Measurement of Critical Temperatures, Critical Pressures and Densities of Acetone–Water Solutions for Simulation
Critical temperature, critical pressure and P–T–ρ–X data of acetone–water solutions with water mole fractions in a range of 0–60% were measured to provide fundamental data for CFD simulations. Critical temperatures were determined via observing critical opalescence in fused quartz capillary tubes. M...
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Veröffentlicht in: | Journal of solution chemistry 2023-12, Vol.52 (12), p.1331-1351 |
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creator | Chen, Zhirong Yao, Yang Yuan, Shenfeng Yin, Hong |
description | Critical temperature, critical pressure and
P–T–ρ–X
data of acetone–water solutions with water mole fractions in a range of 0–60% were measured to provide fundamental data for CFD simulations. Critical temperatures were determined via observing critical opalescence in fused quartz capillary tubes. Meanwhile, critical pressures were measured by heating acetone–water solutions to its critical temperature in an autoclave. The standard deviations of critical temperature and critical pressure were 0.55 K and 0.029 MPa, respectively. The results indicate that only one phase exists during mixing of acetone with water. Moreover,
P–T–ρ–X
data under 15 and 20 MPa in the temperature range of 460–550 K were measured in the autoclave. The relative deviation of density was 0.32%. Volume-translated Peng-Robinson and Soave–Redlich–Kwong state equations were used to illustrate the
P–V–T–X
relationship of acetone–water solutions, and the Peng–Robinson state equation with an average absolute relative deviation of 1.19% between fitting and experimental densities was found more accurate. |
doi_str_mv | 10.1007/s10953-023-01320-0 |
format | Article |
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P–T–ρ–X
data of acetone–water solutions with water mole fractions in a range of 0–60% were measured to provide fundamental data for CFD simulations. Critical temperatures were determined via observing critical opalescence in fused quartz capillary tubes. Meanwhile, critical pressures were measured by heating acetone–water solutions to its critical temperature in an autoclave. The standard deviations of critical temperature and critical pressure were 0.55 K and 0.029 MPa, respectively. The results indicate that only one phase exists during mixing of acetone with water. Moreover,
P–T–ρ–X
data under 15 and 20 MPa in the temperature range of 460–550 K were measured in the autoclave. The relative deviation of density was 0.32%. Volume-translated Peng-Robinson and Soave–Redlich–Kwong state equations were used to illustrate the
P–V–T–X
relationship of acetone–water solutions, and the Peng–Robinson state equation with an average absolute relative deviation of 1.19% between fitting and experimental densities was found more accurate.</description><identifier>ISSN: 0095-9782</identifier><identifier>EISSN: 1572-8927</identifier><identifier>DOI: 10.1007/s10953-023-01320-0</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Acetone ; Autoclaves ; Capillary pressure ; Capillary tubes ; Chemistry ; Chemistry and Materials Science ; Condensed Matter Physics ; Critical pressure ; Critical temperature ; Equations of state ; Fused quartz ; Geochemistry ; Industrial Chemistry/Chemical Engineering ; Inorganic Chemistry ; Oceanography ; Opalescence ; Physical Chemistry ; Temperature ; Transition temperature</subject><ispartof>Journal of solution chemistry, 2023-12, Vol.52 (12), p.1331-1351</ispartof><rights>The Author(s) 2023</rights><rights>The Author(s) 2023. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c314t-9c546c20413e67a31a0d12b914ccb40337c11d62a89a3ed58e189c74dc6dc6873</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s10953-023-01320-0$$EPDF$$P50$$Gspringer$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s10953-023-01320-0$$EHTML$$P50$$Gspringer$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Chen, Zhirong</creatorcontrib><creatorcontrib>Yao, Yang</creatorcontrib><creatorcontrib>Yuan, Shenfeng</creatorcontrib><creatorcontrib>Yin, Hong</creatorcontrib><title>Measurement of Critical Temperatures, Critical Pressures and Densities of Acetone–Water Solutions for Simulation</title><title>Journal of solution chemistry</title><addtitle>J Solution Chem</addtitle><description>Critical temperature, critical pressure and
P–T–ρ–X
data of acetone–water solutions with water mole fractions in a range of 0–60% were measured to provide fundamental data for CFD simulations. Critical temperatures were determined via observing critical opalescence in fused quartz capillary tubes. Meanwhile, critical pressures were measured by heating acetone–water solutions to its critical temperature in an autoclave. The standard deviations of critical temperature and critical pressure were 0.55 K and 0.029 MPa, respectively. The results indicate that only one phase exists during mixing of acetone with water. Moreover,
P–T–ρ–X
data under 15 and 20 MPa in the temperature range of 460–550 K were measured in the autoclave. The relative deviation of density was 0.32%. Volume-translated Peng-Robinson and Soave–Redlich–Kwong state equations were used to illustrate the
P–V–T–X
