Technology of Dispersed Systems and Materials: by Naum B. Uriev

By Naum B. Uriev

Written by means of the founding father of the sector, this practice-oriented advisor summarizes the author's leap forward learn effects and their functions in chemical technology.
The ebook adopts a wholly novel technique, describing the actual chemistry of constitution formation and fabrics synthesis below dynamic stipulations. It starts off by means of constructing the overall idea within the first chapters with as little arithmetic as useful and substantiated by way of experimental leads to each one case. the subsequent chapters take care of the elemental points of rheology, vibrorheology, and superfluidity of dependent dispersed structures in the framework of physicochemical dynamics, whereas the ultimate bankruptcy exemplifies the technological functions of the constructed technique utilizing real-life difficulties of fabrics technological know-how and chemical engineering.
The authoritative consultant to physicochemical dynamics.

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Extra info for Technology of Dispersed Systems and Materials: Physicochemical Dynamics of Structure Formation and Rheology

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Then, liquid dispersion medium penetrates the space between the particles and microgranules that act further as kinetic units are formed. The final stage of this process is association (coalescence) of granules during the collisions accompanied by transition of a dispersed system of the S–L–G type to an S–L system. 31) where ???? and d are the particle density and diameter, respectively. If the liquid medium penetrates the vibration fluidized layer of powder particles and wets their surface, then a capillary meniscus is formed, a granule structure appears, and the granules start interacting.

7), that is, ????lim = ????el + ????el1 . 1) Effective viscosity ???? is determined by the ratio of shear stress P to the deformation rate, that is, ???? = P∕????,̇ where ????̇ = d????∕dt; ???? is the relative deformation; and t is the time. 7 shows kinetics of development and decrease in deformations under stress and unloading in time. 7a). 7b) [1]. In the first case, overall deformation time t including the elastic component (developing at the acoustic speed) and slow one (relaxation) are determined by the time of reaching the initial (before applying the load) linear size of the deformed system.

And Isemura, T. (1963) Colloidal Surfactants: Some Physicochemical Properties, Academic Press, 319 pp. , and Wang, J. (2005) Cohesive force apparatus for interactions between particles in surfactant and polymer solutions. , 266, 32–37. Questions Questions 1. Describe the types of contacts between particles of dispersed phases in dispersed systems and materials. 2. What are strength-reversible and irreversibly destroyed contacts? What are approximate values of force and interaction energy in contacts between particles in the structures of dispersed materials?

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