Vapor–Liquid Equilibria Data for 2‑Piperidineethanol and 1‑(2-Hydroxyethyl)pyrrolidine in Aqueous Solutions and a UNIQUAC Model Representation
This work reports equilibrium data for two amines, 2-piperidineethanol (2-PPE) and 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), and their aqueous solutions. The pressure, temperature, and composition data are used to calculate experimental activities. Data cover temperatures from 363 to 426 K for...
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description | This work reports equilibrium data for two amines, 2-piperidineethanol (2-PPE) and 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), and their aqueous solutions. The pressure, temperature, and composition data are used to calculate experimental activities. Data cover temperatures from 363 to 426 K for the pure amines and from 323 to 373 K for the aqueous solutions. A UNIQUAC model was used to represent the binary vapor–liquid equilibria (VLE), whereas the Antoine equation was used for pure components. In an aqueous solution, the vapor pressure of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD) over the measured composition and temperature ranges is higher than that of 2-piperidineethanol (2-PPE). The developed UNIQUAC models represent the data well. For 2-piperidineethanol (2-PPE), the model gave 1.9% deviations for total pressure, 12.4% for vapor-phase composition, 12.7% for the calculated activity coefficients, and 16.2% for the excess heat capacity. In the case of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), the model was slightly more accurate, representing the data with 1.7% deviation for total pressure, 5.9% for vapor-phase composition, and 5.2% for the calculated activity coefficient. |
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The pressure, temperature, and composition data are used to calculate experimental activities. Data cover temperatures from 363 to 426 K for the pure amines and from 323 to 373 K for the aqueous solutions. A UNIQUAC model was used to represent the binary vapor–liquid equilibria (VLE), whereas the Antoine equation was used for pure components. In an aqueous solution, the vapor pressure of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD) over the measured composition and temperature ranges is higher than that of 2-piperidineethanol (2-PPE). The developed UNIQUAC models represent the data well. For 2-piperidineethanol (2-PPE), the model gave 1.9% deviations for total pressure, 12.4% for vapor-phase composition, 12.7% for the calculated activity coefficients, and 16.2% for the excess heat capacity. In the case of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), the model was slightly more accurate, representing the data with 1.7% deviation for total pressure, 5.9% for vapor-phase composition, and 5.2% for the calculated activity coefficient.</description><identifier>ISSN: 0021-9568</identifier><identifier>EISSN: 1520-5134</identifier><identifier>DOI: 10.1021/acs.jced.1c00726</identifier><identifier>PMID: 35058658</identifier><language>eng</language><publisher>United States: American Chemical Society</publisher><subject>Vapor-Liquid Equilibria and Supercritical Fluid Equilibria</subject><ispartof>Journal of chemical and engineering data, 2022-01, Vol.67 (1), p.159-166</ispartof><rights>2022 The Authors. Published by American Chemical Society</rights><rights>2022 The Authors. Published by American Chemical Society.</rights><rights>2022 The Authors. 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Chem. Eng. Data</addtitle><description>This work reports equilibrium data for two amines, 2-piperidineethanol (2-PPE) and 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), and their aqueous solutions. The pressure, temperature, and composition data are used to calculate experimental activities. Data cover temperatures from 363 to 426 K for the pure amines and from 323 to 373 K for the aqueous solutions. A UNIQUAC model was used to represent the binary vapor–liquid equilibria (VLE), whereas the Antoine equation was used for pure components. In an aqueous solution, the vapor pressure of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD) over the measured composition and temperature ranges is higher than that of 2-piperidineethanol (2-PPE). The developed UNIQUAC models represent the data well. For 2-piperidineethanol (2-PPE), the model gave 1.9% deviations for total pressure, 12.4% for vapor-phase composition, 12.7% for the calculated activity coefficients, and 16.2% for the excess heat capacity. In the case of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), the model was slightly more accurate, representing the data with 1.7% deviation for total pressure, 5.9% for vapor-phase composition, and 5.2% for the calculated activity coefficient.