Y-Ce-ZrO_2-TiC-Al_2O_3复合陶瓷材料的制备及其摩擦磨损特性研究

从提高陶瓷材料的力学性能出发,采用真空热压工艺,制备了混合稀土氧化物稳定的Y-Ce-ZrO2-TiC-Al2O3复合陶瓷材料。对复合陶瓷材料进行了摩擦磨损性能实验研究,采用扫描电镜对其磨损表面形貌进行了观察,对磨损表面物相进行了X射线衍射分析。并与单相ZrO2陶瓷作对比,探讨了复合陶瓷材料的磨损机理。研究表明,该复合陶瓷材料具有较高的综合力学性能,在法向载荷为140 N、转速为200 r/min干摩擦条件下,Y-Ce-ZrO2-TiC-Al2O3复合陶瓷摩擦系数为0.65,磨损率为2.88×10-7mm3/N.m,明显低于单相ZrO2陶瓷,其磨损机理为机械冷焊和粘着磨损。     

Al2O3/Cr3 C2/Ti(C,N)复合材料摩擦磨损性能研究

采用热压烧结技术制备了Al2O3/Cr3 C2/Ti(C,N)复合陶瓷材料,对其力学性能、摩擦磨损性能进行测试,用扫描电镜(SEM)对其磨损表面进行观察.结果表明:Al2O3/Cr3 C2/Ti(C,N)复合陶瓷材料具有良好的综合力学性能,在与硬质合金YG8环块摩擦中表现出较高的减摩抗磨性能,摩擦系数与磨损率较单相Al2O3降低近一半.对其磨损机理研究认为,磨粒磨损为主要磨损机制,高的强度和韧性是其具有良好耐磨性能的主要原因.     

A12O3／Cr3C2／Ti（C，N）复合材料摩擦磨损性能研究

采用热压烧结技术制备了A12O3／Cr3C2／Ti（C,N）复合陶瓷材料,对其力学性能、摩擦磨损性能进行测试,用扫描电镜（SEM）对其磨损表面进行观察。结果表明：A12O3／Cr3C2／Ti（C,N）复合陶瓷材料具有良好的综合力学性能,在与硬质合金YG8环块摩擦中表现出较高的减摩抗磨性能,摩擦系数与磨损率较单相Al2O3降低近一半。对其磨损机理研究认为,磨粒磨损为主要磨损机制,高的强度和韧性是其具有良好耐磨性能的主要原因。     

ZrO2添加量对ZTA陶瓷力学性能及冲蚀磨损行为的影响

以α-Al2O3、ZrO(NO3)2.2H2O和氨水为原料,通过高温煅烧制备了ZTA复相陶瓷材料,研究了ZrO2添加量对ZTA陶瓷物相组成、表面微观形貌、力学性能以及常温固体粒子冲蚀磨损性能的影响。结果表明:随着ZrO2添加量增加,材料的力学性能逐渐提高,当ZrO2添加量为10 vol%时,ZTA复相陶瓷抗弯强度和断裂韧性分别达461MPa和5.77 MPa.m1/2,相对于纯Al2O3陶瓷提升量达21.3%和64.9%。ZTA复相陶瓷材料的体积冲蚀率随着ZrO2添加量的增加而降低,当ZrO2添加量小于4 vol%时,其体积磨损率急剧下降,随后趋于平稳;随后当ZrO2添加量为10 vol%时,其冲蚀率达最低,为0.015 mm3/g。其中,纯Al2O3陶瓷材料的冲蚀磨损机制主要为横向裂纹相互交错导致材料的剥落,添加ZrO2后,其冲蚀磨损机制以塑性变形为主。     

自润滑Al2O3/TiC/CaF2复合陶瓷材料摩擦特性

为了探索自润滑陶瓷材料的开发及应用,采用冷压烧结工艺制备Al2O3/TiC/CaF2自润滑复合陶瓷材料。在摩擦磨损实验机上对其进行摩擦磨损实验,并对其摩擦磨损行为及自润滑效应进行分析。结果表明:在实验过程中,Al2O3/TiC/CaF2复合陶瓷材料物理机械性能优于同条件下制备的Al2O3/TiC复合陶瓷材料,且具有较低的摩擦因数和磨损率,其减摩抗磨效果明显,具有一定的自润滑效应,其减摩抗磨机理为摩擦驱动下CaF2存在于摩擦副表面,形成减摩抗磨层,在表面形成一层平整、光滑的自润滑层,增加摩擦表面实际接触面积,起到自润滑效应。     

