2,055 research outputs found
On the Generalization of the Hébraud-Lequeux Model to Multidimensional Flows
In this article we build a model for multidimensional flows based on the idea of Hébraud and Lequeux for soft glassy materials. Care is taken to build a frame indifferent multi-dimensional model.
The main goal of this article is to prove that the methodology we have developed to study the well-posedness and the glass transition for the original Hébraud-Lequeux model can be successfully generalized. Thus this work may be used as a starting point for more sophisticated studies in the modeling of general flows of glassy materials
A volume-of-fluid formulation for the study of co-flowing fluids governed by the Hele-Shaw equations
We present a computational framework to address the flow of two immiscible
viscous liquids which co-flow into a shallow rectangular container at one side,
and flow out into a holding container at the opposite side. Assumptions based
on the shallow depth of the domain are used to reduce the governing equations
to one of Hele-Shaw type. The distinctive feature of the numerical method is
the accurate modeling of the capillary effects. A continuum approach coupled
with a volume-of-fluid formulation for computing the interface motion and for
modeling the interfacial tension in Hele-Shaw flows is formulated and
implemented. The interface is reconstructed with a height-function algorithm.
The combination of these algorithms is a novel development for the
investigation of Hele-Shaw flows. The order of accuracy and convergence
properties of the method are discussed with benchmark simulations. A
microfluidic flow of a ribbon of fluid which co-flows with a second liquid is
simulated. We show that for small capillary numbers of O(0.01), there is an
abrupt change in interface curvature and focusing occurs close to the exit
Transition from rotating waves to modulated rotating waves on the sphere
We study non-resonant and resonant Hopf bifurcation of a rotating wave in
SO(3)-equivariant reaction-diffusion systems on a sphere. We obtained reduced
differential equations on so(3), the characterization of modulated rotating
waves obtained by Hopf bifurcation of a rotating wave, as well as results
regarding the resonant case. Our main tools are the equivariant center manifold
reduction and the theory of Lie groups and Lie algebras, especially for the
group SO(3) of all rigid rotations on a sphere
Wolfgang von Ohnesorge
This manuscript got started when one of us (G.H.M.) presented a lecture at the Institute of Mathematics and its Applications at the University of Minnesota. The presentation included a photograph of Rayleigh and made frequent mention of the Ohnesorge number. When the other of us (M.R.) enquired about a picture of Ohnesorge, we found out that none were readily available on the web. Indeed, little about Ohnesorge is available from easily accessible public sources. A good part of the reason is certainly that, unlike other “numbermen” of fluid mechanics, Ohnesorge did not pursue an academic career. The purpose of this article is to fill the gap and shed some light on the life of Wolfgang von Ohnesorge. We shall discuss the highlights of his biography, his scientific contributions, their physical significance, and their impact today
Well-posedness of boundary layer equations for time-dependent flow of non-Newtonian fluids
We consider the flow of an upper convected Maxwell fluid in the limit of high
Weissenberg and Reynolds number. In this limit, the no-slip condition cannot be
imposed on the solutions. We derive equations for the resulting boundary layer
and prove the well-posedness of these equations. A transformation to Lagrangian
coordinates is crucial in the argument
On the Tutte-Krushkal-Renardy polynomial for cell complexes
Recently V. Krushkal and D. Renardy generalized the Tutte polynomial from
graphs to cell complexes. We show that evaluating this polynomial at the origin
gives the number of cellular spanning trees in the sense of A. Duval, C.
Klivans, and J. Martin. Moreover, after a slight modification, the
Tutte-Krushkal-Renardy polynomial evaluated at the origin gives a weighted
count of cellular spanning trees, and therefore its free term can be calculated
by the cellular matrix-tree theorem of Duval et al. In the case of cell
decompositions of a sphere, this modified polynomial satisfies the same duality
identity as the original polynomial. We find that evaluating the
Tutte-Krushkal-Renardy along a certain line gives the Bott polynomial. Finally
we prove skein relations for the Tutte-Krushkal-Renardy polynomial..Comment: Minor revision according to a reviewer comments. To appear in the
Journal of Combinatorial Theory, Series
Symmetric factorization of the conformation tensor in viscoelastic fluid models
The positive definite symmetric polymer conformation tensor possesses a
unique symmetric square root that satisfies a closed evolution equation in the
Oldroyd-B and FENE-P models of viscoelastic fluid flow. When expressed in terms
of the velocity field and the symmetric square root of the conformation tensor,
these models' equations of motion formally constitute an evolution in a Hilbert
space with a total energy functional that defines a norm. Moreover, this
formulation is easily implemented in direct numerical simulations resulting in
significant practical advantages in terms of both accuracy and stability.Comment: 7 pages, 5 figure
Role of inertia in two-dimensional deformation and breakup of a droplet
We investigate by Lattice Boltzmann methods the effect of inertia on the
deformation and break-up of a two-dimensional fluid droplet surrounded by fluid
of equal viscosity (in a confined geometry) whose shear rate is increased very
slowly. We give evidence that in two dimensions inertia is {\em necessary} for
break-up, so that at zero Reynolds number the droplet deforms indefinitely
without breaking. We identify two different routes to breakup via two-lobed and
three-lobed structures respectively, and give evidence for a sharp transition
between these routes as parameters are varied.Comment: 4 pages, 4 figure
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