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Nondestructive testing of defects in adhesive joints

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where Qt and Q∞ are the mol% <strong>in</strong>crease <strong>in</strong> sorption at time t and equilibrium respectively. The<br />

type <strong>of</strong> diffusion mechanism has been analysed <strong>in</strong> terms <strong>of</strong> the empirical relation<br />

Q<br />

log<br />

Q<br />

t<br />

∞<br />

= logk + n log t<br />

………….. (2)<br />

k and n have been determ<strong>in</strong>ed from a least square fit <strong>of</strong> log Qt / Q∞ versus log T. Constant k<br />

depends on the structural features <strong>of</strong> the polymer system and its <strong>in</strong>teraction with the solvent<br />

used [17]. The polarity and the size <strong>of</strong> the solvent along with the polar and non-polar segments<br />

<strong>in</strong> the block copolymer determ<strong>in</strong>e the value <strong>of</strong> k parameter. n is the diffusional exponent, which<br />

<strong>in</strong>dicate the transport mechanism. If n =0.5, the mechanism <strong>of</strong> sorption is termed as Fickian,<br />

where the rate <strong>of</strong> polymer cha<strong>in</strong> relaxation is higher than the diffusion rate <strong>of</strong> the penetrant.<br />

When n = 1, the mechanism is said to be non – Fickian where the cha<strong>in</strong> relaxation is slower<br />

than the solvent diffusion. If the value lies between 0.5 and 1, then the mechanism follows<br />

anomalous transport where the polymer cha<strong>in</strong> relaxation rates and the solvent diffusion rates<br />

are similar. By regression analysis, the values <strong>of</strong> n and k are obta<strong>in</strong>ed as slope and <strong>in</strong>tercept and<br />

are consolidated <strong>in</strong> Table III. The correlation coefficient values are found to be 0.999. The<br />

values <strong>of</strong> n range from 0.42 to 0.61, which <strong>in</strong>dicates that the mechanism <strong>of</strong> sorption follows<br />

Fickian mode <strong>in</strong> samples with lower NCO/OH ratios while the mechanism shifts to anomalous<br />

mode with a bias to non – Fickian mode <strong>in</strong> the samples with higher NCO/OH ratios. In the<br />

present study the k values do not show a regular trend.<br />

Sorption k<strong>in</strong>etics<br />

Sorption <strong>of</strong> liquid through polymer samples cause structural rearrangement, which <strong>in</strong>duces<br />

k<strong>in</strong>etic behaviour that <strong>in</strong> turn are affected by the total free volume and its distribution <strong>in</strong> the<br />

polymer system. We have analysed the sorption data <strong>in</strong> terms <strong>of</strong> the first - order k<strong>in</strong>etic model.<br />

The first – order rate constant k1 for the polymer – solvent system was obta<strong>in</strong>ed us<strong>in</strong>g the first –<br />

order equation [20]<br />

dc/dt = k1 (C∞ - Ct) ………………… (3)<br />

where C∞ and Ct are the concentration <strong>of</strong> the penetrant at equilibrium and time t respectively.<br />

C∞ and Ct are equivalent to the equilibrium swell<strong>in</strong>g Q∞ and swell<strong>in</strong>g at time t, which is Qt.<br />

Integration <strong>of</strong> equation (3) gives<br />

k1t = 2.303 log [C∞ / (C∞ - Ct)] ………(4)<br />

Typical plots <strong>of</strong> log (C∞ - Ct ) versus time is given <strong>in</strong> Figure 2 and the estimated rate constants<br />

for the penetrant are given <strong>in</strong> Table IV. A negative slope was observed and the values are found<br />

to range form 3.29 x 10 3 m<strong>in</strong> -1 to 19.30 x 10 3 m<strong>in</strong> -1 .<br />

Transport coefficients<br />

Diffusion <strong>in</strong> polymer is complex and depends strongly on the concentration, degree <strong>of</strong> swell<strong>in</strong>g,<br />

solvent size and size <strong>of</strong> the voids <strong>in</strong> the polymer. From the slope θ <strong>of</strong> the l<strong>in</strong>ear portion <strong>of</strong> the<br />

sorption curve, the diffusion coefficient D has been calculated us<strong>in</strong>g [21]

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