Overdamped Langevin dynamics
= Overdamped Langevin dynamics
Neglecting inertia in <Langevin dynamics> gives the overdamped limit.
For potential $F$ and mobility $\mathcal M$, overdamped Langevin dynamics is
$$
dX_t=-\mathcal M\nabla F(X_t)dt+\sqrt{2k_BT\mathcal M}\,dW_t.
$$
The matching noise amplitude is the fluctuation-dissipation relation that makes the Boltzmann density proportional to $e^{-F/(k_BT)}$ invariant.