[6] As noted above, the state of the near-Earth space is
governed to a large extent by solar events and processes with
different characteristic times. These events and processes are
accompanied by considerable changes in basic solar factors
affecting the near-Earth space. First of all, these are X-ray and
extreme ultraviolet radiation of the Sun ( l 1200 Å) whose
absorption in the Earth's upper atmosphere leads to ionization of
neutral atoms and molecules, i.e., formation of the ionospheric
plasma at altitudes above
~60 km
[Ivanov-Kholodnyy and Nikolskiy, 1969].
The second factor is the solar wind which
consists of fluxes of electrons and protons (whose velocities at the
Earth's orbit amount to 300-1000 km s-1 ) with a frozen-in
interplanetary magnetic field. The solar wind determines to a great
degree the geometry and energetics of separate structures of the
Earth's magnetosphere which, in their turn, exert an influence on
the ionosphere formation
[Akasofu and Chapman, 1974].
At last,
one more factor typically accompanying solar flares should be
mentioned. This is fluxes of highly energetic electrons ( E
20 keV)
and protons ( E
20 MeV). These fluxes also affect the state of the
Earth's magnetosphere and, eventually, ionosphere
[Mizun, 1980].
[7] It is also well known that, owing to the presence of the ionosphere, the near-Earth space contains two global natural resonators where electromagnetic waves (EMW) of definite frequencies can propagate at very long distances almost without attenuation. The first resonator is the space confined between two conducting quasi-spherical surfaces, one of which is the Earth's surface and the other is the ionosphere base [Balokh et al., 1977]. Its fundamental resonance frequencies are above 6 Hz, and the main source of its excitation is intraatmospheric thunderstorms [Borodin and Kolesnik, 2001].
[8] The second quasi-spherical resonator represents the space
confined between the lower ionosphere and the region of the
ionosphere that lies above the basic maximum of electron
concentration ( h 1000 km)
[Belyaev et al., 1989].
This resonator
is referred to as the Alfvén resonator, and its resonance frequencies
lie in the range
<6 Hz. The sources of its excitation are in the
Earth's atmosphere and magnetosphere.
[9] The next group of prerequisites is related to specific
features of the frequency rhythms of separate systems of a human
organism. First of all, these are frequency rhythms of the human
brain. It is known that a human brain generates the electromagnetic
fields in the frequency range
1 40 Hz. They have a resonance
character and form
a,
b, and other biorhythms
[Dolgato and Kholodov, 1987].
In particular, for the
a rhythm the resonance
frequencies lie in a range of 8-12 Hz, and for the
b rhythm the
resonance frequencies are in a range of 14-21 Hz. Thus the
frequency range of the electromagnetic fields generated by the
human brain is rather close to the frequency range of the Schumann
resonator.
[10] The cardiovascular system of a human organism is also able
to generate electromagnetic fields in the range characterized by a
set of harmonics having different frequencies and intensities
[Amoff, 1984],
with the fundamental frequency being in the range
0.8 2.5 Hz. It is evident that, by the frequency range, the
biorhythm of the cardiovascular system of the human organism is
similar to the range of the Alfvén resonator.
Powered by TeXWeb (Win32, v.2.0).