6061铝合金高温流变行为

利用Gleeble-3500热模拟实验机,对6061铝合金在变形温度为350℃、400℃、430℃、460℃、480℃和500℃,应变速率为0.001s-1、0.01s-1、0.1s-1、1s-1和10s-1条件下进行高温压缩实验,得到的真应力-真应变曲线形态基本符合铝合金的热变形力学特征。采用Arrhenius双曲正弦关系描述6061铝合金的高温流变行为,确定其激活能Q=163.4366kJ·mol-1;基于动态材料模型理论绘制6061铝合金热加工图,确定其最佳热加工区域温度为T=420℃~450℃。     

汽车用5182铝合金板材的温拉伸流变行为

在变形温度为323～573 K、应变速率为0.001～0.1/s条件下,采用Instron-8032电子拉伸实验机对汽车用5182铝合金板的流变行为进行研究,采用修正后的Fields-Backofen方程描述5182铝合金温拉伸时的流变行为,建立5182铝合金在温拉伸时的应力-应变本构模型.结果表明:在同一应变速率下,合金的流变应力随温度升高而降低;对于较高温度(448、523和573 K)、较低应变速率(ε=0.001/s),合金的流变应力出现明显的峰值应力,表现出动态再结晶特征;随着应变速率增加,合金的流变应力呈现稳态,表现出动态回复特征.     

6061铝合金低温快速流变行为的研究

采用圆柱体试样，在Gleeble-1500型动态热模拟试验机上进行低温快速压缩试验，研究了6061铝合金低温下快速变形的流变行为，并分析了其变形组织。结果表明，6061铝合金的流变应力随变形温度升高而降低，随应变速率提高而增大；在高应变速率下，发生了不连续动态再结晶；温升强烈地受变形程度的影响；低温快速变形可获得晶粒细小的组织。     

7075铝合金高温流变行为的研究

采用圆柱试样在Gleeble-1500热模拟机上进行高温压缩变形实验，研究了7075铝合金在高温塑性变形过程中流变应力的变化规律。实验在温度为250－500℃、应变速率为0．05－50s^-1的条件下进行。结果表明：应变速率和变形温度的变化强烈影响着合金流变应力的大小，流变应力随变形温度升高而降低，随就变速率提高而增大，可用ZenerHollomon参数的双曲正弦形式来描述7075铝合金高温压缩变形时的流变应力行为。     

4032铝合金的高温压缩变形行为及本构方程

采用Gleeble-1500热模拟试验机对4032铝合金在变形温度370～490℃、应变速率0.02～5 s-1的条件下的流变应力进行了研究.分析了变形温度和应变速率对4032铝合金高温塑性变形应力的影响,计算出了激活能和应力指数值.建立了4032铝合金的本构方程.     

2E12铝合金的高温塑性变形流变应力行为

通过在Gleeble-l500热模拟试验机上进行等温热压缩试验,研究2E12铝合金在变形温度为300～500℃和应变速率为0.0l～l0 s-1条件下的流变应力行为,计算、推导出用包含Arrhenius项的Zener-Hollomon参数描述2E12合金高温压缩流变行为的表达式,并分析形变热、变形温度和应变速率等参数对流变应力的影响规律。结果表明:应变速率和变形温度对2E12合金的流变应力影响显著,流变应力随着温度的升高而降低,随着应变速率的提高而增大;在ε≥1 s-1时,形变热导致流变应力降低,且幅度随着应变速率的增大而增大,随着变形温度的升高而降低。     

5083铝合金热压缩变形流变应力行为

在Gleeble-1500热模拟机上,当变形温度为300-500℃、应变速率为0.01-10 s^-1、真应变为0-0.8时,采用圆柱体等温热压缩实验研究5083铝合金变形流变应力行为。通过分析流变应力指数函数中系数A、β与应变的关系,建立Zener-Hollomon参数的指数关系本构方程。运用该本构方程对5083铝合金不同应变速率、变形温度及应变条件下的流变应力进行预测,发现流变应力预测值与温升修正值吻合得相当好。     

热压缩7075铝合金流变应力特征

采用Gleeble-1500热模拟高温压缩变形试验,研究了7075铝合金高温塑性变形时的流变应力行为.结果表明,应变速率和变形温度的变化影响合金稳态流变应力的大小,在变形温度为350～500℃、应变速率为0.01～1 s^-1的条件下,随变形温度升高,流变应力降低;而随应变速率提高,流变应力增大;应变速率和流变应力之间满足指数关系,温度和流变应力之间满足Arrhenius关系,可用Zener-Hollomon参数描述7075铝合金高温塑性变形时的流变应力行为.     

