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Coil-Globule Transition Versus Aggregation

we describe and compare the results of simulations for two multichain systems corresponding to alternating and protein-like HA copolymers [212], The multichain systems consisting of 127-unit copolymers were simulated for the range of the effective interaction parameter / (which is similar to the Flory-Huggins parameter) under solvent conditions when single chains can form strongly collapsed conformations. [Pg.86]

In Fig. 42, we show the ratio R2P/R2 U (i 2n and R2V are the partial mean-square radii of gyration calculated separately for hydrophobic and hydrophilic beads) as a function of the interaction parameter /. We see that this ratio is an increasing function of /. Qualitatively the same picture is observed for isolated chains. Such behavior is due to the fact that, as the attraction [Pg.86]

The calculated values of AG are presented in Fig. 43 as a function of the interaction parameter x As seen, lowering the temperature, or equivalently, [Pg.87]

Moreover, the thorough analysis of globular conformations shows that this layer is almost absent near the faces of the cylinder [212]. This facilitates the formation of multiglobular aggregates in the solution of regular copolymers. [Pg.88]

These facts explain the more expressed tendency of regular copolymers toward aggregation. [Pg.89]

Generally speaking, the reason for this behavior is simple. It is known that low-molecular-weight surfactants dramatically increase the stabiUty of polymers and are widely used to prevent aggregation in polymer solutions. In the HA model, surfactants , i.e., amphiphihc A groups, are incorporated into the polymer chain, thus ensuring the stabihzing effect. From the tempera- [Pg.89]


See other pages where Coil-Globule Transition Versus Aggregation is mentioned: [Pg.86]    [Pg.86]    [Pg.86]    [Pg.86]   


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