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Online since: January 2016
Authors: Yong Wang, Bao Peng Bi
Microstructure and fracture of tensile samples are analyzed and discussed, deduce that grain boundary sliding (GBS) is the predominant deformation mechanism.
Because the grain material under high temperature grown serious, and high stress deformation strain rate conditions, the coordinated process of 5A06 to less than the internal deformation, stress concentration is not timely relaxation, have an adverse effect on the uniform deformation, causing material the elongation rate decreased.When the temperature of T=375℃, the reason of supplied 5A06 aluminum alloy general elongation is that the strain rate is too low, the samples in the high temperature retention time is longer, the grain to grow, making the sliding of grain boundary decrease, also have an adverse effect on the Superplasticity of the material.
When the fast strain rate tensile fracture hole size and number.This shows that supplied 5A06 aluminum alloy fracture mechanism is different in different strain rate during stretching.
Fig.7 shows that supplied 5A06 aluminum alloy temperature is 400℃ for metallographic image in a strain rate 5×10-3s-1, by the chart to determine the superplastic deformation of 5A06 aluminum alloy is the main mechanism of grain boundary sliding(GBS), grain boundary diffusion of coordination.
(2) The microstructure and fracture of tensile samples are analyzed and discussed, deduce superplastic deformation mechanism of supplied 5A06 aluminum alloy is dominated by grain boundary sliding(GBS), grain boundary diffusion as auxiliary
Because the grain material under high temperature grown serious, and high stress deformation strain rate conditions, the coordinated process of 5A06 to less than the internal deformation, stress concentration is not timely relaxation, have an adverse effect on the uniform deformation, causing material the elongation rate decreased.When the temperature of T=375℃, the reason of supplied 5A06 aluminum alloy general elongation is that the strain rate is too low, the samples in the high temperature retention time is longer, the grain to grow, making the sliding of grain boundary decrease, also have an adverse effect on the Superplasticity of the material.
When the fast strain rate tensile fracture hole size and number.This shows that supplied 5A06 aluminum alloy fracture mechanism is different in different strain rate during stretching.
Fig.7 shows that supplied 5A06 aluminum alloy temperature is 400℃ for metallographic image in a strain rate 5×10-3s-1, by the chart to determine the superplastic deformation of 5A06 aluminum alloy is the main mechanism of grain boundary sliding(GBS), grain boundary diffusion of coordination.
(2) The microstructure and fracture of tensile samples are analyzed and discussed, deduce superplastic deformation mechanism of supplied 5A06 aluminum alloy is dominated by grain boundary sliding(GBS), grain boundary diffusion as auxiliary
Online since: January 2008
Authors: Efstathios I. Meletis, Jiechao Jiang, Z. Yuan, Jian Liu, Jenny Weaver, B. Lin, V. Giurgiutiu, R.Y. Guo, A.S. Bhalla, D. Liu, K.W. White, Chong Lin Chen
Electron diffraction analysis and dark-field
imaging were employed to study the grain orientation of the film.
The size of the grains in Fig. 1(a) varies from 50 nm to 150 nm in diameter with the majority of the grain size being about 75 nm.
The grain size of the nanostructures varies from 30 to 100 nm in diameter and is smaller than that of the BTO grains.
More than 60% BTO grains share a common orientation with their a-axis in the film plane and the [011] direction parallel to the growth direction of the films.
Acknowledgement This work was supported by the National Science Foundation under Award Number NSF/CMS0528873.
The size of the grains in Fig. 1(a) varies from 50 nm to 150 nm in diameter with the majority of the grain size being about 75 nm.
The grain size of the nanostructures varies from 30 to 100 nm in diameter and is smaller than that of the BTO grains.
More than 60% BTO grains share a common orientation with their a-axis in the film plane and the [011] direction parallel to the growth direction of the films.
Acknowledgement This work was supported by the National Science Foundation under Award Number NSF/CMS0528873.
Online since: December 2019
Authors: Alexander V. Klyuev, E.S. Shorstova, Sergei V. Klyuev
The effectiveness of silica fume for the fine-grained concrete used for 3-D technologies is proved in the give scientific paper.
The mathematical modeling is used for the fine-grained concrete high-quality compositions’ development.
Experimental-statistical models of the factors influence for the introduction of silica fume on the properties of fine-grained concrete were obtained.
Pucharenko, Technogenic sands as effective filler for fine-grained fibre concrete, Journal of Physics: Conference Series. 1118 (2018) 012020
Vatin, Fine-grained concrete with combined reinforcement by different types of fibers, MATEC Web of Conferences. 245 (2018) 03006
The mathematical modeling is used for the fine-grained concrete high-quality compositions’ development.
