Secondary pool boiling effects
A pool boiling phenomenon referred to as secondary boiling effects is discussed. Based on the experimental trends, a mechanism is proposed that identifies the parameters that lead to this phenomenon. Secondary boiling effects refer to a distinct decrease in the wall superheat temperature near the cr...
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Veröffentlicht in: | Applied physics letters 2016-02, Vol.108 (5) |
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creator | Kruse, C. Tsubaki, A. Zuhlke, C. Anderson, T. Alexander, D. Gogos, G. Ndao, S. |
description | A pool boiling phenomenon referred to as secondary boiling effects is discussed. Based on the experimental trends, a mechanism is proposed that identifies the parameters that lead to this phenomenon. Secondary boiling effects refer to a distinct decrease in the wall superheat temperature near the critical heat flux due to a significant increase in the heat transfer coefficient. Recent pool boiling heat transfer experiments using femtosecond laser processed Inconel, stainless steel, and copper multiscale surfaces consistently displayed secondary boiling effects, which were found to be a result of both temperature drop along the microstructures and nucleation characteristic length scales. The temperature drop is a function of microstructure height and thermal conductivity. An increased microstructure height and a decreased thermal conductivity result in a significant temperature drop along the microstructures. This temperature drop becomes more pronounced at higher heat fluxes and along with the right nucleation characteristic length scales results in a change of the boiling dynamics. Nucleation spreads from the bottom of the microstructure valleys to the top of the microstructures, resulting in a decreased surface superheat with an increasing heat flux. This decrease in the wall superheat at higher heat fluxes is reflected by a “hook back” of the traditional boiling curve and is thus referred to as secondary boiling effects. In addition, a boiling hysteresis during increasing and decreasing heat flux develops due to the secondary boiling effects. This hysteresis further validates the existence of secondary boiling effects. |
doi_str_mv | 10.1063/1.4941081 |
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Based on the experimental trends, a mechanism is proposed that identifies the parameters that lead to this phenomenon. Secondary boiling effects refer to a distinct decrease in the wall superheat temperature near the critical heat flux due to a significant increase in the heat transfer coefficient. Recent pool boiling heat transfer experiments using femtosecond laser processed Inconel, stainless steel, and copper multiscale surfaces consistently displayed secondary boiling effects, which were found to be a result of both temperature drop along the microstructures and nucleation characteristic length scales. The temperature drop is a function of microstructure height and thermal conductivity. An increased microstructure height and a decreased thermal conductivity result in a significant temperature drop along the microstructures. This temperature drop becomes more pronounced at higher heat fluxes and along with the right nucleation characteristic length scales results in a change of the boiling dynamics. Nucleation spreads from the bottom of the microstructure valleys to the top of the microstructures, resulting in a decreased surface superheat with an increasing heat flux. This decrease in the wall superheat at higher heat fluxes is reflected by a “hook back” of the traditional boiling curve and is thus referred to as secondary boiling effects. In addition, a boiling hysteresis during increasing and decreasing heat flux develops due to the secondary boiling effects. This hysteresis further validates the existence of secondary boiling effects.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.4941081</identifier><identifier>PMID: 30546153</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>United States: American Institute of Physics</publisher><subject>Applied physics ; Boiling ; Heat conductivity ; Heat flux ; Heat transfer coefficients ; Hysteresis ; Microstructure ; Nickel base alloys ; Nucleation ; Parameter identification ; Superalloys ; Thermal conductivity</subject><ispartof>Applied physics letters, 2016-02, Vol.108 (5)</ispartof><rights>AIP Publishing LLC</rights><rights>2016 AIP Publishing LLC.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c539t-b03240879c763f1f17a5c050765ddb5b3208a1c9729458cad1f2b914ef2b342f3</citedby><cites>FETCH-LOGICAL-c539t-b03240879c763f1f17a5c050765ddb5b3208a1c9729458cad1f2b914ef2b342f3</cites><orcidid>0000-0001-9006-7855 ; 0000-0003-1348-0026</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/apl/article-lookup/doi/10.1063/1.4941081$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>230,314,776,780,790,881,4498,27901,27902,76127</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/30546153$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Kruse, C.</creatorcontrib><creatorcontrib>Tsubaki, A.</creatorcontrib><creatorcontrib>Zuhlke, C.</creatorcontrib><creatorcontrib>Anderson, T.</creatorcontrib><creatorcontrib>Alexander, D.</creatorcontrib><creatorcontrib>Gogos, G.</creatorcontrib><creatorcontrib>Ndao, S.