正电子湮没技术研究Zr41Ti14Cu12.5Ni10Be22.5块体非晶合金的结构自由体积

采用X射线衍射(XRD)仪、正电子湮没光谱(PAT)研究Zr41Ti14Cu12.5Ni10Be22.5块体非晶合金的结构特性。结果表明:原始制备的Zr41Ti14Cu12.5Ni10Be22.5块体非晶合金其正电子湮没寿命为176ps(大于正电子在纯铁中点阵空位上湮没的寿命τVFe=165ps)。在过冷液区(T=400℃)等温退火中,正电子湮没寿命随着退火时间的增加而减小。在过冷液区退火,导致Zr41Ti14Cu12.5Ni10Be22.5块体非晶合金的结构更致密。     

Zr41Ti14Cu12.5Ni10Be22.5块体非晶合金结构自由体积周围化学环境的研究

采用X射线衍射(XRD)、正电子湮没技术(PAT)-多普勒展宽谱,研究Zr41Ti14Cu12.5Ni10Be22.5块体非晶合金及其过冷液相区结构自由体积周围的元素分布.结果表明:原始制备的Zr41Ti14Cu12.5Ni10Be22.5块体非晶合金其结构自由体积周围主要富集Zr原子,在过冷液相区(T＝400 ℃)等温退火后,在该合金结构自由体积周围探测到Zr、Ti和Be原子.     

浸渗温度对Wf/Zr非晶复合材料界面及压缩性能的影响

用逆向浸渗工艺制备了直径为0.5mm的钨丝增韧Zr41Ti14Cu12.5Ni10Be22.5块体非晶复合材料。研究了浸渗温度对复合材料界面状态以及压缩性能的影响。当浸渗温度分别为1000、1100和1200K时,复合材料的界面结合分别为机械结合、机械结合与冶金结合共存和反应结合形式。较低的浸渗温度会造成界面结合强度不足,过高的浸渗温度导致钨丝脱熔而形成界面反应产物,二者均对Zr41Ti14Cu12.5Ni10Be22.5块体非晶复合材料的压缩强度和变形行为产生不利影响。在1100K浸渗时、保温30min获得的W/Zr块体非晶复合材料具有2409MPa的最高压缩强度和19.5%的塑性变形能力。     

Al对Ti-Zr-Cu-Ni-Be非晶合金热稳定性和力学性能的影响

利用X射线衍射(XRD)、透射电镜(TEM)、差示扫描量热(DSC)和室温压缩试验等分析手段,通过替代(Ti40Zr20Cu8Ni9Be18Al5)和掺杂[(Ti40Zr25Cu8Ni9Be18)0.95Al0.05)]两种元素添加方法,研究了5%(摩尔分数)Al元素对Ti40Zr25Cu8Ni9Be18非晶合金铸态组织、热稳定性和力学性能的影响。替代和掺杂的Al元素使直径为3mm的非晶合金棒状试样中分别析出了纳米晶和准晶。Al替代Zr使非晶合金薄带试样的过冷液相区从46K升高到50K,而以掺杂方式添加时却使其降低为31K。替代方式添加的Al元素使非晶合金的压缩断裂强度从1924MPa提高到2121MPa,但塑性应变从3.9%降低到了0.2%;而掺杂方式添加的Al元素使非晶合金强度降低为1475MPa,并呈现零塑性。     

Wf／ZrTiCuNiBe非晶合金复合材料的界面特征与性能

用渗流铸造水淬法制备了φ6mm×50mm的W纤维增强的Zr4125Ti13．75Cu12.5Ni10Be22.5非晶合金复合材料。采用扫描电镜（SEM）分析了相同渗流时间，不同渗流温度复合材料的界面反应形貌，并采用Push-out法测定了界面剪切强度，讨论了界面特征、界面剪切强度与宏观压缩断裂行为之间的关系。结果表明：渗流铸造法制备的W纤维增强Zr41.25Ti13．75Cu12.5Ni10Be22.5非晶合金复合材料明显提高了非晶合金的塑性和断裂强度。复合材料界面结合包括界面扩散和界面反应两个过程。界面反应程度加剧时界面剪切强度增大，复合材料的破坏方式由纵向劈裂转变为剪切破坏。     

Zr—Ti—Cu—Ni—Be—Fe大块非晶合金晶化动力学效应

利用非等温差示扫描量热（DSC）分析方法研究了大块Zr41Ti14Cu12.5Ni2Be22.5Fe8非晶合金中的晶化行为,用Kissinger方程计算其经表现激活能,实验表明,在Zr基大块非晶合金中掺下Fe后,其玻璃转变与晶化行为都与加热速率有关,均具有动力学效应,同时,从昌化反应速率常数的角度讨论了非晶形成能力。     

钨丝增强(Zr41.2Ti13.8Cu12.5Ni10Be22.5)100-xNbx非晶复合材料的力学性能

采用XRD、SEM等表征方法研究钨丝增强(Zr41.2Ti13.8Cu12.5Ni10Be22.5)100-xNbx非晶复合材料的力学行为.研究表明,分别加入x=1,3,5,7(atA)的Nb后,制备的复合材料试样基体仍为非晶态:随Nb含量的增加,钨丝增强(Zr41.2Ti13.8Cu12.5Ni10Be22.5)10...     

