Velocity of sound in liquid argon at high pressures and temperatures
Measurements were made of the velocity of sound in liquid argon in the temperature range 86-146 °K and at pressures up to 65 atm. The velocity versus pressure isotherms are steeper and more curved at the higher temperatures. At any one pressure, the velocity is a smoothly decreasing function of temp...
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Veröffentlicht in: | Canadian journal of chemistry 1968-04, Vol.46 (8), p.1175-1180 |
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creator | Bowman, D. H Lim, C. C Aziz, R. A |
description | Measurements were made of the velocity of sound in liquid argon in the temperature range 86-146 °K and at pressures up to 65 atm. The velocity versus pressure isotherms are steeper and more curved at the higher temperatures. At any one pressure, the velocity is a smoothly decreasing function of temperature. Analysis of the results using existing density data showed that the specific heat ratio, γ, decreases with pressure and increases with temperature in this range. The coefficient in Rao's relation was found to increase with temperature at constant pressure, while that in the relation due to Carnevale and Litovitz exhibited no definite trend with temperature or pressure. |
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H ; Lim, C. C ; Aziz, R. A</creator><creatorcontrib>Bowman, D. H ; Lim, C. C ; Aziz, R. A</creatorcontrib><description>Measurements were made of the velocity of sound in liquid argon in the temperature range 86-146 °K and at pressures up to 65 atm. The velocity versus pressure isotherms are steeper and more curved at the higher temperatures. At any one pressure, the velocity is a smoothly decreasing function of temperature. Analysis of the results using existing density data showed that the specific heat ratio, γ, decreases with pressure and increases with temperature in this range. The coefficient in Rao's relation was found to increase with temperature at constant pressure, while that in the relation due to Carnevale and Litovitz exhibited no definite trend with temperature or pressure.</description><identifier>ISSN: 0008-4042</identifier><identifier>EISSN: 1480-3291</identifier><identifier>DOI: 10.1139/v68-201</identifier><language>eng</language><publisher>Ottawa, Canada: NRC Research Press</publisher><ispartof>Canadian journal of chemistry, 1968-04, Vol.46 (8), p.1175-1180</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c221t-35d081bbd32e5c471e9fc9cc433a5b44acd964a310534b449daa76caa397e2bd3</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://cdnsciencepub.com/doi/pdf/10.1139/v68-201$$EPDF$$P50$$Gnrcresearch$$H</linktopdf><linktohtml>$$Uhttps://cdnsciencepub.com/doi/full/10.1139/v68-201$$EHTML$$P50$$Gnrcresearch$$H</linktohtml><link.rule.ids>314,776,780,2919,27901,27902,64401,64979</link.rule.ids></links><search><creatorcontrib>Bowman, D. H</creatorcontrib><creatorcontrib>Lim, C. C</creatorcontrib><creatorcontrib>Aziz, R. A</creatorcontrib><title>Velocity of sound in liquid argon at high pressures and temperatures</title><title>Canadian journal of chemistry</title><addtitle>Revue canadienne de chimie</addtitle><description>Measurements were made of the velocity of sound in liquid argon in the temperature range 86-146 °K and at pressures up to 65 atm. The velocity versus pressure isotherms are steeper and more curved at the higher temperatures. At any one pressure, the velocity is a smoothly decreasing function of temperature. Analysis of the results using existing density data showed that the specific heat ratio, γ, decreases with pressure and increases with temperature in this range. The coefficient in Rao's relation was found to increase with temperature at constant pressure, while that in the relation due to Carnevale and Litovitz exhibited no definite trend with temperature or pressure.</description><issn>0008-4042</issn><issn>1480-3291</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1968</creationdate><recordtype>article</recordtype><recordid>eNp9j01LxDAQhoMoWFfxL-SkIETz1Y8cZf2EBS_qNUyTdBvptjVphf33Ztm96mWGd3hmmAehS0ZvGRPq7qeoCKfsCGVMVpQIrtgxyiilFZFU8lN0FuNXiiXleYYePl03GD9t8dDgOMy9xb7Hnf-evcUQ1kOPYcKtX7d4DC7GORUMiZrcZnQBpt3gHJ000EV3cegL9PH0-L58Iau359fl_YoYztlERG5pxeraCu5yI0vmVGOUMVIIyGspwVhVSBCM5kKmrCxAWRgAoUrH09oCXe_vmjDEGFyjx-A3ELaaUb2T10leJ_lE3uzJPpj0oINg2n_gq7_hA6RH24hfLDxogw</recordid><startdate>19680415</startdate><enddate>19680415</enddate><creator>Bowman, D. H</creator><creator>Lim, C. C</creator><creator>Aziz, R. A</creator><general>NRC Research Press</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19680415</creationdate><title>Velocity of sound in liquid argon at high pressures and temperatures</title><author>Bowman, D. H ; Lim, C. C ; Aziz, R. A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c221t-35d081bbd32e5c471e9fc9cc433a5b44acd964a310534b449daa76caa397e2bd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1968</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bowman, D. H</creatorcontrib><creatorcontrib>Lim, C. C</creatorcontrib><creatorcontrib>Aziz, R. A</creatorcontrib><collection>CrossRef</collection><jtitle>Canadian journal of chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bowman, D. H</au><au>Lim, C. C</au><au>Aziz, R. A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Velocity of sound in liquid argon at high pressures and temperatures</atitle><jtitle>Canadian journal of chemistry</jtitle><addtitle>Revue canadienne de chimie</addtitle><date>1968-04-15</date><risdate>1968</risdate><volume>46</volume><issue>8</issue><spage>1175</spage><epage>1180</epage><pages>1175-1180</pages><issn>0008-4042</issn><eissn>1480-3291</eissn><abstract>Measurements were made of the velocity of sound in liquid argon in the temperature range 86-146 °K and at pressures up to 65 atm. The velocity versus pressure isotherms are steeper and more curved at the higher temperatures. At any one pressure, the velocity is a smoothly decreasing function of temperature. Analysis of the results using existing density data showed that the specific heat ratio, γ, decreases with pressure and increases with temperature in this range. The coefficient in Rao's relation was found to increase with temperature at constant pressure, while that in the relation due to Carnevale and Litovitz exhibited no definite trend with temperature or pressure.</abstract><cop>Ottawa, Canada</cop><pub>NRC Research Press</pub><doi>10.1139/v68-201</doi><tpages>6</tpages></addata></record> |
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title | Velocity of sound in liquid argon at high pressures and temperatures |
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