In general, the diffusion coefficient is roughly equal to the product of the velocity at which a particle moves between collisions, and the mean free path between collisions. In the case of a plasma, the velocity at which particles move is the thermal velocity

 v_{th} \approx \sqrt{\frac{k T}{m}}

where  k is the Boltzmann constant,  T is the temperature and  m is the mass of the particles. The mean free path can be estimated in the following way. If we assume only interaction between neighbouring particles, and we imagine particles with charge  q flying next to each other with impact parameter  b , then the impact parameter at which the deflection angle is of order unity is

 b_{c} \approx \frac{q^2}{k T}

The mean free path for such an interaction is

 l \approx \frac{k^2 T^2}{q^4 n}

where  n is the particle number density. The diffusion coefficient is therefore

 D \approx \sqrt{\frac{k T}{m}} \frac{k^2 T^2}{q^4 n}

We note that the assumption of interaction from nearest neighbours is not entirely justified. At a larger distance the electric field decreases on the one hand, but the number of particle increases, so that different radii have similar contribution, and this introduces a logarithmic correction to cross section.