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Collapse of polymer brushes grafted onto planar ... - Wageningen UR

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COLLAPSE OF POLYMER BRUSHES GRAFTED ONTO PLANAR OR CONVEX S<strong>UR</strong>FACE<br />

V.M. Amoskov, T.M. Birshtein, A.A. Mercurieva<br />

Institute <strong>of</strong> Macromolecular Compounds, Academy <strong>of</strong> Science <strong>of</strong> Russia,<br />

31, Bolshoy pr., V.O., St-Petersburg, 199004, Russia<br />

email: vic@avm.macro.pu.ru<br />

ABSTRACT<br />

The collapse <strong>of</strong> <strong>polymer</strong> <strong>brushes</strong> is investigated. Four types <strong>of</strong> the <strong>polymer</strong> systems are considered: (1)<br />

polyelectrolyte <strong>brushes</strong> in poor solvent, (2) non-ionizable and ionizable <strong>brushes</strong> in binary solvents, (3)<br />

<strong>brushes</strong> with n-cluster interactions and (4) thermotropic LC <strong>brushes</strong>. Both an asymptotic analytical analysis<br />

(for chain length N →∞)<br />

and exact numerical computations (for finite N) are applied for investigating these<br />

systems in a self-consistent field (SCF) framework. The SCF numerical calculations are carried out using the<br />

formalism developed by J.Scheutjens and G.Fleer in their classical works.<br />

For the <strong>brushes</strong> <strong>of</strong> <strong>planar</strong> geometry it has been stated that under suitable external and internal conditions,<br />

collapse in all <strong>of</strong> these systems can occur as a first order phase transition. The solvent quality (system 1), the<br />

fraction <strong>of</strong> better solvent (system 2), the energy <strong>of</strong> isotropic interactions (system 3) and the energy <strong>of</strong> anisotropic<br />

interaction (system 4) are the parameters that govern corresponding phase transitions. The <strong>brushes</strong><br />

<strong>grafted</strong> <strong>onto</strong> convex curved surfaces are also investigated. It is found that for the <strong>brushes</strong> <strong>grafted</strong> <strong>onto</strong><br />

external cylindrical or spherical surfaces (combs, stars, micelles and so on), collapse may also occur as a<br />

first order phase transition.<br />

Though investigated <strong>polymer</strong> systems differ in the interactions as well as in the grafting type, it is shown<br />

that a number <strong>of</strong> features are similar for the phase transitions observed in all <strong>of</strong> them.<br />

At small (or large) enough values <strong>of</strong> the governing parameter, anyone <strong>of</strong> the systems under consideration<br />

exists only in a single-phase state, namely, in extended (or collapsed) state. However, there is an intermediate<br />

range <strong>of</strong> the governing parameter values where the swollen and the collapsed microphases may<br />

coexist, such a state being usually referred as a micro-segregated brush (MSB). It is noteworthy that a more<br />

compact phase is typically located in the neighborhood <strong>of</strong> the grafting surface, while the swollen phase is at<br />

the periphery. If the brush is in the biphasic state, its chains are never partly collapsed and partly extended:<br />

on the contrary, the chains are strictly divided into two groups that are either fully collapsed or fully extended.<br />

The fraction <strong>of</strong> the chains responsible for one or another sublayer in the brush depends on the value <strong>of</strong> the<br />

corresponding governing parameter. <strong>Collapse</strong>d chains never participate in the formation <strong>of</strong> the swollen layer,<br />

thus decreasing the effective grafting density for the remaining chains and allowing their existence in the<br />

swollen state. The free end distribution for any brush in MSB state is bimodal. All these effects are<br />

irrespective <strong>of</strong> the grafting surface type.<br />

At relatively small values <strong>of</strong> the grafting densities and finite values <strong>of</strong> the number <strong>of</strong> segments N in each<br />

chain, the brush collapse takes place in a jump-like manner, that being typical <strong>of</strong> the first order phase<br />

transitions. The size <strong>of</strong> nuclei <strong>of</strong> the collapsed phase is defined as H ~ N δ and grows with the chain length N<br />

slower than the brush size. Hence the first order phase transitions cannot exist at the limit <strong>of</strong> N →∞.

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