By G. Marrucci, G. Ianniruberto (auth.), Antonio Fasano (eds.)

For fluid dynamics and difficulties, there are numerous similar business methods that require the examine and alertness of latest types for advanced move stipulations and platforms. The ambitions of this new edited publication is to provide various commercial program and types that deal with present paintings and effects for a few of these problems.

The booklet includes state of the art surveys for pick out versions and functions that supply the main illustrative use of latest version research and alertness. The chapters are geared up into 3 wide different types: flows of nonlinear fabrics, movement followed via thermal approaches, and nonlinear flows in porous media.

Topics and Features:

* Polymer difficulties in extrusion

* Modeling of glass problems

* Pipelining of gases and slurries

* Polymerization process

* Thermally brought on flows in polymers

* Composite fabrics in manufacturing

* Flows via energetic porous media

The publication is a vital source and reference for the research and modeling of difficulties in fluid dynamics and filtration. All researchers, practitioners, and pros in fluid dynamics, chemical strategy engineering, fabrics engineering, and utilized math will locate the booklet an invaluable presentation of present tools and applications.

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Extra resources for Complex Flows in Industrial Processes

Example text

60, 439 (1987). 14. , A theory of the linear viscoelastic properties of dilute solutions of coiling polymers, J. Chem. , 21, 1272 (1953). 15. , The Physics of Rubber Elasticity, Clarendon Press, Oxford (1975). 2 Sedimentation in Coal- Water Slurry Pipelining FABIO Rosso Universitti di Firenze Dipartimento di Matematica "U. Dini" Firenze, Italy ABSTRACT. In this chapter we present an overview of recent investigations on the problem of sedimentation related to the pipelining of a coal-water slurry.

In a suitable window of E/kT values the stickiness is such that the network is impermanent (the chains can detach by thermal motion, if not too frequently) and the behavior remains liquid-like. As always, the viscosity of the system can be calculated through Eq. 11). , by E / kT. 30) Clearly w is much less than Wo if E/kT is of order 10 or more. , if the chain without sticky points would relax faster than l/w, then detachment becomes the controlling mechanism for relaxation. The relaxation time T of the impermanent network is then just equal to 1/wand 1.

34) The function 1 - M*(t) measures the percentage of P present in Cat time t. 35) can be used, in principle, to determine v. As emphasized in [34] the fully nonlinear problem is rather complicated. In this case it is possible and reasonable, on the basis of a suitable physical approximation, to linearize the problem. 36) where A is a linear operator. 36) turns out to be a Fredholm equation of the first kind, which, as is well known, is ill-posed in the sense of Hadamard. 35) depends mainly on the physical situation.

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