Skip Nav Destination
Close Modal
Search Results for
dislocation boundaries
Update search
Filter
- Title
- Authors
- Author Affiliations
- Full Text
- Abstract
- Keywords
- DOI
- ISBN
- EISBN
- Issue
- ISSN
- EISSN
- Volume
- References
Filter
- Title
- Authors
- Author Affiliations
- Full Text
- Abstract
- Keywords
- DOI
- ISBN
- EISBN
- Issue
- ISSN
- EISSN
- Volume
- References
Filter
- Title
- Authors
- Author Affiliations
- Full Text
- Abstract
- Keywords
- DOI
- ISBN
- EISBN
- Issue
- ISSN
- EISSN
- Volume
- References
Filter
- Title
- Authors
- Author Affiliations
- Full Text
- Abstract
- Keywords
- DOI
- ISBN
- EISBN
- Issue
- ISSN
- EISSN
- Volume
- References
Filter
- Title
- Authors
- Author Affiliations
- Full Text
- Abstract
- Keywords
- DOI
- ISBN
- EISBN
- Issue
- ISSN
- EISSN
- Volume
- References
Filter
- Title
- Authors
- Author Affiliations
- Full Text
- Abstract
- Keywords
- DOI
- ISBN
- EISBN
- Issue
- ISSN
- EISSN
- Volume
- References
NARROW
Format
Topics
Book Series
Date
Availability
1-20 of 544 Search Results for
dislocation boundaries
Follow your search
Access your saved searches in your account
Would you like to receive an alert when new items match your search?
1
Sort by
Image
Published: 01 December 2004
Fig. 8 Bamboo incidental dislocation boundaries spanning lamellar boundaries (LBs) shown in a tracing (a) of microstructure in nickel following 90% cold reduction (cr) (ε vM = 2.7) that includes the geometrically necessary boundaries (solid lines) and bamboo incidental dislocation boundaries
More
Image
Published: 01 December 2004
Fig. 18 The probability density functions of the incidental dislocation boundaries (IDBs) misorientation angles normalized by the average misorientation angle, for cold-rolled aluminum and nickel plus compression-deformed copper. Copper data from Ref 53 and AISI 304L data from Ref 7
More
Image
Published: 01 December 2004
Fig. 9 Schematic representation of dislocation-generated antiphase boundaries (APBs). The lower APB is generated by one edge dislocation, while the upper APB is terminated between a pair of edge dislocations, creating a superlattice dislocation. Source: Ref 9
More
Image
Published: 01 December 2004
Fig. 10 Dislocation-generated antiphase domain boundaries in ordered Fe 3 Al. Thin-foil electron micrograph. 20,000×. Source: Ref 9
More
Series: ASM Handbook
Volume: 9
Publisher: ASM International
Published: 01 December 2004
DOI: 10.31399/asm.hb.v09.a0003742
EISBN: 978-1-62708-177-1
..., dislocation boundaries, and macroscopic properties. It discusses three different microstructural types: cell blocks, TL blocks, and equiaxed subgrains. The article also emphasizes the behavior of metals and single-phase alloys processed under plastic deformation (dislocation slip) conditions. It provides...
Abstract
Microstructure and crystallographic texture are the key material features used in the continuous endeavor to relate the processing of a metal with its final properties. This article emphasizes several aspects of deformation microstructures, namely, microstructural evolution, dislocation boundaries, and macroscopic properties. It discusses three different microstructural types: cell blocks, TL blocks, and equiaxed subgrains. The article also emphasizes the behavior of metals and single-phase alloys processed under plastic deformation (dislocation slip) conditions. It provides information on the microstructural parameters, measurement techniques, and microstructural relationships, which assist in predicting the mechanical properties and recrystallization behavior of materials. The article concludes with an analysis of the general relationship between the microstructural parameters and properties.
