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Showing papers on "Grain boundary strengthening published in 1968"



Journal ArticleDOI
TL;DR: In this article, a solute-clustering model is proposed for grain boundary quench-hardening based on preferential solutevacancy interactions and non-ideal thermodynamic behavior of the binary system.

226 citations


Journal ArticleDOI
TL;DR: In this article, the grain boundary allotriomorphs were measured in the temperature range 200°-325°C in an Al-4 % Cu alloy, and it was found that both the lengthening and thickening rates were orders of magnitude too rapid to be controlled by the volume diffusion of Cu toward the growing allotrimorphs.

198 citations



Journal ArticleDOI
TL;DR: Grain boundary precipitation in an Al-4% Cu alloy has been studied by transmission electron microscopy as discussed by the authors, where electron diffraction was used to determine the crystallographic details of the boundary and to identify the boundary precipitates.

79 citations


Journal ArticleDOI
TL;DR: In this paper, the authors applied the grain size dependence of dislocation density to Cottrell's theory of the Portevin-Lechatelier effect, and showed that the critical strain ∊0, necessary to initiate serrated flow, should depend on the grain sizes at constant strain rate, according to the relationship ∊ 0 = (constant)μ p, where p=n/(m + β).
Abstract: When the grain size dependence of dislocation density is applied to Cottrell's theory of the Portevin–Lechatelier effect, the result indicates that the critical strain ∊0, necessary to initiate serrated flow, should depend on the grain size μ, at constant strain rate, according to the relationship ∊0 = (constant)μ p , where p=n/(m + β). The parameters n and (m + β) are evaluated by dislocation density measurements and strain rate experiments respectively to give ∊0 ∝ μ½. Direct experimental determination of ∊0 as a function of grain size is in agreement with that predicted theoretically, indicating that the effect arises from the influence of grain size on the average velocity of mobile dislocations. The period and amplitude of the serrations decrease with increasing grain size. This effect is consistent with the idea that each serration corresponds to a yield point followed by a local Luders strain. The period and amplitude of the serrations decrease with increasing grain size. This effect is co...

74 citations


Journal ArticleDOI
TL;DR: In this article, the electron microscope was used to examine polycrystalline nickel (grain size 0.04 mm) after annealing and then after plastically straining at room temperature to between 0.4 and 12% elongation.
Abstract: Polycrystalline nickel (grain size 0.04 mm) has been examined with the electron microscope after annealing and then after plastically straining at room temperature to between 0.4 and 12% elongation. In addition to measuring the grain-interior dislocation density (ρ, cm/cm3), the number (n) per cm3 of three-fold nodes was counted and the arrangement and density (p, cm/cm2) of dislocations in the grain boundaries was examined. The applied tensile stress σ = 1.4 Gb ρ½ = 1.3 Gb n⅓ (where G is the shear modulus, b the Burgers vector). The node density was high and the dislocation network tightly linked at all strains, which is a necessary feature if attractive junctions are to contribute substantially to the flow stress. Straining evidently does not change the shape of the network so much as refine it, and the refinement is presumably the essential feature of strain-hardening. Superimposed on the refinement there developed the normal cellular structure. The grain boundaries trapped dislocations and he...

64 citations


Journal ArticleDOI
TL;DR: In this paper, the effects of hydrostatic pressure on the fracture stress of polycrystalline metals have been analyzed in the dislocation pileup model of Stroh and the wall splitting model of Friedel.
Abstract: The dislocation pileup model of Stroh and the wall splitting model of Stroh and Friedel have been used to calculate the effects of hydrostatic pressure on the fracture stress of polycrystalline metals. For each model, the three critical stages of fracture, nucleation, propagation through a grain, and the propagation across a grain boundary have been considered in turn. The variation of the critical cleavage‐crack orientation with respect to the tensile axis has been shown to be a function of the hydrostatic pressure. The fracture stress depends upon the grain size and at high pressures where grain boundary propagation is the critical stage, a d−1/2 dependence was found. This analysis both predicts and provides a physical interpretation of the ductility‐transition curve.

