The planetary system

In the preceding text, a link was observed between the occurrence or otherwise of several plant species in the meadow and the revolution of the earth around the sun.
For this purpose, we will first dwell on our assumption of the existence of various types of waves.
If we run two slightly differing waves, x and x+m, around a circular orbit, these might interfere and consequently display beats. These beats will have to link up at all times alongside the orbit for the flow to go on. In-between two beats there is a wave package (G). If we choose a larger circle and use the same waves, a whole number of wave packages (nG) will have to be added to ensure the interfering waves will remain intact.
The radius of the circle becomes ppc45.gifbigger.
The beat time (z) of the two interfering waves, x and x+m, can be deduced from : :

ppc46.gif

Regular repetition of this principle leads to an entire system of circles alongside which the waves can freely run. It seems an interaction like this can be quite stable the more so if some harmonic waves cooperate.

fig-0.gif


The procedure described is applied to the waves found in the three groups of plant species in the meadow.
According to figure 3 the following periods apply: wood : 4 years, ruderal : 3 years, meadow : 3.5 years,
The following wave packages may occur:

wave 1wave2combinating package
(years)(years)(years)
43 12
33.521
43.528

As an illustration, we will make cycles using the wave package of 12 years (G12).
In table 3 , under A, one wave package is added to what precedes. Gradually, longer and longer chains develop by which circular orbits can be formed. In this case, the revolution of a chain with n-links is 12n years.
Under B (table 3 ), the revolutions of the inner planets are indicated where they suit best. All inner planets will find a place on the condition that row A is divided by 100.
This does not alter the above principle in any way.

The earth, however, and particularly Mars, do not really fit into the table. These two planets can better be described using G21. Consequently, 1.05 years and 1.89 years, respectively, will be found as revolution.
This demonstrates a connection between the behaviour of the plants in the meadow and the revolution of the earth around the sun.


 
Titius-Bode


The data under A and B (table 3 remind us of the law of Titius-Bode. The connection with it is made by the "distances" mentioned under C :
ppc47.gifyears.

In the 18th century already, Titius (1729-1796) was aware of the interrelation of the planets. With a simple direction he was able to accurately indicate the ratio between the distances of the planets to the sun.( See Cambridge page 162,254 and also Menzel, Astronomy, chapter 15 ). (see literature).
To find the ratio, take 0 and the number 3 and multiply it constantly by 2. However (and here it comes): only after adding 4 to it, will it be in line with the observations D and E.( table 3 ).
Why such a peculiar way?

By this, I now think he wished to express the following:
The waves (the number of 3 multiplied constantly by 2) that created the planets, emanated from a swollen sun which later on shrunk to the size we now know (add 4).

When the protosun ignited, it became overheated to such an extent that it swelled to 'the Orbit of Mercury'. It then made such a huge turning and vibrating magnetic field (whose lines of force are perpendicular to the equatorial surface of the sun) that electric cycles were formed, found in the, partly emitted, matter on the equatorial surface. Electric cycles (as described above) sometimes lay the foundation for the origin of planets.

Actually never "the swollen sun" did occur. Yet table 3 refers to the Law of Titius-Bode. ( table 3 ).
In this context "add 4" may mean "add 4 to more waves".
However, we don't know which waves have to be increased in number by 4.

Titius' method can be linked to the table although initially two differing issues are at stake:

revolutions and distances.

Yet we can do so, because Titius describes an 'accidental' result of the distances to the sun which had been fixed in the planet orbits through interference of two waves.

The planet orbits are fundamental, the distance to the sun a result.

More than other ones, planet orbits that are established by more than two interfering waves, will have a preference for forming planets. If the beats are locally more or less linked up to each other, a point of rest may be formed on the circular orbit where matter will gather. The number of possibilities is nonetheless restricted as other requirements should also be met.
However, there will be a certain regularity in distance (Titius) among them as we are dealing with harmonic waves.
Our starting point, i.e. waves of 4 years, 3.5 years and 3 years, concerns waves that already consist of wave packages. They were formed out of the interference of waves of 4.95 years, 3.36 years and 2.71 years. These appear in twos in the sun wind (see figures 6 and 8 ) and cause beats of 6 years, 10.5 years and 14 years.
When pursuing this line and having G21 and G28 cooperate with each other, the following applies:

ppc48.gifyears, the built-up 'fundamental'

Using G21 and G28 it is possible to describe all outer planets.

We are actually dealing with a Fourier synthesis which leads to circular, tranquil orbits assembling matter.

