Fe3Al金属间化合物的高温抗氧化性能

当温度超过１０００℃时,二元ＦｅＡｌ的抗氧化性能随温度上升而争剧下降,对１２００℃氧化试样的ＳＥＭ分析发现试样表面存在晶须状氧化物,氧化层与基体的界面上有大量的孔洞。微量的Ｃｅ加入Ｆｅ３Ａｌ可显著地改善合金的抗氧化性能,在１２００℃长时间氧化后,含Ｃｅ的Ｆｅ３Ａｌ试样表面平整致密,且无氧化物剥落,其抗氧化性能比不含Ｃｅ的合金提高了一个数据级。     

Fe3Al基合金高温变形过程中原位再结晶现象

ＴＥＭ及金相分析发现Ｆｅ３Ａｌ在高温变形过程中伴生原位再结晶。Ｆｅ３Ａｌ合金良好的高温塑性与ＩＳＲ有密切的关系，形变产生的晶格位错通过攀移或交滑移形成位错墙，在进一步的变形中，位错墙通过吸收晶内滑移位错增大两侧晶体的位向差，并逐渐向亚晶界和大角晶界演化。     

Fe_3Al和FeAl合金的高温氧化行为

研究了含Nb、Nb和Cr的Fe_3Al合金,含Zr的FeAl合金在1050℃的氧化行为。结果表明Fe_3Al和FeAl合金氧化增重均符合抛物线规律。对于Fe_3Al合金,氧化层由Al_2O_3和Fe_2O_3组成;加入少量Nb,增加了氧化层的粘附性,从而改善合金的抗氧化性。对FeAl合金,氧化层为Al_2O_3;Zr的加入,虽然引起合金的内氧化,但却提高Al_2O_3的粘附性。     

Fe3Al基合金的高温氧化行为

测定了Ｆｅ３Ａｌ基合金铁静态和拉庆务态下的氧化增重曲线，并与０Ｃｒ２５Ａｌ５合金进行比较，结果表明，在较低温度下Ｆｅ３Ａｌ基合金的静态氧化性能不如０Ｃｒ２５Ａｌ５；当温度高于９００℃时，Ｆｅ３Ａｌ基合金的氧化性能要比０Ｃｒ２５Ａｌ５好。但Ｆｅ３Ａｌ基合金在拉应力作用下的动态氧化性能比０Ｃｒ２５Ａｌ５差。动态下合氧化增重不仅与和氧化时间有关，还与拉应力的大小有关。文中人这似的动态氧化△ｗ＝ｋ１ｔ＾２     

B2结构Fe3Al单晶室温力学行为各向异性的研究

研究了Ｂ２结构Ｆｅ３Ａｌ单晶室温下的力学行要现,依取向不同。材料的屈服强度,延伸率,加工硬化率存在很大差异,近「１１０」取向具有最高延伸率为４２％,而近「１００」取向只获得了１４．１％的延伸率,近「１１０」取人有的高加工硬化率是位错交互作用的结果。二分位错分解为单根位错导致交滑移。进一步提高高延伸率近「２１１」取向的低加工硬化率是单系滑移的结果。在此取向下直至断裂,样品中仍为二分位错。     

Fe3Al基合金室温塑性的改善

进行了不同成分、表面状态、相结构，显微结构的Ｆｅ３Ａｌ基合金在真空及气中的温拉伸试验，结果表明，与二元Ｆｅ３Ａｌ相比，本研究Ｃｒ、Ｍｏ、Ｔｉ、Ｍｎ、Ｎｉ、Ｓｉ等代位合金元素中，仅有Ｃｒ的添加提高真空室温拉伸伸长率。     

两相NiAl—Fe金属间化合物的高温氧化行为研究

研究了ＮｉＡｌ、ＮｉＡｌ－２０Ｆｅ、ＮｉＡｌ－３０Ｆｅ金属间化合物在１０００℃￣１１００℃空气中的氧化行为。ＮｉＡｌ和ＮｉＡｌ－２０Ｆｅ显示较好的抗氧化性能,ＮｉＡｌ－３０Ｆｅ的抗氧化性能却很差。从合金相组成探讨了ＮｉＡｌ－Ｆｅ合金的氧化机制。     

