The Brownian motion was discovered in 1827 by the English botanist Robert Brown while observing pollen grains dispersed on the surface
of a liquid under a microscope. It originates from the countless collisions between the molecules of
the liquid and the grains. This phenomenon was particularly studied by Albert Einstein (1905) and later,
thanks to the experiments of Jean Perrin, it became essential proof of the atomic structure
of matter. These studies were then pursued from a mathematical perspective,
notably by Paul Lévy [01] and one of his students, Benoît Mandelbrot.
The Brownian motion of a particle
consists of a series of random displacements (in direction and magnitude) that are independent of each
other. The resulting structures give rise to generally difficult mathematical problems. For example,
Benoît Mandelbrot conjectured that the fractal dimension
of the envelope —white curve— of
two-dimensional Brownian motion —colored curve— was equal to 4/3, and this was proven
in 1999 by Greg Lawler, Oded Schramm, and Wendelin Werner [02].
This phenomenon is actually omnipresent: in Physics, Chemistry, Biology [03], certain industrial
processes, and even in the world of finance, where it serves as a model for the evolution of asset prices over time.
It is possible to study it in two and three dimensions on our computers
in the form of virtual experiments. To do so, we will place ourselves inside a rectangular (or
parallelepipedic) domain and arrange particles on a square (or cubic) lattice. These particles will
be of two types: on one hand, so-called light particles, initially animated with random
velocities in direction but of equal magnitude; they will be represented by small colored spheres. On
the other hand, so-called heavy particles, initially immobile; they will be represented
by small white spheres. Over time, collisions [04] will occur between all these particles,
and gradually, the heavy particles will be set in motion.
Synthesis of the four preceding virtual experiments.
We then observe that the heavier the white particles (Robert Brown's "pollen grains"), the less
easily they are set in motion by the colored particles (Albert Einstein's "molecules") [05].
[01]
Paul Lévy was a professor at the École Polytechnique.
[02]
Wendelin Werner received the Fields Medal in 2006 for this achievement.
[03]
This is, for example, how the molecules inside an animal or plant cell move, encounter each other, and thus interact.
[04]
Here, the impacts are assumed perfectly elastic, thus meaning that momentum is conserved.
[05]
Obviously the number of particles used as well as the mass ratio are very far from what is observed in nature.