M. Grujicic et P. Dang, A MOLECULAR-DYNAMICS STUDY OF TRANSFORMATION TOUGHENING IN THE GAMMA-TIAL BETA TI-V SYSTEM/, Materials science & engineering. A, Structural materials: properties, microstructure and processing, 219(1-2), 1996, pp. 109-125
The materials evolution in a region surrounding the crack tip was carr
ied out using molecular dynamics simulations for the case of a crack i
n the gamma TiAl phase impinging at the right angle onto the interface
between a gamma TiAl phase and a metastable Ti-15V (at.%) phase. The
corresponding linear anisotropic continuum solutions for the singular
stress and displacement fields were developed using an enriched finite
element method. These solutions were used to both generate the initia
l crack and to prescribe the boundary conditions applied to the comput
ational atomistic crystal during the molecular dynamics simulation run
s. The atomic interactions were described in terms of the appropriated
embedded atom method (EAM) type interatomic potentials. The crack-tip
behavior for the two-phase gamma/beta material was ultimately compare
d with the one in the corresponding single phase gamma and single phas
e beta materials. The simulation results showed that under the same ap
plied level of external stress, the crack tip becomes blunted and the
crack stops propagating in the gamma TiAl/beta Ti-15V bicrystal and in
the single beta-phase crystal while the crack extends by brittle clea
vage in the single-phase gamma crystal. The blunting process was found
to be controlled by the martensitic transformation which takes place
in the beta phase ahead of the crack tip. Depending on the local stres
s conditions, which are significantly affected by the presence of inte
rfacial dislocations, the crystal structure of martensite was found to
be either close packed hexagonal, body centered orthorhombic and/or f
ace centered orthorhombic. Finally, the implications of crack tip mart
ensitic transformation on materials toughness are analyzed in quantita
tive terms using the concept of the Eshelby's conservation integral, i
.e. the energy release rate.