Fe－Mn－Si－Ni－Co合金中形变应力诱发ε马氏体的稳定化及其对记忆效应的影响

Ｆｅ－２５．６Ｍｎ－５．１Ｓｉ－４．１Ｎｉ－１．８Ｃｏ（ｗｔ％）合金在一８０℃变形时，可逆应变量ε＿ｒ随预应变量ε＿ｔ增大而迅速增大；当ε＿ｔ＞２．５％，增大速度减慢；当４．２％＜ε＿ｔ＜１０．８％，ε＿ｒ基本保持恒定值。逆相变温度Ａ＿ｆ随ε＿ｔ增大而连续升高，但Ａ＿ｓ不随ε＿ｔ变化。应力诱发ε马氏体及其逆相变后的残留显微组织分析表明，应力诱发ε马氏体片在形成过程中因相互交叉产生塑性变形，引起稳定化，是引起多晶Ｆｅ－Ｍｎ－Ｓｉ系合金可逆应变量低的一个重要原因。文中还讨论了应力诱发ε马氏体稳定化的特点及可能的改善途径。     

预应变对铝基体中复合的TiNi合金丝马氏体逆相变的影响

采用示差扫描热分析(DSC)、X射线衍射(XRD)和扫描电子显微分析(SEM)等方法,研究了预应变对铝基体中复合的TiNi形状记忆合金丝的马氏体逆相变的影响.结果表明,预应变的TiNi丝发生两种逆相变,一种是热致马氏体(TIM)的逆相变,另一种是应力诱发马氏体(SIM)的逆相变.预应变样品的TIM逆相变的起始温度与未预应变样品的基本相同.SIM逆相变的起始温度随预应变的增大而升高.TIM和SIM逆相变的分数随预应变的增大而减少.     

NiTi形状记忆合金丝在Al基复合材料的约束态马氏逆相变特征

利用DSC,XRD,SEM等实验手段研究了NiTi记忆合金丝在铝合金丝在铝基体约束状上的马氏体逆相变特征,研究结果表明,预应变NiTi记忆合金丝在加热过程中发生两种马氏体逆相变,热致马氏体转变（M^T→P) 应力诱发马氏体逆转变（M^d→P）,其中热致马氏体相变温度与未预应变样品基本相同,且不受参应变影响,而应力诱发马氏体向母相转变温度随预应变增加而升高,随预应变增加,热致马体与应力诱发马氏体的转变时减少,文中引入马氏体变形度概念,并对马氏体在逆转变过程中的变形度变化进行了讨论。     

陶瓷薄膜与金属间的浸润性及其界面的研究

本文在对 ＴｉＮ、ＴｉＣ陶瓷薄膜与金属 Ａｇ、 Ｃｕ、 Ｎｉ、 Ｆｅ间的浸润性测量的基础上，用扫描电子显微镜（ＳＥＭ）、电子探针（ＥＰＭＡ）对其界面进行了观察。结果表明：浸润性较差的Ａｇ、Ｃｕ与ＴｉＮ、ＴｉＣ的界面平整，几乎没有发生相互扩散和化学反应；而浸润性较好的 Ｆｅ、Ｎｉ与 ＴｉＮ、ＴｉＣ的界面有明显的扩散和化学反应现象沿着ＴｉＮ、ＴｉＣ的晶界扩散；薄膜部分甚至全部溶入金属中。ＴｉＣ薄膜与Ｆｅ的界面反应程度大于ＴｉＮ 薄膜。     

多孔陶瓷薄膜表面形貌研究

用原子力显微镜（ＡＦＭ）观察Ａｌ２Ｏ３、Ａｌ２Ｏ３－ＳｉＯ２及Ａｌ２Ｏ３－ＳｉＯ２－ＴｉＯ２复合陶瓷薄膜的表面形貌,Ｘ射线衍射（ＸＲＤ）分析表明,Ａｌ２Ｏ３薄膜的上为γ－Ａｌ２Ｏ３;Ａｌ２Ｏ３－ＳｉＯ２薄由γ－Ａｌ２Ｏ３和非晶诚ＳｉＯ２组成;而Ａｌ２Ｏ３－ＳｉＯ２－ＴｉＯ２薄膜的相成分为Ａｌ２Ｏ３、ＴｉＯ２、Ａｌ４Ｔｉ２ＳｉＯ１２和非晶态ＳｉＯ２,各相的含量随化学成分变化而变化,ＡＦＭ观察结果表明     

