Fluids, colloids, and soft materials: an introduction to by Alberto Fernandez-Nieves PDF

By Alberto Fernandez-Nieves

ISBN-10: 111806562X

ISBN-13: 9781118065624

ISBN-10: 1119220513

ISBN-13: 9781119220510

ISBN-10: 1119220521

ISBN-13: 9781119220527

ISBN-10: 111922053X

ISBN-13: 9781119220534

This publication offers a compilation of self-contained chapters protecting quite a lot of themes in the huge box of soppy condensed subject. every one bankruptcy starts off with uncomplicated definitions to deliver the reader up to date at the subject handy, describing tips to use fluid flows to generate tender fabrics of excessive worth both for functions or for easy learn. insurance comprises themes regarding colloidal suspensions Read more...

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This e-book offers a compilation of self-contained chapters overlaying quite a lot of subject matters in the wide box of soppy condensed matter. Read more...

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Extra info for Fluids, colloids, and soft materials: an introduction to soft matter physics

Sample text

12], among others, for scaling laws of the size of the drops and the electric current, and Barrero et al. [13] for extensions of these results to cone-jets in baths of dielectric liquids. A stable cone-jet exists only within a range of values of the flow rate that shifts toward lower flow rates when the conductivity increases [9]. Fernández de la Mora and Loscertales [10] claim that charge relaxation effects are always important in a certain region around the tip of the meniscus of characteristic size Re = (????0 ????Q∕K)1∕3 , which is also the order of the size of the spray drops.

Fernández de la Mora [1] pointed out that the scaling laws for the length and radius of the jet derived by Cherney [17] on the basis of Fernández de la Mora and Loscertales [10] model suggest that the jet could effectively disappear, or break up before the transfer of charge to its surface is complete, when the flow rate is of order ????Q0 . As an alternative explanation, Guerrero et al. [18] noted that the dynamics of the relaxation region is largely independent of the rest of the meniscus. This region is able to suck a flow rate of order ???? Q0 or larger independently of the flow rate injected through the capillary, which may make a stationary configuration impossible when the latter flow rate is small compared to ????Q0 .

Phys Fluids 1981;24:1967–1972. [25] Wohlhuter FK, Basaran OA. Shapes and stability of pendant and sessile drops in an electric field. J Fluid Mech 1992;235:481–510. [26] Ashley H, Landahl M. Aerodynamics of Wings and Bodies. Chapter 6. Reading (MA): Addison-Wesley; 1965. [27] Hinch EJ. Perturbation Methods. Cambridge: Cambridge University Press; 1991. [28] Barrero A, Gañán-Calvo AM, Dávila J, Palacios A, Gómez-González E. The role of the electrical conductivity and viscosity on the motions inside Taylor cones.

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Fluids, colloids, and soft materials: an introduction to soft matter physics by Alberto Fernandez-Nieves


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