304不锈钢表面CrAlN涂层制备及其耐腐蚀性能研究

采用电弧离子镀膜技术在单晶硅和304不锈钢表面制备了CrN、CrAlN涂层，对涂层的微观结构、表面形貌、机械性能及在人工海水中的耐腐蚀性能进行了研究。通过XRD、SEM对涂层的微观结构及表面形貌的研究结果表明：CrAlN涂层具有更少的表面缺陷和内部大颗粒，截面有着更致密的结构，CrN涂层沿CrN(200)择优生长，而CrAlN涂层则沿CrN(111)择优生长。对CrN、CrAlN涂层及304不锈钢基底的摩擦系数测试表明：CrAlN涂层的摩擦系数均比CrN涂层和304不锈钢的摩擦系数低。对304不锈钢基底及涂层在人工海水中的电化学极化曲线、Nyquist图进行的测试结果表明：CrAlN涂层的容抗弧半径远大于CrN涂层以及304不锈钢，其腐蚀电流密度与自腐蚀电位与CrN涂层相当，均比304不锈钢表现更为优异。     

多弧离子镀制备的大厚度Cr/Cr_2N/CrN多层涂层的结构和力学性能（英文）

采用多弧离子镀制备一种厚度为24.4μm的Cr/Cr2N/CrN多层结构涂层。采用场发射扫描电子显微镜(FESEM)、X射线光电子能谱(XPS)、能量散射谱(EDS)、X射线衍射(XRD)和透射电镜(TEM)对涂层进行表征,并用纳米压痕和划痕仪测试其硬度和结合力。用UMT-3MT往复式摩擦磨损试验机对涂层在大气和海水环境中的摩擦性能进行测试。结果表明,该涂层由3种相结构组成,分别是Cr相、Cr2N相和CrN相。相对于单层CrN涂层,多层涂层的结合力明显提高,该涂层的硬度为(21±2)GPa。多层结构涂层在人工海水中的耐蚀性能显著优于单层CrN涂层的耐蚀性能,且在大气和海水中多层结构涂层的摩擦因数均低于单层CrN涂层的摩擦因数。     

调制周期对Cr/CrN纳米多层膜的结构与性能的影响

采用多弧离子镀技术在65Mn钢表面制备了不同调制周期的Cr/CrN纳米多层膜.采用俄歇能谱仪(AES)、扫描电子显微镜(SEM)、X射线衍射仪(XRD)、纳米硬度仪、轮廓仪和划痕仪,分析了不同调制周期Cr/CrN纳米多层膜的成分分布、微观结构、力学性能、残余应力和结合强度.结果表明,Cr/CrN纳米多层膜的表面平整致密,截面层状调制结构清晰,其调制结构为Cr层-过渡层-CrN层的"三明治"结构,调制比约为1∶ 1.多层膜由CrN、Cr2N和Cr相组成,在CrN(200)方向上出现择优取向.当调制周期为80 nm时,多层膜的硬度值相对较高.随调制周期的增大,Cr/CrN多层膜的残余应力值减小,结合强度值先增大后减小.当调制周期为120 nm时,涂层的划痕临界载荷值相对较高,为69 N.     

基体偏压对高功率脉冲磁控溅射制备CrAlN薄膜性能的影响

为了防止氢扩散导致金属材料的失效,通常在其表面制备一层CrN阻氢薄膜。但是CrN涂层的热稳定性较差,抗氧化温度低于600℃。采用高功率脉冲磁控溅射技术,利用Cr和Al双靶共沉积CrAlN薄膜来提高其高温抗氧化性能。试验变量为基体负偏压的大小,分别为-100 V、-200 V、-300 V和-400 V。结果表明,四组CrAlN薄膜均为柱状晶结构,随着基体偏压提高,膜层的致密度提高,但同时薄膜沉积速率下降;CrAlN薄膜的择优生长方向为Cr(200)晶面法线方向。四组CrAlN薄膜的氢抑制率均超过70%,氢原子扩散系数最低比316L不锈钢基体低3个数量级。当基体偏压为-300 V时,可以同时获得最优的氢抑制率(87.4%)和最低的氢原子扩散系数(6.188×10^-10 cm²/s)。600℃、氧气气氛下保温60 min,CrAlN膜基结合面处氧含量仅为表面处的30%左右。相比于CrN薄膜,在相同基体偏压下,CrAlN薄膜的氢原子扩散系数更小;高偏压下制备的CrAlN薄膜氧增重量仅为316L不锈钢基体的10%,抗氧化性能更好。     