The calculations often involve nice whole numbers which is due to our choice of unit: one of the components of the system, namely the revolution of the earth (1 year).
Titius, too, made use of this.

The data described enable us to construct a working model of the planetary system which can serve as background for any future research.
 
Calculation of revolutions

Suppose that during ignition of the sun mixtures of hot gases have burst out, gases that formed the planets. Then the revolutions of the planets around the sun can be calculated.

In the preceding text, we observed several waves as well as wave packages of 12 years, 21 years and 28 years and later on also of 6 years, 10.5 years and 14 years.

A characteristic feature of these wave packages is that they contain several of the factors 2, 3 and 3.5. At the top of table 4 we have included some more wave packages that meet these conditions : (84/2 , 84/3 , 84/4 , ... , 84/n). Using the list of whole numbers in the table and multiplying them, we will attempt to calculate the revolutions of the planets.

For example, multiplying 10.5 in the upper row with 10 in the same column, yields 105 which is found in column labelled T.B., while the column next to it mentions the number of 100, which refers to the desired revolution around the sun. So the number of 105 is quite a close calculation of this revolution with a whole number of wave packages. The same applies for 14 x 600 = 8400, while the column next to it mentions 8401, Uranus. But it also goes that 10.5 x 800 = 8400. There are many possibilities.

The numbers calculated must still be multiplied with 10-2 to find the revolutions in years. Using the numbers in bold we have calculated column T.B.

Initially it was said that by adding nG wave packages to a certain circular orbit, the
radius of the circle will become ppc47.gif bigger.

There is a connection between the two, through nG . The rays of the planet orbits meet the Law of Titius-Bode, but this means the revolutions around the sun must also meet this Law. The column of numbers in bold is the Law of Titius-Bode.

In formula:

planetfactors in distance | revolution
n + 24 + 3   2 n

It is a known fact that by doing so it is not possible to find Neptune. This Law indicates the number of wave packages that are on the various planet orbits but says nothing about the lengths of the wave packages involved.

The Law of Titius-Bode is a simple description of the planetary system insofar as it concerns the distances and revolutions of the planets. This Law may even be seen to be a cryptogram concerning the generation of our planetary system. This may be read from table 4 Obviously Pluto also takes part in the Kuiper-belt.

If we only use the Law of Titius-Bode in table 4 , the revolutions of the small planets are found on the left side of the dark line, while those of the large planets are found using the numbers to the right of the dark line.

The waves and wave packages on the left can be primarily characterised by a wave of

6  10-2 years

and those to the right by a wave of

7   10-2 years.

Apparently, two types of waves were of influence on the origin of the planetary system. In one spot, in the overlap (at the dark line near 14) they had such an opposing effect on each other that only debris could be formed: the Planetoids.

During the formation of the planetary system a similar dangerous situation existed in the neighbourhood of the Earth. According to table 4 , the revolution time of the Earth around the sun may be approximated by means of G12 and G21. In this region these sets of waves easily may counteract each other. They may form either debris or two planets of different origin close together. The latter may only take place by a slow accumulation of the various elements present in the rotating cloud. Such a beautiful planet like the Earth can only come into being in a quiet environment. Therefore the existance of the Earth and its large Moon is something special, a particularity of our planetary system.

 
Planets and Plants

To compute the true distances of the planets to the sun in kilometres, all terms of Titius-Bode's law must be multiplied by one and the same number :

150     10 5 (in this Law, the Earth is already 10).

According to table 4 , however, the revolutions of the various planets also complies with the Law of Titius-Bode. One would expect that these too would have to be multiplied by one number to find the revolutions. However, looking at table 4 we can see that for every planet a different wave or different wave package must be used to obtain the correct revolution. These can be harmonised by positioning the waves and wave packages on the planet orbits with the speed of light (9460 109 kilometres a year). We can then use the waves and wave packages to bring the planet concerned to the revolution appropriate to it.

In doing so, it seems likely that glaring hydragon "light" and helium "light" both gave rise to fiercely trembling magnetic fields in the rotating cloud. By reflection standing waves may have come into being.

All planets are now revolving around the sun in the same direction and the angular momentum has been transferred onto them. It is impossible for the sun to make a catastrophic pirouette.

In general all suns flaring up will also try to evade this somehow. It seems that the most obvious way to do so is to create a double star as this is often found. To create a stable planetary system a few more additional conditions have to be met.

Part of the trembling magnetic field is still present in the solar wind. According to Rozelot (5) the solar wind contains the following waves:

0.137, 2.19, 2.83, 3.75, 4.9, 7.03, 8.56, 10.2, 12.2, 14.8 years.

