Combined Dielectrophoretic Electrohydrodynamic-PDF Free Download

Collodial Cluster Arrays by Electrohydrodynamic Printing Sibel Korkut, Dudley A. Saville,† and Ilhan A. Aksay* Department of Chemical Engineering, Princeton UniVersity, Princeton, New Jersey 08544-5263 ReceiVed July 22, 2008.ReVised Manuscript ReceiVed September 1, 2008 A “stable” electrohydrodynamic jet is used to print arrays of colloidal suspensions on hydrophobic surfaces.

Abstract Stability of electrohydrodynamic flows is essential to a . jump conditions are needed to relate the interfacial and bulk properties. Except for the empirical no-slip condition (Eq. 30e), the following jump

Stability Condition 554 11.5. Helmholtz and Bernoulli Equations 555 . 11.8. Electrohydrodynamic Stability 561 11.9. Electrohydrodynamic Flow in a Circular Cylindrical Conduit . . 567 11.10. Electrogasdynamic Energy Converter 569 . 12.11. Interfacial Stability of Ferrofluids 603 12.12. Other Problems in Ferrofluids 608 Problems 609 CHAPTER 13

A linear stability analysis of a novel electrohydrodynamic Kelvin-Helmholtz system consisting of the superposition of two uniformly rotating dielectric media is presented. The characteristic equation for such an arrangement is derived, which in turn yields a stability criterion for velocity differences of disturbances at a given rotation frequency.

332 A.A. Mohamed et al./Journal of Computational and Applied Mathematics 60 (1995) 331 346 However, recent studies of the nonlinear electrohydrodynamic stability showed that both the normal field and the tangential field play roles in stability criterion [17, 18].

ResearchArticle Study on Electrohydrodynamic Rayleigh-Taylor Instability with Heat and Mass Transfer MukeshKumarAwasthi1 andVineetK.Srivastava2 .

Insulating Electrohydrodynamic Micro-/Nanopatterns . linear stability analysis predicts a characteristic wavelength , which corresponds to the spacing between patterned pillars, with the fastest linear growth . under the given EHDP condition (h 13 μm, d 28 μm, f 0.464, and U 200V).

The Preparation of Electrohydrodynamic Bridges from Polar Dielectric Liquids Adam D. Wexler 1 , Mónica López Sáenz 2 , Oliver Schreer 2 , Jakob Woisetschläger 3 , Elmar C. Fuchs 1 1 Applied Water Physics, Wetsus - Centre of Excellence for Sustainable Water Technology

OÞ past a convective heat stretched/shrinked sheet is examined. A stagnation point fluid flow with velocity slip constrains and heat source or sink is deliberated. The combined set of PDEs is translated into ODEs by including approved similarity transformations. HAM is applied for the solution to the obtained nonlinear system.

surface. e boundary condition, corresponding to normal component of the electric eld, at the interface is given by 0, where ( n E ) is the normal component of the electric eld. e interfacial condition, which expresses the conserva-tion of mass across the interface, is given by the equation 0 at .

the interfacial stability problems are important in the pres-ence of mass and heat transfer. e mechanism of heat and mass transfer across an interface is of a great importance in numerous industrial and environmental problem processes. ese include the design of many types of contacting equip-ment, for example, boilers, condensers, evaporators, gas

plied magnetic field on the behavior of the stability. The study of electrohydrodynamic (EHD) K-H instability of free charges, separating two semi-infinite dielectric strea- ming fluids and influenced by an electric field, has been discussed by Lyon [2]. Also, he added the effect of com-pressibility and applied electric field, but he neglected

Electrohydrodynamic processes involve the interaction of an electric field with the flow of a fluid. The assembly of thin polymer films into ordered patterns under the influence of an electric field applied across the polymer film is called electrohydro-dynamic lithography (EHD). The experimental investigation of polymer pattern for-

» Saad 1993, Compressible Fluid Flow, 2. nd . Ed. Prentice Hall. » Huerre and Rossi 1998, Ch.2 in Hydrodynamics and Nonlin

process within OpenFOAM, an open-source computational fluid dynamics (CFD) solver. Further discussion has been provided to show simulations of the process at typical high resolution e-jet printing scales and to present existing limitations of the model. Keywords: Electrohydrodynamic jet printing, CFD, modeling . Introduction

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