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Self-Assembly of Synthetic and Biological Polymeric Systems of ...

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temperatures, the chains are mixed homogeneously, as in any polymer melt. As the<br />

temperature is reduced the tendency for the blocks to segregate is enhanced, i.e. the enthalpic<br />

process <strong>of</strong> demixing is favoured. However, this is necessary accompanied by a reduction in the<br />

entropy as the chain configuration becomes more constrained. The extent <strong>of</strong> segregation <strong>of</strong><br />

the copolymer may be expressed using the reduced parameter N. Here, is the Flory-Huggins<br />

interaction parameter, which contains a significant enthalpic contribution, <strong>and</strong> is governed by<br />

the incompatibility <strong>of</strong> the monomers; <strong>and</strong> N is the copolymer degree <strong>of</strong> polymerization,<br />

reflecting the N-dependent translational <strong>and</strong> configurational entropy. The transition from<br />

homogeneous melt <strong>of</strong> chains to heterogeneous melt <strong>of</strong> ordered microphase-separated<br />

domains occurs at a critical value <strong>of</strong> N, depending on the composition <strong>of</strong> the copolymer (65).<br />

In bulk, the minority block is segregated from the majority block forming regularly shaped <strong>and</strong><br />

uniformly-spaced nanodomains. The shape <strong>of</strong> the segregated domains in a diblock is governed<br />

by the volume fraction <strong>of</strong> the minority block, f, <strong>and</strong> block incompability. Figure 3.1 shows the<br />

equilibrium morphologies documented for diblock copolymers as an example. At a volume<br />

fraction <strong>of</strong> ≈ 20 %, the minority block forms a body-centred cubic spherical phase in the matrix<br />

<strong>of</strong> the majority block. It changes to hexagonally packed cylinders at a volume fraction ≈ 30 %.<br />

Alternating lamellae are formed at approximately equal volume fractions for the two blocks. At<br />

a volume fraction <strong>of</strong> ≈ 38 %, the minority block forms bicontinuous structures at moderate <strong>and</strong><br />

high incompatibility, respectively (64)(65)(69).<br />

A Block B Block<br />

Sphere Cylindric Bicontinuous Lamellar<br />

Figure 3.1. Regular structures in block copolymer leaded by theirs self-assembling.<br />

The physical properties <strong>of</strong> copolymeric materials have been applied in a wide range <strong>of</strong> fields.<br />

For example, by decades copolymeric materials in solid state have been used as thermoplastic<br />

<strong>and</strong> elastomeric materials, foams, <strong>and</strong> glues owing to their high compatibility, sensitivity, <strong>and</strong><br />

92

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