Fe—17Mn—10Cr—5Si—4Ni合金低温应力诱发相变特点及其形状记？…

用Ｘ射线衍射分析、显微组织观察等研究了Ｆｅ－１７Ｍｎ－１０Ｃｒ－５Ｓｉ－４Ｎｉ合金在低温（低于室温）下应力诱发相变的特点及其形状记忆效应。合金在室温拉伸变形时,当应变量超过５％由于应力诱发ε马氏体的相变作用而形成的α′马氏体;当变形温度低于室温时应力优先诱发γ－α′马氏体转变。正是这种应力诱发相应特征的转变使合金的形状记忆效应在室温以下出现奇特低谷。     

工艺参数对AgInSbTe薄膜性能的影响

采用射频磁控溅射工艺,在 Ｋｇ玻璃基片上用 Ａｇ－Ｉｎ－Ｓｂ－Ｔｅ合金靶制备了 Ａｇ_δＩｎ＿（１４）Ｓｂ＿（５５）Ｔｅ＿（２３） 相变薄膜,将沉积态薄膜在３００℃进行了热处理．测量了薄膜的光学性质和静态存储性能,研究了 溅射气压和功率对薄膜光学性质和静态存储性能的影响．结果表明,适当的溅射气压和溅射功率可使 Ａｇ_δＩｎ＿（１４）Ｓｂ＿（５５）Ｔｅ＿（２３）相变薄膜具有较大的反射率对比度,从而提高其存储性能．     

用Sol─Gel法制备PZT铁电陶瓷及薄膜

用Ｓｏｌ－Ｇｅｌ法制备了Ｐｂ（Ｚｒ＿（０．５）Ｔｉ＿（０．５））Ｏ＿３（ＰＺＴ）铁电陶瓷与薄膜，观察了它们的结晶情况并测定了它们的电学性能。利用Ｓｏｌ－Ｇｅｌ法，可降低ＰＺＴ陶瓷粉料的预烧温度约２００℃，所得陶瓷致密，晶粒均匀；具有较好的介电性能。ＰＺＴ陶瓷显示弥散相变特征。ＰＺＴ薄膜的晶化受基底影响很大。基底晶格越完整，与ＰＺＴ薄膜的晶格失配率越小，ＰＺＴ薄膜的晶化就越好。采用ＰｂＴｉＯ＿３过渡层促进ＰＺＴ薄膜在镀铂硅片上晶化。ＰｂＴｉＯ＿３过渡层与ＰＺＴ薄膜构成串联电路。其表现电学性能与相应的ＰＺＴ体材料相近。     

爆炸合成NiTi／NiTi合金的相变行为

采用爆炸焊将两块原子百分比不同的NiTi合金制成大块成分不均匀的NiTi／NiTi复合板，并在此基础上对其相变行为以及相应的回复应变特征进行了研究。结果表明焊后的复合板具有良好的界面结合和可逆马氏体相变；冷变形后NiTi／NiTi合金的逆相变温度及其相变温度范围随预应变量的增大而升高；同时，在较宽的温度范围内得到两步回复应变。     

NiTi形状记忆合金丝在Al基复合材料中的约束态马氏体逆相变特征

利用DSC,XRD,SEM等实验手段研究了NiTi记忆合金丝在铝基体约束状态下的马氏体逆相变特征。研究结果表明,预应变NiTi记忆合金丝在加热过程中发生两种马氏体逆相变：热致马氏体逆转变(MT→P)与应力诱发马氏体逆转变(Md→P),其中热致马氏体逆相变温度与未预应变样品基本相同,且不受预应变影响;而应力诱发马氏体向母相转变温度随预应变增加而升高;随预应变增加,热致马氏体与应力诱发马氏体的逆转变量减少。文中引入马氏体变形度概念,并对马氏体在逆转变过程中的变形度变化进行了讨论。     

Ni含量对激冷贫镍TiNi形状记忆合金薄带相变行为的影

用激冷甩带法制备了Til-xNix(x=45％～49.8％)(原子分数)形状记忆合金(SMA)薄带,用示差扫描量热仪研究了Ni含量对铸态及450℃、500℃退火态TiNi SMA薄带相变行为的影响.结果表明,冷却/加热时,铸态和退火态Ti1-xNix(x=45％～49％)SMA薄带发生A→M/M→A一阶马氏体相变;当Ni含量为49.8％时,铸态和退火态TiNi SMA薄带冷却时发生A→ R→M两阶段相变,加热时发生M→A一阶段相变.随Ni含量增加,TiNi SMA薄带马氏体正、逆相变温度范围先增大后减小,Ni含量为48％时相变温度范围最宽.退火态比铸态TiNi SMA薄带相变温度范围窄.随Ni含量增加,TiNi SMA薄带马氏体正、逆相变温度升高,相变热滞增大.当Ni含量为49％时,SMA薄带的马氏体相变温度达最大值,当Ni含量为49.8％时马氏体相变温度迅速下降.     