调制比对Cr/CrN/Cr/CrAlN多层膜结构及性能的影响

目的 探究Cr/CrN/Cr/CrAlN多层膜的最佳调制比.方法 利用电弧离子镀技术,在TC4钛合金上制备了不同调制比的Cr/CrN/Cr/CrAlN多层膜.利用扫描电子显微镜观察膜层表面和截面形貌;用Image-Pro分析软件对表面的大颗粒进行定量分析;利用X射线衍射法表征膜层的晶体结构;采用维氏硬度计测量膜层的显微硬度;采用划痕试验仪测量膜层与基体之间的结合力(临界载荷);通过基片弯曲法测量并计算得到膜层的残余应力;利用根据ASTM G76-05标准特制的AS600-喷砂试验机进行了抗冲蚀性能测试;采用三维表面轮廓仪测量冲蚀坑深度.结果 膜层表面质量和生长取向与LCr/CrN:LCr/CrAlN调制比密切相关,随着Cr/CrN比例的增加,膜层表面质量越来越好,择优取向由(111)晶面转为(200)晶面.多层膜的硬度随Cr/CrN比例的增加,呈下降趋势,结合力、残余应力和韧性则随之呈先升后降的趋势,并在LCr/CrN:LCr/CrAlN为1:2时,达到最佳.多层膜的抗砂粒冲蚀性能变化与力学性能变化一致,在LCr/CrN:LCr/CrAlN为1:2时达到最佳,其抗冲蚀能力是TC4基材的3倍以上,多层膜呈典型的脆性断裂失效形式.结论 在调制比LCr/CrN:LCr/CrAlN=1:2时,膜层获得最佳的抗冲蚀性能.     

CrN/CrAlSiN涂层海水环境下的摩擦学性能

为提高海洋装备摩擦零部件的摩擦学性能,采用多弧离子镀技术在316L不锈钢上制备了CrN/CrAlSiN涂层。通过XRD、XPS表征涂层的物相及成分,SEM和TEM表征涂层的形貌和微观结构,并用纳米压痕仪测试其硬度,采用摩擦磨损试验机对涂层在大气和海水环境中的摩擦磨损性能进行测试。结果表明:CrN/CrAlSiN涂层的微观结构主要有CrN相、AlN相以及非晶态Si_3N_4包裹CrN、AlN相,(111)择优取向最为明显;基于微观结构与CrN过渡层的设计,CrAlSiN涂层硬度高达35.5 GPa;较之于316L基底,涂层致密的结构使其在海水环境下表现出更好的耐腐蚀性能;在大气和海水环境下,CrN/CrAlSiN涂层的摩擦因数及磨损率均明显降低,在海水环境下达到最优。     

磁控溅射制备的Cr/CrN和Cr/CrN/CrAlN涂层耐腐蚀性能对比研究

目的比较Cr/CrN/CrAlN涂层和Cr/CrN交替涂层的耐腐蚀性能。方法利用电化学极化曲线、阻抗谱和中性盐雾试验进行测量,结合扫描电子显微镜(SEM)和原子力显微镜(AFM)表征微观形貌,分析两种涂层耐腐蚀性能的差异。同时,为研究涂层在服役中的损伤工况,分析了预制划痕对Cr/CrN/CrAlN涂层耐腐蚀性能的影响。结果Cr/CrN/CrAlN涂层的自腐蚀电流密度较Cr/CrN交替涂层和TC4基体低2个数量级,腐蚀速率较小。无损伤的Cr/CrN/CrAlN涂层的极化电阻Rp为868.7 kΩ·cm^2,预制1条损伤划痕涂层的极化电阻为792.0 kΩ·cm^2,而带有5条损伤划痕涂层的极化电阻Rp仅为77.2 kΩ·cm^2,减小至原始涂层的8%。Cr/CrN/CrAlN涂层经288 h连续盐雾腐蚀后增重仅为0.1 mg/cm^2,远小于CrN涂层和TC4基体,且增重速率趋于平缓。CrN涂层在连续盐雾腐蚀24 h后,腐蚀增重速率明显增加。结论由于Cr/CrN/CrAlN涂层结构增加了微裂纹和位错运动的界面阻塞,避免孔隙的连通,阻碍了腐蚀介质进入基体,因此涂层的耐腐蚀性能提高。对于表面预制划痕的Cr/CrN/CrAlN涂层,首先发生涂层的局部腐蚀,通过阴极极化加速后,腐蚀凹坑延伸到涂层/基体界面,加剧涂层的局部剥离。     

