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1.
通过成分设计得到Zr51Cu24.7Ni14.34Al9.96非品成分,可制备临界10 mm<Dmax<12 mm的非晶合金,其具有高的玻璃形成能力参数:Tg=728 K,Tx=790 K,T1=1174 K.玻璃形成能力判据Trg=0.707是迄今为止发现的Zr基非晶合金中最高值.从理论上证明了其具有高的玻璃形成能力...  相似文献   

2.
采用非等温差热扫描量热分析方法,研究了压力对Zr55Cu30Al10Ni5大块非晶合金玻璃转变的影响。用Kissinger方程计算其玻璃转变的表观激活能。实验表明:玻璃转变与加热速度有关,具有动力学效应。不同压力下,大块非晶合金在远低于玻璃转变温度等温退火后,其玻璃转变温度和玻璃转变表观激活能均呈现出非单调的变化。  相似文献   

3.
Cu47Ti34Zr11Ni8块体非晶合金的制备   总被引:2,自引:5,他引:2  
采用差压铸造法成功制备了圆棒状与板片状的Cu417Ti34Zr11Ni8块体非晶合金,研究了合金的热稳定性。在试验条件下,Cu47Ti34Zr11Ni8块体非晶合金棒状试样的最大直径可达3mm,板片状试样的最大厚度可达1mm。该成分块体非晶合金具有良好的热稳定性,其玻璃转变温度Tg=672K,晶化温度Txl=735K,过冷液相区△Tx=63K,约化玻璃温度Trg=0.575。  相似文献   

4.
采用低纯度的原料,通过电弧熔炼铜模铸造法制备了直径达10mm的Zr56.6Cu17.3Ni12.5Al9.6Ti4非晶合金圆棒.该合金玻璃转变温度tg=385.8℃,晶化温度tx=464.2℃,过冷液相区温差Δtx=78.4℃,约化玻璃温度trg(tg/tmL)=0.62.以基于DTA的合金凝固点偏移的方法确定该合金的临界冷却速度Rc=7.1℃/s,低于商业合金Vit.105合金的临界冷速(约为10℃/s).楔形试样对比结果显示:Zr56.6合金试样中的非晶组织区域明显大于Vit.105合金的,预示前者具有较好的实际玻璃形成能力.以上结果表明,Zr56.6Cu17.3Ni12.5Al9.6Ti4合金是Zr-Al-Ni-Cu-Ti系中玻璃形成能力最强的合金之一.  相似文献   

5.
反复熔炼对Zr基大块非晶合金玻璃形成能力的影响   总被引:3,自引:0,他引:3  
研究了反复熔炼对Zr60Al15Ni25和Zr65Al7.5Ni10Cu17.5合金的玻璃形成能力的影响。DSC分析表明,随着熔炼次数的增多,Zr60Al15Ni25非晶合金的玻璃转变温度和晶化开始温度都提高,而Zr60Al7.5Ni10Cu17.5非晶合金的特征温度基本没有发生变化。Zr60Al15Ni25合金的熔化焓由于反复熔炼而降低,在热力学上有利于非晶相的形成。根据反复熔炼对铸锭凝固组织进而对合金熔体中的短程序的影响,讨论了玻璃形成能力的变化及原子间的结合力对短程序尺寸的影响,分析了2种合金对反复熔炼处理的敏感性的不同。  相似文献   

6.
利用DSC、TGA试验手段研究了氧化对大块非晶合金Zr55Cu30Al10Ni5热稳定性的影响.结果表明,在氧气气氛下连续升温时,大块非晶合金的玻璃转变点消失;氧化速率在过冷液相区内明显加快,这源于在过冷液相区中原子的快速扩散;在玻璃转变温度上下温度作等温氧化处理对大块非晶合金的热稳定性没有明显影响.  相似文献   

7.
Sn对ZrTiNiCuAl非晶合金玻璃形成能力的影响   总被引:1,自引:4,他引:1  
研究了固溶元素Sn掺杂对Zr52.5Ti5Ni14.6Cu17.9Al10非晶合金玻璃形成能力(GFA)的影响,结果发现,掺杂不同含量的Sn会使玻璃化温度Tg,晶化温度Tx不同程度地向高温移动,但对合金熔化温度Tm温度不大。当Sn的摩尔分数为1.86%时,合金玻璃化温度Tg提高了17℃,晶化温度Tx提高了36℃,从而使△Tx提高了19℃,玻璃化温度与合金熔点温度的比值Trg由0.63提高到0.65分析了Sn元素对Tg,Tx及玻璃形成能力的影响。  相似文献   