Y2O3/ZrO2复合泡沫陶瓷烧结的初步研究

本文采用有机泡沫浸渍法制备了Y2O3/ZrO2双层复合、Y2O3/Y2O3-ZrO2/ZrO2三层复合及Y2O3和ZrO2单相泡沫陶瓷,分析了两种复合泡沫陶瓷层间的结合及各层显微结构随烧结温度的变化,并与单相氧化物陶瓷进行了对比。结果表明:双层复合陶瓷层间有较大缝隙,这是因为两种氧化物陶瓷烧结不同步造成的。三层复合陶瓷中Y2O3-ZrO2混合中间层的存在减弱了Y2O3、ZrO2烧结不同步引起的层间应力,层间结合明显改善,并大大减少了泡沫陶瓷表面宏观裂纹。两种复合陶瓷的ZrO2内层的烧结程度都低于单相ZrO2,这主要是因为先于ZrO2烧结的Y2O3外层阻碍了内部气体的排出从而阻碍ZrO2的烧结所致。     

泥浆中磨粒对Al2O3增强Y-TZP复合陶瓷材料耐磨性的影响

在不同磨粒的5;NaOH泥浆中,采用销-盘式摩擦磨损试验机考察了磨粒对氧化铝增强四方氧化锆多晶陶瓷材料(ADZ)耐磨性的影响进行了研究.结果表明:尖锐SiO2磨粒对ADZ复合陶瓷材料磨损的影响要比球形SiO2磨粒严重得多,磨料硬度是影响陶瓷材料磨损率的重要因素,磨损率随磨粒硬度的提高而增大.在不同形状的SiO2磨粒的泥浆中,ADZ陶瓷材料的主要磨损机理为塑性变形和微犁削.在高硬度Al2O3磨料的泥浆中,ADZ陶瓷材料磨损表面以断裂机制占主导地位.     

添加纳米Ti(C7N3)的ZrO2基纳米陶瓷模具材料

本文针对模具对陶瓷材料的要求,从提高陶瓷模具材料的综合力学性能出发,采用纳米复合方法制备出具有较高综合力学性能的纳米陶瓷模具材料.研究了纳米Ti(C7N3)和Y2O3的组分含量对纳米陶瓷模具材料微观结构和力学性能的影响,结果表明添加纳米Ti(C7N3)和Y2O3的氧化锆纳米陶瓷模具材料的力学性能优于纯氧化锆陶瓷材料,纳米颗粒的添加改善了材料的微观结构和力学性能.当纳米Ti(C7N3)和Y2O3的添加量分别为17.15vol;和5 mol;时,材料的综合性能最好,其抗弯强度为814MPa、断裂韧性6.35 MPa· m1/2、维氏硬度11.87 GPa.     

含MgO-Lu2O3-Re2O3三元添加剂Si3N4陶瓷摩擦磨损性能的研究

利用球盘式摩擦磨损试验机,研究了含MgO-Lu2O3-Re2O3(La2O3,Sm2O3,Gd2O3,Er2O3)三元添加剂Si3 N4陶瓷的摩擦磨损性能.结果表明:机械磨损和摩擦化学反应为主要磨损机理.在三元添加剂中,随着第二稀土离子Re3+半径的增加,粘附层增加,Si3N4摩擦系数降低.基于横向断裂理论模型,Si3N4陶瓷单位磨损率随着1/(KB1/2H5/8)的增加而增加,其中含有第二相Lu4Si2N2O7的样品SN-LuSm和SN-LuEr优于此线性关系,表现出更好的抗磨损性能.     

添加纳米固体润滑剂的自润滑陶瓷材料高温摩擦磨损性能研究

采用真空热压烧结工艺制备了一种添加纳米固体润滑剂CaF2的自润滑陶瓷材料,研究其在室温25℃到600℃环境下与40Cr钢销干摩擦时的摩擦磨损性能.结果表明:自润滑陶瓷材料的摩擦系数与磨损率随环境温度的升高而逐渐降低,600℃时摩擦系数降低到0.21,磨损率降低到2.4×10-6 mm3/N·m.常温下自润滑陶瓷材料的磨损机理是磨粒磨损,高温环境同时存在磨粒磨损和粘着磨损.高温环境下摩擦表面纳米CaF2含量的增加和固体润滑膜的形成是摩擦磨损性能改善的主要原因.     

(C2N2H10)2Mg(HP2O7)2·2H2O synthesis and crystal structure

(C₂N₂H₁₀)₂Mg(HP₂O₇)₂·2H₂O, is a new inorganic organic hybrid structure. It has been synthetized using wet chemistry. Its crystal structure consists of cis- and trans-edge sharing [MgO₄(H₂O)₂] octahedra resulting in chains, which are linked via [HP₂O₇] units to form [Mg(HP₂O₇)₂(H₂O)₂]⁴⁻ layers. The Mg²⁺ cations and the ethylendiammonium cations are located on centers of inversion. The ethylendiammonium cations are alternately located in the interlayer space. The cohesion of the crystal is well ensured by coulombic interactions between anions and cations and by several hydrogen bonds. The diphosphate anion shows an eclipsed conformation.     