39 citations


Journal ArticleDOI
TL;DR: In this article, the theory of Clarke for the formation of grain boundary cracks in anisotropic polycrystalline materials, is re-examined in the light of recent experimental data.
Abstract: The theory of Clarke for the formation of grain boundary cracks in anisotropic polycrystalline materials, is re-examined in the light of recent experimental data. The theory predicts correctly the conditions for the formation of grain boundary cracks of length similar to a grain dimension. However, the theory cannot be used to explain the experimentally observed strength/grain size and strength/irradiation dose relationships, for example for BeO. The theory supposes that the process controlling catastrophic fracture is the growth of a crack from a grain boundary pore with an energy absorption rate corresponding to the grain boundary surface energy of ∼103 erg/cm2. In practice, the process controlling catastrophic fracture is the subsequent growth of a crack from a grain dimension, with a higher energy absorption rate corresponding to an effective surface energy of ∼104 erg/cm2.

31 citations


Journal ArticleDOI
TL;DR: In this paper, it was shown that grain-boundary sliding is always easier than grain deformation in the high-temperature creep of polycrystalline aggregates, and that the latter generally determines the rate laws for creep.

27 citations


Journal ArticleDOI
TL;DR: In this paper, the authors examined grain boundary sliding in symmetrically oriented bicrystals of high purity zinc and showed that sliding in the absenoe of transcrystalline deformation exhibits a strong dependence on the direction of shear along the boundary plane.

Journal ArticleDOI
TL;DR: In this paper, the true and apparent angular distributions of grain boundary cavities have been measured for OFHC copper deformed over a range of creep rates at 415°C, and no effect of strain rate was observed, the f...
Abstract: The true and apparent angular distributions of grain boundary cavities have been measured for OFHC copper deformed over a range of creep rates at 415°C. No effect of strain rate was observed, the f...

Journal ArticleDOI
TL;DR: In this paper, grain boundaries lying in certain directions relative to adjacent grains have been found to be preferred sites for zirconium hydride precipitation in Zircaloy-2, and the most favourable sites are those grain boundaries which make angles of 35°−40° and 60°−75° to the basal planes of the adjacent grains.




Journal ArticleDOI
TL;DR: In this paper, a method for growing KCl single crystals from the melt with dislocation densities lower than 103 cm-2 and completely free of grain boundaries is described, which is achieved by preventing thermal stresses, such as are introduced by thermal shock affecting the seed during initial growth and by thermal gradients due to preferential growth in radial directions, as well as by stresses created by the convection of the ambient gas.

Journal ArticleDOI
TL;DR: In this article, the effect of local slipping induced by the active slip systems of the neighbouring macrocrystals was found to be induced by local stress along the slip direction of active slip planes in the neighbouring crystals.
Abstract: Lattice distortions of deformed aluminium macrocrystals were observed by Electron-microprobe-Kossel techniques. Grain boundary effects due to deformation appeared in various ways such as extraordinary separation and branching of Kossel lines, and as intergranular rotation of the grains in pseudo-Kossel X-ray diffraction patterns obtained from the grain boundary regions of the specimens. Such distortions of the patterns peculiar to the grain boundary regions were attributed to the effect of local slipping induced by the active slip systems of the neighbouring crystals. By the interpretation of these patterns and the orientation relationships between neighbouring grains, it was found that the local slipping was induced towards the slip direction of the active slip plane in the neighbouring crystals, or induced by a type of local stress along the slip direction of the active slip planes in the neighbouring crystals. It was also recognised that at an early stage of stressing, deformation bands were produced in the grain boundary region as a result of a grain boundary effect.

Book ChapterDOI
K. T. Aust1
01 Jan 1968
TL;DR: A summary of previous studies, together with new observations, of the interfacial hardening effect is presented in this paper, where the authors provide support for a solute-clustering model for grain boundary quench-hardening.
Abstract: A summary of previous studies, together with new observations, of the interfacial hardening effect is presented. The topics considered include: hardening associated with vacancies and vacancy-solute interactions, examination by transmission electron-microscopy, vacancy condensation pits, solute-vacancy binding energies, solute clustering and impurity segregation. The results provide support for a solute-clustering model for grain boundary quench-hardening. The general implications of this work to other metallurgical phenomena are briefly considered.

