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磁形状记忆合金Mn2NiGa的第一性原理计算 被引量:1
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作者 李春梅 胡岩菲 +4 位作者 高明 黄仁忠 封文江 张扬 范晓岚 《沈阳师范大学学报(自然科学版)》 CAS 2019年第4期289-295,共7页
Mn 2NiGa磁形状记忆合金立方奥氏体相因在室温下具有可逆马氏体相变,同时居里温度高达588 K,在高温下具有优异的磁热效应,因而在相应的学术领域和应用领域中具有重要的研究价值。掌握Mn 2NiGa磁形状记忆合金的原子占位、结构相变、磁性... Mn 2NiGa磁形状记忆合金立方奥氏体相因在室温下具有可逆马氏体相变,同时居里温度高达588 K,在高温下具有优异的磁热效应,因而在相应的学术领域和应用领域中具有重要的研究价值。掌握Mn 2NiGa磁形状记忆合金的原子占位、结构相变、磁性质和弹性常数是实现Mn 2NiGa合金磁形状记忆性能优化的关键。采用目前国际上较为先进的第一性原理精确Muffin-Tin轨道方法,系统计算研究了0 K下Mn 2NiGa合金立方奥氏体相与四方马氏体相的晶格结构参数、磁矩、弹性常数、电子结构及总能。研究结果表明,Mn 2NiGa合金立方奥氏体相具有Hg 2CuTi型晶格结构,而非传统Ni 2MnGa的L 2 1结构;Mn原子是合金总磁矩的主要提供者,且2种Mn原子磁矩呈反平行排列;奥氏体相的剪切模量(C′=(C 11-C 12)/2)小于0,因而低温下立方结构不稳定,可以发生由立方相到四方相的马氏体相变;根据Jahn-Teller效应,低温下四方相相对于立方相的稳定性,主要源于2种Mn和Ni原子分别与Ga原子的共价结合作用。上述理论结果有望为Mn 2NiGa合金性能的进一步优化提供理论指导。 展开更多
关键词 磁形状记忆合金 MN 2NiGa 弹性常数 第一性原理计算
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单向压力对Ni-Mn-Ga磁形状记忆合金马氏体相变的影响 被引量:1
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作者 刘静 陆兴 +1 位作者 覃作祥 赵云燕 《大连铁道学院学报》 2004年第2期64-67,共4页
采用电阻和应变测量的方法,研究了单向压力对Heusler合金Ni56.3Mn19.3Ga22.8C1.6马氏体相变的影响 结果表明:在压力小于4.44MPa时相变温度随压力值的升高而降低,dTdσ=0.648K/MPa,说明了一定的压力阻碍马氏体相变的发生,当压力大于点升... 采用电阻和应变测量的方法,研究了单向压力对Heusler合金Ni56.3Mn19.3Ga22.8C1.6马氏体相变的影响 结果表明:在压力小于4.44MPa时相变温度随压力值的升高而降低,dTdσ=0.648K/MPa,说明了一定的压力阻碍马氏体相变的发生,当压力大于点升高,其原因可能是压力超过了临界值而引发了另一种相变 展开更多
关键词 单向压应力 马氏体相变 镍-锰-镓合金 磁形状记忆合金
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Co掺杂对NiMnIn磁形状记忆合金相变性能的影响
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作者 沈渊 张宝红 《河北农机》 2016年第3期39-39,共1页
本文采用电弧熔炼的方法制备了不同Co原子含量掺杂的Ni50Mn37In13磁形状记忆合金,使用示差扫描量热仪(DSC)测量合金马氏体相变的温度。研究结果表明:Co原子掺杂改变了合金的价电子浓度和结构,使合金马氏体相变温度降低。
关键词 磁形状记忆合金 相变 价电子浓度
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超高温度梯度定向凝固NiMnFeGa磁致形状记忆合金 被引量:1
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作者 李建国 郑红星 +2 位作者 马伟增 卢玉英 季诚昌 《航空材料学报》 EI CAS CSCD 2003年第z1期1-4,共4页
利用超高温度梯度定向凝固装置制备出定向Ni_(51.2)Mn_(20.0)Fe_(13.0)Ga_(15.8)磁致形状记忆合金。沿晶体生长方向凝固组织由等轴晶逐渐过渡为柱状晶,马氏体变体取向性明显,γ相愈加细小,分布愈加均匀。Ni_(51.2)Mn_(20.0)-Fe_(13.0)Ga... 利用超高温度梯度定向凝固装置制备出定向Ni_(51.2)Mn_(20.0)Fe_(13.0)Ga_(15.8)磁致形状记忆合金。沿晶体生长方向凝固组织由等轴晶逐渐过渡为柱状晶,马氏体变体取向性明显,γ相愈加细小,分布愈加均匀。Ni_(51.2)Mn_(20.0)-Fe_(13.0)Ga_(15.8)合金在加热和冷却过程中发生热致马氏体相变及逆相变,马氏体相变温度M_s=121.3℃,M_f=99.3℃,A_3=118℃,A_f=147℃。 展开更多
关键词 NiMnFeGa合金 定向凝固 形状记忆合金 马氏体相变
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新型磁驱动形状记忆合金研究进展 被引量:2
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作者 袁比飞 《材料工程》 EI CAS CSCD 北大核心 2007年第2期62-66,共5页
磁驱动形状记忆合金是一种新型功能材料,由于兼具大的输出应变和高响应频率等综合特性,成为智能材料领域的研究热点之一。本研究首先总结了Ni-Mn-Ga合金在相变和磁致应变性能方面的特点,然后着重介绍了Co-Ni-Ga和Ni-Fe-Ga两类新型磁驱... 磁驱动形状记忆合金是一种新型功能材料,由于兼具大的输出应变和高响应频率等综合特性,成为智能材料领域的研究热点之一。本研究首先总结了Ni-Mn-Ga合金在相变和磁致应变性能方面的特点,然后着重介绍了Co-Ni-Ga和Ni-Fe-Ga两类新型磁驱动记忆合金在结构、相变、形状记忆效应、磁性能等方面的研究进展,并对其中存在的问题进行了讨论。 展开更多
关键词 驱动形状记忆合金 Ni-Mn—Ga Co-Ni—Ga Ni-Fe-Ga
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NiMnIn基磁致形状记忆合金晶体学研究进展 被引量:1
