By Matthias Kind, Wolfgang Peukert, Heinz Rehage, Heike P. Schuchmann
This booklet offers with colloidal structures in technical methods and the impact of colloidal platforms by means of technical strategies. It explores how new size functions can provide the opportunity of a dynamic improvement of medical and engineering, and examines the beginning of colloidal structures and its use for brand new products.
The destiny demanding situations to colloidal strategy engineering are the improvement of applicable apparatus and methods for the construction and obtainment of multi-phase constructions and vigorous interactions in market-relevant amounts. The ebook explores the proper strategies and for managed construction and the way they are often used throughout all scales.
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Dreiss CA (2007) Wormlike micelles: where do we stand? Recent developments, linear rheology and scattering techniques. Eccleston GM (1990) Multiple-phase oil-in-water emulsions. Ferreira TM, Bernin D, Topgaard D (2013) NMR studies of nonionic surfactants. Goetz RJ, El-Aasser MS (1990) Dilute phase behavior of cetyl alcohol, sodium lauryl sulfate, and water. Goetz RJ, Khan A, El-Aasser MS (1990) FT PGSE NMR investigations of the supramolecular structure of a dilute gel phase. Gradzielski M (2003) Vesicles and vesicle gels—structure and dynamics of formation.
Resolved Numerical Simulation of Particle Agglomeration 49 Depending on the resolution of the numerical grid, the relaxation time parameter can limit the maximum Reynolds number. A more detailed description of the basic principles of the LBM can be found in previous publications [11–13, 21] as well as in Crouse , which also gives details on the implemented tree data structure. e. primary particles as well as agglomerates) are fully resolved by the numerical grid whereby details of the flow around the particles are captured and the forces on the particles follow from the boundary condition of the LBM.
3) are described. 5). M. Ernst and M. 1 Lattice-Boltzmann Method The Lattice-Boltzmann method is a numerical scheme for fluid simulations which originated from molecular dynamics models such as the lattice gas automata. g. the Navier-Stokes equations, the LBM describes the fluid behaviour on a so-called mesoscopic scale [7, 19]. The basic parameter in the Boltzmann statistics is the distribution function f = f (x, ξ, t), which represents the number of fictitious fluid elements having the velocity ξ at the location x and the time t.