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Nucleation and Growth of CVD Diamond Films on Smooth SiSubstrate Pretreated by Nanodiamond Powders
SHAO Le-Xi,XIE Er-Qing,HE De-Yan,CHEN Guang-Hua,XU Kang
1998 Vol. 13 (6): 0931
Abstract(
1799 )
PDF(356KB)(
912
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Ultradispersed nanodiamond powder synthesized by explosive detonation was used for the pretreatment of mirror Si substrate for nucleation and growth of diamond by microwave plasma-CVD. Compared with the scratching pretreatment, it is found that the pretreatment method by coating substrate with the slurry loading nanodiamond powder not only enhances both of density (up to 109 cm-2 and nucleation rate, improving the quality of grown-up film greatly, but also controls nucleation easily. In addition, this pretreatment is also very cost-effective, non-damaging, and reproducible as well.
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Research Progress on H2S Gas Sensing Materials
FANG Guo-Jia,LIU Zu-Li,JI Xiang-Dong,YAO Kai-Lun
1998 Vol. 13 (6): 769775
Abstract(
1967 )
PDF(417KB)(
1056
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The application of H2S gas sensing materials and research progress on H2S gas sensing materials in the form of solid electrolytes and semiconductive oxides (sintered block, thick film andthin film) were reviewed in this paper, and the latest development of room temperature H2S gassensing thin films was discussed especially.
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Effect of Buoyancy Driven Convection and Crystal Growth
JIN Wei-Qing,PAN Zhi-Lei,LIU Zhao-Hua
1998 Vol. 13 (6): 776782
Abstract(
1902 )
PDF(459KB)(
940
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A high temperature in-situ observation method was used to observe two different states of convection: diffusive-advective flow and diffusive-convective flow. Characteristic diffusion distance L can be easily measured from Schlieren photograph and it ranges from 0.01~0.1cm for two different states of convection. By observation of rotating crystal growth processes in the KNbO3 melt, the widths of interfacial concentration, heat and momentum transition zone were obtained, which are 7.5×10-3cm, 8.6×10-2cm and 4.4×10-1cm respectively.
An investigation of growth kinetics of KNbO3 crystal related to the different states of the convection in high temperature melts was performed by this method. Irrespective of the state of convection in the melt, at the lower supercooling two dimensional nucleation growth was obtained. At the same supercooling, the discrepancy between the growth rates for two different states of convection was assigned to the buoyancy convective enhancement of the interfacial mass flow. The free energy per unit length of a step ε, and the thermodynamic potential barrier for two-dimensional nucleation Δ G*, were calculated from the experimental data for two different states of convection. These data are significant for consideration of the influence of convective flow on the interface growth kinetics. The effect of convection is to enhance the sharpness of the interface.
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Specific Heats of LiIO3 Crystal Grown in Space and on the Earth
XIE Hua-Qing,XI Tong-Geng,WANG Jin-Chang,WU Qing-Ren
1998 Vol. 13 (6): 783786
Abstract(
1967 )
PDF(220KB)(
943
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The specific heat of LiIO3 crystal grown in space and on the earth from --110-350℃ wasmeasured by the DSC method. The fitting equations from experimental data of specific heat weregiven. The maximal deviation of the values calculated by empirical equation from experiment datawas about ±1/%. The results show that the specific heats of LiIO3 crystas grown in space and onthe earth have no obvious differentiation.
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Investigation on Nd:Sr5(PO4)3F Single Crystal
MENG Xian-Lin,ZHU Li,ZHANG Huai-Jin,ZHANG Hong-Zhen,YANG Zhao-He,WANG Pu,Dawes J,WANG Chang-Qing,CHOW Y T
1998 Vol. 13 (6): 787792
Abstract(
1917 )
PDF(352KB)(
792
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The growth, structure, spectra, laser preperties and some physical properties of a new laser crystal Nd:Sr5(PO4)3F (Nd:SFAP) were studied in order to search and evaluate the applications of the crystal to laser. The Nd:SFAP single crystals were successfully grown by Czochralski method and the laser experiment of the crystal crystal pumped by laser diode (LD) was demonstrated. The properties of as-grown crystal were measured by advanced equipments. Experimental results showed that Effective distribution coeffcient Keff of Nd was 0.52. π polarization light with wavelength of 806nm was the best pumping light. The fluorescence lifetime of 2 at % Nd:SFAP crystal was 175μs. The pumping threshold of Nd:SFAP laser was 15mW and its slope efficiency was 31.8%. From the investigation we can draw a conchusion: the Nd:SFAP crystal is an ideal laser mateiral for lower power lasers, but it isn’t suited to be applied to higher power lasers.
