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Hygrothermal aging of a filled epoxy resin - Schneider Electric

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<strong>Schneider</strong> <strong>Electric</strong> 2007 - Conferences publications<br />

mass <strong>of</strong> 6% measured for the un<strong>filled</strong> samples, this<br />

value leads to a filler content <strong>of</strong> 58% which corresponds<br />

well with the “rated” filler content <strong>of</strong> 60%. To simplify<br />

the comparisons, the variations <strong>of</strong> the residual masses<br />

were neutralized in the results displayed in Figure 3.<br />

This shows the relative mass losses between the initial<br />

mass values <strong>of</strong> the samples and the residual masses.<br />

A mass loss between 50°C and 200°C can be observed,<br />

as in un<strong>filled</strong> samples. In these cases, the variations<br />

correspond well with the water uptake measured before.<br />

The <strong>resin</strong> decomposition can be observed in the same<br />

temperature range as above. As shown in the zoom in<br />

Figure 3, decomposition started at lower temperatures<br />

for longer conditioning periods. This is clear if we<br />

compare the curves for 50 and 70 days, which fit the<br />

curve <strong>of</strong> 14 days until about 200°C and decrease faster<br />

between 200°C and 300°C. This indicates an evolution<br />

<strong>of</strong> the material produced by the hygrothermal<br />

conditioning after about 50 days. Since this effect was<br />

not encountered in samples without fillers, the<br />

<strong>epoxy</strong>/silica interface regions are necessarily involved.<br />

We have already mentioned that the mass measurements<br />

suggest an accumulation <strong>of</strong> matter close to these<br />

interfaces. We may consider that this evolution is due to<br />

an hydrolysis <strong>of</strong> the filler/matrix interface regions which<br />

creates a degraded inter-phase region. Since the filler<br />

content is large, this degraded region may also fill the<br />

whole gap between neighbouring fillers and constitute<br />

“weak” path between them. This hydrolysis occuring<br />

after about 50 days is probably correlated with the<br />

increase <strong>of</strong> the mass uptake observed at the same time.<br />

The possible explanation <strong>of</strong> this is as follows: free space<br />

is created by the hydrolytic reactions consisting mainly<br />

in the attack <strong>of</strong> the ester linkages and creation <strong>of</strong> acid<br />

groups [4]. This allows extra water molecules to<br />

accumulate between the filler and the degraded region.<br />

However, the extra quantity <strong>of</strong> water involved in this<br />

mechanism would be low in comparison with the total<br />

quantity <strong>of</strong> absorbed water, which was almost entirely<br />

lost between 50°C and 150°C. Further experiments are<br />

under way to confirm this hypothesis.<br />

DMA results<br />

The dynamic mechanical analysis was carried out on<br />

four <strong>filled</strong> and four un<strong>filled</strong> samples after 0, 5, 14 and<br />

50 days <strong>of</strong> conditioning. The evolution <strong>of</strong> the elastic<br />

moduli E’ is displayed in Figure 4a. The magnitudes for<br />

the <strong>filled</strong> samples were about three times larger in the<br />

glassy state and five times larger in the rubbery state.<br />

The elastic modulus decreased during conditioning,<br />

especially in the glassy state. In practice, water<br />

molecules break the hydrogen bonds established inside<br />

the network. The bound water increases also the<br />

mobility <strong>of</strong> the polymer chains and causes a decrease <strong>of</strong><br />

the elastic modulus. This is the well-known waterinduced<br />

plasticization effect.<br />

In the rubbery state, we would expect the effect to be<br />

less marked since the chains are already mobile. Thus in<br />

this case, the modulus E’ depends theoretically on the<br />

density <strong>of</strong> cross-links in the <strong>epoxy</strong> network [14].<br />

Nevertheless, the conditioning induced a decrease <strong>of</strong> the<br />

elastic moduli E’ for the <strong>filled</strong> samples. For un<strong>filled</strong><br />

samples, the measurements were conducted at the lower<br />

limit <strong>of</strong> sensitivity <strong>of</strong> the DMA instrument. Such a<br />

decrease <strong>of</strong> the rubbery modulus has already been<br />

observed in [15]. It is not due to the plasticization but<br />

may be attributed to a degradation <strong>of</strong> the polymer,<br />

which probably results from hydrolysis <strong>of</strong> the <strong>resin</strong>.<br />

(a)<br />

M(Minitial-Mfinal)%<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

REF<br />

5 days<br />

14 days<br />

50 days<br />

70 days<br />

REF<br />

5 days<br />

14 days<br />

50 days<br />

70 days<br />

0 100 200 300 400 500 600<br />

T(°C)<br />

Figure 3: Weight loss during a TGA dynamic test for<br />

<strong>filled</strong> samples before (•) and after conditioning at 80°C<br />

and 80%HR during 5 (+), 14 (), 50 () and 70 () days<br />

with a zoom in the temperature range 0-350°C between<br />

92 and 100%.<br />

(b)<br />

Figure 4: Elastic modulus E’ (a) and loss modulus E’’<br />

(b) vs temperature <strong>of</strong> un<strong>filled</strong> (---) samples and <strong>filled</strong><br />

( ___ ) samples before (•) and after conditioning at 80°C,<br />

80%HR during 5(+), 14() and 50 () days.<br />

241

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