Effect of rarefaction on axial vortex using direct simulation Monte Carlo

The effect of rarefaction on the axial vortex inside a lid-rotating closed cylinder is studied in the present work. The Direct Simulation Monte Carlo (DSMC) method has been used to simulate the flow inside the cylinder. The cylinder is closed and filled with Argon gas. Here, we look at the effect of...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Hauptverfasser: Dhurandhar, Shesh N., Mohan, Vishnu, Sharma, Manjul, Sameen, A.
Format: Tagungsbericht
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page
container_issue 1
container_start_page
container_title
container_volume 2996
creator Dhurandhar, Shesh N.
Mohan, Vishnu
Sharma, Manjul
Sameen, A.
description The effect of rarefaction on the axial vortex inside a lid-rotating closed cylinder is studied in the present work. The Direct Simulation Monte Carlo (DSMC) method has been used to simulate the flow inside the cylinder. The cylinder is closed and filled with Argon gas. Here, we look at the effect of rarefaction and compressibility on such flows by varying the Knudsen number (Kn) and Mach Number (Ma) of the flow. The Kn of the flow has been varied from 0.025 to 0.5 for Ma of 0.75 and 1 for a fixed aspect ratio of the cylinder 2.5. Thermal transport is characterized as the function of Ma and refraction. A three-dimensional Navier-Stokes-Fourier (NSF) solver with appropriate temperature jump and velocity slip boundary conditions has been used to compare the DSMC result for Kn=0.025. It is seen that DSMC and NSF results agree with each other at this low Kn. Note that increasing Kn reduces the peak axial velocity uz, as less momentum is transferred from the top plate to gases due to rarefaction. The velocity slip between the cylinder wall and the adjacent layer of fluid increases with an increase in Kn. Effect of rarefaction on radial pressure distribution has been discussed. The torque acting on the bottom plate was found to be decreasing with increasing rarefaction. The effect of rarefaction on flow topology and other regimes are also discussed.
doi_str_mv 10.1063/5.0187617
format Conference Proceeding
fullrecord <record><control><sourceid>proquest_scita</sourceid><recordid>TN_cdi_proquest_journals_2923487206</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2923487206</sourcerecordid><originalsourceid>FETCH-LOGICAL-p253t-68300b1a722f74c9c8d9522e8c3d0a1ca2ff0951b55fdcbaf6235eb2d63cb4543</originalsourceid><addsrcrecordid>eNotkE1LxDAQhoMoWKsH_0HAm9A1mTRNe5RlXRdWvCh4C2maSJZusyaprP_e7gcMzBwe5n15ELqnZEZJxZ74jNBaVFRcoIxyTovpri5RRkhTFlCyr2t0E-OGEGiEqDO0WlhrdMLe4qCCsUon5wc8jdo71eNfH5LZ4zG64Rt3LhzY6LZjr47cmx-SwXMVen-Lrqzqo7k77xx9viw-5q_F-n25mj-vix1wloqqZoS0VAkAK0rd6LprOICpNeuIolqBtaThtOXcdrpVtgLGTQtdxXRb8pLl6OH0dxf8z2hikhs_hmGKlNAAK2sBk4gcPZ6oqF06dpW74LYq_ElK5EGV5PKsiv0DfaFa8g</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>conference_proceeding</recordtype><pqid>2923487206</pqid></control><display><type>conference_proceeding</type><title>Effect of rarefaction on axial vortex using direct simulation Monte Carlo</title><source>AIP Journals Complete</source><creator>Dhurandhar, Shesh N. ; Mohan, Vishnu ; Sharma, Manjul ; Sameen, A.</creator><contributor>Xu, Kun ; Wu, Jong-Shinn ; Myong, Rho Shin</contributor><creatorcontrib>Dhurandhar, Shesh N. ; Mohan, Vishnu ; Sharma, Manjul ; Sameen, A. ; Xu, Kun ; Wu, Jong-Shinn ; Myong, Rho Shin</creatorcontrib><description>The effect of rarefaction on the axial vortex inside a lid-rotating closed cylinder is studied in the present work. The Direct Simulation Monte Carlo (DSMC) method has been used to simulate the flow inside the cylinder. The cylinder is closed and filled with Argon gas. Here, we look at the effect of rarefaction and compressibility on such flows by varying the Knudsen number (Kn) and Mach Number (Ma) of the flow. The Kn of the flow has been varied from 0.025 to 0.5 for Ma of 0.75 and 1 for a fixed aspect ratio of the cylinder 2.5. Thermal transport is characterized as the function of Ma and refraction. A three-dimensional Navier-Stokes-Fourier (NSF) solver with appropriate temperature jump and velocity slip boundary conditions has been used to compare the DSMC result for Kn=0.025. It is seen that DSMC and NSF results agree with each other at this low Kn. Note that increasing Kn reduces the peak axial velocity uz, as less momentum is transferred from the top plate to gases due to rarefaction. The velocity slip between the cylinder wall and the adjacent layer of fluid increases with an increase in Kn. Effect of rarefaction on radial pressure distribution has been discussed. The torque acting on the bottom plate was found to be decreasing with increasing rarefaction. The effect of rarefaction on flow topology and other regimes are also discussed.