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Crystal Growth and TG-DTA Properties of K2Ln(NO3)5.2H2O(Ln=La, Ce, Pr, Nd, Sm)
DONG Wen-Ting,ZHANG Hong-Jie,SU Qiang
1998 Vol. 13 (6): 793797
Abstract(
1897 )
PDF(367KB)(
868
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Single crystals of KLnN(Ln=La, Ce, Pr, Nd, Sm) can be grown in water solution with pH≈1~2 at about 40℃. Crystals of KLnN (Ln=La, Ce, Pr, Nd) are orthorhombic with space group Fdd2. KPrN crystal was grwon and its crystal structure was determined for the first time. The KPrN crystal parameters obtained by the direct method are as follows: a=21.411(3)A, b=11.2210(10)A, c=12.208(2)A, Z=6, R=0.0240. The TG-DTA curves of KLnN(Ln= La, Ce, Pr, Nd, Sm) demonstrate that the processes of dehydration , melt, irreversible phase transition and decomposition of NO-3 take place in sequence with the temperature increasing(except KCN). There are three steps in the decomposition of NO-3 in KLnN(Ln=La, Nd, Sm) while two steps in KLnN(Ln=Ce, Pr). K2Ln(NO3)5·2H2O are formed at about 225℃ by the reaction of the starting materials of KNO3 and Ln(NO3)3·nH2O.
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Study on Phase Diagram of Bi2O3-SiO2 System
FEI Yi-Ting,FAN Shi--Ji,SUN Ren-Ying,M. Ishii
1998 Vol. 13 (6): 798802
Abstract(
1844 )
PDF(290KB)(
1210
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Stable and metastable phase equilibria in a binary Bi2O3-SiO2 system were studied and a complete phase diagram of the system was proposed with DTA and XRD. A peritectic reaction L + SiO2←→Bi4Si3O12 at the SiO2-rich side of stable phase diagram was identified to have peritectic temperature at about 1030℃ and peritectic point close to the end of the peritectic isotherm. Bi4Si3O12 was observed to be a nearly congruently melting compound and liquidus of the peritectic reaction was identified by quenching microstructure method. Crystallization behavior of Bi2O3 -SiO2 system was also investigated. The results show that metastable Bi2SiO5 crystallizes out at 845℃.
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Synthesis of Ultrafine α-Alumina Powder by Pyrolysis of Ammonium Aluminium Carbonate Hydroxide
LI Ji-Guang,SUN Xu-Dong,ZHANG Min,LI Xiao-Dong,RU Hong-Qiang
1998 Vol. 13 (6): 803807
Abstract(
2518 )
PDF(384KB)(
1174
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By using ammonium aluminium sulfate and ammonium hydro-carbonate as the starting materials, the synthesis of ammonium aluminium carbonate hydroxide (NH4AlO(OH)HCO3) was studied. It was found that NH4AlO(OH)HCO3 can be synthesized by adding ammonium aluminium sulfate solution to ammonium hydro-carbonate solution with a adding rate less than 1.2L·h-1. Under other conditions the precipitate was γ-AlOOH in the experimental range. The sequence of phase transformation of γ-AlOOH during heating was found to be γ-AlOOH →γ-Al2O3→δ-Al2O3→θ-Al2O3→α-Al2O3; while that of NH4AlO(OH)HCO3 was found to be NH4AlO(OH)HCO3 →amorhous Al2O3→θ -Al2O3→α-Al2O3. The transformation temperatures of NH4AlO(OH)HCO3 to θ-Al2O3 and α-Al2O3 were both about 100→ lower than those of γ-AlOOH. γ-AlOOH can transform to α-Al2O3 completely by calcining at 1200℃ for 1h, and the obtained powder,with a particle size of 150nm, can be sintered to 84.46% relative density at 1450→ for 2h. NH4AlO(OH)HCO3 can transform to α-Al2O3 completely by calcining at 1100℃ for 1h, and the obtained powder, with a particle size of 70nm, can be sintered to 97.80% relative density under the same sintering condition.
