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Online since: December 2013
Authors: Aleksei Belyi, Anton D. Teresov, Yurii F. Ivanov, Vladimir E. Ovcharenko
The Structure and Properties of Hard Metals Irradiated by High-energy Electron Beam
Ivanov Yurii1, a, Ovcharenko Vladimir2,b, Belyi Aleksei3,c ,
Teresov Anton4,d
1National Research Tomsk Polytechnic University, Tomsk, 634050, Russia
2Institute of Strength Physics and Materials Science SB RAS, , 634021, Tomsk, Russia
3Physico-tecnhnical Institute NAS Belarus’, 220141, Minsk, Belarus
4Institute of High Current Electronics SB RAS, Tomsk, 634055, Russia
ayufi55@mail.ru, bove45@mail.ru, cphti@belhost.by, dtad514@sibmail.com
Keywords: hard metal, pulse electron beam, structure, properties.
These advantages include a potential for good control and adjustment of input energy, high uniformity of energy distribution over the beam cross-section area as large as tens of square centimeters, and high efficiency factor for low reflectivity factor surfaces.
Microhardness tester was used for mechanical strength characterization.
One can see the top (2-3) mm thickness layer, transition 5 mm thickness layer and heat-affected layer separated by a chain of microvoids from the base metal.
The underlying layer of hard metal carbide 30-40mm microcrystallites is developed within the heat affected zone after pulse electron beam treatment of the hard metal.
These advantages include a potential for good control and adjustment of input energy, high uniformity of energy distribution over the beam cross-section area as large as tens of square centimeters, and high efficiency factor for low reflectivity factor surfaces.
Microhardness tester was used for mechanical strength characterization.
One can see the top (2-3) mm thickness layer, transition 5 mm thickness layer and heat-affected layer separated by a chain of microvoids from the base metal.
The underlying layer of hard metal carbide 30-40mm microcrystallites is developed within the heat affected zone after pulse electron beam treatment of the hard metal.
Online since: October 2014
Authors: Pavel Peterka, Stanislav Kropuch, Jozef Krešák, Andrea Bérešová
Design accuracy is assessed according to strength and deformation properties of wires a rope is made of and a rope cross-section construction is taken in account as well.
The paper presents models of ropes equally loaded which eliminates the most unfavorable factors affecting their life cycle.
The strands in the rope together with the tensile modulus in the tension of wires and Poisson's steel ratio [7] for wire ropes used are the parameters which should be assigned to the put to sleep effect of the rope strands and the rope itself including lubrication reducing the friction between the wires when the rope is working [8].There is a number of factors affecting the service life of wire ropes but one of the fundamental ones is load of a rope, strands and wires.
The bindings in the nodes 1-6 detract two degrees of freedom, one of the binding forces is affecting the tangent of the circle written by the strand.
Peterka, Steel wire ropes quality evaluation by the mechanical properties, Acta Montanistika Slovaca 1 (1997) 37-42.
The paper presents models of ropes equally loaded which eliminates the most unfavorable factors affecting their life cycle.
The strands in the rope together with the tensile modulus in the tension of wires and Poisson's steel ratio [7] for wire ropes used are the parameters which should be assigned to the put to sleep effect of the rope strands and the rope itself including lubrication reducing the friction between the wires when the rope is working [8].There is a number of factors affecting the service life of wire ropes but one of the fundamental ones is load of a rope, strands and wires.
The bindings in the nodes 1-6 detract two degrees of freedom, one of the binding forces is affecting the tangent of the circle written by the strand.
Peterka, Steel wire ropes quality evaluation by the mechanical properties, Acta Montanistika Slovaca 1 (1997) 37-42.
Online since: September 2012
Authors: Zhi Hua Sha, Sheng Fang Zhang, Yi Wang, Shao Xing Zhang
In this paper, based on the structure analysis of feeding system in a certain type of silicon ultra-precision grinding machine, the rigid body coupling virtual prototype model of the feeding system is established using ADAMS, the factors which influencing the stick-slip is analyzed deeply via the dynamic simulation of the virtual prototype.
Introduction As a core part of the silicon ultra-precision grinding machine, the performance indicators of the feed system is one of the key factors which influence affects the machining precision of the silicon wafer.
By combining the function of HyperMesh, ANSYS and ADAMS, the elastic properties of the object can be simulated, so the more practical stick-slip simulation analysis can be achieved.
In order to effectively reduce the occurrence of stick-slip, the factors which influencing the stick-slip of the feeding system in silicon ultra-precision grinding machine is analyzed deeply.
Gao: Chinese Journal of Mechanical Engineering, Vol. 40, 2004, p. 107 [3] J.Y.
Introduction As a core part of the silicon ultra-precision grinding machine, the performance indicators of the feed system is one of the key factors which influence affects the machining precision of the silicon wafer.