</creatorcontrib><title>Secondary pool boiling effects</title><title>Applied physics letters</title><addtitle>Appl Phys Lett</addtitle><description>A pool boiling phenomenon referred to as secondary boiling effects is discussed. Based on the experimental trends, a mechanism is proposed that identifies the parameters that lead to this phenomenon. Secondary boiling effects refer to a distinct decrease in the wall superheat temperature near the critical heat flux due to a significant increase in the heat transfer coefficient. Recent pool boiling heat transfer experiments using femtosecond laser processed Inconel, stainless steel, and copper multiscale surfaces consistently displayed secondary boiling effects, which were found to be a result of both temperature drop along the microstructures and nucleation characteristic length scales. The temperature drop is a function of microstructure height and thermal conductivity. An increased microstructure height and a decreased thermal conductivity result in a significant temperature drop along the microstructures. This temperature drop becomes more pronounced at higher heat fluxes and along with the right nucleation characteristic length scales results in a change of the boiling dynamics. Nucleation spreads from the bottom of the microstructure valleys to the top of the microstructures, resulting in a decreased surface superheat with an increasing heat flux. This decrease in the wall superheat at higher heat fluxes is reflected by a “hook back” of the traditional boiling curve and is thus referred to as secondary boiling effects. In addition, a boiling hysteresis during increasing and decreasing heat flux develops due to the secondary boiling effects. This hysteresis further validates the existence of secondary boiling effects.</description><subject>Applied physics</subject><subject>Boiling</subject><subject>Heat conductivity</subject><subject>Heat flux</subject><subject>Heat transfer coefficients</subject><subject>Hysteresis</subject><subject>Microstructure</subject><subject>Nickel base alloys</subject><subject>Nucleation</subject><subject>Parameter identification</subject><subject>Superalloys</subject><subject>Thermal conductivity</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNp90MtKAzEUBuAgiq3VhS8gBTcqTM3JdbIRpHiDggt1HTKZpI5MJ3UyLfj2RlrrDVwdQj7-_DkIHQIeARb0HEZMMcA5bKE-YCkzCpBvoz7GmGZCceihvRhf0pETSndRj2LOBHDaR0cPzoamNO3bcB5CPSxCVVfNdOi8d7aL-2jHmzq6g_UcoKfrq8fxbTa5v7kbX04yy6nqsgJTwnAulZWCevAgDbeYYyl4WRa8oATnBqySRDGeW1OCJ4UC5tKgjHg6QBer3PmimLnSuqZrTa3nbTVL1XQwlf5501TPehqWWpA8F5KkgJN1QBteFy52elZF6-raNC4soibApRBAVZ7o8S_6EhZtk76XFAEFHDOW1OlK2TbE2Dq_KQNYf2xdg15vPdmj7-038nPNCZytQLRVZ7oqNBuzDO1Xkp6X_j_89-l39EqWGw</recordid><startdate>20160201</startdate><enddate>20160201</enddate><creator>Kruse, C.</creator><creator>Tsubaki, A.</creator><creator>Zuhlke, C.</creator><creator>Anderson, T.</creator><creator>Alexander, D.</creator><creator>Gogos, G.</creator><creator>Ndao, S.</creator><general>American Institute of Physics</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0001-9006-7855</orcidid><orcidid>https://orcid.org/0000-0003-1348-0026</orcidid></search><sort><creationdate>20160201</creationdate><title>Secondary pool boiling effects</title><author>Kruse, C. ; Tsubaki, A. ; Zuhlke, C. ; Anderson, T. ; Alexander, D. ; Gogos, G. ; Ndao, S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c539t-b03240879c763f1f17a5c050765ddb5b3208a1c9729458cad1f2b914ef2b342f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Applied physics</topic><topic>Boiling</topic><topic>Heat conductivity</topic><topic>Heat flux</topic><topic>Heat transfer coefficients</topic><topic>Hysteresis</topic><topic>Microstructure</topic><topic>Nickel base alloys</topic><topic>Nucleation</topic><topic>Parameter identification</topic><topic>Superalloys</topic><topic>Thermal conductivity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kruse, C.</creatorcontrib><creatorcontrib>Tsubaki, A.</creatorcontrib><creatorcontrib>Zuhlke, C.</creatorcontrib><creatorcontrib>Anderson, T.</creatorcontrib><creatorcontrib>Alexander, D.</creatorcontrib><creatorcontrib>Gogos, G.</creatorcontrib><creatorcontrib>Ndao, S.</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kruse, C.</au><au>Tsubaki, A.</au><au>Zuhlke, C.</au><au>Anderson, T.</au><au>Alexander, D.</au><au>Gogos, G.</au><au>Ndao, S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Secondary pool boiling effects</atitle><jtitle>Applied physics letters</jtitle><addtitle>Appl Phys Lett</addtitle><date>2016-02-01</date><risdate>2016</risdate><volume>108</volume><issue>5</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>A pool boiling phenomenon referred to as secondary boiling effects is discussed. Based on the experimental trends, a mechanism is proposed that identifies the parameters that lead to this phenomenon. Secondary boiling effects refer to a distinct decrease in the wall superheat temperature near the critical heat flux due to a significant increase in the heat transfer coefficient. Recent pool boiling heat transfer experiments using femtosecond laser processed Inconel, stainless steel, and copper multiscale surfaces consistently displayed secondary boiling effects, which were found to be a result of both temperature drop along the microstructures and nucleation characteristic length scales. The temperature drop is a function of microstructure height and thermal conductivity. An increased microstructure height and a decreased thermal conductivity result in a significant temperature drop along the microstructures. This temperature drop becomes more pronounced at higher heat fluxes and along with the right nucleation characteristic length scales results in a change of the boiling dynamics. Nucleation spreads from the bottom of the microstructure valleys to the top of the microstructures, resulting in a decreased surface superheat with an increasing heat flux. This decrease in the wall superheat at higher heat fluxes is reflected by a “hook back” of the traditional boiling curve and is thus referred to as secondary boiling effects. In addition, a boiling hysteresis during increasing and decreasing heat flux develops due to the secondary boiling effects. This hysteresis further validates the existence of secondary boiling effects.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>30546153</pmid><doi>10.1063/1.4941081</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0001-9006-7855</orcidid><orcidid>https://orcid.org/0000-0003-1348-0026</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Applied physics Boiling Heat conductivity Heat flux Heat transfer coefficients Hysteresis Microstructure Nickel base alloys Nucleation Parameter identification Superalloys Thermal conductivity |
title | Secondary pool boiling effects |
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