Effect of Pre-strain on the Transformation and Recovery Behaviours of a Ti44Ni47Nb9 Shape Memory Alloy

The recovery strain, stress and transformation temperature of different pre-strained specimens of Ti44Ni47Nb9 were investigated by tensile test and electrical resistance measurement. The results indicated that pre-strain increases the reverse martensitic transformation temperature (A ' (s)) and hysteresis (A(s) - M-s). The recovery strain and stress are higher if the specimens are pre-strained between M-s and A(s) temperature than outside this temperature range. There exists an optimal pre-strain value, about 10%, at which the specimen exhibits maximum recovery strain and stress.     

Superelasticity of free‐standing NiTi films depending on the oxygen impurity of the used targets

Off‐stoichiometric NiTi sputter targets were manufactured by ingot metallurgy in order to produce Ni‐rich NiTi thin films. Crystalline samples, which undergo a martensitic transformation, were fabricated by magnetron sputtering and subsequent thermal treatment. The sacrificial layer technique was applied to obtain free‐standing NiTi films. The stoichiometry of the sputtered film is different to the stoichiometry of the target material. Sputtering targets with a Ti content higher than 49.5 at.% have a typical Ti‐loss rate in the order of 4.3 at.%, whereas at more Ni‐rich targets a Ti loss rate of only 0.5–1.5 at.% is observed. Due to this Ti loss rate target composites of Ti‐53.1Ni‐46.9 at.% and Ti‐53.2Ni‐46.8 at.% were taken. The NiTi films obtained from these two targets were compared. The main difference between the two targets is the impurity content of oxygen and carbon. Auger electron spectroscopy measurements were performed to determine qualitatively the content of oxygen in the free‐standing NiTi films. Transformation temperatures and hysteresis properties of the martensitic transformation were characterised by differential scanning calorimetry. Free‐standing films obtained from the Ti‐53.1Ni‐46.9 at.% and Ti‐53.2Ni‐46.8 at.% sputtering targets revealed superelastic properties at 45 °C as demonstrated by tensile testing. Tensile tests were taken at various temperatures of 40 °C, 45 °C, 50 °C, 55 °C and 60 °C, revealing e.g. a maximum superelastic strain of approximately 5 % at 45 °C.     

Characteristics of Deformation and Recovery in Shape Memory Alloy

The mechanical behavior and the effect of pre-strain on recovery behavior of Ti50Ni47Fe3 (at. pct) alloy were investigated systematically by tensile and recovered tests accompanied by electrical resistance measurement. Ti50Ni47Fe3 alloy has different deformation behaviors at different temperature ranges, the deformation curves in different temperature range can be classified into four kinds. The start temperature of recovery increases with the increase of pre-strain. There exists an optimal deformation condition, at which the specimen exhibits maximum free recovery strain. With increasing pre-strain the recovery stress increases and reaches the maximum at 8% pre-strain. R-phase to parent transition offered about 0.2% recovery strain. With pre-strain increasing the recovery stress increases and reaches to the maximum at 8% pre-strain. The recovery stress is corresponding with the critical stress of stress-induced martensitic transformation.     

Characteristics of Deformation and Recovery in Ti50Ni47Fe3 Shape Memory Alloy

The mechanical behavior and the effect of pre-strain on recovery behavior of Ti50Ni47Fe3 (at. pct) alloy were investigated systematically by tensile and recovered tests accompanied by electrical resistance measurement. Ti50Ni47Fe2 alloy has different deformation behaviors at different temperature ranges, the deformation curves in different temperature range can be classified into four kinds. The start temperature of recovery increases with the increase of pre-strain.There exists an optimal deformation condition, at which the specimen exhibits maximum free recovery strain. With increasing pre-strain the recovery stress increases and reaches the maximum at 8% pre-strain. R-phase to parent transition offered about 0.2% recovery strain. With pre-strain increasing the recovery stress increases and reaches to the maximum at 8% pre-strain. The recovery stress is corresponding with the critical stress of stress-induced martensitic transformation.     

