氮在离子氮碳共渗中的作用

研究了在离子氮碳共渗过程中氮对化合物层厚度的影响,同时对化合物层的微观组织结构和显微硬度进行了分析.结果表明:在离子氮碳共渗过程中,气氛中低氮势不利于ε相的生成,且渗层的显微硬度较低;高氮势有利于ε相的生成,同时提高了渗层的显微硬度;当氮势超过60%后对化合物层厚度影响不大.     

稀土对42CrMo钢等离子体氮碳共渗表层组织的影响

对42CrMo钢在不同温度和时间下进行有、无稀土添加的脉冲等离子体氮碳共渗的工艺进行研究。通过金相检验和XRD分析,归纳出稀土对等离子体氮碳共渗的影响。结果表明：稀土的添加改善了渗层的显微组织,并降低了渗氮初期的化合物层厚度;使渗层的e相含量降低,γ＇相含量增加;并且使表面氮含量提高。     

DC53钢的离子氮碳共渗工艺及稀土催渗研究

为了探究DC53钢的优化氮碳共渗工艺,对DC53钢在530℃不同共渗时间、NH3/CO2不同气氛比值、不同炉内气压情况下的离子氮碳共渗效果进行了研究.运用OM、XRD、SEM、EDS、显微硬度、摩擦磨损实验,对材料的显微组织、显微硬度和耐磨性进行了分析.研究表明:对于冷作模具钢DC53,10 h、NH3/CO2为15∶1、炉内气压为800～1000 Pa时,氮碳共渗效果最好;随着稀土镧(La)的加入,渗层变厚且渗层与基体更致密,表层到心部的硬度梯度更小,氮碳共渗效果更佳.     

丙烷浓度对45钢离子碳氮共渗的影响

首次以丙烷作为供碳剂对45钢进行离子碳氮共渗。利用金相显微镜、X射线衍射仪和显微硬度计研究了丙烷浓度对试样截面形貌、物相组成和表面硬度的影响。结果表明:随丙烷浓度的增加,化合物层厚度和表面硬度均呈现先增大后减小的趋势。当丙烷浓度为1.5%时,510℃离子碳氮共渗4h后,化合物层厚度和表面硬度分别达到最大值40μm和779HV0.05,同时得到以ε相为主,并伴有极少量渗碳体的最优物相组成。当丙烷浓度超过1.5%时,化合物层厚度和表面硬度均下降,这是由于渗碳体相含量随丙烷的增加而增加,并当丙烷浓度为2.5%时渗碳体成为主要物相,从而阻碍了C、N原子向基体内的进一步扩渗。     

气体氮碳共渗中NH3和CO流量对低碳钢渗层组织及其性能的影响

通过调控气体氮碳共渗过程中的NH_3和CO流量来调控气氛中的氮化势和碳势,从而调控共渗层的微观组织和性能。采用扫描电镜、X射线衍射仪、显微硬度计和电化学分析仪研究了气体氮碳共渗过程中的NH_3和CO流量对低碳钢氮碳共渗层的微观组织结构及其性能的影响。研究结果表明:气体氮碳共渗气氛中,随着NH_3流量的增加,化合物层厚度增大但致密性降低;随着CO流量的增加,化合物层致密性逐渐增大,但渗层厚度先增大后减小。氮碳共渗过程中C的加入可抑制γ'相的形成而促进ε相的产生,过量的C会形成θ相,但是C的渗入对渗层腐蚀性能影响较小。NH_3和CO对氮碳共渗过程中的协同作用表现为,当NH_3流量增加时,可相应增加CO流量来获得较厚、致密、耐腐蚀的化合物层。     

离子碳氮共渗技术的研究与应用

离子碳氮共渗具有渗速快,渗层及表面质量好,变形小及节能的优点。850—870℃离子碳氮共渗后直接淬火,更适合于精密零件的热处理。实践证明这是具有推广价值的新工艺。     

钛铝基合金离子碳氮共渗及其耐磨性的研究

为提高TiAl基合金的耐磨性及抗高温氧化性,利用渗氮在TiAl基合金表面形成氮化物,以提高耐磨性;渗碳形成致密且与基体结合牢固的碳化物层,提高抗高温、抗氧化性;将二者结合,采用辉光离子碳氮共渗的方法,研究了渗层的相结构组成、不同工艺参数对TiAl基合金离子碳氮共渗后渗层厚度以及表面硬度和耐磨性的影响.结果表明:TiAl基合金共渗层是由碳氮化合物层与过渡层组成的复合相结构;随共渗温度的升高和时间的延长,渗层厚度增加;与未经共渗处理的试样相比,表面硬度及耐磨性显著提高.X射线衍射结果显示,渗层主要由TiC,TiN,AlTi3,Al2O3等组成.     

