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1.
用动态DSC方法研究了预退火对超微晶Fe73.5Cu1Nb3Si13.5B9稳定性的影响.经过预退火处理后与制备态相比可提高合金的晶化温度TX、放热峰值温度TP和晶化激活能θK,从而可提高超微晶合金的稳定性。经510℃预处理后合金的晶化激活能可由制备态的380kJ/mol提高到500kJ/mol.  相似文献   

2.
用霍普金森效应及X射线研究了铁基超微晶合金Fe73.5Cu1Nb8Si18.5B9的居里温度和晶化过程。合金在500℃退火1h开始出现晶化相。随着退火温度的升高,晶化相的居里点由500℃上升到570℃。同时,剩余非晶基体的居里点也发生变化。  相似文献   

3.
超微晶合金Fe73.5Cu1Nb3Si13.5B9晶化过程的X射线研究   总被引:2,自引:1,他引:2  
用X射线衍射方法研究了超微晶合金Fe73.5Cu1Nb3Si13.5B9在退火过程中晶化相及晶格常数的变化。经480℃×1h退火后,合金中出现bccFe(Si)相,600℃出现Fe3B相,670℃出现Fe23B6相。退火温度升高时,Fe(Si)相的晶格常数由0.2838nm上升到0.2849nm合金经过550℃×4h退火后仍只有Fe(Si)一个晶化相,其晶格常数随时间的变化不明显。  相似文献   

4.
FeCuNbSiB合金的纳米晶化过程研究   总被引:4,自引:0,他引:4  
郑裕芳  余正方 《金属功能材料》1997,4(4):159-161,182
应用X射线衍射分析和穆斯堡尔谱学研究了Fe73.5Cu1Nb3Si13.5B9非晶合金的纳米晶化过程.Fe73.5Cu1Nb3Si13.5B9合金在500~600℃温度范围内分别退火1h,可形成纳米DO3结构的FeSi相和剩余非晶相。随着退火温度的升高,有更多的FeSi相析出。在500℃等温退火中FeCuNbSiB合金出现二阶段纳米晶化过程。  相似文献   

5.
用X射线衍射方法研究了超微晶合金Fe78.5Cu1Nb3Si18B9在退火过程中晶化相及晶格常数的变化。经480℃×1h退火后,合金中出现bccFe(Si)相,600℃出现Fe3B相,670℃出现Fe23B6相。退火温度升高时,Fe(Si)相的晶格常数由0.2838nm上升到0.2849um。合金经过550℃×4h退火后仍只有Fe(Si)一个晶化相,其晶格常数随时间的变化不明显。  相似文献   

6.
超微晶合金Fe73.5Cu1Nb3Si13.5B9晶化相的电镜观察及能谱分析   总被引:2,自引:1,他引:2  
用透射电镜和能谱仪分析了Fe73.5Cu1Nb3.Si13.5B9合金经不同温度退火后的组织,晶化相结构以及不同晶化相中的各元素含量变化,合金于450℃退火1h析出尺寸小于5nm的bccFe(Si)相,并且其尺寸随退火温度的升高而增大到约15min,于600℃退火时合金中析了四方结构的Fe3B相,其晶格常数为a=0.878nm,c=0.439nm在700℃退火时出现面心立结构的Fe23B6相,其晶  相似文献   

7.
测定了Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9合金的单辊快淬制备态条带及其经热处理后的室温透射Mssbauer谱.制备态谱为典型非晶展宽六线谱,其内磁场平均值Hi=17.01MA/m.在N_2气氛保护下经480℃退火0.5h已有明显结构弛豫或部分晶化发生;530℃退火1h后样品已显著晶化,其主要组成为α-Fe(Si)固溶体纳米晶和剩余非晶相,后者约占39.1%,并随退火温度升高而减少,至620℃退火后约为25%.非晶相的Hi值在结构弛豫阶段稍有上升,而在显著晶化温度以上则随温度升高而减小.在550℃退火样品中存在不同取向的体相磁织构.  相似文献   

8.
白魁昌  江自应 《金属学报》1994,30(2):B066-B071
测定了Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9合金的单辊快淬制备态条带及其经热处理后的室温透射Mssbauer谱.制备态谱为典型非晶展宽六线谱,其内磁场平均值Hi=17.01MA/m.在N_2气氛保护下经480℃退火0.5h已有明显结构弛豫或部分晶化发生;530℃退火1h后样品已显著晶化,其主要组成为α-Fe(Si)固溶体纳米晶和剩余非晶相,后者约占39.1%,并随退火温度升高而减少,至620℃退火后约为25%.非晶相的Hi值在结构弛豫阶段稍有上升,而在显著晶化温度以上则随温度升高而减小.在550℃退火样品中存在不同取向的体相磁织构.  相似文献   

