Fe对Ni-Mn-Ga合金微丝形状记忆效应的影响

以Ni-Mn-Ga合金微丝为基础分析Fe元素掺杂前后对合金微丝的形状记忆效应的变化。用真空磁控钨极电弧熔炼炉制备Ni-Mn-Ga-Fe合金,并用高真空精密熔体抽拉设备将母合金制备成微丝。采用EDS能谱分析仪、DSC差示扫描量热分析仪、XRD、DMA动态机械分析仪,研究Fe元素掺杂Ni-Mn-Ga合金微丝后的物相、马氏体相变行为、微丝的形状记忆效应。结果表明,Ni-Mn-Ga-Fe合金微丝显示的是四方结构马氏体相和面心立方结构奥氏体相的混合相,对微丝采用步进式阶梯有序化热处理,有序化热处理能有效降低微丝内部缺陷,释放内应力,细化微丝内部晶粒,收缩晶格体积,马氏体孪晶界面更加平直,孪晶面更易移动,微丝的伸长率提高。在258 K下对制备态Ni-Mn-Ga-Fe合金微丝进行单程形状记忆的测试,拉伸到350 MPa后卸载到0 MPa,随后将微丝升温到奥氏体态后,应变恢复率为78.75%,而在289K对有序化热处理态Ni-Mn-Ga-Fe合金微丝进行单程形状记忆测试,应变恢复率达到100%。在126 MPa和240 MPa下分别对有序化热处理态三元Ni-Mn-Ga合金微丝和Ni-Mn-Ga-Fe合金微丝进行恒应力拉伸,两种微丝双程形状恢复能力均接近100%,但Ni-Mn-Ga-Fe合金微丝在发生形变时的弹性应变储能略高于Ni-Mn-Ga合金微丝。Fe的加入使得到的合金微丝的力学性能高于传统三元形状记忆合金微丝;制备态下和热处理态的Ni-Mn-Ga-Fe合金微丝的马氏体相变温度较Ni-Mn-Ga合金微丝分别提高6.0 K和11.5 K,热滞分别降低6.7 K和1.5 K。

Ni-Mn基多晶铁磁形状记忆合金的韧化

固态制冷技术由于具有环保、高效、节能的特点,因而有望取代传统的气体压缩式制冷技术。在各种有竞争力的制冷剂中,Ni-Mn基铁磁形状记忆合金由于具有磁热效应、弹热效应、压热效应、磁阻、磁致应变等多功能特性而受到了人们的广泛关注。近年来,材料工程师及科学家们对Ni-Mn基磁形状记忆合金的热效应开展了一列深入的研究并取得了众多研究成果,但Ni-Mn基合金韧性较低,导致性能衰减快、循环稳定性差,限制了Ni-Mn基合金的应用。综述了传统的过渡族元素、稀土元素和类金属元素掺杂引起的固溶强化、第二相强化、细晶强化和晶界净化与修饰对Ni-Mn基合金韧性的影响规律,比较了不同方法在Ni-Mn基合金韧性增强方面的优缺点,归纳了近年来受到重视的尺寸效应和全d轨道杂化等强韧化机理,分析了轨道杂化途径存在的主要问题,展望了Ni-Mn基合金的研究和发展方向,对促进Ni-Mn基合金在功能器件等领域的应用具有重要的意义。

