Natural convection of water–CuO nanofluid in a cavity with two pairs of heat source–sink
Natural convection in a two-dimensional square cavity filled with a water–CuO nanofluid is numerically studied. Two pairs of heat source–sink are considered to cover the entire length of the bottom wall of the cavity while the other walls are thermally insulated. The nanofluid is assumed to be homog...
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Veröffentlicht in: | International communications in heat and mass transfer 2011-05, Vol.38 (5), p.672-678 |
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description | Natural convection in a two-dimensional square cavity filled with a water–CuO nanofluid is numerically studied. Two pairs of heat source–sink are considered to cover the entire length of the bottom wall of the cavity while the other walls are thermally insulated. The nanofluid is assumed to be homogenous and Newtonian. The governing differential equations are discretised by the control volume approach and the coupling between velocity and pressure is solved using the SIMPLE algorithm. A comparison study is presented between two cases with different arrangements of the two pairs on the bottom wall. The effects of Rayleigh number and solid volume fraction of the nanofluid on the heat transfer rate have also been examined. The results show that regardless of the position of the pairs of source–sink, the heat transfer rate increases with an increase of the Rayleigh number and the solid volume fraction. |
doi_str_mv | 10.1016/j.icheatmasstransfer.2011.03.013 |
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Two pairs of heat source–sink are considered to cover the entire length of the bottom wall of the cavity while the other walls are thermally insulated. The nanofluid is assumed to be homogenous and Newtonian. The governing differential equations are discretised by the control volume approach and the coupling between velocity and pressure is solved using the SIMPLE algorithm. A comparison study is presented between two cases with different arrangements of the two pairs on the bottom wall. The effects of Rayleigh number and solid volume fraction of the nanofluid on the heat transfer rate have also been examined. The results show that regardless of the position of the pairs of source–sink, the heat transfer rate increases with an increase of the Rayleigh number and the solid volume fraction.</description><identifier>ISSN: 0735-1933</identifier><identifier>EISSN: 1879-0178</identifier><identifier>DOI: 10.1016/j.icheatmasstransfer.2011.03.013</identifier><language>eng</language><publisher>Elsevier Ltd</publisher><subject>COMPOSITES ; CONVECTION ; COPPER OXIDE ; FLUID FLOW ; HEAT TRANSFER ; HOLES ; MICROSTRUCTURES ; Nanocomposites ; Nanofluid ; Nanofluids ; Nanomaterials ; Nanostructure ; Natural convection ; Source–sink ; Square cavity ; Volume fraction ; Walls ; WATER</subject><ispartof>International communications in heat and mass transfer, 2011-05, Vol.38 (5), p.672-678</ispartof><rights>2011 Elsevier Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c407t-c2a87fda457788a2b79de7432098e15b6ecd48f424a15fb0046a6018d9d17c913</citedby><cites>FETCH-LOGICAL-c407t-c2a87fda457788a2b79de7432098e15b6ecd48f424a15fb0046a6018d9d17c913</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0735193311000492$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids></links><search><creatorcontrib>Aminossadati, S.M.</creatorcontrib><creatorcontrib>Ghasemi, B.</creatorcontrib><title>Natural convection of water–CuO nanofluid in a cavity with two pairs of heat source–sink</title><title>International communications in heat and mass transfer</title><description>Natural convection in a two-dimensional square cavity filled with a water–CuO nanofluid is numerically studied. 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The results show that regardless of the position of the pairs of source–sink, the heat transfer rate increases with an increase of the Rayleigh number and the solid volume fraction.