等径弯曲通道制备的超细晶铜的疲劳性能

研究了等径弯曲通道(ECAP)变形后的超细晶T3铜在恒应力幅控制条件下的疲劳寿命和循环形变行为.通过扫描电镜观察了疲劳试样表面的滑移带,并利用电子背散射技术观察了疲劳前、后晶粒尺寸的变化.结果表明,超细晶T3铜具有较高的疲劳极限(σ-1=153 Mpa),是粗晶铜疲劳极限的2倍.在低周疲劳域内表现出疲劳软化,而在高周疲劳域内表现比较稳定的疲劳行为,甚至出现疲劳硬化.类似驻留滑移带(PSB)的剪切带与最后一次挤压的剪切面一致,剪切带的形成和晶界滑移是疲劳裂纹形核和疲劳断裂的主要原因.     

退火处理对超细晶Cu-Cr合金组织和性能的影响

对Cu-0．4Cr合金进行ECAP（等通道转角挤压）8道次的挤压，得到晶粒尺寸为500nm的等轴晶组织，然后在电阻炉内进行退火试验，通过对ECAP细晶的铜铬合金在473～873K退火1h，分析合金的组织和性能，研究该合金的硬度和导电性能。研究发现，弥散的Cr可以有效地阻止合金的晶粒长大；723K退火后，Cu-0．4Cr合金的电导率和硬度分别可达80．3％IACS和210．9HV，并有较好的综合性能。     

等通道转角挤压Al-Cu合金的应力和应变疲劳行为比较

通过恒应力和恒塑性应变控制疲劳实验,比较了等通道转角挤压四道次的Al—0．7％Cu(质量分数)合金的疲劳寿命、表面变形形貌、疲劳开裂和疲劳断口．结果表明：样品发生明显的循环软化,致使应变和应力疲劳寿命在高、低应力范围存在差别．在应变控制疲劳样品中,塑性变形既可由剪切带来承担,也可以由剪切带和形变带共同承担,进而疲劳裂纹分别沿剪切带或形变带萌生．而应力控制疲劳的塑性变形只集中在剪切带中,并导致剪切疲劳开裂．疲劳断口上存在典型的疲劳裂纹萌生区、缓慢扩展区、快速扩展区和最后瞬断区．     

等径弯曲通道变形制备高性能Cu-Cr合金的组织性能

用两种方式等径弯曲通道变形(equal-channel angular pressing,简称ECAP)制备了的具有等轴晶组织的超细晶Cu-0.4Cr合金,晶粒尺寸为500nm。研究了不同挤压方式、不同挤压道次合金的组织和性能的变化。探讨了不同退火温度对5～8道次材料导电率和硬度的影响。结果表明,经ECAP挤压后的Cu-0.4Cr合金具有很好的综合性能,拉伸强度可达565MPa;硬度和导电率分别为225 HV和66.4%IACS;723K退火1h后材料的导电率和硬度可达80.3%IACS和210.9HV;软化温度可达723K。     

等通道转角挤压过程中fcc金属的微观结构演化与力学性能

系统总结了面心立方(fcc)金属材料在等通道转角挤压(ECAP)变形后的晶粒细化、微观结构演化规律和力学性能.根据ECAP变形的特点,利用具有特殊取向的Al单晶体和Cu双晶体,经过一道次ECAP挤压发现:材料在ECAP模具对角面附近发生严重塑性变形;除了沿模具对角面切应力的作用外,沿垂直于模具对角面的切应力也起重要作用.此外,通过设计特殊取向的Cu单晶体、Al单晶体和粗晶Cu-3%Si合金经过一道次ECAP挤压,系统研究了层错能、晶粒尺寸和晶体学取向对fcc金属形变孪生所需的孪生应力的影响.对具有不同层错能的Cu-Al合金进行多道次ECAP挤压表明,随着层错能降低,Cu-Al合金的晶粒细化机制逐步从位错分割机制转变为孪生碎化机制,最小晶粒尺寸逐步减小,具有较高或较低层错能材料比中等层错能材料更容易获得均匀的微观组织;Cu-Al合金的拉伸强度和均匀延伸率随着层错能的降低同步提高,即随着层错能的降低,Cu-Al合金的强度-塑性匹配性提高.     

