Thermal conductivity of high strength polyethylene fiber in low temperature
High strength polyethylene fiber (Toyobo, Dyneema® fiber, hereinafter abbreviated to DF) used as reinforcement of fiber‐reinforced plastics for cryogenic use has a high thermal conductivity. To understand the thermal conductivity of DF, the relation between fiber structure and thermal conductivity o...
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Veröffentlicht in: | Journal of polymer science. Part B, Polymer physics Polymer physics, 2005-06, Vol.43 (12), p.1495-1503 |
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container_title | Journal of polymer science. Part B, Polymer physics |
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creator | Yamanaka, Atsuhiko Fujishiro, Hiroyuki Kashima, Toshihiro Kitagawa, Tooru Ema, Kimiko Izumi, Yoshinobu Ikebe, Manabu Nishijima, Shigehiro |
description | High strength polyethylene fiber (Toyobo, Dyneema® fiber, hereinafter abbreviated to DF) used as reinforcement of fiber‐reinforced plastics for cryogenic use has a high thermal conductivity. To understand the thermal conductivity of DF, the relation between fiber structure and thermal conductivity of several kinds of polyethylene fibers having different modulus from 15 to 134 GPa (hereinafter abbreviated to DFs) was investigated. The mechanical series‐parallel model composed of crystal and amorphous was applied to DFs for thermal conductivity. This mechanical model was obtained by crystallinity and crystal orientation angle measured by solid state NMR and X‐ray. Thermal conductivity of DF in fiber direction was dominated by that of the continuous crystal region. The thermal conductivity of the continuous crystal part estimated by the mechanical model increases from 16 to 900 mw/cmK by the increasing temperature from 10 to 150K, and thermal diffusivity of the continuous crystal part was estimated to about 100 mm2/s, which is almost temperature independent. The phonon mean free path of the continuous crystal region of DF obtained by thermal diffusivity is almost temperature independent and its value about 200 Å. With the aforementioned, the mechanical series‐parallel model composed of crystal and amorphous regions could be applied to DFs for thermal conductivity. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 1495–1503, 2005 |
doi_str_mv | 10.1002/polb.20428 |
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To understand the thermal conductivity of DF, the relation between fiber structure and thermal conductivity of several kinds of polyethylene fibers having different modulus from 15 to 134 GPa (hereinafter abbreviated to DFs) was investigated. The mechanical series‐parallel model composed of crystal and amorphous was applied to DFs for thermal conductivity. This mechanical model was obtained by crystallinity and crystal orientation angle measured by solid state NMR and X‐ray. Thermal conductivity of DF in fiber direction was dominated by that of the continuous crystal region. The thermal conductivity of the continuous crystal part estimated by the mechanical model increases from 16 to 900 mw/cmK by the increasing temperature from 10 to 150K, and thermal diffusivity of the continuous crystal part was estimated to about 100 mm2/s, which is almost temperature independent. The phonon mean free path of the continuous crystal region of DF obtained by thermal diffusivity is almost temperature independent and its value about 200 Å. With the aforementioned, the mechanical series‐parallel model composed of crystal and amorphous regions could be applied to DFs for thermal conductivity. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 1495–1503, 2005</description><identifier>ISSN: 0887-6266</identifier><identifier>EISSN: 1099-0488</identifier><identifier>DOI: 10.1002/polb.20428</identifier><identifier>CODEN: JPLPAY</identifier><language>eng</language><publisher>Hoboken: Wiley Subscription Services, Inc., A Wiley Company</publisher><subject>Applied sciences ; Exact sciences and technology ; Fibers and threads ; Forms of application and semi-finished materials ; low temperature ; polyethylene fiber ; Polymer industry, paints, wood ; Technology of polymers ; thermal conductivity</subject><ispartof>Journal of polymer science. Part B, Polymer physics, 2005-06, Vol.43 (12), p.1495-1503</ispartof><rights>Copyright © 2005 Wiley Periodicals, Inc.