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Predicted thermal performance of triple vacuum glazing
The simulated triple vacuum glazing (TVG) consists of three 4 mm thick glass panes with two vacuum gaps, with each internal glass surface coated with a low-emittance coating with an emittance of 0.03. The two vacuum gaps are sealed by an indium based sealant and separated by a stainless steel pillar...
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Published in: | Solar energy 2010-12, Vol.84 (12), p.2132-2139 |
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creator | Fang, Yueping Hyde, Trevor J. Hewitt, Neil |
description | The simulated triple vacuum glazing (TVG) consists of three 4
mm thick glass panes with two vacuum gaps, with each internal glass surface coated with a low-emittance coating with an emittance of 0.03. The two vacuum gaps are sealed by an indium based sealant and separated by a stainless steel pillar array with a height of 0.12
mm and a pillar diameter of 0.3
mm spaced at 25
mm. The thermal transmission at the centre-of-glazing area of the TVG was predicted to be 0.26
W
m
−2
K
−1. The simulation results show that although the thermal conductivity of solder glass (1
W
m
−1
K
−1) and indium (83.7
W
m
−1
K
−1) are very different, the difference in thermal transmission of TVGs resulting from the use of an indium and a solder glass edge seal was 0.01
W
m
−2
K
−1. This is because the edge seal is so thin (0.12
mm), consequently there is a negligible temperature drop across it irrespective of the material that the seal is made from relative to the total temperature difference across the glazing. The results also show that there is a relatively large increase in the overall thermal conductance of glazings without a frame when the width of the indium edge seal is increased. Increasing the rebate depth in a solid wood frame decreased the heat transmission of the TVG. The overall heat transmission of the simulated 0.5
m by 0.5
m TVG was 32.6% greater than that of the 1
m by 1
m TVG, since heat conduction through the edge seal of the small glazing has a larger contribution to the total glazing heat transfer than that of the larger glazing system. |
doi_str_mv | 10.1016/j.solener.2010.09.002 |
format | article |
fullrecord | <record><control><sourceid>proquest_osti_</sourceid><recordid>TN_cdi_osti_scitechconnect_21396187</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0038092X10002859</els_id><sourcerecordid>1777163912</sourcerecordid><originalsourceid>FETCH-LOGICAL-c459t-a4e5c2bec7faf94016e142c95565587bb0c06a8671f13b592ce134d25350e8e23</originalsourceid><addsrcrecordid>eNqF0VFrFDEQB_AgCp7VjyAsitSXPWeym2TzJFJqFQr2QcG3kMvOtjn2NmeyW7Cf3jnu8KEP-pQQfplk5i_Ea4Q1AuoP23VJI02U1xL4DOwaQD4RK2wN1iiVeSpWAE1Xg5U_n4sXpWwB0GBnVkLfZOpjmKmv5jvKOz9We8pD4t0UqEpDNee4H6m692FZdtXt6B_idPtSPBv8WOjVaT0TPz5ffr_4Ul9_u_p68em6Dq2yc-1bUkFuKJjBD7blzxK2MliltFKd2WwggPadNjhgs1FWBsKm7aVqFFBHsjkTb491U5mjKyHOFO5CmiYKs5PYWM1dsDo_qn1OvxYqs9vFEmgc_URpKa5jZ1FaZPn-nxKNMagbxkzfPKLbtOSJu3UdGKsYtozUEYWcSsk0uH2OO59_OwR3CMdt3SkcdwjHgXUcDt97dyruS_DjkHnasfy9LJtWg4aO3cejIx7yfeQqPAPiZPqYDyPoU_zPS38AP62lHg</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>807957714</pqid></control><display><type>article</type><title>Predicted thermal performance of triple vacuum glazing</title><source>Elsevier</source><creator>Fang, Yueping ; Hyde, Trevor J. ; Hewitt, Neil</creator><creatorcontrib>Fang, Yueping ; Hyde, Trevor J. ; Hewitt, Neil</creatorcontrib><description>The simulated triple vacuum glazing (TVG) consists of three 4
mm thick glass panes with two vacuum gaps, with each internal glass surface coated with a low-emittance coating with an emittance of 0.03. The two vacuum gaps are sealed by an indium based sealant and separated by a stainless steel pillar array with a height of 0.12
