Dangers
from space fields and bodies
In
geological history over several billion years the Earth went through
tens of ecological disasters, accompanied by processes of a varied nature
and intensity, leading to global rearrangements in its atmosphere,
lithosphere and biosphere. The boundaries of the megacycles associate
with the periods of revolution of the Sun about the center of the Galaxy
which gradually increased from 180 to 250 million years (My).
The
main disasters of geological periods, including times of mass fall-out
onto the Earth of cosmic bodies and the formation of strong geochemical
anomalies, correspond to the moments of entry of the Solar system into
streams of galactic matter. These moments during the last 700My
periodically changed from 19My in the Permian and Cambrian periods
to 37 My in
the Jurassic, Silurian and Upper Riphean. The periodicity of these
changes corresponds to the modern length of the galactic year which is
equal to 250My.
The
last time the Sun entered the jet stream (arm of Orion-Cygnus) about
3My ago and emerged from it 0.7My ago. Therefore, the raised
geological activity of the Earth and other planets of the Solar system
noted today, the excited state of the bodies of the asteroid belt and
also the strong “dustiness” of the interplanetary cosmic space
and the presence in it of a large number of meteorites, secondary
comets and asteroids with extremely short life times offer a complex of
mutually linked phenomena of residual character due to the recent
emergence of the Solar system from the stream.
In
turn, the Solar system will be exposed to the action of the objects of
the galactic stream in 18My.
Table
1. Sources
of cosmic disasters
|
Space
Fields
|
Space
bodies
|
|
Galactic
Electromagnetic Spiral Branches
|
Galactic
Streams of Matter
|
|
Cosmic
rays
|
Stars
|
|
Solar
irradiance variations
|
Comets
|
|
Solar
flares
|
Meteors
|
The
Solar System
Orbital
movements of planets stabilize the rhythms of the solar activity. The
solar activity and moon-sun tidal waves create the system of the main geophysical
processes in the shells of the
Earth.
Planets
have 99.5% of the moment of revolving momentum of the solar system (Mrev ). During the
movement of the large outer planets portions of the revolving momentum
of the planets are transferred to the Sun. The Sun’s periodic
accelerations create stable oscillations in solar processes, when the
Sun is revolving about the unsteady barycenter of the system.
Barycenter’s movement changes distances rj between celestial bodies of
the system and the center of gravity. That is why all bodies have the
same perturbated periods, but these periods have the different changes in
amplitudes, because of all planets and the Sun have various forces of
interaction, masses (mj ) and
constants:
rj
= (Mj rev / 2p mj )1/2(Tj)1/2
where
rj and Tj
- an orbital radius and
period, Mj rev - moment of
revolving momentum of a celestial body.
The
tidal influences of Mercury, Venus, the Earth, and Jupiter (parameter It ) and also the
movements of the Sun about the unsteady center of gravity of the system
(barycenter) during displacements of large outer planets, Jupiter,
Saturn, Uranus, and Neptune (parameter Mrev
) form the common
cycles of the Sun and Solar System, which can be found by the
investigation of periodical components of solar and terrestrial
dangerous processes.
Only
the planets of Mars and Pluto don’t really participate in forming
cycles of solar system because they have small parameters It
and Mrev
simultaneously (Table 2).
Table
2.Relative
planetary data, tidal interactions (It) of planets and the Sun, and their moments of revolving
momentum (Mrev
)
|
Planet
|
Distance
from Sun, r
|
Revolving
period, Trev.
|
Mass,
m
|
Mrev
=
mr2/T
£ %
|
It
=
m/r3
T
£ %
|
| Mercury
|
0.387
|
0.241
|
0.060
|
0.0373<<0.1%
|
1.03=15.6%
|
| Venus
|
0.723
|
0.615
|
0.820
|
0.6970<0.1%
|
2.17=32.9%
|
| Earth
|
1.000
|
1.000
|
1.000
|
1.0000<0.1%
|
1.00=15.1%
|
| Mars
|
1.524
|
1.880
|
0.110
|
0.1359<<0.1%
|
0.03=0.45%
|
| Jupiter
|
5.203
|
11.860
|
318.000
|
725.8000=61.5%
|
2.26=34.2%
|
| Saturn
|
9.539
|
29.460
|
95.100
|
293.7000=24.9%
|
0.11=1.7%
|
| Uranus
|
19.182
|
84.010
|
14.500
|
63.5100=5.4%
|
0.002<0.1%
|
| Neptune
|
30.058
|
164.800
|
17.300
|
94.8000=8.0%
|
6
10-4<<0.1%
|
| Pluto
|
39.439
|
247.700
|
0.002
|
0.0130<<0.1%
|
3
10-8<<0.1%
|
Solar
Variability and Climate Changes
The
complexity of the climate system is too great to create prognostic
physical-chemical models. The paradigm suggested the connects of the
stable oscillations in the mean annual air temperatures of the Northern
Hemisphere (NH) with periodic solar system processes. The
physical-empirical
model bases on the paradigm and empirical data of tree ring series
(1656-1967).
The
model’s prognostic ability to generate multiperiodic systematic
climate signals was verified by the sunspot series (1700-1997).
Coincidence of the main oscillations of the climate and the solar
activity can be seen better when 11-year solar periods of Wolf (W)
number are transformed in
22-year harmonics. The neighboring 11-year cycles of W correspond to the
different orientation of the magnetic fields of the sunspots (22-year cycle
of Hale). In the graph, the even-numbered 11-year cycles correspond to
negative W values and depressed temperatures and the odd-numbered ones
to positive W values and increased air temperatures.
The
model simultaneously generates the anomalies of decreased temperatures
coinciding with well known solar activity minima such as the Maunder (1645-1715) and Dalton
(1790-1840) minima (Fig.).

Fig.
Modeled Northern Hemisphere Temperature Anomalies (MNHTA) and Indexes
of Sunspot Numbers (SSN) which presented as Hale cycles (Berry, 1992).
MNHTA(PDI)
- Modeled NHTA on the Proxy Data Interval (PDI), 1656-1967, the
correlation coefficient is r =
0.407 for 1700-1997, its statistical significance at the 0.001
level.
References:
Berry,
B. L. 1992. Basic systems of geospheric - biospheric cycles and the
prediction of natural conditions. Biophysics, Vol.37, N3, 414-428, (in
Russian), Pergamon Press Ltd. Printed in Great Britain, 1993, 328-341
(in English).
Berry,
B. L., 1998. Regularities of natural cycles, prediction of climate and
surface conditions. Hydrol. Process. 12,
2267-2278.
|