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Influence of repetitive stiffness variation on crack growth behaviour in wood
Softwoods have a repetitive variation in stiffness over their growth rings, which is due to the difference in cellular structure between the latewood and earlywood. In this paper, the influence of the repetitive stiffness variation on radially growing cracks is studied by detailed finite element ana...
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Published in: | Journal of materials science 2000-12, Vol.35 (24), p.6259-6266 |
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creator | Thuvander, F Jernkvist, L. O Gunnars, J |
description | Softwoods have a repetitive variation in stiffness over their growth rings, which is due to the difference in cellular structure between the latewood and earlywood. In this paper, the influence of the repetitive stiffness variation on radially growing cracks is studied by detailed finite element analyses, in which the wood material is represented by a layered orthotropic continuum. The distribution of stress around the crack is found to be very different from crack tip stress fields in homogenous isotropic materials. The latewood layer ahead of the crack experiences a significant tensile stress, which indicates that formation of new secondary cracks ahead of the primary crack front is a likely mechanism for crack propagation. This mechanism is also favoured by the fact that the primary crack is subjected to a significant shielding from the stiff latewood, which tends to arrest the primary crack in the soft earlywood layer. Analyses are performed for materials with various growth ring widths, and the calculated results are compared with reported experimental observations. |
doi_str_mv | 10.1023/A:1026766203501 |
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O ; Gunnars, J</creator><creatorcontrib>Thuvander, F ; Jernkvist, L. O ; Gunnars, J</creatorcontrib><description>Softwoods have a repetitive variation in stiffness over their growth rings, which is due to the difference in cellular structure between the latewood and earlywood. In this paper, the influence of the repetitive stiffness variation on radially growing cracks is studied by detailed finite element analyses, in which the wood material is represented by a layered orthotropic continuum. The distribution of stress around the crack is found to be very different from crack tip stress fields in homogenous isotropic materials. The latewood layer ahead of the crack experiences a significant tensile stress, which indicates that formation of new secondary cracks ahead of the primary crack front is a likely mechanism for crack propagation. This mechanism is also favoured by the fact that the primary crack is subjected to a significant shielding from the stiff latewood, which tends to arrest the primary crack in the soft earlywood layer. Analyses are performed for materials with various growth ring widths, and the calculated results are compared with reported experimental observations.</description><identifier>ISSN: 0022-2461</identifier><identifier>ISSN: 1573-4803</identifier><identifier>EISSN: 1573-4803</identifier><identifier>DOI: 10.1023/A:1026766203501</identifier><identifier>CODEN: JMTSAS</identifier><language>eng</language><publisher>Heidelberg: Kluwer Academic Publishers</publisher><subject>Applied sciences ; cell structures ; Cellular structure ; Crack propagation ; Crack tips ; Cracks ; earlywood ; Exact sciences and technology ; finite element analysis ; Finite element method ; Hållfasthetslära ; Isotropic material ; latewood ; Materials science ; Mathematical analysis ; Polymer industry, paints, wood ; Polymera konstruktionsmaterial ; Polymeric Composite Materials ; Properties and testing ; Shielding ; softwood ; Softwoods ; Solid Mechanics ; Stiffness ; Stress concentration ; Stress distribution ; Tensile stress ; Wood ; Wood. Paper. Non wovens</subject><ispartof>Journal of materials science, 2000-12, Vol.35 (24), p.6259-6266</ispartof><rights>2001 INIST-CNRS</rights><rights>Journal of Materials Science is a copyright of Springer, (2000). All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c347t-3b5a6781f405e70880aedaa49f1b7107416358a36b97ea77914bc12f81377743</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27901,27902</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=826888$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://urn.kb.se/resolve?urn=urn:nbn:se:ltu:diva-13828$$DView record from Swedish Publication Index$$Hfree_for_read</backlink></links><search><creatorcontrib>Thuvander, F</creatorcontrib><creatorcontrib>Jernkvist, L. O</creatorcontrib><creatorcontrib>Gunnars, J</creatorcontrib><title>Influence of repetitive stiffness variation on crack growth behaviour in wood</title><title>Journal of materials science</title><description>Softwoods have a repetitive variation in stiffness over their growth rings, which is due to the difference in cellular structure between the latewood and earlywood. In this paper, the influence of the repetitive stiffness variation on radially growing cracks is studied by detailed finite element analyses, in which the wood material is represented by a layered orthotropic continuum. The distribution of stress around the crack is found to be very different from crack tip stress fields in homogenous isotropic materials. The latewood layer ahead of the crack experiences a significant tensile stress, which indicates that formation of new secondary cracks ahead of the primary crack front is a likely mechanism for crack propagation. This mechanism is also favoured by the fact that the primary crack is subjected to a significant shielding from the stiff latewood, which tends to arrest the primary crack in the soft earlywood layer. Analyses are performed for materials with various growth ring widths, and the calculated results are compared with reported experimental observations.