Crystal structure of Rb2[GeO2(OH)2]·2H2O

Single crystals of Rb₂[GeO₂(OH)₂] · 2H₂O are studied by X-ray diffraction. The crystals belong to the orthorhombic system, sp. gr. Pna2₁, a = 13.523(6) Å, b = 8.143(4) Å, c = 13.407(6) Å, Z = 8, R ₁ = 0.0506. In [GeO₂(OH)₂]^2? anions, the Ge-O distances (1.71–1.73(1) Å) are shorter than the Ge-OH distances (1.76–1.80(1) Å). Anions are linked to each other by pairs of hydrogen bonds to form infinite chains. The chains are linked by hydrogen bonds involving water molecules to form a 3D structure. The assignment of the bands in the IR spectrum of the compound under study is performed.     

Ultraviolet Absorption of Hg2Cl2-and Hg2Br2 Single Crystals

The optical unpolarized absorption spectra of Hg₂Cl₂ and Hg₂Br₂ single crystals were measured in the spectral range 230–400 nm. A sharp exciton peak and other absorption bands of both halides were observed near the fundamental absorption edge. The absorption peaks due to the splitting of the halogen doublet were also observed. Positions of the exciton peaks are characteristic for the Frenkel (localized) type of excitons. Possible interpretations of the other observed bands are discussed.     

Elastic properties of the dithionates Na2S2O6 · 2 H2O,K2S2O6, Rb2S2O6, CaS2O6 · 4H2O and SrS2O6 · 4 H2O

Single crystals of the title compounds having optical quality and dimensions of several cm were grown from aqueous solutions. The elastic and thermoelastic constants were determined from ultrasonic resonance frequencies of thick plates. The true point symmetry of K₂S₂O₆ and Rb₂S₂O₆, which is screened by a hexagonal hypermorphy, could be clearly revealed to be trigonal (32) by the existence of the elastic constant c₁₄. In the case of CaS₂O₆ · 4H₂O and SrS₂O₆ · 4H₂O the constant c₁₄ of the specimens appeared too small to confirm the trigonal symmetry group required from electrooptic and non-linear optic effects unambiguously. The isotypy of K₂S₂O₂ and Rb₂S₂O₆ as well as that of CaS₂O₆ · 4H₂O and SrS₂O₆ · 4H₂O is confirmed by their elastic behaviour. The mean elastic stiffness of dithionates is closely related to that of the corresponding sulphates. In the vicinity of the second-order phase transition of K₂S₂O₆ near 235 K weak anomalies of the temperature derivatives of the longitudinal elastic stiffnesses are observed.     

Optical properties of the germanate melilites Sr2MgGe2O7, Sr2ZnGe2O7 and Ba2ZnGe2O7

Refractive indices and their dispersion in the wavelength range from 365 nm to 2325 nm and transmission ranges of the tetragonal melilite‐type germanates Sr₂MgGe₂O₇, Sr₂ZnGe₂O₇ and Ba₂ZnGe₂O₇ were determined. The uniaxial positive crystals Sr₂MgGe₂O₇ and Ba₂ZnGe₂O₇ both offer the possibility for phase matched second harmonic generation, a detailed analysis of phase matching conditions is given. The refractive indices of Sr₂ZnGe₂O₇ show an isoindex (isotropic) point at 467 nm. The investigation was performed on Czochralski grown large single crystals. The crystal structure of all three germanates were determined by means of X ‐ray diffraction. The results corroborate unmodulated melilite‐type structures at room temperature. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Identification of a new family of diphosphate compounds, AI2BII3(P2O7)2: Structures of Ag2Co3(P2O7)2, Ag2Mn3(P2O7)2, and Na2Cd3(P2O7)2

