Fracture mechanics testing techniques are typically utilized for
evaluation of the effects of metallurgical or environmental variables
on EAC where the specimen contains a sharp crack. One of the most
common and relatively simple techniques for incorporation of fracture
mechanics techniques for the evaluation of EAC is through the
use of constant load or constant deflection specimens. In the
case of constant load specimens, a load is applied to a fracture
mechanics specimen using a directly applied dead weight or through
a pulley or lever system to magnify the dead weight load. These
methods are analogous to those used for constant load tensile
specimens discussed previously.
The most common types of specimens utilized for evaluation of
EAC are the compact tension (CT), single-edge notched bend (SENB),
or double-cantilever beam (DCB) varieties (see Figs. 7-9).
Normally, they are fatigue pre-cracked prior to exposure to the
environment to produce a sharp crack tip. The fatigue pre-cracking
must be performed at a low enough stress intensity to minimize
the plastic zone ahead of the crack. This is usually accomplished
through load-shedding techniques whereby an initially high peak
load is used to initiate the fatigue precrack and the cyclic load
is then decreased as the precrack approaches its desired length.
In the testing of precracked specimen, it has been found that
excessive initial stress intensity of precracked specimens can
produce a large plastic zone that can act as a barrier to EAC
initiation. In these cases, the effect will be to produce nonconservative
data.
The stress intensity at the tip of the crack can be calculated
using standard equations as given in ASTM E399 for CT and SENB
specimens and in NACE TM0177, Method D for the DCB specimen.
As shown for the DCB specimen, side grooves can be utilized to
assist in keeping the crack growing in a planar fashion under
plane strain conditions. In some cases the crack will tend to
grow out of plane resulting in an invalid test. The important
consequence of using side grooves is that the equation for the
CT or DCB must contain a correction factor that accounts for the
geometry and dimension of the side grooves.
Dead weight-loaded specimens are often used to monitor time to
crack initiation and can be used to monitor crack growth rate
vs. stress intensity K. This is normally performed by measurement
of crack opening displacement, which can be related to crack length
for a particular specimen geometry using compliance techniques.
In the latter case, however, provisions must be made to monitoring
crack opening displacement at a rapid rate because the crack growth
rate will tend to increase with increasing K as the crack proceeds
through the specimen.
An attractive alternative to dead weight-loaded specimens is constant
deflection specimens. In this situation, either CT or DCB specimens
are loaded to an initial level of crack tip stress intensity by
deflection of the arms of the specimen. This deflection is obtained
either by inserting the wedge into the specimen or by tightening
a bolt arrangement that deflects the arms of the specimen. The
initial stress intensity must be above the threshold stress for
EAC which allows cracking to initiate. Once cracking initiates,
it proceeds while the stress intensity decreases as the crack
propagates through the specimen. Thus, this type of test is commonly
referred to as a decreasing K test and is extensively utilized
for evaluation of EAC in its various forms. Once the stress intensity
at the crack tip reaches a value insufficient to sustain crack
growth, crack growth will stop. These conditions of load and
crack length can be used to define the threshold stress intensity
using the appropriate equations for either the CT or DCB specimens.
Sometimes the period required to run a decreasing K test is very
long. An alternative is to use a rising load test whereby the
fracture mechanics specimen is subjected to an increasing load.
In this case, the crack open displacement and load are monitored
simullaneously and the results are analyzed in a similar manner
to conventional fracture mechanics tests. One of the difficulties
in the interpretation of rising load tests is that the threshold
stress intensity obtained by this method often differs from that
determined by decreasing K tests. The dynamic strain rate in the
rising load test can complicate the interpretation of the test
result particularly if HE or HEC are the prevalent cracking mechanisms.
In these cases, a loading rate is usually selected that results
in data that correlate with the results of service experience
in terms of resistance to EAC.