Image
Published: 01 December 2004
Fig. 2 (a) Flow lines in a 304L stainless steel high-temperature forging revealed by a macroetch and optical microscopy. (b) Microstructure of long dislocation boundaries in 304L stainless steel revealed by transmission electron microscope (TEM) following a moderate deformation, equivalent von
More
Image
Published: 01 December 2004
Fig. 14 Parameters in a large strain dislocation structure containing sheets of extended lamellar boundaries (LBs) with stippled low-angle (bamboo) incidental dislocation boundaries (IDBs) bridging between them. High-angle LBs are represented by heavy line weight and medium-angle LBs by medium
More
Image
Published: 01 December 2004
Fig. 15 The boundary spacing and misorientation angle for (a) incidental dislocation boundaries (IDBs) and (b) geometrically necessary boundaries (GNBs), respectively, as a function of strain in cold-rolled nickel (99.99%). Source: Ref 15
More
Image
Published: 01 December 2004
Fig. 6 Typical cell block dislocation structures composed of long geometrically necessary boundaries (GNBs) (i.e., dense dislocation walls, or DDWs, and microbands, or MBs) and incidental dislocation boundaries (IDBs) observed by TEM following low to medium deformation. (a) Aluminum (99.996
More
Image
Published: 01 December 2004
Fig. 7 Dislocation microstructures typical for large strain deformation with very long and well-developed geometrically necessary boundaries (GNBs) nearly parallel to the rolling direction with short bamboo incidental dislocation boundaries (IDBs) bridging between them observed by transmission
More
Image
Published: 01 December 2004
Fig. 17 Power-law relationship between misorientation angle versus strain for both geometrically necessary boundaries (GNBs) (filled symbols) and incidental dislocation boundaries (IDBs) (open symbols) for three different cold-rolled metals and one tension-deformed (down triangle); data from
More
Image
Published: 01 December 2004
Fig. 1 (a) Optical micrograph of a slip-line pattern in polycrystalline iron from the late 19th century. Source: Ref 1 . (b) Transmission electron micrograph of planar dislocation boundaries the “carpet structure” in a copper single-crystal middle of the 20th century. Source: Ref 2
More
Image
Published: 01 December 2004
Fig. 11 Dislocations in a small-angle tilt boundary in gold. Thin-foil transmission electron micrograph. See also Fig. 10 24,000×. Courtesy of R.W. Balluffi
More
Image
Published: 01 December 2004
Fig. 12 Dislocations in a small-angle twist boundary in gold. Thin-foil transmission electron micrograph. See also Fig. 10 Courtesy of R.W. Balluffi
More
Image
Published: 01 January 1986
Fig. 59 A dislocation array associated with a low-angle grain boundary in an aluminum alloy. The diffraction vector is g = (200).
More
Image
Published: 01 January 1986
Fig. 69 Dislocation interaction with existing subgrain boundary (arrow) during tensile deformation of austenitic stainless steel. Thin foil TEM specimen
More
Image
Published: 01 December 2009
Fig. 10 Dislocations (shown as the boundaries between slipped and unslipped regions) in the γ/γ′ microstructure of −0.3% lattice misfit under 152 MPa [001] tensile stress. Cross-sectional view on the slip plane for (b) 1 / 2 [ 101 ] ( 1 ¯ 1 ¯ 1 ) dislocations
More
Image
Published: 01 November 2010
Fig. 3 Basic dislocation configuration of a low-angle twist boundary. (a) A single family of parallel screw dislocations results in a shear deformation, but two perpendicular families of dislocations result in a pure rotation. (b) Transmission electron microscopy image of a low-angle twist
More
Series: ASM Handbook
Volume: 14A
Publisher: ASM International
Published: 01 January 2005
DOI: 10.31399/asm.hb.v14a.a0004020
EISBN: 978-1-62708-185-6
... in fine-grain metals has encompassed many ideas, such as the diffusional creep, dislocation creep with diffusional accommodation at grain boundaries, and concepts of grain-mantle deformation. The article concludes with information on the kinetics of superplastic deformation processes, including low stress...
Abstract
The constitutive relations for metalworking include elements of behavior at ambient temperature as well as high-temperature response. This article presents equations for strain hardening and strain-rate-sensitive flow, with alternate sections on empirically determined properties, followed by the models of constitutive behavior. It provides a discussion on creep mechanisms involving dislocation and diffusional flow, such as the Nabarro-Herring creep and the Coble creep. The equations for the several creep rates are also presented. Research on the mechanism of the superplastic flow in fine-grain metals has encompassed many ideas, such as the diffusional creep, dislocation creep with diffusional accommodation at grain boundaries, and concepts of grain-mantle deformation. The article concludes with information on the kinetics of superplastic deformation processes, including low stress behavior, concurrent grain growth, and high stress behavior.
Book Chapter
Series: ASM Handbook
Volume: 9
Publisher: ASM International
Published: 01 December 2004
DOI: 10.31399/asm.hb.v09.a0003784
EISBN: 978-1-62708-177-1
... Abstract Pure metals normally solidify into polycrystalline masses, but it is relatively easy to produce single crystals by directional solidification from the melt. This article illustrates the dislocations present in a metal crystal, which is often polygonized into sub-boundaries during grain...
Abstract
Pure metals normally solidify into polycrystalline masses, but it is relatively easy to produce single crystals by directional solidification from the melt. This article illustrates the dislocations present in a metal crystal, which is often polygonized into sub-boundaries during grain growth after solidification. It provides a description of small-angle and large-angle grain boundaries of polycrystalline metals.
1