热压缩7075铝合金流变应力特征

采用Gleeble-1500热模拟高温压缩变形试验,研究了7075铝合金高温塑性变形时的流变应力行为。结果表明,应变速率和变形温度的变化影响合金稳态流变应力的大小,在变形温度为350～500℃、应变速率为0.01～1s-1的条件下,随变形温度升高,流变应力降低;而随应变速率提高,流变应力增大;应变速率和流变应力之间满足指数关系,温度和流变应力之间满足Arrhenius关系,可用Zener-Hollomon参数描述7075铝合金高温塑性变形时的流变应力行为。     

复杂应变率敏感性铝合金流变行为的表征

以NUMISHEET 2016 BM3中5系铝合金AA5086-H111为研究对象,建立其准静态温拉伸流变应力的本构模型。该材料在室温状态下的流变应力表现为负应变率敏感性; 150℃时,随着应变率增加,由负应变率敏感性变为正应变率敏感性;240℃时为正应变率敏感性。针对传统指数型应变率相关项是一种单调函数,构成的本构模型一般用来描述正应变率敏感性的流变行为,很难表征这种复杂应变率敏感性流变行为的问题,给出了一种新的应变率相关项,并称其值为健壮系数。在不同应变率范围内,健壮系数可以表现出不同的单调性。结果表明,耦合新应变率相关项的本构模型可以较好地表征AA5086-H111在不同温度、不同应变率下的流变行为。     

Solidification behavior of 6061 wrought aluminum alloy during rheo-diecasting process with self-inoculation method

The semisolid slurry of the 6061 wrought aluminum alloy was prepared by the self-inoculation method (SIM). The effects of the isothermal holding parameters on microstructures of rheo-diecastings were investigated, and the solidification behavior of 6061 wrought aluminum alloy during the rheo-diecasting process was analyzed using OM, SEM, EDS and EBSD. The results indicate that the isothermal holding process during slurry preparation has great effect on primary α(Al) particles (α₁), but has little effect on the microstructure of secondary solidification in the process of thin-walled rheo-diecasting. Nucleation is expected to take place in the entire remaining liquid when the remaining liquid fills the die cavity, and the secondary solidification particles (α₂) are formed after the process of stable growth, unstable growth and merging. The solute concentration of remaining liquid is higher than that of the original alloy due to the existence of α₁ particles, hence the contents of Mg and Si in α₂ particles are higher than those in α₁ particles.     

6061铝合金冲击载荷作用下的变形断裂行为

利用常见的落锤冲击试验机和自行设计的夹具装置,研究6061铝合金材料在冲击载荷作用下的变形断裂行为。结果表明:6061铝合金受冲击载荷时的断裂行为与准静态拉伸相比无明显变化,损伤形式仍是由晶界处的微孔洞连接形成微裂纹,宏观上仍产生明显颈缩,试样的断裂面与拉伸轴方向大约成45°角。摆锤高度不同,试样表面的变形带不同,摆锤高度为141°时,出现了"白色变形带"。微观断口是由韧窝组成,冲击速度越大,韧窝越小。     

2A12硬铝合金热拉伸流变行为及本构建模

在变形温度350~500℃、应变速率0.01~1 s~(-1)条件下,利用Gleeble-3500热模拟实验机对2A12硬铝合金板进行热拉伸实验。结果表明:峰值应力随温度升高而减小,随应变速率提高而增大;随着应变速率减小,断裂总伸长率升高,而均匀伸长率降低;应变速率较低时,其断裂总伸长率在350~450℃时较高,升高到500℃时迅速降低,均匀伸长率则对温度变化不敏感;应变速率较高时,试样断裂总伸长率对温度变化不敏感,均匀伸长率随温度升高而降低。根据实验结果,采用Z参数建立的流变应力本构模型,能较好地描述2A12铝合金板材热拉伸变形下的流变行为。     