</description><identifier>ISSN: 0094-243X</identifier><identifier>EISSN: 1551-7616</identifier><identifier>DOI: 10.1063/5.0187617</identifier><identifier>CODEN: APCPCS</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Argon ; Aspect ratio ; Boundary conditions ; Compressibility effects ; Direct simulation Monte Carlo method ; Flow simulation ; Mach number ; Pressure distribution ; Rarefaction ; Rotating cylinders ; Topology</subject><ispartof>AIP conference proceedings, 2024, Vol.2996 (1)</ispartof><rights>Author(s)</rights><rights>2024 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/acp/article-lookup/doi/10.1063/5.0187617$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>309,310,314,777,781,786,787,791,4498,23911,23912,25121,27905,27906,76133</link.rule.ids></links><search><contributor>Xu, Kun</contributor><contributor>Wu, Jong-Shinn</contributor><contributor>Myong, Rho Shin</contributor><creatorcontrib>Dhurandhar, Shesh N.</creatorcontrib><creatorcontrib>Mohan, Vishnu</creatorcontrib><creatorcontrib>Sharma, Manjul</creatorcontrib><creatorcontrib>Sameen, A.</creatorcontrib><title>Effect of rarefaction on axial vortex using direct simulation Monte Carlo</title><title>AIP conference proceedings</title><description>The effect of rarefaction on the axial vortex inside a lid-rotating closed cylinder is studied in the present work. The Direct Simulation Monte Carlo (DSMC) method has been used to simulate the flow inside the cylinder. The cylinder is closed and filled with Argon gas. Here, we look at the effect of rarefaction and compressibility on such flows by varying the Knudsen number (Kn) and Mach Number (Ma) of the flow. The Kn of the flow has been varied from 0.025 to 0.5 for Ma of 0.75 and 1 for a fixed aspect ratio of the cylinder 2.5. Thermal transport is characterized as the function of Ma and refraction. A three-dimensional Navier-Stokes-Fourier (NSF) solver with appropriate temperature jump and velocity slip boundary conditions has been used to compare the DSMC result for Kn=0.025. It is seen that DSMC and NSF results agree with each other at this low Kn. Note that increasing Kn reduces the peak axial velocity uz, as less momentum is transferred from the top plate to gases due to rarefaction. The velocity slip between the cylinder wall and the adjacent layer of fluid increases with an increase in Kn. Effect of rarefaction on radial pressure distribution has been discussed. The torque acting on the bottom plate was found to be decreasing with increasing rarefaction. The effect of rarefaction on flow topology and other regimes are also discussed.</description><subject>Argon</subject><subject>Aspect ratio</subject><subject>Boundary conditions</subject><subject>Compressibility effects</subject><subject>Direct simulation Monte Carlo method</subject><subject>Flow simulation</subject><subject>Mach number</subject><subject>Pressure distribution</subject><subject>Rarefaction</subject><subject>Rotating cylinders</subject><subject>Topology</subject><issn>0094-243X</issn><issn>1551-7616</issn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2024</creationdate><recordtype>conference_proceeding</recordtype><recordid>eNotkE1LxDAQhoMoWKsH_0HAm9A1mTRNe5RlXRdWvCh4C2maSJZusyaprP_e7gcMzBwe5n15ELqnZEZJxZ74jNBaVFRcoIxyTovpri5RRkhTFlCyr2t0E-OGEGiEqDO0WlhrdMLe4qCCsUon5wc8jdo71eNfH5LZ4zG64Rt3LhzY6LZjr47cmx-SwXMVen-Lrqzqo7k77xx9viw-5q_F-n25mj-vix1wloqqZoS0VAkAK0rd6LprOICpNeuIolqBtaThtOXcdrpVtgLGTQtdxXRb8pLl6OH0dxf8z2hikhs_hmGKlNAAK2sBk4gcPZ6oqF06dpW74LYq_ElK5EGV5PKsiv0DfaFa8g</recordid><startdate>20240208</startdate><enddate>20240208</enddate><creator>Dhurandhar, Shesh N.