Fe3Al金属间化合物堆焊材料的应用

采用东南大学研制的Fe3Al基合金的成分配方研制的堆焊材料成功堆焊18－8系不锈钢，形成了完整的焊接工艺和工艺参数，为Fe3Al的应用开辟了一条新的途径，取得了明显的经济效益。     

手弧堆焊Fe3Al堆焊层的组织形貌与抗氧化性能

通过将Fe     

超重力场辅助燃烧合成技术快速制备Fe3Al合金

利用超重力场辅助燃烧合成技术成功制备Fe3Al合金。在超重力场的辅助下,自蔓延高温反应的产物可以迅速分离和致密化,样品中仅存在极少量的气孔,孔径普遍低于2μm。研究了超重力场对自蔓延燃烧反应的影响,提高超重力系数,有利于克服坩埚内外的压力差,抑制质量和热量对外传递,提高金属产物的产率。但超重力场过大会加剧铁铝比例的失调,超重力系数越高,合金中的残留铁越多。合金与石墨坩埚接触的边缘地方发现渗碳体的形成,随着合金中残留铁的比例增高,渗碳体的数量逐渐增多,引起合金的硬度逐步增大。渗碳体的脆性很大,这会加剧Fe3Al合金的室温脆性,所以要尽可能地减少铁的残留以及防止碳的掺入。     

The corrosion of Fe3Al alloy in liquid zinc

A systematic study of the isothermal corrosion testing and microscopic examination of Fe₃Al alloy in liquid zinc containing small amounts of aluminum (less than 0.2 wt.%) at 450 °C was carried out in this work. The results showed the corrosion of Fe₃Al alloy in molten zinc was controlled by the dissolution mechanism. The alloy exhibited a regular corrosion layer, constituted of small metallic particles (diameter: 2-5 μm) separated by channels filled with liquid zinc, which represented a porosity of about 29%. The XRD result of the corrosion layer formed at the interface confirmed the presence of Zn and FeZn_6.67. The corrosion rate of Fe₃Al alloy in molten zinc was calculated to be approximately 1.5 × 10⁻⁷ g cm⁻² s⁻¹. Three steps could occur in the whole process: the superficial dissolution of metallic Cr in the corrosion layer, the new phase formation of FeZn_6.67 and the diffusion of the dissolved species in the channels of the corrosion layer.     

Fatigue crack growth of Fe3Al,Cr alloys

The ternary alloy undergoes an increase in crack propagation rate and a loss of fracture toughness in hydrogen gas and moisture bearing environments. A similar effect was seen on the ductility of the ternary alloy in tensile test. The embrittling effect in air is attributed to the oxidation of aluminum by water vapor to release hydrogen gas. The Fe---Al---Cr---Zr alloy is also embrittled by moisture in air in the same manner. However, laboratory air had a much less drastic effect on the crack growth rate and fracture toughness of the Fe---Al---Cr---Zr alloy. The addition of Zr appears to improve the crack growth characteristics of Fe₃Al-type alloys.     

Processing of high carbon Fe3Al based intermetallic alloy

A melting procedure for air induction melting (AIM) of an Fe₃Al based intermetallic alloy Fe-15.38 wt%Al-1.1 wt%C is described. Use of an appropriate slag cover during AIM results in elimination of hydrogen gas porosity in cast AIM ingots. Criteria for slag selection and slag to metal ratio are discussed. Refining by slag-metal reactions results in significant reduction in impurity levels (S, O, N) during AIM. Consequently, low cost raw materials such as mild steel scrap and commercial aluminium were used for melting the alloy. The AIM ingot exhibited excellent tensile properties. The ductility and hot workability of the ingot may be further improved by subsequent processing through electroslag remelting. It is also argued that the presence of carbon may be necessary to get AIM castings with desirable mechanical properties.     

Pulsed electric current sintered Fe3Al bonded WC composites

WC based composites with 5, 10 and 20 vol.% Fe₃Al binder were consolidated via pulsed electric current sintering (PECS) in the solid state for 4 min at 1200 °C under a pressure of 90 MPa. Microstructural analysis revealed a homogeneous Fe₃Al binder distribution, ultrafine WC grains and dispersed Al₂O₃ particle clusters. The WC-5 vol.% Fe₃Al composite combines an excellent Vickers hardness of 25.6 GPa with very high Young’s modulus of 693 GPa, a fracture toughness of 7.6 MPa m^1/2 and flexural strength of 1000 MPa. With increasing Fe₃Al binder content, the hardness and stiffness decreased linearly to 19.9 and 539 GPa, respectively with increasing binder content up to 20 vol.%, while the fracture toughness and flexural strength were hardly influenced by the binder content. Compared to WC–Co cemented carbides processed under exactly the same conditions, the WC–Fe₃Al composites exhibit a substantially higher hardness and Young’s modulus.     