Book ChapterDOI
01 Jan 1968
TL;DR: In this paper, the interaction energy of a grain boundary with a precipitate particle or inclusion of a second phase was investigated. But the nature of the inclusion was not considered, and two regimes emerged: (a) the grain boundary may enter and pass through certain coherent inclusions, leaving them coherent; (b) the boundary may envelop and bypass the inclusion, causing one which was coherent to lose coherency.
Abstract: The interaction energy of a grain boundary with a precipitate particle or inclusion of a second phase is considered in detail When the nature of the inclusion is considered, two regimes emerge: (a) the grain boundary may enter and pass through certain coherent inclusions, leaving them coherent; (b) more commonly, the grain boundary may envelop and bypass the inclusion, causing one which was coherent to lose coherency The maximum pinning force exerted by an inclusion or particle on a boundary depends on its nature

01 Feb 1968
TL;DR: In this paper, the work hardening behavior of alpha-titanium with four impurity contents and various grain sizes, tested in the temperature range 4.2K to 800K, was examined by transmission electron microscopy.
Abstract: : Mechanical properties data are reported for alpha-titanium of four impurity contents and various grain sizes, tested in the temperature range 4.2K to 800K. Dislocation substructures produced by deformation of commercial purity and high purity alpha-titanium at room temperature were examined by transmission electron microscopy and representative examples are presented and discussed. Work hardening behavior is connected with long-range interactions and is modified by both purity and grain size as well as temperature. The effect of impurity content appears to be related to the degree to which dislocations are restricted to their slip planes. Grain size also influences the yield and flow stresses, the relations observed being approximately of the Hall-Tetch type. The effects of grain size are shown to be athermal in nature and are accounted for in terms of work hardening model. Thermal activation analysis is used to show that the behavior reported is in agreement with the concept that the rate controlling process for low temperature deformation is thermally activated dislocation glide on first order prism planes over barriers associated with individual interstitial impurity atoms. The analysis shows that the nature of barriers is the same in all four materials and that the rate controlling process is unaffected by either grain size or plastic strain. (Author)


Patent
10 May 1968
TL;DR: In this paper, an endless conveysor belt type grain pick-up is used for removing grain from the pick-ups and a drive-per-roller is used to remove grain.
Abstract: AN ENDLESS CONVEYOR BELT TYPE GRAIN PICK-UP PROVIDED WITH FLEXIBLE PICK-UP TYNES AND A DRIVEN STRIPPER ROLLER FOR REMOVING GRAIN FROM THE TYNES. THE STRIPPER ROLLER IS LOCATED BELOW THE DISCHARGE END OF THE CONVEYOR AND KEPT A CONSTANT DISTANCE THEREFROM. THE ANGULAR RELATONSHIP OF THE STRIPPER ROLLER AND DISCHARGE END OF THE CONVEYOR RELATIVE TO THE GROUND IS VARIABLE. D R A W I N G


Proceedings ArticleDOI
TL;DR: In this paper, the results of the rupture tests conducted before exposure showed an excellent correlation with grain size and Ni3Cb plate size, and after exposure, rupture ductility increased and strength decreased due to overaging.
Abstract: Uniform, fine grain size is generally preferred in forgings of Alloy 718 for optimum properties. However, due to limitations imposed by forging equipment, forging size and forging configuration, it is often impossible to produce this desired grain size; instead, some grain duplexing or grain coarsening occurs in certain areas throughout the forging. Stress-rupture tests were conducted before exposure, and after exposing specimens at 1250°F, 50 ksi or 1300°F, 50 ksi for 500 hrs. on material having (1) uniform fine grain size (ASTM 7 or finer), (2) duplex grain size, and (3) uniform coarse grain size (ASTM 5 or coarser). These grain sizes were obtained in forgings with a simple pansake configuration using varying forging techniques. The results of the rupture tests conducted before exposure showed an excellent correlation with grain size and Ni3Cb plate size. After exposure, rupture ductility increased and strength decreased due to overaging. In duplexed samples the controlling factor appears to be the amount and size of the coarse grain. The optimum grain size for the best balance of rupture properties appears to be ASTM 6–7.