</rights><rights>2005 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4388-61958b9827becc55cb070fa5053aad4e5ac5d97f2affd3e2806b1daec0f121e23</citedby><cites>FETCH-LOGICAL-c4388-61958b9827becc55cb070fa5053aad4e5ac5d97f2affd3e2806b1daec0f121e23</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fpolb.20428$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fpolb.20428$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>315,781,785,1418,27926,27927,45576,45577</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=16830181$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Yamanaka, Atsuhiko</creatorcontrib><creatorcontrib>Fujishiro, Hiroyuki</creatorcontrib><creatorcontrib>Kashima, Toshihiro</creatorcontrib><creatorcontrib>Kitagawa, Tooru</creatorcontrib><creatorcontrib>Ema, Kimiko</creatorcontrib><creatorcontrib>Izumi, Yoshinobu</creatorcontrib><creatorcontrib>Ikebe, Manabu</creatorcontrib><creatorcontrib>Nishijima, Shigehiro</creatorcontrib><title>Thermal conductivity of high strength polyethylene fiber in low temperature</title><title>Journal of polymer science. Part B, Polymer physics</title><addtitle>J. Polym. Sci. B Polym. Phys</addtitle><description>High strength polyethylene fiber (Toyobo, Dyneema® fiber, hereinafter abbreviated to DF) used as reinforcement of fiber‐reinforced plastics for cryogenic use has a high thermal conductivity. To understand the thermal conductivity of DF, the relation between fiber structure and thermal conductivity of several kinds of polyethylene fibers having different modulus from 15 to 134 GPa (hereinafter abbreviated to DFs) was investigated. The mechanical series‐parallel model composed of crystal and amorphous was applied to DFs for thermal conductivity. This mechanical model was obtained by crystallinity and crystal orientation angle measured by solid state NMR and X‐ray. Thermal conductivity of DF in fiber direction was dominated by that of the continuous crystal region. The thermal conductivity of the continuous crystal part estimated by the mechanical model increases from 16 to 900 mw/cmK by the increasing temperature from 10 to 150K, and thermal diffusivity of the continuous crystal part was estimated to about 100 mm2/s, which is almost temperature independent. The phonon mean free path of the continuous crystal region of DF obtained by thermal diffusivity is almost temperature independent and its value about 200 Å. With the aforementioned, the mechanical series‐parallel model composed of crystal and amorphous regions could be applied to DFs for thermal conductivity. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 1495–1503, 2005</description><subject>Applied sciences</subject><subject>Exact sciences and technology</subject><subject>Fibers and threads</subject><subject>Forms of application and semi-finished materials</subject><subject>low temperature</subject><subject>polyethylene fiber</subject><subject>Polymer industry, paints, wood</subject><subject>Technology of polymers</subject><subject>thermal conductivity</subject><issn>0887-6266</issn><issn>1099-0488</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNp9kEFv1DAQRq2qSN0WLvwCX8oBKe3YWcfOEXZhqVi1CBXBzXKccePWm2xtLyX_npRt4cZpDvPeO3yEvGZwxgD4-XYIzRmHOVcHZMagrguYK3VIZqCULCpeVUfkOKVbgOkn6hn5fN1h3JhA7dC3O5v9T59HOjja-ZuOphyxv8kdnboj5m4M2CN1vsFIfU_D8EAzbrYYTd5FfEleOBMSvnq6J-Tbxw_Xi0_F-mp1sXi3Luy8VKqoWC1UUysuG7RWCNuABGcEiNKYdo7CWNHW0nHjXFsiV1A1rDVowTHOkJcn5M2-u43D_Q5T1hufLIZgehx2SXPFJICSE_h2D9o4pBTR6W30GxNHzUA_7qUf99J_9prg06eqSdYEF01vffpnVKoEptjEsT334AOO_ynqL1fr98_tYu_4lPHXX8fEO13JUgr9_XKll8sfcrVYftWX5W8xrItS</recordid><startdate>20050615</startdate><enddate>20050615</enddate><creator>Yamanaka, Atsuhiko</creator><creator>Fujishiro, Hiroyuki</creator><creator>Kashima, Toshihiro</creator><creator>Kitagawa, Tooru</creator><creator>Ema, Kimiko</creator><creator>Izumi, Yoshinobu</creator><creator>Ikebe, Manabu</creator><creator>Nishijima, Shigehiro</creator><general>Wiley Subscription Services, Inc., A Wiley