Al-Cr-Fe-Mn-Ni高熵合金中的L2_(1)相的相稳定性及其性能研究

为开发兼具良好强度与塑性的BCC基高熵合金,可引入与基体共格的B2或L2_(1)相。L2_(1)相具有更好的抗蠕变性能,有望在高温环境中得到应用。但是,目前对BCC型高熵合金中L2_(1)相的存在规律、相稳定性及其对合金性能的影响还缺乏深入的研究。为此,本工作研究了电弧熔炼制备的铸态Al_(0.5)Cr_(2.5-x)FeMn_(x)Ni(x=0.5~1.75)、Al_(0.75)Cr_(2.25-y)FeMn_(y)Ni(y=0.25~1.5)、AlCr_(2-z)FeMn_(z)Ni(z=0.5~1.5)高熵合金的相组成,及800℃或1000℃真空退火120 h对合金组织和相组成的影响。研究表明,这些合金中L2_(1)相的成分特征由40%~50%(原子分数)Ni和15%~20%(原子分数)Al、Mn组成。L2_(1)相只存在于Al含量为10%~15%(原子分数)的合金中,且多以BCC+L2_(1)两相共存,获得的组织为编织网状的调幅分解组织。当Al含量达到20%(原子分数)后,合金则由BCC+B2两相构成。L2_(1)相的存在会使BCC型XRD特征峰出现明显的峰分裂。经过800℃或1000℃退火后,合金中L2_(1)相仍能稳定存在,合金显微组织发生粗化并会形成σ或FCC相。铸态合金的硬度随Mn含量的增加而降低,含L2_(1)相的合金的硬度在463HV~558HV范围内。800℃退火会使含5%~15%(原子分数)Mn的合金硬度降低70HV~100HV,但由于硬质σ相的析出,含20%~30%(原子分数)Mn的合金硬度提高200HV以上;1000℃退火后,由于软质FCC相的形成,合金的硬度略有降低,这些结果将为BCC型高熵合金的设计奠定基础。

Ni-Mn基磁性形状记忆合金弹热制冷效应的研究现状

弹热制冷不仅具有大而可逆的温度变化,而且其驱动方式更为简单,同时兼具环保、高效、节能的特点,平衡了成本、制冷量、效率以及可行性,有望成为替代传统蒸汽压缩冷却技术的候选之一。本文综述了Ni-Mn基磁性形状记忆合金弹性热效应的研究进展,从掺杂合金元素、热处理方法以及制备工艺等多个方面,总结了近年来对Ni-Mn基合金弹性热效应进行改进优化的研究成果。然而,目前Ni-Mn基合金弹热制冷材料的研究仍处于探索阶段,实现其实际应用还需进一步深入研究。未来的研究重点应集中在降低驱动能耗、提升疲劳寿命和循环稳定性、提高绝热温变以及优化传热效率等方面。

First-principles calculations of Ni–(Co)–Mn–Cu–Ti all-d-metal Heusler alloy on martensitic transformation,mechanical and magnetic properties

The martensitic transformation,mechanical,and magnetic properties of the Ni_(2)Mn_(1.5-x)Cu_(x)Ti_(0.5) (x=0.125,0.25,0.375,0.5) and Ni_(2-y)Co_(y)Mn_(1.5-x)Cu_(x)Ti_(0.5)[(x=0.125,y=0.125,0.25,0.375,0.5) and (x=0.125,0.25,0.375,y=0.625)]alloys were systematically studied by the first-principles calculations.For the formation energy,the martensite is smaller than the austenite,the Ni–(Co)–Mn–Cu–Ti alloys studied in this work can undergo martensitic transformation.The austenite and non-modulated (NM) martensite always present antiferromagnetic state in the Ni_(2)Mn_(1.5-x)Cu_(x)Ti_(0.5) and Ni_(2-y)Co_(y)Mn_(1.5-x)Cu_(x)Ti_(0.5) (y<0.625) alloys.When y=0.625 in the Ni_(2-y)Co_(y)Mn_(1.5-x)Cu_(x)Ti_(0.5) series,the austenite presents ferromagnetic state while the NM martensite shows antiferromagnetic state.Cu doping can decrease the thermal hysteresis and anisotropy of the Ni–(Co)–Mn–Ti alloy.Increasing Mn and decreasing Ti content can improve the shear resistance and normal stress resistance,but reduce the toughness in the Ni–Mn–Cu–Ti alloy.And the ductility of the Co–Cu co-doping alloy is inferior to that of the Ni–Mn–Cu–Ti and Ni–Co–Mn–Ti alloys.The electronic density of states was studied to reveal the essence of the mechanical and magnetic properties.