Experimental-statistical models of the factors influence for the introduction of silica fume on the properties of fine-grained concrete were obtained.
Pucharenko, Technogenic sands as effective filler for fine-grained fibre concrete, Journal of Physics: Conference Series. 1118 (2018) 012020
Vatin, Fine-grained concrete with combined reinforcement by different types of fibers, MATEC Web of Conferences. 245 (2018) 03006
Online since: July 2011
Authors: Wan Shan Wang, Zi Rui Pang, Tian Biao Yu, Jing Qiang Zhang
Mechanism of nano-ceramic bond toughening is not only the role of nano-phase can inhibiti glass grain growth but also have relation with the following processes.
(c) The potential nano-crystallization of micron grain [6,7].
Vitrified bond in the dispersion of nano-phase sub-crystal interface generate a huge residual stress inside the grains, it makes a large number of potential sub-boundaries and microcracks in matrix crystal phase which can effectively inhibited the growth of bond matrix grain.
And it can reduce the number of defects grain to further enhance the bond strength.
It can be seen that the stoma number and size of 1# traditional vitrified bond is the maximum.
(c) The potential nano-crystallization of micron grain [6,7].
Vitrified bond in the dispersion of nano-phase sub-crystal interface generate a huge residual stress inside the grains, it makes a large number of potential sub-boundaries and microcracks in matrix crystal phase which can effectively inhibited the growth of bond matrix grain.
And it can reduce the number of defects grain to further enhance the bond strength.
It can be seen that the stoma number and size of 1# traditional vitrified bond is the maximum.
Online since: November 2012
Authors: Rishi Vyas, Sarla Sharma, Vijay Y K
It may be assumed that the heat gets confined within the grain volume.
This gives rise to non-equilibrium state which raises the volume of the grains resulting in grain agglomeration after irradiation [12].
The PL signal from the irradiated nanocomposite is an average effect of two processes among them one is due to the irradiation induced encapsulation free TiO2 nanoparticles providing large number of surface states which in turn increase the PL signal in addition to irradiation induced changes in microstructure of PMMA and other is due to the irradiation induced growth in grain size of TiO2 nanoparticles thereby decreasing the PL signal.
At higher fluence decrease in PL signal is attributed to the irradiation induced grain growth in TiO2 nanoparticles.
Choudhury, SHI-induced grain growth and grain fragmentation effects in polymer embedded CdS quantum dots systems, Mater.
This gives rise to non-equilibrium state which raises the volume of the grains resulting in grain agglomeration after irradiation [12].
The PL signal from the irradiated nanocomposite is an average effect of two processes among them one is due to the irradiation induced encapsulation free TiO2 nanoparticles providing large number of surface states which in turn increase the PL signal in addition to irradiation induced changes in microstructure of PMMA and other is due to the irradiation induced growth in grain size of TiO2 nanoparticles thereby decreasing the PL signal.
At higher fluence decrease in PL signal is attributed to the irradiation induced grain growth in TiO2 nanoparticles.
Choudhury, SHI-induced grain growth and grain fragmentation effects in polymer embedded CdS quantum dots systems, Mater.
Online since: July 2013
Authors: Diana A. Lados, Anastasios Gavras, Anthony Spangenberger
Secondary microstructural phases and the grain structure of all studied alloys are shown in Fig. 1 (equiaxed grain structure for the cast alloys and recrystallized “pancake” grain structure for the 6061 alloy, 1:3 ratio, 180 mm x 550 μm).
For the cast A535-F (a) (f) Grain size: 450 μm SDAS: ~40 μm 319-T6 (b) (g) Grain size: 800 μm SDAS: ~60 μm A356-T6 (c) (h) Grain size: 700 μm SDAS: ~60 μm A390-T6 (d) (i) Grain size: 750 μm 6061-T6 (e) (j) Fig. 1.
Thus, microstructural constituents within the matrix, smaller than the grain size, control the crack growth process in this alloy.
After N number of cycles at a given crack propagation rate, the flaw will advance by an increment of Δa, which when added to the initial flaw size, ainitial, yields the current crack length, acurrent.
Conclusions The long FCG behaviour in A535 is affected by grain size, while the crack growth in 3xx series and 6061 alloys is influenced by microstructural features within the grains.
For the cast A535-F (a) (f) Grain size: 450 μm SDAS: ~40 μm 319-T6 (b) (g) Grain size: 800 μm SDAS: ~60 μm A356-T6 (c) (h) Grain size: 700 μm SDAS: ~60 μm A390-T6 (d) (i) Grain size: 750 μm 6061-T6 (e) (j) Fig. 1.