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Pure Phase Ba2Ti9O20 Powders Prepared by Conventional Processing
YAO Yao,ZHAO Mei-Yu,WU Wen-Jun,WANG Yi-Lin
1998 Vol. 13 (6): 808812
Abstract(
1641 )
PDF(294KB)(
805
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Pure Ba2Ti9O20 powder was prepared by using traditional ceramic technological process with BaTiO3 and TiO as the starting raw materials. In order to explore the phase development sequence, the mixed powder of BaTiO3 and TiO2 was calcined with different temperatures from 800℃ to 1150℃ and different keeping hours from 1/60 to 64h, then identified by X-ray powder diffraction. The results show that the pure phase of Ba2Ti9O20 can be obtained at 1000~1150℃/4~32h, and the homogeneity of the constituents is an important processing factor for obtaining pure Ba2Ti9O20 powder.
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Preparation of Uniform Acicular Hematite Particles by Two Steps Hydrothermal Method from Fe(OH)3 Gel
ZHAO Jian-Lu,WEI Yu JIANG Yu-Min
1998 Vol. 13 (6): 813817
Abstract(
1923 )
PDF(371KB)(
1017
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Uniform acicular hematite particles were prepared by two steps hydrothermal method from Fe(OH)3 gel. The effect of nucleating temperature, pH and Sn4+ ions on the morphologies of hematite particles was studied. The experiments showed that uniform acicular particles can be obtained. First the suspension of Fe(OH)3 aged at 50~80℃ for 2h, crystal growing agent was then added, and put into a stainless steel autoclave with stirring at 150~170℃ for 1.5h. The key problem of the poor repeatability of experimental result was solved. The results were characterized by TEM and XRD.
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Studies On the Behavior of α-Al2O3 Slurry
XIE Zhuo-Li,SUN Hong-Wei,ZHENG Chong
1998 Vol. 13 (6): 818822
Abstract(
1720 )
PDF(283KB)(
1036
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The influences of different kinds and contents of dispersents and pH values of slumes on thestabilities of the slumes were studied. The slurry with suitable viscosity, mobility, stability wasobtained, which can be used to prepare α--A12O3 microporous membrane.
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Relationship Between Dielectric Relaxation Behavior and B-site Ordering of Lead Magnesium Niobate Ferroelectric Ceramics
LI Xin-Yuan,FENG Chu-De,LI Cheng-En,BAO Jun
1998 Vol. 13 (6): 823829
Abstract(
1993 )
PDF(487KB)(
1152
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The mechanism of the B-site ordering and disordering in Lead Magnesium Niobate (PMN) was examined by using both heat treatment and La-doped methods. The B-site structural ordering characteristics were exposed by X-ray diffraction (XRD), selected area electron diffraction (SAED) and high-resolution electron microscopy (HREM). The reason of the pyrochlore phase presenting with the La-doped increased was studied. Based on the analysis of dielectric properties, the increase in the degree of diffuse phase transition (DPT) in annealed and La-doped PMN observed was interpreted as the Mg2+:Nb5+=1:1 nonstoichiometric short-range ordered domain accompanied with the segregation of the Nb5+ in the disordered area. Furthermore, it was demonstrated that the kinetic mechanism of the ordering micro-domain growing was ion diffusion equilibrium by the effects of the heat treatment on DPT properties of the various amounts of La-doped.
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Ba(Mg1/3Ta2/3(1+x))O3陶瓷烧结性、微观结构及微波介电性能
BIAN Jian-Jiang,ZHAO Mei--Yu,YAO Yao,YIN Zhi-Wen
1998 Vol. 13 (6): 830834
Abstract(
1841 )
PDF(334KB)(
941
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Sintering behavior, microstructure and microwave dielectric properties of the nonstoichiometric Ba(Mg1/3Ta2/3(1+x)O3 with --0.01≤ x≤0.01 were investigated. The sintered density was improved by increasing Ta concentration. The ordering parameter S was not only related to the presence of defect in the specimen but also sensitive to the type of defects. The presence of B-site vacancy might hinder the ordering procedure much more significantly than that of A-site vacancy. The Q· f value decreased and the dielectric constant increased with the increase of tantalum contents.
