[17] Now we consider in detail the diurnal dependencies of the
averaged values of TEC
I
, of the relative
dI/I
and of the absolute
dI
amplitudes of TEC variations for several quiet and disturbed days.
We start our analysis with the conditions of the midlatitude
ionosphere and then will note the features of the high-latitude
and equatorial ionosphere.
![]() |
Figure 1 |
![]() |
Figure 2 |
[19] Figures 1 and 2 show a smooth variation of
I
in quiet period with the TEC maximum reaching in the
daytime (1200-1600 LT). This behavior corresponds to the regular
TEC behavior obtained for a quiet period by the measurement of the
turning angle of the polarization plane of the VHF signals of
geostationary satellites [Afraimovich et al.,
1999; Davies, 1980] and also by
the measurement of the difference in the phase and group delay of
the GPS signals at two coherently related frequencies [Kotake et al., 2006; Mannucci et al.,
1998]. The absolute amplitude
dI
for MS and IS ionospheric irregularities varies within 0.1-0.7
TECU (TECU
=1016 m-2 ) and 0.01-0.03 TECU,
respectively, reaching maximum value also in the daytime.
[20] However, in disturbed conditions the character of
dI
dependence changes considerably. The value of the
absolute amplitude
dI
increases by a factor of
3-4 (Figure 1) or even by an order of magnitude (Figure 2),
reaching 3 TECU. At the same time the
dI
maximum
shifts to the time moment corresponding to the maximum deviation
of the
Dst and very high level
Kp=9. This effect is especially
visual during the main phase of the strong magnetic storm on 30
October 2003. Nevertheless, the maximum values of
dI
are observed mainly in the daytime.
[21] The diurnal behavior of the relative amplitude
dI/I
differs cardinally from the corresponding dependence
of
dI
. It is especially distinctly pronounced in
quiet conditions: the
dI/I
maximums for MS and
IS ionospheric irregularities are observed at night, not in the
daytime.
[22] In disturbed conditions the changes in
dI/I
are governed not only by diurnal behavior but by the magnetic
field as well. The vertical line in Figure 2 shows the moment of a
sharp peak of
dI
on 30 October 2003, when the
value of
dI
reached 3 TECU. This example shows
that the geomagnetic control of the amplitude of TEC variations at
high levels of the magnetic field disturbances appear to be more
important than the regular diurnal variations.
![]() |
Figure 3 |
![]() |
Figure 4 |
[24] Moreover, at high latitudes one can note a slight
difference in amplitudes
dI
and
dI/I
of TEC variations for ionospheric irregularities of
different scales (not more than by a factor of 2). At middle
latitudes this difference reaches an order of magnitude. This fact
indicates that there is a cardinal decrease in the declination of
the power spectrum of TEC disturbances due to the increase in the
amplitude of the small-scale part of the spectrum [Afraimovich et al., 2001].
![]() |
Figure 5 |
![]() |
Figure 6 |
![]() |
Figure 7 |
[27] In quiet conditions the nighttime dI/I values significantly exceed the daytime value by a factor of 3-5 at low and high latitudes and by a factor of 2 at middle latitudes. At a high level of magnetic field disturbance, the geomagnetic control of the TEC variation amplitude is even more significant than the regular diurnal variations.
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