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作者 闫海乐 黄晓明 +3 位作者 杨波 李宗宾 赵骧 左良 《中国材料进展》 CAS CSCD 北大核心 2021年第12期996-1006,共11页
NiMnIn基合金是一类新型磁控功能材料,具有优异的磁致形状记忆效应和磁热效应等。该合金磁控性能来源于磁场诱发的逆马氏体相变,即从弱磁性马氏体转变为铁磁性奥氏体。奥氏体和马氏体的晶体结构、马氏体微观组织晶体学特征、马氏体相变... NiMnIn基合金是一类新型磁控功能材料,具有优异的磁致形状记忆效应和磁热效应等。该合金磁控性能来源于磁场诱发的逆马氏体相变,即从弱磁性马氏体转变为铁磁性奥氏体。奥氏体和马氏体的晶体结构、马氏体微观组织晶体学特征、马氏体相变取向关系等晶体学知识,对于深入理解和优化该合金多功能磁控行为具有重要的指导意义。基于近年来在NiMnIn基磁致形状记忆合金晶体学研究方面取得的主要进展,围绕奥氏体和6M调制马氏体晶体结构特征、6M调制马氏体微观组织的晶体学特征及其形成机制、马氏体相变晶体学取向关系、马氏体相变转变路径、6M调制马氏体在外加载荷下的变体重排行为及其机制5个方面展开讨论。最后,对NiMnIn基磁致形状记忆合金晶体学研究存在的主要问题和发展趋势进行了总结和展望。 展开更多
关键词 NiMnIn 形状记忆合金 调制马氏体 马氏体相变 变体选择 相变取向关系 晶体学
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B元素对Ni-Fe-Ga-Co磁致形状记忆合金相变及力学性能的影响
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作者 张清华 《化工管理》 2021年第29期37-38,42,共3页
文章研究了B元素的添加对Ni_(46)-xFe_(18)Ga_(27)Co_(9)B_(x)(at.%,x=0,0.1,0.5)磁致形状记忆合金显微组织、相变温度和力学性能的影响。结果表明:在Ni_(46)-xFe_(18)Ga_(27)Co_(9)B_(x)(at.%,x=0,0.1,0.5)合金中用B元素替代部分Ni元素... 文章研究了B元素的添加对Ni_(46)-xFe_(18)Ga_(27)Co_(9)B_(x)(at.%,x=0,0.1,0.5)磁致形状记忆合金显微组织、相变温度和力学性能的影响。结果表明:在Ni_(46)-xFe_(18)Ga_(27)Co_(9)B_(x)(at.%,x=0,0.1,0.5)合金中用B元素替代部分Ni元素,合金的抗压强度和塑性同时得到了提高,其相变温度随B含量的增加而降低。常温下各成分合金都为奥氏体相,随着B含量的增加会有弥散相析出。 展开更多
关键词 Ni_(46)-xFe_(18)Ga_(27)Co_(9)B_(x) 形状记忆合金 相变温度 力学性能
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直流磁控溅射Ni_(49.54)Mn_(29.59)Ga_(20.87)磁驱动记忆合金薄膜的XPS研究
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作者 高来勖 刘超 +3 位作者 高智勇 安旭 蔡伟 赵连城 《功能材料》 EI CAS CSCD 北大核心 2007年第1期50-52,共3页
采用直流磁控溅射技术沉积了Ni49.54Mn29.59Ga20.87磁驱动形状记忆合金薄膜。XRD结果表明,Ni49.54Mn29.59Ga20.87薄膜室温下为5层调制型结构马氏体。X射线光电子能谱(XPS)分析表明,放置于空气中2个月的沉积态薄膜表面吸附少量氧和碳杂... 采用直流磁控溅射技术沉积了Ni49.54Mn29.59Ga20.87磁驱动形状记忆合金薄膜。XRD结果表明,Ni49.54Mn29.59Ga20.87薄膜室温下为5层调制型结构马氏体。X射线光电子能谱(XPS)分析表明,放置于空气中2个月的沉积态薄膜表面吸附少量氧和碳杂质。随Ar+刻蚀深度的增加,表面C杂质易被剥蚀掉,而部分氧杂质以MnO状态存在;Ni、Mn、Ga元素含量由薄膜表面向内层逐渐增加,化学价由正价向零价转变。 展开更多
关键词 NI-MN-GA 驱动形状记忆合金 薄膜 溅射
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Ni-Fe-Ga磁致形状记忆合金中间马氏体相变 被引量:9
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作者 郑红星 刘剑 +1 位作者 夏明许 李建国 《物理学报》 SCIE EI CAS CSCD 北大核心 2005年第4期1719-1721,共3页
采用差示扫描量热和x射线衍射技术研究Ni Fe Ga磁致形状记忆合金的马氏体相变行为 .结果发现 ,在多晶Ni56 5Fe1 9 0 Ga2 4 5和Ni56 3Fe1 7 0 Ga2 6 7合金中除马氏体相变外 ,还观察到一次完整的、正相变和逆相变对应出现、单纯由温... 采用差示扫描量热和x射线衍射技术研究Ni Fe Ga磁致形状记忆合金的马氏体相变行为 .结果发现 ,在多晶Ni56 5Fe1 9 0 Ga2 4 5和Ni56 3Fe1 7 0 Ga2 6 7合金中除马氏体相变外 ,还观察到一次完整的、正相变和逆相变对应出现、单纯由温度诱发的中间马氏体相变 .该中间马氏体相变与马氏体相变均为热弹性相变 .室温下合金的稳态马氏体为 14层单斜结构 . 展开更多
关键词 镍-铁-镓 形状记忆合金 中间马氏体相变 热弹性相变
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Ni-Fe-Ga磁致形状记忆合金的马氏体相变和晶体结构的研究 被引量:1
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作者 白静 王新丽 +3 位作者 顾江龙 李艳波 赵骧 左良 《材料研究学报》 EI CAS CSCD 北大核心 2014年第12期881-886,共6页
使用DSC、XRD、SEM和TEM等分析测试手段,对Ni50+xFe25-xGa25(x=3,4.5,6)合金的马氏体相变温度、精细显微结构以及复杂马氏体晶体结构进行了系统研究。结果表明,Ni50+xFe25-xGa25合金的马氏体相变温度Tm随Ni含量增加而升高。Ni56Fe19Ga2... 使用DSC、XRD、SEM和TEM等分析测试手段,对Ni50+xFe25-xGa25(x=3,4.5,6)合金的马氏体相变温度、精细显微结构以及复杂马氏体晶体结构进行了系统研究。结果表明,Ni50+xFe25-xGa25合金的马氏体相变温度Tm随Ni含量增加而升高。Ni56Fe19Ga25合金的马氏体板条非常清晰细密,且存在着多种不同取向的变体;该种合金由6M+14M混合马氏体和γ相组成。Ni56Fe19Ga25合金既具有适合实际应用的马氏体相变温度,又具有有利于磁致应变的晶体结构。 展开更多
