Einstein diffusion relation
= Einstein diffusion relation
{c}
For translational drag coefficient $\zeta$ and <mobility> $1/\zeta$, <thermal equilibrium> requires $D=k_BT/\zeta$. This connects random displacement to dissipative response and is a form of the <fluctuation-dissipation theorem>. Combining it with <Stokes drag law> gives the <Stokes–Einstein relation>.