micellar solutions: one may be controlled by a chemorheological process involving actual breakdown and reformation of the entanglement network, presumably by scission and re-formation of the threadlike micelles themselves, and the other by disentanglement due to diffusion of the network chains but without accompanying their breakdown. An important feature of the type I11 behavior is that the mechanism is a single relaxation time process. This result suggests that the relaxation of the entanglement network of the micellar solutions in the type I11 region is due to a chemorheological process independent of the length of the threads rather than to a diffusional process highly dependent on the thread length. The peculiar dependence of 7, on CsCD-' of this chemorheological process of entanglement relaxation should reflect the stability of the threadlike micelles under the given environment. In the micellar solutions with CsCD-' above 1, the micelles are coexisting with excess Nasal. Therefore, scission and reformation of the micelles may happen rather easily by exchange of the CTAB units of the CTAB/NaSal complexes between the threadlike micelles a t the sites of entanglement, where the threadlike micelles can pass through each other with a certain characteristic time (T,,,) reflecting the rate of this process. Scission of the threadlike micelles may also take place, especially in the highly strained portions between entanglement points by the similar mechanism of exchange of the CTAB units with free Nasal molecules in the medium. Since the solubility of CTAB is rather low in the aqueous medium, the exchange rate must be higher; hence the relaxation time is shorter in solutions with a larger excess of Nasal. Although the detailed features of the dependence of 7, on CSCD-'~~ such as seen in Figure 6 cannot be adequately explained at the moment, the general tendency of the Cs and C D dependences of 7, and J,O may be interpreted as discussed above. The type I and type I1 behavior are the results of the onset of entanglement and the fully developed entanglement network as the threadlike micelles are formed with increasing C&-' up to the critical value of approximately 1. On the other hand, the type I11 (Maxwell model) behavior is the result of actual breakdown and re-formation of the entanglement network with the rate dependent on CsCD-1'2 but with the entanglement density being practically constant after CsCD-' exceeds the critical value.
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