Let us consider a plasma in a uniform, constant magnetic field . The equation of motion for an electron in this environment is
where is the elementary charge, is the speed of light, is the electron mass, is the external electric field and is the time between collisions (see Spitzer Resistivity). We are interested in the steady state solution, so we can drop the time derivative. We also want to get rid of as many of the dimensional parameters, so we can massage the equation into the following form
where and is the Bohm parameter. For the component of the velocity and electric field parallel to the magnetic field we get
For the component perpendicular to the magnetic field we get
The current density is given by , where is the number density. The magnitude of the current density changes with the angle of the electric field relative to the magnetic field, and it can also be misaligned with the direction of the electric field. For this reason the conductivity in this case is a tensor. When the plasma is said to be in the resistive regime, when it is said to be in the ambipolar regime, and when it is said to be in the Hall regime.