TY - JOUR
T1 - Creep Behavior of Ti6Al4Nb4Zr Fabricated by Powder Bed Fusion Using a Laser Beam
AU - Yamabe-Mitarai, Yoko
AU - Inoue, Takashi
AU - Kuroda, Tomoki
AU - Matsunaga, Sae
AU - Toda, Yoshiaki
AU - Matsunaga, Tetsuya
AU - Ito, Tsutomu
AU - Ozasa, Ryosuke
AU - Ishimoto, Takuya
AU - Nakano, Takayoshi
N1 - Publisher Copyright:
©2023 The Japan Institute of Metals and Materials.
PY - 2023
Y1 - 2023
N2 - Powder bed fusion using a laser beam (PBF-LB) was performed for Ti6Al4Nb4Zr (mass%) developed by our group to improve the oxidation resistance at temperatures greater than 600°C by adding Nb and Zr to near-α alloys. Microstructure evolution of the PBF-LB samples by heat treatment was investigated, especially for heat treatment duration in the α + β phase, cooling rate, and heat treatment in the β phase. The equiaxed α phase formed during heat treatment along the melting-pool boundaries. The high volume fraction of the α phase and high Nb contents in the β phase was obtained by slow cooling (furnace cooling) compared with fast cooling (air cooling). The α/β lamellar structure formed in the melting pool boundaries with 100μm in size and no equiaxed α phase formed along the boundaries by heat treatment in the β phase regime. Creep life at 600°C and 137 MPa was similar for the air-cooled and furnace-cooled samples, but the slightly slower deformation was obtained in the furnace-cooled sample. Creep life of the sample in the β phase region drastically increased due to the absence of the equiaxed α phase. Dominant deformation mechanism of creep was grain boundary sliding. The small equiaxed α phase accelerated grain boundary sliding.
AB - Powder bed fusion using a laser beam (PBF-LB) was performed for Ti6Al4Nb4Zr (mass%) developed by our group to improve the oxidation resistance at temperatures greater than 600°C by adding Nb and Zr to near-α alloys. Microstructure evolution of the PBF-LB samples by heat treatment was investigated, especially for heat treatment duration in the α + β phase, cooling rate, and heat treatment in the β phase. The equiaxed α phase formed during heat treatment along the melting-pool boundaries. The high volume fraction of the α phase and high Nb contents in the β phase was obtained by slow cooling (furnace cooling) compared with fast cooling (air cooling). The α/β lamellar structure formed in the melting pool boundaries with 100μm in size and no equiaxed α phase formed along the boundaries by heat treatment in the β phase regime. Creep life at 600°C and 137 MPa was similar for the air-cooled and furnace-cooled samples, but the slightly slower deformation was obtained in the furnace-cooled sample. Creep life of the sample in the β phase region drastically increased due to the absence of the equiaxed α phase. Dominant deformation mechanism of creep was grain boundary sliding. The small equiaxed α phase accelerated grain boundary sliding.
KW - creep
KW - deformation mechanism
KW - heat treatment
KW - heat-resistant Ti alloys
KW - selective laser melting
UR - http://www.scopus.com/inward/record.url?scp=85161699785&partnerID=8YFLogxK
U2 - 10.2320/matertrans.MT-ME2022010
DO - 10.2320/matertrans.MT-ME2022010
M3 - 学術論文
AN - SCOPUS:85161699785
SN - 1345-9678
VL - 64
SP - 1175
EP - 1182
JO - Materials Transactions
JF - Materials Transactions
IS - 6
ER -