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Composite Materials Research Progress

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<strong>Research</strong> Directions in the Fatigue Testing of Polymer <strong>Composite</strong>s 211<br />

gauge length, because the inevitable slip in the clamps can lead to serious errors in the strain<br />

calculation. Depending on the fibre and matrix type and the stacking sequence, the stiffness<br />

degradation can range from a few percent to several tens of percent [2-7].<br />

If the transverse strain is measured additionally, the Poisson’s ratio νxy can be followed as<br />

well. It has been recently showed by Van Paepegem et al. [8] that the evolution of the<br />

Poisson’s ratio is a very sensitive parameter for fatigue damage. Figure 1 shows the evolution<br />

of the Poisson’s ratio for a [0°/90°]2s unidirectional glass fabric/epoxy composite in tensiontension<br />

fatigue. The νxy – εxx curves in strain-controlled fatigue between 0.0006 and 0.006<br />

show a highly nonlinear behaviour and are upper-bounded by the static degradation of the<br />

Poisson’s ratio.<br />

ν xy [-]<br />

0.20<br />

0.15<br />

0.10<br />

0.05<br />

-0.00<br />

0.000 0.005 0.010 0.015 0.020<br />

-0.05<br />

-0.10<br />

-0.15<br />

-0.20<br />

ν xy versus ε xx for [0°/90°] 2s fatigue test W_090_8<br />

ε xx [-]<br />

static [0°/90°] 2s test IF4<br />

static [0°/90°] 2s test IF6<br />

[0°/90°] 2s fatigue test W_090_8: cycle 600 + 5<br />

[0°/90°] 2s fatigue test W_090_8: cycle 3600 + 5<br />

[0°/90°] 2s fatigue test W_090_8: cycle 37200 + 5<br />

Figure 1. Evolution of the Poisson’s ratio ν xy in function of the longitudinal strain ε xx for a glass/epoxy<br />

[0°/90°] 2s specimen at three chosen intervals in the fatigue test [8].<br />

Another online technique is the use of embedded optical fibre sensors with a Bragg<br />

grating. The Bragg grating is a periodical variation of the optical refractive index that is<br />

written in the core of the glass fibre and is typically a few millimetres in length (Figure 2).<br />

When broadband light is transmitted into the optical fibre, the Bragg grating acts as a<br />

wavelength selective mirror. For each grating only one wavelength, the Bragg wavelength, λB<br />

is reflected with a Full Width at Half Maximum of typically 100 pm, while all other<br />

wavelengths are transmitted. The Bragg wavelength is directly proportional with the period of<br />

the Bragg grating. If the optical fibre sensor is embedded in a composite laminate, the strain<br />

in the loaded laminate will cause the period of the Bragg grating to change, and hence the<br />

value of the reflected Bragg wavelength.

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