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1.
张志  陈春玲  王朝龙  余东满 《物理学报》2006,55(11):5975-5979
室温下在等静压最高达~0.5GPa的条件下,利用超声回波技术测量了超声波横波和纵波在Nd60Al10Fe20Co10块体金属玻璃中的传播时间来确定横波和纵波速度.测量时所采用的超声波频率为10MHz.利用所测量的数据,建立了超声波波速、样品的密度、弹性模量以及Debye温度等与所施加的压力之间的相互关系.并且推导出Murnaghan状态方程.另外,基于非晶态与晶态物理性能的相似性,对此块体非晶的压缩曲线、弹性常数和Debye温度等进行了理论计算,结果表明Nd60Al10Fe20Co10块体金属玻璃的弹性性能与其组成的元素有着密切的关系. 关键词: 块体金属玻璃 弹性性能 等静压  相似文献   

2.
研究了Pr60Al10Ni10Cu20 大块金属玻璃 的结构和磁性随Fe含量 的变化关系,结果表明Pr基合金逐步从玻璃状态,转变为非晶与纳米晶的复合状态,最后成 为纳米晶合金,Pr基合金的磁性也相应地发生变化.提出了一种通过对大块稀土基金属玻璃 进行Fe掺杂,制备出微观结构和性能具有可调控性的大块纳米晶合金的方法, 并讨论了纳米 晶结构和性能的关系. 关键词: 金属玻璃 大块纳米晶 掺杂  相似文献   

3.
研究了Nd0.5Ca0.5MnO3体系的结构和输运特性. 结构 分析表明,在300K下,体系表现为O′型正交结构并存在典型的Jahn-Teller畸变.在8 T磁场 下,体系出现顺磁绝缘-铁磁金属的转变,庞磁电阻效应发生. 磁测量发现,样品的奈尔温 度TN和电荷有序转变温度TCO分别在150和240K左右,在41K左右出 现典型再入型自旋玻璃行为,同时观察到了负的磁化率异常. 结果表明,Nd关键词: 庞磁电阻 自旋玻璃态 负磁化强度 电荷有序  相似文献   

4.
通过X射线衍射和磁性测量等手段研究了(Nd1-xGdx)3Fe27.31Ti1.69(0≤x≤0.6)化合物的结构和磁性.X射线衍射测量结果表明Gd替代后并未改变Nd3(Fe,Ti)29化合物的晶体结构,但引起了晶胞体积收缩.随着Gd含量的增加,化合物的居里温度TC和室温磁晶各向异性场Ba单调增加,而自旋重取向 关键词: 1-xGdx)3Fe27.31Ti1.69化合物')" href="#">(Nd1-xGdx)3Fe27.31Ti1.69化合物 磁晶各向异性 自旋重取向 磁相图  相似文献   

5.
用电弧熔炼法制备了Nd3.6Pr5.4Fe83Co3B5合金铸锭,然后利用熔旋快淬法在铜辊转速V=20m/s下制备了Nd3.6Pr5.4Fe83Co3B5薄带.快淬带主要由软磁相α-Fe和Nd2Fe14B型的硬磁相组成.采用直流退磁剩磁曲线方法分析了样品在反磁化过程中的可逆与不可逆磁化部分,并研究了软磁相和硬磁相的反磁化行为,得到样品的不可逆磁化形核场Hno约为440kA/m.同时研究了样品的磁黏滞性,结果表明由于软磁相的存在使得热激活体积较大. 关键词:  相似文献   

6.
Zr60Al15Ni25大块非晶合金晶化动力学研究   总被引:1,自引:0,他引:1       下载免费PDF全文
通过等温示差扫描量热法研究了Zr60Al15Ni25大块非 晶合金的晶化动力学.实验结果表明,晶化过程的孕育期很短,即使在743 K这样低的温度下也不过0.52 min,而放热峰宽(反应整个晶化过程进行的时间)却随退火温度的降低明显增大,这说明了结晶过程是一个晶核长大控制的过程.Avrami指数表明在不同的退火温度,该合金的晶化机制发生了变化.晶化机制的变化是由于合金原子在不同温度下的扩散能力相差很大所致. 关键词: 晶化动力学 60Al15Ni25大块非晶合金')" href="#">Zr60Al15Ni25大块非晶合金 示差扫 描量热法(DSC)  相似文献   

7.
测量了超导金属玻璃Zr78Co22的磁阻和上临界磁场Hc2。磁阻的实验结果定性地与包含自旋-轨道散射的三维弱局域化理论相符,而定量则有明显的偏差,其偏差主要来源于超导涨落效应。在所测量的温区内,上临界磁场Hc2随温度呈线性变化,同时还得出超导金属玻璃Zr78Co22中的非弹性散射主要来源于电子-声子相互作用,其散射几率τi-1=1.3×1O10T2,略小于Bergmann理论所预言的值。 关键词:  相似文献   

