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Creep at very low rates

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dc.contributor.author Nabarro, FRN en_US
dc.date.accessioned 2007-03-26T11:40:43Z en_US
dc.date.accessioned 2007-06-07T10:08:03Z
dc.date.available 2007-03-26T11:40:43Z en_US
dc.date.available 2007-06-07T10:08:03Z
dc.date.issued 2002-02 en_US
dc.identifier.citation Nabarro, FRN. 2002. Creep at very low rates. Metallurgical and Materials Transactions A, vol. 33(2), pp 213-218 en_US
dc.identifier.issn 1073-5623 en_US
dc.identifier.uri http://hdl.handle.net/10204/2055 en_US
dc.description.abstract The creep rate in a land-based power station must be less than 10(-11) s(-1). At these low rates of deformation the transport of matter occurs by the migration of vacancies rather than by the glide of dislocations. A quantitative understanding of these diffusional processes is, therefore, important. First type of diffusional creep (Nabarro-Herring (N-H)): the sources and sinks of vacancies are grain boundaries. The vacancies may diffuse through the bulk of the grain or along the grain boundaries (Coble (C)). Second type (Harper-Dorn (H-D)): the vacancies diffuse from edge dislocations with their Burgers vectors parallel to the major tensile axis to those with Burgers vectors perpendicular to this axis. The coherence of the polycrystalline aggregate is maintained by sliding along the grain boundaries. The three mechanisms of vacancy migration, grain boundary sliding, and dislocation glide may all interact. The theories of N-H and C creep in pure metals are established and confirmed, but H-D creep and grain boundary sliding are less well understood. Practical engineering materials are usually strengthened by precipitates that accumulate on grain boundaries and slow down creep in complicated ways. en_US
dc.format.extent 77368 bytes en_US
dc.format.mimetype application/pdf en_US
dc.language.iso en en_US
dc.publisher Minerals Metals Materials Society en_US
dc.rights Copyright: 2002 Minerals Metals Materials Society en_US
dc.subject Creep rates en_US
dc.subject Dislocations en_US
dc.subject Diffusional creeps en_US
dc.subject Mechanisms of vacancy migration en_US
dc.subject Materials sciences en_US
dc.subject Metallurgical engineering en_US
dc.title Creep at very low rates en_US
dc.type Article en_US
dc.identifier.apacitation Nabarro, F. (2002). Creep at very low rates. http://hdl.handle.net/10204/2055 en_ZA
dc.identifier.chicagocitation Nabarro, FRN "Creep at very low rates." (2002) http://hdl.handle.net/10204/2055 en_ZA
dc.identifier.vancouvercitation Nabarro F. Creep at very low rates. 2002; http://hdl.handle.net/10204/2055. en_ZA
dc.identifier.ris TY - Article AU - Nabarro, FRN AB - The creep rate in a land-based power station must be less than 10(-11) s(-1). At these low rates of deformation the transport of matter occurs by the migration of vacancies rather than by the glide of dislocations. A quantitative understanding of these diffusional processes is, therefore, important. First type of diffusional creep (Nabarro-Herring (N-H)): the sources and sinks of vacancies are grain boundaries. The vacancies may diffuse through the bulk of the grain or along the grain boundaries (Coble (C)). Second type (Harper-Dorn (H-D)): the vacancies diffuse from edge dislocations with their Burgers vectors parallel to the major tensile axis to those with Burgers vectors perpendicular to this axis. The coherence of the polycrystalline aggregate is maintained by sliding along the grain boundaries. The three mechanisms of vacancy migration, grain boundary sliding, and dislocation glide may all interact. The theories of N-H and C creep in pure metals are established and confirmed, but H-D creep and grain boundary sliding are less well understood. Practical engineering materials are usually strengthened by precipitates that accumulate on grain boundaries and slow down creep in complicated ways. DA - 2002-02 DB - ResearchSpace DP - CSIR KW - Creep rates KW - Dislocations KW - Diffusional creeps KW - Mechanisms of vacancy migration KW - Materials sciences KW - Metallurgical engineering LK - https://researchspace.csir.co.za PY - 2002 SM - 1073-5623 T1 - Creep at very low rates TI - Creep at very low rates UR - http://hdl.handle.net/10204/2055 ER - en_ZA


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