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Online since: October 2007
Authors: Keizo Uematsu, Satoshi Tanaka, Yoshiaki Kinemuchi, Koji Watari, Hiromi Nakano, Hisashi Kaga
Hence it can be considered that the number of
potential barrier, which is inversely proportional to the grain diameter, eventually changes with the
amount of aluminum addition.
Tilt angle of the grains, that is angle made by the [ 0011 ] of the both grains, is ranged between 13 and 16.5° in this grain boundary.
In addition, segregation of aluminum at grain boundary was also observed at incoherent grain boundary as shown in Fig.3.
(1) Here, e is the electric charge, Ns density of trap at grain boundary, ε relative dielectric constant, ε0 the dielectric constant in vacuum, n carrier concentration in grain, vn thermal velocity of the electron, L length of specimen, V applied voltage to the specimen, ng the number of grain boundary along L, k the Boltzmann constant, and T absolute temperature [7].
Because the grain boundary plays an important role in the variation in mobility, grain boundary structure was modified via magnetic texturing which enabled to align c-axes of grains highly.
Tilt angle of the grains, that is angle made by the [ 0011 ] of the both grains, is ranged between 13 and 16.5° in this grain boundary.
In addition, segregation of aluminum at grain boundary was also observed at incoherent grain boundary as shown in Fig.3.
(1) Here, e is the electric charge, Ns density of trap at grain boundary, ε relative dielectric constant, ε0 the dielectric constant in vacuum, n carrier concentration in grain, vn thermal velocity of the electron, L length of specimen, V applied voltage to the specimen, ng the number of grain boundary along L, k the Boltzmann constant, and T absolute temperature [7].
Because the grain boundary plays an important role in the variation in mobility, grain boundary structure was modified via magnetic texturing which enabled to align c-axes of grains highly.
Online since: July 2016
Authors: Dariusz Rozumek, Sebastian Faszynka
The EN AW-2017A alloy consists of a grains and the Al2Cu phase.
Between large elongated grains are also visible cluster very small equiaxed α phase grains in the system band.
At the same time, the number of load cycles N was recorded.
In many cases, they are generated at the grain boundary of the solid solution.
Fatigue crack length „a” versus number of cycles N (active side specimen).
Between large elongated grains are also visible cluster very small equiaxed α phase grains in the system band.
At the same time, the number of load cycles N was recorded.
In many cases, they are generated at the grain boundary of the solid solution.
Fatigue crack length „a” versus number of cycles N (active side specimen).
Online since: July 2015
Authors: Günter Gottstein, Lazar S. Shvindlerman
Although the number of triple junctions depends on the number of boundaries, all peculiarities in the behavior of polycrystals during grain growth have been solely attributed to the motion of grain boundaries so far.
The grain boundary GB12 was vicinal to a twin boundary 60° <111>, and the other two grain boundaries were random high-angle grain boundaries.
Grain 2 Grain 3 Grain 1 Fig. 7.
The normal grain growth is driven by curvature, particularly of grain boundaries at conventional grain size, but predominantly by triple line curvature at nanometer grain size dimension.
The triple line excess energy is the difference between the total energy of a polycrystalline volume and the total energy of a single crystal with the same number of atoms plus the excess energy due to the grain boundaries present.
The grain boundary GB12 was vicinal to a twin boundary 60° <111>, and the other two grain boundaries were random high-angle grain boundaries.
Grain 2 Grain 3 Grain 1 Fig. 7.
The normal grain growth is driven by curvature, particularly of grain boundaries at conventional grain size, but predominantly by triple line curvature at nanometer grain size dimension.
The triple line excess energy is the difference between the total energy of a polycrystalline volume and the total energy of a single crystal with the same number of atoms plus the excess energy due to the grain boundaries present.
Online since: March 2014
Authors: J. Nemati, Hani Mizhir Magid, G.H. Majzoobi, B.T.H.T. Baharudin, M.A. Azmah Hanim, Sreenivasan Sulaiman
Because of these large strains, materials grains get finer.
Their results indicate that for route BC, it was kept constant when the number of passages N was increased.
The grain size was measured according to the ASTM standard E112.
The yield and total strains are increased by increasing the pass numbers.
The results of experiments indicated that the strength of the extruded materials increased by increasing the numbers of ECAE passes and hence the grain refinement.
Their results indicate that for route BC, it was kept constant when the number of passages N was increased.
The grain size was measured according to the ASTM standard E112.
The yield and total strains are increased by increasing the pass numbers.