Corrosive wear behavior of 2014 and 6061 aluminum alloy composites

Alloys of 2014 and 6061 aluminum reinforced with 0.1 volume fraction of alumina particles (VFAP) were subjected to impact scratching during a corrosive wear process. The transient currents generated due to the impact were measured in the two composites as well as in their respective monoliths. The effect of solutionizing time on the transient currents was correlated to the near surface microstructures, scratch morphology, concentration of quenched-in vacancies, and changes in grain sizes. It was observed that the transient current values increase with an increase in solutionizing time, indicating that the corrosive wear behavior is not strongly affected by the grain boundaries. However, a combination of pitting and the galvanic corrosion may account for the typical corrosive wear behavior exhibited by the alloys and the composites of this study.     

固溶工艺对6061铝合金组织和拉伸性能的影响

采用光学显微镜、扫描电镜和拉伸试验等方法,研究了固溶处理工艺对6061铝合金微观组织和力学性能的影响。结果表明,随固溶时间的延长和固溶温度的升高,合金中可溶第二相粒子逐渐溶解,再结晶增强,晶粒细化,合金拉伸性能升高;进一步延长固溶时间和提高固溶温度,合金晶粒粗化,合金强度下降。热处理后残留粗大第二相粒子的多少和合金晶粒大小是影响合金拉伸性能和断口形貌的主要因素。时效工艺为180 ℃×8 h条件下,6061铝合金的最佳固溶工艺为535 ℃×80 min。     

Deformation characteristics during Y-shaped tube hydroforming of 6061 aluminum alloy

To manufacture lightweight tube components for aerospace oil circuit systems, an experiment was run to investigate the deformation characteristics on Y-shaped tube hydroforming of 6061 aluminum alloy. Both strain state and metallurgical structure indicate that there are four kinds of prevailing defects during Y-shaped tube hydroforming: bursting, lack of cylindricity, wrinkling, and thinning due to the poor plastic property of 6061 aluminum alloy. The danger of bursting prevails at the early stage of the operation as a result of excessively high internal pressure. In contrast, wrinkling prevails after the middle stage of the operation as a result of excessively axial feeding and cannot be eliminated during subsequent deformation. Lack of cylindricity is mainly because of insufficient axial feeding and internal pressure but can be eliminated by increasing internal pressure. Elongation and compression deformations are originated on protrusion and main pipe of Y-shape tube respectively all the way through the bulging process. Consequently, minimum and maximum thicknesses are at the top of protrusion and the bottom of Y-shape tube respectively, which induces a V-shape borderline of thickness distribution. According to the excessive plastic deformation, microstructure evolution is originated. Crystal grain of protrusion is elongated and its grain size is about 150 μm. In contrast, crystal grain of the middle zone of main tube is refined greatly, which grain size is 50 μm, decreased by 75%. These are useful to improve the component.     

铝合金双轴肩搅拌摩擦焊过程材料流动行为

由于下轴肩的引入,双轴肩搅拌摩擦焊(BT-FSW)过程中的材料流动行为较常规搅拌摩擦焊更为剧烈和复杂,显著影响接头力学性能.以2219铝合金为研究对象,基于耦合欧拉-拉格朗日方法建立了BT-FSW过程三维热力耦合模型,并利用示踪粒子技术分析了焊接过程中材料的流动行为.结果表明,BT-FSW过程中的材料流动存在不同时性,...     

6061铝合金淬火冷却过程中的表面换热系数

通过6061铝合金末端淬火测得的冷却曲线,结合有限差分法和反传热求解法,研究了6061合金固溶处理在不同冷却方式下的冷速及表面换热系数与温度的变化规律。结果表明,6061铝合金在水雾冷和喷水冷却过程中,端面冷速先增大后减小,在400℃左右达到峰值,峰值冷速约为30℃/s。6061铝合金的表面换热系数与温度呈非线性关系,其大小随着温度的降低先逐渐增大,在150～100℃范围内达最大值,然后下降;在风冷过程中,表面换热系数值先急剧增大,当温度下降到500℃后增速明显减慢。