关键词 金属材料 功能材料 Ni-Fe-Ga 形状记忆合金 晶体结构 显微组织 马氏体相变
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Ni_(50)Mn_(37)In_(13)磁驱动形状记忆合金薄膜中的交换偏置 被引量:1
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作者 周广宏 潘旋 +1 位作者 朱雨富 王寅岗 《稀有金属材料与工程》 SCIE EI CAS CSCD 北大核心 2014年第1期130-134,共5页
研究了磁场冷却前后Ni50Mn37In13磁驱动形状记忆合金薄膜在低温下的磁学行为。结果表明:磁场冷却后的Ni50Mn37In13薄膜在10 K温度下表现出一定的交换偏置效应。在特征温度Tf以下,零场冷却状态下的Ni50Mn37In13合金处于超自旋玻璃态,而... 研究了磁场冷却前后Ni50Mn37In13磁驱动形状记忆合金薄膜在低温下的磁学行为。结果表明:磁场冷却后的Ni50Mn37In13薄膜在10 K温度下表现出一定的交换偏置效应。在特征温度Tf以下,零场冷却状态下的Ni50Mn37In13合金处于超自旋玻璃态,而经磁场冷却后发生了从自旋玻璃态向磁有序的超铁磁结构的变化。超铁磁结构中的超铁磁团簇与反铁磁基体构成了铁磁/反铁磁耦合,从而导致了交换偏置的产生。 展开更多
关键词 交换偏置 驱动形状记忆合金 薄膜
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多晶Ni_(2.1)Mn_(0.9)Ga_(0.9)C_(0.1)合金的马氏体相变特征 被引量:1
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作者 陆兴 陈晓琴 +2 位作者 邱立新 邱明辉 覃作祥 《大连铁道学院学报》 2000年第4期51-54,68,共5页
采用电阻、热膨胀、磁致伸缩及光学金相等试验方法研究了多晶Ni2.1Mn0.9Ga0.9C0.1 合金的马氏体相变特征.结果表明:Ni2.1Mn0.9Ga0.9C0.1合金在400~100K之间发生两次相 变,第一次为马... 采用电阻、热膨胀、磁致伸缩及光学金相等试验方法研究了多晶Ni2.1Mn0.9Ga0.9C0.1 合金的马氏体相变特征.结果表明:Ni2.1Mn0.9Ga0.9C0.1合金在400~100K之间发生两次相 变,第一次为马氏体相变,它的热滞后比较小,马氏体相的电阻率高于母相的电阻率;而 第二次相交的结构变化尚未澄清,它的热滞后比较大,新相的电阻率低于母相的电阻率. 马氏体相变时,合金结晶方向长度收缩,磁致伸缩急剧减小.合金中马氏体基本为相互 平行的片状组织. 展开更多
关键词 马氏体相变 致伸缩 Ni-Mn-CA合金 磁形状记忆合金 相变温度 相变特征
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Magnetocaloric effect in Ni-Mn-In-Co microwires prepared by Taylor-Ulitovsky method 被引量:1
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作者 张学习 苗生沛 孙剑飞 《Transactions of Nonferrous Metals Society of China》 SCIE EI CAS CSCD 2014年第10期3152-3157,共6页
Ni-Mn-In-Co microwires with diameter of 30-100 μm are prepared by glass-coated metal filaments(Taylor–Ulitovsky) method. The effects of magnetic field on martensite transformation temperature in the as-prepared an... Ni-Mn-In-Co microwires with diameter of 30-100 μm are prepared by glass-coated metal filaments(Taylor–Ulitovsky) method. The effects of magnetic field on martensite transformation temperature in the as-prepared and annealed microwires are investigated using a physical property measurement system(PPMS). Magnetocaloric effect(MCE) attributed to field-induced austenite transformation in the as-prepared and annealed microwires is analyzed indirectly from the isothermal magnetization(M-B) curves. The as-prepared microwire has a 7-layer modulated martensite structure(7M) at room temperature. The changes of austenite starting temperature induced by an external magnetic field(ΔAs/ΔB) in the as-prepared and annealed microwires are-1.6 and-4 K/T, respectively. Inverse martensite to austenite transformation exists in annealed microwires when an external magnetic field is applied at temperatures near As. The entropy change(ΔS) obtained in the annealed microwires is 3.0 J/(kg·K), which is much larger than that in the as-prepared microwires 0.5 J/(kg·K). The large entropy change and low price make Ni-Mn-In-Co microwires a potential working material in magnetic refrigeration. 展开更多
