Data of the EISCAT and IMAGE magnetic observatories chains in combination w
ith data of three Russian observatories (St. Petersburg, Borok and Moscow)
were used to determine the eastward and westward electrojet dynamics in the
course of magnetic storms. During the storm main phase and maximum substor
m intensity the eastward electrojet is located at latitudes lower than usua
l. During intervals between substorms the westward electrojet centre shifts
equatorwards as Dst increases. At a substorm maximum the westward electroj
et widens polewards. The spectrograms of precipitating electrons and ions o
f auroral energies obtained onboard the DMSP F8, F10 and F11 satellites all
ow to connect the regions of the electrojet location with characteristic pl
asma structures at ionospheric altitudes. The eastward electrojet in the ev
ening sector is located in the region of diffuse electron precipitations. T
he electrojet centre coincides with the latitude of an energy flux maximum
of auroral protons. In the course of substorms the westward electrojet at t
he nightside is located at latitudes of both diffuse and discrete electron
precipitations. The electrojets and plasma region boundaries are mapped to
the magnetosphere. The paraboloid model of the magnetosphere is used here.
The influence of paraboloid model input parameters on the dayside cusp lati
tude, on the ionospheric boundaries between open and closed as well as dipo
le-like and tail-like field lines is considered. It is shown that tail curr
ents influence magnetic field line configuration in the nightside magnetosp
here stronger than the ring current. (C) 1999 Elsevier Science Ltd. All rig
hts reserved.