TY - JOUR
T1 - Icosahedral-phase formation and stability in Ti-Zr-Co alloys
AU - Kim, W. J.
AU - Kelton, K. F.
PY - 1996/12
Y1 - 1996/12
N2 - We present the first report of icosahedral phase (i-phase) formation in rapidly quenched alloys of Ti53Zr27Co20Electron diffraction patterns of i(TiZrCo) contain features, such as anisotropic spot shapes and arcs of diffuse scattering, that are characteristic of the disordered icosahedral phases found in Ti-3d transition metal-Si-O and Ti-Zr-Fe alloys. The features are less prominent than in those alloys, however, suggesting that this i-phase may have structural order intermediate between those strongly disordered i-phases and more ordered Ti-Zr-Ni i-phases, showing none of these features. The quasilattice constant for i(TiZrCo), aq=0.51 nm, is close to that of i(TiZrNi). The i-phase in rapidly quenched Ti-Zr-Co alloys is deeply metastable and transforms exothermically to the hexagonal Laves phase about 500° C. The Laves phase transforms to the bcc solid solution phase (β -Ti) and the Ti2Ni-type fcc structure for T > 630° C. A reversible transformation between the β -Ti and the hexagonal solid solution phase (α-Ti) is observed on temperature cycling; the Ti2Ni-type fcc phase is stable over the entire temperature range.
AB - We present the first report of icosahedral phase (i-phase) formation in rapidly quenched alloys of Ti53Zr27Co20Electron diffraction patterns of i(TiZrCo) contain features, such as anisotropic spot shapes and arcs of diffuse scattering, that are characteristic of the disordered icosahedral phases found in Ti-3d transition metal-Si-O and Ti-Zr-Fe alloys. The features are less prominent than in those alloys, however, suggesting that this i-phase may have structural order intermediate between those strongly disordered i-phases and more ordered Ti-Zr-Ni i-phases, showing none of these features. The quasilattice constant for i(TiZrCo), aq=0.51 nm, is close to that of i(TiZrNi). The i-phase in rapidly quenched Ti-Zr-Co alloys is deeply metastable and transforms exothermically to the hexagonal Laves phase about 500° C. The Laves phase transforms to the bcc solid solution phase (β -Ti) and the Ti2Ni-type fcc structure for T > 630° C. A reversible transformation between the β -Ti and the hexagonal solid solution phase (α-Ti) is observed on temperature cycling; the Ti2Ni-type fcc phase is stable over the entire temperature range.
UR - https://www.scopus.com/pages/publications/0030381469
U2 - 10.1080/095008396179977
DO - 10.1080/095008396179977
M3 - Article
AN - SCOPUS:0030381469
SN - 0950-0839
VL - 74
SP - 439
EP - 448
JO - Philosophical Magazine Letters
JF - Philosophical Magazine Letters
IS - 6
ER -