Tensile creep of polycrystalline near-stoichiometric NiAl
Long term tensile creep studies were conducted on binary NiAl in the temperature range 700–1200 K with the objectives of characterizing and understanding the creep mechanisms. Inverse and normal primary creep curves were observed depending on stress and temperature. It is concluded that the primary...
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Veröffentlicht in: | Materials science & engineering. A, Structural materials : properties, microstructure and processing Structural materials : properties, microstructure and processing, 2003-09, Vol.356 (1), p.283-297 |
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description | Long term tensile creep studies were conducted on binary NiAl in the temperature range 700–1200 K with the objectives of characterizing and understanding the creep mechanisms. Inverse and normal primary creep curves were observed depending on stress and temperature. It is concluded that the primary creep of NiAl is limited by dislocation mobility. The stress exponent for creep, n, decreased from 13.9 at 700 K to 5.5 at 1200 K. The true activation energy for creep, Q
c, was constant and equal to about 400 kJ mol
−1 between 20 and 50 MPa but decreased to a constant value of 250 kJ mol
−1 between 50 and 110 MPa. The activation energy was observed to be stress dependent above 110 MPa. The tensile creep results reported in this investigation were compared with compression creep data reported in the literature. A detailed discussion of the probable dislocation creep mechanisms governing compressive and tensile creep of NiAl is presented. It is concluded that the non-conservative motion of jogs on screw dislocations influenced the nature of the primary creep curves, where the climb of these jogs involves either the next nearest neighbor or the six-jump cycle vacancy diffusion mechanism. A phenomenological model discusses the nature of the atom–vacancy exchange process likely to lead to the climb of these jogs. |
doi_str_mv | 10.1016/S0921-5093(03)00137-0 |
format | Article |
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c, was constant and equal to about 400 kJ mol
−1 between 20 and 50 MPa but decreased to a constant value of 250 kJ mol
−1 between 50 and 110 MPa. The activation energy was observed to be stress dependent above 110 MPa. The tensile creep results reported in this investigation were compared with compression creep data reported in the literature. A detailed discussion of the probable dislocation creep mechanisms governing compressive and tensile creep of NiAl is presented. It is concluded that the non-conservative motion of jogs on screw dislocations influenced the nature of the primary creep curves, where the climb of these jogs involves either the next nearest neighbor or the six-jump cycle vacancy diffusion mechanism. A phenomenological model discusses the nature of the atom–vacancy exchange process likely to lead to the climb of these jogs.</description><identifier>ISSN: 0921-5093</identifier><identifier>EISSN: 1873-4936</identifier><identifier>DOI: 10.1016/S0921-5093(03)00137-0</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>Activation energy ; Applied sciences ; Condensed matter: structure, mechanical and thermal properties ; Creep ; Exact sciences and technology ; High temperature deformation ; Mechanical and acoustical properties of condensed matter ; Mechanical properties of solids ; Metals. Metallurgy ; NiAl ; Physics ; Primary creep ; Tensile creep</subject><ispartof>Materials science & engineering. A, Structural materials : properties, microstructure and processing, 2003-09, Vol.356 (1), p.283-297</ispartof><rights>2003 Elsevier Science B.V.</rights><rights>2003 INIST-CNRS</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c415t-ba24e237dab66540e588760c7148ea6fc286d2eefb6dae6d132601043df646b3</citedby><cites>FETCH-LOGICAL-c415t-ba24e237dab66540e588760c7148ea6fc286d2eefb6dae6d132601043df646b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/S0921-5093(03)00137-0$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=14942104$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Raj, S.V.</creatorcontrib><title>Tensile creep of polycrystalline near-stoichiometric NiAl</title><title>Materials science & engineering. A, Structural materials : properties, microstructure and processing</title><description>Long term tensile creep studies were conducted on binary NiAl in the temperature range 700–1200 K with the objectives of characterizing and understanding the creep mechanisms. Inverse and normal primary creep curves were observed depending on stress and temperature. It is concluded that the primary creep of NiAl is limited by dislocation mobility. The stress exponent for creep, n, decreased from 13.9 at 700 K to 5.5 at 1200 K. The true activation energy for creep, Q
c, was constant and equal to about 400 kJ mol
−1 between 20 and 50 MPa but decreased to a constant value of 250 kJ mol
