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Online since: June 2015
Authors: Khamirul Amin Matori, Mohd Sabri Mohd Ghazali, Azmi Zakaria, Wan Rafizah Wan Abdullah, Mohd Zaid Mohd Hafiz
The average grain size (d) was determined by lineal intercept method [19], given by d = 1.56L/MN, where L is the random line length on the micrograph, M is the magnification of the micrograph, and N is the number of the grain boundaries intercepted by lines.
TiO2 is commonly used as the grain growth enhancer to achieve large grain growth [22, 23].
For low-voltage varistors, grain growth is desired to reduce the number of grain boundaries across the terminals of the varistor device.
Less number of grain boundaries will reduce the number of potential barriers and give rise to lower voltage across the terminals thus qualifying the varistors as a low-voltage model.
Grain junction properties of ZnO varistors, Appl.
TiO2 is commonly used as the grain growth enhancer to achieve large grain growth [22, 23].
For low-voltage varistors, grain growth is desired to reduce the number of grain boundaries across the terminals of the varistor device.
Less number of grain boundaries will reduce the number of potential barriers and give rise to lower voltage across the terminals thus qualifying the varistors as a low-voltage model.
Grain junction properties of ZnO varistors, Appl.
Online since: January 2009
Authors: Z.H. Huang, Rongshi Chen, En-Hou Han
Fig. 1 Microstructures of ZW61 alloy (a) as-cast, (b) hot extruded and (c) 8 passes ECAE processed
Some large grains disperse in the matrix with small grains and a small number of second-phase
particles of Mg3YZn6 (i.e. the dark particles) scatter along the grain boundaries.
In addition, a large number of strips oriented in the extrusion direction are present (Fig.1 (b)).
Lots of recrystallized small grains and some coarse grains are observed.
Liquid, indicated (c) (a) (b) by the presence of Mg3Zn6Y particles after quenching, has appeared both along grain boundaries and as tiny liquid pockets within the grains (Figure. 2 (a), (b) and (c)).
Obviously, with the increasing temperature, grain coarsens evidently.
In addition, a large number of strips oriented in the extrusion direction are present (Fig.1 (b)).
Lots of recrystallized small grains and some coarse grains are observed.
Liquid, indicated (c) (a) (b) by the presence of Mg3Zn6Y particles after quenching, has appeared both along grain boundaries and as tiny liquid pockets within the grains (Figure. 2 (a), (b) and (c)).
Obviously, with the increasing temperature, grain coarsens evidently.
Online since: March 2007
Authors: Kojiro F. Kobayashi, Akio Hirose, Kengo Takahashi, Tomokazu Sano
The ablation depth is governed
by the optical penetration depth, which is the inverse number of the absorption coefficient of the
material at the laser wavelength.
The numbers of pulses irradiated were 8, 33, or 250 pulses depending on the irradiated energy.
The Ablation depth is obtained by dividing the numbers of pulses irradiated into the crater depth.
The BMG has no grain boundaries.
Hot electrons pass grain boundaries some times.
The numbers of pulses irradiated were 8, 33, or 250 pulses depending on the irradiated energy.
The Ablation depth is obtained by dividing the numbers of pulses irradiated into the crater depth.
The BMG has no grain boundaries.
Hot electrons pass grain boundaries some times.
Online since: March 2010
Authors: K. Yang, A.V. Nagasekhar, C.H. Caceres
This
definition again implicitly assumes uniformity in the overall grain size distribution.
Sequeira and Dunlop [1] and Rodrigo et al. [6] defined the skin as the region outside the mean hardness number across the specimen's thickness.
After testing the coordinates of the indentation points and hardness numbers were profiled into a 3D hardness surface map using a commercial software package (Surfer).
Figure 2a shows the fine grain structure that prevails along the surface.
The grains structure, however, is not fully uniform, as shown by the mixture of fine and large grains, Fig. 2b, and the presence of occasional microporosity, Fig. 2c.
Sequeira and Dunlop [1] and Rodrigo et al. [6] defined the skin as the region outside the mean hardness number across the specimen's thickness.
After testing the coordinates of the indentation points and hardness numbers were profiled into a 3D hardness surface map using a commercial software package (Surfer).