9.
测定了Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9合金的单辊快淬制备态条带及其经热处理后的室温透射Mssbauer谱.制备态谱为典型非晶展宽六线谱,其内磁场平均值Hi=17.01MA/m.在N_2气氛保护下经480℃退火0.5h已有明显结构弛豫或部分晶化发生;530℃退火1h后样品已显著晶化,其主要组成为α-Fe(Si)固溶体纳米晶和剩余非晶相,后者约占39.1%,并随退火温度升高而减少,至620℃退火后约为25%.非晶相的Hi值在结构弛豫阶段稍有上升,而在显著晶化温度以上则随温度升高而减小.在550℃退火样品中存在不同取向的体相磁织构.  相似文献   

10.
刘涛  郭应焕 《金属学报》1995,31(4):B159-B163
用丰电子湮没技术和微观磁学方法研究了纳米晶Fe73.5Cu1nb3Si13.5B9合金结构缺陷在退火过程中的变化规律,表明晶化初期形成的界面结构只引入少量的缺陷,晶化后期由于出现大量晶界,缺陷浓度急剧上升;非晶制备过程中以及晶化时引入的准位错偶极子造成的应力场对其软磁性能有很大的影响,并可以解释在最佳退火温度的磁性行为。  相似文献   

11.
The magnetic properties and the crystallization and its influence on the magnetic and struc-tural properties for rapidly quenched amorphous Nd_6Fe_(81)B-(13) alloy have been studied.The lowtemperature magnetic properties,the Curie temperature and the crystallization behavior arediscussed.A small addition(6at.-%)of Nd in amorphous Fe-B alloys increases largely thecrystallization temperature T_x but causes a decrease of the Curie temperature Tc·A newphase was observed in the sample annealed at 873 K.  相似文献   

12.
In the view of crystallization activation energy of amorphous alloy,the mechanism of coarse grain in annealed Sm5Fe80Cu1Si5B3C2.5ZR3.5 amorphous alloy was analyzed.It reveals the e4ffect of preannealing on the process crystallization.The results show that preannealing can be used to change the crystallization behavior of the α-Fe phase in the Sm5Fe80Cu1Si5B3C2.5Zr3.5 amorphous alloy,whick is helpful for forming α-Fe phase grains;and it is not large for Sm2Fe17Cx phase.  相似文献   

13.
采用快速凝固粉末冶金技术制备热挤压Mg_(80)Cu_(10)Y_(10)合金棒材,研究了快速凝固Mg_(80)Cu_(10)Y_(10)合金薄带及热挤压后合金的相结构,并对热处理工艺对合金棒材组织结构及力学性能的影响进行了分析.研究表明,采用单辊快速凝固法在辊速为1800 r/min下制备的Mg_(80)Cu_(10)Y_(10)合金薄带为完全非晶态;在热挤压过程中Mg_(80)Cu_(10)Y_(10)合金中有Mg_2Cu和Mg晶体相析出,其显微硬度比薄带有所提高,这与合金中细小Mg_2Cu颗粒的弥散析出有关;在450 ℃保温4 h后的热挤压Mg_(80)Cu_(10)Y_(10)合金中没有新相析出;随着热处理温度的升高或保温时间的延长,由于Mg_2Cu颗粒出现重溶及聚集长大现象,使得热挤压Mg_(80)Cu_(10)Y_(10)合金的显微硬度表现出逐渐下降的变化趋势.  相似文献   

14.
The causes of changes in the magnetic properties of an amorphous Co–Ni–Fe–Cr–Si–B alloy obtained by melt spinning in the form of a thin ribbon subjected to heat treatment and subsequent action of temperatures corresponding to various conditions of its exploitation have been analyzed. We have established the regimes of heat treatment that provide for the highest values of the maximum magnetic permeability of the alloy and the shielding factor of a magnetic shield made from the alloy. We have analyzed changes in the magnetic properties, shielding properties, and total magnetization distribution in an alloy ribbon at a temperature well below the crystallization temperature. We have found the temperature ranges that determine the practical application of this alloy.  相似文献   

15.
《Intermetallics》2006,14(8-9):1085-1090
Differential scanning calorimetry (DSC), X-ray diffraction (XRD) and transmission electron microscopy (TEM) were used as the main method to investigate the effect of relaxation on the glass transition and crystallization of Cu47Ti33Zr11Ni8Si1 metallic glass powders. The preannealing treatments were performed at temperatures close to the experimentally determined glass transition temperature. It was found that the thermal stability is profoundly affected by preannealing since the crystallization temperature is strongly influenced by preannealing and decreases with increase in preannealing temperature. In contrast, the annealing treatment does not change the glass transition temperature. During heat treatment at temperatures around the calorimetric glass transition temperature, Tg, the glassy powder undergoes microstructural alterations as revealed by TEM but not discernible by XRD. Fine nanocrystals of about 4–6 nm homogeneously dispersed in an amorphous matrix are observed by TEM after annealing at 698 K for 60 min. Kissinger analysis reveals that the preannealing decreases the activation energy for nanocrystallization thereby promoting partial crystallization of the glass.  相似文献   