−1 between 50 and 110 MPa. The activation energy was observed to be stress dependent above 110 MPa. The tensile creep results reported in this investigation were compared with compression creep data reported in the literature. A detailed discussion of the probable dislocation creep mechanisms governing compressive and tensile creep of NiAl is presented. It is concluded that the non-conservative motion of jogs on screw dislocations influenced the nature of the primary creep curves, where the climb of these jogs involves either the next nearest neighbor or the six-jump cycle vacancy diffusion mechanism. A phenomenological model discusses the nature of the atom–vacancy exchange process likely to lead to the climb of these jogs.</description><subject>Activation energy</subject><subject>Applied sciences</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Creep</subject><subject>Exact sciences and technology</subject><subject>High temperature deformation</subject><subject>Mechanical and acoustical properties of condensed matter</subject><subject>Mechanical properties of solids</subject><subject>Metals. Metallurgy</subject><subject>NiAl</subject><subject>Physics</subject><subject>Primary creep</subject><subject>Tensile creep</subject><issn>0921-5093</issn><issn>1873-4936</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2003</creationdate><recordtype>article</recordtype><recordid>eNqFkEtLxDAQgIMouFZ_gtCLoofq5NG0Pcmy-IJFD-49pOkUI9mmJl1h_72tu-hRGJg5fPP6CDmncEOByts3qBjNcqj4FfBrAMqLDA7IjJYFz0TF5SGZ_SLH5CTGDxgpAfmMVCvsonWYmoDYp75Ne--2JmzjoJ2zHaYd6pDFwVvzbv0ah2BN-mLn7pQctdpFPNvnhKwe7leLp2z5-vi8mC8zI2g-ZLVmAhkvGl1LmQvAvCwLCaagokQtW8NK2TDEtpaNRtlQziRQELxppZA1T8jlbmwf_OcG46DWNhp0TnfoN1GxEgpW0nwE8x1ogo8xYKv6YNc6bBUFNXlSP57UJEHBGJOnsUjIxX6Bjka7NujO2PjXLCrBpnsScrfjcHz2y2JQ0VjsDDY2oBlU4-0_m74BhtR77w</recordid><startdate>20030915</startdate><enddate>20030915</enddate><creator>Raj, S.V.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20030915</creationdate><title>Tensile creep of polycrystalline near-stoichiometric NiAl</title><author>Raj, S.V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c415t-ba24e237dab66540e588760c7148ea6fc286d2eefb6dae6d132601043df646b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><topic>Activation energy</topic><topic>Applied sciences</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Creep</topic><topic>Exact sciences and technology</topic><topic>High temperature deformation</topic><topic>Mechanical and acoustical properties of condensed matter</topic><topic>Mechanical properties of solids</topic><topic>Metals. Metallurgy</topic><topic>NiAl</topic><topic>Physics</topic><topic>Primary creep</topic><topic>Tensile creep</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Raj, S.V.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Materials science & engineering. A, Structural materials : properties, microstructure and processing</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Raj, S.V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Tensile creep of polycrystalline near-stoichiometric NiAl</atitle><jtitle>Materials science & engineering. A, Structural materials : properties, microstructure and processing</jtitle><date>2003-09-15</date><risdate>2003</risdate><volume>356</volume><issue>1</issue><spage>283</spage><epage>297</epage><pages>283-297</pages><issn>0921-5093</issn><eissn>1873-4936</eissn><abstract>Long term tensile creep studies were conducted on binary NiAl in the temperature range 700–1200 K with the objectives of characterizing and understanding the creep mechanisms. Inverse and normal primary creep curves were observed depending on stress and temperature. It is concluded that the primary creep of NiAl is limited by dislocation mobility. The stress exponent for creep, n, decreased from 13.9 at 700 K to 5.5 at 1200 K. The true activation energy for creep, Q
c, was constant and equal to about 400 kJ mol
−1 between 20 and 50 MPa but decreased to a constant value of 250 kJ mol
−1 between 50 and 110 MPa. The activation energy was observed to be stress dependent above 110 MPa. The tensile creep results reported in this investigation were compared with compression creep data reported in the literature. A detailed discussion of the probable dislocation creep mechanisms governing compressive and tensile creep of NiAl is presented. It is concluded that the non-conservative motion of jogs on screw dislocations influenced the nature of the primary creep curves, where the climb of these jogs involves either the next nearest neighbor or the six-jump cycle vacancy diffusion mechanism. A phenomenological model discusses the nature of the atom–vacancy exchange process likely to lead to the climb of these jogs.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/S0921-5093(03)00137-0</doi><tpages>15</tpages><oa>free_for_read</oa></addata></record> |
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source | ScienceDirect Journals (5 years ago - present) |
subjects | Activation energy Applied sciences Condensed matter: structure, mechanical and thermal properties Creep Exact sciences and technology High temperature deformation Mechanical and acoustical properties of condensed matter Mechanical properties of solids Metals. Metallurgy NiAl Physics Primary creep Tensile creep |
title | Tensile creep of polycrystalline near-stoichiometric NiAl |
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