Figure 2a shows the fine grain structure that prevails along the surface.
The grains structure, however, is not fully uniform, as shown by the mixture of fine and large grains, Fig. 2b, and the presence of occasional microporosity, Fig. 2c.
Online since: January 2020
Authors: A.V. Ryabov
Free-machining Cr-Mo structural steel, containing low-melting elements, has ASTM grain size of the number of 7–8.
The investigated steels containing low-melting elements had austenite grain size not larger than of the ASTM number 7 (Table 4).
The investigated steels containing low-melting elements had austenite grain size not larger than of the ASTM number 7 (Table 4).
Effect of tin, lead, boron, nitrogen and aluminium on austenite grain size Steel Element, % [Al], % ASTM grain size number 30KhM 0.04 8 AS30KhM 0.24 Pb 0.03 7 ASTs30KhM 0,23 Pb 0.04 8 AO30KhM 0.07 Sn 0.06 7–8 A30KhMAR 0.008 B, 0.008 N 0.02 7–8 Conclusion 1.
Free-machining Cr-Mo steel of the 30KhM type alloyed with low-melting elements has ASTM grain size number of 7–8.
The investigated steels containing low-melting elements had austenite grain size not larger than of the ASTM number 7 (Table 4).
The investigated steels containing low-melting elements had austenite grain size not larger than of the ASTM number 7 (Table 4).
Effect of tin, lead, boron, nitrogen and aluminium on austenite grain size Steel Element, % [Al], % ASTM grain size number 30KhM 0.04 8 AS30KhM 0.24 Pb 0.03 7 ASTs30KhM 0,23 Pb 0.04 8 AO30KhM 0.07 Sn 0.06 7–8 A30KhMAR 0.008 B, 0.008 N 0.02 7–8 Conclusion 1.
Free-machining Cr-Mo steel of the 30KhM type alloyed with low-melting elements has ASTM grain size number of 7–8.
Online since: April 2012
Authors: Alexandre P. Zhilyaev, Terry R. McNelley, Oscar Ruano
For single pass the general form of the shear strain is given by [17]:
, so that (7)
where N is the number of passes.
The microhardness profile across the HPT disk for various numbers of turns is shown in Fig 6c.
By contrast, the grains at the edge are clear and grain interiors are almost dislocation free.
Both within and outside of these zones, the Al matrix grains were equiaxed with well-defined grain boundaries.
This suggests that the Si particles assist in grain refinement in the Al–7% Si alloy by pinning the grain boundaries and inhibiting grain boundary migration.
The microhardness profile across the HPT disk for various numbers of turns is shown in Fig 6c.
By contrast, the grains at the edge are clear and grain interiors are almost dislocation free.
Both within and outside of these zones, the Al matrix grains were equiaxed with well-defined grain boundaries.
This suggests that the Si particles assist in grain refinement in the Al–7% Si alloy by pinning the grain boundaries and inhibiting grain boundary migration.
Online since: March 2013
Authors: Ming Chen, Hong Yang Zhao, Xiao Dong Hu, Dong Ying Ju
Optimization of Process Parameters for
Unidirectional Solidification of Magnesium Alloy
Ming Chen1,a Xiao-Dong Hu1,b Hong-yang Zhao1,c Dong-Ying Ju1,d
University of Science and Technology Liaoning, Anshan, China 114051,
1a:cchen552@163.com,1,b:hulinas@sohu.com,1,c:zhy@ustl.edu.cn,1,d: dyju@sit.ac.jp
Corresponding author: Dong-Ying Ju, E-mail: dyju@sit.ac.jp, Phone:86-412-5928052,
Fax : 86-412-5929554
Keywords: unidirectional solidification, finite element method, phase field, columnar grain
Abstract: The unidirectional solidification process of magnesium alloy needs to establish a specific temperature gradient in casting mold, the direction of crystal growth and heat flow are in the opposite direction in the unidirectional solidification.
The process can better control the grain orientation, and eliminate the horizontal grain boundary to obtain excellent performance of magnesium alloy.
(5) (6) The parametermeans the strength of anisotropy and is a mode number of anisotropy, for the magnesium alloy we assign the value of 6 to.
