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1.
采用电弧离子镀技术及后续热处理工艺在镍基高温合金上制备了均匀NiCrAlY涂层和梯度NiCrAlY涂层,分析了2种涂层的组织结构,对比研究了2种涂层静态空气下1000和1100℃恒温氧化行为以及1100℃的循环氧化行为.结果表明:均匀NiCrAlY涂层由γ′/γ相和少量β-NiAl相、α-Cr相组成,成分分布均匀;梯度NiCrAlY涂层具有外层富Al和内层富Cr的结构,其中外层由β-NiAl相和少量γ′/γ相、α-Cr相组成.一方面,梯度涂层的初始Al含量较高;另一方面,氧化过程中其富Cr区两侧出现了对富Al区的Al向基体扩散起阻碍作用的Cr(W)析出带.这两方面使梯度涂层长时间维持更多的Al存储相,提升了氧化膜的迅速生成及再生成能力,从而使涂层具有较好的抗氧化性能.  相似文献   

2.
通过调整固体粉末渗铝法工艺在镍基高温合金DZ417G基体上制备了Ni-Al二元成分区间内组织可控的γ′-Ni3Al、γ′-Ni3Al+β-NiAl、β-NiAl、β-NiAl+δ-Ni2Al3和δ-Ni2Al3涂层,采用光学显微镜、X射线衍射仪和扫描电镜对涂层的结构、断面形貌以及高温氧化后的表面形貌进行观察和分析。900℃和1 100℃空气恒温氧化实验结果表明:涂层能显著提高材料的抗氧化性能,在涂层厚度相同的情况下,NiAl涂层抗氧化性能最好。  相似文献   

3.
目的通过电弧离子镀技术,获得抗氧化性能优良的NiAl涂层。方法采用电弧离子镀技术,在弧流为110 A,偏压为-50 V的参数下沉积NiAlHf涂层。通过X射线衍射仪(XRD)和扫描电子显微镜(SEM)对涂层的物相结构和形貌进行分析,通过能谱仪(EDS)分析涂层的成分。采用恒温氧化增重实验对涂层的氧化动力学进行分析。结果由电弧离子镀技术制备的NiAl涂层致密均匀,无大颗粒、孔洞等缺陷。涂层主要由β-NiAl相组成,活性元素Hf固溶在主相中。NiAlHf涂层表现出良好的抗高温氧化性能,动力学曲线符合抛物线规律,在1150℃下恒温氧化200h的平均氧化速率为0.0841g/(m^2×h),远优于传统MCrAlY涂层体系。NiAlHf涂层在氧化初期形成保护性的α-Al2O3氧化皮以及少量亚稳态的θ-Al2O3,随后θ-Al2O3逐渐转变为稳态的α-Al2O3。Hf在涂层表面富集从而形成HfO2,对氧化皮形成了钉扎作用,增强了氧化皮的粘附性,提高了涂层的抗氧化性能。随着氧化的进行,涂层中的β-NiAl相逐渐转变为γ'-Ni3Al相。结论 NiAlHf涂层在1150℃下仍具备优良的抗高温氧化性能,对下一代耐更高温度涂层开发,电弧离子镀NiAl涂层的技术推广及工业化应用有一定的指导作用。  相似文献   

4.
以镍基高温合金GH586为基体材料,采用电镀Pt和固体粉末包埋渗铝的方法在其表面制备PtAl涂层。采用X射线衍射(XRD)、扫描电镜(SEM)对不同渗铝时间下PtAl涂层的高温氧化过程中各阶段的物相结构及微观组织变化进行表征及分析。研究表明,在高温氧化过程中,随着渗铝时间的增加,涂层中β-NiAl相转变为γ'-Ni_3Al相的几率越小,迅速生成Al_2O_3膜的时间越短,形成起扩散障作用的Cr、W等元素富集区的厚度越大,从而大大提高了镍基合金的抗氧化性。渗铝3 h的PtAl涂层具有最优的抗氧化性能,其氧化速率常数k_(3h)=1.17×10~(-6)。  相似文献   

