1975
DOI: 10.1016/0026-0800(75)90038-5
|View full text |Cite
|
Sign up to set email alerts
|

Distribution of plastic strain in alloys containing small particles

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
30
1

Year Published

1977
1977
2020
2020

Publication Types

Select...
4
3

Relationship

0
7

Authors

Journals

citations
Cited by 120 publications
(31 citation statements)
references
References 6 publications
0
30
1
Order By: Relevance
“…In ODS steels, the oxides are often referred to as nano-oxide dispersions since typical oxide particle diameters on the order of < 100 nm. [43][44][45][46][47] Mobile dislocations interact with nanometer-sized oxide particles via mechanisms involving direct particle shearing [48,49] and/or circumventing the particle via a bypass manoeuver, such as the looping mechanism as proposed by Orowan, [50] depending on the particle-matrix coherency and degree of bonding between the particle and the matrix, the energy penalty of this bypass mechanism being proportional to the material flow stress. [51,52] However as particle size and spacing increases, their ability to hinder dislocation mobility via individual particle-dislocation interactions diminishes, and their relatively large volumes cause multiple dislocations to agglomerate in the form of dislocation forests on the surface of oxide particles.…”
Section: Discussionmentioning
confidence: 99%
“…In ODS steels, the oxides are often referred to as nano-oxide dispersions since typical oxide particle diameters on the order of < 100 nm. [43][44][45][46][47] Mobile dislocations interact with nanometer-sized oxide particles via mechanisms involving direct particle shearing [48,49] and/or circumventing the particle via a bypass manoeuver, such as the looping mechanism as proposed by Orowan, [50] depending on the particle-matrix coherency and degree of bonding between the particle and the matrix, the energy penalty of this bypass mechanism being proportional to the material flow stress. [51,52] However as particle size and spacing increases, their ability to hinder dislocation mobility via individual particle-dislocation interactions diminishes, and their relatively large volumes cause multiple dislocations to agglomerate in the form of dislocation forests on the surface of oxide particles.…”
Section: Discussionmentioning
confidence: 99%
“…Precipitate shearing mechanism occurs when the precipitates are small in size so that dislocations can cut through (shearable or penetrable) the precipitates easily, while the Orowan looping mechanism takes place when the precipitates are large and impenetrable by dislocations [42][43][44][45][46][47]. In other words, precipitation strengthening depends on how dislocations interact with precipitates [46].…”
Section: The Strengthening Mechanisms Of Nano-scale Precipitates Strementioning
confidence: 99%
“…For Cu [33] and TiC [40] precipitates, the yield strength increment reaches its peak at a critical precipitate size of 2 to 6 nm and drops with a further increase of size. The increase in yield strength with increasing a precipitate size can be understood as the precipitates become more difficult to cut through when the precipitates become larger [46,47]. After the maximum strength increment, a further increase of precipitate size might lead to Orowan looping.…”
Section: The Strengthening Mechanisms Of Nano-scale Precipitates Strementioning
confidence: 99%
See 2 more Smart Citations