槽电压对纯铁表面液相等离子体电解硼碳氮三元共渗层摩擦磨损性能的影响

利用液相等离子体电解渗技术分别在340,360V和380V槽电压下对纯铁进行硼碳氮三元共渗(PEB/C/N)表面处理。分析纯铁表面PEB/C/N共渗层的形貌、成分、相组成和显微硬度分布。采用球-盘摩擦磨损仪评估槽电压对渗层摩擦磨损性能的影响,并分析渗层与ZrO_2球对磨时磨损机理。纯铁表面的PEB/C/N三元共渗层厚度随着放电电压升高而增大,最高硬度也相应增加。380V处理1h后硼碳氮三元共渗层中渗硼层和过渡层厚度分别达到26μm和34μm,渗层最高硬度可以达到2318HV。硼碳氮三元共渗层的磨损率仅为纯铁基体的1/10。硼碳氮共渗处理大幅度降低纯铁的摩擦因数和磨损率,但不同槽电压下制备的PEB/C/N共渗层的摩擦因数和磨损率变化较小。     

表面纳米化38CrMoAl钢的低温离子氮碳共渗

采用表面机械研磨处理（SMAT）技术实现了38CrMoAl钢的表面纳米化,并对表面纳米化后的样品进行了490℃离子氮碳共渗。采用扫描电镜、X-衍射、透射电镜、显微硬度仪等分析和测试手段,对处理后的样品进行观察分析及性能测试。结果表明：经SMAT处理的样品实现了低温离子氮碳共渗,渗层中渗入较多的氮、碳原子,并析出大量细小的高硬度化合物,获得了较好的硬度分布。     

钛合金表面等离子体电解氮碳共渗的研究

在含有硝酸铵、甘油、乙醇的水溶液中,利用等离子体电解渗入技术在Ti6Al4V钛合金表面制备了氮碳共渗层.利用SEM、XRD、GDS以及显微硬度计分析了渗层的形貌、成分、组织和显微硬度,探讨了渗层形成的机理和过程.结果表明:(1)以300V的电压经45min处理制备的渗层总厚度约为100μm,其中化合物层约为20μm,主要由Ti(C,N)相组成;(2)渗层最高显微硬度超过2000HK0.0025.等离子体电解渗入技术可以较快地在钛合金表面制备出厚度大、硬度高的氮碳共渗层.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Thermoelectric power of single-phase samples of Tl2CaBa2Cu2O y and Ba2CaSr2Cu2O y

Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-T _c . The thermopower was positive and decreased linearly with increasing temperature aboveT _c (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model.     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Structure of Na2O·2TiO2 glass

X-ray radial distribution analysis and Raman spectroscopic measurement were carried out on Na₂O-2TiO₂ glass prepared by twin-roller quenching method. It is found that four-coordinated Ti⁴⁺ ions may be predominant over six-coordinated ones in the present glass. It is also found that the fraction of six-coordinated Ti⁴⁺ ions is larger in the present glass than in K₂O·2TiO₂ and Cs₂O·2TiO₂ glasses. Poorer glass-forming ability of the Na₂O-TiO₂ system compared with the K₂O-TiO₂ and Cs₂O-TiO₂ systems is ascribed to a larger fraction of TiO₆ octahedron for the former system.     

SiO2—TiO2—ZrO2系涂层的制备及其特性

用溶胶－凝胶法（sol-gel method）在不锈钢表面制备了SiO2-TiO2-ZrO2系无机氧化膜（STZ）。用DTA／TG、IR、XRD和SEM等手段研究了涂层制备时由凝胶向玻璃态的转变以及涂层薄膜的显微结构特点，考察了涂层对基体的保护效果。试验结果表明，在溶胶至凝胶最终转变为无机氧化物的过程中形成了无机网络，Si^4 和Zr^4 充当了网络骨架的形成离子。涂层为无定型玻璃态，其间混有石英、锐钛矿或金红石等微晶。     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.     

Investigation of Instability of Lattice of Bi_2Sr_2CaCu_2O_x

Bi2Sr2CaCu2Ox superconductor was studied by differential scanning calorimetry (DSC) and thermogravimetry (TG) in different atmospheres. It is discovered that there is a thermal anomaly in the DSC curve, associated with a weight loss in the TG curve before the melting of the sample. Careful thermal analysis and high temperature X-ray diffraction reveal that the thermal anomaly and the weight loss show an instability of the crystalline Iattice. By annealing the sample in oxygen and argon, respectively and then by TC measurement and thermal analysis, the coincidence of transition temperature with the instability is found. The coincidence is further confirmed by Y-doped 2212 phase.     

Thermal conductivity of the system N2O4 ⇄ 2NO2 ⇄ 2NO + O2

Experimental data on the thermal conductivity of dissociating nitrogen tetroxide have been obtained by the hot-wire method in the temperature range from 290 to 870° K at pressures up to 10⁵ N/m².