THERMODYNAMICS OF MARTENSITIC TRANSFORMATION IN Fe-Mn-C AND Fe-Ni-C ALLOYS

A Central Atom Model is introduced and the LFG and Hsu models are modified in order to evaluate the driving force for the martensitic transformation in Fe-Mn-C and Fe-Ni-C al- loys.The results show that the relationship between the driving force and the yield strength of austenite at Ms temperature,σ_(0.2)~γ/M_s,fits Hsu's formula;ΔG~=2.1σ_(0.2)~γ/M_s+907 J/mol.The M_s temperatures of Fe-Mn-C and Fe-Ni-C alloys are also calculated.The calculated results are in good agreement with experimental values.

Martensitic Transformation and Magnetic-Field-Induced Strain in Ni-Mn-Ga-RE (RE=Tb, Sm) Alloys

The effects of microamount additions of RE (Tb, Sm) on martensitic transition, the magnetic-field-induced strain and the bending strength of highly textured polycrystalline Ni_(48)Mn_(33)Ga_(19) alloy were investigated. The experimental results show that the addition of RE elements decreases the martensitic transformation temperature and the Curie temperature. But the bending strength of Ni-Mn-Ga-RE (RE=Tb, Sm) alloys increases remarkably because of the grain refinement. As a result, Ni-Mn-Ga-RE alloys will be applied practically with higher reliability and stability due to favorable plasticity and toughness. In addition, the replacement of small amounts Ga by Tb or Sm decreases the magnetic-field-induced strain of the alloys at room temperature.

Factors Affecting Transformation Temperatures in Fe-Mn-Si-Cr-Ni Shape Memory Alloy

The effects of prestrain and annealing temperature on phase transformation temperatures in Fel4Mn5Si8Cr4Ni shape memory alloy have been studied. The results showed that when the annealing temperature was 673 K, both the At and the Ms temperatures increased appreciably as the prestrain increased, the As temperature increased slightly with increasing prestrain; the resistivity difference at 303 K between the heating and cooling curve also increased with increasing prestrain, which agreed with the recovery strain. The shape memory effect in Fe-Mn-Si-Cr-Ni shape memory alloy is caused by the stress-induced γ→ε martensite transformation and its reverse transformation. When the prestrain was 10%, the Ms temperature decreased remarkably as the annealing temperature increased.

Effects of Sm on Phase Transformation in Ni-Mn-Ga Alloys

The effects of small amount additions of Sm on the martensitic transition and magnetic phase transition of polycrystalline Ni-Mn-Ga alloys were investigated. The experimental results show that the Sm doped alloys also undergo a thermal-elastic martensitic transformation and reverse transformation during cooling and heating process and the addition of Sm decreases the martensitic transformation temperature and Curie temperature in different degree respectively. Ni-Mn-Ga alloys of adding Sm still possess Heusler structure, but their crystal lattice parameters are modified slightly. The addition of a proper amount of Sm does not basically decrease T_c of the alloy when avoiding the appearance of second phase. In addition, the doped alloys have favorable toughness because of grain refinement of Sm.

Shape Memory Effect of As-aged Fe-14Mn-5Si-8Cr-4Ni-0.2C Alloy

The effects of aging temperature on shape memory effect, mechanical properties and microstruc-ture of Fe-14Mn-5Si-8Cr-4Ni-0.2C shape memory alloy have been studied. The results showed that the second phase particles rich in chromium, manganese and silicon precipitate during aging, and thereby increase the hardness and strength of the alloy. The shape recovery ratio can be remarkably improved by aging and a maximum value can be obtained at 1223 K, which is 68% higher than that of the specimen in solid solution state. When the aging temperature is below 1223 K, the amount of second phase particles increases as the aging temperature increases. The size of austenite grain increases with increasing aging temperature. When the temperature is over 1223 K, the second phase particles can not precipitate. The lack of second phase particles and the increase of grain size make the hardness and shape recovery ratio drastically decrease, when the temperature is over 1223 K.

