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Fig. 3.14.
CRRES and Kakioka (
L
=1
.
26) data for the selected
Pi
2events.The
CRRES field components are respectively
B
ρ
: radial;
B
ϕ
: azimuthal, positive east-
ward;
B
z
: northward. The CRRES
E
ϕ
electric field component is dusk-to-dawn. Bot-
tom: The Kakioka magnetic field. After [99]
Multisatellite observations of substorm onsets on the nightside at 4
<
L<
7 revealed transversal waves with frequency depending on
L
that can
be attributed to the FLR. About 30% of the
Pi
2eventsontheEarthare
accompanied by nightside toroidal pulsations [98].
Analysis of low latitude magnetic data from the Combined Release and
Radiation Effects Satellite (CRRES) and at low latitude station Kakioka
(
L
=1
.
26) shows that the
Pi
2 pulsations appear when both CRRES and
Kakioka were on midnight. At CRRES the pulsations were detected in the
FMS-mode. An example of the
Pi
2 pulsations simultaneously observed in
space and on the ground is shown in Fig. 3.14 [99].
Using one of the reference works by Anderson [1], we cite only the tabulated
results of observations of MHD-waves in the magnetosphere. Basing the clas-
sification of magnetospheric perturbations on their periods and polarizations,
Anderson distinguishes 6 pulsation types: compressional
Pc
5, poloidal
Pc
4,
compressional
Pc
3, toroidal field line harmonics, toroidal
Pc
5 and incoher-
ent noise (see Table 3.1). Here
b
ν
,b
,
and
b
ϕ
mark, respectively, the radial,
longitudinal and azimuthal magnetic components.
Notes:
1. Compressional
Pc
3
,
4 relate to wave-particle interaction in the foreshock
and shock.
2. Toroidal
Pc
3
,
4 or multi-harmonics are field line resonance harmonics in
Pc
3
,
4 range. Compressional
Pc
3
,
4 is a driver (coupling with the funda-
mental toroidal mode).
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