We recognize the four numbers printed in bold. We have come across the three numbers underlined through the periodic behaviour of some meadow plant species. This brings us back to the beginning of this article.


 
Summary

The Law of Titius-Bode approximates both the distances of the planets from the sun and their times of revolution around the sun. The first step of the Law suggests that the larger planets have been formed first and after that the smaller planets have come into being.

The Earth scarcely escaped from destruction.

The Law of Titius-Bode turned out to be a cryptogram referring to the evolution of our planetary system. The behaviour of some groups of plants on Earth indicated how to unriddle the mystery.

see table 4

see table 5


I am greatly indebted to mrs. A.M. de Vries who has helped me for many years and co-ordinated many things.
I would also like to thank mr. H.C. Timmner for his help in writing the last part of this article

 
EPILOGUE

Looking back on the entire article, it appears that one and the same principle is discussed over and over again.
A certain amount of energy which remains constant for some time, is subdivided into energy waves. The cooperation between several of these waves sometimes results in the formation of various planets and sometimes in the adjustment of various plant species to one of those planets.
Nature departs from a number of simple, basic principles which are applied in various ways. As a result, many highly ingenuous structures are formed with a mutual relationship which is scarcely perceptible or not at all.






CONSIDERATION

With 10 figures we calculate everything.
With 30 letters we can describe all languages.
With 90 elements we can visualize all chemicals.
With 270 principles an image of the universe is formed.
With all this extensive knowledge we still know nothing.






 
OUR EXISTENCE


We humans, who find ourselves in overpopulated, thin, locally unstable plates
- the continents -,
grating in-between, floating on boiling, liquid rock
- the magma -,
congelations that are partly flooded by masses of water continuously threatening us
- the oceans -,
in which the crumbly crusts surge up and down because of the gravitation exerted on our insignificantly small, elastic celestial body
- the earth -,
a celestial body which together with a number of congeners
- the planets -,
constantly revolves around its swinging, slanting axis thereby blazing an elliptic trail around a moderately hot sun of average size
- of which millions exist -,
although we have revolved with this sun and its followers only twenty times in
4.5 billion years ( 4.5 . 109 ) around the centre
- the black hole -,
of a perfectly ordinary galaxy
- of which also millions exist -,
a galaxy moving in a space
- the universe -,
a space, which even with the speed of light seems boundless and unfeasible to travel across,
we humans should not think so much of ourselves.
Our existence is insecure.
We are of no meaning whatsoever in this universe.























table 1. Summary of the Formations and classes of the various plant communities


Formation class

I 1 to 6 water plants and plants on boundary water - land

II 7 plants in chasms and on walls
ppc49.gif III 8 to 13 pioneer vegetations annual
IV 14 to 15 pioneer vegetations perennial
V 16 to 18 pioneer vegetations perennial, on distburbed soil, nitrogen-rich
ppc50.gif VI 19 pioneer vegetations, high groundwater, mostly constantly wet
VII 20 to 23 plants on grass land, dry, above groundwater
VIII 24 to 25 plants on grass land, humid, influence of groundwater

IX 26 to 28 plants on peat; vegetation rises and falls according to level of groundwater
ppc51.gif X 29 to 30 plants on high moor peat bulges, heath, matgrass lands
XI 31 brushwood communities, soil dry and lime-rich
XII 32 to 34 shrubs
XIII 35 to 38 woods




TABLE OF PLANTS WHICH WERE FOUND IN 9 YEARS,
ARRANGED ACCORDING TO CLASS



ruderal, wood and meadow
achillea millefolium water milfoil
agrostis stolonifera
dactylis glomerata cocksfoot
epilobium hirsutum hairy willow-herb
poa pratensis meadow grass

ruderal and meadow
agrostis tenuis
elytrigia repens couch grass
sedum acre stonecrop
sonchus palustris sow thistle
vicia sativa augustifolia vetch (small-leafed)

ruderal
artemisia vulgaris
bromus mollis brome (soft)
capsella bursa-pastoris shepherd's purse
chenopodium album goosefoot
cichorium intybus chicory (wild)
cirsium vulgare thistle (spear)
cirsium arvense thistle (field)
digitalis purpurea foxglove
dipsacus fullonum teasel (wild)
juncus effusus soft rush
lamium purpureum dead nettle (purple)
lamium album dead nettle (white)
mentha rotundifolia mint (white)
oenothera biennis evening primrose
papaver dubium poppy (small)
petasites hybridius butterbur
polygonum persicaria redshank
ranunculus arvensis buttercup (field)
sisymbrium officinale hedge mustard (ordinary)
solanum nigrum nightshade (black )
solidago canadensis
sonchus arvensis milk thistle (field)
tanacetum vulgare tansy
thlaspi arvense pennycress
utrica urens stinging-nettle (small)