关键词 magnetic shape memory alloys MICROWIRES martensitic transformation magnetocaloric effect magnetization curve
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Ferroic domain characterization of Ni_(55)Mn_(20.6)Ga_(24.4) ferromagnetic shape memory alloy
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作者 宋红章 曾华荣 +2 位作者 李永祥 殷庆瑞 胡行 《Transactions of Nonferrous Metals Society of China》 SCIE EI CAS CSCD 2011年第9期2015-2019,共5页
The microstructure and coupling between structural and magnetic domains of ferromagnetic shape memory alloy Ni55Mn20.6Ga24.4 were investigated by scanning electron acoustic microscopy (SEAM). Stripe ferroelastic dom... The microstructure and coupling between structural and magnetic domains of ferromagnetic shape memory alloy Ni55Mn20.6Ga24.4 were investigated by scanning electron acoustic microscopy (SEAM). Stripe ferroelastic domains (martensite variants) exist in every grain, and exhibit the configurations of the typical self-accommodation arrangement. Magnetic domain structure of Ni55Mn20.6Ga24.4 was observed by the Bitter method and magnetic force microscopy (MFM). Due to the unique subsurface imaging capability of SEAM, combined with the Bitter method, the ferroelastic domain structure can be compared with in situ ferromagnetic domain structure. It is found that the martensitic variant boundaries coincide well with the ferromagnetic domain walls, which is beneficial for the understanding of the correlation between two kinds of ferroic domains. 展开更多
关键词 ferroic domain ferromagnetic shape memory alloy scanning electron acoustic microscopy
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Effect of Sn substitution and heat treatment on microstructure and microhardness of Co_(38)Ni_(34)Al_(28-x)Sn_x magnetic shape memory alloys
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作者 苏佳佳 谢致薇 杨元政 《Transactions of Nonferrous Metals Society of China》 SCIE EI CAS CSCD 2012年第9期2158-2163,共6页
Sn was used to replace Al in Co38Ni34Al28 alloy. The microstructure and microhardness of Co38Ni34Al28-xSnx (x=0, 1, 2, 3) magnetic shape memory alloys were investigated at different heat treatment temperatures (137... Sn was used to replace Al in Co38Ni34Al28 alloy. The microstructure and microhardness of Co38Ni34Al28-xSnx (x=0, 1, 2, 3) magnetic shape memory alloys were investigated at different heat treatment temperatures (1373 K, 1473 K, and 1573 K) for 2 h. The results show that more Sn substitution reduces the content of γ-phase and a partial phase of martensite can be obtained in Co38Ni34Al28-xSnx (x=1, 2, 3) alloys after treatment at 1573 K for 2 h. The maximum martensite phase appears when 2% Al is substituted by Sn. The reverse martensitic transformation temperature of Co38Ni34Al28-xSnx alloys increases at x=1 and 2, then decreases as x=3. As the content of Sn and the temperature increase, the microhardness will increase. 展开更多