16.
This study deals with the Fe65.5Cr4Mo4Ga4P12C5B5.5 ferromagnetic bulk amorphous alloy. XRD analysis showed an amorphous structure of the as-cast sample. The same method revealed that, after annealing at 973 K for τ=10 min, the sample displayed a crystalline structure with crystalline phases formed. The crystallization process of the alloy was examined by DTA analysis. It was shown that crystallization took place in the temperature range between 810 K and 860 K with the exo-maximum peak temperature at 846 K with a heating rate of 20 K·min-1. The method also showed that, at temperatures ranging from 753 K to 810 K, the alloy exhibited the properties of supercooled liquids. A correlation between heat-induced structural changes and magnetic properties of the alloy was determined by thermomagnetic measurements. Maximum magnetization M=3.7 Am2·kg-1 of the alloy was reached after its annealing at 733 K for τ=10 min. Upon annealing, the alloy exhibited a relaxed amorphous structure. Annealing the alloy above the crystallization temperature led to a decrease in bulk magnetization. After annealing at 973 K for τ=10 min, the bulk magnetization of the alloy was M'=0.45 Am2·kg-1. Accordingly, after crystallization and formation of new compounds, the magnetization of the alloy was decreased by a factor of about 7.7. The strength of the magnetic field applied during the measurements was H=10 k A·m-1. The samples were tested for changes in the microstructure and hardness of both the amorphous phase and the resulting crystalline phase.  相似文献   

17.
对Zr57Cu15.4Ni12.6Al10Nb5块体非晶合金进行了等温热处理,用X射线衍射仪、扫描电镜、显微硬度计与压缩试验机研究了不同温度下的等温热处理后合金的组织结构变化、硬度变化与压缩性能变化。该非晶合金出现晶化的温度随热处理时间的增长而降低。在热处理时间相同的条件下,随热处理温度升高,合金的显微硬度有增大趋势。当非晶合金出现相分离或晶化时,其抗压缩强度将急剧下降,断裂方式由非晶态的断裂方式向晶态的断裂方式转变。  相似文献   

18.
利用铜模铸造法制备了(La0.6Ce0.4)65Al10Cu25块体非晶合金,并在其过冷液相区内不同温度下,采用不同压力对该非晶合金进行加压退火处理,通过X射线衍射仪和差示扫描量热法研究了加压退火处理对该非晶合金晶化行为及热稳定性的影响。结果表明,加压退火促进了(La0.6Ce0.4)65Al10Cu25非晶合金的晶化过程,使得晶化初始温度Tx降低(dTx/dP=-5.17K/GPa),晶化激活能Ep随退火压力的增加而增大,并从能量和化学短程序畴的角度解释了加压退火对(La0.6Ce0.4)65Al10Cu25非晶合金晶化过程的影响机理。  相似文献   

19.
采用熔体快淬法制备(FeCo)78Nb6B15Cu1非晶薄带,通过DSC测试薄带的晶化特性,并据此在400,500,700和750℃进行1h退火处理。用XRD和SEM分析薄带在不同退火温度下的晶化行为,并用VSM测试薄带与粉体的静态磁参数。结果表明:对于固定成分的Hitperm合金,选择合适的退火温度,可控制晶粒大小和晶相比例。由于晶粒表面无序磁矩含量的变化,导致材料比饱和磁化强度发生变化,同时更小的纳米晶粒对降低矫顽力有利。由于淬态引入的微量结晶,薄带存在表面晶化现象,这在一定程度上会恶化材料的静态磁特性。  相似文献   

20.
Mg_(80)Cu_(15)Y_5合金的非晶形成能力及晶化行为   总被引:1,自引:0,他引:1  
采用单辊快速凝同法制备出厚约40μm的Mg_(80)Cu_(15)Y_5非品合金薄带,利用XRD、DSC、TEM和HRTEM研究了非品合金的非品形成能力和晶化行为,分析了品化对合金组织结构与性能的影响.结果表明:Mg_(80)Cu_(15)Y_5合金的过冷液态温度区间△T_x和约化玻璃转变温度T_(rg)分别为55K和0.58,表明其具有较强的非晶形成能力;该合金在退火温度高于473 K后发牛明显晶化,从非品基体中析出 Mg_2Cu、Cu_2Y和Mg晶体相;随着退火温度的升高,合金的硬度呈现出先升高后降低的变化趋势,这与纳米品体相颗粒的弥散析出、重溶及粗化有关.  相似文献   

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