Authors: Duo Sheng Li, Xian Liang Zhou, Ai Hua Zou, Xiao Zhen Hua, Y.W. Yu
Abstract: The fabrication process and fracture characterization of 35 and 65 vol% SiCp particulate-reinforced Al matrix (SiCp/Al) composites have been investigated. SiCp composites having different volume fractions of the n-SiCp were synthesized via by pressureless-infiltration at near-net-shape route and were uniaxially tested at room temperature. The SiC particles were mixed with silicasol as an inorganic binder in distilled water. The mixtures were consolidated in a mold by pressing and dried in two step process, followed by calcination at 1000 °C. The SiCp/Al composites were fabricated by the infiltration of Al melt into SiC performs. The experimental results show that volume fraction of reinforced particles in SiCp/Al composites had a significant influenec on fracture section surface characterization in tensile tests. Composite with 45 vol% SiCp, fracture was firstly happen in Al matrix, shallow dimples and intergranular fractures were seen in all the fractographs. With increasing of vol% SiCp, fracture was more brittle in appearance in the composites and the fracture surfaces were flat and less plastic deformations.
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Authors: Duo Sheng Li, Xian Liang Zhou, Ai Hua Zhou, Xiao Zhen Hua, Y.W. Yu
Abstract: ZL101 Al alloy reinforced with 55% silicon carbide particulate metal-matrix SiCp/Al composite has been fabricated by pressureless-infiltration. The microstructure characterization of composite has been studied by optical microscope (OM), scanning electron microscope (SEM), X-ray spectroscopy (EDX), respectively. The results show that the SiCp are uniformly distributed in Al alloy matrix, however, there are some casting defects such as shrinkage and gas porosities in the matrix. When Mg was added into the composite, it can improve wettability property of between Al matrixes and strengthen particle SiCp and decrease micro-defects such as gas porosities, the Microstructure of SiCp/Al composite prepared was compact and uniform. The SiCp particles evenly distributed in the matrix and without significant partial segregation phenomenon. It improves the whole performance of the composites.
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Authors: Xian Liang Zhou, Duo Sheng Li, Ai Hua Zou, Xiao Zhen Hua, G.Z. Ye, Qing Jun Chen, Jian Yun Zhang, Yong Jin Tang
Abstract: SiCp/Al composite was fabricated by the method of pressureless-infiltration. In atmospheric environment, the atmospheric corrosion behavior of SiCp/Al composites (ZL101+49%SiC+5%Mg) was studied by mass loss, optical microscope (OM), scanning electron microscope (SEM), X-ray diffraction (XRD), energy dispersive spectrometer (EDS) and Fourier transform infrared spectroscopy (FTIR), respectivelhy.The results show that the corrosion rate of the SiCp/Al composites increases with increasing of time in atmospheric environment. Pitting corrosion is the main characteristic of SiCp/Al composite, and corrosion area gradually extends around with time increasing. At last, sheet like corrosion substrates distribute in the surface of n the SiCp/Al composites. Amorphous Al2O3 and amorphous AlxSO4yOHz are the main corrosion products.
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Authors: Duo Sheng Li, Dun Wen Zuo, X.L. Zhou, Xiao Zhen Hua
Abstract: Shell diamond film was prepared by DC plasma CVD, and substrate shape had an important influence on the growth of shell diamond film. Simulations of the substrate temperature field have been done respectively when the substrates are convex and concave. The simulation results show that, DC plasma flow more easily on convex substrate than concave substrate, and temperature field of convex substrate is more uniform than concave substrate; uniform temperature field was help to prepare high quality shell diamond film. In this study, shell diamond films were prepared on convex and concave substrate, respectively in experience. The results indicate that the growth of diamond film on convex substrate was better than on concave substrate, and Raman spectrum shows, on the convex substrate, high quality shell diamond film was prepared successfully, and it accords with the simulation results.
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Authors: Bing Kun Xiang, Dun Wen Zuo, Duo Sheng Li, Rong Fa Chen, Ming Wang
Abstract: Micro-nanocrystalline diamond (M-NCD) Film may be successfully prepared on Mo substrate with DC arc plasmas jet deposition device. This paper studies the influences of carbon source concentration on the shape of M-NCD Film particles under circumstances of stable electric arc, and characterizes the grain size and quality of samples through SEM, AFM and Raman spectrum. The research result shows that, in the state of stable electric arc, relatively low carbon source concentration (1%) could deposit high-quality microcrystalline diamond film on the substrate, with a growth rate of up to 8.3μm/h and grain size of about 2~4μm; relatively high carbon source concentration (10% or 15%) could deposit high-quality nanocrystalline diamond(NCD) film on the microcrystalline diamond film at high speed, with a growth rate of up to above 12.6μm/h or 19.7μm/h, grain size of about 4~80nm and average grain size of 27.4nm.
