Glass-forming ability and crystallization behavior of Nd60Al10Ni10Cu20−xFex (x = 0, 2, 4) bulk metallic glass with distinct glass transition

2004 ◽  
Vol 385 (1-2) ◽  
pp. 38-43 ◽  
Author(s):  
Z. Zhang ◽  
W.H. Wang ◽  
Y. Hirotsu
2003 ◽  
Vol 18 (10) ◽  
pp. 2288-2291 ◽  
Author(s):  
H. Ma ◽  
E. Ma ◽  
J. Xu

We report a new Mg-based bulk metallic glass-forming alloy: Mg65Cu7.5Ni7.5Zn5 Ag5Y10. The alloy exhibits a glass-forming ability significantly stronger than all previously discovered Mg-based glass formers. Fully glassy rods 9 mm in diameter can be obtained by using copper mold casting. The critical cooling rate for glass formation was estimated to be <50 Ks−1. The reduced glass-transition temperature (Trg) of the glass was determined to be 0.59.


2002 ◽  
Vol 754 ◽  
Author(s):  
Hao Chen ◽  
Mahadevan Khantha ◽  
Takeshi Egami

ABSTRACTMolecular Dynamics simulation was carried out to study the glass transition and crystallization in the metal-metalloid binary system with pair-wise potentials. The results show that a repulsive potential between metalloid (small) atoms increases the glass forming ability. The observation is consistent with the recent theory of bulk metallic glass formation through local glass transition and nano-glass formation. The theory predicted that the compositional short-range order (CSRO) prevents the small atom pairing so as to increase the glass forming ability (GFA). The present results demonstrate the important role of CSRO in bulk metallic glass formation.


2007 ◽  
Vol 539-543 ◽  
pp. 2071-2076 ◽  
Author(s):  
Tohru Yamasaki ◽  
S. Maeda ◽  
Daisuke Okai ◽  
Takeshi Fukami ◽  
Yokoyama Yoshihiko ◽  
...  

Viscosity of a Zr55Cu30Al10Ni5 supercooled liquid alloy having bulk metallic glass forming ability has been measured by using a penetration viscometer with a cylindrical probe under high speed heating conditions at rates between 20°C/min and 400°C/min in the temperature range from the glass transition temperatures (Tg) up to above the crystallization temperatures (Tx). The viscosity of the alloy decreased with increasing the heating rate and tended to saturate at the heating rate of 200°C/min and above. Corresponding measurements of the differential thermal calorimetry (DSC) under the high-speed heating conditions have been also done.


1996 ◽  
Vol 455 ◽  
Author(s):  
Ralf Busch ◽  
Andreas Masuhr ◽  
Eric Bakke ◽  
William L. Johnson

ABSTRACTThe viscosities of the Zr46.75Ti8.25Cu7.5Ni10Be27.5 and the Zr41.2Ti13.8Cu12.5Ni10Be22.5 bulk metallic glass forming liquids was determined from the melting point down to the glass transition in the entire temperature range of the supercooled liquid. The temperature dependence of the viscosity in the supercooled liquid obeys the Vogel-Fulcher-Tammann (VFT) relation. The fragility index D is about 20 for both alloys and the ratio between glass transition temperature and VFT temperature is found to be 1.5. A comparison with other glass forming systems shows that these bulk metallic glass formers are strong liquids comparable to sodium silicate glass. Furthermore, they are the strongest among metallic glass forming liquids. This behavior is a main contributing factor to the glass forming ability since it implicates a higher viscosity from the melting point down to the glass transition compared to other metallic liquids. Thus, the kinetics in the supercooled liquid is sluggish and yields a low critical cooling rate for glass formation. The relaxation behavior in the glass transition region of the alloys is consistent with their strong glassy nature as reflected by a stretching exponent that is close to 0.8. The microscopic origin of the strong liquid behavior of bulk metallic glass formers is discussed.


2019 ◽  
Vol 6 (6) ◽  
pp. 065202 ◽  
Author(s):  
Majid Samavatian ◽  
Reza Gholamipour ◽  
Vahid Samavatian ◽  
Fahimeh Farahani

2014 ◽  
Vol 29 (10) ◽  
pp. 1217-1222 ◽  
Author(s):  
Chuntao Chang ◽  
Jianhua Zhang ◽  
Baolong Shen ◽  
Weihua Wang ◽  
Akihisa Inoue

Abstract


2014 ◽  
Vol 125 ◽  
pp. 151-153 ◽  
Author(s):  
H.Y. Ding ◽  
Y. Shao ◽  
P. Gong ◽  
J.F. Li ◽  
K.F. Yao

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