relationship of acetone–water solutions, and the Peng–Robinson state equation with an average absolute relative deviation of 1.19% between fitting and experimental densities was found more accurate.</description><subject>Acetone</subject><subject>Autoclaves</subject><subject>Capillary pressure</subject><subject>Capillary tubes</subject><subject>Chemistry</subject><subject>Chemistry and Materials Science</subject><subject>Condensed Matter Physics</subject><subject>Critical pressure</subject><subject>Critical temperature</subject><subject>Equations of state</subject><subject>Fused quartz</subject><subject>Geochemistry</subject><subject>Industrial Chemistry/Chemical Engineering</subject><subject>Inorganic Chemistry</subject><subject>Oceanography</subject><subject>Opalescence</subject><subject>Physical Chemistry</subject><subject>Temperature</subject><subject>Transition temperature</subject><issn>0095-9782</issn><issn>1572-8927</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><recordid>eNp9kM1KxDAUhYMoOI6-gKuAW6v5aZtkOYy_MKLgiMuQSW-lQ9uMSbpw5zv4hj6JGSvMTkgIX84598JB6JSSC0qIuAyUqIJnhKVLOSMZ2UMTWgiWScXEPpqQpGdKSHaIjkJYk8RS5RPkH8CEwUMHfcSuxnPfxMaaFi-h24A3MWnhfPf9lHDrD9j0Fb6CPiQhUYrOLETXw_fn16uJ4PGza4fYuD7g2iVquqE1Wz5GB7VpA5z8vVP0cnO9nN9li8fb-_lskVlO85gpW-SlZSSnHEphODWkomylaG7tKiecC0tpVTIjleFQFRKoVFbklS3TkYJP0dk4d-Pd-wAh6rUbfJ9WaiaFoEUpGEsuNrqsdyF4qPXGN53xH5oSve1Wj93q1K3-7VaTFOJjKCRz_wZ-N_qf1A_8Bn5h</recordid><startdate>20231201</startdate><enddate>20231201</enddate><creator>Chen, Zhirong</creator><creator>Yao, Yang</creator><creator>Yuan, Shenfeng</creator><creator>Yin, Hong</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20231201</creationdate><title>Measurement of Critical Temperatures, Critical Pressures and Densities of Acetone–Water Solutions for Simulation</title><author>Chen, Zhirong ; Yao, Yang ; Yuan, Shenfeng ; Yin, Hong</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c314t-9c546c20413e67a31a0d12b914ccb40337c11d62a89a3ed58e189c74dc6dc6873</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Acetone</topic><topic>Autoclaves</topic><topic>Capillary pressure</topic><topic>Capillary tubes</topic><topic>Chemistry</topic><topic>Chemistry and Materials Science</topic><topic>Condensed Matter Physics</topic><topic>Critical pressure</topic><topic>Critical temperature</topic><topic>Equations of state</topic><topic>Fused quartz</topic><topic>Geochemistry</topic><topic>Industrial Chemistry/Chemical Engineering</topic><topic>Inorganic Chemistry</topic><topic>Oceanography</topic><topic>Opalescence</topic><topic>Physical Chemistry</topic><topic>Temperature</topic><topic>Transition temperature</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chen, Zhirong</creatorcontrib><creatorcontrib>Yao, Yang</creatorcontrib><creatorcontrib>Yuan, Shenfeng</creatorcontrib><creatorcontrib>Yin, Hong</creatorcontrib><collection>Springer Nature OA Free Journals</collection><collection>CrossRef</collection><jtitle>Journal of solution chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chen, Zhirong</au><au>Yao, Yang</au><au>Yuan, Shenfeng</au><au>Yin, Hong</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Measurement of Critical Temperatures, Critical Pressures and Densities of Acetone–Water Solutions for Simulation</atitle><jtitle>Journal of solution chemistry</jtitle><stitle>J Solution Chem</stitle><date>2023-12-01</date><risdate>2023</risdate><volume>52</volume><issue>12</issue><spage>1331</spage><epage>1351</epage><pages>1331-1351</pages><issn>0095-9782</issn><eissn>1572-8927</eissn><abstract>Critical temperature, critical pressure and
P–T–ρ–X
data of acetone–water solutions with water mole fractions in a range of 0–60% were measured to provide fundamental data for CFD simulations. Critical temperatures were determined via observing critical opalescence in fused quartz capillary tubes. Meanwhile, critical pressures were measured by heating acetone–water solutions to its critical temperature in an autoclave. The standard deviations of critical temperature and critical pressure were 0.55 K and 0.029 MPa, respectively. The results indicate that only one phase exists during mixing of acetone with water. Moreover,
P–T–ρ–X
data under 15 and 20 MPa in the temperature range of 460–550 K were measured in the autoclave. The relative deviation of density was 0.32%. Volume-translated Peng-Robinson and Soave–Redlich–Kwong state equations were used to illustrate the
P–V–T–X
relationship of acetone–water solutions, and the Peng–Robinson state equation with an average absolute relative deviation of 1.19% between fitting and experimental densities was found more accurate.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10953-023-01320-0</doi><tpages>21</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Acetone Autoclaves Capillary pressure Capillary tubes Chemistry Chemistry and Materials Science Condensed Matter Physics Critical pressure Critical temperature Equations of state Fused quartz Geochemistry Industrial Chemistry/Chemical Engineering Inorganic Chemistry Oceanography Opalescence Physical Chemistry Temperature Transition temperature |
title | Measurement of Critical Temperatures, Critical Pressures and Densities of Acetone–Water Solutions for Simulation |
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