</creator><creator>Mohan, Vishnu</creator><creator>Sharma, Manjul</creator><creator>Sameen, A.</creator><general>American Institute of Physics</general><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20240208</creationdate><title>Effect of rarefaction on axial vortex using direct simulation Monte Carlo</title><author>Dhurandhar, Shesh N. ; Mohan, Vishnu ; Sharma, Manjul ; Sameen, A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p253t-68300b1a722f74c9c8d9522e8c3d0a1ca2ff0951b55fdcbaf6235eb2d63cb4543</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Argon</topic><topic>Aspect ratio</topic><topic>Boundary conditions</topic><topic>Compressibility effects</topic><topic>Direct simulation Monte Carlo method</topic><topic>Flow simulation</topic><topic>Mach number</topic><topic>Pressure distribution</topic><topic>Rarefaction</topic><topic>Rotating cylinders</topic><topic>Topology</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dhurandhar, Shesh N.</creatorcontrib><creatorcontrib>Mohan, Vishnu</creatorcontrib><creatorcontrib>Sharma, Manjul</creatorcontrib><creatorcontrib>Sameen, A.</creatorcontrib><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Dhurandhar, Shesh N.</au><au>Mohan, Vishnu</au><au>Sharma, Manjul</au><au>Sameen, A.</au><au>Xu, Kun</au><au>Wu, Jong-Shinn</au><au>Myong, Rho Shin</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Effect of rarefaction on axial vortex using direct simulation Monte Carlo</atitle><btitle>AIP conference proceedings</btitle><date>2024-02-08</date><risdate>2024</risdate><volume>2996</volume><issue>1</issue><issn>0094-243X</issn><eissn>1551-7616</eissn><coden>APCPCS</coden><abstract>The effect of rarefaction on the axial vortex inside a lid-rotating closed cylinder is studied in the present work. The Direct Simulation Monte Carlo (DSMC) method has been used to simulate the flow inside the cylinder. The cylinder is closed and filled with Argon gas. Here, we look at the effect of rarefaction and compressibility on such flows by varying the Knudsen number (Kn) and Mach Number (Ma) of the flow. The Kn of the flow has been varied from 0.025 to 0.5 for Ma of 0.75 and 1 for a fixed aspect ratio of the cylinder 2.5. Thermal transport is characterized as the function of Ma and refraction. A three-dimensional Navier-Stokes-Fourier (NSF) solver with appropriate temperature jump and velocity slip boundary conditions has been used to compare the DSMC result for Kn=0.025. It is seen that DSMC and NSF results agree with each other at this low Kn. Note that increasing Kn reduces the peak axial velocity uz, as less momentum is transferred from the top plate to gases due to rarefaction. The velocity slip between the cylinder wall and the adjacent layer of fluid increases with an increase in Kn. Effect of rarefaction on radial pressure distribution has been discussed. The torque acting on the bottom plate was found to be decreasing with increasing rarefaction. The effect of rarefaction on flow topology and other regimes are also discussed.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0187617</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 0094-243X
ispartof AIP conference proceedings, 2024, Vol.2996 (1)
issn 0094-243X
1551-7616
language eng
recordid cdi_proquest_journals_2923487206
source AIP Journals Complete
subjects Argon
Aspect ratio
Boundary conditions
Compressibility effects
Direct simulation Monte Carlo method
Flow simulation
Mach number
Pressure distribution
Rarefaction
Rotating cylinders
Topology
title Effect of rarefaction on axial vortex using direct simulation Monte Carlo
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-18T04%3A27%3A41IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_scita&rft_val_fmt=info:ofi/fmt:kev:mtx:book&rft.genre=proceeding&rft.atitle=Effect%20of%20rarefaction%20on%20axial%20vortex%20using%20direct%20simulation%20Monte%20Carlo&rft.btitle=AIP%20conference%20proceedings&rft.au=Dhurandhar,%20Shesh%20N.&rft.date=2024-02-08&rft.volume=2996&rft.issue=1&rft.issn=0094-243X&rft.eissn=1551-7616&rft.coden=APCPCS&rft_id=info:doi/10.1063/5.0187617&rft_dat=%3Cproquest_scita%3E2923487206%3C/proquest_scita%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2923487206&rft_id=info:pmid/&rfr_iscdi=true