感应区熔法制备Al2O3/MgAl2O4/ZrO2共晶陶瓷

利用感应区熔法制备了Al2O3/MgAl2O4/ZrO2共晶陶瓷.当坩埚壁温为2200℃、行走速度为2mm/h时,制备了φ10 mm ×62 mm表面光滑致密的陶瓷样品.扫描电镜微观组织图显示Al2O3相和MgAl2O4相为基体相,ZrO2相以棒状镶嵌在基体中.定向凝固共晶陶瓷硬度和断裂韧性达到12 GPa和6.1 MPa·m1/2,为预烧结体的2倍和1.7倍.气孔和晶界的消失及细小规整ZrO2相在基体中的弥散分布,有效提高了材料的硬度和断裂韧性.     

区熔法制备Al2O3/MgAl2O4共晶陶瓷

利用感应区熔法制备了Al2O3/MgAl2O4共晶陶瓷.当坩埚壁温为2150℃、行走速度为5 mm/h时,获得了φ10 mm×104 mm表面光滑的圆棒.结果表明共晶陶瓷由Al2O3相和MgAl2O4相组成,分别按照(110)(311)晶面生长;Al2O3相为基体相,MgAl2O4相以非连续的片状均匀地分布在基体相之中.定向凝固共晶陶瓷的密度是理论值的99;;硬度和断裂韧性分别达到18.7 GPa和3.74 MPa·m1/2,约是预烧结体的2倍.气孔和界面非晶相的消失以及以单晶形态存在的Al2O3基体相,有效提高了材料的硬度和断裂韧性.     

Al2O3／（W，Ti）C纳米复合陶瓷材料的显微结构

使用纳米、亚微米级的α-Al2O3粉体和微米级的(W,Ti)C粉体为原料,采用热压烧结工艺制备了Al2O3/(W,Ti)C纳米复合陶瓷材料.对热压后材料的硬度、断裂韧性和抗弯强度进行了测试和分析,利用透射电镜、扫描电镜及X衍射仪对Al2O3/(W,Ti)C纳米复合陶瓷材料的微观组织和结构进行了研究.结果表明,增强相(W,Ti)C与基体Al2O3互相穿插、包裹,界面结合良好,形成了典型的骨架结构;球磨后的(W,Ti)C颗粒粒度分布广泛,热压烧结后与基体材料形成了内晶/晶间型结构;断裂模式的改变、内部残余应力场、位错机制、裂纹分叉和偏转等促进了材料强度和韧性的提高.     

Al2O3/Y2O3复合助剂对碳化硅蜂窝陶瓷烧结性能的影响研究

以碳化硅为主要原料,以羟丙基甲基纤维素(HPMC)为粘结剂,以Al2O3和Y2O3作为复合烧结助剂,采用挤出成型工艺制备出碳化硅多孔蜂窝陶瓷.探究了复合助剂Al2O3/Y2O3的加入量对蜂窝陶瓷物相组成和微观形貌的影响;研究了烧结温度对碳化硅陶瓷物相、微观形貌以及孔隙率、线收缩率、体积密度、抗压强度的影响规律.结果表明:Al2O3/Y2O3复合助剂的加入量增大和烧结温度的提高,陶瓷液相量增多;在钇铝石榴石(YAG)的共晶点1760 ℃附近,更易于析出结晶形成YAG相.烧结温度升高,陶瓷收缩率增大;体积密度和抗压强随烧结温度变化规律接近;体积密度和抗压强度在1750℃达到最大值分别为1.8 g/cm3和14.09 MPa.     

W对Mo2NiB2金属陶瓷微观结构和性能的影响

以Mo粉、Ni粉、B粉、C粉、W粉为原料,用冷压成型法及真空液相烧结法制成Mo2NiB2金属陶瓷,研究不同W含量对Mo2NiB2金属陶瓷组织与性能的影响.结果 表明:掺杂W的Mo2NiB2金属陶瓷在1000℃、120 h氧化时,属于完全抗氧化级,表面氧化物层的主晶相是Ni2O3和具有尖晶石结构的NiW2O4,随着W含量的增加,Mo2NiB2金属陶瓷的硬度逐渐增加,但其弯曲强度与断裂韧性则不断降低.     

以透辉石为烧结助剂的Al2O3陶瓷的力学性能和显微结构

利用无压烧结方法制备了添加透辉石的Al2O3基陶瓷,研究了烧结温度和保温时间对Al2O3基陶瓷的相对密度、硬度、抗弯强度和断裂韧性的影响,探讨了烧结工艺参数对Al2O3陶瓷力学性能和微观结构的影响.结果表明,Al2O3陶瓷的力学性能随烧结温度和保温时间变化趋势与材料密度的变化趋势一致;添加透辉石的Al2O3陶瓷在1520 ℃烧结140 min时,具有最佳的综合力学性能;显微结构分析表明,Al2O3陶瓷的力学性能受到其气孔率、晶粒发育情况和断裂模式的影响.     

添加剂对超重力下燃烧合成Al_2O_3/ZrO_2(4Y)的影响

基于超重力下燃烧合成Al2O3/ZrO2(4Y),通过调整SiO2引入量,研究添加剂对材料显微结构、形态与性能的影响。结果表明:添加SiO2不改变复合陶瓷相组成,但随SiO2引入量增加,陶瓷共晶团发生胞状向棒状形态的转变,且其长径比增大、体积分数下降。陶瓷致密性随SiO2引入量增加而增大,陶瓷硬度与弯曲强度则在SiO2引入量为6%时均呈现最大值,而陶瓷断裂韧性在SiO2引入量为4%时,因裂纹偏转与桥接增韧效应显著而获得最高值。     

LaMgAl11O19-Al2O3复相陶瓷的制备及其力学性能的研究

以板片状结构的LaMgAl11O19作为第二相来对Al2O3陶瓷进行增韧补强,采用无压烧结工艺在1650℃下保温4 h制备了LaMgAl11O19-Al2O3复相陶瓷,研究了LaMgAl11O19的添加量对LaMgAl11O19-Al2O3复相陶瓷的物相组成、体积密度和力学性能的影响,并结合复相陶瓷试样断面的SEM照片分析了其强韧化机理。研究表明,添加一定量的LaMgAl11O19后,LaMgAl11O19-Al2O3复相陶瓷材料的抗弯强度和断裂韧性均有明显提高,当添加LaMgAl11O19的质量分数为10%时,LaMgAl11O19-Al2O3复相陶瓷的抗弯强度和断裂韧性分别为321 MPa和5.03 MPa.m1/2,其中片状晶的拔出效应、裂纹偏转作用以及裂纹分支等增韧机制发挥了主导作用。     

ZrO2对热压AlN陶瓷的显微结构与力学性能的影响

通过添加纳米ZrO2粉体,并结合Y2O3烧结助剂,采用热压烧结制备了AlN陶瓷.结果表明,加入ZrO2后,热压AlN陶瓷的物相包含AlN主相、Al5Y3O12晶界相以及ZrN新相.随着ZrO2的加入,热压AlN陶瓷的维氏硬度基本没有变化,然而其断裂韧性逐渐提高.这主要是由于添加的ZrO2与AlN发生高温反应生成了ZrN,导致AlN陶瓷从单一的沿晶断裂模式转变为包含沿晶和穿晶的混合断裂模式,强化了晶界,进而改善了断裂韧性.     

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.     

(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)     

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.     

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.     

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.