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196 3 IG!wtioiinl Specfrri us N Probe of Sfiw-tiird Order<br />

tan,, t Hours)<br />

Figure 3-60. 1 : 1 molar mixture<br />

of n-CzJHqg and n-C.5HF2. Kinetics<br />

of the process of diffusion<br />

at four different temperatures.<br />

Data from calorimetric<br />

measurements<br />

conformational deformations at chain ends; (iii) diffusion which generates the<br />

interpenetration of chains; and (iv) the full collapse towards a liquid-like structure.<br />

Conclusion no. 7<br />

As a consequence of such longitudinal motion, if crystallites of n-alkanes are suitably<br />

brought together thermally activated transport of matter can take place and<br />

diffusion of molecules from one crystallite to another can occur. The kinetic of<br />

diffusion is function of temperature, length of the chain, contacts between crystallites<br />

(ie., pressure put on the sample), etc.<br />

We can proceed further and try to understand the mechanism at the molecular<br />

level which drives the chains outside their own lamella by a thermally activated<br />

process.<br />

We refer the reader to [ 1031, [ 1551 and [ 1451 for a first analysis of the various data.<br />

We simply mention the line of thought followed by various authors on this rather<br />

complex problem.<br />

Several theoretical models have been proposed in an attempt to account for the

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