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Equation of state of initially liquid carbon monoxide and nitrogen mixture
The modified liquid perturbation variational theory and the improved vdW-1f model were applied to calculating the equation of the state of liquid CO-N 2 mixture with the ratio of 1:1, 4:1 and 1:4, respectively, in the shock pressure range of 9–49 GPa. It was shown that the calculated result for CO-N...
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Published in: | Science China. Physics, mechanics & astronomy mechanics & astronomy, 2008-06, Vol.51 (6), p.599-606 |
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creator | Yang, JinWen Sun, Dong Sun, Yue Shi, ShangChun |
description | The modified liquid perturbation variational theory and the improved vdW-1f model were applied to calculating the equation of the state of liquid CO-N
2
mixture with the ratio of 1:1, 4:1 and 1:4, respectively, in the shock pressure range of 9–49 GPa. It was shown that the calculated result for CO-N
2
mixture with the ratio of 1:1 is well consistent with the earlier experimental data. The thermodynamics equilibrium, chemical equilibrium and phase equilibrium were all considered in detail. It was found that Hugoniot of liquid CO-N
2
mixture is moderately softened in the pressure range of 20–30 GPa and 30–49 GPa for different initial proportions, and that the Hugoniot is more softened in the latter pressure range, which means that the structural phase transition occurs near 20 GPa and 30 GPa. Since the shock productions may absorb a plenty of systematic energy, the shock temperature and pressure decline compared with the case of no chemical reaction. Pressures and temperatures increase gradually with the increase in the mole fraction of nitrogen composition. The results for the 1:1 CO-N
2
mixture lie in the middle of two others. Therefore, it was shown that the modified Lorentz-Berthelor rule used in the scheme is effective to study shock-compression properties of liquid CO-N
2
mixture under high temperatures and high pressures. |
doi_str_mv | 10.1007/s11433-008-0068-8 |
format | article |
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2
mixture with the ratio of 1:1, 4:1 and 1:4, respectively, in the shock pressure range of 9–49 GPa. It was shown that the calculated result for CO-N
2
mixture with the ratio of 1:1 is well consistent with the earlier experimental data. The thermodynamics equilibrium, chemical equilibrium and phase equilibrium were all considered in detail. It was found that Hugoniot of liquid CO-N
2
mixture is moderately softened in the pressure range of 20–30 GPa and 30–49 GPa for different initial proportions, and that the Hugoniot is more softened in the latter pressure range, which means that the structural phase transition occurs near 20 GPa and 30 GPa. Since the shock productions may absorb a plenty of systematic energy, the shock temperature and pressure decline compared with the case of no chemical reaction. Pressures and temperatures increase gradually with the increase in the mole fraction of nitrogen composition. The results for the 1:1 CO-N
2
mixture lie in the middle of two others. Therefore, it was shown that the modified Lorentz-Berthelor rule used in the scheme is effective to study shock-compression properties of liquid CO-N
2
mixture under high temperatures and high pressures.</description><identifier>ISSN: 1672-1799</identifier><identifier>ISSN: 1674-7348</identifier><identifier>EISSN: 1862-2844</identifier><identifier>EISSN: 1869-1927</identifier><identifier>DOI: 10.1007/s11433-008-0068-8</identifier><language>eng</language><publisher>Heidelberg: SP Science in China Press</publisher><subject>Astronomy ; Carbon monoxide ; Chemical reactions ; Classical and Continuum Physics ; Compressive properties ; Equations of state ; Equilibrium ; High temperature ; Mixtures ; Nitrogen ; Observations and Techniques ; Phase equilibria ; Phase transitions ; Physics ; Physics and Astronomy ; Thermodynamic equilibrium</subject><ispartof>Science China. Physics, mechanics & astronomy, 2008-06, Vol.51 (6), p.599-606</ispartof><rights>Science in China Press and Springer-Verlag GmbH 2008</rights><rights>Science in China Press and Springer-Verlag GmbH 2008.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c299t-547b3343e07f6f23a4e01691b3f5a26f148dde5113902a06823518086c06e4393</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Yang, JinWen</creatorcontrib><creatorcontrib>Sun, Dong</creatorcontrib><creatorcontrib>Sun, Yue</creatorcontrib><creatorcontrib>Shi, ShangChun</creatorcontrib><title>Equation of state of initially liquid carbon monoxide and nitrogen mixture</title><title>Science China. Physics, mechanics & astronomy</title><addtitle>Sci. China Ser. G-Phys. Mech. Astron</addtitle><description>The modified liquid perturbation variational theory and the improved vdW-1f model were applied to calculating the equation of the state of liquid CO-N
2
mixture with the ratio of 1:1, 4:1 and 1:4, respectively, in the shock pressure range of 9–49 GPa. It was shown that the calculated result for CO-N
2
mixture with the ratio of 1:1 is well consistent with the earlier experimental data. The thermodynamics equilibrium, chemical equilibrium and phase equilibrium were all considered in detail. It was found that Hugoniot of liquid CO-N
2
mixture is moderately softened in the pressure range of 20–30 GPa and 30–49 GPa for different initial proportions, and that the Hugoniot is more softened in the latter pressure range, which means that the structural phase transition occurs near 20 GPa and 30 GPa. Since the shock productions may absorb a plenty of systematic energy, the shock temperature and pressure decline compared with the case of no chemical reaction. Pressures and temperatures increase gradually with the increase in the mole fraction of nitrogen composition. The results for the 1:1 CO-N
2