8.
研究了Nd6 0 Al1 0 Fe2 0 Co1 0 大块金属玻璃磁性随温度的变化关系 ,结果表明Nd6 0 Al1 0 Fe2 0 Co1 0 在室温下表现为永磁性 ,随着温度的降低 ,矫顽力和磁滞回线形状都有很大的变化 .交流磁化率在 18K左右出现尖峰而且峰值温度随频率变化 ,表明该大块非晶体系中存在自旋玻璃态  相似文献   

9.
大块金属玻璃Zr41Ti14Cu12.5Ni10Be22.5的流变行为研究   总被引:2,自引:0,他引:2       下载免费PDF全文
王敬丰  柳林  蒲健  肖建中 《物理学报》2004,53(6):1916-1922
采用静态拉伸方法在连续升温条件下动态地测量了大块金属玻璃Zr41Ti14Cu12.5Ni10Be22.5(Vit1)的黏度随温度的变化关系.在应变速率与温度的关系曲线中,观测到了与玻璃转变和晶化过程相联系的多个应变速率峰.在玻璃转变温度Tg以上,大块金属玻璃Zr41Ti14Cu12.5Ni10Be22.5的过冷液体呈现Newton流体特征,其黏度与温度的关系符合Vogel Fulcher-Tammann (VFT)关系式,拟合得到脆度D*=36,VFT温度T0=319K,脆度参数m=30,这说明Zr41T 关键词: 大块金属玻璃 应变速率 剪切黏度 自由体积  相似文献   

10.
郭古青  杨亮  张国庆 《物理学报》2011,60(1):16103-016103
应用同步辐射X射线衍射(XRD)和广延X射线吸收精细结构边方法(EXAFS),结合反蒙特卡罗(RMC)拟合、Voronoi分形技术等对Zr50Cu50二元和Zr48Cu45Al7三元金属玻璃材料的微观结构进行了系统的研究.结果表明:ZrCuAl三元金属玻璃中Al原子与Zr原子、Cu原子之间存在强相互作用,表现为键长的明显缩短,导致其微观结构中的Voronoi团簇体积普遍小于Zr50关键词: 大块金属玻璃 原子结构 玻璃形成能力 同步辐射技术  相似文献   

11.
Bulk amorphous ferromagnet alloys of composition Nd60Fe30Al10, Nd60Fe20Co10Al10 and Pr58Fe24Al18 have been prepared by argon arc melting and quenching into a copper mould. General insight into the magnetic behaviour of the alloys was gained from measurement of the major hysteresis loop at room temperature, and from zero-field cooled and field-cooled magnetisation measurements in the range 10-400 K. Measurements of the coercivity were made from 10 to 400 K, and for all alloys, the coercivity is seen to increase steeply with decreasing temperature to a peak at a temperature in the range 25-50 K, before decreasing. For all alloys, the temperature dependence of the coercivity between 50 and 400 K is well explained by the strong pinning model of domain walls of Gaunt [Philos. Mag. B 48 (1983) 261]. Quantities deduced from the Gaunt model, along with other relevant magnetic parameters, are used to estimate values for the exchange and anisotropy constants.  相似文献   

12.
Magnetocaloric effect and refrigerant capacity of Gd-based Gd60FexCo30−xAl10 metallic glasses are investigated for x = 0, 10 , 20 and 30. It is found that the non-linearity of saturation magnetization in crystalline Co-Fe binary alloys can be transferred to the quaternary metallic glass. Whereas the magnetocaloric specific values of Gd60Co30Al10 are comparable in magnitude with those of other Gd-based metallic glasses, Fe addition leads to an increase of the saturation magnetization and refrigerator capacity with a maximum for x = 20. Simultaneously, the temperature of maximum isothermal change of magnetic entropy TΔSmax increases from 145 to 200 K with increasing Fe-content and also the halfwidth ΔTSmax/2 of the ΔS-T-curve is considerably broadened. Furthermore, the effect of thermal treatment slightly above the first crystallization event on the magnetocaloric effect are investigated, showing a lowering of the working temperature in the first place.  相似文献   

13.
The Gd60Co26Al6Ge8 alloy has been prepared by the copper-mold suck-casting and its phase component has been investigated by X-ray diffraction (XRD), scanning electron microscopy (SEM), and energy-dispersive spectroscopy (EDS). It is shown that this alloy consists of primary crystalline Gd5Ge3 phase and amorphous matrix. The glass transition temperature (Tg) and crystallization temperatures (Tx) occur at 292 and 320 °C, respectively. The maximal magnetic entropy change (ΔSM) under 0-5 T field is about 7.6 J (kg−1 K−1) at 155 K and the refrigeration capacity (RC) is about 768 J kg−1, which makes Gd60Co26Al6Ge8 bulk metallic glass matrix composite a promising candidate for magnetic refrigerant.  相似文献   

