An express technique for the determination of static and dynamic fracture toughness ( KIC, KId) of bcc metals and alloys
Despite many investigations carried out during the last four decades on the fracture mechanics, a reliable, easy and economical technique has not been developed for low and middle strength (low carbon low alloyed) steels which have a widespread use in metallic constructions. This prohibited the reli...
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Veröffentlicht in: | Mechanics of materials 2004-11, Vol.36 (11), p.1129-1142 |
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description | Despite many investigations carried out during the last four decades on the fracture mechanics, a reliable, easy and economical technique has not been developed for low and middle strength (low carbon low alloyed) steels which have a widespread use in metallic constructions. This prohibited the reliability of such constructions in view of fracture mechanics. The technique described in the ASTM E399 Standard is very troublesome and this hindered the evaluation of fracture toughness of many steels exhibiting similar properties, because the Standard requires very big samples to satisfy the plane strain conditions. This study, which depends on a 20 years investigation, explains an express technique for the determination of fracture toughness of bcc metals and alloys for the temperatures 0⩽
T⩽0.2
T
melt [K] and for the deformation rate
ε
′⩽10
5 s
−1. According to the proposed technique,
K
IC (
T,
ε
′) graph can be constructed by only two experiments: one is a uniaxial tension test at room temperature with a small smooth cylindrical specimen and the other is a fracture toughness test at a low temperature (i.e. 77 K) in accordance with ASTM E399. At this temperature the cracked sample is also very small. The mathematical relations obtained on a realistic theoretical base give results similar to experimentally obtained previous results in a high accuracy. The main assumptions in the theoretical base contain two observations: (1) the fracture toughness exponentially depends on the thermoactivation energy of plastic deformation at the crack tip, (2) a microcrack is formed at a certain distance ahead of the crack tip under a critical stress and this is unified with the main crack to cause the growth. |
doi_str_mv | 10.1016/j.mechmat.2003.11.005 |
format | Article |
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T⩽0.2
T
melt [K] and for the deformation rate
ε
′⩽10
5 s
−1. According to the proposed technique,
K
IC (
T,
ε
′) graph can be constructed by only two experiments: one is a uniaxial tension test at room temperature with a small smooth cylindrical specimen and the other is a fracture toughness test at a low temperature (i.e. 77 K) in accordance with ASTM E399. At this temperature the cracked sample is also very small. The mathematical relations obtained on a realistic theoretical base give results similar to experimentally obtained previous results in a high accuracy. The main assumptions in the theoretical base contain two observations: (1) the fracture toughness exponentially depends on the thermoactivation energy of plastic deformation at the crack tip, (2) a microcrack is formed at a certain distance ahead of the crack tip under a critical stress and this is unified with the main crack to cause the growth.</description><identifier>ISSN: 0167-6636</identifier><identifier>EISSN: 1872-7743</identifier><identifier>DOI: 10.1016/j.mechmat.2003.11.005</identifier><identifier>CODEN: MSMSD3</identifier><language>eng</language><publisher>Lausanne: Elsevier Ltd</publisher><subject>Exact sciences and technology ; Fracture mechanics (crack, fatigue, damage...) ; Fracture toughness ; Fundamental areas of phenomenology (including applications) ; Physics ; Solid mechanics ; Structural and continuum mechanics ; Temperature ; Theory and numerical methods ; Thermoactivation energy ; Yield strength</subject><ispartof>Mechanics of materials, 2004-11, Vol.36 (11), p.1129-1142</ispartof><rights>2003 Elsevier Ltd</rights><rights>2004 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c368t-b5808d873b09aa44106017bd4f62a2c1b874792d96b4f5ed17d74fb0080a77963</citedby><cites>FETCH-LOGICAL-c368t-b5808d873b09aa44106017bd4f62a2c1b874792d96b4f5ed17d74fb0080a77963</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.mechmat.2003.11.005$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3549,27923,27924,45994</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=15896551$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Said, Galip</creatorcontrib><creatorcontrib>Tasgetiren, Suleyman</creatorcontrib><title>An express technique for the determination of static and dynamic fracture toughness ( KIC, KId) of bcc metals and alloys</title><title>Mechanics of materials</title><description>Despite many investigations carried out during the last four decades on the fracture mechanics, a reliable, easy and economical technique has not been developed for low and middle strength (low carbon low alloyed) steels which have a widespread use in metallic constructions. This prohibited the reliability of such constructions in view of fracture mechanics. The technique described in the ASTM E399 Standard is very troublesome and this hindered the evaluation of fracture toughness of many steels exhibiting similar properties, because the Standard requires very big samples to satisfy the plane strain conditions. This study, which depends on a 20 years investigation, explains an express technique for the determination of fracture toughness of bcc metals and alloys for the temperatures 0⩽
T⩽0.2
T
melt [K] and for the deformation rate
ε
′⩽10
5 s
−1. According to the proposed technique,
K
IC (
T,
ε