Effect of Alloying Elements on Microstructure,Martensitic Transformation and Mechanical Properties of Ni-Mn Based Alloys

The microstructural features, shape memory behavior and mechanical properties of Ni-Mn based alloys were investigated by differential scanning calorimetry （DSC）, scanning electron microscopy （SEM）, transmission electron microscopy （TEM） and thermal cycling test under various stresses. The transformation temperatures shifted toward lower temperatures when adding a third element into the Ni-Mn system. The addition of 10 at. pct Fe increased considerably the mechanical properties exhibiting still high transformation temperatures. However, it was found that in NiMn40Fe10 alloy the martensitic transformation is not thermoelastic in nature. The mechanism of this transformation and the crystallography of Ni-Mn（50-x）-Fex （x=5, 7, 10, 20 at. pct） alloys are presented.

Changes of Tempering Microstructure and Properties of Fe-Cr-V-Ni-Mn-C Cast Alloys

The changes of tempering microstructure and properties of Fe-Cr-V-Ni-Mn-C cast alloys with martensite matrix and much retained austenite are studied. The results showed that when tempering at 200 °C the amount of retained austenite in the alloys is so much that is nearly to as-cast, and a lot of retained austenite decomposes when tempering at 350°C and the retained austenite decomposes almost until tempering at 560 °C. When tempering at 600 °C, the retained austenite in the alloys all decomposes. At 560°C the hardness is highest due to secondary hardening. The effect of nickel and manganese on the microstructure and properties of Fe-Cr-V-C cast alloy were also studied. The results show that the Fe-Cr-V-C cast alloy added nickel and manganese can obtain martensite matrix and much retained austenite microstructure, and nickel can also prevent pearlite transformation. With the increasing content of nickel and manganese, the hardness of as-cast alloy will decreases gradually, so one can improve the hardness of alloy by tempering process. When the content of nickel and manganese is 1.3-1.7%, the hardness of secondary hardening is the highest (HRC64). But when the content of nickel and manganese increase continually, the hardness of secondary hardening is low slightly, and the tempering temperature of secondary hardening rises.

Crystalline structure and morphology of X phase in Cu Al-Ni-Mn-Ti alloy

The composition, morphology, crystalline structure and formation and evolution of X phase in a Cu 12.3Al 2Ni 2Mn 1Ti alloy were studied. The results show that the X phase is a Ti rich phase with atomic ratio of (Cu+Ni)∶ Ti∶Al=2∶1∶1 and DO 3 or L2 1 structure; it is directly formed in the liquid phase by crystallization in the process of solidification of the alloy; there forms free particle X phase through the progressive dissolution and breakdown of the inter dendritic microstructure in the following homogenization process. The X phase has three different morphologies, i.e. X L, X LS and X S, whose contents in the matrix rely on the heat treatment conditions. [

CRYSTAL STRUCTURE AND PHASE ABUNDANCE OF Zr-Mn-Ni LAVES PHASE HYDROGEN STORAGE ALLOYS

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Temperature Dependent Work-hardening Behaviour in an Fe-Mn-Si-Cr-Ni Shape Memory Alloy

The work-hardening behaviour in an Fe-Mn-Si-Cr-Ni alloy has been investigated using tensile test at different temperatures and TEM observation. It was found that besides the intersection of εmartensite, the intersections of ε martensite with stacking fault and the cross-slip of dislocation which is difficult to occur in the alloy with low stacking fault energy are also important factors to the temperature dependent work-hardening behaviour.

