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James Hilton's Home Page
[Research] [Teaching]
[Publications] [MANIFEST]
Research
Computational Fluid Dynamics
Currently I'm working in the Complex Systems group in Trinity College Dublin.
My research focuses on rheology models of non-Newtonian fluids and granular
media. I'm using continuum models to simulate systems with various constitutive
stress relations for comparison to both theory and experimental work . I'm also
simulating two phase systems, such as fluid and gas systems, using the level set
method.
I'm developing software for the simulation of non-Newtonian viscoelastic
fluid flow, using a ‘log-conformation’ representation and using it to investigate stresses induced on objects in streams of these viscoelastic fluids.
I'm also working on extensions to the level set method to include interfacial
forces in complex fluids.
Here's a nice picture of a
von Karman street
developing behind a cylinder using my software. The Reynolds number is 10,000
for this simulation and the colour scale shows the magnitude of the velocity:

Video here, you'll need the XVid
codec.
Microfluidics and Bubble Dynamics
Two phase systems, such as gases and liquids, can be modelled using the
level set method, (pioneered by Sethian and Osher). The method provides a
very natural way to handle the changing topology of the system as the interface
is represented as the zero of a scalar level set value. This value is less than
zero on one side of the interface and greater than zero on the other. This
scalar obeys a simple advection expression, and the motion of the interface can
easily be tracked by finding the zero value at each timestep. Another good
property of the level set method is the ability to easily determine the
interface curvature (as the normal of the interface is given by the gradient of
the level set). This allows the addition of surface tension to the method, and
so one application of this is for modelling of bubble dynamics. At the
moment I'm using this method for simulating microbubble generators. The bubble
size is highly dependant on the geometry of the system, and we're currently
investigating how the various parameters of the setup determine the resulting
bubble dimensions. The simulation software has just been updated to handle 3D
geometry, here's a cross section of the bubble generation in a microfluidic
bubble generator. The system dimensions are 1cmx2cm:

3D Video here (mpg).

Video here (mpg).
Elastic Solid and Fluid Interaction
I'm also developing a way of simulating both elastic solids and liquids in the same
system. This means you can do interesting things like simulate interacting
particles in air currents and model sedimentation effects. Of course, the
particles can be any shape, such as the 'U' shapes below. The elasticity
constant can be set to a low value, to give some nice dynamics:
Video here, you'll need the XVid
codec. Furthermore, the solid phase can also be determined at each timestep by
the system itself, i.e. you can simulate complex liquids which have a solid
phase, such as Bingham plastics. Below is a video in which the solid phase is
temperature dependant, so the solid melts above a certain temperature. The
square is the initial solid, and it sits on a fixed heat source. The blob that drops off behaves elastically:
Video here, you'll need the XVid
codec. Charged Droplets
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The sequence of pictures on the left show the formation of
Rayleigh jets forming for charged droplets in 3D, using the level set
method.
Rayleigh, while studying droplet formation in
thunderclouds, proposed that a droplet of a radius r, with charge q, and
surface tension s
remains stable as long as the
fissility of the droplet remains below one. The fissility is given as X =
q²/(64p²esr³).
If the droplet fissility is above the critical limit a small perturbation
will cause the droplet to deform into an ellipsoid and eject the excess
charge in jets along the ellipsoid axes. Shown to the left
is a droplet with a net charge over this limit (right hand side) and under
this limit (left hand side) at increasing timesteps. The droplet on the
left hand side is stable, and oscillates. The droplet on the right hand
side is unstable and ejects jets. The simulation starts with the droplets
elliptical to mimic an external perturbation. The the liquid phases are
air and water. |
Computational Magnetics
During my research I found a few new useful magnetic designs. These include a new cylindrical magnetic field source with a uniform
field more homogeneous than any existing design. Some designs based on ‘flux
sheets’ were also developed, which could generate either a uniform field
gradient or regions of constant field and field gradient product. Several of
these designs were commissioned and the computational simulations exactly agreed with the
fields measured.
I developed automated finite element simulation software, using the ‘IEEE
Japan’ magnetostatic vector potential formulation. The program included various
optimization techniques for solving inverse design problems such as sequential
golden section searches and simulated annealing etc. You can download it
here, along with some scripting examples. The program also
includes a new computational algorithm I developed, based on the charge model,
which can calculate fields from arbitrary magnetic structures composed of hard
magnetic materials. The program can handle any shapes of hard material, since it
sums over the boundary surfaces.
Teaching
(Links below to detailed information are restricted to local users).
Publications
J. Hilton and S. McMurry, “Halbach Cylinders with Improved Field Homogeneity and Tailored Gradient Fields”
IEEE Transactions on Magnetics, Volume 43, Issue 5, May 2007, Pages
1898-1902
[Link]
N. B. Chaure, F. M. F. Rhen, J. Hilton and J. M. D. Coey, “Design and application of a magnetic field gradient electrode”,
Electrochemistry Communications, Volume 9, Issue 1 , January 2007, Pages 155-158
[Link]
P.A. Dunne, J. Hilton and J.M.D. Coey, “Levitation in paramagnetic liquids”,
Journal of Magnetism and Magnetic Materials (article in press)
[Link]
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