Abstract
Surprisingly enough, the properties of thin polymer films can be covered by hydrodynamic equations originally devised for classical liquids, provided that surface slip is properly taken into account. This was the key insight of Chap. 4. However, this is of course not entirely correct—put simply, it depends on the chain length of the polymer. If the polymer properties are brought into play, the thin films display viscoelastic behaviour. Chapter 5 introduces the concepts needed to cover this case and explains how the thin film equations are modified in this case. Finally, the chapter addresses microscopic properties of thin films like the slip length and glassy behaviour.
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Notes
- 1.
Note that the Jeffreys model is used in several parametrizations in the literature. Upon multiplying Eq. (5.20) with the elastic modulus G we can find the form \(G\widehat{\tau} + \eta_{1} \dot{\rule{0pt}{7.pt}\widehat{\tau}} = G\eta_{1} \dot{\rule{0pt}{7.pt}\widehat{\gamma}} + \eta_{0}\eta_{1}\ddot{\widehat{\gamma}} \) which is used by Vilmin and Raphaël (2006).
- 2.
We omit the \(\widehat{\hphantom{a}}\)-symbol in the following to simplify notation.
- 3.
One notes a difference of a factor of 1/2 between this equation and equation (5.9). This is convention-dependent. We use the convention used in Rauscher et al. (2005). In comparing both cases, it suffices to assume that the additional factor has been absorbed in the definition of the viscosity η, see Eq. (5.25) below.
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Blossey, R. (2012). Viscoelastic Thin Films. In: Thin Liquid Films. Theoretical and Mathematical Physics. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-4455-4_5
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