scholarly journals On Welch-Gong Transformation Sequence Generators

Author(s):  
G. Gong ◽  
A. M. Youssef
2019 ◽  
Vol 780 ◽  
pp. 743-748
Author(s):  
Cheng Liu ◽  
Lei Jin ◽  
Fang-Zu Yang ◽  
Zhong-Qun Tian

2016 ◽  
Vol 113 ◽  
pp. 75-78 ◽  
Author(s):  
C.M. Koller ◽  
A. Kirnbauer ◽  
R. Rachbauer ◽  
S. Kolozsvári ◽  
P.H. Mayrhofer

2000 ◽  
Vol 48 (4) ◽  
pp. 933-941 ◽  
Author(s):  
Th Hentschel ◽  
D Isheim ◽  
R Kirchheim ◽  
F Müller ◽  
H Kreye

2014 ◽  
Vol 62 (4) ◽  
pp. 406 ◽  
Author(s):  
Dueng-Yuan Hueng ◽  
Yung-Sheng Cheng ◽  
Chin Lin ◽  
Yen-Po Cheng ◽  
Yi-Lin Yu ◽  
...  

2010 ◽  
Vol 146-147 ◽  
pp. 1477-1481 ◽  
Author(s):  
An Hui Cai ◽  
Wei Ke An ◽  
Xiao Song Li ◽  
Yun Luo ◽  
Tie Lin Li

The influence of Zr on the property of Cu(50+x)Zr(40-x)Ti10 (0≤x≤30 at.%) alloys were investigated. The results show that the maximum size for the glass formation in this Cu-Zr-Ti system is less than 8 mm. The hardness increases with decreasing of the Zr content, then decreases when the Zr content exceeds 10~15 at.% due to the obvious alteration of the type of the crystalline phases and the microstructure. With decreasing of the Zr content, the transformation sequence of the main Cu-Zr phase is Cu10Zr7→Cu5Zr→Cu51Zr14; the transformation sequence of Cu-Ti phase is Cu4Ti3→CuTi→CuTi3. In addition, the atom ratio of Cu60Zr30Ti10 alloys is coherent with that of their corresponding crystalline phase, resulting in its better glass forming ability.


2006 ◽  
Vol 385-386 ◽  
pp. 555-557 ◽  
Author(s):  
Nobuo Tezuka ◽  
It-Meng Low ◽  
Ian J. Davies ◽  
Michael Prior ◽  
Andrew Studer

1994 ◽  
Vol 364 ◽  
Author(s):  
G. Shao ◽  
P. Tsakiropoulos ◽  
A. P. Miodownik

AbstractThe microstructures in arc melted ingots and melt spun ribbons have been investigated by electron microscopy and thermodynamic modelling has been used to study the phase transformations. In the ingot, solidification starts with the bcc β phase and at room temperature the structure consists of B2, ωordered, γ and α2 phases. The calculated equilibrium phase transformation sequence during cooling is L → L+ β→β→β + α→β2+α → α+β2+γ → α2+γ + B2. The phase transformation sequence is dramatically changed by rapid quenching from the melt. Athermal ordered w phase is formed in metastable B2 and the α→α2 ordering process is completely suppressed in the melt spun ribbons. The volume fraction of the α precipitates is also dependent on cooling rates.


2005 ◽  
Vol 80 (10) ◽  
pp. 2677-2680 ◽  
Author(s):  
Altaf H. Carim ◽  
Gregory S. Rohrer ◽  
Neal R. Dando ◽  
Shih-Ying Tzeng ◽  
Cathy L. Rohrer ◽  
...  

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