铜基大块非晶合金的压缩断裂行为

铜基大块非晶合金Cu52.5Ti30Zr11.5Ni6与Cu53.1Ti31.4Zr9.5Ni6（at％）具有高的抗压缩断裂强度（σc,f），分别为2212MPa和2184MPa；断裂伸长率（εc,f）分别为2．1％和2．2％。断口微观形貌分析表明，Cu基大块非晶合金具有3种不同类型的微观形貌，分别与断口的3个断裂扩展区域相对应。由于断裂沿着2个不同方向进行，条带型脉状网络的产生，使得Cu基非晶具有高的抗压缩断裂强度。     

高Cu高强Zr基块体非晶合金的制备与力学性能

利用铜模铸造的方法制备了(Zr41.2Ti13.8Ni10Be22.5)1-x/87.5Cu12.5 x(x=1.6,6,11.2)块体非晶合金及其复相组织,分析了合金的相组成,热稳定性、力学性能及断口形貌.结果表明:随着铜含量的不断增多,尽管过冷液相区(ΔTx)逐渐增大,但非晶形成能力却不断下降.当合金的铜含量提高到18.5%时,非晶合金的压缩断裂强度达到2.2 Gpa,进一步增加铜含量到23.7%,压缩强度出现下降趋势.     

Zr-Ti-Cu-Ni-Be大块非晶合金等温晶化过程相分离研究

利用差示扫描量热法(DSC)和透射电镜(TEM)对Zr41.2Ti13.8Cu12.5Ni10Be22.5(at％)大块非晶合金的等温晶化过程和析出相进行了研究。结果表明，大块非晶合金在等温晶化过程中表现出多阶段相析出行为，并且在不同的晶化阶段，析出相也有所不同。在第1个晶化阶段，析出相主要是体心四方(b.c．t)结构的Zr2Cu相；而在晶化的第2个阶段，晶化相主要为简单六方结构的ZrBe2相。从一定程度上证实了Zr41.2Ti13.8Cu12.5Ni10Be22.5大块非晶合金在发生晶化时会形成富Zr区和富Be区，即有相分离的趋势。XRD测试的结果也证实了非晶合金在发生完全晶化时，主要的晶化产物为Zr2Cu和ZrBe2相。     

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.     

Theoretical Analysis for the Motion and Temperature of Melt Droplets in Spray Degassing Process

The motion of melt droplets in spray degassing process was analyzed theoretically. The height of the treatment tank in spray degassing process could be determined by the results of theoretical calculation of motion of melt droplets. To know whether the melt droplets would solidify during spraying process, the balance temperature of melt droplets was also theoretically analyzed. Then proof experiments for theoretical results about temperature of melt droplets were carried. In comparison, the experimental results were nearly similar to the calculation results.     

Growth Kinetics of Single Inclusion Particle in Molten Melts

On the basis of the single-particle framework, a new theory on inclusion growth in metallurgical melts is developed to study the kinetics of inclusion growth on account of reaction and collision. The studies show that the early growth of inclusion depends on reaction growth and Brawnian motion collision, and where the former is decisive, the late growth depends on turbulence collision and Stokes＇ collision, and where the former is dominant; collision growth is very quick during the smelting process, lessened in the refining process, but nearly negligible in the continuous casting process.     

An Easy Way to Quantify the Adhesion Energy of Nanostructured Cu/X(X=Cr,Ta,Mo,Nb,Zr) Multilayer Films Adherent to Polyimide Substrates

An approach based on film buckling under simple uniaxial tensile testing was utilized in this paper to quantitatively estimate the interfacial energy of the nanostructured multilayer films(NMFs) adherent to flexible substrates. The interfacial energies of polyimide-supported NMFs are determined to be *5.0 J/m2 for Cu/Cr, *4.1 J/m2 for Cu/Ta,*2.8 J/m2 for Cu/Mo, *1.1 J/m2 for Cu/Nb, and *1.2 J/m2 for Cu/Zr NMFs. Furthermore, a linear relationship between the adhesion energy and the interfacial shear strength is clearly demonstrated for the Cu-based NMFs, which is highly indicative of the applicability and reliability of the modified models.     

High-Speed Friction Stir Welding of SiC_p/Al–Mg–Si–Cu Composite

A 17 vol% SiCp/Al–Mg–Si–Cu composite plate with a thickness of 3 mm was successfully friction stir welded(FSWed) at a very high welding speed of 2000 mm/min for the first time. Microstructural observation indicated that the coarsening of the precipitates was greatly inhibited in the heat-affected zone of the FSW joint at high welding speed, due to the significantly reduced peak temperature and duration at high temperature. Therefore, prominent enhancement of the hardness was achieved at the lowest hardness zone of the FSW joint at this high welding speed, which was similar to that of the nugget zone. Furthermore, the ultimate tensile strength of the joint was as high as 369 MPa, which was much higher than that obtained at low welding speed of 100 mm/min(298 MPa). This study provides an effective method to weld aluminum matrix composite with superior quality and high welding efficiency.     

新型的治疗阿尔茨海默氏症药物(1-二甲基磷酰基-2,2,2-三氯)-乙基-1-醇烟酸醋对体外神经细胞的作用

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。     

A STUDY OF TEMPERATURE-DEPENDENT VALENCE BOND STRUCTURE OF TITANIUM

On the basis of energy and shape method for the determination of the valence bond (VB) structures of crystal, the valence bond structure of titanium is redetermined at room temperature and calculated in the whole temperature range of 0-1943K. The outer shell electronic distribution of Ti is e_c~(2.9907) · (s_c~(0.4980) d_c~(2.4927)) ef1.0093 in crystal. The temperature dependences of the VB structures of hcp and bcc phases are the same. The VB structures of hcp and bcc phases monotonically increase or decrease with the increase in temperature, but show discontinuous changes at the phase-transformation temperature 1155K.