Surfactant systems surface morphology

In what follows we will discuss systems with internal surfaces, ordered surfaces, topological transformations, and dynamical scaling. In Section II we shall show specific examples of mesoscopic systems with special attention devoted to the surfaces in the system—that is, periodic surfaces in surfactant systems, periodic surfaces in diblock copolymers, bicontinuous disordered interfaces in spinodally decomposing blends, ordered charge density wave patterns in electron liquids, and dissipative structures in reaction-diffusion systems. In Section III we will present the detailed theory of morphological measures the Euler characteristic, the Gaussian and mean curvatures, and so on. In fact, Sections II and III can be read independently because Section II shows specific models while Section III is devoted to the numerical and analytical computations of the surface characteristics. In a sense, Section III is robust that is, the methods presented in Section III apply to a variety of systems, not only the systems shown as examples in Section II. Brief conclusions are presented in Section IV. 

MORPHOLOGY OF SURFACES IN MESOSCOPIC POLYMERS, SURFACTANTS, ELECTRONS, OR REACTION-DIFFUSION SYSTEMS METHODS, SIMULATIONS, AND MEASUREMENTS... 

Morphology of Surfaces in Mesoscopic Polymers, Surfactants, Electrons, or Reaction-Diffusion Systems Methods,... 

Gold nanoparticles of different shapes were synthesized in the same system with and without the use of reducing agent. The surfactants act as shape regulators due to their selective adsorption to the nanoparticle surfaces resulting in different morphologies of the nanoparticles. Size control over the capped nanoparticles was obtained by altering the aqueous phase content. More relevant information can be foimd in [55-62]. 

Recently reported meso- and macroscale self-assembly approaches conducted, respectively, in the presence of surfactant mesophases [134-136] and colloidal sphere arrays [137] are highly promising for the molecular engineering of novel catalytic mixed metal oxides. These novel methods offer the possibility to control surface and bulk chemistry (e.g. the V oxidation state and P/V ratios), wall nature (i.e. amorphous or nanocrystalline), morphology, pore structures and surface areas of mixed metal oxides. Furthermore, these novel catalysts represent well-defined model systems that are expected to lead to new insights into the nature of the active and selective surface sites and the mechanism of n-butane oxidation. In this section, we describe several promising synthesis approaches to VPO catalysts, such as the self-assembly of mesostructured VPO phases, the synthesis of macroporous VPO phases, intercalation and pillaring of layered VPO phases and other methods. 

In the Current State of the Art we will review some of the recent SANS and reflectivity data from ISIS, which also serve to point to future directions and opportunities. Recent reflectivity measurements, on the adsorption of polymers and polymer/surfactant mixtures at interfaces, surface ordering in block copolymer systems, time dependent inter-diffusion at polymer-polymer interfaces, and the contribution of capillary waves to interfacial widths, will be described. The use of SANS to investigate the dynamic of trans-esterification of polyester blends, the deformation of copolymers with novel morphologies, and the use of diffraction techniques to determine the structure of polymeric electrolytes, will be presented. 

In order to better understand the pathophysiology associated with these various forms of pulmonary edema, a review of the morphology associated with the capillary-alveolar—intestinal interlace is useful (Fig. 6). From this review it can be seen that fluid in pulmonary capillaries is separated from the alveolar interstitial tissue by the capillary endothelial cells and the capillary basement membrane (commonly called the endothelial barrier). The alveolar surface is separated from the interstitial space by the alveolar-airway barrier, which consists of the alveolar basement membrane, alveolar epithelium, and a layer of pulmonary surfactant within the alveolus. As described previously, the alveolar interstitial tissue is made up of connective tissue (elastin and collagen), fibronectin, and mucopolysaccharides. The interstitial space also contains the pulmonary lympatic system, which functions to drain proteins, large particulate matter, and excess fluid away from the tissue space and to return them to the blood. 

---