Interfaces for the 21st Century: New Research Directions in by Marc K. Smith, Michael J. Miksis, Geoffrey B. McFadden, G.

By Marc K. Smith, Michael J. Miksis, Geoffrey B. McFadden, G. Paul Neitzel, David R. Canright, Stephen H. Davis

This paintings highlights a few advances in interfacial examine within the fields of fluid dynamics and fabrics technology initially of the twenty first century. it really is an extension of the displays made through the convention "Interfaces for the Twenty-First Century", hung on 16-18 August 1999, in Monterey, California. It contains papers via sixteen specialists within the box of interfacial mechanics, abstracts contributed through examine scientists, and a precis of a panel dialogue on destiny examine instructions. The textual content covers experimental and theoretical ways, with the unifying philosophy being the research of recent options for modelling the dynamics of interfaces. a couple of answer equipment and experimental reports, in addition to the actual difficulties that initiated them, are provided.

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Extra resources for Interfaces for the 21st Century: New Research Directions in Fluid Mechanics and Materials Science : A Collection of Research Papers Dedicated to Steven H. Davis in Commemoration of hi

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Da. ( 3 3 ) ]n(l + a/2K)~" The integral can be expressed in terms of exponential integrals, but must be evaluated numerically. The asymptotic values for large and small K are given by t ^ l + iK^K»1' ,0 8 Wo t *~16KHl/2K)^K«1- M The large K asymptotic value for t* is accurate to within less than one per cent for K > 1. Some calculated values of t* are shown in Table 1. It should be noted Table 1. The lifetime of a drop for C

To demonstrate the significant features of the solution of this model problem, it is sufficient to treat the special case of zero Bond number. The initial conditions are given in Eq. (7). In the outer region, the height profile of the drop can be written as h = hc + Ch1} hc = — (a2 - r2) , 0app = —, y = - / , (18) where the last equation represents the global mass balance (6). After one integration, the evolution equation (4) gives dr \ dr2 rdr J a3 dt J \ 2a2 The solution of this equation subject to the boundary conditions can easily be determined.

Michalland, Euro. J. Mech. B/Fluids 10, 253 (1991). 20. H. Z. Cummins, L. Fourtune, and M. Rabaud, Phys. Rev. E 47, 1727 (1993). 21. S. Michalland and M. Rabaud, Physica D 61, 197 (1992). 22. S. Michalland, M. Rabaud, and Y. Couder, Europhys. Lett. 22, 17 (1993). 23. V. Hakim, M. Rabaud, H. Thome, and Y. Couder, Proc. NATO Adv. Workshop in New Trends in Nonlinear Dynamics and Pattern Forming Phenomena: the Geometry of Nonequilibrium, Cargese, France (1988). 24. A. M. McEwan and G. I. Taylor, J.

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