The results of experiments indicated that the strength of the extruded materials increased by increasing the numbers of ECAE passes and hence the grain refinement.
Online since: June 2014
Authors: B.T. Hang Tuah Baharudin, Shamsuddin Sulaiman, G.H. Majzoobi, M.A. Azmah Hanim, J. Nemati
The grain diameter reduced from 45µm to 2.8 µm after 6 passes of ECAE.
The refinement in grain size causes dislocation pile- up at the grain boundary, which impedes dislocation movement and increases the yield stress of the material.
His study also included the optimal choice of the processing route and number of passes.
Their results demonstrated that the grain size of the alloy gradually reduced with the increase of the pass number and the mechanical properties were significantly improved after the ECAE.
Fig.8 shows Scatter plot of the Vickers Microhardness across the flow direction for different number of passes.
The refinement in grain size causes dislocation pile- up at the grain boundary, which impedes dislocation movement and increases the yield stress of the material.
His study also included the optimal choice of the processing route and number of passes.
Their results demonstrated that the grain size of the alloy gradually reduced with the increase of the pass number and the mechanical properties were significantly improved after the ECAE.
Fig.8 shows Scatter plot of the Vickers Microhardness across the flow direction for different number of passes.
Online since: January 2016
Authors: Ruslan Z. Valiev, Ilchat Sabirov, Maxim Yu. Murashkin, Eva Moreno-Valle
This was attributed to the development of very thin layers of a Zn-rich grain boundary phase, which leads readily to the occurrence of enhanced grain boundary sliding at room temperature.
Homogeneous coarse-grained (CG) microstructure with an average grain size of 50 μm was observed in the annealed material.
Summary CP Cu and Al 6063 alloy were subjected to ECAP and ECAP-PC processing for varying number of passes.
Langdon, Twenty-five years of ultrafine-grained materials: Achieving exceptional properties through grain refinement, Acta Mater. 61 (2013) 51-59
Langdon, Enhanced ductility of nanocrystallien and ultra-fine grained metals, Rev.
Homogeneous coarse-grained (CG) microstructure with an average grain size of 50 μm was observed in the annealed material.
Summary CP Cu and Al 6063 alloy were subjected to ECAP and ECAP-PC processing for varying number of passes.
Langdon, Twenty-five years of ultrafine-grained materials: Achieving exceptional properties through grain refinement, Acta Mater. 61 (2013) 51-59
Langdon, Enhanced ductility of nanocrystallien and ultra-fine grained metals, Rev.
Online since: December 2014
Authors: Xiao Dong Mi, Song Feng Tian, Hong Jian Yu, Ying Guang Liu, Rong Yuan Ju, Xiu Lei Peng
One efficient approach is processing NC material that combine grains with bimodal distribution in which NC grains provide high strength, whereas coarse grains can enhance ductility.
As such the total density of dislocation can be described by , where and are the volume fraction of the coarse grains and NC grains, respectively, and are the density of stored dislocation in the coarse grains and NC grains[9], respectively.
The total back stress stemmed from all dislocations accumulated along the grain boundaries[10] is expressed by : (3) where is the number of dislocations stopped at the grain boundaries, and,is the density of nano/microcracks ,is the maximum number of dislocation that can be emitted from the nano/microcracks tip along one slip plane.
To calculate the maximum number of lattice dislocations that can be emitted along one slip pline , we use the following calculation procedure as introduced by Ovid’ko and Sheinerman[11].
Fig. 1 Dependence of the maximum number of edge dislocation that can be emitted from the crack tip along one slip plane on the grain size d in bimodal copper It has been proved that the number of nano/microcracks in BNC materials increases during plastic deformation, which leads to the density of nano/microcrack being sensitive to the applied load.
As such the total density of dislocation can be described by , where and are the volume fraction of the coarse grains and NC grains, respectively, and are the density of stored dislocation in the coarse grains and NC grains[9], respectively.
The total back stress stemmed from all dislocations accumulated along the grain boundaries[10] is expressed by : (3) where is the number of dislocations stopped at the grain boundaries, and,is the density of nano/microcracks ,is the maximum number of dislocation that can be emitted from the nano/microcracks tip along one slip plane.
To calculate the maximum number of lattice dislocations that can be emitted along one slip pline , we use the following calculation procedure as introduced by Ovid’ko and Sheinerman[11].
Fig. 1 Dependence of the maximum number of edge dislocation that can be emitted from the crack tip along one slip plane on the grain size d in bimodal copper It has been proved that the number of nano/microcracks in BNC materials increases during plastic deformation, which leads to the density of nano/microcrack being sensitive to the applied load.
