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Oscillations, Waves, and Interactions - GWDG

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

Figure 14. Relaxation amplitude Af (•) <strong>and</strong> relaxation rate τ −1<br />

f<br />

(◦) of the sonic relaxation<br />

term reflecting the fast monomer exchange in sodium dodecylsulfate solutions in water at<br />

25 ◦ C [71] displayed versus concentration exceeding the cmc. Lines indicate the theoretical<br />

relations (Eqs. (30,31)) when according to Eq. (35) the monomer concentration [N1] is used<br />

instead of the cmc in the scaled concentration x (Eq. (29)).<br />

to the concentration [N1] of surfactant monomers <strong>and</strong> [Ni] of class i aggregates.<br />

Here bi+1 is the equilibrium constant. Assuming the effective degree of dissociation<br />

αi = 1 − Ji/i for proper micelles to be independent of i within the micelle region<br />

(αi = α m), an implicit relation for the monomer concentration as a function of total<br />

surfactant concentration C follows:<br />

where<br />

[N1] = Nγ<br />

�<br />

C<br />

− 1<br />

[N1]<br />

� 1/(m(2−α m) �<br />

Nγ =<br />

1 + α m<br />

�√ 2πσ mbm<br />

� �� (1−α m)/(2−α m)<br />

C<br />

− 1<br />

[N1]<br />

� 1/[m(2−α m)]<br />

(35)<br />

. (36)<br />

Deriving these equations m ≈ m + 1 has been tacitely assumed. Using the monomer<br />

concentration [N1] from Eq. (35) instead of the cmc in the scaled concentration<br />

parameter x (Eq. (29)) <strong>and</strong> assuming the reasonable degree of dissociation αm =<br />

0.33 [73] the Teubner-Kahlweit-Aniansson-Wall theory nicely represents the experimental<br />

sonic amplitudes <strong>and</strong> relaxation times. The monomer concentrations following<br />

from the analysis of spectra are shown in Fig. 15 as a function of surfactant concentration.<br />

Also presented in that diagram is the cmc <strong>and</strong> the [N1]-versus-C dependence<br />

for nonionic surfactant systems, as simulated by α m = 1 in the above relations. With<br />

the ionic surfactant solutions the monomer concentration after reaching the cmc decreases<br />

significantly whereas the [N1] values of the nonionic surfactant system slightly<br />

increase with C. The tendency in the monomer concentration of ionic surfactants to<br />

decrease above the cmc is a well-established fact [5].<br />

Another extension of the Teubner-Kahlweit model is required to properly account<br />

for the ultrasonic attenuation spectra of surfactant systems close to the cmc [74–

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