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Oxygen Sensitive Resistance Properties of Sr2V2O7
CHEN Yong-Sheng,ZHANG Zu-Ren,LIU Zhen-Xiang
1998 Vol. 13 (6): 835840
Abstract(
1905 )
PDF(194KB)(
883
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The possibility of Sr2V2O7 to be a resistive oxygen-sensitive material was evaluated by studying its electrical properties, bulk and surface resistances of ceramic Sr2V2O7 at different temperatures and/or oxygen partial pressures were measured experimentally. After mathematical process of the data, some properties of Sr2V2O7 were achieved. Phase transformation has little influence on the electrical properties; the activation energies for surface and bulk conductances are 1.91eV and 1.31eV respectively; It has an oxygen sensitive factor m=6 and a relative high temperature coefficient. Sr2V2O7 needs surface modification if it serves as a potential exhaust gas sensor material.
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Effect of Temperature on Dynamic Fatigue Behaviour of Si3N4 Material
WANG Hong-Jie,WANG Yong-Lan,JIN Zhi--Hao,ZHOU Hui-Jiu
1998 Vol. 13 (6): 841846
Abstract(
1680 )
PDF(374KB)(
777
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The dynamic fatigue behaviours of Si3N4 material at room temperature, 800and 1100℃ were investigated. It was discovered that the fracture strength decreases with the increase of σ at a high stress rate, and that the stress corrosion exponent n decreases also with the temperature increasing. The former is the same as that in transformation toughening ceramics and glass-ceramics, but is of some deviation from the theoretical prediction. The fractographic observation showed that the dynamic fatigue failure mechanism of Si3N4 at elevated temperature is the softing of the glass phase in grain boundaries.
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Fracture and Failure of Brittle Materials under Biaxial Stress
BAO Yi-Wang,SUN Li
1998 Vol. 13 (6): 847852
Abstract(
1943 )
PDF(436KB)(
1314
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Brittle thin plate with a straight-through crack under biaxial and uniaxial tension in-plane was investigated by thermomechanical method. The critical stress intensity factor under those two loading modes was measured with disk-shaped specimens of glass and ceramics. The results show that the crack resistance of brittle materials increases with increasing stress parallel to the crack plane. The effects of biaxial stress reveal that the conventional criterion with the stress intensity factor is imperfect for biaxial stress issues. It is demonstrated that the crack opening and growth is governed by the strain at the crack tip.
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Formation and Oxidation Behavior of β-Sialon-Melilite Solid Solution Ceramics
ZHANG Jun-Hong,WANG Pei-Ling,JIA Ying-Xin,ZHANG Jiong
1998 Vol. 13 (6): 853858
Abstract(
1782 )
PDF(377KB)(
845
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The formation behavior of the composition of β10-Sialon(Si5.23Al0.77O0.77N7.23) plus 7.26wt% Nd-melilite solid solution (Nd2Si2AlO4N3) prepared by pressureless sintering was studied. Nd ions in the composition enter α-sialon at low temperature, dissolve in the liquid phase of the material with temperature increasing. Melilite solid solution can be formed as a grain boundary phase of the ceramics by heat-teatment at 1550℃ for 24h. The oxidation behavior of the hot-pressed and post-sintered samples was also investigated in the range of 1000~400℃. The melilite solid solution doesn’t caues severe cracking of the material in oxidation at 1000℃ At high temperature, the oxidized surface of the sample contains preferentially oriented A-Nd2Si2O7 grains and bubbles, which are formed because of the decrease of the silicate viscosity, incurred by the accumulation of Nd ions to the surface.