磁控溅射Cr/CrN和Cr/CrN/CrAlN涂层的抗高温氧化性能

为了提高航空紧固件涂层的高温工况防护能力,采用磁控溅射技术在钛合金表面分别制备 Cr/ CrN 交替涂层和 Cr/ CrN / CrAlN 涂层,研究氧化时间和氧化温度对涂层高温氧化性能影响。 利用 SEM、EDS 和 XRD 进行微观形貌和物相成分分析,采用热重法分析氧化增重量( w) 和氧化速率常数( k) ,使用显微硬度计测试涂层高温氧化后硬度。 结果表明:随着氧化时间和氧化温度的增加,涂层硬度均降低,但 Cr/ CrN / CrAlN 涂层下降趋势更缓; 两种涂层的 w 和 k 均上升,其中 Cr/ CrN / CrAlN 涂层 w 和 k 增幅均低于 Cr/ CrN 交替涂层,950 ℃ 氧化 96 h 后 Cr/ CrN / CrAlN 涂层和 Cr/ CrN 交替涂层的 w 值分别为 40 mg / cm ² 和 135. 7 mg / cm ² ,其对应的 k 分别为 0. 1996 和 0. 4092,说明 Cr/ CrN / CrAlN 涂层抗高温氧化性更好。 Cr/ CrN / CrAlN 涂层活化能 E_a 值比 Cr/ CrN 交替涂层高 48. 5%,Cr/ CrN / CrAlN 涂层在高温下产生 Cr₂O₃ 和 Al ₂O₃ 的混合氧化物,结构更致密,Cr/ CrN / CrAlN 涂层抗高温氧化性能高于 Cr/ CrN 交替涂层。     

TiAlN/CrAlN纳米结构多层膜的结构与性能

采用射频磁控溅射方法制备了单层TiAlN、CrAlN复合薄膜以及不同调制周期和不同层厚比(lTiAlN/lCrAlN)的TiAlN/CrAlN纳米结构多层膜.薄膜采用X射线衍射仪、扫描电子显微镜、显微硬度仪进行表征.结果表明:TiAlN、CrAlN复合薄膜和TiAlN/CrAlN多层膜均为面心立方结构,呈(111)面择优取向.TiAlN/CrAlN多层膜的择优取向与调制周期和层厚比无关.层厚比为1的TiAlN/CrAlN多层膜的硬度依赖于调制周期,在调制周期为8 nm时,达到最大;固定TiAlN的厚度为4 nm,改变CrAlN层的厚度,在研究范围内,多层膜的硬度随着CrAlN层厚度的增加而增加.探讨了多层膜的致硬机制.TiAlN/CrAlN多层膜抗氧化温度比其组成单层膜高了近200 ℃,并讨论了其抗氧化机制.     

TC4钛合金表面涂层改性:CrN素多层

目的 提高TC4钛合金的硬度和耐磨损性,改善CrN硬质涂层与TC4钛合金的适应性.方法 采用等离子体增强磁控溅射系统,通过调节热丝放电电流,在TC4钛合金基体表面沉积疏密CrN单层和素多层涂层.利用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、能谱仪(EDS)、纳米压痕仪、洛氏压痕仪、摩擦磨损仪以及台阶仪,表征涂层形貌、成分、物相及性能.采用动电位极化法表征涂层的耐腐蚀性.结果 当热丝放电电流为较低的4 A×4时,沉积的CrN单层涂层为具有针孔、孔洞等缺陷的疏松结构,8 A×4沉积的CrN单层涂层具有致密结构,周期性调节热丝放电电流则获得疏密交替的CrN素多层涂层.CrN涂层均由单一面心立方结构的CrN相组成,疏松CrN单层涂层的衍射晶面为(111)、(200)、(220)及(222),致密CrN单层涂层沿(111)晶面择优生长,随着疏密子层调制比的增大,CrN素多层涂层的(111)衍射峰不断增强.疏松CrN单层涂层的最小H和最大E分别为13.0 GPa和207.5 GPa,调制比为1:4的疏密CrN素多层涂层的最小H和最大E分别为17.0 GPa和257.4 GP.在1470 N载荷下洛式压痕法表明,致密CrN单层涂层的结合强度最低,等级为HF5,其余涂层均为HF1—HF4.CrN涂层的自腐蚀电位较TC4钛合金均发生了正移.结论 CrN硬质涂层可以有效提高TC4钛合金的硬度和耐磨损性,表面得到明显强化.周期性调节等离子体密度所沉积的疏密CrN素多层涂层与单层相比,涂层性能明显改善.     

