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Composite Materials Research Progress

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238<br />

Maria Pia Cavatorta and Davide Salvatore Paolino<br />

initiation point for delaminations and fiber breaks which may dramatically reduce the local<br />

and or global laminate stiffness thus affecting the load-time response. The literature also<br />

acknowledges that more damaging energy absorption mechanisms (such as delamination,<br />

fiber pull-out, fiber/matrix debonding and fiber fracture) follows matrix cracking and that<br />

they significantly reduce the strength and stiffness of the laminate. Considering the<br />

importance of damage assessment, there have been several attempts in the literature to look<br />

for measurable test quantities that could be correlated to the damage process [6, 12-19].<br />

Under low-velocity impact loading conditions, the time of contact between the impactor<br />

and the target is relative long. Even though vibratory load responses from the composite<br />

sample, the impactor and the specimen supporting fixture are common features of impact<br />

loading history, the load history can still yield important information concerning damage<br />

initiation and growth [20]. Several authors have used the force-time history to compare the<br />

structural response from impact tests: in particular, values of the First Damage Force (FDF)<br />

[14-21], the Delamination Threshold Load (DTL) [6] or Hertzian Failure Load (Ph) [15] as<br />

well as of the Peak Force (Fpeak) [2-3, 17, 22-24] have often been used to rank laminate<br />

performance. Identification of the FDF poses no troubles as it corresponds to the first load<br />

drop which can be detected in the load-time history. However, comparison of laminate<br />

performance on such basis can be risky since the level of laminate damage associated with the<br />

first load drop may be quite different for a given laminate tested under different impact<br />

energies, or for different laminates tested at a given impact energy. In this respect, definition<br />

of the DTL and of the Ph appear more suitable for ranking laminate performance as they are<br />

intended to identify a more specific damage condition, that is the initiation of significant<br />

damage. In the case of the DTL, significant damage is defined as predominately delamination,<br />

while for the Ph energy absorption mechanisms other than matrix cracking are considered.<br />

The DTL and Ph do not necessarily correspond to the first load drop; rather, they are<br />

associated to the load drop at which a significant change in the slope of the forcedisplacement<br />

curve may be detected and which signals a change in laminate stiffness.<br />

Experimental determination of these load thresholds, which are shown to vary with the<br />

laminate thickness to the 3/2 power, may prove helpful for damage tolerant design: no<br />

significant damage threat is associated to impact events for which Fpeak is below the laminate<br />

DTL or Ph. On the contrary, for impact events for which Fpeak is above the laminate DTL or<br />

Ph, a damage threat exists, even if no information can be obtained on the final amount of<br />

cumulative damage that will occur.<br />

Difficulties and possible ambiguities in determining the DTL or the Ph have often led<br />

researchers to use Fpeak instead, considering it as the turning point between rather limited and<br />

more significant forms of damage. In [17,25], Liu suggested that for any composite laminate<br />

there exists a maximum value of Fpeak. When the impact energy is such that Fpeak is below this<br />

maximum value, the laminate suffers indentation and local matrix cracking, whereas when<br />

loaded by the maximum Fpeak significant delamination starts to take place.<br />

The idea of Fpeak as the signaling point of significant damage initiation is the basis of the<br />

dimensionless parameter introduced in 1975 by Beaumont et al. [16] called the Ductility<br />

Index (DuI). The DuI, which is proposed as a useful tool for ranking the impact performance<br />

of different materials under similar testing conditions, is defined as the ratio between the<br />

propagation energy Epropagation and the initiation energy Einitiation and it is given by the<br />

expression:

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