  The behaviour of a relativistic electron-positron plasma in the pulsar
magnetosphere is investigated. The equation of the motion of the magnetospheric
plasma is discussed, from which it follows that, if the plasma particle radial
velocity ${V_r}>{c/{\sqrt 2}}$ (where c is the speed of light), the centrifugal
acceleration changes its sign and the particle braking begins. The stability of
the magnetospheric plasma with respect to the radially oriented potential
perturbations is discussed and the possibility of the electrostatic field
generation in this plasma along the pulsar magnetic field lines is shown.