5.
采用磁控溅射和电弧离子镀技术在γ-TiAl合金表面制备NiCrAlY/Al复合涂层,研究了复合涂层对提高γ-TiAl合金抗高温氧化性能的作用机理。经950℃恒温氧化100 h后,涂层表面未发现裂纹和脱落,涂层试样氧化增重值较基体大幅减小。对氧化层进行了SEM、EDS和XRD分析,结果表明无保护涂层的基体γ-TiAl合金表层疏松多孔,无法抵抗高温环境下氧气对基体合金的侵蚀。复合涂层表面的NiCrAlY镀层在氧化过程中形成了Cr2O3,α-Al2O3和β-NiAl相组成的致密防护涂层,阻隔了氧气与基体的接触,中间的Al层为表层持续生成Al2O3提供了Al源。NiCrAlY/Al复合涂层显著提高了基体在950℃下的抗高温氧化性能。  相似文献   

6.
用磁控溅射法在镍基单晶高温合金基体上沉积NiCrAlY涂层,研究了真空热处理对涂层组织结构及抗氧化性能的影响。结果表明,溅射NiCrAlY涂层主要由γ-Ni和β-NiAl两相组成,元素分布均匀;经真空热处理后,涂层主要由γ‘-Ni3Al、β-NiAl相和极少量的α-Al2O3相组成,元素分布变得不均匀,最外层富Al贫Cr。真空热处理可使溅射NiCrAlY涂层表面较早生成保护性能良好的α-Al2O3.1000℃氧化200h,溅射涂层氧化膜有较大部分已经剥落,但真空热处理涂层的氧化膜仍较好地粘附在涂层基体上。真空热处理使溅射NiCrAlY涂层表面生成的氧化膜粘附性更好,提高了溅射NiCrAlY涂层的抗氧化性能。  相似文献   

7.
高温合金渗铝涂层抗高温氧化性能的研究   总被引:4,自引:0,他引:4  
采用固体粉末包埋渗铝法,在K438高温合金表面制备渗铝涂层。对渗铝试样做了1000℃、500h高温氧化实验。实验结果表明:在氧化过程中,K438高温合金表面的涂层已转变成连续致密的α—Al2O3氧化膜、富Al的β-NiAl和富Ni的β—NiAl化合物层,氧化膜与基体合金粘附良好,在高温氧化过程中无明显剥落现象。随着氧化时间的增加,β相分解较慢,到500h时涂层仍具有良好的抗高温氧化性能。  相似文献   

8.
为提高镍基高温合金抗高温氧化性能,采用两步法制备了内扩散型铬铝涂层与单一渗铝涂层。当保温时间9 h、渗铬温度为1080℃、渗铬剂配比为:Cr粉含量为30%、NH4Cl含量为1%、Al2O3含量为69%;渗铝保温时间15 h、温度为750℃、渗铝剂配比为:Al粉含量为10%、NH4Cl含量为1.5%、Al2O3含量为88.5%;热处理保温时间为15 h、温度为800℃时可以得到期望的内扩散型β-NiAl和γ'-NiAl相,涂层组织均匀致密,可显著提高镍基高温合金基体在1100℃的抗高温氧化性能。  相似文献   

9.
目的 探究某重型燃气轮机涡轮叶片服役过程中表面裂纹的形成原因。方法 利用场发射扫描电子显微镜及能谱仪确定开裂叶片裂纹周围的显微组织及元素分布情况,揭示高温氧化导致的涂层外表面及涂层/叶片基体界面处的组织演变规律。结果 此叶片经高温长时间服役后,表面未发现热障涂层,抗氧化涂层是NiCoCrAlY涂层,主要显微组织为γ-Ni相+β-NiAl相;叶片基体材质为GTD-111镍基高温合金,主要显微组织为γ-Ni相+γ’-Ni3(Al, Ti)相及γ/γ’共晶组织和块状(Ti, Ta)C碳化物。表面裂纹主要集中于叶身与叶根的过渡平台位置。涂层内部、裂纹周围及涂层/叶片基体界面处均发现明显的金属氧化现象,氧化产物主要为金属Al和Cr的氧化物。高温服役环境下,铝元素的氧化导致涂层外表面的β-NiAl相及涂层/叶片基体界面位置的γ’-Ni3(Al, Ti)相向γ-Ni相转变,导致上述2位置的弱化。此外,截面形貌表明,在涂层表面位置,裂纹与凹坑相连接,并呈现向涂层内部扩展的态势,局部位置已贯穿抗氧化涂层,并扩展进入叶片基体。结论 由于高温氧化导致涂层表面Al含...  相似文献   