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Preparation and Photoluminescence of Mesoporous ZrO2/(1-n)SiO2-nAl2O3 Nanocomposites
YAO Lian--Zeng,MO Ji-Mei,LI Yuang-Hong,CAI Wei-Li,
1998 Vol. 13 (6): 859865
Abstract(
1891 )
PDF(424KB)(
905
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(1-n)SiO2-nAl2O3 (n=0, 0.01, 0.1) aerogels were prepared by using a sol-gel route and followed by the supercritical drying technique. Nano-ZrO2 precipitates were introduced into the pores of the aerogels. Photoluminescence of the ZrO2/(1-n)SiO2-nAl2O3 nanocomposites was measured. The results show that the luminescence peak at about 540nm (2.30eV) for nano-ZrO2 bulk sample shifts to 400nm (3.10eV) (blue shift) for ZrO2/(1-n)SiO2-nAl2O3 nanocomposites, when the excitation wavelength is 316nm (3.92eV) at room temperature. The blue shift is about 140nm. The relative intensities of the luminescence peak change with the doping amount of the nano-Al2O3. Mechanism of change of the luminescence peak in the visible region was proposed.
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Preparation of Nano-TiO2 Thick Film and its Electrical Properities
WANG Jun,GAO Lian,SONG Zhe,ZHOU Wei
1998 Vol. 13 (6): 866870
Abstract(
1851 )
PDF(254KB)(
923
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Nano-TiO2 and micro-TiO2 thick films were prepared on a-Al2O3 substrates by silk netlithograph method, the measured film resistance of nano-TiO2 was higher than that of micro-TiO2 in experimental temperature range, nano-TiO2 film demonstrated more change as the O2 partialpressure changed. XRD and SEM were also used to characterize the stucture of the prepared films.
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Friction and Wear Behaviours Between Ce-TZP-(Al2O3 ) Ceramics and Cr12 Steel
ZHENG Yong,LI Bao-Shun,ZHANG Yu-Feng,HUANG Xiao-Xian
1998 Vol. 13 (6): 871876
Abstract(
1836 )
PDF(373KB)(
830
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Friction and wear characteristics of Ce-TZP-(Al2O3 ) against Cr12 steel under the loads of 100--500N were studied in different environments ( air, water, acetic acid, ammonia solution). The wear mechanisms of zirconia ceramics were analyzed based on the morphology and phase composition of all worn surfaces. Under the load of 100N, the high friction coefficient and wear rate were measured and the main wear mechanism was abrasive wear in air; whereas in liquid, the friction coefficient and wear rate were all low, and delamination became dominant. Under the load of above 200N, Martensitic transformation occurred on the worn surfaces, and brittle fracture processing was the controlling mechanism. The friction coefficient decreased while the wear rate increased with increasing load.
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Biological metion Properties and Mechanism of UHMWPE-SiC Ceramics Friction Pair
WANG Chang-Xiang,ZHENG Chang-Qiong,ZHOU Xin,YIN Guang-Fu,DENG Jie,MENG Yong-Gang,WEN Shi-Zhu
1998 Vol. 13 (6): 877881
Abstract(
1865 )
PDF(342KB)(
986
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The biological friction and wear properties of UHMWPE rubbing against SiC ceramics lubricated with fresh plasma were evaluated by using Falex at 37℃, and the surfaces of the specimenwere observed with SEM and surface profile meter. The results show that the friction coefficient of UHMWPE against SiC is about 0.05, and the wear factor of UHMWPE is lower than8.45×10--10mm3/N.m. The wear loss of SiC ceramics is very small. Based on the results of XPSanalysis, the mechanism was proposed.
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Preparation of Coated ZrO2(3Y) Powder
ZHANG Ju-Xian,YANG Jing-yi,YU Xin HOU,Yao-Yong,GAO Long--Qiao
1998 Vol. 13 (6): 882883
Abstract(
1817 )
PDF(391KB)(
896
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Zro2(3Y) precursor which uniformly mixed with Y2O3 was prepared via hydrous-zirconia,which was prepared by microwave heating, coated with Y(OH)3 by heterogeneous nucleation processing. After ZrO2(3Y) precursor was calcined, its phase structure was analyzed by XRD. It wasfound that m-ZrO2 didn t exist in ZrO2(3Y) powder at room temperature. The results indicatedthat Y2O3 can uniformly be added in ZrO2 by coating means and the amount of metastable t-ZrO2 in ZrO2(3Y) powder can be increased.
