Interactions charged polymers

The text largely contains fundamental material and focuses on understanding the basic principles rather than learning factual information. Since it is impossible to include all branches of surface science in such an introductory book because of its wide and multidisciplinary scope, a specific and narrow topic, the interfacial interactions between solids and liquids, has been chosen for this book. For this reason, the ionic interactions, charged polymers, electrochemistry, electrokinetics and the colloid and particulate sciences cannot be included. Some fundamental physical chemistry subjects such as basic thermodynamics are covered, and many equations are derived from these basic concepts throughout the book in order to show the links between applied surface equations and the fundamental concepts. This is lacking in most textbooks and applied books in surface chemistry, and for this reason, this book can be used as a textbook for a course of 14-15 weeks. 

The deposition-reduction (DR) method is based on the weak electrostatic interactions of polymer surfaces with the oppositely charged Au(III) complex ions, leading to the reduction of Au(III) exclusively on the polymer surfaces. Appropriate anionic or cationic Au(III) precursors are chosen based on the zeta potentials of polymer supports (Figure 3.6) [43]. 

Figure 6.8 Illustration of colloid-templated nanoparticle assemblies. The process involves the layer-by-layer adsorption of charged polymers and oppositely charged nanoparticles onto the surfaces of the colloidal template. The colloidal core particles may then be removed to generate a hollow sphere of nanoparticles, held together by electrostatic interactions with the linear polymer glue ...

The structure of this interface determines fhe sfabilify of PEMs, the state of water, the strength of interactions in the polymer/water/ion system, the vibration modes of side chains, and the mobilities of wafer molecules and protons. The charged polymer side chains contribute elastic ("entropic") and electrostatic terms to the free energy. This complicated inferfacial region thereby largely contributes to differences in performance of membranes wifh different chemical architectures. Indeed, the picture of a "polyelectro-lyfe brush" could be more insighttul than the picture of a well-separated hydrophobic or hydrophilic domain structure in order to rationalize such differences. ... 

In 1991 Decher and coworkers introduced a new method to prepare multilayered thin films by electrostatic interaction between oppositely charged polyelectrolytes [3, 62, 63]. In this fashion, thin molecular films comprised of charged polymers. 

In general, the adsorption of a surfactant on particles with previously adsorbed polymer can be influenced by (i) a reduction of surface area available for adsorption as a result of the presence of adsorbed polymer, (ii) possible interactions between polymer and surfactant in the bulk solution or in the interfacial region (that is, surfactant with loops, tails or trains of adsorbed polymer molecules), (iii) the steric effect of adsorbed polymer, preventing approach of surfactant molecules for adsorption at the surface, or (iv) possible electrostatic effects if polymer and/or surfactant are charged species. 

Fabrication of organic thin films based on sponfaneous molecular assembly has been considered as one of fhe powerful approaches to create novel supramolecular systems. In this context, multilayer films were fabricated by layer-by-layer electrostatic deposition techniques based on the electrostatic interaction between dsDNA and the positively charged polymer poly(diallyldimethylammonium chloride) (PDDA) on GC surfaces. A uniform assembly of PDDA/DNA multilayer films was achieved, based on the adsorption of the negatively charged DNA molecules on the positively charged substrate [55]. 

The relatively high charge density along the backbone chain of a polyelectrolyte leads to some interesting properties. Titration data show that counterions (including protons in polyacids) bind to polyelectrolytes more readily than they bind to monomeric electrolytes. This effect arises from the additivity of electrostatic interactions between polymer-fixed ions and counterions. At high... 

What is the Gibbs free energy of an electric double layer The energy of an electric double layer plays a central role in colloid science, for instance to describe the properties of charged polymers (polyelectrolytes) or the interaction between colloidal particles. Here, we only give results for diffuse layers because it is simpler and in most applications only the diffuse layer is relevant. The formalism is, however, applicable to other double layers as well. 

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