By combining the function of HyperMesh, ANSYS and ADAMS, the elastic properties of the object can be simulated, so the more practical stick-slip simulation analysis can be achieved.
In order to effectively reduce the occurrence of stick-slip, the factors which influencing the stick-slip of the feeding system in silicon ultra-precision grinding machine is analyzed deeply.
Gao: Chinese Journal of Mechanical Engineering, Vol. 40, 2004, p. 107 [3] J.Y.
Online since: November 2005
Authors: Satoshi Izumi, Chan Wee Ping, Makoto Yamaguchi, Shinsuke Sakai, Atsushi Suzuki, Yuzuru Ueda
Hence, there is a need to clarify the mechanical
characteristics such as fracture strength of such beams.
Until now, many researches have been performed to determine the mechanical properties of MEMS.
Note that the load factor can be obtained by numerically integrating the load factor PDF.
The damages due to the etching process is influenced by many factors such as the plasma gas concentration and flow characteristics, and orientation of the wafer.
It can be considered that the severe damage greatly affected fracture strength.
Until now, many researches have been performed to determine the mechanical properties of MEMS.
Note that the load factor can be obtained by numerically integrating the load factor PDF.
The damages due to the etching process is influenced by many factors such as the plasma gas concentration and flow characteristics, and orientation of the wafer.
It can be considered that the severe damage greatly affected fracture strength.
Online since: August 2008
Authors: Maria do Carmo de Andrade Nono, Olivério Moreira Macedo Silva, M.V. Ribeiro, José Vitor C. Souza
The measurement of the hardness
is an usual procedure to get information about the mechanical properties of cast irons.
This is one of the main factors, in particular, for tool wear in machining process CGI.
The mechanical shocks are non-negligible factors to in forming this kind of wear morphology to α-SiAlON cutting tool Fig 4.
Conclusions The α-SiAlON cutting tools presented high physical and mechanical properties.
Dawson, Hollinger L, Smiles P., The mechanical and physical properties of compacted graphite iron, 1998, company brochure, SinterCast Ltd
This is one of the main factors, in particular, for tool wear in machining process CGI.
The mechanical shocks are non-negligible factors to in forming this kind of wear morphology to α-SiAlON cutting tool Fig 4.
Conclusions The α-SiAlON cutting tools presented high physical and mechanical properties.
Dawson, Hollinger L, Smiles P., The mechanical and physical properties of compacted graphite iron, 1998, company brochure, SinterCast Ltd
Online since: December 2003
Authors: William Bonfield, Min Wang, L.Y. Leung, P.K. Lai
Both biological and mechanical properties of this material have been
extensive studied.
To understand the behaviour and determine mechanical properties of HA/PE composite under the bending condition, flexural tests of the composite were conducted in this investigation.
Investigations into basic mechanical properties of HA/PE had mainly concentrated on its tensile, torsional and viscoelastic properties [5-8].
It has also been found that tensile and torsional properties of HA/PE composite were affected by a number of materials factors [6, 7].
Other properties of raw materials can be found elsewhere [6, 7].
To understand the behaviour and determine mechanical properties of HA/PE composite under the bending condition, flexural tests of the composite were conducted in this investigation.
Investigations into basic mechanical properties of HA/PE had mainly concentrated on its tensile, torsional and viscoelastic properties [5-8].
It has also been found that tensile and torsional properties of HA/PE composite were affected by a number of materials factors [6, 7].
Other properties of raw materials can be found elsewhere [6, 7].
Online since: May 2014
Authors: Leszek Adam Dobrzański, Paweł Nuckowski, Błażej Tomiczek, Mirosława Pawlyta
The composite materials obtained as a result of mechanical alloying and hot extrusion are characterized with the structure of evenly distributed, disperse mineral phase particles in fine-grain matrix of AA-6061 alloy, facilitate the obtainment of higher values of strength properties, compared to the initial alloy.
Cauchy type (y = (1+ax2)−1) or Gauss type (y = exp(−ax2)) in the approximation methods were used for the experimental description of diffraction line intensity distribution, due to factors caused by apparatus, as well as physical ones.
Adamiak, The effect of TiAl and Ti3Al reinforcement on microstructure changes and properties of aluminium matrix composites, Arch.
Lukaszkowicz, Structure and properties of PVD coatings deposited on aluminium alloys, Surf.
Lutyński, Selected properties of the halloysite as a component of Geosynthetic Clay Liners (GCL), J.
Cauchy type (y = (1+ax2)−1) or Gauss type (y = exp(−ax2)) in the approximation methods were used for the experimental description of diffraction line intensity distribution, due to factors caused by apparatus, as well as physical ones.
Adamiak, The effect of TiAl and Ti3Al reinforcement on microstructure changes and properties of aluminium matrix composites, Arch.
Lukaszkowicz, Structure and properties of PVD coatings deposited on aluminium alloys, Surf.
