Published by Patrick Mutisya · 14 days ago
Brownian motion is the erratic, random movement of tiny particles (typically of the order of a few micrometres) when they are suspended in a fluid (liquid or gas). The motion is observable under a microscope and provides direct evidence for the kinetic theory of matter.
According to the particle model, a fluid consists of a huge number of molecules moving constantly in random directions with a range of speeds. When a suspended particle is present, it is continuously struck by these molecules. Because the impacts are:
the net force on the particle fluctuates rapidly, causing it to jitter about its original position. This jitter is what we observe as Brownian motion.
The mean square displacement \$\langle x^{2} \rangle\$ of a particle undergoing Brownian motion in one dimension after a time \$t\$ is given by:
\$\langle x^{2} \rangle = 2 D t\$
where \$D\$ is the diffusion coefficient, related to temperature \$T\$, fluid viscosity \$\eta\$, and particle radius \$r\$ by the Stokes‑Einstein equation:
\$D = \frac{k_{\mathrm{B}} T}{6 \pi \eta r}\$
Here \$k_{\mathrm{B}}\$ is Boltzmann’s constant.
| Observation | Interpretation |
|---|---|
| Particles suspended in a liquid move erratically. | Continuous, random impacts from moving molecules. |
| Motion becomes more vigorous as temperature rises. | Higher molecular kinetic energy → faster, more forceful collisions. |
| Smaller particles show larger displacements. | Force from each collision has a greater effect on a smaller mass. |
Brownian motion is a clear, observable phenomenon that demonstrates the particle nature of matter. It arises from the random, incessant bombardment of fluid molecules on suspended particles, and its characteristics (temperature dependence, particle‑size dependence, randomness) are all consistent with the kinetic theory of gases and liquids.