Online since: December 2012
Authors: Hong Xia Yang
Experimental Study on Compaction and Strength Characteristic of Wetland Fine Grained Soil
Hongxia Yang
School of Civil Engineering, Shandong Jiaotong University, Jinan, Shandong, 250023, China
yanghongxia0531@163.com
Keywords: Wetland, Fine grained soil, Compaction curve, Strength.
This paper through test study on the compaction and strength of several typical fine grained soil subgrade filler come from Ji-He expressway wetland soil field, discusses compaction characteristics of the fine grained soil under the condition of moisture content changes in a wide range,and change rule of compaction soil unconfined compressive strength and CBR value with the compaction work and moisture content.
Table 1 The fine grained soil physical property indexes No.
A large number of construction experience also shows, the moisture content is close to the optimum moisture content conditions,using made in China roller generally able to achieve the degree of compaction of the heavy standard, but for a higher moisture content over wet soil, it is difficult to achieve heavy standard requirements the degree of compaction.
[5] Hua Li.The Family of Compaction Curves for Fine grained Soils and There Engineering Behaviors.University of Alberta.2001
This paper through test study on the compaction and strength of several typical fine grained soil subgrade filler come from Ji-He expressway wetland soil field, discusses compaction characteristics of the fine grained soil under the condition of moisture content changes in a wide range,and change rule of compaction soil unconfined compressive strength and CBR value with the compaction work and moisture content.
Table 1 The fine grained soil physical property indexes No.
A large number of construction experience also shows, the moisture content is close to the optimum moisture content conditions,using made in China roller generally able to achieve the degree of compaction of the heavy standard, but for a higher moisture content over wet soil, it is difficult to achieve heavy standard requirements the degree of compaction.
[5] Hua Li.The Family of Compaction Curves for Fine grained Soils and There Engineering Behaviors.University of Alberta.2001
Online since: December 2007
Authors: Jaroslav Pokluda, Pavel Lejček, Jozef Janovec
Stress induced macroscopic separation of the material along the grain
boundaries is mostly attributed to grain boundary weakening due to intergranular precipitation
and/or impurity segregation [1,2].
The composition of grain boundaries was studied by Auger electron spectroscopy (AES) using a Microlab 310F VG.
It consists of twinned austenite grains separated by straight boundaries.
(5) Owing to a number of measured and theoretically assessed quantities of various uncertainty levels, a possible deviation ∆ i γcoh = ∆ i γcoh (∆f, ∆ktd , ∆kmd, ∆k * , ∆RS) of the intergranular fracture energy was determined following the standard error analysis.
The former mechanism was observed in ASS due to grain boundary precipitation of carbide particles.
The composition of grain boundaries was studied by Auger electron spectroscopy (AES) using a Microlab 310F VG.
It consists of twinned austenite grains separated by straight boundaries.
(5) Owing to a number of measured and theoretically assessed quantities of various uncertainty levels, a possible deviation ∆ i γcoh = ∆ i γcoh (∆f, ∆ktd , ∆kmd, ∆k * , ∆RS) of the intergranular fracture energy was determined following the standard error analysis.
The former mechanism was observed in ASS due to grain boundary precipitation of carbide particles.
Online since: March 2011
Authors: Leonid Klinger, Eugen Rabkin
Stress Generation During Grain Boundary Interdiffusion
L.
We show that the inequality of intrinsic grain boundary diffusion coefficients of the two components leads to plating out of additional material at the grain boundary in the form of extra material wedge, which generates an elastic stress field in the vicinity of the grain boundary.
As pointed out by Hwang et al., “…the mass gained or lost by the unequal diffusion in the grain boundary is compensated for by a mass flow in a direction perpendicular to the grain-boundary plane…” [8].
We will further suppose that a total number of atoms of both components per unit area of the GB is constant: ; ; , (3) where d is the GB thickness.
Mishin: Fundamentals of grain and interphase boundary diffusion.
We show that the inequality of intrinsic grain boundary diffusion coefficients of the two components leads to plating out of additional material at the grain boundary in the form of extra material wedge, which generates an elastic stress field in the vicinity of the grain boundary.
As pointed out by Hwang et al., “…the mass gained or lost by the unequal diffusion in the grain boundary is compensated for by a mass flow in a direction perpendicular to the grain-boundary plane…” [8].
We will further suppose that a total number of atoms of both components per unit area of the GB is constant: ; ; , (3) where d is the GB thickness.
Mishin: Fundamentals of grain and interphase boundary diffusion.