Thus, microstructural constituents within the matrix, smaller than the grain size, control the crack growth process in this alloy.
After N number of cycles at a given crack propagation rate, the flaw will advance by an increment of Δa, which when added to the initial flaw size, ainitial, yields the current crack length, acurrent.
Conclusions The long FCG behaviour in A535 is affected by grain size, while the crack growth in 3xx series and 6061 alloys is influenced by microstructural features within the grains.
Online since: May 2013
Authors: Fu Wei Kang, Hai Chao Li, Yan Dong Jia, Jian Fei Sun, Xin Hong Zhang
Heterogeneous nucleation was the main nucleation way and the microstructures were dendrite grains for the most of over-spray powder.
From the photo, we can clearly find that the fine-equiaxed grain distributed in the matrix.
The reason was the broken dendrites after impacting in the semi-liquid layer, and the broken dendrites format would become a large number of nucleating centers.
The result would be the formation of equiaxed grain.
The reason was that during the deposition process the solidified dendrites impact with each other to form a large number of small nuclei.
From the photo, we can clearly find that the fine-equiaxed grain distributed in the matrix.
The reason was the broken dendrites after impacting in the semi-liquid layer, and the broken dendrites format would become a large number of nucleating centers.
The result would be the formation of equiaxed grain.
The reason was that during the deposition process the solidified dendrites impact with each other to form a large number of small nuclei.
Online since: August 2019
Authors: Vikas Upadhyay, Chaitanya Sharma
Finer are the grains, higher will be their number offering larger grain boundry area which favors pitting corrosion.
WNZ showed dynamically recrystallized equiaxed grains (Fig. 2b).
The high temperature in WNZ promotes recrystallization and formation of fine size grains of equal dimension i.e. equiaxed grain structure as compared to base metal.
Strengthening precipitates were seen in less numbers in WNZ as compared to base metal and other FSW zones because of dissolution.
Grains in both the parts of SZ were finer than the base metal.
WNZ showed dynamically recrystallized equiaxed grains (Fig. 2b).
The high temperature in WNZ promotes recrystallization and formation of fine size grains of equal dimension i.e. equiaxed grain structure as compared to base metal.
Strengthening precipitates were seen in less numbers in WNZ as compared to base metal and other FSW zones because of dissolution.
Grains in both the parts of SZ were finer than the base metal.
Online since: December 2010
Authors: Z. Horita, Yosuke Harai, Hideaki Iwaoka
Introduction
It is well known that severe plastic deformation (SPD) is a powerful method to produce ultrafine grains in metallic materials by introducing very large strain [1].
The microstructural evolution is also examined as a function of the number of evolutions.
The center area at the mid height appears dark and it increases the width with increasing the number of revolutions for both 2mm and 4mm samples.
Original grain boundaries are still visible near both upper and lower edges although they are strongly oriented parallel to the upper and lower surfaces.
(2) As the number of revolutions increases, the intense-strained regions expand along the thickness direction.
The microstructural evolution is also examined as a function of the number of evolutions.
The center area at the mid height appears dark and it increases the width with increasing the number of revolutions for both 2mm and 4mm samples.
Original grain boundaries are still visible near both upper and lower edges although they are strongly oriented parallel to the upper and lower surfaces.
(2) As the number of revolutions increases, the intense-strained regions expand along the thickness direction.
Online since: July 2014
Authors: R.H. Biswas
The OSL decay shape depends on number of traps participating in the process, and different photo-ionization cross-sections of each trap.
Single grain method.
However, comparing single aliquot and single grain analyses to poorly bleached samples, Olley et al. [63] have suggested that the age models can be applied to single aliquot provided the aliquots are composed of small number of grains, when single aliquot measurement tends to single grain measurement [65].
Selecting the appropriate age model and minimum number of measurements are still in the grey area in luminescence dating field. 3.1.5.
They propose ‘hotspot’ model to quantify the spread solely due to the number and positional fluctuations of feldspar grains (source of beta dose) in the matrix.
Single grain method.
However, comparing single aliquot and single grain analyses to poorly bleached samples, Olley et al. [63] have suggested that the age models can be applied to single aliquot provided the aliquots are composed of small number of grains, when single aliquot measurement tends to single grain measurement [65].
Selecting the appropriate age model and minimum number of measurements are still in the grey area in luminescence dating field. 3.1.5.
They propose ‘hotspot’ model to quantify the spread solely due to the number and positional fluctuations of feldspar grains (source of beta dose) in the matrix.