Effects of Post-weld Heat Treatment on Microstructure,Mechanical Properties and the Role of Weld Reinforcement in 2219 Aluminum Alloy TIG-Welded Joints

In as-welded state, each region of 2219 aluminum alloy TIG-welded joint shows diff erent microstructure and microhardness due to the diff erent welding heat cycles and the resulting evolution of second phases. After the post-weld heat treatment, both the amount and the size of the eutectic structure or θ phases decreased. Correspondingly, both the Cu content in α-Al matrix and the microhardness increased to a similar level in each region of the joint, and the tensile strength of the entire joint was greatly improved. Post-weld heat treatment played the role of solid solution strengthening and aging strengthening. After the post-weld heat treatment, the weld performance became similar to other regions, but weld reinforcements lost their reinforcing eff ect on the weld and their existence was more of an adverse eff ect. The joint without weld reinforcements after the post-weld heat treatment had the optimal tensile properties, and the specimens randomly crack in the weld zone.     

The First Phase of the SRIF Industrialized Base in ＂West Area＂ Has Been Put into Operation

After nearly two years＇ tense construction, the first phase of industrialized base of Shenyang Research Institute of Foundry （SRIF）, located at the Tiexi Casting and Forging Industrial Park in the west of Tiexi District, has now been completed and formally put into operation.     

Thermodynamics Study on the Decomposition of Chromite with KOH

Institute of Process Engineering, Chinese Academy of Sciences, China, has proposed a method for oxidative leaching of chromite with potassium hydroxide. Understanding the mechanism of chromite decomposition, especially in the potassium hydroxide fusion, is important for the optimization of the operating parameters of the oxidative leaching process. A traditional thermodynamic method is proposed and the thermal decomposition and the reaction decomposition during the oxidative leaching of chromite with KOH and oxygen is discussed, which suggests that chromite is mainly destroyed by reactions with KOH and oxygen. Meanwhile, equilibrium of the main reactions of the above process was calculated at different temperatures and oxygen partial pressures. The stable zones of productions, namely, K2CrO4 and Fe2O3, increase with the decrease of temperature, which indicates that higher temperature is not beneficial to thermodynamic reactions. In addition, a comparison of the general alkali methods is carried out, and it is concluded that the KOH leaching process is thermodynamically superior to the conventional chromate production process.     

Influence of Heat Treatment on Damping Behaviour of the Magnesium Wrought Alloy AZ61

The effect of isochronal heat treatments for 1h on variation of damping, hardness and microstructural change of the magnesium wrought alloy AZ61 was investigated. Damping and hardness behaviour could be attributed to the evolution of precipitation process. The influence of precipitation on damping behaviour was explained in the framework of the dislocation string model of Granato and Lücke.     

Effect of Rare Earth Doping on Impedance,Modulus and Conductivity Properties of Multiferroic Composites:0.5(BiLa_xFe_(1-x)O_3)–0.5(PbTiO_3)

The Lanthanum-doped bismuth ferrite–lead titanate compositions of 0.5(Bi LaxFe1-xO3)–0.5(Pb Ti O3)(x = 0.05,0.10,0.15,0.20)(BLxF1-x-PT) were prepared by mixed oxide method.Structural characterization was performed by X-ray diffraction and shows a tetragonal structure at room temperature.The lattice parameter c/a ratio decreases with increasing of La(x = 0.05–0.20) concentration of the composites.The effect of charge carrier/ion hopping mechanism,conductivity,relaxation process and impedance parameters was studied using an impedance analyzer in a wide frequency range(102–106Hz) at different temperatures.The nature of Nyquist plot confirms the presence of bulk effects only,and non-Debye type of relaxation processes occurs in the composites.The electrical modulus exhibits an important role of the hopping mechanism in the electrical transport process of the materials.The ac conductivity and dc conductivity of the materials were studied,and the activation energy found to be 0.81,0.77,0.76 and 0.74 e V for all compositions of x = 0.05–0.20 at different temperatures(200–300 °C).     