关键词 magnetic shape memory alloy Sn substitution Co-Ni-Al alloy MICROSTRUCTURE martensitic transformation
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Effect of Co substitution on magnetic properties of Ni-Mn-Sn magnetic shape memory alloys 被引量:2
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作者 曹伽牧 谭昌龙 +4 位作者 田晓华 李钦赐 郭二军 王丽萍 曹一江 《Transactions of Nonferrous Metals Society of China》 SCIE EI CAS CSCD 2014年第4期1053-1057,共5页
The effect of Co substitution on magnetic properties of Ni-Mn-Sn shape memory alloy was revealed by first-principles calculations. Large magnetization difference in Ni-Mn-Sn alloy obtained by addition of Co arises fro... The effect of Co substitution on magnetic properties of Ni-Mn-Sn shape memory alloy was revealed by first-principles calculations. Large magnetization difference in Ni-Mn-Sn alloy obtained by addition of Co arises from enhancement of magnetization of austenite due to change of Mn-Mn interaction from anti-ferromagnetism to ferromagnetism. Total energy difference between paramagnetic and ferromagnetic austenite plays an important role in magnetic transition of Ni-Co-Mn-Sn. The altered Mn 3d states due to Co substitution give rise to difference in magnetic properties. 展开更多
关键词 ferromagnetic shape memory alloys Ni-Mn-Sn first-principles calculation magnetic properties
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Microstructure, martensitic transformation and mechanical properties of Ni-Mn-Sn alloys by substituting Fe for Ni 被引量:2
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作者 Chang-long TAN Zhi-cheng FENG +3 位作者 Kun ZHANG Ming-yang WU Xiao-hua TIAN Er-jun GUO 《Transactions of Nonferrous Metals Society of China》 SCIE EI CAS CSCD 2017年第10期2234-2238,共5页
The effects of partial substitution of Fe element for Ni element on the structure,martensitic transformation and mechanicalproperties of Ni50-xFexMn38Sn12(x=0and3%,molar fraction)ferromagnetic shape memory alloys were... The effects of partial substitution of Fe element for Ni element on the structure,martensitic transformation and mechanicalproperties of Ni50-xFexMn38Sn12(x=0and3%,molar fraction)ferromagnetic shape memory alloys were investigated.Experimentalresults indicate that by substitution of Fe for Ni,the microstructure and crystal structure of the alloys change at room temperature.Compared with Ni50Mn38Sn12alloy,the martensitic transformation starting temperature of Ni47Fe3Mn38Sn12alloy is decreased by32.5K.It is also found that martensitic transformation occurs over a broad temperature window from288.9to352.2K.It is found that themechanical properties of Ni-Mn-Sn alloy can be significantly improved by Fe addition.The Ni47Fe3Mn38Sn12alloy achieves amaximum compressive strength of855MPa with a fracture strain of11%.Moreover,the mechanism of the mechanical propertyimprovement is clarified.Fe doping changes the fracture type from intergranular fracture of Ni50Mn38Sn12alloy to transgranularcleavage fracture of Ni47Fe3Mn38Sn12alloys. 展开更多
