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1.
Ni56Fe17Ga27-xCox合金的组织结构与马氏体相变 总被引:1,自引:1,他引:0
采用光学显微镜、X射线衍射分析及差示扫描量热法系统研究了Co含量对Ni56Fe17Ga27-xCox合金组织结构和马氏体相变的影响.结果表明,室温下铸态Ni56Fe17Ga27-xCox合金显微组织由马氏体和γ相两相组成,γ相随Co含量增加而增多, Ni56Fe17Ga21Co6合金中γ相的体积百分含量达到70%.马氏体相为单斜6M结构.试验合金冷却和加热过程中发生一步马氏体相变及其逆转变,相变温度(Ms、As)随Co含量增加而升高. 相似文献
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用电阻、恢复率同步测量的方法,研究了热循环对Ni47Ti44Nb9合金马氏体相变和记忆性的影响,并通过X-射线衍射、金相观察等方法对其微观机理进行了探讨。结果表明,随着热循环次数的增加,合金Ms明显下降;但热循环下不能诱发R相变,并对合金记忆性无明显影响。 相似文献
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Fe对β基Co-Ni-Al合金马氏体相变和磁性转变的影响 总被引:1,自引:0,他引:1
利用金相和SEM显微组织分析技术,示差扫描量热法(DSC)和振动磁力计(VSM)考察了Fe元素对Co38Ni33Al29和Co72-xNixAl28合金马氏体相变和铁磁性转变的影响。研究发现对于1623K×2h淬火的Co38-xNi33Al29Fex合金,最初的2%Fe使Curie点提高了15K,但随着Fe含量提高,Curie点增加速度提高,在8%Fe范围内平均每1%Fe元素使Curie点大约提高20K。用2%Fe元素代替Co72-xNixAl28合金中同等含量的Co元素时,1623K×2h淬火后Curie点升高20~30K,马氏体相变温度降低150~170K;1523K×12h淬火后Curie点升高30~70K,马氏体相变温度降低50~130K。在β基Co-Ni-Al合金基础上,用Fe元素代替Co元素提高Curie点,降低马氏体相变温度,但扩大了Tc>Tm的CoNiAlFe铁磁性形状记忆合金的成分范围,使其向富Ni低Co、Al方向移动。用平均s+d电子浓度解释了马氏体相变温度和Curie点的变化。 相似文献
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研究了Fe-29.44Mn-6.20Si合金中的r→←ε相变和顺磁性→→反铁磁性转变(以下简称磁转变)。用电阻测量跟踪了此过程。用X射线珩射法(XRD0作了相分析。硅急剧增加六方相的电阻率,ε→r相变表现为电阻降低,r→ε转变表现为电阻升高。XRD表明,淬火后样品除r相外有少量六方ε相。扭转形变恢复率与形变量和形变前无热诱发马氏体存在有很大关系。 相似文献
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通过设计试样原始表面形状和冷轧的方法获得了一种原位内生形状记忆合金复合材料。利用设计试样原始表面形状的方法,将具有不同位错密度的宏观区域引入形状记忆合金内部,则整个材料就获得了复合材料的特征。结果表明在第一次加热过程中正弦试样DSC曲线上出现双峰,分别对应于设计试样内部的不同变形区域,且由于位错织构和马氏体变体界面的作用,使得逆转变温度扩展到一个较大的温度范围。所设计的材料具体可以应用于所谓的广域温度记忆效应和类因瓦效应领域。所有上述现象表明为控制材料的热特性而进行适当的位错织构设计的方法是可行的。 相似文献
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CuZnAlMnNi形状记忆合金马氏体相变焓的研究 总被引:2,自引:0,他引:2
采用差示扫描量热分析技术在5℃/min以及在超低降温速率下,研究了CuZnAlMnNi形状记忆合金马氏体相变的热焓。通过实验和计算,由母相向马氏体转变时单位质量的相变总焓、热容改变焓和马氏体相变焓分别是3.22J/g、1.88J/g和1.34J/g。 相似文献
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应用具有变温样品室的X射线衍射仪及扫描电镜研究了铁磁形状记忆合金Co50Ni20Ga32样品马氏体相变的特性.研究发现,多晶Co50Ni20Ga32合金具有可恢复的热弹性马氏体转变特性.y相的存在对马氏体转变的自协作形貌有很大影响.γ相含量多时,马氏体变体的自协作形貌以金刚石形为主,γ相含量少时,马氏体变体的自协作形貌以平行形为主.在大约520℃以上时,y相的含量随温度升高而增加. 相似文献
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A. L. Liu J. H. Sui Y. C. Lei W. Cai Z. Y. Gao L. C. Zhao 《Journal of Materials Science》2007,42(14):5791-5794
In the present work, 1 at% Y was added to Ti-50.7at%Ni alloy to prepare Ti-50.2Ni-1Y alloy and the effects of rare earth Y
addition on the microstructure and martensitic transformation behavior of Ti-50.7at%Ni alloy was investigated by optical microscope,
scanning electronic microscope (SEM) X-ray diffraction (XRD) and differential scanning calorimetry (DSC). The results show
the microstructure of Ti-50.2Ni-1Y alloy is different with that of Ti-50.7at.%Ni alloy, and its microstructure consists of
B19′martensite and the Y-rich phase, which may be YNi phase. One-step martensitic transformation occurs in Ti-50.2Ni-1Y ternary
alloy. The phase transformation temperatures increase rapidly with Y addition, and the increase of Ms is about 85°C. 相似文献
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F. Chen Y.X. TongX.L. Lu X. WangB. Tian L. LiY.F. Zheng C.Y. ChungL.W. Ma 《Materials Letters》2011,65(7):1073-1075
In this investigation, the effect of graphite addition on martensitic transformation and damping behavior of Ni50Ti50 (at.%) shape memory alloy has been studied. It is found that martensitic transformation temperature decreases obviously with the addition of graphite. Microstructural observation shows that TiC precipitates and forms whiskers when the carbon content is increased beyond ~ 0.6%. With the increase of graphite content, the damping capacity during reverse transformation increases initially and then decreases while the damping capacity of full martensite is remarkably improved by the addition of graphite particles. It is proposed that the enhancement of damping capacity can be ascribed to the high damping capacity of graphite itself, as well as, the increase of the amount of interface between martensite and austenite can be beneficial to the damping capacity. 相似文献