8.
Zr55Al10Cu30Ni5-xPdx块状非晶合金的玻璃形成能力和热稳定性   总被引:2,自引:0,他引:2  
用铜模铸造方法制备了不同尺寸的Zr55Al10Cu30Ni5-xPdx(x=0,1,3,5)块状非晶合金,采用X射线衍射(XRD)、扫描差热分析(DSC)和透射电镜(TEM)分别为Zr55Al10Cu30Ni5-xPdx块状非晶样品的结构、热稳定性和微观组织进行了研究。结果表明:x=1时,合金具有最高的过冷液相区(高达100K)及最大的热稳定性,而对合金的玻璃形成能力影响不大,这说明用适量的Pd代表Zr55Al10Cu30Ni5合金中的Ni会提高合金的热稳定性;x=3时,合金的热稳定性有所提高,但降低了合金的玻璃形成能力;x=5时,非晶合金的热稳定性和玻璃形成能力同时降低。  相似文献   

9.
近年来已能用较低的冷却速度 (1~ 10 0K/s)直接由熔体制取厚度 10mm左右的高玻璃形成能力的大块非晶合金。这种大块非晶合金也具有在晶化前很宽的过冷液相区和高变形率超塑性以及在过冷液相状态优良的加工性。在 2 0 0 1年日本熊本大学解决了大块非晶合金材料的焊接问题 ,  相似文献   

10.
Zr55Al10Ni5Cu30大块非晶合金的超塑性挤压成形性能   总被引:8,自引:3,他引:8  
通过示差扫描量热分析确定了Zr55Al10Ni5Cu30大块非晶合金的过冷温度区域范围,采用应变速率突变压缩实验分析了合金在450℃时的力学性能,研究了合金在不同挤压速度、不同真空度等工艺条件下的挤压成形性能.结果表明:Zr55Al10Ni5Cu30大块非晶合金的玻璃化转变开始温度Tg为422.4℃,晶化开始温度Tx为482.4℃;在450℃、应变速率小于5×10-3s-1的条件下,合金的流动应力小于40 MPa在挤压速度为0.002~0.004mm/s范围内挤压时,合金的最大挤压载荷变化较小;在挤压温度为450℃时,合金的最大挤压力随着真空度(2~2×10-3Pa)的提高而增加;大块非晶合金在超塑性成形时呈现出比一般金属材料更大的摩擦阻力.  相似文献   

11.
Electron beam (EB) is becoming very popular for the modification of the surfaces as it involves localized melting and fast cooling which helps in achieving the non-equilibrium phases as well as fine microstructure. Surface modification of Zr-based amorphous alloy Zr55Cu30Al10Ni5 has been carried out by EB melting. Differential scanning calorimetry (DSC) was employed to determine the supercooled liquid region and activation energy of crystallization. The as-cast and modified surfaces of amorphous alloy at different beam conditions were characterized using X-ray diffraction (XRD), scanning electron microscopy (SEM) and energy dispersive spectroscopy (EDS) techniques. Various phases like NiZr2, CuZr2 and Cu10Zr7 were identified which resulted in the enhancement of hardness of the modified alloy surface.  相似文献   

12.
通过磁悬浮熔炼和铜模吸铸法制备直径3mm的(Zr0.55Al0.10Ni0.05Cu0.30)100-xFex(x=0,1,2,3,4)合金试样,研究Fe元素的微量添加对Zr55Al10Ni5Cu30块体金属玻璃非晶形成能力和力学性能的影响。研究表明,合理添加Fe元素(不超过3%,摩尔分数)导致约化玻璃转变温度Trg(=Tg/Tl)和参数γ(=Tx/(Tg+Tl))增大,因而其非晶形成能力增大,但添加过量的Fe元素(4%)会导致其非晶形成能力的降低。添加Fe元素也会显著地改善Zr55Al10Ni5Cu30块体金属玻璃的压缩塑性及提高其压缩断裂强度,当Fe元素的添加量为2%时,直径3mm、长度6mm的试样在压缩时出现一定的塑性及加工硬化现象。Fe元素添加量为4%形成的金属玻璃基复合材料,同样也显示良好的压缩塑性和高的压缩断裂强度。  相似文献   

13.
14.
将Zr52.5Cu17.9Ni14.6Al10Ti5(Vit105)块体非晶合金棒用水砂纸和抛光膏打磨到不同粗糙度,研究表面粗糙度对试样压缩变形行为的影响。结果表明,随着试样表面粗糙度的降低,屈服强度并没有明显变化,但压缩塑性从2.3%提高到4.5%。在扫描电镜下观察断裂试样的侧面发现,塑性越大的试样,剪切带的密度越大。因此,对于非晶合金,要得到较大的塑性,降低表面粗糙度是必要的。  相似文献   