Lutyński, Selected properties of the halloysite as a component of Geosynthetic Clay Liners (GCL), J.
Online since: March 2007
Authors: Ji Hyun Yoon, Bong Sang Lee, Eui Pak Yoon
The microstructural examinations were performed to relate key microstructural
features to mechanical properties.
The prerequisite material parameters for LBB design are mechanical properties such as J-R fracture resistance and tensile strength at reactor operating temperature to demonstrate the flaw stability [1].
However, it has been observed that the mechanical properties of type 347 welds varied diversely heat by heat.
Tensile properties of type 347 welds.
To obtain a deeper understanding of the microstructual factors affecting fracture property of type 347weld, fractured J-R specimens were examined with SEM in conjunction with EDS.
The prerequisite material parameters for LBB design are mechanical properties such as J-R fracture resistance and tensile strength at reactor operating temperature to demonstrate the flaw stability [1].
However, it has been observed that the mechanical properties of type 347 welds varied diversely heat by heat.
Tensile properties of type 347 welds.
To obtain a deeper understanding of the microstructual factors affecting fracture property of type 347weld, fractured J-R specimens were examined with SEM in conjunction with EDS.
Online since: May 2012
Authors: Yu Hong Ling, Hong Hua Ling
Based on these two important properties, different types of SMA energy dissipation devices have been developed.
Ling et al. [5] [6] firstly conducted tests on mechanical properties of NiTi wires, then hysteresis curve of the self-centring damper was simulated by programming based on Ma's work.
Mechanical model of re-centring SMA damper SMA Damper Behavior.
Parameters of Energy Dissipating Group The working principle of energy dissipating group is same as that of common metal damper, so the factors affecting its damping effect including[8]: (1) the ratio B/D of initial stiffness of energy components and stiffness of brace; (2) the ratio SR of initial stiffness of component consisted of brace and energy dissipating group and stiffness of corresponding structural layer; (3) the ratio β of yield displacement of energy components and yield displacement of corresponding structural layer; (4) the ratio α of the second stiffness and initial stiffness of energy components.
Fig.9 shows how parameter Q affects damping effect of re-centring SMA damper.
Ling et al. [5] [6] firstly conducted tests on mechanical properties of NiTi wires, then hysteresis curve of the self-centring damper was simulated by programming based on Ma's work.
Mechanical model of re-centring SMA damper SMA Damper Behavior.
Parameters of Energy Dissipating Group The working principle of energy dissipating group is same as that of common metal damper, so the factors affecting its damping effect including[8]: (1) the ratio B/D of initial stiffness of energy components and stiffness of brace; (2) the ratio SR of initial stiffness of component consisted of brace and energy dissipating group and stiffness of corresponding structural layer; (3) the ratio β of yield displacement of energy components and yield displacement of corresponding structural layer; (4) the ratio α of the second stiffness and initial stiffness of energy components.
Fig.9 shows how parameter Q affects damping effect of re-centring SMA damper.
Online since: August 2004
Authors: Cheol Woong Kim, Dong Joon Oh, Sam Hong Song
This fatigue delamination was affected by
the stacking sequence.
Table 1 shows the mechanical properties of the used UD GFRP prepreg.
Mechanical properties of unidirectional GFRP prepreg Fiber type Ultimate tensile strength(MPa) Tensile modulus (GPa) Tensile strain to failure (%) Density (g/cm 3 ) S-glass 4600 86 5.3 2.55 GFRP laminated as four different stacking sequences on the laminate configurations was cured by a hot-plate-press.
In addition, Table 2 showed the mechanical properties of GFRP laminates according to four different stacking sequences under N1 = 1,000 N/m, M1 = 50,000 Nm/m.
Mechanical properties of GFRP laminates under four different stacking sequences y x # 1 # 2 # 3 # 4 Notch x y x' y' θθθθ x, y : Laminate Axis x', y' : Ply Axis Fig. 2 Laminate configurations of stacking sequence at the laminate-axis vs. ply-axis Fig. 3.
Table 1 shows the mechanical properties of the used UD GFRP prepreg.
Mechanical properties of unidirectional GFRP prepreg Fiber type Ultimate tensile strength(MPa) Tensile modulus (GPa) Tensile strain to failure (%) Density (g/cm 3 ) S-glass 4600 86 5.3 2.55 GFRP laminated as four different stacking sequences on the laminate configurations was cured by a hot-plate-press.
In addition, Table 2 showed the mechanical properties of GFRP laminates according to four different stacking sequences under N1 = 1,000 N/m, M1 = 50,000 Nm/m.
Mechanical properties of GFRP laminates under four different stacking sequences y x # 1 # 2 # 3 # 4 Notch x y x' y' θθθθ x, y : Laminate Axis x', y' : Ply Axis Fig. 2 Laminate configurations of stacking sequence at the laminate-axis vs. ply-axis Fig. 3.