Electron Microscopy Analysis of Deformation Induced ε Martensite Transformation in an Fe-Mn-Si-Cr-Ni Alloy

The configurations of stacking faults and morphologies of strain induced ε martensite plates in an FeMnSiCrNi alloy were investigated through electron microscopy analysis. The Shockley partial dislocation structures. sensitive to external stress. determine the configurations of stacking faults in γphase Partial dislocations at the front sides of stacking faults are usetul for the nucleation of εmartensite plates. The growth of ε martensite plates is accompanied with the disappearance of local pre-existing stacking faults, The ε martensite vanants behave in three morphologies of respective stopping. continuous penetrating and intersections with the formation of secondary ε martensite plates

Effect of Austenite Pre-deformation on Isothermal Martensite Transformation in an Fe-20.5Ni-4.8Mn Alloy

With electron microscopy the investigation on isothermal martensite transformation in an Fe20.5Ni-4.8Mn alloy has been carried out to clarify the effect of austenite state on the transformation, by applying pre-deformation to austenite before isothermal holding. Under the condition without pre-deformation, the isothermal martensite products are lath martensite with {111}fhabit planes. Dislocations in austenite seem to contribute to nucleation of martensite, and in this nascent Stage austenite substructure has no obvious effect on martensite growth. The consequent thickening of martensite laths is apparently influenced by local austenite states, resulting in the changes in orientation, morphology as well as substructure of martensite lath. The kinetics of isothermal martensite transformation is controlled by intedece dislocation determined nucleation of martensite in primary stage, but to a larger extent, by the austenite accommodation for the shape strain of martensite in the thickening Stage

Cavitation Erosion Behavior of as-Welded Cu12Mn8Al3Fe2Ni Alloy

Cavitation erosion behavior of as-welded Cu12Mn8Al3Fe2Ni alloy in 3.5% NaCl aqueous solution was studied bymagnetostrictive vibratory device for cavitation erosion. The results show that the cavitation erosion resistance ofthe as-welded Cu12Mn8Al3Fe2Ni alloy is much more superior to that of the as-cast one. The cumulative mass lossand the mass loss rate of the as-welded Cu12Mn8Al3Fe2Ni alloy are almost 1/4 that of the as-cast one. SEM analysisof eroded specimens reveals that the as-cast Cu12Mn8Al3Fe2Ni alloy is attacked more severely than the as-weldedone. Microcracks causing cavitation damage initiate at the phase boundaries.

Influence of Ni/Mn ratio on magnetostructural transformation and magnetocaloric effect in Ni48-xCo2Mn38+xSn12(x=0,1.0,1.5,2.0,and 2.5)ferromagnetic shape memory alloys

An investigation on the magnetostructural transformation and magnetocaloric properties of Ni48-xCo2Mn38＋xSn12（x = 0, 1.0, 1.5, 2.0, and 2.5） ferromagnetic shape memory alloys is carried out. With the partial replacement of Ni by Mn in the Ni_（48）Co2Mn38Sn12 alloy, the electron concentration decreases. As a result, the martensitic transformation temperature is decreased into the temperature window between the Curie-temperatures of austenite and martensite. Thus, the samples with x = 1.5 and 2.0 exhibit the magnetostructural transformation between the weak-magnetization martensite and ferromagnetic austenite at room temperature. The structural transformation can be induced not only by the temperature,but also by the magnetic field. Accompanied by the magnetic-field-induced magnetostructural transformation, a considerable magnetocaloric effect is observed. With the increase of x, the maximum entropy change decreases, but the effective magnetic cooling capacity increases.

GROWTH OF ISOTHERMAL MARTENSITE IN AN Fe-Ni-Mn ALLOY

The substructural development of martensite plates at different stage of the transformation for an Fe-21Ni-4Mn alloy has been investigated by using transmission electron microscope. Twinning was found in small thin platelets at the initial stage.Fine twins extend to the whole platelet.The dislocations and twins were found in the thick platelets at a later stage.Bending of the twins was also observed frequently at this stage.Finally,several platelets coalesce with each other to form a macroscopic(252)_f martensite“plate”.The original habit plane of the individual platelet was measured to be close to(121)_f.