mm and a pillar diameter of 0.3
mm spaced at 25
mm. The thermal transmission at the centre-of-glazing area of the TVG was predicted to be 0.26
W
m
−2
K
−1. The simulation results show that although the thermal conductivity of solder glass (1
W
m
−1
K
−1) and indium (83.7
W
m
−1
K
−1) are very different, the difference in thermal transmission of TVGs resulting from the use of an indium and a solder glass edge seal was 0.01
W
m
−2
K
−1. This is because the edge seal is so thin (0.12
mm), consequently there is a negligible temperature drop across it irrespective of the material that the seal is made from relative to the total temperature difference across the glazing. The results also show that there is a relatively large increase in the overall thermal conductance of glazings without a frame when the width of the indium edge seal is increased. Increasing the rebate depth in a solid wood frame decreased the heat transmission of the TVG. The overall heat transmission of the simulated 0.5
m by 0.5
m TVG was 32.6% greater than that of the 1
m by 1
m TVG, since heat conduction through the edge seal of the small glazing has a larger contribution to the total glazing heat transfer than that of the larger glazing system.</description><identifier>ISSN: 0038-092X</identifier><identifier>EISSN: 1471-1257</identifier><identifier>DOI: 10.1016/j.solener.2010.09.002</identifier><identifier>CODEN: SRENA4</identifier><language>eng</language><publisher>Kidlington: Elsevier Ltd</publisher><subject>Analytic model ; Applied sciences ; Double vacuum glazing ; Energy ; ENERGY CONSERVATION, CONSUMPTION, AND UTILIZATION ; Energy. Thermal use of fuels ; Exact sciences and technology ; Finite volume model ; GLASS ; Glazing ; GLAZING MATERIALS ; Heat transfer ; Heat transmission ; Indium ; SEALS ; SIMULATION ; Solar energy ; Solders ; Temperature ; Theoretical studies. Data and constants. Metering ; THERMAL CONDUCTION ; THERMAL CONDUCTIVITY ; Thermal performance ; Triple glazing ; Triple vacuum glazing (TVG) ; Vacuum technology ; WIDTH</subject><ispartof>Solar energy, 2010-12, Vol.84 (12), p.2132-2139</ispartof><rights>2010 Elsevier Ltd</rights><rights>2015 INIST-CNRS</rights><rights>Copyright Pergamon Press Inc. Dec 2010</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c459t-a4e5c2bec7faf94016e142c95565587bb0c06a8671f13b592ce134d25350e8e23</citedby><cites>FETCH-LOGICAL-c459t-a4e5c2bec7faf94016e142c95565587bb0c06a8671f13b592ce134d25350e8e23</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,315,786,790,891,27957,27958</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=23460608$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/21396187$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Fang, Yueping</creatorcontrib><creatorcontrib>Hyde, Trevor J.</creatorcontrib><creatorcontrib>Hewitt, Neil</creatorcontrib><title>Predicted thermal performance of triple vacuum glazing</title><title>Solar energy</title><description>The simulated triple vacuum glazing (TVG) consists of three 4
mm thick glass panes with two vacuum gaps, with each internal glass surface coated with a low-emittance coating with an emittance of 0.03. The two vacuum gaps are sealed by an indium based sealant and separated by a stainless steel pillar array with a height of 0.12
mm and a pillar diameter of 0.3
mm spaced at 25
mm. The thermal transmission at the centre-of-glazing area of the TVG was predicted to be 0.26
W
m
−2
K
−1. The simulation results show that although the thermal conductivity of solder glass (1
W
m
−1
K
−1) and indium (83.7
W
m
−1
K
−1) are very different, the difference in thermal transmission of TVGs resulting from the use of an indium and a solder glass edge seal was 0.01
W
m
−2
K