等通道转角挤压处理的镁合金AZ31的低周疲劳行为

研究了一道次等通道转角挤压(ECAP)处理的镁合金AZ31挤压棒材的低周疲劳行为,结果表明:在塑性应变幡为0.5％时,材料表现出显著地循环软化;而在应变幅不大于0.2％时,基本表现为循环稳定或微弱的循环软化.疲劳裂纹主要萌生于细晶区,并沿着细晶区扩展,并导致最终的断裂.     

铬含量对ECAP铜铬合金组织和显微硬度的影响

制备不同质量百分含量铬的铜铬合金试样,对合金试样进行等径角挤压(ECAP)处理。然后采用金相显微镜和硬度测试仪等进行合金微观组织和力学性能的研究。结果表明,铬合金元素在合金中以颗粒状均勺分布,ECAP加工的道次越多,晶粒细化程度越大。其中Cu-7.5wt%Cr和Cu-11.25wt%Cr合金经ECAP加工处理后晶粒细化效果最为明显。同时,经过ECAP后试样各表面的显微硬度值均有不同程度的增加。     

时效时间对Al-4.5Cu-0.6Mg合金力学性能的影响

通过硬度测试和拉伸性能测试,研究了时效时间对热挤压Al-4.5Cu-0.6Mg合金力学性能的影响;利用SEM对Al-4.5Cu-0.6Mg合金拉伸断口形貌进行观察。结果表明:随时效时间的延长,Al-4.5Cu-0.6Mg合金的硬度和强度先增大后减小,断裂伸长率明显降低,其中在180℃时效10 h时,合金表现出良好的综合力学性能;固溶+时效态Al-4.5Cu-0.6Mg合金的断口呈现沿晶和穿晶混合断裂特征。     

ECAP对连铸Cu-Ag合金断口形态及力学性能的影响

采用连续铸造和等径角挤压变形(ECAP)加工集成技术制备Cu-Ag合金,研究其力学性能和相应的拉伸断口形态。研究发现,Cu-Ag合金的强度随着ECAP加工道次和Ag含量的增加而增加,而延伸率却下降。连续铸造和ECAP加工的合金与传统浇铸和ECAP加工的合金相比,缩颈前静态韧性有所提高。同时发现,只有连铸的Cu-Ag合金在断裂前表现出缩颈现象,而经ECAP挤压后试样的断裂变为剪切模式,随着ECAP道次的增加出现不同的剪切断裂角。基于实验结果,讨论了经ECAP挤压后连铸Cu-Ag合金的拉伸断裂机制。     

等通道转角挤压制备超细晶Mg15Al双相合金组织与性能

对高铝双相合金Mg15Al在553K以Bc路线进行了不同道次的等通道挤压(ECAP),获得了超细晶高铝镁合金。通过OM,SEM,TEM分析了ECAP前后合金的微观组织结构及断口形貌,并测试了不同挤压道次后合金的硬度和室温拉伸性能,分析了ECAP细化晶粒机理及其性能改善原因。结果表明,随挤压道次增加,累计形变增强,网状硬脆相β-Mg17Al12破碎,合金晶粒显著细化,但对单相区和两相混合区细化效果不同。在α、β两相共存区内,4道次ECAP后形成100nm～200nm的细晶粒;在α单相区,4道次ECAP后晶粒为1μm以下,且在初晶α-Mg内析出弥散细小的β相,起到细晶强化和弥散强化作用。8道次ECAP后,晶粒略有长大。ECAP使合金的硬度、抗拉强度和延伸率同时得到提高,尤其是4道次ECAP后,硬度提高了32.04%,抗拉强度σb从150MPa提高到269.3MPa,延伸率δ由0.05%提高到7.4%;8道次ECAP后,硬度、抗拉强度略有下降,延伸率略有上升。SEM断口观察显示ECAP使合金拉伸断口形貌由铸态的解理断裂特征转变为延性韧窝断裂特征。     

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.