10.
NiCrAlY涂层/Ni基单晶高温合金的元素扩散及界面特性   总被引:5,自引:0,他引:5  
采用磁控溅射方法在Ni基单晶高温合金上沉积NiCrAlY涂层,研究了真空热处理及高温氧化过程中,NiCrAlY涂层/Ni基单晶合金界面显微结构的变化及元素扩散行为。结果表明,原始涂层成分分布比较均匀,各元素分布在涂层/基体界面呈陡然变化。真空热处理时,涂层与基体间发生互扩散,NiCrAlY涂层的显微结构和相结构发生变化:涂层/基体界面区出现互扩散层(内、外扩散层);出现γ-Ni3Al和α-Cr两新相,导致涂层局部区域富Cr。1000℃氧化200h后,涂层/基体界面区的互扩散层增厚,并且在其下的基体中出现扩散影响层。Ta在涂层中扩散时,置换了部分γ-Ni3Al相中的Al,导致γ相的晶格常数α0增大。  相似文献   

11.
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.  相似文献   

12.
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.  相似文献   

13.
吴玉梅  熊晓云  靳蓉  孙敬民  杨林  罗晓星 《金属学报》2005,10(10):1100-1103
目的: 观察本实验室合成的一种治疗阿尔茨海默氏症(AD)的药物(1-二甲基磷酰基-2, 2, 2 -三氯)-乙基-1-醇烟酸醋(NMF),对体外培养的皮层神经细胞活性的影响以及对海人藻酸(KA)所致的神经损伤的保护作用。方法: 采用体外培养皮层神经元的方法,解剖分离 15 d胚胎小鼠皮层神经细胞, 接种于 96孔板,48 h 后加药并培养 72 h,以 MIT 法 观察 NMF 对小鼠皮层神经细胞活性的影响;同时将接种于 24 孔板的细胞预先给予 NMF,d 3 时加或不加KA处理后,以台盼蓝染色鉴别并计数死、活细胞,可得出细胞的存活率。结果: NMF 明显促进胎鼠皮层神经元活性,其中 NMF1、0. 1、10nmol·L-1促进神经元活性增殖率分别高达 34.7%、37.4%、36. 7%, NMF 明显促进正常胎鼠皮层神经元存活卒,与对照组比较,10nmol·L-1 NMF 对皮层神经元的存活率分别提高 39.3%、73.5%。 NMF能显著 对抗 KA 所致的神经元损伤,与 KA 损伤组相比, NMF0.1、10、10nmol·L-1对损伤皮层神经元的保护率分别为 77.30%、80.10%、84.15%。结论: NMF 明 显促进胎鼠皮层神经元的洁性、提高正常皮层神经元,的存活卒,并能有效地保护KA所致的神经元损伤,提示 NMF 是一种很有潜力的治疗 AD 的药物。  相似文献   

14.
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.  相似文献   

15.
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.  相似文献   

16.
Coherent second phase often exhibits anisotropic morphology with specifi c orientations with respect to both the second and the matrix phases. As a key feature of microstructure, the morphology of the coherent particles is essential for understanding the second-phase strengthening eff ect in various industrial alloys. This letter reports anisotropic growth of coherent ferrite from austenite matrix in pure iron based on molecular dynamics simulation. We found that the ferrite grain tends to grow into an elongated plate-like shape, independent of its initial confi guration. The fi nal shape of the ferrite is closely related to the misfi t between the two phases, with the longest direction and the broad facet of the plate being, respectively, consistent with the best matching direction and the best matching plane calculated via the Burgers vector content(BVC) method. The strain energy calculation in the framework of Eshelby's inclusion theory verifi es that the simulated orientation of the coherent ferrite is energetically favorable. It is anticipated that the BVC method will be applicable in analysis of anisotropic growth and morphology of coherent second phase in other phase transformation systems.  相似文献   

17.
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).  相似文献   

18.
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.  相似文献   

19.
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.  相似文献   

20.
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.  相似文献   

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