15.
In the present study, fatigue tests were conducted on a zirconium-based bulk metallic glass (BMG), BMG-11 (Zr–10Al–5Ti–17.9Cu–14.6Ni, atomic percent), in air and vacuum to elucidate the possible environmental effects. In air, the fatigue endurance limit and the fatigue ratio were found to be 907 MPa and 0.53, respectively. These values are better than many conventional high-strength crystalline alloys. Unexpectedly, the fatigue lifetimes in vacuum were found to be lower than in air. Additional testing indicated that dissociation of residual water vapor to atomic hydrogen in the vacuum via a hot-tungsten-filament ionization gauge, and subsequent hydrogen embrittlement of the BMG-11, could have been a factor causing the lower fatigue lifetimes observed in vacuum.  相似文献   

16.
We present mechanical properties of monolithic bulk metallic glass (BMG) Zr62Al8Ni13Cu17 under uniaxial compression and tensile tests. It is found that the Zr62Al8Ni13Cu17 BMG exhibits pronounced plasticity of nearly 14% without catastrophic failure upon compression. However, it is destroyed under tension in a brittle manner. High energy X-ray diffraction has been used to detect the structural change in this BMG during both conditions. No deformation-induced nanocrystallization is detected in a 55% strained sample under compression while it only appears in the fracture-affected region upon tension. No excess free volume is obviously found in the fractured samples. We suggest that monolithic BMG alloys with small differences in atomic affinity and atomic sizes among components might have high plasticity under compression.  相似文献   

17.
In this work, a small amount of Mn was added to a Gd55Ni25Al20 glass forming alloy, as a replacement for Ni, and a Gd55Ni22Mn3Al20 bulk metallic glass (BMG) was obtained by suction casting. Its glass forming ability (GFA) was characterized by X-ray diffraction and differential scanning calorimetry, and its magnetic properties were measured using a magnetic property measurement system. It is found that the minor Mn addition can significantly improve both the GFA and the magnetocaloric effect (MCE) of the alloy. The refrigerant capacity (RC) of the BMG can reach a high value of 825 J kg−1 under a field of 3979 kA/m, which is about 29% larger than that of a Gd55Ni25Al20 BMG. The effect of the minor Mn addition on the GFA and MCE of the BMG was investigated in the study.  相似文献   

18.
采用差示扫描量热仪(DSC)和X射线衍射仪(XRD)研究Zr55Cu30Ni5Al10大块金属玻璃的非等温晶化转变动力学和在过冷液相区的等温晶化动力学行为。在非等温过程中,采用不同方法(Kissinger,Flynn-Wall-Ozawa和Augis-Bennett)得到的Zr55Cu30Ni5Al10大块金属玻璃平均激活能彼此之间吻合很好。此外,采用Johnson-Mehl-Avrami(JMA)模型描述Zr55Cu30Ni5Al10大块金属玻璃的等温转变动力学。研究结果表明:Zr55Cu30Ni5Al10大块金属玻璃的Avrami指数n介于2.2和2.9之间,表明其晶化机制主要是扩散控制过程。在等温晶化的过程中,晶核长大主要是三维的长程有序扩散控制的过程,平均激活能为469kJ/mol。  相似文献   

19.
The glass forming ability, thermal stability and non-isothermal crystallization kinetics of Zr63.5Al10.7Cu10.7Ni15.1 glass forming alloy were investigated. Its maximum glass forming dimension is up to 6 mm and its critical cooling rate is less than 40 K s−1. It manifests two crystallization procedures and the second crystallization peak is more sensitive to heating rate than the first crystallization peak. The glass transition and crystallization both have remarkable kinetics effects. The ms fitted by Arrhenius and VF equations are consistent with each other. Small m value about 17 indicates better thermodynamic stability and GFA of Zr63.5Al10.7Cu10.7Ni15.1.  相似文献   

20.
本文通过x射线衍射(XRD)、差示扫描量热法(DSC)和透射电子显微镜(TEM)研究了退火温度对Zr48Cu36Ag8Al8金属玻璃微观结构演化的影响。结果表明,快速凝固获得的样品为典型的非晶态结构。当样品在703K保温20分钟时,均一的非晶基体相分离成两种非晶合金,即,发生相分离。由于相分离结构与非晶基体在等温退火过程是竞争的关系,这个结构很容易向晶化态进行转变,形成AlZr2 AlAg3相。Zr48Cu36Ag8Al8金属玻璃的微观结构在过冷液相区等温退火过程中经历了的局部结构转变,相分离以及纳米晶转变,这个过程意味着Zr48Cu36Ag8Al8金属玻璃的微观结构对退火温度十分敏感。此外,相分离的形成可以加速纳米晶的形成。  相似文献   

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