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MAGNETOSPHERIC PLASMA
Β
Magnetopause
High pressure
Low pressure
Magnetosheath
.
SOLAR WIND PLASMA
Magnetosphere
MAGNETOSPHERIC PLASMA
φ
A
p
C
Β
Magnetopause
φ
2
High pressure
Low pressure
φ
2
∂ ϕ
.
SOLAR WIND PLASMA
φ
(a)
(b)
Fig. 3.7. Suggested scenario in which the large changes in the solar wind dynamic
pressure produces a unipolar FAC proportional to the azimuthal derivative of the
pressure perturbations (a) After Glassmeier et al. (1989). (b) A stepwise pressure
change and a bipolar system of FAC is proportional to the second derivative of the
pressure perturbation. After Kivelson and Southwood (1991)
eastern stations which corresponds to the tailward motion of the convective
perturbation.
The equivalent current system constructed from these data and supple-
mented by records from the Greenland station chain is shown in the upper
MIK
ROS
KIR
NAT
PIT
MIK
ROS
KIR
NAT
PIT
0730
0740
0740
0740
0740
0740
0740
(a)
(b)
Fig. 3.8. Simultaneous NS - (upper part of panel (b)), and EW - magnetograms
(lower part) from the Scandinavian magnetometer array of stations (a) [23]
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