</description><subject>Vapor-Liquid Equilibria and Supercritical Fluid Equilibria</subject><issn>0021-9568</issn><issn>1520-5134</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp1kc1u1DAUhS0EotOWPSvkZZGawXZij2eDNBoKrTRA-Rm21k3sUFeeOLUTRHZ9BQRP2CfBmRkqWLCxF_c75_4chJ5SMqWE0RdQxel1ZfSUVoTMmHiAJpQzknGaFw_RhCQmm3MhD9BhjNeEkGLG6GN0kHPCpeBygn59gdaHu9ufK3vTW43P0utsGSzgV9ABrn3A7O72x6VtTbDaNsZ0V9B4h6HRmKbKCcvOBx389yFVBve8HULwboti2-DFTW98H_En7_rO-iZuhYDX7y4-rBdL_NZr4_BH0wYTTdPByByjRzW4aJ7s_yO0fn32eXmerd6_uVguVhkUed5l-Zyx2VwWnJc14XUFtaRM1jIvqoKSkuqiYOV4mboUOTVc88qApkCBlEKIIj9CL3e-bV9ujK5S_wBOtcFuIAzKg1X_Vhp7pb76b0rOBBMiTwYne4Pg056xUxsbK-McNOPSignGmGRSkISSHVoFH2Mw9X0bStQYpkphqjFMtQ8zSZ79Pd694E96CTjdAVup70OTrvV_v98GKLDA</recordid><startdate>20220113</startdate><enddate>20220113</enddate><creator>Hartono, Ardi</creator><creator>Nøkleby, Christina</creator><creator>Kim, Inna</creator><creator>Knuutila, Hanna K</creator><general>American Chemical Society</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0003-2057-1743</orcidid><orcidid>https://orcid.org/0000-0003-1764-1034</orcidid></search><sort><creationdate>20220113</creationdate><title>Vapor–Liquid Equilibria Data for 2‑Piperidineethanol and 1‑(2-Hydroxyethyl)pyrrolidine in Aqueous Solutions and a UNIQUAC Model Representation</title><author>Hartono, Ardi ; Nøkleby, Christina ; Kim, Inna ; Knuutila, Hanna K</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a433t-3922798455bf05fcaf8128f834c410b1d442b1c00fb631e5d5cead1a1a0b66643</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Vapor-Liquid Equilibria and Supercritical Fluid Equilibria</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hartono, Ardi</creatorcontrib><creatorcontrib>Nøkleby, Christina</creatorcontrib><creatorcontrib>Kim, Inna</creatorcontrib><creatorcontrib>Knuutila, Hanna K</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Journal of chemical and engineering data</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hartono, Ardi</au><au>Nøkleby, Christina</au><au>Kim, Inna</au><au>Knuutila, Hanna K</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Vapor–Liquid Equilibria Data for 2‑Piperidineethanol and 1‑(2-Hydroxyethyl)pyrrolidine in Aqueous Solutions and a UNIQUAC Model Representation</atitle><jtitle>Journal of chemical and engineering data</jtitle><addtitle>J. Chem. Eng. Data</addtitle><date>2022-01-13</date><risdate>2022</risdate><volume>67</volume><issue>1</issue><spage>159</spage><epage>166</epage><pages>159-166</pages><issn>0021-9568</issn><eissn>1520-5134</eissn><abstract>This work reports equilibrium data for two amines, 2-piperidineethanol (2-PPE) and 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), and their aqueous solutions. The pressure, temperature, and composition data are used to calculate experimental activities. Data cover temperatures from 363 to 426 K for the pure amines and from 323 to 373 K for the aqueous solutions. A UNIQUAC model was used to represent the binary vapor–liquid equilibria (VLE), whereas the Antoine equation was used for pure components. In an aqueous solution, the vapor pressure of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD) over the measured composition and temperature ranges is higher than that of 2-piperidineethanol (2-PPE). The developed UNIQUAC models represent the data well. For 2-piperidineethanol (2-PPE), the model gave 1.9% deviations for total pressure, 12.4% for vapor-phase composition, 12.7% for the calculated activity coefficients, and 16.2% for the excess heat capacity. In the case of 1-(2-hydroxyethyl)pyrrolidine (1-(2HE)PRLD), the model was slightly more accurate, representing the data with 1.7% deviation for total pressure, 5.9% for vapor-phase composition, and 5.2% for the calculated activity coefficient.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>35058658</pmid><doi>10.1021/acs.jced.1c00726</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0003-2057-1743</orcidid><orcidid>https://orcid.org/0000-0003-1764-1034</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Vapor-Liquid Equilibria and Supercritical Fluid Equilibria |
title | Vapor–Liquid Equilibria Data for 2‑Piperidineethanol and 1‑(2-Hydroxyethyl)pyrrolidine in Aqueous Solutions and a UNIQUAC Model Representation |
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