This report requires report and source code.
PDF format.
Should include Introduction, maths model, result and discussion, conclusions, references.
aims for “computational modelling” but its OK to deviate own ideas
Code preferably
C/C++ python matlab/Octave, java, D, Fortran, Mathematica
Requirement can be found in attachement
Lecture notes can be found in
http://undergraduate.csse.uwa.edu.au/units/CITS4403/schedule.htm

CITS4403, Computational ModellingThe Hardy–de Pazzis–Pomeau (HPP) latticegas model”Pascal R BuenzliMay 2013TaskImplement the ‘HPP’ cellular automaton rule, which model a gas of colliding par-ticles. The HPP lattice gas automata is defined on a 2D square lattice. Particlescan move along the orthogonal directions of the lattice. Particles are associatedwith both a position on the lattice (lattice site), and a discrete velocity (four cardi-nal directions), i.e. the velocity with which the particle is assumed to haveenteredthe site (see Figure). An exclusion principle is assumed, which prevents more thanone particle to be at a same position with the same velocity. However, more thanone particle can be found at a lattice site if the particles have different velocities.Four bits of information in each site are enough to describe the system duringits evolution. For instance, if at timetthe lattice site atrhas the following states(t,r) = [1011], it means that three particles are entering the site along directions1, 3, and 4, respectively.The CA rule describing the evolution ofs(t,r)is usually split into two steps:collision and motion. The collision phase specifies how particles entering thesame site will interact and change their trajectories. During the motion phase,or propagation, the particles are actually moved to the nearest neighbor site theywere traveling to.The figure (right) illustrates the HPP rules:(a)a single particle has a ballistic motion until it experiences a collision(b) and (c)the two nontrivial collisions of the model: two particles experiencinga head-on collision are deflected in the perpendicular direction. In the othersituations, the motion is ballistic, that is the particles are transparent to eachother when they cross the same site.1

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