′) graph can be constructed by only two experiments: one is a uniaxial tension test at room temperature with a small smooth cylindrical specimen and the other is a fracture toughness test at a low temperature (i.e. 77 K) in accordance with ASTM E399. At this temperature the cracked sample is also very small. The mathematical relations obtained on a realistic theoretical base give results similar to experimentally obtained previous results in a high accuracy. The main assumptions in the theoretical base contain two observations: (1) the fracture toughness exponentially depends on the thermoactivation energy of plastic deformation at the crack tip, (2) a microcrack is formed at a certain distance ahead of the crack tip under a critical stress and this is unified with the main crack to cause the growth.</description><subject>Exact sciences and technology</subject><subject>Fracture mechanics (crack, fatigue, damage...)</subject><subject>Fracture toughness</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Physics</subject><subject>Solid mechanics</subject><subject>Structural and continuum mechanics</subject><subject>Temperature</subject><subject>Theory and numerical methods</subject><subject>Thermoactivation energy</subject><subject>Yield strength</subject><issn>0167-6636</issn><issn>1872-7743</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNqFkE1rGzEQhkVpIK6TnxDQpaWF7EbaD0l7KsHkixhyac5CK83WMruSK8kl_vfVxoYec5kZhud9h3kRuqKkpISym205gd5MKpUVIXVJaUlI-wktqOBVwXlTf0aLzPGCsZqdoy8xbkkmupYv0Nutw_C2CxAjTtnF2T97wIMPOG0AG0gQJutUst5hP-CY8qixcgabg1NTnoegdNoHwMnvf2_cbPQdPz-trnMxP2ZRrzWeIKkxvgvVOPpDvEBnQ97A5akv0ev93a_VY7F-eXha3a4LXTORir4VRBjB6550SjUNJYxQ3ptmYJWqNO0Fb3hXmY71zdCCodzwZugJEURx3rF6ib4dfXfB59dikpONGsZROfD7KCtRV6xuZrA9gjr4GAMMchfspMJBUiLnnOVWnnKWc86SUplTzLqvpwMqajXmOJy28b-4FR1rW5q5n0cO8rd_LQQZtQWnwdgAOknj7QeX_gEtJ5W4</recordid><startdate>20041101</startdate><enddate>20041101</enddate><creator>Said, Galip</creator><creator>Tasgetiren, Suleyman</creator><general>Elsevier Ltd</general><general>Elsevier Science</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>8BQ</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>JG9</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>20041101</creationdate><title>An express technique for the determination of static and dynamic fracture toughness ( KIC, KId) of bcc metals and alloys</title><author>Said, Galip ; Tasgetiren, Suleyman</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c368t-b5808d873b09aa44106017bd4f62a2c1b874792d96b4f5ed17d74fb0080a77963</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><topic>Exact sciences and technology</topic><topic>Fracture mechanics (crack, fatigue, damage...)</topic><topic>Fracture toughness</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Physics</topic><topic>Solid mechanics</topic><topic>Structural and continuum mechanics</topic><topic>Temperature</topic><topic>Theory and numerical methods</topic><topic>Thermoactivation energy</topic><topic>Yield strength</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Said, Galip</creatorcontrib><creatorcontrib>Tasgetiren, Suleyman</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Mechanics of materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Said, Galip</au><au>Tasgetiren, Suleyman</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>An express technique for the determination of static and dynamic fracture toughness ( KIC, KId) of bcc metals and alloys</atitle><jtitle>Mechanics of materials</jtitle><date>2004-11-01</date><risdate>2004</risdate><volume>36</volume><issue>11</issue><spage>1129</spage><epage>1142</epage><pages>1129-1142</pages><issn>0167-6636</issn><eissn>1872-7743</eissn><coden>MSMSD3</coden><abstract>Despite many investigations carried out during the last four decades on the fracture mechanics, a reliable, easy and economical technique has not been developed for low and middle strength (low carbon low alloyed) steels which have a widespread use in metallic constructions. This prohibited the reliability of such constructions in view of fracture mechanics. The technique described in the ASTM E399 Standard is very troublesome and this hindered the evaluation of fracture toughness of many steels exhibiting similar properties, because the Standard requires very big samples to satisfy the plane strain conditions. This study, which depends on a 20 years investigation, explains an express technique for the determination of fracture toughness of bcc metals and alloys for the temperatures 0⩽
T⩽0.2
T
melt [K] and for the deformation rate
ε
′⩽10
5 s
−1. According to the proposed technique,
K
IC (
T,
ε
′) graph can be constructed by only two experiments: one is a uniaxial tension test at room temperature with a small smooth cylindrical specimen and the other is a fracture toughness test at a low temperature (i.e. 77 K) in accordance with ASTM E399. At this temperature the cracked sample is also very small. The mathematical relations obtained on a realistic theoretical base give results similar to experimentally obtained previous results in a high accuracy. The main assumptions in the theoretical base contain two observations: (1) the fracture toughness exponentially depends on the thermoactivation energy of plastic deformation at the crack tip, (2) a microcrack is formed at a certain distance ahead of the crack tip under a critical stress and this is unified with the main crack to cause the growth.</abstract><cop>Lausanne</cop><cop>Amsterdam</cop><cop>New York, NY</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.mechmat.2003.11.005</doi><tpages>14</tpages></addata></record> |
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source | Elsevier ScienceDirect Journals Complete - AutoHoldings |
subjects | Exact sciences and technology Fracture mechanics (crack, fatigue, damage...) Fracture toughness Fundamental areas of phenomenology (including applications) Physics Solid mechanics Structural and continuum mechanics Temperature Theory and numerical methods Thermoactivation energy Yield strength |
title | An express technique for the determination of static and dynamic fracture toughness ( KIC, KId) of bcc metals and alloys |
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