mixture lie in the middle of two others. Therefore, it was shown that the modified Lorentz-Berthelor rule used in the scheme is effective to study shock-compression properties of liquid CO-N
2
mixture under high temperatures and high pressures.</description><subject>Astronomy</subject><subject>Carbon monoxide</subject><subject>Chemical reactions</subject><subject>Classical and Continuum Physics</subject><subject>Compressive properties</subject><subject>Equations of state</subject><subject>Equilibrium</subject><subject>High temperature</subject><subject>Mixtures</subject><subject>Nitrogen</subject><subject>Observations and Techniques</subject><subject>Phase equilibria</subject><subject>Phase transitions</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Thermodynamic equilibrium</subject><issn>1672-1799</issn><issn>1674-7348</issn><issn>1862-2844</issn><issn>1869-1927</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNp1kFFLwzAQx4MoOOY-gG8FwbdqLpemyaOM6ZSBL_oc0jYdka7Zkha2b29GBUHw4bgj_P7H5UfILdAHoLR8jAAcMadUphIylxdkBlKwnEnOL9MsSpZDqdQ1WcToKoqAyISgM_K2OoxmcL7PfJvFwQz2PLjeDc503Snr3GF0TVabUCVm53t_dI3NTN9kiQl-a9OrOw5jsDfkqjVdtIufPiefz6uP5TrfvL-8Lp82ec2UGvKClxUiR0vLVrQMDbcUhIIK28Iw0QKXTWMLAFSUmfQdhgVIKkVNheWocE7up7374A-jjYPeuVjbrjO99WPUiIUEUZQJvPsDfvkx9Ok2zRTIohQiaZsTmKg6-BiDbfU-uJ0JJw1Un_XqSa9OevVZr5Ypw6ZMTGy_teF38_-hb6nJeyU</recordid><startdate>20080601</startdate><enddate>20080601</enddate><creator>Yang, JinWen</creator><creator>Sun, Dong</creator><creator>Sun, Yue</creator><creator>Shi, ShangChun</creator><general>SP Science in China Press</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>P5Z</scope><scope>P62</scope><scope>PCBAR</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PTHSS</scope><scope>7TB</scope><scope>7U5</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>20080601</creationdate><title>Equation of state of initially liquid carbon monoxide and nitrogen mixture</title><author>Yang, JinWen ; Sun, Dong ; Sun, Yue ; Shi, ShangChun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c299t-547b3343e07f6f23a4e01691b3f5a26f148dde5113902a06823518086c06e4393</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>Astronomy</topic><topic>Carbon monoxide</topic><topic>Chemical reactions</topic><topic>Classical and Continuum Physics</topic><topic>Compressive properties</topic><topic>Equations of state</topic><topic>Equilibrium</topic><topic>High temperature</topic><topic>Mixtures</topic><topic>Nitrogen</topic><topic>Observations and Techniques</topic><topic>Phase equilibria</topic><topic>Phase transitions</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Thermodynamic equilibrium</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yang, JinWen</creatorcontrib><creatorcontrib>Sun, Dong</creatorcontrib><creatorcontrib>Sun, Yue</creatorcontrib><creatorcontrib>Shi, ShangChun</creatorcontrib><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest One Sustainability</collection><collection>ProQuest Central</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>Natural Science Collection</collection><collection>Earth, Atmospheric & Aquatic Science Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>ProQuest advanced technologies & aerospace journals</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Earth, Atmospheric & Aquatic Science Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Engineering collection</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Science China. Physics, mechanics & astronomy</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yang, JinWen</au><au>Sun, Dong</au><au>Sun, Yue</au><au>Shi, ShangChun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Equation of state of initially liquid carbon monoxide and nitrogen mixture</atitle><jtitle>Science China. Physics, mechanics & astronomy</jtitle><stitle>Sci. China Ser. G-Phys. Mech. Astron</stitle><date>2008-06-01</date><risdate>2008</risdate><volume>51</volume><issue>6</issue><spage>599</spage><epage>606</epage><pages>599-606</pages><issn>1672-1799</issn><issn>1674-7348</issn><eissn>1862-2844</eissn><eissn>1869-1927</eissn><abstract>The modified liquid perturbation variational theory and the improved vdW-1f model were applied to calculating the equation of the state of liquid CO-N
2
mixture with the ratio of 1:1, 4:1 and 1:4, respectively, in the shock pressure range of 9–49 GPa. It was shown that the calculated result for CO-N
2
mixture with the ratio of 1:1 is well consistent with the earlier experimental data. The thermodynamics equilibrium, chemical equilibrium and phase equilibrium were all considered in detail. It was found that Hugoniot of liquid CO-N
2
mixture is moderately softened in the pressure range of 20–30 GPa and 30–49 GPa for different initial proportions, and that the Hugoniot is more softened in the latter pressure range, which means that the structural phase transition occurs near 20 GPa and 30 GPa. Since the shock productions may absorb a plenty of systematic energy, the shock temperature and pressure decline compared with the case of no chemical reaction. Pressures and temperatures increase gradually with the increase in the mole fraction of nitrogen composition. The results for the 1:1 CO-N
2
mixture lie in the middle of two others. Therefore, it was shown that the modified Lorentz-Berthelor rule used in the scheme is effective to study shock-compression properties of liquid CO-N
2
mixture under high temperatures and high pressures.</abstract><cop>Heidelberg</cop><pub>SP Science in China Press</pub><doi>10.1007/s11433-008-0068-8</doi><tpages>8</tpages></addata></record> |
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subjects | Astronomy Carbon monoxide Chemical reactions Classical and Continuum Physics Compressive properties Equations of state Equilibrium High temperature Mixtures Nitrogen Observations and Techniques Phase equilibria Phase transitions Physics Physics and Astronomy Thermodynamic equilibrium |
title | Equation of state of initially liquid carbon monoxide and nitrogen mixture |
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