One example of this phenomenon was constructed by taking the limit of the linear interpolation of the dyadic rationals, which converges uniformly.
One example of this phenomenon was constructed by taking the limit of the linear interpolation of the dyadic rationals, which converges uniformly. A fluctuation-diffusion relation for this phenomenon sets the diffusion constant proportional to mobility times temperature. Considering only a drag force and a random force of zero mean lets this phenomenon be modeled by the (*) Langevin equation. Only when the temperature of the pawl is higher than the paddle can work be extracted from this process in a thought experiment of Feynman. The average displacement of a particle in this process is proportional to the square root of the time, as in a random walk. For 10 points, name this process modeling the random motion of particles in a fluid.
One example of this phenomenon was constructed by taking the limit of the linear interpolation of the dyadic rationals, which converges uniformly.
Brownian motion [or Wiener process]