Gj. Shiflet et Jh. Vandermerwe, THE ROLE OF STRUCTURAL LEDGES AT PHASE BOUNDARIES .2. FCC-BCC INTERFACES IN NISHIYAMA-WASSERMAN ORIENTATION, Acta metallurgica et materialia, 42(4), 1994, pp. 1189-1198
The ledge mode of misfit accommodation was first postulated for bounda
ries between b.c.c. and f.c.c. metal phases; the interfaces being {111
} f.c.c.-{110} b.c.c. planes and relative orientations varying from Ni
shiyama-Wassermann (NW) to Kurdjumov-Sachs (KS). Here the geometrical
quantities are uniquely related by the misfit ratio r of atomic diamet
ers. We consider the so-called NW-x configuration in which the orienta
tion is imposed by close matching along the [211BAR] f.c.c. and [110BA
R] b.c.c. (taken as x-) directions. From the fact that no net shear pa
ttern displacements are present with x-ledges (ledges normal to the x-
direction) it is concluded that they are energetically preferable to y
-ledges and justifies the approach of an energetic comparison between
stepped interfaces with x-ledges and a planar interface containing con
ventional misfit dislocations (MDs). The NW-x stepped configuration is
at first subjected to a rigid model analysis, i.e. a model with rigid
crystals and periodic (truncated Fourier representation) interfacial
interaction. This analysis provides (i) energetic justification for a
relation between terrace periodicity and misfit cancellation, (ii) val
ues of upper and lower average energy bounds, (iii) a method for estim
ating interfacial shear moduli, and (iv) a motivation for the suggesti
on that a relative rigid translation of the crystals is needed for ene
rgy minimization. The average energy per atom of a stepped interface (
epsilon(s)BAR) provides for misfit at the terrace patch and riser inte
rface, as well as for misfit normal to the interface. The planar inter
face energy epsilon(p)BAR accounts for interfacial misfit only. From a
display of the excess energy DELTAepsilonBAR = epsilon(s)BAR - epsilo
n(p)BAR plotted against r it is concluded that stepped interfaces are
more stable than planar interfaces for all meaningful values of the mi
sfit ratio r, i.e. within the range where the NW-x orientation is viab
le.