01 Mar 1968
TL;DR: In this article, a bubble model was used to study grain boundary sliding and migration in real crystals, and two important results emerged which, they believe, apply to boundaries in real crystal.
Abstract: : Stress-induced grain boundary sliding and migration was studied using a bubble model. Two important results emerge which, we believe, apply to boundaries in real crystals. First, sliding occurs by the propagation of grain boundary dislocations, which may have large burgers vectors, in the plane of the boundary; the magnitude of the burgers vector, and the pre-existing density of these dislocations in the boundary depends on the boundary angle and orientation. Second, migration is very like the process of crystal growth from the vapour: atoms leave or join one side of the boundary at steps; a boundary of which one side is a close-packed plane rarely migrated. The process of sliding periodically places atoms in a position which favours their leaving one side of the boundary and joining the other; this can result in sliding and migration which are proportional, and suggests a model for thermally activated grain-boundary sliding. (Author)

Journal ArticleDOI
TL;DR: In this article, the formation of porosity in an aluminum alloy A1-4%Cu with grain size in ranges 1000-200 and 120-85 μ, in technical grade aluminum Al (grain size 80-60 μ) during a thermal cycling treatment, each cycle of which included aging in water at 100 ° C.
Abstract: Metallographic examination was used to study the formation of porosity in an aluminum alloy A1-4%Cu with grain size in ranges 1000-200 and 120-85 μ, in technical grade aluminum Al (grain size 80-60 μ), and in type D1 alloy (grain size 30-10 μ) during a thermal cycling treatment, each cycle of which included aging in water at 100 ° C. The character of porosity depends on alloy composition and grain size. In coarsely granular materials the pores are formed inside grains, have clearly defined form, and reach a size of 10–20 μ after 60 cycles. The pore size in finely granular materials is smaller by one order of magnitude; the pores are formed predominantly along grain boundaries with some pores formed in the grain interior. Pores formed in alloy D1 are of an irregular form and grow to sizes exceeding the grain size. Data on changes in the specimen length, diameter, and volume were obtained. The relative increase in specimen volume reaches 0.5–1.0% per cycle. In spite of differences revealed by metallographic examination, the phenomena taking place in specimens with large and small grain size are of the same nature.

Journal ArticleDOI
TL;DR: In this paper, a method was proposed for calculating the grain size differential correlated with qualitative observations of differences in grain size, showing that an increase in the heating temperature of cold-worked steel 4Kh12N8G8MFB shifts the critical strain toward larger values.
Abstract: 1. An increase in the heating temperature of cold-worked steel 4Kh12N8G8MFB shifts the critical strain toward larger values. 2. A method was proposed for calculating the grain size differential correlated with qualitative observations of differences in grain size. 3. Heating of samples strained after quenching to 1100°C induces the largest difference in grain size at critical strain (1–4%). 4. On recrystallization heating of steel heated at 1050°C before deformation one observes two peaks of grain size on the recrystallization diagrams that correspond to 1 and 4% strain and are due to the difference in grain size.

Journal ArticleDOI
Abstract: The effect of the grain sizel of commerical nickel on the lower yield point, σy, and flow stress, σ f , has been investigated. From the relationship between σy andl −1/2 and between σ f andl −1/2, and also by extrapolation, the parameters σ1(σ i ) and ky(kf), which occur in Petch's well-known expression, were determined. It was found that the values of these parameters depend on the previous history of the samples. It is suggested that the more marked dependence of the deformation resistance of nickel on grain size arising from certain thermal treatments is due to the segregation of impurities to the grain boundaries. It is shown that this is in accord with the presence of grain-boundary hardening and with its dependence on quenching temperature.