For the constant value of , which is according to the macro analysis result when cooling intensity is ~5000W/m2k and pulling speed is 0.1mm/s, we can see the developed columnar grain structure.
For the constant value of , it can be seen that the columnar grain structure is more developed, through the comparison of different value of , it can be known that the higher cooling intensity is, the more developed the columnar grain structure is, but it is hard to make the value less than 1.5 in the actual process, that needs very large cooling intensity.
The process can better control the grain orientation, and eliminate the horizontal grain boundary to obtain excellent performance of magnesium alloy.
(5) (6) The parametermeans the strength of anisotropy and is a mode number of anisotropy, for the magnesium alloy we assign the value of 6 to.
For the constant value of , which is according to the macro analysis result when cooling intensity is ~5000W/m2k and pulling speed is 0.1mm/s, we can see the developed columnar grain structure.
For the constant value of , it can be seen that the columnar grain structure is more developed, through the comparison of different value of , it can be known that the higher cooling intensity is, the more developed the columnar grain structure is, but it is hard to make the value less than 1.5 in the actual process, that needs very large cooling intensity.
Online since: June 2017
Authors: Xin Ying Teng, Shu Min Xu, Xing Jing Ge, Jin Yang Zhang
From Fig. 2d it can be clearly seen that the grain structures are equiaxed with an average grain size of about 9.82μm.
It can hinder the grain growth during solidification.
According to the average grain size reduced, the grain boundary increased.
Dislocation slip can be strong impeded by a large number of grain boundary [19].
After solution treatment, a large number of lamellar tissues spreading to α-Mg matrix made the grain boundary fused and not continuous.
It can hinder the grain growth during solidification.
According to the average grain size reduced, the grain boundary increased.
Dislocation slip can be strong impeded by a large number of grain boundary [19].
After solution treatment, a large number of lamellar tissues spreading to α-Mg matrix made the grain boundary fused and not continuous.
Online since: January 2011
Authors: Xin Chun Shang, Jiu Mei Xiao, Bin Wen
The scanning electron microscopy (SEM) experimental results indicated that: under the force, non-crystalline materials distorted, crystal faces were torn along grain boundaries and crystal grains were disrupted.
So crystal size became smaller, more grain boundaries and more voids were formed, which supplied more free space for the movement of crystal grains and chain segments.
Introduction Ultra-high molecular weight polyethylene (UHMWPE) is a linear polymer with number average molecular weight in the range from one to ten million.
So crystal size became smaller, more grain boundaries and more voids were formed, which supplied more free space for the movement of chain segments and crystal grains.
So crystal size became smaller, more grain boundaries and more voids were formed, which supplied more free space for the movement of crystal grains and chain segments.
So crystal size became smaller, more grain boundaries and more voids were formed, which supplied more free space for the movement of crystal grains and chain segments.
Introduction Ultra-high molecular weight polyethylene (UHMWPE) is a linear polymer with number average molecular weight in the range from one to ten million.
So crystal size became smaller, more grain boundaries and more voids were formed, which supplied more free space for the movement of chain segments and crystal grains.
So crystal size became smaller, more grain boundaries and more voids were formed, which supplied more free space for the movement of crystal grains and chain segments.
Online since: September 2017
Authors: Sergey Demakov, Fedor V. Vodolazskiy, D.V. Gadeev
At lower temperatures, it is followed by the medium-temperature stage accompanied by precipitation of grain-boundary alpha and the formation of coarse secondary alpha-lamellae.
The low-temperature stage has been established to be characterized by the formation of dispersed alpha-platelets within beta-grains.
In addition to the treatments, the number of specimens were furnace heated and then water quenched.
The second stage includes the formation and subsequent growth of grain-boundary α as well as growth of coarse secondary α platelets from the grain boundaries which are referred to as α**.
With an increase of the heating temperature from 880 to 920 °C, the number of transformation stages was found to increase.
The low-temperature stage has been established to be characterized by the formation of dispersed alpha-platelets within beta-grains.
In addition to the treatments, the number of specimens were furnace heated and then water quenched.
The second stage includes the formation and subsequent growth of grain-boundary α as well as growth of coarse secondary α platelets from the grain boundaries which are referred to as α**.
With an increase of the heating temperature from 880 to 920 °C, the number of transformation stages was found to increase.