关键词 Ni-Mn-Sn alloys martensitic transformation mechanical properties ferromagnetic shape memory alloys
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Mechanocaloric materials for solid-state cooling 被引量:5
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作者 Binfeng Lu Jian Liu 《Science Bulletin》 SCIE EI CAS CSCD 2015年第19期1638-1643,共6页
This article reviews the up-to-date progress in mechanocaloric effect and materials near ambient temperature. For elastocaloric materials, we focus on directly measured temperature change and its entropy origin in non... This article reviews the up-to-date progress in mechanocaloric effect and materials near ambient temperature. For elastocaloric materials, we focus on directly measured temperature change and its entropy origin in nonmagnetic and magnetic shape memory alloys. In terms of barocaloric materials, change in magnetic state, volume and shift of transition temperature due to hydrostatic pressure are systematically compared. We propose advantages and challenges of elastocaloric materials for solidstate cooling. Strategies to enhance elastocaloric and mechanical stability under long-term mechanical cycles are presented. Finally, we conclude with an outlook on the prospect of elastocaloric cooling application. 展开更多
关键词 Elastocaloric effect Barocaloric effect Shape memory alloy ENTROPY
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Composition dependent elastic modulus and phase stability of Ni_2MnGa based ferromagnetic shape memory alloys
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作者 HU QingMiao LUO HuBin +2 位作者 LI ChunMei VITOS Levente YANG Rui 《Science China(Technological Sciences)》 SCIE EI CAS 2012年第2期295-305,共11页
Ni2MnGa based ferromagnetic alloys are ideal candidates for applications such as actuators, magnetic refrigerators or magne-tostrictive transducers due to their attractive properties such as magnetic field induced sha... Ni2MnGa based ferromagnetic alloys are ideal candidates for applications such as actuators, magnetic refrigerators or magne-tostrictive transducers due to their attractive properties such as magnetic field induced shape memory effect and large magnetocaloric effect. The properties of these alloys (e.g., the martensitic transformation temperature TM) sensitively depend on the composition. Understanding the composition dependence of these properties so as to design the alloy as desired is one of the main research topics in this area. In recent years, we have investigated the composition dependent elastic modulus and phase stability of Ni2MnGa-based alloys by using a first-principles method, in hope of clarifying their connection to the properties of these alloys. In this article, we review the main results of