TY - JOUR
T1 - Influence of growth direction on the microstructure of unidirectionally solidified Cu-Pb monotectic alloy using zone-melt technique
AU - Aoi, Ichiro
AU - Ishino, Makoto
AU - Yoshida, Makoto
AU - Fukunaga, Hideharu
AU - Nakae, Hideo
PY - 2001/2
Y1 - 2001/2
N2 - The influence of growth direction on the monotectic structure of the Cu-Pb alloy is studied. In order to examine the influence under a 1 g environment, both the upward (opposite to the direction of gravity) and downward (the direction of gravity) unidirectional solidifications (UDS) are carried out. In the case of the upward UDS, a banded structure, which consists of Pb-rich and Cu-rich layers, is observed. The L2 droplets pile up in front of the solid/liquid interface. On the other hand, in the downward UDS, the irregularly shaped L2 phase uniformly disperses in the specimen and no banded structure is found. The gravity macrosegregation of the L2 liquid is observed at the bottom of the molten alloy in the downward solidified specimen. This is caused by the difference in the density between the L1 and L2 phases. Furthermore, a mechanism for the formation of a banded structure is suggested. This mechanism suggests that the coalesced L2 phase covers the solid/liquid interface by producing a Pb-rich layer that permits an increase in the undercooling of the L1/L2 interface compared to the monotectic temperature. As nucleation of the α-Cu phase occurs on the Pb-rich layer, the coexisting three phases are then restored. The temperature at the growth front is also returned to the monotectic temperature. The repetition mentioned above will result in the banded structure found in the upward UDS.
AB - The influence of growth direction on the monotectic structure of the Cu-Pb alloy is studied. In order to examine the influence under a 1 g environment, both the upward (opposite to the direction of gravity) and downward (the direction of gravity) unidirectional solidifications (UDS) are carried out. In the case of the upward UDS, a banded structure, which consists of Pb-rich and Cu-rich layers, is observed. The L2 droplets pile up in front of the solid/liquid interface. On the other hand, in the downward UDS, the irregularly shaped L2 phase uniformly disperses in the specimen and no banded structure is found. The gravity macrosegregation of the L2 liquid is observed at the bottom of the molten alloy in the downward solidified specimen. This is caused by the difference in the density between the L1 and L2 phases. Furthermore, a mechanism for the formation of a banded structure is suggested. This mechanism suggests that the coalesced L2 phase covers the solid/liquid interface by producing a Pb-rich layer that permits an increase in the undercooling of the L1/L2 interface compared to the monotectic temperature. As nucleation of the α-Cu phase occurs on the Pb-rich layer, the coexisting three phases are then restored. The temperature at the growth front is also returned to the monotectic temperature. The repetition mentioned above will result in the banded structure found in the upward UDS.
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U2 - 10.1016/S0022-0248(00)01008-3
DO - 10.1016/S0022-0248(00)01008-3
M3 - Article
AN - SCOPUS:0035250984
SN - 0022-0248
VL - 222
SP - 806
EP - 815
JO - Journal of Crystal Growth
JF - Journal of Crystal Growth
IS - 4
ER -