−1. This is because the edge seal is so thin (0.12
mm), consequently there is a negligible temperature drop across it irrespective of the material that the seal is made from relative to the total temperature difference across the glazing. The results also show that there is a relatively large increase in the overall thermal conductance of glazings without a frame when the width of the indium edge seal is increased. Increasing the rebate depth in a solid wood frame decreased the heat transmission of the TVG. The overall heat transmission of the simulated 0.5
m by 0.5
m TVG was 32.6% greater than that of the 1
m by 1
m TVG, since heat conduction through the edge seal of the small glazing has a larger contribution to the total glazing heat transfer than that of the larger glazing system.</description><subject>Analytic model</subject><subject>Applied sciences</subject><subject>Double vacuum glazing</subject><subject>Energy</subject><subject>ENERGY CONSERVATION, CONSUMPTION, AND UTILIZATION</subject><subject>Energy. Thermal use of fuels</subject><subject>Exact sciences and technology</subject><subject>Finite volume model</subject><subject>GLASS</subject><subject>Glazing</subject><subject>GLAZING MATERIALS</subject><subject>Heat transfer</subject><subject>Heat transmission</subject><subject>Indium</subject><subject>SEALS</subject><subject>SIMULATION</subject><subject>Solar energy</subject><subject>Solders</subject><subject>Temperature</subject><subject>Theoretical studies. Data and constants. Metering</subject><subject>THERMAL CONDUCTION</subject><subject>THERMAL CONDUCTIVITY</subject><subject>Thermal performance</subject><subject>Triple glazing</subject><subject>Triple vacuum glazing (TVG)</subject><subject>Vacuum technology</subject><subject>WIDTH</subject><issn>0038-092X</issn><issn>1471-1257</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqF0VFrFDEQB_AgCp7VjyAsitSXPWeym2TzJFJqFQr2QcG3kMvOtjn2NmeyW7Cf3jnu8KEP-pQQfplk5i_Ea4Q1AuoP23VJI02U1xL4DOwaQD4RK2wN1iiVeSpWAE1Xg5U_n4sXpWwB0GBnVkLfZOpjmKmv5jvKOz9We8pD4t0UqEpDNee4H6m692FZdtXt6B_idPtSPBv8WOjVaT0TPz5ffr_4Ul9_u_p68em6Dq2yc-1bUkFuKJjBD7blzxK2MliltFKd2WwggPadNjhgs1FWBsKm7aVqFFBHsjkTb491U5mjKyHOFO5CmiYKs5PYWM1dsDo_qn1OvxYqs9vFEmgc_URpKa5jZ1FaZPn-nxKNMagbxkzfPKLbtOSJu3UdGKsYtozUEYWcSsk0uH2OO59_OwR3CMdt3SkcdwjHgXUcDt97dyruS_DjkHnasfy9LJtWg4aO3cejIx7yfeQqPAPiZPqYDyPoU_zPS38AP62lHg</recordid><startdate>20101201</startdate><enddate>20101201</enddate><creator>Fang, Yueping</creator><creator>Hyde, Trevor J.</creator><creator>Hewitt, Neil</creator><general>Elsevier Ltd</general><general>Elsevier</general><general>Pergamon Press Inc</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7ST</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>KR7</scope><scope>L7M</scope><scope>SOI</scope><scope>7SU</scope><scope>7TG</scope><scope>KL.</scope><scope>OTOTI</scope></search><sort><creationdate>20101201</creationdate><title>Predicted thermal performance of triple vacuum glazing</title><author>Fang, Yueping ; Hyde, Trevor J. ; Hewitt, Neil</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c459t-a4e5c2bec7faf94016e142c95565587bb0c06a8671f13b592ce134d25350e8e23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Analytic model</topic><topic>Applied sciences</topic><topic>Double vacuum glazing</topic><topic>Energy</topic><topic>ENERGY CONSERVATION, CONSUMPTION, AND UTILIZATION</topic><topic>Energy. Thermal use of fuels</topic><topic>Exact sciences and technology</topic><topic>Finite volume model</topic><topic>GLASS</topic><topic>Glazing</topic><topic>GLAZING MATERIALS</topic><topic>Heat transfer</topic><topic>Heat transmission</topic><topic>Indium</topic><topic>SEALS</topic><topic>SIMULATION</topic><topic>Solar energy</topic><topic>Solders</topic><topic>Temperature</topic><topic>Theoretical studies. Data and constants. Metering</topic><topic>THERMAL CONDUCTION</topic><topic>THERMAL CONDUCTIVITY</topic><topic>Thermal performance</topic><topic>Triple glazing</topic><topic>Triple vacuum glazing (TVG)</topic><topic>Vacuum technology</topic><topic>WIDTH</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Fang, Yueping</creatorcontrib><creatorcontrib>Hyde, Trevor J.