The dislocation structure of a single-crystal gamma+gamma ' two-phase alloy after tensile deformation

Citation
Zp. Luo et al., The dislocation structure of a single-crystal gamma+gamma ' two-phase alloy after tensile deformation, MATER CHAR, 43(5), 1999, pp. 293-301
Citations number
16
Categorie Soggetti
Material Science & Engineering
Journal title
MATERIALS CHARACTERIZATION
ISSN journal
10445803 → ACNP
Volume
43
Issue
5
Year of publication
1999
Pages
293 - 301
Database
ISI
SICI code
1044-5803(199911)43:5<293:TDSOAS>2.0.ZU;2-A
Abstract
The dislocation structures of an industrial single-crystal gamma + gamma' t wo-phase alloy DD3 after tensile deformation from room temperature to 1273K were studied by transmission electron microscopy. The strength of this all oy decreased with an increase in the temperature, and showed a strength pea k at 1033K. At room temperature, the dislocations shearing the gamma partic les were found to be 1/3[112] partial dislocations on the dodecahedral slip system [112]{111}. Some dislocation pairs on the cubic [110]{100} system t hat blocked the glide of dislocations were found at a medium temperature of 873K. As a result, dislocation bands were formed. Shearing of gamma' parti cles by 1/3[112] partial dislocations on the dodecahedral slip system [112] {111} was also found at this temperature. At the peak temperature of 1033K, because of the strong interaction between dislocations on the {111} and {1 00} planes, the extent of dislocation bands with high dislocation densities was extensive. The 1/3[112] partial dislocations on the dodecahedral slip system [112]{111} also existed. When the temperature reached the high tempe rature of 1133K, the range of dislocation bands was limited. The gamma' par ticles were sheared by [110] dislocation pairs on the octagonal [110]{111} system and the cubic [110]{100} system. At 1273K, the regular hexagonal dis location networks were formed in the gamma matrix and at the gamma/gamma' i nterface. The Burgers vectors of the network were found to be b(1) = 1/2[11 0], b(2) = 1/2[1-10], b(3) = [100], and the last one was formed by the reac tion of b(1) + b(2) --> b(3). Dislocations shearing the gamma' particles we re found to be [110] dislocation pairs on the octagonal system [110]{111} a nd cubic slip system [110]{100} at 1273K. (C) Elsevier Science Inc., 1999. All rights reserved.