Structure and crystallography of directionally solidified Al2O3—ZrO2—Y2O3 eutectic by the floating zone melting method

1986 ◽  
Vol 5 (2) ◽  
pp. 150-152 ◽  
Author(s):  
J. Echigoya ◽  
Y. Takabayashi ◽  
H. Suto ◽  
M. Ishigame
2001 ◽  
Vol 294 (1-2) ◽  
pp. 202-205 ◽  
Author(s):  
Yuji Arita ◽  
Satoshi Mitsuda ◽  
Yoshimasa Nishi ◽  
Tsuneo Matsui ◽  
Takanori Nagasaki

2005 ◽  
Vol 475-479 ◽  
pp. 745-748 ◽  
Author(s):  
X.P. Guo ◽  
Ping Guan ◽  
X. Ding ◽  
Jun Zhang ◽  
K. Kusabiraki ◽  
...  

The directionally solidified specimens of Nb-13.52 Si-22.60 Ti–6.88 Hf–2.54 Cr–2.24 Al alloy were prepared in an electron beam floating zone melting furnace at the withdrawing rate of 0.1, 0.3, 0.6, 1.0, 2.4 and 6.0 mm/min. All the primary Nb solid solution (Nbss) columns, Nbss + (Nb)3Si/(Nb)5Si3 eutectic colonies and divorced (Nb)3Si/(Nb)5Si3 plates or chains align well along the longitudinal axis of the specimens. With increasing of the withdrawing rate, the microstructure is gradually refined, and the amount of Nbss + (Nb)3Si/(Nb)5Si3 eutectic colonies increases. Both the room temperature ultimate tensile strength σb and fracture toughness KQ are improved for the directionally solidified specimens. The tensile fracture occurs in a cleavage way.


Author(s):  
Naoki Date ◽  
Shunya Yamamoto ◽  
Yoshimi Watanabe ◽  
Hisashi Sato ◽  
Shizuka Nakano ◽  
...  

AbstractIn this study, the effects of solidification conditions on the grain refinement capacity of heterogeneous nuclei TiC in directionally solidified Ti6Al4V alloy were investigated using experimental and numerical approaches. Ti6Al4V powder with and without TiC particles in a Ti6Al4V sheath was melted and directionally solidified at various solidification rates via the floating zone melting method. In addition, by using the phase field method, the microstructural evolution of directionally solidified Ti6Al4V was simulated by varying the temperature gradient G and solidification rate V. As the solidification rate increased, the increment of the prior β grain number by TiC addition also increased. There are two reasons for this: first, the amount of residual potent heterogeneous nuclei TiC is larger. Second, the amount of TiC particles that can nucleate becomes larger. This is because increasing the constitutional undercooling ΔTc leads to the activation of a smaller radius of heterogeneous nuclei and a higher nucleation probability from each radius. At a cooling rate R higher than that in the floating zone melting experiment (R = 3 to 1000 K/s), the maximum degree of constitutional undercooling ΔTc,Max has a peak value, which suggests that constitutional undercooling ΔTc has a smaller contribution at higher cooling rates, such as those that occur during electron beam melting (EBM), including laser powder bed fusion (LPBF).


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