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Synthesis of Al2O3 Nanopowders Using Inorganic Salt and Its Physical Chemistry
ZENG Wen-Ming,CHEN Nian-Yi,GUI Lin--Hua,WANG Jun,GAO Lian,GUO Jing-Kun
1998 Vol. 13 (6): 887892
Abstract(
1847 )
PDF(259KB)(
980
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Boehmite (γ-AlOOH) powder was first prepared by Sol-Freeze Drying method using cheap AlCl3·6H2O as raw materials, and then γ-Al2O3 nanopowder with the average diameter of 6nm and α-Al2O3 nanopowder with the mean diameter of 30nm were obtained by the calcination of the above γ-AlOOH powder at 500 and 1100℃, respectively. The potential~pH diagrams of Al-H2O system at 25 and 90℃ were presented, separately. Thermodynamic analysis of the main reactions in the process of thermal decomposition of Al(OH)3 was also made using Temkin-Schwarzman’s method and by means of regression analysis. Investigations of the potential-pH diagrams of Al-H2O system and thermodynamic analysis of the thermal decomposition of Al(OH)3 provide a certain guide for the formation of boehmite sol and the heat treatment of boehmite powder, respectively.
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14%mol Ce-TZP and Al2O3/Ce-TZP Layered Microcomposites
YU Hai-Jiang,WAN Ju-Lin,LIANG Kai-Ming,WANG Da-Ning,LIU Feng-Ru
1998 Vol. 13 (6): 893898
Abstract(
1887 )
PDF(301KB)(
855
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Through the testing of KIC value of 14mol%Ce-TZP and Ce-TZP/Al2O3 layered microcomposites with different fabric parameters, the influence of Al2O3 layer thickness and Ce-TZP content in Al2O3 layer on the mechanical property of the materials was analysed in material and mechanics perspective. In order to obtain the qulitatively explanation of the influence of Al2O3 layer on the transformation zone shape and transformation quantity, the Laser-Ramman Micro Zone analysis on the section and side of KIC sample fractured was adopted, thus the toughening mechanism of materials such as Ce-TZP/Al2O3 layered microcomposites can be expected.
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Enhancement of the Luminescent Intensity of Nano-Scale Y2O3:Eu3+ Powders
LI Qiang,GAO Lian,YAN Dong--Sheng
1998 Vol. 13 (6): 899903
Abstract(
1749 )
PDF(187KB)(
977
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Nano-scale Y2O3:Eu3+ powders with different grain sizes and Eu3+ concentrations were prepared by chemical process, and dealed with coating. It was found that the Eu3+ critical concentration of nano-scale Y2O3:Eu3+ powders was increased obviously, and it caused the luminescentintensity improved. In addition, because the hanging bonds on the surface of coating nano-scaleY2O3:Eu3+ powders were mostly vanished, the luminescent intensity was further enhanced.
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Mechanical Properties and Microstructure of Al2O3 Ceramics Superfast Densified by SPS
GAO Lian,HONG Jin-Sheng,MIYAMOTO Hiroki,DIAZDELA TORRE Sebastian
1998 Vol. 13 (6): 904908
Abstract(
1653 )
PDF(325KB)(
1212
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Al2O3 ceramics were successfully superfast densified by spark plasma sintering (SPS) under the conditions of heating rate as high as 600℃/min, no holding time at the sintering temperature from 1350 to 1700 ℃ and then fast cooling to 600℃ within 3 minutes. It showed that Al2O3 ceramics could reach to a higher density at a lower sintering temperature by SPS, as compared with by normal pressureless sintering. The bending strength of pure Al2O3 ceramics superfast densified by SPS at the temperature range of 1400~1550℃ was as high as about 800 MPa, which is an excellent datum being of more than a double of the bending strength for normal pure Al2O3 ceramics. SEM micrographs showed that the intragranular fracture was a preponderant fracture mode in these Al2O3 ceramics being of very high bending strength.
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Study on the Preparation and Structure of Mullite Membrane
HUANG Yong-Qian,ZHENG Chang-Qiong,XIE Chang-Qing
1998 Vol. 13 (6): 909912
Abstract(
2024 )
PDF(341KB)(
951
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Supported;and unsupported mullite membranes were prepared by sol-gel process from bothtetraethyoxysilane (TEOS) and aluminium nitrate precursors. Structure, appearance and poresize of the mullilte membrane were characterized by DAT-TG, XRD, SEM and BET. The resultsshowed non-crystal xerogel membrane transformed into the mullite membrane after heat treatmentat 1050℃. The most concentrative pore diameter of unsupported mullite membrane was about3. 71nm.
