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When do we need attractive-repulsive intermolecular potentials?
The role of attractive-repulsive interactions in direct simulation Monte Carlo (DSMC) simulations is studied by comparing with traditional purely repulsive interactions. The larger collision cross section of the long-range LJ potential is shown to result in a higher collision frequency and hence a l...
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description | The role of attractive-repulsive interactions in direct simulation Monte Carlo (DSMC) simulations is studied by comparing with traditional purely repulsive interactions. The larger collision cross section of the long-range LJ potential is shown to result in a higher collision frequency and hence a lower mean free path, by at least a factor of two, for given conditions. This results in a faster relaxation to equilibrium as is shown by comparing the fourth and sixth moments of the molecular velocity distribution obtained using 0-D DSMC simulations. A 1-D Fourier-Couette flow with a large temperature and velocity difference between the walls is used to show that matching transport properties will result in identical solutions using both LJPA and VSS models in the near-continuum regime. However, flows in the transitional regime with Knudsen number, Kn ∼ 0.5 show a dependence on the intermolecular potential in spite of matching the viscosity coefficient due to differences in the collision frequency. Attractive-repulsive potentials should be used when both transport coefficients and collision frequencies should be matched. |
doi_str_mv | 10.1063/1.4902583 |
format | conference_proceeding |
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The larger collision cross section of the long-range LJ potential is shown to result in a higher collision frequency and hence a lower mean free path, by at least a factor of two, for given conditions. This results in a faster relaxation to equilibrium as is shown by comparing the fourth and sixth moments of the molecular velocity distribution obtained using 0-D DSMC simulations. A 1-D Fourier-Couette flow with a large temperature and velocity difference between the walls is used to show that matching transport properties will result in identical solutions using both LJPA and VSS models in the near-continuum regime. However, flows in the transitional regime with Knudsen number, Kn ∼ 0.5 show a dependence on the intermolecular potential in spite of matching the viscosity coefficient due to differences in the collision frequency. Attractive-repulsive potentials should be used when both transport coefficients and collision frequencies should be matched.</description><identifier>ISSN: 0094-243X</identifier><identifier>EISSN: 1551-7616</identifier><identifier>DOI: 10.1063/1.4902583</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS ; COMPARATIVE EVALUATIONS ; Computer simulation ; COMPUTERIZED SIMULATION ; COUETTE FLOW ; CROSS SECTIONS ; Dependence ; Direct simulation Monte Carlo method ; EQUILIBRIUM ; INTERMOLECULAR FORCES ; KNUDSEN FLOW ; Matching ; MATHEMATICAL SOLUTIONS ; MEAN FREE PATH ; MONTE CARLO METHOD ; POTENTIALS ; RELAXATION ; Transport properties ; VELOCITY ; Velocity distribution ; VISCOSITY</subject><ispartof>AIP Conference Proceedings, 2014, Vol.1628 (1), p.130</ispartof><rights>2014 AIP Publishing LLC.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,309,310,314,780,784,789,790,885,23930,23931,25140,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22390555$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Ayyaswamy, Venkattraman</creatorcontrib><title>When do we need attractive-repulsive intermolecular potentials?</title><title>AIP Conference Proceedings</title><description>The role of attractive-repulsive interactions in direct simulation Monte Carlo (DSMC) simulations is studied by comparing with traditional purely repulsive interactions. The larger collision cross section of the long-range LJ potential is shown to result in a higher collision frequency and hence a lower mean free path, by at least a factor of two, for given conditions. This results in a faster relaxation to equilibrium as is shown by comparing the fourth and sixth moments of the molecular velocity distribution obtained using 0-D DSMC simulations. A 1-D Fourier-Couette flow with a large temperature and velocity difference between the walls is used to show that matching transport properties will result in identical solutions using both LJPA and VSS models in the near-continuum regime. However, flows in the transitional regime with Knudsen number, Kn ∼ 0.5 show a dependence on the intermolecular potential in spite of matching the viscosity coefficient due to differences in the collision frequency. Attractive-repulsive potentials should be used when both transport coefficients and collision frequencies should be matched.