2013
DOI: 10.1016/j.msea.2012.08.042
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Temperature dependence of strengthening mechanisms in the nanostructured ferritic alloy 14YWT: Part I—Mechanical and microstructural observations

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Cited by 70 publications
(38 citation statements)
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“…16 which suggests that FSW causes the complete loss of particle strengthening even for the low heat input condition. This overall conclusion is also strongly supported by research by Kim on 14YWT which concluded that oxide particles greater than 100 nm in size (comparable to all oxide particles following FSW in this research) would result in s P being less than 50 MPa [53,54]. It is worth noting that particles in 14YWT are Y-Ti-O particles as opposed to the Y-Al-O particles in MA956 and the work by Kim did not include any conditions that would cause a comparable degree of particle coarsening as that seen here, but the calculation method used by Kim is very similar to that presented by Wang and used here in Eq.…”
Section: Discussionsupporting
confidence: 83%
“…16 which suggests that FSW causes the complete loss of particle strengthening even for the low heat input condition. This overall conclusion is also strongly supported by research by Kim on 14YWT which concluded that oxide particles greater than 100 nm in size (comparable to all oxide particles following FSW in this research) would result in s P being less than 50 MPa [53,54]. It is worth noting that particles in 14YWT are Y-Ti-O particles as opposed to the Y-Al-O particles in MA956 and the work by Kim did not include any conditions that would cause a comparable degree of particle coarsening as that seen here, but the calculation method used by Kim is very similar to that presented by Wang and used here in Eq.…”
Section: Discussionsupporting
confidence: 83%
“…5 times finer particles and 100 times more particles), the athermal Orowan strengthening at low temperatures can be as much as 5 times larger than for the present alloys. This very fine microstructure means, however, that strength is more temperature dependent than for the present alloys as thermally activated deformation processes, such as Coble creep in grain boundaries or dislocation activation over particles, operate more easily [3,4,6,7]. It is well known, for example, that coarse particles lead to less Orowan strengthening, since their separation is large, but thermal activation of dislocations over obstacles is too easy when excessively fine particles, e.g.<2-20 nm, are present [49].…”
Section: Comparison Of Present Materials With Other Ods Fecr(al) Alloysmentioning
confidence: 83%
“…The rapid loss of strength of finegrained 14YWT from 500°C means that this material has similar strength to the present alloys in the most-relevant 600-800°C range. Nanocluster-strengthened alloys such as 14YWT have very fine grain size, 100-500 nm [3,4,6,7] and very large numbers of 2-5 nm sized dispersoids [1][2][3][4]. Since these nanodispersion-strengthened alloys contain many more oxide particles than the present materials (e.g.…”
Section: Comparison Of Present Materials With Other Ods Fecr(al) Alloysmentioning
confidence: 92%
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