Company</general><general>Wiley</general><scope>BSCLL</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20050615</creationdate><title>Thermal conductivity of high strength polyethylene fiber in low temperature</title><author>Yamanaka, Atsuhiko ; Fujishiro, Hiroyuki ; Kashima, Toshihiro ; Kitagawa, Tooru ; Ema, Kimiko ; Izumi, Yoshinobu ; Ikebe, Manabu ; Nishijima, Shigehiro</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4388-61958b9827becc55cb070fa5053aad4e5ac5d97f2affd3e2806b1daec0f121e23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>Applied sciences</topic><topic>Exact sciences and technology</topic><topic>Fibers and threads</topic><topic>Forms of application and semi-finished materials</topic><topic>low temperature</topic><topic>polyethylene fiber</topic><topic>Polymer industry, paints, wood</topic><topic>Technology of polymers</topic><topic>thermal conductivity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yamanaka, Atsuhiko</creatorcontrib><creatorcontrib>Fujishiro, Hiroyuki</creatorcontrib><creatorcontrib>Kashima, Toshihiro</creatorcontrib><creatorcontrib>Kitagawa, Tooru</creatorcontrib><creatorcontrib>Ema, Kimiko</creatorcontrib><creatorcontrib>Izumi, Yoshinobu</creatorcontrib><creatorcontrib>Ikebe, Manabu</creatorcontrib><creatorcontrib>Nishijima, Shigehiro</creatorcontrib><collection>Istex</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of polymer science. Part B, Polymer physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yamanaka, Atsuhiko</au><au>Fujishiro, Hiroyuki</au><au>Kashima, Toshihiro</au><au>Kitagawa, Tooru</au><au>Ema, Kimiko</au><au>Izumi, Yoshinobu</au><au>Ikebe, Manabu</au><au>Nishijima, Shigehiro</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Thermal conductivity of high strength polyethylene fiber in low temperature</atitle><jtitle>Journal of polymer science. Part B, Polymer physics</jtitle><addtitle>J. Polym. Sci. B Polym. Phys</addtitle><date>2005-06-15</date><risdate>2005</risdate><volume>43</volume><issue>12</issue><spage>1495</spage><epage>1503</epage><pages>1495-1503</pages><issn>0887-6266</issn><eissn>1099-0488</eissn><coden>JPLPAY</coden><abstract>High strength polyethylene fiber (Toyobo, Dyneema® fiber, hereinafter abbreviated to DF) used as reinforcement of fiber‐reinforced plastics for cryogenic use has a high thermal conductivity. To understand the thermal conductivity of DF, the relation between fiber structure and thermal conductivity of several kinds of polyethylene fibers having different modulus from 15 to 134 GPa (hereinafter abbreviated to DFs) was investigated. The mechanical series‐parallel model composed of crystal and amorphous was applied to DFs for thermal conductivity. This mechanical model was obtained by crystallinity and crystal orientation angle measured by solid state NMR and X‐ray. Thermal conductivity of DF in fiber direction was dominated by that of the continuous crystal region. The thermal conductivity of the continuous crystal part estimated by the mechanical model increases from 16 to 900 mw/cmK by the increasing temperature from 10 to 150K, and thermal diffusivity of the continuous crystal part was estimated to about 100 mm2/s, which is almost temperature independent. The phonon mean free path of the continuous crystal region of DF obtained by thermal diffusivity is almost temperature independent and its value about 200 Å. With the aforementioned, the mechanical series‐parallel model composed of crystal and amorphous regions could be applied to DFs for thermal conductivity. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 1495–1503, 2005</abstract><cop>Hoboken</cop><pub>Wiley Subscription Services, Inc., A Wiley Company</pub><doi>10.1002/polb.20428</doi><tpages>9</tpages></addata></record> |
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subjects | Applied sciences Exact sciences and technology Fibers and threads Forms of application and semi-finished materials low temperature polyethylene fiber Polymer industry, paints, wood Technology of polymers thermal conductivity |
title | Thermal conductivity of high strength polyethylene fiber in low temperature |
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