our investigations. We show that the tetragonal shear modulus C' is a better predictor of the composition dependent TM than the number of valence electrons per atom (e/a) since the general TM-C' correlation works for some of the alloys for which the TM-ela correlation fails, although there exist several cases for which both the general TM-C' and TM-ela correlations break down. Employing the experimentally determined modulation function, the complex 5-layer modulated (5M) structure of the martensite of Ni2MnGa and the Al-doping effect on it are studied. We find that the shuffle and shear of the 5M structure are linearly coupled. The relative stability of the austenite and the marten- sites is examined by comparing their total energies. The non-modulated martensite β'″ with the tetragonality of the unit cell c/a〉1 is shown to be globally stable whereas the 5M martensite with c/a〈1 is metastable. The critical Al atomic fraction over which the martensitic transformation between the 5M martensite and austenite cannot occur is predicted to be 0.26, in reason- able agreement with experimental findings. 展开更多
关键词 NieMnGa martensitic transformation elastic modulus phase stability density functional theory
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Influence of stresses on martensitic transformation in ferromagnetic shape memory Ni_(50)Mn_(19)Fe_6Ga_(25) ribbons
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作者 MENG Fanbin LI Yangxian +4 位作者 LIU Heyan QU Jingping LIU Zhuhong CHEN Jinglian WU Guangheng 《Science China(Technological Sciences)》 SCIE EI CAS 2004年第6期710-715,共6页
The influence of stresses on martensitic transformation in Ni50Mn19Fe6Ga25 melt-spun ribbons was studied. X-ray diffraction examination shows that the ribbon has a pure cubic L21 phase at room temperature and that the... The influence of stresses on martensitic transformation in Ni50Mn19Fe6Ga25 melt-spun ribbons was studied. X-ray diffraction examination shows that the ribbon has a pure cubic L21 phase at room temperature and that the ribbon surface exhibits [100] preferentially oriented texture, while the [110] axis is about 45° tilted from the normal of the ribbon. By calculating the d spacing at different angles with the length direction of the ribbon, the tension was observed. It was found that the direction of the stress was along [010] direction of the oriented textured grains. During cooling, there is no obvious structural transition observed in as-spun ribbons. However, when the ribbons were annealed at 900 K for 24 h, the tension along [010] direction disappeared and the structural transition from cubic to tetragonal occurred obviously during cooling. It indicates that it is the tension along [010] direction to suppress the martensitic transformation in the as-spun ribbons. 展开更多
关键词 STRESS martensitic transformation ferromagnetic shape memory alloy
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