  In this work we analyze the motion of charged particles in the background of
the Kiselev geometry, which is considered here as an exact solution in the
context of power-Maxwell electrodynamics. As it is well known, one can use
either an electric ansatz or a magnetic one for the nonlinear electromagnetic
field. We study the motion of an electrically charged particle for an
electrically charged black hole and also for a magnetically charged black hole.
In the second case the motion is restricted to Poincar\'e cones of various
angles, as expected.
