Nonlinear Dynamics
Items for this website e.g. publications,
links, comments and opinions can be
e-mailed to Roumen
Anguelov at
roumen.anguelov@up.ac.za
Project: Stationary states of diffusion aggregation
models
1. One dimensional
simulation showing the evolution in time of the solution to the aggregation
diffusion equation where the attractive kernel has compact support. The initial
condition is given by a random distribution.
(Comp1D)
2. Two dimensional simulations showing the side and top views of the
evolution in time of the solution to the aggregation diffusion
equation with a compactly supported attractive kernel. The
initial condition is given by a random distribution. (Patt2Dtop and Patt2Dside)
3. Two-dimensional simulation showing the top view
of the evolution in time of the solution to the aggregation diffusion equation,
given a time dependent attractive kernel with infinite support. An exogenous
force, given by a cluster of four Gaussian functions situated at the bottom
left corner of the domain, is incorporated into the model. The final state of
the simulation is a single swarm. This is a result of the attractive kernel
having infinite support, preventing the formation of a stationary state with
multiple swarms. (ChangingW2DInf)
4. Two-dimensional simulation showing the top
view of the evolution in time of the solution to the aggregation diffusion
equation, given a time dependent attractive kernel with compact support. A
randomly distributed exogenous force is incorporated into
the model. The social attractive force is initiated
at the start of the simulation, in absence of
the exogenous force. At time 0:37 in the
video, the social attractive force is suspended and the exogenous force
is initiated. At time 1:03, the attractive force is initiated again,
while the exogenous force is suspended. This process allows for
swarms to break away into a random distribution and then aggregate
again over time, forming different patterns. The initial condition is
given by a random distribution. (ChangingW2DComp)