ruderal and wood
aegopodium podagraria goutweed
alliaria petiolata garlic mustard
bromus sterilis brome (thin)
calystegia sepium convolvulus (hedge)
galium aparine cleavers
glechoma hederacea ground ivy
lamium maculatum dead nettle (spotted )
lolium perenne rye-grass (English)
lychnis flos-cuculi cuckooflower (day)
origanum vulgare marjoram (wild)
poa trivialis meadow grass (rough)
ranunculus repens buttercup (creaping)
rumex obtusifolius sorrel
stellaria graminea chickweed
urtica dioica stinging-nettle (large)
vicia sepium vetch (hedge)

wood
acer pseudoplatanus maple
alnus glutinosa alder (black)
betula pendula birch
corylus avellana hazel
doronicum willdenowii doronicum (bastard)
heracleum mantegazzianum hogweed (large)
hesperis matronalis dame's violet
populus nigra ( poplar Lombardy)
quercus robur oak (summer)
rosa villosa rose (rose-hip)
rubus idaeus raspberry
salix caprea willow (wood)
salix aurita willow (eared)
salix alba willow (white)
stellaria holostea chickweed (large flowers)

wood and meadow
anthriscus sylvestris cow parsley
crepis paludosa
epilobium parviflorum loosestrife (small-leafed )
eriophorum vaginatum cotton grass (annual)
heracleum sphondylium hogweed
hieracium lachenalii hawkweed
holcus lanatus
hypericum perforatum St John's wort
iris pseudacorus iris (yellow)
myosotis scorpioides forget-me-not (marsh)
plantago lanceolata plantain (small-leafed)
prunella vulgaris self-heal
ranunculus acris buttercup (kingcup)
ranunculus ficaria lesser celandine
rumex acetosa sorrel (field

meadow
angelica sylvestris angelica
bellis perennis daisy
cardamine pratensis pratensis lady-smock
centaurera pratensis knapweed
cerastium semidecandrum mouse-ear (sand)
chrysanthemum leucanthemum moondaisy
crepis biennis
epilobium palustre loosestrife (marsh)
equisetum palustre
festuca pratensis bluegrass
hieracium aurantiacum hawkweed (orange)
hieracium caespitosum hawkweed (meadow)
juncus subuliflorus rushes (marsh)
lotus uliginosus bird's-foor (marsh)
myosotis ramosissima forget-me-not (rough)
phleum pratense
potentilla tabernaemontani tormentil (spring)
potentilla reptans potentilla
ranunculus lingua buttercup (big)
satureja acinos thyme (rock, small)
sedum album sedum (white)
taraxacum dandelion
trifolium pratense clover (red)
trisetum flavescens oat-grass (golden)
valeriana officinalis valerian

plants unclassified
ajuga reptans
alchemilla vulgaris
borage officinalis borage
cardamine hirsuta meadow cress (small)
crocus vernus tomasinianus crocus
festuca rubra
geranium molle wild geranium
hypochaeris radicata
lunaria annua satinflower
malva moschata moschatel
pulmonaria officinalis lungwort
sempervivum tectorum houseleek


LITERATURE
1. V. Westhoff, P.A. Bakker, C.G. van Leeuwen, E.E. van der Voo. Wilde planten. Vereniging tot Behoud van Natuurmonumenten in Nederland
2. V. Westhoff and A.J. den Held. Plantengemeenschappen in Nederland. Thieme & Cie Zutphen 1975.
3. Heukels-van Ooststroom. Flora van Nederland. (16th edition), Wolters-Noordhoff, Groningen, 1970
4. Cambridge encyclopedie van de Astronomie, Natuur & Techniek. Maastricht, 1978
5. J.P. Rozelot Solar variability and Climatology. Proc. Symp. Seismology of the Sun and Sun-like Stars. Spain, 1988, ESA SP-286 (December 1988)
See also :
7. H.D. Foth Fundamentals of Soil Science. Wiley and Sons, New York 1984
8.Moderne Sterrenkunde, stichting Teleac Utrecht 1980/1981
Hoofdstuk 7, Planetenonderzoek blz 184-189


ADDRESSES

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