Direct determination of IMF B-Y-related cusp current systems, using SuperDARN radar and multiple ground magnetometer data: A link to theory on cusp current origin
O. Amm et al., Direct determination of IMF B-Y-related cusp current systems, using SuperDARN radar and multiple ground magnetometer data: A link to theory on cusp current origin, J GEO R-S P, 104(A8), 1999, pp. 17187-17198
We analyze an ionospheric "enhanced convection event" in the cusp on Novemb
er 13, 1996, at 1900 UT, by using data of the SuperDARN radar, and of the I
MAGE, Greenland, MACCS and CANOPUS magnetometer arrays; and from other magn
etometer stations. The event occurs similar to 20 minutes after a transitio
n of the IMF B-Y component from positive to negative and an associated reco
nfiguration of the ionospheric electric potential pattern. The data allow a
n instantaneous two-dimensional view of the event in terms of the ionospher
ic electric and ground magnetic field. The "method of characteristics" is u
sed to obtain distributions of ionospheric conductances, actual ionospheric
currents, and field-aligned currents (FACs) for the interval under study.
Our results show that the region of enhanced convection observed by the rad
ar is associated with a region of low conductances, ranging only slightly a
bove the UV conductance values. However, owing to the strongly enhanced ele
ctric field, it produces enhanced westward flowing Hall and southward flowi
ng Pedersen currents. At the northern and southern borders of the enhanced
convection region, sheets of downward and upward FACs are observed, respect
ively, with magnitudes of around 0.5 A/km(2). The geometry of the current s
ystem resembles a DPY current system [Friis-Christensen and Wilhjelm, 1975]
. Using our results, we test alternative theories on cusp current origin th
at lead to different predictions of the relative location of the cusp curre
nt system with respect to the open-closed field line boundary. The location
of this boundary is inferred from DMSP F10 satellite data. The center of o
ur resulting current system is located clearly poleward of the open-closed
field line boundary, thus favoring the idea of Lee et al. [1985] that the c
usp FACs are caused by a rotational discontinuity of the magnetic field at
the magnetopause. In contrast, the idea of Clauer and Banks [1986] that a m
apping of the solar wind E-z component to the ionosphere is responsible for
the cusp current system is not supported.