4-dioxane with n-hexane or n-heptane or n-octane

Ultrasonic velocity, u , density, ρ , and viscosity, η , have been measured in the binary liquid mixture of 1,4-dioxane with n -hexane or n -heptane or n -octane at 308.15, 313.15, and 318.15 K over the entire composition range. Properties such as molar volume, V m , intermolecular free length, L f...

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Veröffentlicht in:Journal of thermal analysis and calorimetry 2016-03, Vol.123 (3), p.2241-2255
Hauptverfasser: Nayeem, Sk. Md, Kondaiah, M., Sreekanth, K., Srinivasa Reddy, M., Krishna Rao, D.
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container_issue 3
container_start_page 2241
container_title Journal of thermal analysis and calorimetry
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creator Nayeem, Sk. Md
Kondaiah, M.
Sreekanth, K.
Srinivasa Reddy, M.
Krishna Rao, D.
description Ultrasonic velocity, u , density, ρ , and viscosity, η , have been measured in the binary liquid mixture of 1,4-dioxane with n -hexane or n -heptane or n -octane at 308.15, 313.15, and 318.15 K over the entire composition range. Properties such as molar volume, V m , intermolecular free length, L f , acoustic impedance, Z , internal pressure, π i , enthalpy, Δ H , Gibb’s free energy of activation of viscous flow, Δ G ∗ , and their excess/deviation properties such as deviations in ultrasonic speed, ∆ u , viscosity, Δ η , excess molar volume, V m E , excess intermolecular free length, L f E , excess acoustic impedance, Z E , excess internal pressure, π i E , excess enthalpy, Δ H E , and excess Gibb’s free energy of activation of viscous flow, Δ G ∗ E , have been calculated from the experimental data. The calculated deviation/excess properties have been fitted to the Redlich–Kister-type polynomial equation. Partial molar volumes, ( V ¯ m,1 , V ¯ m,2 ), and excess partial molar volumes, ( V ¯ m,1 E , V ¯ m,2 E ), have also been evaluated. The observed positive and negative values of the relevant deviation/excess properties are attributed to the dominance of weak interactions (physical interactions) between the unlike molecules in the mixtures, and the strength of weak interactions follows the order: (1,4-dioxane +  n -octane) > (1,4-dioxane +  n -heptane) > (1,4-dioxane +  n -hexane). The prevailing physical interactions are found to increase with the increase in temperature. The experimental data of ultrasonic velocity and viscosity have been used to check the applicability of various velocity and viscosity theory models at all temperatures under investigation.
doi_str_mv 10.1007/s10973-015-4994-1
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Properties such as molar volume, V m , intermolecular free length, L f , acoustic impedance, Z , internal pressure, π i , enthalpy, Δ H , Gibb’s free energy of activation of viscous flow, Δ G ∗ , and their excess/deviation properties such as deviations in ultrasonic speed, ∆ u , viscosity, Δ η , excess molar volume, V m E , excess intermolecular free length, L f E , excess acoustic impedance, Z E , excess internal pressure, π i E , excess enthalpy, Δ H E , and excess Gibb’s free energy of activation of viscous flow, Δ G ∗ E , have been calculated from the experimental data. The calculated deviation/excess properties have been fitted to the Redlich–Kister-type polynomial equation. Partial molar volumes, ( V ¯ m,1 , V ¯ m,2 ), and excess partial molar volumes, ( V ¯ m,1 E , V ¯ m,2 E ), have also been evaluated. The observed positive and negative values of the relevant deviation/excess properties are attributed to the dominance of weak interactions (physical interactions) between the unlike molecules in the mixtures, and the strength of weak interactions follows the order: (1,4-dioxane +  n -octane) &gt; (1,4-dioxane +  n -heptane) &gt; (1,4-dioxane +  n -hexane). The prevailing physical interactions are found to increase with the increase in temperature. 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The observed positive and negative values of the relevant deviation/excess properties are attributed to the dominance of weak interactions (physical interactions) between the unlike molecules in the mixtures, and the strength of weak interactions follows the order: (1,4-dioxane +  n -octane) &gt; (1,4-dioxane +  n -heptane) &gt; (1,4-dioxane +  n -hexane). The prevailing physical interactions are found to increase with the increase in temperature. 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Md</creatorcontrib><creatorcontrib>Kondaiah, M.</creatorcontrib><creatorcontrib>Sreekanth, K.</creatorcontrib><creatorcontrib>Srinivasa Reddy, M.</creatorcontrib><creatorcontrib>Krishna Rao, D.</creatorcontrib><collection>CrossRef</collection><collection>Gale In Context: Science</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of thermal analysis and calorimetry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nayeem, Sk. 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Properties such as molar volume, V m , intermolecular free length, L f , acoustic impedance, Z , internal pressure, π i , enthalpy, Δ H , Gibb’s free energy of activation of viscous flow, Δ G ∗ , and their excess/deviation properties such as deviations in ultrasonic speed, ∆ u , viscosity, Δ η , excess molar volume, V m E , excess intermolecular free length, L f E , excess acoustic impedance, Z E , excess internal pressure, π i E , excess enthalpy, Δ H E , and excess Gibb’s free energy of activation of viscous flow, Δ G ∗ E , have been calculated from the experimental data. The calculated deviation/excess properties have been fitted to the Redlich–Kister-type polynomial equation. Partial molar volumes, ( V ¯ m,1 , V ¯ m,2 ), and excess partial molar volumes, ( V ¯ m,1 E , V ¯ m,2 E ), have also been evaluated. The observed positive and negative values of the relevant deviation/excess properties are attributed to the dominance of weak interactions (physical interactions) between the unlike molecules in the mixtures, and the strength of weak interactions follows the order: (1,4-dioxane +  n -octane) &gt; (1,4-dioxane +  n -heptane) &gt; (1,4-dioxane +  n -hexane). The prevailing physical interactions are found to increase with the increase in temperature. The experimental data of ultrasonic velocity and viscosity have been used to check the applicability of various velocity and viscosity theory models at all temperatures under investigation.</abstract><cop>Dordrecht</cop><pub>Springer Netherlands</pub><doi>10.1007/s10973-015-4994-1</doi><tpages>15</tpages></addata></record>
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1572-8943
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source SpringerLink Journals
subjects Acoustic impedance
Activation energy
Analytical Chemistry
Chemistry
Chemistry and Materials Science
Deviation
Dioxane
Inorganic Chemistry
Internal pressure
Investigations
Mathematical models
Measurement Science and Instrumentation
Molar volume
Physical Chemistry
Polymer Sciences
Thermodynamics
Viscosity
Viscous flow
title Thermoacoustic, volumetric, and viscometric investigations in the binary mixtures of 1,4-dioxane with n-hexane or n-heptane or n-octane
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