Effects of Ta Addition on NiTi Shape Memory Alloys

1. IntroductionSince NiTi shape memory alloy have excellentshape memory effect, good mechanical properties, excellent biocompatibility and high corrosion resistance,they have been used for various applications, espysctally in the biomedical fi.ldll~4]. However, the lowX-ray visibility of NiTi shape memory alloys has limited some medical applicatinns. With low X-ray visibility, the detection of the very small implacable devices or tools which are made of NiTi alloys can bevery difficult. So…     

Microstructure and martensitic transformation of Ti49Ni51 − xHfx high temperature shape memory alloys

In present work, the microstructure and martensitic transformation of Ti₄₉Ni_51 − xHf_x (x = 3-15) alloys were studied. The microstructure of Ti₄₉Ni_51 − xHf_x alloys consists of B19′ martensite and (Ti,Hf)₂Ni phase at room temperature. The martensitic transformation behavior is characterized by a single-stage transformation. With increasing Hf content, the transformation temperature increases from 75 to 279 °C resulting from the reduced valence electron concentration, indicating that the replacement of Hf for Ni is effective in increasing the transformation temperatures. The results suggest that the Ti₄₉Ni_51 − xHf_x shape memory alloy is one of potential candidates for high temperature applications.     

Shape memory characteristics and superelasticity of Ti-Ni-Cu alloy ribbons with nano Ti2Ni particles

Microstructures and deformation behaviour of Ti-45Ni-5Cu and Ti-46Ni-5Cu alloy ribbons prepared by melt spinning were investigated by transmission electron microscopy, thermal cycling tests under constant load and tensile tests. Spherical Ti2Ni particles coherent with the B2 parent phase were observed in the alloy ribbons when the melt spinning temperature was higher than 1773 K. Average size of Ti2Ni particles in the ribbons obtained at 1873 K was 8 nm, which was smaller than that (10 nm) in the ribbons obtained at 1773 K. Volume fraction of Ti2Ni phase in the ribbons obtained at 1873 K was 40%, which was larger than that (20%) in the ribbons obtained at 1773 K. The stress required at temperatures of Af + 10 K for the stress-induced martensitic transformation increased from 93 MPa to 229 MPa and apparent elastic modulus of the B2 parent phase increased from 56 GPa to 250 GPa with increasing the melt spinning temperature from 1673 K to 1873 K in Ti-45Ni-5Cu alloy ribbons. The critical stress for slip deformation of the ribbons increased by coherent Ti2Ni particles, and thus residual elongation did not occur even at 160 MPa, while considerable plastic deformation occurred at 60 MPa in the ribbons without Ti2Ni particles. Almost perfect superelastic recovery was found in the ribbons with coherent Ti2Ni particles, while only partial superelastic recovery was observed in the ribbons without coherent Ti2Ni particles.     

Crystallization kinetics and martensitic transformation of Ti49Ni46.5Ce4.5 alloy thin film

The Ti₄₉Ni_46.5Ce_4.5 alloy thin film was prepared by direct current (DC) magnetron sputtering system for the first time. Crystallization kinetics, phase composition and the behaviors of martensitic transformation were studied. The results by X-ray diffraction (XRD) and differential scanning calorimeter (DSC) demonstrated that the primary second phase of TiNiCe alloy thin films was Ce₂Ni₇ phase, apparent activation energy was determined to be 510 kJ/mol at the continuous heating process, Avrami exponents for different isothermal temperature were in the range of 1.1-1.88 between 713 and 730 K, one-step martensitic transformation was observed in the crystallized Ti₄₉Ni_46.5Ce_4.5 alloy thin films. The influence of thermal process on martensitic transformation temperature was investigated with non-isothermal and isothermal crystallization. The reason behind the transformation temperature change was also discussed.     

TiNi合金在恒应力约束下的不完全相变

利用DSC对预应变TiNi形状记忆合金丝在恒应力约束下的马氏体不完全逆相变进行了研究,发现不完全相变热循环样品在第二次自由态加热过程中出现两步马氏体逆转变和两段应变回复现象.分析认为:经过恒应力约束下的不完全逆相变后,TiNi样品中存在不同的马氏体,在随后的加热过程中先后逆转变,产生两段回复应变.