14.
崔晓  徐保臣  王知鸷  王丽芳  张博  祖方遒 《物理学报》2013,62(1):16101-016101
以1at% Ag元素分别等量替代Zr57Cu20Al10Ni8Ti5金属玻璃的各个组元,利用差示扫描量热升温分析获得不同试样的热力学参数,并结合不同尺寸(Φ8,Φ10,Φ12)吸铸试样的X-射线衍射分析结果,考察、验证元素替代后合金的实际玻璃形成能力及热稳定性的变化规律.经比较发现,Ag替代Ti元素,其玻璃形成能力显著提高(直径实际增大4 mm),同时热稳定性也明显改善,且临界冷却速率也明显降低,而Ag替代其他组元却无明显规律.针对玻璃形成能力的相关数据比较分析表明,本文结果未显示符合其Inoue的尺寸准则,混合焓判据也未显示出明显符合的现象.通过对堆垛密度的计算发现,1 at% Ag替代Ti元素后使金属玻璃体系内部的堆垛密度增加.通过动力学分析,从晶化激活能、晶化反应速率常数两方面探讨了元素替代对玻璃形成能力和热稳定性的作用机理.  相似文献   

15.
In situ high-energy X-ray diffraction of Nd60Fe30Al10 and Ce70Al10Cu20 metallic glasses is carried out under high pressure. During compression, Ce70Al10Cu20 and Nd60Fe30Al10 exhibit a polyamorphic transition from low-density state below 2.0 and 10.0?GPa, to high-density state above 8.4 and 21.1?GPa, respectively. The intermediate hysteresis regions are the mixture of both phases. Electrical resistance measurements under high pressure show that Ce70Al10Cu20 display a discontinuous change in pressure dependence curve of resistivity at around 1.7?GPa. The addition of Fe atom gives a significant standoff of phase transition pressure in Nd60Fe30Al10. The results in this work suggest that the solute element and microstructure of lanthanide solvent aggregates have implications on the polyamorphic transition in metallic glasses.  相似文献   

16.
In this paper, compact bulk nanocomposite Nd2Fe14B/α-Fe magnetic materials were prepared by hot extrusion of amorphous and nanocrystalline powders, which were prepared by high-energy ball-milling (HEBM) of the Nd2Fe14 B-type hard magnetic phase with 20 vol% of α-Fe as soft magnetic phase. The extrusion temperature has important influence on magnetic properties and microstructure of magnetic materials. The results show that the grain size of Nd2Fe14B and α-Fe phase increases steadily with increasing extrusion temperature. Furthermore, optimal extrusion temperature of 1223 K occurs, at which the highest magnetic properties and relative density can be obtained.  相似文献   

17.
胡勇  闫红红  林涛  李金富  周尧和 《物理学报》2012,61(8):87102-087102
将Zr55Al10Ni5Cu30块体非晶合金在715 K等温退火30 min, 引入少量纳米晶, 然后于室温以不同的应变速率进行轧制, 用差示扫描量热仪考察不同应变量样品的热稳定性和自由体积演化. 结果表明:即使轧制到95%的最大应变量, 样品的热稳定性也几乎没有发生改变. 在各种应变速率下, 随着应变量的增加, 自由体积含量持续上升. 但随着应变速率的增加, 相同应变量下自由体积的含量先上升后降低, 该规律与单一非晶态结构合金在塑性变形过程中自由体积的变化情况截然不同.  相似文献   

18.
Rare-earth based metallic glasses with high saturation magnetization show a sizeable magnetocaloric effect (MCE) and are subject of extensive research concerning magnetic refrigeration materials. In this work, the magnetic phase transition from paramagnetic to ferromagnetic of Gd60Co30Al10 metallic glass has been characterized and three different methods were applied for the determination of its magnetocaloric specific parameters: (a) direct measurement of the adiabatic temperature change by exposing the material to an adiabatically applied magnetic field; (b) determination of the magnetization M(H,T) and calculation of the temperature dependent magnetic field induced entropy change ΔSm by application of the Maxwell relation and (c) measuring the total heat capacity Cp(H,T) in zero and non-zero magnetic field. Gd60Co30Al10 glassy ribbons were prepared by melt spinning, a technique that offers very high cooling rates due to the low dimensionality of the sample. Depending on the particular method of measurement, pieces of these glassy ribbons form samples with different appropriate total volume and dimensions. We show that the combination of the pronounced two-dimensionality of the ribbon pieces (aspect ratio ∼100) together with the very high magnetic permeability principally can cause strong internal demagnetizing fields that cannot be neglected when evaluating the intrinsic MCE parameters obtained from different methods.  相似文献   

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