Fatigue Crack Paths 2003
Theoretical prediction of ModeI (principal stress dominated) fatigue crack paths in
two dimensions is relatively simple. The crack path is a line and only Modes I and II
can be present. In each increment of crack growth all that is needed to define the crack
path is a direction, together with the amount of crack growth. Twodimensional ModeI
crack path predictions, for an initial mixed Modes I and II crack, have been carried out
by a number of authors using the same general scheme [11]. Calculations are carried out
numerically using small increments of straight crack growth. The direction taken by
each increment is selected using the criterion that it is pure ModeI. Predicted paths in
general tend to a curve. Agreement between theoretical predictions and experimental
data obtained using thin sheets is variable [33]. This is not surprising because three
dimensional effects are not taken into account.
In three dimensions the situation is muchmore complicated. If fatigue crack growth
is assumed to be in ModeI then, in the general case in which ModeIII displacements
are present on the initial crack, a twist crack (Figs 14, 16, 17) is produced. At the
present state of the art it is not possible to predicted the path of a twist crack on a scale
of observation, say 0.1 mm, at which the individual ModeI facets of a twist crack can
be distinguished. It is merely possible to describe observed twist cracks.
If a larger scale of observation, say 1 mm,is used then a twist crack growth surface
may be regarded as smooth but crack growth is not, in general, in pure ModeI. If an
appropriate criterion were available it would be possible to define the direction of crack
growth at points on the crack front together with amounts of crack growth. This then
determines a new crack front, and the process is repeated to build up a net of crack
fronts and crack trajectories.
In a practical numerical implementation [35] for a slant crack specimen similar to
that shown in Fig. 15, the strain energy rate release criterion was used to determine
crack growth directions and increments. It was pointed out that the predicted crack path
could only be regarded as a qualitative estimate. Nevertheless a plausible crack path was
obtained in which the ModeII stress intensity factor was zero and, as the crack grew,
the ModeIII stress intensity factor tended to zero.
C O N C L U D IRNEGM A R K S
Paths taken by growing fatigue cracks have been of industrial interest for a very long
time. A large amount of empirical knowledge has been accumulated, but at the present
state of the art the factors controlling the path taken by a growing fatigue crack are not
completely understood.
The numerous possible crack configurations [36] mean that a systematic theoretical
approach to fatigue crack paths isn't feasible so particular practical problems need to be
tackled on an ad hoc basis. In carrying out analyses care has to be taken to view fatigue
crack paths at an appropriate scale.
The examples given have been chosen to illustrate some of the more important
aspects of fatigue crack paths in metals.
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