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Composite Materials Research Progress

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Damage Variables in Impact Testing of <strong>Composite</strong> Laminates 253<br />

perforation, the increase is on the contrary very rapid. Differently from the DuI which keeps<br />

to a constant low level up to a few impacts before perforation (Figure 12), the DI allows to<br />

monitor the initial phase of steady damage accumulation helping foreseen perforation. The<br />

initial slow decrease of DD values from the first to the second impact is followed by a<br />

constant phase up to the 17 th impact, after which the DD increases rapidly and reaches a value<br />

of one at perforation. Likewise the DuI, DD data are not very sensitive for predicting laminate<br />

perforation as, apart from the last 2-3 impacts, the constant phase of Figure 14b does not<br />

differ from the asymptotic trends of Figures 13a and 13b, where no perforation is achieved.<br />

Also, DD values at the first impact are about the same, regardless of the level of impact<br />

energy.<br />

Conclusion<br />

Impact test data obtained on different laminates are used to compare damage variables which<br />

have been proposed in the literature over the years. To this aim, definition of the two energy<br />

contributions used to compute the DuI has been extended to analyze impact tests with<br />

rebound.<br />

In single impact tests performed at different impact energies, data for Fpeak and DuI point<br />

out the existence of an impact energy threshold at about 40-50% Pn, below which the energy<br />

absorption mechanism is mainly matrix cracking. Graphs of Fpeak vs. impact energy show a<br />

bi-linear trend with a change in slope around the energy threshold; while values of the DuI are<br />

almost null below the energy threshold to then increase quite abruptly up to penetration.<br />

Interestingly, the energy threshold is about the same for all the laminates analyzed in the<br />

study, whose thickness varies from tenths to tens of millimeters. DI data increase<br />

monotonically for increasing impact energies and show very limited scattering up to the<br />

energy threshold. DD values and data in the Master Curve give no indications on the laminate<br />

damage tolerance; rather, they provide a measure of the absorption capability of the laminate.<br />

Results show that thicker laminates are characterized by a higher efficiency of energy<br />

absorption.<br />

Main advantage of the DI variable is the possibility to distinguish between the<br />

penetration and perforation energy thresholds. The distinction is essential when dealing with<br />

thick laminates, for which the impact energy that causes laminate perforation can by far<br />

exceed the penetration energy. In the range of the penetration process, the DI effectively<br />

monitors the impactor moving deeper and deeper into the laminate.<br />

Also in case of repeated impact tests, the DI provides important pieces of information.<br />

For impact energies that cause no laminate perforation within test duration, the DI stays at a<br />

constant low value throughout the test, owing to a negligible damage accumulation besides<br />

initial laminate indentation. For impact energies that cause perforation, the DI shows an initial<br />

phase of linear growth with the number of impacts, owing to a steady accumulation of<br />

damage. A few impacts before perforation, the DI starts raising quite abruptly, helping<br />

foreseeing laminate failure.<br />

Results for Fpeak show that it maintains a constant value when perforation is not achieved<br />

while it decreases rapidly otherwise. However, graphs of Fpeak versus impact number do not<br />

signal any change in the rate of damage accumulation. DuI values are almost null throughout<br />

the test when no perforation occurs. Low and constant values also characterize tests at higher

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