</description><subject>COMPOSITES</subject><subject>CONVECTION</subject><subject>COPPER OXIDE</subject><subject>FLUID FLOW</subject><subject>HEAT TRANSFER</subject><subject>HOLES</subject><subject>MICROSTRUCTURES</subject><subject>Nanocomposites</subject><subject>Nanofluid</subject><subject>Nanofluids</subject><subject>Nanomaterials</subject><subject>Nanostructure</subject><subject>Natural convection</subject><subject>Source–sink</subject><subject>Square cavity</subject><subject>Volume fraction</subject><subject>Walls</subject><subject>WATER</subject><issn>0735-1933</issn><issn>1879-0178</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqNkcGO0zAQhi0EEqXwDr6xl4SZOImdG6iChdWKvcANyZo6jtYltYvttNob78Ab8iS46t6QEKc5zP9_-md-xq4QagTs3-xqZ-4t5T2llCP5NNlYN4BYg6gBxRO2QiWHClCqp2wFUnQVDkI8Zy9S2gEAKlQr9u0z5SXSzE3wR2uyC56HiZ8o2_j756_Ncsc9-TDNixu585y4oaPLD_zk8j3Pp8AP5GI6e85peApLNLY4k_PfX7JnE83Jvnqca_b1w_svm4_V7d31p82728q0IHNlGlJyGqntpFSKmq0cRitb0cCgLHbb3pqxVVPbtITdtAVoe-pL_nEYUZoBxZq9vnAPMfxYbMp675Kx80zehiVpJTuQ2Jfz1-zqn0qUbSuhU6Iv0rcXqYkhpWgnfYhuT_FBI-hzBXqn_65AnyvQIHSpoCBuLghbjj-6sk3GWW_s6GL5tR6D-3_YHwiZnjY</recordid><startdate>20110501</startdate><enddate>20110501</enddate><creator>Aminossadati, S.M.</creator><creator>Ghasemi, B.</creator><general>Elsevier Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>H8G</scope><scope>JG9</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>20110501</creationdate><title>Natural convection of water–CuO nanofluid in a cavity with two pairs of heat source–sink</title><author>Aminossadati, S.M. ; Ghasemi, B.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c407t-c2a87fda457788a2b79de7432098e15b6ecd48f424a15fb0046a6018d9d17c913</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>COMPOSITES</topic><topic>CONVECTION</topic><topic>COPPER OXIDE</topic><topic>FLUID FLOW</topic><topic>HEAT TRANSFER</topic><topic>HOLES</topic><topic>MICROSTRUCTURES</topic><topic>Nanocomposites</topic><topic>Nanofluid</topic><topic>Nanofluids</topic><topic>Nanomaterials</topic><topic>Nanostructure</topic><topic>Natural convection</topic><topic>Source–sink</topic><topic>Square cavity</topic><topic>Volume fraction</topic><topic>Walls</topic><topic>WATER</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Aminossadati, S.M.</creatorcontrib><creatorcontrib>Ghasemi, B.</creatorcontrib><collection>CrossRef</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Copper Technical Reference Library</collection><collection>Materials Research Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>International communications in heat and mass transfer</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Aminossadati, S.M.</au><au>Ghasemi, B.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Natural convection of water–CuO nanofluid in a cavity with two pairs of heat source–sink</atitle><jtitle>International communications in heat and mass transfer</jtitle><date>2011-05-01</date><risdate>2011</risdate><volume>38</volume><issue>5</issue><spage>672</spage><epage>678</epage><pages>672-678</pages><issn>0735-1933</issn><eissn>1879-0178</eissn><abstract>Natural convection in a two-dimensional square cavity filled with a water–CuO nanofluid is numerically studied. Two pairs of heat source–sink are considered to cover the entire length of the bottom wall of the cavity while the other walls are thermally insulated. The nanofluid is assumed to be homogenous and Newtonian. The governing differential equations are discretised by the control volume approach and the coupling between velocity and pressure is solved using the SIMPLE algorithm. A comparison study is presented between two cases with different arrangements of the two pairs on the bottom wall. The effects of Rayleigh number and solid volume fraction of the nanofluid on the heat transfer rate have also been examined. The results show that regardless of the position of the pairs of source–sink, the heat transfer rate increases with an increase of the Rayleigh number and the solid volume fraction.</abstract><pub>Elsevier Ltd</pub><doi>10.1016/j.icheatmasstransfer.2011.03.013</doi><tpages>7</tpages></addata></record> |
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subjects | COMPOSITES CONVECTION COPPER OXIDE FLUID FLOW HEAT TRANSFER HOLES MICROSTRUCTURES Nanocomposites Nanofluid Nanofluids Nanomaterials Nanostructure Natural convection Source–sink Square cavity Volume fraction Walls WATER |
title | Natural convection of water–CuO nanofluid in a cavity with two pairs of heat source–sink |
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