</creatorcontrib><creatorcontrib>Hewitt, Neil</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Environment Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Environment Abstracts</collection><collection>Environmental Engineering Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>OSTI.GOV</collection><jtitle>Solar energy</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fang, Yueping</au><au>Hyde, Trevor J.</au><au>Hewitt, Neil</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Predicted thermal performance of triple vacuum glazing</atitle><jtitle>Solar energy</jtitle><date>2010-12-01</date><risdate>2010</risdate><volume>84</volume><issue>12</issue><spage>2132</spage><epage>2139</epage><pages>2132-2139</pages><issn>0038-092X</issn><eissn>1471-1257</eissn><coden>SRENA4</coden><notes>ObjectType-Article-1</notes><notes>SourceType-Scholarly Journals-1</notes><notes>ObjectType-Feature-2</notes><notes>content type line 23</notes><abstract>The simulated triple vacuum glazing (TVG) consists of three 4
mm thick glass panes with two vacuum gaps, with each internal glass surface coated with a low-emittance coating with an emittance of 0.03. The two vacuum gaps are sealed by an indium based sealant and separated by a stainless steel pillar array with a height of 0.12
mm and a pillar diameter of 0.3
mm spaced at 25
mm. The thermal transmission at the centre-of-glazing area of the TVG was predicted to be 0.26
W
m
−2
K
−1. The simulation results show that although the thermal conductivity of solder glass (1
W
m
−1
K
−1) and indium (83.7
W
m
−1
K
−1) are very different, the difference in thermal transmission of TVGs resulting from the use of an indium and a solder glass edge seal was 0.01
W
m
−2
K
−1. This is because the edge seal is so thin (0.12
mm), consequently there is a negligible temperature drop across it irrespective of the material that the seal is made from relative to the total temperature difference across the glazing. The results also show that there is a relatively large increase in the overall thermal conductance of glazings without a frame when the width of the indium edge seal is increased. Increasing the rebate depth in a solid wood frame decreased the heat transmission of the TVG. The overall heat transmission of the simulated 0.5
m by 0.5
m TVG was 32.6% greater than that of the 1
m by 1
m TVG, since heat conduction through the edge seal of the small glazing has a larger contribution to the total glazing heat transfer than that of the larger glazing system.</abstract><cop>Kidlington</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.solener.2010.09.002</doi><tpages>8</tpages></addata></record> |
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language | eng |
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source | Elsevier |
subjects | Analytic model Applied sciences Double vacuum glazing Energy ENERGY CONSERVATION, CONSUMPTION, AND UTILIZATION Energy. Thermal use of fuels Exact sciences and technology Finite volume model GLASS Glazing GLAZING MATERIALS Heat transfer Heat transmission Indium SEALS SIMULATION Solar energy Solders Temperature Theoretical studies. Data and constants. Metering THERMAL CONDUCTION THERMAL CONDUCTIVITY Thermal performance Triple glazing Triple vacuum glazing (TVG) Vacuum technology WIDTH |
title | Predicted thermal performance of triple vacuum glazing |
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