Brownian motion is random particle motion in a liquid or gas, typically modeled mathematically by the Wiener process.
Brownian motion is the random motion of particles suspended in a medium such as a liquid or a gas. In the traditional mathematical description, it is modeled by the Wiener process (often called “Brownian motion” itself). Physically, the motion appears as irregular fluctuations of a particle’s position within a small region, followed by relocation to another region; this repeats over time. This behavior is characteristic of a fluid at thermal equilibrium at a given temperature. In equilibrium there is no preferred direction of flow: the fluid’s overall linear and angular momenta remain zero over time. The particle’s kinetic energy is part of the fluid’s internal energy, consistent with the equipartition theorem, where translational, rotational, and vibrational molecular motions collectively contribute to the caloric component of internal energy. The phenomenon is named after Robert Brown, who observed pollen grains in water undergoing continuous jittery motion under a microscope. The underlying physical picture is that the particle is bombarded by molecules whose directions and impacts change rapidly, producing the seemingly random trajectory; because the full many-body dynamics cannot be solved directly, probabilistic models are used to describe the motion.
Brownian motion is random particle motion in a liquid or gas, typically modeled mathematically by the Wiener process.
In thermal equilibrium, Brownian motion has no preferred flow direction; overall momentum remains null over time.
The irregular trajectory arises from incessant, rapidly changing molecular bombardment, so probabilistic (statistical) models are used rather than exact many-body dynamics.
The random motion of particles suspended in a fluid (liquid or gas), typically modeled by the Wiener process.
A continuous-time stochastic process that serves as the standard mathematical model for Brownian motion.
A state of a fluid at a fixed temperature where there is no preferred direction of flow and macroscopic momentum remains zero over time.
A principle stating that energy is shared among degrees of freedom so that translational, rotational, and vibrational motions contribute to the internal energy.
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