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grain-boundary migration
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Image
Published: 01 November 2010
Fig. 23 Grain-boundary migration coupled to a shear deformation for a 17.8°<100> symmetrical tilt boundary after 68 min annealing at 375 °C under a tensile stress of 0.27 MPa. The coupling factor, β, is determined as the ratio of lateral grain translation (s) to normal boundary
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Published: 01 November 2010
Fig. 25 Recorded grain-boundary migration in a zinc bicrystal by optical microscopy in polarized light (video frames). Source: Ref 2
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Published: 01 November 2010
Fig. 27 Measured grain-boundary migration rate versus driving force of a flat boundary in a bicrystal of bismuth exposed to a magnetic field. Source: Ref 78
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Published: 01 November 2010
Fig. 30 Measured grain-boundary migration rate versus reduced driving force of U-shaped boundaries in aluminum bicrystals (half-loop technique). Source: Ref 80
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Published: 01 November 2010
Fig. 48 Activation energy of grain-boundary migration (ε = 0.57 eV, Lennard-Jones potential for aluminum) as a function of misorientation angle from computer simulations of grain-boundary motion. Source: Ref 10
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Published: 01 November 2010
Fig. 49 Dependence of grain-boundary migration rate on driving force in the presence of impurity drag. In the interval denoted by T , the transition from the loaded to the free boundary and vice versa occurs discontinuously.
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Series: ASM Handbook
Volume: 22B
Publisher: ASM International
Published: 01 November 2010
DOI: 10.31399/asm.hb.v22b.a0005507
EISBN: 978-1-62708-197-9
... for measuring grain-boundary surface tension. The atomistic simulations of grain-boundary energy, measurement of grain-boundary migration and the techniques used to monitor grain-boundary migration are reviewed. Several considerations and effects influencing the computation of grain-boundary mobility are also...
Abstract
Grain boundaries are interfaces between crystallites of the same phase but different crystallographic orientation. They can be characterized as being low angle or high angle. This article discusses the measurements of grain-boundary energy with a brief summary of different schemes for measuring grain-boundary surface tension. The atomistic simulations of grain-boundary energy, measurement of grain-boundary migration and the techniques used to monitor grain-boundary migration are reviewed. Several considerations and effects influencing the computation of grain-boundary mobility are also discussed.
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005422
EISBN: 978-1-62708-196-2
... Abstract This article reviews network models and their applications for the simulation of various physical phenomena related to grain-boundary migration. It discusses the steps involved in the implementation of two and three-dimensional network models, namely, acquisition and discretization...
Abstract
This article reviews network models and their applications for the simulation of various physical phenomena related to grain-boundary migration. It discusses the steps involved in the implementation of two and three-dimensional network models, namely, acquisition and discretization of the microstructure, formulation of the equation of motion, and implementation of the topological transformations. The article presents examples that illustrate the simulation of physical phenomena to demonstrate the predictive power and flexibility of network models.
Image
Published: 01 November 2010
Fig. 20 Average interface velocity versus driving force for the migration of grain boundaries during recrystallization of cold-worked copper (99.96%). The boundary migration rates were estimated from stereological measurements. The instantaneous driving force for boundary migration
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Image
Published: 01 January 2005
migration and recrystallization may cause cracks to open at triple points. (b) Examples of grain-boundary voids and triple-point cracking at the prior beta grain boundaries in hot-forged Ti-6Al-2Sn-4Zr-2Mo-0.1Si with a colony-alpha starting microstructure. Source: Ref 19 , Ref 20
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Image
Published: 01 January 1986
Fig. 11 Dot map for zinc at the grain boundaries of copper showing diffusion-induced grain-boundary migration. The concentration levels mapped extend down to approximately 0.5% Zn, with a maximum concentration of 10% in the field. Source: Ref 20
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Image
Published: 01 December 1998
Fig. 1 Sequence of metallurgical stages in the DB process. (a) Initial contact: limited to a few asperities (room temperature). (b) First stage: deformation of surface asperities by plastic flow and creep. (c) Second stage: grain-boundary diffusion of atoms to the voids and grain-boundary
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Image
Published: 31 October 2011
Fig. 2 Sequence of metallurgical stages in diffusion bonding process. (a) Initial contact: limited to a few asperities (room temperature). (b) First stage: deformation of surface asperities by plastic flow and creep. (c) Second stage: grain-boundary diffusion of atoms to the voids and grain
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Image
Published: 01 January 1993
Fig. 2 Sequence of metallurgical stages in diffusion bonding process. (a) Initial contact: limited to a few asperities (room temperature). (b) First stage: deformation of surface asperities by plastic flow and creep. (c) Second stage: grain boundary diffusion of atoms to the voids and grain
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in Metallography and Microstructures of Powder Metallurgy Alloys
> Metallography and Microstructures
Published: 01 December 2004
in only a few particle boundaries with considerable grain growth, grain boundary migration, and spheroidization of pores. All with 2% nital etch at 300×.
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Image
Published: 01 January 1993
Fig. 14 Three-stage mechanistic model of diffusion welding. (a) Initial asperity contact. (b) First-stage deformation and interfacial boundary formation. (c) Second-stage grain boundary migration and pore elimination. (d) Third-stage volume diffusion and pore elimination. Source: Ref 7
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Published: 01 November 2010
Fig. 21 Various boundary geometries in bicrystalline specimens for the study of grain-boundary migration. (a) Wedge technique. (b) Reversed-capillary technique. (c) Constant driving force technique (quarter-loop technique). (d) Constant driving force technique (half-loop technique). Source
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Published: 01 November 2010
Fig. 59 Activation volume ( V * ) versus activation enthalpy ( H ) of tilt grain-boundary migration in aluminum (tilt axis indicated). Source: Ref 145
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Book Chapter
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005606
EISBN: 978-1-62708-174-0
... contact: limited to a few asperities (room temperature). (b) First stage: deformation of surface asperities by plastic flow and creep. (c) Second stage: grain-boundary diffusion of atoms to the voids and grain-boundary migration. (d) Third stage: volume diffusion of atoms to the voids During...
Abstract
This article provides a qualitative summary of the theory of diffusion bonding, as distinguished from the mechanisms of other solid-state welding processes. Diffusion bonding can be achieved for materials with adherent surface oxides, but the resultant interface strengths of these materials are considerably less than that measured for the parent material. The article describes three stages of diffusion bonding: microasperity deformation, diffusion-controlled mass transport, and interface migration. It concludes with information on diffusion bonding with interface aids.
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001350
EISBN: 978-1-62708-173-3
... bonding process. (a) Initial contact: limited to a few asperities (room temperature). (b) First stage: deformation of surface asperities by plastic flow and creep. (c) Second stage: grain boundary diffusion of atoms to the voids and grain boundary migration. (d) Third stage: volume diffusion of atoms...
Abstract
Diffusion bonding is only one of many solid-state joining processes wherein joining is accomplished without the need for a liquid interface (brazing) or the creation of a cast product via melting and resolidification. This article offers a qualitative summary of the theory of diffusion bonding. It discusses factors that affect the relative difficulty of diffusion bonding oxide-bearing surfaces. These include surface roughness prior to welding, mechanical properties of the oxide, relative hardness of the metal and its oxide film, and prestraining or work hardening of the material. The article describes the mechanism of diffusion bonding in terms of microasperity deformation, diffusion-controlled mass transport, and interface migration. It concludes with a discussion on diffusion bonding with interface aids.
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