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《Materials Science & Technology》2013,29(14):1795-1800
AbstractThe influence of Co additions on the microstructure, second phase precipitates, phase transformation and mechanical properties of cast Ni51?xTi49Cox (x?=?0, 0·5, 1·5 and 4 at-%) shape memory alloys was investigated. At the expense of Ni, Co added to NiTi alloy significantly increases the martensitic transformation temperature. The matrix phase in the microstructure of Ni51Ti49Co0 alloy is the austenite phase (B2) in addition to martensite phase (B19′) and precipitates of NiTi intermetallic compounds. However, the parent phase in the other three alloys, Ni50·5Ti49Co0·5, Ni49·5Ti49Co1·5 and Ni47Ti49Co4, is martensite. Ti2Ni phase was found in the microstructures of the all investigated alloys; however, Ni3Ti2 phase precipitated only in the NiTi alloy with 0 at-%Co. The volume fraction of Ti2Ni phase decreased by the additions of 0·5 and 1·5 at-%Co, while it is slightly increased with 4 at-%Co. The hardness value of NiTi alloy is affected by Co additions. 相似文献
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The shape memory effect in Ni-49 Ti alloy after solution treatment at 800° C for 0.5 h and ageing at 400, 500, 600and 700° C for 1 h has been investigated by means of transmission electron microscopy and differential thermal analysis (DTA) measurement. Ageing at 400 and 500° C for 1 h causes the precipitation of characteristic temperatures towards higher values. In sample aged at 500° C three distinct DTA peaks arise giving evidence of intermediate stages of the martensite transformation. 相似文献
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Abstracts are not published in this journal
This revised version was published online in November 2006 with corrections to the Cover Date. 相似文献
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The present study reports on direct magneto-microstructural observations made during the stress-induced martensitic transformation
in Co49Ni21Ga30 alloy single crystals with optical, scanning electron, and magnetic force microscopy (MFM). The evolution of the microstructure
and the associated magnetic domain morphology as a function of applied strain were investigated in the as-grown condition
and after thermo-mechanical training. The results demonstrated that the stress-induced martensite (SIM) evolves quite differently
in the two conditions and depending on the martensite formation mechanisms, the magnetic domain configuration was dissimilar.
In the as-grown crystals two twin-related martensite variants were formed and the growth of these twin variants resulted in
large strain. After thermo-mechanical training a morphology similar to a self-accommodating martensite structure was present
at the initial stages of the transformation and thereafter martensite reorientation (MR) was the main transformation mechanism.
The magnetic domains were found to be superimposed on the nano-scaled martensite twins in the as-grown condition, whereas
training brought about the formation of domains on the order of a few microns without showing the one-to-one correspondence
between domains and the twin structure. After the thermo-mechanical training detwinning at high-strain levels led to the formation
of stripe-like domain structures. The ramifications of the results with respect to the magneto-microstructural coupling that
may cause the magnetic shape memory effect (MSME) in Co–Ni–Ga alloys under constant external stress is addressed. 相似文献
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通过熔体抽拉技术制备Ni50.1Mn24.1Ga20.3Fe5.5多晶纤维,采用步进式热处理释放因快速凝固引起的内应力和缺陷,利用场发射扫描电子显微镜、透射电子显微镜、XRD衍射仪对其微结构和相结构进行表征,采用动态机械拉伸仪测试其相变行为和双程形状记忆性能。结果表明:热处理后原子有序度显著提高,孪晶界平直,在恒应力作用下一个热循环中母相和马氏体相的形状得到完全恢复。双程形状记忆曲线显示了热弹性马氏体相变的两个基本特征:可逆性和热滞性。在热循环实验中,纤维被加载到198 MPa时,其马氏体态总应变达到1.32%。根据热机械拉伸测量,发现相变温度遵循Clausius-Clapeyron关系式。与诸如Ti-Ni和Cu-Al-Ni的其他合金相比,Fe掺杂的纤维显示出较小的应变-应力依赖性,在恒应变输出的驱动中是有益的。 相似文献