MICROSTRUCTURE-BASED 3D FINITE-ELEMENT MODELING OF LATTICE MISFIT ANDLONG-RANGE INTERNAL-STRESSES IN CREEP-DEFORMED NICKEL-BASE SUPERALLOYSINGLE-CRYSTALS
H. Feng et al., MICROSTRUCTURE-BASED 3D FINITE-ELEMENT MODELING OF LATTICE MISFIT ANDLONG-RANGE INTERNAL-STRESSES IN CREEP-DEFORMED NICKEL-BASE SUPERALLOYSINGLE-CRYSTALS, Materials science & engineering. A, Structural materials: properties, microstructure and processing, 214(1-2), 1996, pp. 1-16
In the present paper, residual stresses and direction-dependent lattic
e parameters and lattice misfits in the gamma'-hardened, tensile creep
-deformed monocrystalline nickel-base superalloy SRR 99 have been stud
ied by three-dimensional finite element modelling based on a ''simplif
ied creep process''. The main results are as follows. (i) After creep
and cooling to room temperature, the internal strains and stresses in
both phases gamma and gamma' in the directions [001] (parallel to the
stress axis) and [100]/[010] are different. From these, differences be
tween the lattice parameters and lattice misfits in the [001] and the
[100]/[010] directions follow. During cooling to room temperature afte
r creep, the change in thermal stresses can cause plastic back flow of
the gamma-phase. The internal stress state is relaxed accordingly. (i
i) During the subsequent heating (after creep and cooling to room temp
erature), the differences of the lattice parameters in the [100] direc
tions decrease with increasing temperature. (iii) During final cooling
from a stress-free state at 105 degrees C, the lattice misfit and the
internal stresses between the [001] and the [100]/[010] directions in
crease with decreasing temperature. The influences of the creep-induce
d dislocation networks at the gamma/gamma' interfaces, of the coherenc
y stresses and of thermal stresses on the lattice misfit and internal
stresses are discussed in detail. The differences between the values o
f the lattice misfit measured by TEM and by X-ray diffraction are reco
nciled. The differences between two- and three-dimensional finite elem
ent modelling are also discussed. The results are in reasonable agreem
ent with the experimentally measured data.