Quantitative Analysis of the Crystallographic Orientation Relationship Between the Martensite and Austenite in Quenching–Partitioning–Tempering Steels

The orientation relationships(ORs)between the martensite and the retained austenite in low-and medium-carbon steels after quenching–partitioning–tempering process were studied in this work.The ORs in the studied steels are identified by selected-area electron diffraction(SAED)as either K–S or N–W ORs.Meanwhile,the ORs were also studied based on numerical fitting of electron backscatter diffraction data method suggested by Miyamoto.The simulated K–S and N–W ORs in the low-index directions generally do not well coincide with the experimental pole figure,which may be attributed to both the orientation spread from the ideal variant orientations and high symmetry of the low-index directions.However,the simulated results coincide well with experimental pole figures in the high-index directions{123}_(bcc).A modified method with simplicity based on Miyamoto’s work was proposed.The results indicate that the ORs determined by modified method are similar to those determined by Miyamoto’method,that is,the OR is near K–S OR for the low-carbon Q–P–T steel,and with the increase of carbon content,the OR is closer to N–W OR in medium-carbon Q–P–T steel.     

Using Finite Element and Contour Method to Evaluate Residual Stress in Thick Ti-6Al-4V Alloy Welded by Electron Beam Welding

This work was to reveal the residual stress profile in electron beam welded Ti-6Al-4V alloy plates(50 mm thick) by using finite element and contour measurement methods.A three-dimensional finite element model of 50-mmthick titanium component was proposed,in which a column–cone combined heat source model was used to simulate the temperature field and a thermo-elastic–plastic model to analyze residual stress in a weld joint based on ABAQUS software.Considering the uncertainty of welding simulation,the computation was calibrated by experimental data of contour measurement method.Both test and simulated results show that residual stresses on the surface and inside the weld zone are significantly different and present a narrow and large gradient feature in the weld joint.The peak tensile stress exceeds the yield strength of base materials inside weld,which are distinctly different from residual stress of the thin Ti-6Al-4V alloy plates presented in references before.     

Microstructures and Tensile Properties of Ultrafine-Grained Ni–(1–3.5) wt% SiC_(NP) Composites Prepared by a Powder Metallurgy Route

Silicon carbide nanoparticle-reinforced nickel-based composites(Ni–Si CNP),with a Si CNPcontent ranged from1 to 3.5 wt%,were prepared using mechanical alloying and spark plasma sintering.In addition,unreinforced pure nickel samples were also prepared for comparative purposes.To characterize the microstructural properties of both the unreinforced pure nickel and the Ni–Si CNPcomposites transmission electron microscopy(TEM) was used,while their mechanical behavior was investigated using the Vickers pyramid method for hardness measurements and a universal tensile testing machine for tensile tests.TEM results showed an array of dislocation lines decorated in the sintered pure nickel sample,whereas,for the Ni–Si CNPcomposites,the presence of nano-dispersed Si CNPand twinning crystals was observed.These homogeneously distributed Si CNPwere found located either within the matrix,between twins or on grain boundaries.For the Ni–Si CNPcomposites,coerced coarsening of the Si CNPassembly occurred with increasing Si CNPcontent.Furthermore,the grain sizes of the Ni–Si CNPcomposites were much finer than that of the unreinforced pure nickel,which was considered to be due to the composite ball milling process.In all cases,the Ni–Si CNPcomposites showed higher strengths and hardness values than the unreinforced pure nickel,likely due to a combination of dispersion strengthening(Orowan effects) and particle strengthening(Hall–Petch effects).For the Ni–Si CNPcomposites,the strength increased initially and then decreased as a function of Si CNPcontent,whereas their elongation percentages decreased linearly.Compared to all materials tested,the Ni–Si CNPcomposite containing 1.5% Si C was found more superior considering both their strength and plastic properties.     

Directional Growth of Tin Crystals Controlled by Combined Solute Concentration Gradient Field and Static Magnetic Field

A new method was introduced to achieve directional growth of Sn crystals. Microstructures in liquid(Pb)/liquid(Sn) diffusion couples were investigated under various static magnetic fields. Results show that the β-Sn crystals mainly reveal an irregular dendritic morphology without or with a relatively low static magnetic field(B0.3 T). When the magnetic field is increased to 0.5 T, the β-Sn dendrites close to the final stage of growth begin to show some directional character. With a further increase in the magnetic field to a higher level(0.8–5 T), the β-Sn dendrites have an enhanced directional growth character, but the dendrites show a certain deflection. As the magnetic field is increased to 12 T, the directional growth of the β-Sn dendrites in the center of the couple is severely destroyed. The mechanism of the directional growth of the β-Sn crystals and the deflection of the β-Sn crystals with the application of static magnetic field was tentatively discussed.     

电化学噪声数据处理方法概述

综述了常见的电化学噪声数据处理方法,介绍了直流趋势剔除、统计分析、快速傅立叶变换(FFT)法计算功率谱密度(PSD)以及小波变换处理电化学噪声信号的基本过程,并阐释了各种数学处理及所得参数的物理意义。