</description><subject>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS</subject><subject>COMPARATIVE EVALUATIONS</subject><subject>Computer simulation</subject><subject>COMPUTERIZED SIMULATION</subject><subject>COUETTE FLOW</subject><subject>CROSS SECTIONS</subject><subject>Dependence</subject><subject>Direct simulation Monte Carlo method</subject><subject>EQUILIBRIUM</subject><subject>INTERMOLECULAR FORCES</subject><subject>KNUDSEN FLOW</subject><subject>Matching</subject><subject>MATHEMATICAL SOLUTIONS</subject><subject>MEAN FREE PATH</subject><subject>MONTE CARLO METHOD</subject><subject>POTENTIALS</subject><subject>RELAXATION</subject><subject>Transport properties</subject><subject>VELOCITY</subject><subject>Velocity distribution</subject><subject>VISCOSITY</subject><issn>0094-243X</issn><issn>1551-7616</issn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2014</creationdate><recordtype>conference_proceeding</recordtype><recordid>eNqFjs1KxDAYRYMoWEcXvkHBdcfky0-T1SCDfzDgRtFdSZOvTIea1CbV17egC3euzl0cDpeQS0bXjCp-zdbCUJCaH5GCScmqWjF1TApKjahA8LdTcpbSgVIwda0LsnndYyh9LL-wDIi-tDlP1uX-E6sJx3lIyyr7kHF6jwO6ebBTOcaMIfd2SJtzctItxItfrsjL3e3z9qHaPd0_bm92VWTK5KpTUnnHLGjhvLAdFZoBcM1bK7h3HSgECS1FLXUttZOMddB6jbV3oLzkK3L1040p901yfUa3dzEEdLlZSoZK-ccap_gxY8rNIc5TWI41wEAJY6jS_1vSLM--AQeoYaU</recordid><startdate>20141209</startdate><enddate>20141209</enddate><creator>Ayyaswamy, Venkattraman</creator><general>American Institute of Physics</general><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20141209</creationdate><title>When do we need attractive-repulsive intermolecular potentials?</title><author>Ayyaswamy, Venkattraman</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o169t-f656dc1a284cd4af048122383ba43dcf26e252b0e858758c511f2bd8e7dc26d53</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2014</creationdate><topic>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS</topic><topic>COMPARATIVE EVALUATIONS</topic><topic>Computer simulation</topic><topic>COMPUTERIZED SIMULATION</topic><topic>COUETTE FLOW</topic><topic>CROSS SECTIONS</topic><topic>Dependence</topic><topic>Direct simulation Monte Carlo method</topic><topic>EQUILIBRIUM</topic><topic>INTERMOLECULAR FORCES</topic><topic>KNUDSEN FLOW</topic><topic>Matching</topic><topic>MATHEMATICAL SOLUTIONS</topic><topic>MEAN FREE PATH</topic><topic>MONTE CARLO METHOD</topic><topic>POTENTIALS</topic><topic>RELAXATION</topic><topic>Transport properties</topic><topic>VELOCITY</topic><topic>Velocity distribution</topic><topic>VISCOSITY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ayyaswamy, Venkattraman</creatorcontrib><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ayyaswamy, Venkattraman</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>When do we need attractive-repulsive intermolecular potentials?</atitle><btitle>AIP Conference Proceedings</btitle><date>2014-12-09</date><risdate>2014</risdate><volume>1628</volume><issue>1</issue><epage>130</epage><issn>0094-243X</issn><eissn>1551-7616</eissn><abstract>The role of attractive-repulsive interactions in direct simulation Monte Carlo (DSMC) simulations is studied by comparing with traditional purely repulsive interactions. The larger collision cross section of the long-range LJ potential is shown to result in a higher collision frequency and hence a lower mean free path, by at least a factor of two, for given conditions. This results in a faster relaxation to equilibrium as is shown by comparing the fourth and sixth moments of the molecular velocity distribution obtained using 0-D DSMC simulations. A 1-D Fourier-Couette flow with a large temperature and velocity difference between the walls is used to show that matching transport properties will result in identical solutions using both LJPA and VSS models in the near-continuum regime. However, flows in the transitional regime with Knudsen number, Kn ∼ 0.5 show a dependence on the intermolecular potential in spite of matching the viscosity coefficient due to differences in the collision frequency. Attractive-repulsive potentials should be used when both transport coefficients and collision frequencies should be matched.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4902583</doi></addata></record> |
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subjects | CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS COMPARATIVE EVALUATIONS Computer simulation COMPUTERIZED SIMULATION COUETTE FLOW CROSS SECTIONS Dependence Direct simulation Monte Carlo method EQUILIBRIUM INTERMOLECULAR FORCES KNUDSEN FLOW Matching MATHEMATICAL SOLUTIONS MEAN FREE PATH MONTE CARLO METHOD POTENTIALS RELAXATION Transport properties VELOCITY Velocity distribution VISCOSITY |
title | When do we need attractive-repulsive intermolecular potentials? |
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