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Oscillations, Waves, and Interactions - GWDG

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386 U. Kaatze <strong>and</strong> R. Behrends<br />

of the system <strong>and</strong>, on favourable conditions, can be obtained from experimental data.<br />

At reasonable values of the parameters of Eqs. (41,42) a Gaussian size distribution<br />

of micelles follows also from this procedure. According to<br />

σ 2 = (sf + sr) −1<br />

the variance of the distribution is given by the slope parameters in the dependencies<br />

of the rate constants upon the aggregate size.<br />

The adequacy of the above relations has been demonstrated by considering results<br />

for solutions of proper micelles [75]. As the numerical evaluation of the isodesmic<br />

reaction scheme (Eq. (25)) avoids approximations of the analytical treatment, it is<br />

capable of revealing some special features of short chain surfactant solutions which<br />

remain unnoticed otherwise. For parameters modelling the n-HepACl system the size<br />

distribution of the micellar species at some surfactant concentrations is displayed in<br />

Fig. 19. Some characteristics of these distribution functions attract attention. The<br />

less pronounced relative minimum in the size distribution � Ni(i) � contrasts the deep<br />

minimum presumed by the Teubner-Kahlweit-Aniansson-Wall model for the oligomer<br />

region. Hence there exists a noticeable content of small oligomeric structures in<br />

the short chain surfactant solutions <strong>and</strong> the separation between the slow <strong>and</strong> the<br />

fast relaxation process is reduced or absent at all. At C ≈ cmc <strong>and</strong> C < cmc the<br />

relative maximum in � Ni(i) � , as characteristic for the Gaussian distribution of proper<br />

micelles, is absent. Even at surfactant concentrations distinctly smaller than the cmc,<br />

a noticeable content of oligomeric species is formed.<br />

The eigenrate spectrum of the isodesmic reaction scheme (Eq. (25)) near the cmc<br />

confirms the absence of any slow relaxation process due to the absence of a pronounced<br />

relative minimum in the size distribution � Ni(i) � . As indicated by the<br />

Figure 19. Distribution of the equilibrium concentration ˆ Ni<br />

˜ of aggregates from i<br />

monomers as resulting from the extended Teubner-Kahlweit model [75]. In the numerical<br />

calculations parameters have been chosen to correspond with the n-heptylammonium<br />

chloride/water system at surfactant concentration C.<br />

(43)

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