Syntheses and single-crystal X-ray structural results are reported for three new mixed diphosphates of the family A^I ₂B^II ₃(P₂O₇)₂; Ag₂Co₃(P₂O₇)₂ (I), Ag₂Mn₃(P₂O₇)₂ (II), and Na₂Cd₃(P₂O₇)₂ (III). All crystallize in the triclinic system, space group P1 bar: (I) a = 5.351(4), b = 6.375(4), c = 16.532(4) Å, = 80.83(6) = 81.45(4), = 72.87(5)°, V = 528.9(6) ų, Z = 2, D _calc = 4.649 mg/m³, R/Rw = 0.0428/0.0548 for 3949 obs. reflns; (II) a = 5.432(7), b = 6.619(6), c = 16.51(3) Å, = 80.78(8) = 82.43(9), = 72.82(7)°, V = 557.7(13) ų, Z = 2, D _calc = 4.338 mg/m³, R/Rw = 0.0679/0.1303 for 2100 obs. reflns and (III) a = 5.67(3), b = 7.08(4), c = 7.90(4) Å, = 77.0(2), = 82.5(2), = 67.8(2)°, V = 286(3) ų, Z = 2, D _calc = 4.249 mg/m³, R/Rw = 0.0307/0.0342 for 1945 obs. reflns. (I) and (II) are isostructural but (III) is of a different type. All three structures are characterized by layers of P₂O₇ groups alternating with layers of mixed metal atoms. Differences are seen in the conglomerate bonding patterns of B atoms and in the irregular geometry of Ag in (I) and (II) compared to the octahedral bonding seen for Na in (III). The differences in structure may be understood in terms of the ratios of the ionic radii of A and B atoms.     

Crystal structure of bis 4-benzyl piperidinium monohydrogenmonophosphate pentahydrate, [C6H5CH2CHCH2CH2NH2CH2CH2]2HPO4·5H2O

The salt bis 4-benzyl piperidinium monohydrogenmonophosphate pentahydrate is orthorhombic with the following unit cell dimensions: a = 11.235(2) Å, b = 27.924(6) Å, c = 9.321(4) Å space group Pca2₁ with Z = 4. The structure was solved by the Patterson method and refined to final R value of 0.049 for 1802 independent reflections. The flack parameter is 0.14 with an e.s.d. of 0.23. The structure consists of infinite parallel two-dimensional [110] planes built of mutually connected ions and water molecules by strong O—H,...,O and N—H,...,O hydrogen bonding. There are no contacts other than normal van der Waals interactions between the layers.     

Synthesis and characterization of (NH4)2CuBr2Cl2·2H2O crystals

Single crystals of a new compound, (NH₄)₂CuBr₂Cl₂.2H₂O, were grown from saturated aqueous solution at room temperature by slow evaporation method. The grown crystals were characterized through elemental, powder XRD, thermal and DSC analyses and FTIR and far IR spectra. The elemental analysis and the decomposition pattern formulated using the TG‐DTG studies confirm the stoichiometry of the compound. The crystallinity of the compound is confirmed from the powder XRD pattern. A preliminary single crystal X‐ray diffraction structural analysis reveals that the title compound belongs to the orthorhombic system with a = 7.7466 Å, b = 7.783 Å and c = 8.1211 Å. The low temperature DSC shows thermal anomalies at –161.1, –156.5, –152.4, –145.2, –134, –18.5, and 1.4°C during the heating run and at –4.3, –54.8, –66.1, –90.6, –109.7 and –147.2 °C during the cooling run. The thermal hysterses indicate first order phase transitions in the title compound at these temperatures. The FTIR spectra were used to assign the characteristic vibrational frequencies due to NH₄⁺, CuX₄^2– ions and other chemical bonds. The effect of substitution of two bromine atoms on the phase transitions of a closely related crystal, diammonium tetrachloro cuprate dihydrate is also discussed. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Optical Properties of MnIn2S2Se2 Single Crystals

Optical transmittance and reflectance spectra of MnIn₂S₂Se₂ single crystals are measured in the wavelength range from 0.5 to 30 μm. The interference method is used to determine the refractive index of the compound for wavelengths between 0.8 and 12 μm. From an analysis of the absorption spectrum it follows that the fundamental edge is due to forbidden indirect transitions between parabolic bands for the polarization E ⊥ c with a gap energy of 1.50 eV at room temperature.     

Oxygen-conducting compounds with La2Mo2O9 structure in the ternary system La2Mo2O9-Sm2W2O9-Sm2Mo2O 9 + : Synthesis and properties

Polycrystalline samples in the ternary system La₂Mo₂O₉-Sm₂W₂O₉-Sm₂Mo₂O ₉ ⁺ were synthesized in air. The region of the existence of compounds with the lanthanum molybdate (La₂Mo₂O₉) structure in this system was determined. The polymorphism of the synthesized compounds was studied. Doping with samarium or with samarium and tungsten was shown to lead to the suppression of the transition between the monoclinic and cubic phases α → β and the appearance of the transition β _ms → β between two cubic phases. In samples with a high samarium content, the phase transition β _ms → β manifests itself as significant anomalies in the temperature dependences of the dielectric permeability and electric conductivity. An increase in the concentration of samarium in the samples leads to a substantial decrease in the conductivity compared with the nondoped compound La₂Mo₂O₉.