</description><subject>Applied sciences</subject><subject>cell structures</subject><subject>Cellular structure</subject><subject>Crack propagation</subject><subject>Crack tips</subject><subject>Cracks</subject><subject>earlywood</subject><subject>Exact sciences and technology</subject><subject>finite element analysis</subject><subject>Finite element method</subject><subject>Hållfasthetslära</subject><subject>Isotropic material</subject><subject>latewood</subject><subject>Materials science</subject><subject>Mathematical analysis</subject><subject>Polymer industry, paints, wood</subject><subject>Polymera konstruktionsmaterial</subject><subject>Polymeric Composite Materials</subject><subject>Properties and testing</subject><subject>Shielding</subject><subject>softwood</subject><subject>Softwoods</subject><subject>Solid Mechanics</subject><subject>Stiffness</subject><subject>Stress concentration</subject><subject>Stress distribution</subject><subject>Tensile stress</subject><subject>Wood</subject><subject>Wood. Paper. Non wovens</subject><issn>0022-2461</issn><issn>1573-4803</issn><issn>1573-4803</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2000</creationdate><recordtype>article</recordtype><recordid>eNpd0MtrFEEQB-AmKLhGzx7TEPCU0ap-j7cl8RGIeDB6bWom3ZtOJtNr98wu_vdO2CAiFPwuH_Vi7A3COwQh368_LGGsMQKkBjxiK9RWNsqBfMZWAEI0Qhl8wV7WegcA2gpcsa-XYxzmMPaB58hL2IYpTWkXeJ1SjGOole-oJJpSHvlSfaH-nm9K3k-3vAu3tEt5LjyNfJ_zzSv2PNJQw-unPGbXnz5en39prr59vjxfXzW9VHZqZKfJWIdRgQ4WnAMKN0SqjdhZBKvQSO1Imq61gaxtUXU9iuhQWmuVPGZnh7Z1H7Zz57clPVD57TMlf5F-rn0uGz9Ms0fphFv42wPflvxrDnXyD6n2YRhoDHmuXljtAJRZ4Ol_8G45blwu8ULo1rVOS_uPotrTEAuNfap_l3DCOPc49OSgImVPm7KIH98FoFlej1YiyD8yl4GL</recordid><startdate>20001201</startdate><enddate>20001201</enddate><creator>Thuvander, F</creator><creator>Jernkvist, L. 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O ; Gunnars, J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c347t-3b5a6781f405e70880aedaa49f1b7107416358a36b97ea77914bc12f81377743</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2000</creationdate><topic>Applied sciences</topic><topic>cell structures</topic><topic>Cellular structure</topic><topic>Crack propagation</topic><topic>Crack tips</topic><topic>Cracks</topic><topic>earlywood</topic><topic>Exact sciences and technology</topic><topic>finite element analysis</topic><topic>Finite element method</topic><topic>Hållfasthetslära</topic><topic>Isotropic material</topic><topic>latewood</topic><topic>Materials science</topic><topic>Mathematical analysis</topic><topic>Polymer industry, paints, wood</topic><topic>Polymera konstruktionsmaterial</topic><topic>Polymeric Composite Materials</topic><topic>Properties and testing</topic><topic>Shielding</topic><topic>softwood</topic><topic>Softwoods</topic><topic>Solid Mechanics</topic><topic>Stiffness</topic><topic>Stress concentration</topic><topic>Stress distribution</topic><topic>Tensile stress</topic><topic>Wood</topic><topic>Wood. Paper. Non wovens</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Thuvander, F</creatorcontrib><creatorcontrib>Jernkvist, L. 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O</au><au>Gunnars, J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Influence of repetitive stiffness variation on crack growth behaviour in wood</atitle><jtitle>Journal of materials science</jtitle><date>2000-12-01</date><risdate>2000</risdate><volume>35</volume><issue>24</issue><spage>6259</spage><epage>6266</epage><pages>6259-6266</pages><issn>0022-2461</issn><issn>1573-4803</issn><eissn>1573-4803</eissn><coden>JMTSAS</coden><abstract>Softwoods have a repetitive variation in stiffness over their growth rings, which is due to the difference in cellular structure between the latewood and earlywood. In this paper, the influence of the repetitive stiffness variation on radially growing cracks is studied by detailed finite element analyses, in which the wood material is represented by a layered orthotropic continuum. The distribution of stress around the crack is found to be very different from crack tip stress fields in homogenous isotropic materials. The latewood layer ahead of the crack experiences a significant tensile stress, which indicates that formation of new secondary cracks ahead of the primary crack front is a likely mechanism for crack propagation. This mechanism is also favoured by the fact that the primary crack is subjected to a significant shielding from the stiff latewood, which tends to arrest the primary crack in the soft earlywood layer. Analyses are performed for materials with various growth ring widths, and the calculated results are compared with reported experimental observations.</abstract><cop>Heidelberg</cop><pub>Kluwer Academic Publishers</pub><doi>10.1023/A:1026766203501</doi><tpages>8</tpages></addata></record> |
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subjects | Applied sciences cell structures Cellular structure Crack propagation Crack tips Cracks earlywood Exact sciences and technology finite element analysis Finite element method Hållfasthetslära Isotropic material latewood Materials science Mathematical analysis Polymer industry, paints, wood Polymera konstruktionsmaterial Polymeric Composite Materials Properties and testing Shielding softwood Softwoods Solid Mechanics Stiffness Stress concentration Stress distribution Tensile stress Wood Wood. Paper. Non wovens |
title | Influence of repetitive stiffness variation on crack growth behaviour in wood |
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