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Online since: September 2006
Authors: Michael E. Fitzpatrick
The material has a small grain size of ~5 µm, and the mean particle size in the material is ~3 µm.
It was therefore not possible in this experiment to determine whether the misfit stresses continue to evolve or cycle at greater numbers of stress cycles.
However, in this experiment it was not possible to determine unambiguously if there is stabilization of the misfit stresses at these or larger numbers of cycles.
At the peak tension and compression loads, the strains becoming increasingly tensile and compressive, respectively, as the number of cycles increases.
It is not clear from the results whether the shape misfits have completely stabilized after the five cycles that were applied, or whether there would be further changes at greater numbers of load cycles.
Online since: December 2014
Authors: Marcelo Brison de Mattos, Evaldo José Corat, Vladimir Jesus Trava-Airoldi, Lânia Auxiliadora Pereira
The X45CrSi93 steel were sanded with sandpaper of different grain sizes, polished with diamond past of 3 and 0,25 µm, after that the samples were cleaned with neutral soap, deionized water and acetone on ultrasonic bath for 8 minutes each.
Fig. 1 – Effect of varying the number of incident ions on steel X45 CrSi 9-3.
The Fig. 2 shows the vacancies number and backscattering ions due to silicon ions subimplanted energy.
Notes that when the polarization tension increases the vacancies/ions number increases too.
Fig. 2 – Vacancies/ions number and backscattering ions as function of polarization tension.
Online since: December 2010
Authors: Wen Jie Fan, Fang Liu, Chuan Xun Zhou
Choosing Experimental Samples and Numbering In order to study on impact resistance performance and test method of PDC, five common typical macro-interfaces (planar structure, v-groove, u-groove, ring groove, ring claw-tooth) are used as objects of this study.
Table 1 Samples’ serial number and their picture Number 1# 2# 3# 4# 5# Interface Planar structure v-groove u-groove Ring groove Ring claw-tooth Picture Test Methods of PDC Impact Resistance Fig.2 Sketch map of test method for PDC impact resistance performance The impact resistance performance of PDC indicates its comprehensive performance, and is of crucial importance to PDC application effect.
However, the PDC selected for this test is of good performance and high quality, so the work load will be much more and not convenient for us to do because of having a great number of wok loads.
Table 2 Test result of PDC impact resistance at normal temperature Samples number Interface structure Impact frequency total impact energy 1# planar structure 20 78.4 2# v-groove 45 176.4 3# T-groove 70 274.4 4# Ring groove 90 352.8 5# Ring claw-tooth 130 509.6 During the drilling process of PDC tooth, there are two critical temperatures for the tooth’s thermal wear, 350°C and 750°C.
Beside, most of crystalline grains in the diamond layer have combined into the D-D structure.
Online since: September 2020
Authors: Andrii Plugin, Maryna Sukhanevych, Kateryna Pushkarova
The dispersions were prepared in a cavitation principle homogenizer that ensures uniform distribution of nanoparticles in the plasticizer, the number of nanotubes was 1% by weight of the plasticizer.
Due to this adsorption, depending on the number of anionic functional groups, the C3A, C4AF sections are neutralized or even recharged, which significantly reduces the shear resistance and the viscosity of the system.
Nanoparticles - aggregates of surfactants with carbon nanotubes have a significant number of anionic groups oriented in all directions along the tube (Table 1, item 6).
The introduction of UCNT dispersions leads to structural changes in the cement-sand solution with the formation of a dense shell on the surface of the solid phases of cement grains and quartz sand.
The number of contact interactions in the structured boundary layers increases, and spatial frame cells are formed in the cement matrix with dense crystalline hydrate layers, which leads to a general seal of the matrix.
Online since: June 2012
Authors: Qiu Qin Lu, Guang Qiu Huang
Fig.1 The approximate representation of solid grain boundary in flow field Equation of state transition.
The coefficient represents drag force of Stokes and its equation is as follows: , where represents Reynolds number of solid particles.
Fr represents Froude numbers.
Theory of low Reynolds-number flows [M].Beijing:Beijing University Press,(2002) [7]O.Filippova and D.
[9]Qi D.Lattice-Boltzmann simulations of particles in non-zero-Reynolds-number flows[J].Journal of Fluid Mechanics, (385)(1999), p.41-62
Online since: April 2018
Authors: Alexander Sivkov, Yuliya Shanenkova, Alexander Ivashutenko, Julia Polovinkina
This method manages to obtain such composites, but this method has a significant drawback, which is a large number of small cracks in the final material structure.
This method has such advantages as ecological purity, high profitability, a small time interval for the powder consolidation that allows preserving the fine-grained structure of the synthesized material, which causes the high physical and mechanical properties.
The SEM-image shows that a large number of micropores are formed in the carbon fiber layer, which could not be filled with powder metal.
Such placement leads to increase in the total number of aluminum and carbon fiber layers.
In the second sample, the final characteristics will be slightly better only due to the larger number of precursors layers placed in the molds before sintering.
Online since: February 2011
Authors: Peter Nesvadba, Milan Turňa, Jozef Ondruška, Mária Behúlová
This standard corresponds to EN1563 (material designation: GJS-400-15, material number: JS1030).
Intermixing of welded materials Plastic strain of ferritic grains in matrix Plastic strain of graphite globules CuSn8 Fig. 3: A detail of weld boundary of MCI – SnCu8 bimetal The character of boundary was in detail studied by EDX and EBSD microanalyses and it will be the subject of lecture.
Online since: September 2014
Authors: Hamza Abobakr O. Ali Ammar, Xiao Xing Li
However, defects such as excessive thinning, coarse grains and bulging can be controlled by multi-step forming, etc. [1,2].
Fig. 6 Stretch force 120 mm Fig. 7 Compare 5 results (1st, 2nd, 3rd, 4th, 5th ) Simulations Fig, 8 Stretching distance 90 mm with angle 15o Summary Using the simulation system to run experiments save effort and money as well as time, it is conducting a number of tests, chooses the best results.
Online since: November 2014
Authors: Min Zhu, Yan Bo Wu, Xing Tao Sun, Jun Xi Shi
(1a) where (1b) with (2a) (2b) (2c) is the root-mean square backscattered voltage, is the mass concentration and is the sediment grain density.
According to Eq. 1a, due to the random phase of the backscattered signal, is obtained by averaging over a number of independent backscattered signals.
Online since: June 2018
Authors: Rodrigo S. Pessoa, Mariana A. Fraga, Andre Contin, Graziela S. Savonov, Divani C. Barbosa, Vladimir J. Trava Airoldi
It can be observed that UNCD film presents a very fine grain material grown with a high renucleation rate, whereas MCD film has a very roughness surface and a columnar growth regime.
Acknowledgments To FAPESP (processes number: 12/15857-1, 14/18139-8 and 13/25939-8) and CNPq for financial support.
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