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

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2.9.1.- Viscoelasticity<br />

Many materials can be classified as solid or fluids, displaying elastic <strong>and</strong> viscous behaviour<br />

respectively. Viscoelastic materials such as polymers combine the characteristics <strong>of</strong> both<br />

elastic <strong>and</strong> viscous materials depending on the experimental time scale. Application <strong>of</strong> a stress<br />

<strong>of</strong> relatively long duration may cause some flow <strong>and</strong> irrecoverable deformation, while a rapid<br />

shearing would induce an elastic response in some polymeric fluids. Then, a classification <strong>of</strong><br />

these materials should include a consideration <strong>of</strong> the timescale <strong>of</strong> the measurement relative to<br />

the characteristic time <strong>of</strong> the material. This ratio is given by the Deborah number (De): when De<br />

is 1 the material will display both viscous <strong>and</strong> elastic behaviour <strong>and</strong> is described as viscoelastic,<br />

whilst, for De » 1 <strong>and</strong> De « 1 the material has solid-like <strong>and</strong> viscous-like behaviour, respectively<br />

(49)(50).<br />

Pure elastic solid behaviour may be exemplified by a Hookean spring, <strong>and</strong> pure viscous flow<br />

can be exemplified by the behaviour <strong>of</strong> a dashpot, which is essentially a piston moving in a<br />

cylinder <strong>of</strong> Newtonian fluid. Nevertheless, the viscoelasticity cannot be described accurately by<br />

neither spring nor dashpot alone, but a combination <strong>of</strong> both. In this way, several mechanical<br />

models have been developed to describe the viscoelastic response <strong>of</strong> a given material. All <strong>of</strong><br />

these mechanical models are, then, supported on the combination <strong>of</strong> these two simple<br />

elements (spring <strong>and</strong> dashpot), which represented the elastic behaviour <strong>of</strong> a solid body, <strong>and</strong><br />

the viscous flow for a liquid, respectively. Among all models, Maxwell’s <strong>and</strong> Kelvin-Voigt’s<br />

models are the most frequently used (Figure 2.21) (50).<br />

a) b)<br />

<br />

E<br />

<br />

Figure 2.21. a) Maxwell’s <strong>and</strong> b) Voigt’s models.<br />

The use <strong>of</strong> mechanical models such as the spring <strong>and</strong> dashpot as analogues <strong>of</strong> the behaviour <strong>of</strong><br />

real materials enables us to describe very complex experimental behaviours using a simple<br />

combination <strong>of</strong> models. The uses <strong>of</strong> models to represent a wide range <strong>of</strong> deformation are not<br />

restricted to the application <strong>of</strong> shear stress; however, in this section, we will focus on the shear<br />

properties <strong>of</strong> the material (1).<br />

E<br />

<br />

59

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