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