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Investigation on the Composite Plating for Non-corrosive Steel-based
lLIU Hai--Rong,CHEN Zong-Zhang,BAI Xiao-Jun
1998 Vol. 13 (6): 913917
Abstract(
1901 )
PDF(293KB)(
962
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The influence of proceeding treatment technology on properties of Ni--HAP composite coatingwas investigated. From the results, the degree of combination of the matrix being treated byelectropolishing with the composite coating was denser and firmer than that of the matrix beingtreated by mechemical polishing with the composite coating. As a result, a new-applied noncorrosive steel-based Ni-HAP composite biomaterial was produced. Moreover, a tentative studyabout the technology and mechanism of getting high-HAP contents coating was done.
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Plasma Spray Boron Carbide Coating
ZENG Yi,ZHANG Ye-Fang,HUANG Jing-Qi,XIA Ji-Yu,DING Chuan-Xian
1998 Vol. 13 (6): 918922
Abstract(
2234 )
PDF(351KB)(
1041
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The phase composition and microstructure of boron carbide coatings by plasma spray wereinvestigated through X-Rad, XPS and SEM. The porosity and microhardness of the coatings werealso measured. The results showed that The plasma spray boron carbide coatings by using theimproved F4-MB plasma gun under atmospheric pressure had the lower porosity 3%~4% and theclosed microhardness Hv>28GPa compared with the coatings obtained under up to 2kpa argonpressure.
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Investigation on Structural Transform of Nano Titania PowdersDuring Plasma Spraying Process
ZHU Ying-Chun,HUANG Min-Hui,CHANG Cheng-Kang,DING Chuan--Xian
1998 Vol. 13 (6): 923926
Abstract(
1782 )
PDF(288KB)(
832
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The characteristics of phase transformation and microstructure of nano titanium oxide powders during plasma spraying were discussed. XRD and TEM methods were used to determine thecrystal structure and microstructure of the plasma sprayed nano titanium oxide powders. Moreover, the nano titanium oxide powders were also sintered in a furnace and characterized with XRDand TEM. The results show that plasma spraied titanium oxide powders belong to the triclinicsystem, whose particle size ranges from several nanometers to one hundred nanometers
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Dynamic Coloration Properties of Spin-coated WO3 Thin Films
WANG Zhong-Chun,HU Xing-Fang
1998 Vol. 13 (6): 932936
Abstract(
1984 )
PDF(287KB)(
1029
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WO3 thin films were fabricated on ITO glass substrates by the spin-coating technique using H2WO4 and H2O2 as precursors. The films annealed at 150℃ for 1h show dynamic coloration and bleaching efficiencies of 10.0, 8.6 cm2/C respectively at 633nm during cycling between --1 and +1V (vs. SCE) in LiClO4/PC at the scan rate of 20mV/s. The films annealed at 350℃ show improved cycling stability while losing some efficiency. The films annealed at 150℃ have also been electrochemically cycled by a constant current charge injection, which is found to be more easy to control the amount of charge injected into the films, and avoid overcharging the films, especially the surface layer.
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Characteristic of P~E Loop of PMN Relaxor Ferroelectric Ceramic Material
HUANG Zhong-Zang,CHAN H.L.W.,CHOY C.L
1998 Vol. 13 (6): 941943
Abstract(
2079 )
PDF(153KB)(
827
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According to the method proposed by Swarts and Shrout, PMN ceramic material with single perovskite phase was prepared, and no any pyrochloride one was detected by X-ray diffraction analyses. SEM observation shows that the sample was dense without the apparent pores. The hysteresis (P~E) loop was measured by using a Radiant Technology RT 66a and an amplifier. The change of P~E loop of the sample with the frequency measured shows that the dependence of the polarization on the field of PMN relaxor ferroelectric ceramic material at low frequency (e.g.10 Hz) is a curve without any hysteresis at room temperature, and P~E loop appears with the increase of frequency measured(e.g.>100 Hz), the higher the frequency, the larger the P~E loop, which differs from that of normal ferroelectrics.
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