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Authors: Duo Sheng Li, Dun Wen Zuo, Wen Zhuang Lu, Rong Fa Chen, Bing Kun Xiang, M. Wang
Abstract: Diamond film was deposited on spherical molybdenum substrate by DC arc plasma CVD
method. Diamond film morphology, purities and orientation evolution, obtained from atomic force
microscopy, scanning electron microscopy, Raman spectroscopy, X ray diffraction respectively, has
showed that grains on the growth surface are compact, continuous and uniform. Characteristic
diamond (111), (220), (311) peaks were found and (111) facets were predominant. It revealed that
diamond film was polycrystalline texture characteristic. There is a typical diamond Raman spectrum
peaks at 1332.0 cm-1, and not graphite and amorphous carbon characteristic peak. High purity
diamond film was deposited. When methane concentration was increased, diamond film has more
local clusters and vacancy defects such as voids, graphite inclusion, and hydrogen cluster. Therefore,
some important parameters such as methane concentration and substrate temperature should be
optimized in depositing diamond film.
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Authors: Rong Fa Chen, Dun Wen Zuo, Yu Li Sun, Duo Sheng Li, Wen Zhuang Lu, Min Wang
Abstract: Strain films in the thin film resistance strain gauge are prepared by magnetron sputtering
method. Some results concerning the electromechanical and structural properties of nichrome
(Ni80Cr20 wt.%) thin films are presented. As compared to the well-known Ni-Cu (constantan) alloy
film, which are widely used for manufacturing pressure and force sensors, nichrome (Ni80Cr20
wt.%) thin films exhibit gauge factor values of the same order of magnitude, but they are much
more corrosion resistant and adherent to the substrate. The influences of composition and
post-deposition annealing on the electrical resistance, temperature coefficient of resistance (TCR)
and gauge factor of nichrome (Ni80Cr20 wt.%) thin films are discussed.
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Authors: Duo Sheng Li, Dun Wen Zuo, Rong Fa Chen, Yu Li Sun, Bing Kun Xiang, Wen Zhuang Lu
Abstract: In this paper, a new polishing technique was proposed to polish concave spherical surface
by diamond spherical shell deposited by DC-Plasma Jet CVD(chemical vapor deposition), and
preparation was studied from both experiment and theory. The deposited films were investigated by
some techniques including: scanning electron microscopy (SEM), atom force microscopy (AFM),
Raman spectroscopy, and roughness-profile-meter, which were used to analyze surface phase,
microstructure, internal quality and surface roughness. The results show that the deposited diamond
spherical shell film has some remarkable properties, such as high surface density, high hardness.
Compared to traditional polishing techniques, it will have some potential advantages as convenient,
flexible, efficient and precious. To adjust some important parameters as methane concentration,
depositing time, and it can deposit the different size grain diamond spherical shell films, which are
used to polish different precision degree concave spherical surfaces. Meantime, to change curvature
of diamond spherical shell, it can adapt to polish various curvature radius concave spherical surfaces.
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Authors: Duo Sheng Li, Dun Wen Zuo, Yu Li Sun, Rong Fa Chen, Wen Zhuang Lu, Bing Kun Xiang, Min Wang
Abstract: Diamond spherical shell thick film was prepared by high power DC-plasma jet CVD.
Atom force microscopy, scanning electron microscopy, Raman spectroscopy and
roughness-profile-meter were used to characterize microstructure, morphology, impurities and
orientation evolution of diamond spherical shell thick film. The results show that, when nucleation
begins, grains grow random orientation. The grain size of spherical diamond film prepared is
compact, clear, uniform, continuous and no remarkable bigger grain over the whole surface of film.
On the growth surface, (100) facets were dominant, and the cross-section SEM indicated that film
columnar spreading grew from the substrate surface to the diamond film surface. The roughness of
the growth surface was much more than that of the nucleation surface. To adjust some important
parameters as methane concentrate, depositing time, and matrix temperature, and high quality
diamond spherical shell thick film was deposited.
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Authors: Yu Li Sun, Dun Wen Zuo, Duo Sheng Li, Rong Fa Chen, Min Wang
Abstract: Hardness, elastic modulus and scratch resistance of single silicon wafer are measured by
nanoindentation and nanoscratching using a nanoindenter. Fracture toughness is measured by
indentation using a Vickers indenter. The results show that the hardness and elastic modulus at a peak
indentation depth of 100 nm are 12.6 and 166.5 GPa respectively. These values reflect the properties
of the silicon wafer, the bulk material. The fracture toughness value of the silicon wafer is 0.74
Mpa·m1/2. The material removal mechanisms are seen to be directly related to the normal force on the
tip. The critical load and scratch depth estimated from the scratch depth profile after the scratching
and the friction profile are 138.64 mN and 54.63 nm respectively. If the load and scratch depth are
under the critical values, the silicon wafer will undergo plastic flow rather than fracture. The critical
scratch depth is different from that calculated from the formula of critical-depth-of-cut described by
Bifnao et al and some reasons are given.
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