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Nondestructive testing of defects in adhesive joints

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Effect <strong>of</strong> prist<strong>in</strong>e nano silica filler on oxidative degradation characteristics <strong>of</strong><br />

EVA/LDPE blends<br />

The control blend (EL6/4) exhibited greater thermal stability than the pure EVA and LDPE<br />

[Figure 1(a)]. Also, EVA was also found to be thermally more stable than LDPE. Thus <strong>in</strong><br />

presence <strong>of</strong> EVA, LDPE was stabilized. In all silica filled blends there were two dist<strong>in</strong>ct and well<br />

separated steps <strong>in</strong> the thermogravimetric curves (TG) (correspond<strong>in</strong>g weight loss peaks <strong>in</strong><br />

derivative thermgravimetric, DTG) curves as represented <strong>in</strong> Figure 1 (b) and (c). The first step<br />

(309-315 0 C) for all samples (unfilled and filled) was possibly due to de-acetylation <strong>of</strong> v<strong>in</strong>yl<br />

acetate group <strong>of</strong> EVA with the elim<strong>in</strong>ation <strong>of</strong> acetic acid. As a result, double bonds were formed<br />

[10] <strong>in</strong> the ma<strong>in</strong> cha<strong>in</strong>. The second step (413-418 0 C) might be assigned to the further degradation<br />

<strong>of</strong> polyacetylene-ethylene cha<strong>in</strong>s formed <strong>in</strong> the first step accompanied with the degradation <strong>of</strong><br />

LDPE [10].<br />

As compared to <strong>in</strong>ert atmosphere, it was observed that the <strong>in</strong>itial stages <strong>of</strong> degradation for<br />

all samples were accelerated <strong>in</strong> the presence <strong>of</strong> oxygen [Fig. 2(a)]. Thus the rate <strong>of</strong> reaction might<br />

be controlled by O2 diffusion <strong>in</strong> the polymeric matrix. There was also an <strong>in</strong>itial ga<strong>in</strong> <strong>in</strong> weight<br />

prior to deacetylation <strong>in</strong> the presence <strong>of</strong> oxygen. This suggested a rapid <strong>in</strong>itial oxidation <strong>of</strong> the<br />

blends. Due to the presence <strong>of</strong> SiO2 particles, the onsets <strong>of</strong> degradation <strong>of</strong> filled blends were<br />

shifted towards higher temperatures as compared to the unfilled one. Therefore, the filled systems<br />

were thermally more stable than the pure blend. But <strong>in</strong>terest<strong>in</strong>gly, at very high temperature (~<br />

above 425 0 C) the presence <strong>of</strong> nano silica accelerated degradation <strong>of</strong> filled blends. This might be<br />

due to the fact that at these temperatures silica acted as an acid catalyst. The outcomes from TGA<br />

are represented <strong>in</strong> Table 2. As compared to samples prepared follow<strong>in</strong>g sequence-2,<br />

ELS6/4/3-1 exhibited higher thermal stability at lower temperature ranges. This <strong>in</strong>dicated<br />

the occurrence <strong>of</strong> <strong>in</strong>termix<strong>in</strong>g <strong>of</strong> LDPE and EVA <strong>in</strong> ELS6/4/3-1. In TEM observations<br />

also silica particles were found to be dispersed <strong>in</strong> both phases as well as <strong>in</strong> the <strong>in</strong>terface<br />

for this system. Si69 <strong>in</strong>creased the compatibility between two phases (<strong>in</strong> ELS6/4/3-2-<br />

Si69) and made silica well dispersed <strong>in</strong> the polymeric matrix. Hence, ELS6/4/3-1 and<br />

ELS6/4/3-2-Si69 exhibited greater thermal stability than the rest <strong>of</strong> the samples. The<br />

degradation behavior was well correlated with the morphology analyzed by TEM and<br />

FESEM. The details <strong>of</strong> the analysis are not given <strong>in</strong> this brief article. It will be mentioned<br />

dur<strong>in</strong>g the presentation.<br />

The iso-conversional <strong>in</strong>tegral method named Flynn-Wall-Ozawa method suggested <strong>in</strong>dependently<br />

by Ozawa [11] and Flynn and Wall [12] uses Doyle’s approximation [13] <strong>of</strong> the temperature<br />

<strong>in</strong>tegral. From Eq. (1) and us<strong>in</strong>g Doyle’s approximation, the result <strong>of</strong> the <strong>in</strong>tegration after tak<strong>in</strong>g<br />

logarithms is:<br />

log β = log (AE/g (α)R) - 2.315 – 0.457 E/RT.......................(1)<br />

where β is the heat<strong>in</strong>g rate, A is the pre-exponential factor, E is the activation energy, α is the<br />

degree <strong>of</strong> conversion and T is the temperature. Thus, for α = constant, the plot <strong>of</strong> log β versus<br />

1000/T obta<strong>in</strong>ed at several heat<strong>in</strong>g rates should yield a straight l<strong>in</strong>e whose slope can be used to<br />

evaluate the activation energy.<br />

All the filled samples showed higher activation energy <strong>of</strong> degradation than the control sample.<br />

This implied that the thermal stability <strong>of</strong> the silica filled nanocomposites was higher than the neat<br />

control blend. From plots (not shown <strong>in</strong> text) it can be observed that the best fitted straight l<strong>in</strong>es<br />

(with at least 90% correlation) were nearly parallel to each other and thus confirmed the<br />

applicability <strong>of</strong> this method with <strong>in</strong> the conversion range studied. Interest<strong>in</strong>gly, mean activation<br />

energy <strong>of</strong> ELS6/4/3-2 was higher than that <strong>of</strong> ELS6/4/3-1. The k<strong>in</strong>etic analysis was performed by<br />

both dynamic and static methods and the results were well correlated. However, the details <strong>of</strong><br />

k<strong>in</strong>etic analysis will be discussed dur<strong>in</strong>g presentation.<br />

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