The stress anomaly in FeAl–Fe3Al alloys

The anomalous stress peak observed near 500–600 °C in Fe–Al alloys has now been convincingly explained using a model of hardening by immobile thermal vacancies on the lower temperature side of the peak and the loss of hardening as these vacancies become mobile at higher temperatures. The large numbers of vacancies required for such hardening are associated with compositions close to stoichiometry, i.e. 40–50%Al, raising the question of whether such a vacancy hardening model can be adopted for Fe₃Al alloys, which show a similar stress peak anomaly. Examination of data on vacancy formation over the entire range of composition, Fe–Fe₃Al–FeAl, shows that, indeed, a vacancy hardening model appears capable of explaining the stress anomaly for both FeAl and Fe₃Al.     

Processing of Fe3Al and FeAl alloys by reaction synthesis

The effects of powder particle size, alloy composition, and reaction atmosphere on reaction synthesis of binary Fe---Al alloys were studied. Reactions were observed in an open (air) furnace, under static vacuum (in an evacuated quartz tube) and in a dynamic vacuum furnace. Reactions occurring in the open furnace and in the evacuated quartz tube were recorded using high-speed video equipment. High-speed videotapes of reaction synthesis of compacts formed from 45 μm Fe and 10 μm Al particles reacted in air and under static vacuum revealed that an unusual ‘two-stage’ reaction exists in this system under these conditions. Compacts formed from 9 μm Fe and 3 μm Al powder particles do not exhibit a two-stage reaction under any of the conditions examined in this work. The first stage of the two-stage reaction lasts several seconds and starts at round 650 °C. The second stage begins at about 900 °C, reaching temperatures between 1250 and 1350 °C. The progress of the reaction to the second stage is sensitive to the alloy composition and reaction atmosphere. The reaction behavior is explained in terms of thermodynamics and heat transfer, which control the delicate balance between heat accumulation and heat loss during reaction synthesis.     

Effect of Al concentration on pseudoelasticity in Fe3Al single crystals

Pseudoelasticity in Fe₃Al single crystals with different Al contents was investigated focusing on the dislocation configuration and the ordered domain structure. Giant pseudoelasticity only appeared in the D0₃-ordered Fe₃Al single crystals, while the B2-ordered crystals and those with the disordered phase exhibited small strain recovery. The amount of shape recovery in the D0₃-ordered crystals showed a maximum near 23.0at.%Al and decreased with increasing deviation from this Al concentration. In the D0₃ phase at 22.0–25.0at.%Al, 1/4[1 1 1] superpartial dislocations moved individually dragging the nearest-neighbour antiphase boundaries (NNAPB), while couplets of the superpartials were observed to bow out, dragging the next-nearest-neighbour antiphase boundaries (NNNAPB) in Fe–28.0at.%Al. In Fe–22.0–25.0at.%Al single crystals, the NNAPB pulled back the superpartials to decrease its energy during unloading, resulting in the giant pseudoelasticity. In contrast, the surface tension of the NNNAPB was lower than that of the NNAPB, leading to the small strain recovery in Fe–28.0at.%Al.     

Electrochemical behavior of microbiologically influenced corrosion on Fe3Al in marine environment

In this article, microbiologically influenced corrosion behavior of Fe₃Al intermetallic compound in microorganism culture medium has been investigated by using weight loss methods, electrochemical techniques, and electron microscopy. Polarization curves showed that a sharp electrical current peak caused by surface pitting could be observed after Fe₃Al electrodes were immersed in culture medium for 15 days when the polarization potential was about -790 mV vs SCE. Based on the electrochemical impedance spectroscopy (EIS) and the equivalent circuit parameters of the associated system, the corrosion products were found to exhibit a two-layer structured feature and the microorganisms could induce pitting and erosion corrosion of the inner layer. In addition, the passivating film of the inner layer was absolutely destroyed by microbial metabolic products.