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Nondestructive testing of defects in adhesive joints

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⎛ hθ<br />

D = π⎜<br />

⎜<br />

⎝ 4Q<br />

∞<br />

⎞<br />

⎟<br />

⎠<br />

2<br />

………………….(5)<br />

where h is the thickness <strong>of</strong> the sample. Due to the swell<strong>in</strong>g <strong>in</strong> a short period <strong>of</strong> time, swell<strong>in</strong>g<br />

correction is necessary to get correct diffusion coefficient known as the <strong>in</strong>tr<strong>in</strong>sic diffusion<br />

coefficient (D * ) [22]<br />

D* =<br />

D<br />

7 / 3<br />

φ<br />

……………………(6)<br />

where φ is the volume fraction <strong>of</strong> the polymer. The variation <strong>in</strong> D * value depends on the nature <strong>of</strong><br />

the crossl<strong>in</strong>k, penetrant size and polarity. The values <strong>of</strong> D * along with sorption and permeation<br />

coefficients are tabulated <strong>in</strong> Table V.<br />

The D * values varied with NCO/OH ratios, with the maximum value obta<strong>in</strong>ed <strong>in</strong> sample with<br />

NCO/OH ratio 1.1. With further <strong>in</strong>crease <strong>in</strong> NCO/OH ratios, D * values showed a steady decrease.<br />

This observation can be correlated to the equilibrium swell<strong>in</strong>g uptake that was found to be<br />

maximum <strong>in</strong> sample with NCO/OH ratio 1.1. To sum up, D * depends more on the molecular<br />

<strong>in</strong>teraction between the penetrant and the polymer system. A better understand<strong>in</strong>g <strong>of</strong> the<br />

<strong>in</strong>teractions and their strengths can be obta<strong>in</strong>ed from the sorption coefficient S, which can be<br />

calculated as follows<br />

S =<br />

M<br />

M<br />

S …………………(7)<br />

P<br />

Where Ms is the mass <strong>of</strong> the solvent molecules at equilibrium swell<strong>in</strong>g and Mp is the <strong>in</strong>itial mass<br />

<strong>of</strong> the polymer sample [20]. The S value is high <strong>in</strong> sample show<strong>in</strong>g high equilibrium swell<strong>in</strong>g<br />

uptake values, i.e. the sample with NCO/OH ratio 1.1. The high S value <strong>in</strong> this system shows the<br />

better accommodation <strong>of</strong> the water molecules due to the favourable <strong>in</strong>teractions with the polar<br />

region <strong>of</strong> the block copolymer. The permeability coefficient P depends on doth D and S, s<strong>in</strong>ce<br />

permeation is a comb<strong>in</strong>ed effect <strong>of</strong> diffusion and sorption [20].<br />

P = D.S ……………………(8)<br />

The permeation values are yet aga<strong>in</strong> high <strong>in</strong> sample with NCO/OH ratio 1.1. The P values reflect<br />

the net effect <strong>of</strong> diffusion and sorption. In the block copolymer studied, S values are higher<br />

compared to D * and P, show<strong>in</strong>g a larger tendency for the penetrant molecules to sorb rather than<br />

diffuse <strong>in</strong>to the polymer. Thus sorption predom<strong>in</strong>ates over diffusion <strong>in</strong> the systems under study.<br />

Effect <strong>of</strong> NCO/OH ratio and pH on overshoot<strong>in</strong>g effect<br />

In Figure 1 and Figure 3, the dynamic swell<strong>in</strong>g curves correspond<strong>in</strong>g to copolymers swollen <strong>in</strong><br />

water and at pH 9 respectively exhibit overshoot. Initially, the samples <strong>in</strong>crease their swell<strong>in</strong>g<br />

ratio, later on they reach a maximum and f<strong>in</strong>ally they deswell until an equilibrium value is<br />

reached. The sample with NCO/OH ratio 1.3, 1.4 and 1.5 exhibit overshoot <strong>in</strong> water while all the<br />

NR/PEG samples exhibit overshoot<strong>in</strong>g effect at pH 4, pH 7 and pH 9. We have attributed this<br />

feature to the anomalous transport with a bias to the non – Fickian mode (Table III). The primary<br />

factor contribut<strong>in</strong>g to overshoot<strong>in</strong>g effect is the difference exist<strong>in</strong>g between the relaxation and<br />

diffusion rates at experimental conditions. The stress generated due to the slow relaxation rate

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