DIAGRAM No.1
In the upper half the diagram represents a sectional view of the P-charge of a capacitor of
5 000 µF capacity, connected to a tension 1 V, and its energy components - ES, EZ and interzones.
The energy components of all kinds of P-charges copy the shape of the source. To simplify
calculations of energy spaces for objects of irregular shapes we will consider them as having
a spherical shape though they vary a shape of sphere. The ES of the given capacitor has thus
the form of a sphere 12cm in radius. For lucidity we will specify, also for the other diagrams,
only the radii of energy spaces. Their volumes can be readily calculated. The EZ and the
interones in the form of envelopes copy the shape of the ES, in our case that of a sphere.
Their radius cannot be determined, as they are lost in the energy components of other P-charges.
Capacitors can be used in a large number of various experiments. It is interesting to follows the movement of energy components when changing voltage on the terminals. Also interesting is to move slowly two charged capacitors one towards the other and watch how at the moment when their energy spaces unite, how their two P-charges merge into a single one. This basic rule does not govern only the P-charges of capacitors, as it holds for all kinds of P-charges. On the given diagram as well as on the others, each third EZ is marked red, its width is larger by a factor of ten and it is energetically more powerful. This rule also applies to all kinds of P-charges.
Bottom half of diagram No. 1
This diagram shows the interaction of the P-charge of capacitor 5000 µF/1 V with the P-charge of a piece of rock. In comparison with the previous diagram, where the same capacitor had the value of rES = 12 cm, jointly with the rock weighing 10 kg it shows rES value that is 5times higher. The value of the P-charge of the rock before the experiment was lower than record able by our untraditional identification method - I have found no value. The rock has therefore accumulated energy of the capacitor P-charge.
DIAGRAM No.2
In order to emphasize the relation between accumulated energy in a rock and the capacitor
voltage, I used a piece of rock 35kg in weight on which I placed a capacitor connected to three
subsequent voltages. The given values of rock rES are exhibited immediately after connecting the
capacitor to the voltage source, and disappear right after disconnecting and short-circuiting the
capacitor. To make the rock retain some of the energy, the energized capacitor must be kept on
the rock for several tens of minutes (this depends on the rock size and the source capacity).
The material that has thus acquired the energy will lose it slowly for several hours. No comments
here are necessary; the experiment may be continued with increasing the voltage. I may recommend
such experiments to be carried out with capacitors placed to other materials. The results should
be similar. The distances between EZ are not marked on any of the diagrams: they can be derived
from the rES.
DIAGRAM No.3
I regard capacitors, especially those connected to higher voltages, as the largest sources of
cosmic energy (I have not experimented with radioactive elements), by means of which the
P-charges of other materials can be increased. The energy components of metals, semiprecious
stones, precious stones, crystals, water streams, power distribution lines and others are
additional sources allowing the energy value of other P-charges to be increased.
The diagram at first demonstrates the permanent value of P-charge of a piece of iron weighing 17 kg, whose ES radius amounts to 43 cm. When a piece of rock weighing 8 kg, and with the unidentifiable rES is placed on the iron, the two materials exhibit the rES of 60 cm. When the two materials are separated after one hour, the iron will keep its original rES of 43 cm. The stone will exhibit rES = 23 cm, having acquired energy from the iron, but will lose the energy within several hours. It is interesting to note that the stone has acquired energy from iron but iron has lost none. For transfer of energy the two or more materials need not be in a common energy space. The transfer of energy proceeds in the same way when the material accepts the energy in the EZ of the material passing on the energy.
DIAGRAM No.4
The diagram shows the energy components of the human body, which differ from energy components
of other P-charges just in their energy values. All the properties of cosmic energy that I have
described and will describe below also apply to the P-charge of the human body and all organisms.
DIAGRAM No.5
Flowing water appears to be the largest earthly producer of P-charges. The diagram shows the
ES of a creek with a flow-rate of about 10 liters per minute. In the case of this small creek its
energy space has the form of expanding cylinder (depending on the increasing flow-rate),
copying its track. When taking into account that a ten-liter flow-rate produces an energy
space corresponding to a cylinder 670 cm in diameter, it is almost impossible to imagine the
diameter of such a cylinder produced by large rivers having flow-rates of hundred thousands
cubic meters, or that of a sea stream where the rate of flow is given in millions cubic meters
per second.
There are incredible numbers of energy components of flowing water (ES, EZ and interzones) everywhere (including underground springs), and all interact with energy components of other P-charges. In the course of long-term experiments (of course limited by our possibilities) I have never noted a case where some material would bar their penetration.
DIAGRAM No.6
The diagram shows two large trees and their energy components. The experiment had the purpose
to demonstrate conductivity of EZ for cosmic energy. The transfer of energy will proceed from
point "A" situated in the third EZ of tree No. 1, and point "B" placed in the sixth EZ of tree
No. 2. The two points were chosen arbitrarily, the performance is identical between any other
two points in the EZ of the trees. The experiment will have the following course: A group of
capacitors with a total capacity of about 1.5 F is placed at point A. The assistant is then
seated on a wooden chair at point B. I determine the assistant's energy space and record the
value rES = 40 cm. Then I connect the group of capacitors to a 12 V source. On rechecking the
assistant's energy space I find the value of rES = 110 cm. The experiment can be repeated and
always gives the same result. The same rule governs transfer of energy between all kinds of
P-charges. On entry of the smaller P-charge into the energy component of the larger P-charge,
the rES of the former will immediately increase to the final value, acquired by one-hour dwell
in the energy component of the larger P-charge. Short-term exposure to the energy component
of the larger P-charge brings about no energy yield.
It may be useful to pay some more attention to diagram No. 6. To simplify the matter I have plotted just the EZ, between which there are interzones. The diagram represents an area larger than a soccer field. To get at least an approximate idea of the density of the grid, we would have to draw in the energy components of several dozen underground springs, additional components of adjoining natural charges and several dozen EZ belonging to distant large P-charges. We should also take in mind that the circles in the diagram represent in fact huge three-dimensional spherical envelopes.
I have carried out many such experiments and encountered difficulties with making people sit somewhere for one hour. I have solved the problem by replacing the assistant with an artificial P-charge. This purpose was well served by a plastic bottle filled with water (previously boiled in a microwave oven). The results were equally satisfactory and in addition I have acquired a new finding, of which there is no shortage in the research of P-charge interactions: The water pre-boiled in the microwave oven retained the charge for several weeks, unlike the water boiled in another way. Since then I had at my disposal an unlimited number of willing "assistants" and was able to carry out experiment in more places at a time.
DIAGRAM No.7,8,9,10
Diagrams No. 7, 8, 9 and 10 show the energy components of a high-voltage power line. Long-term exposure of man to the energy space of HV power lines will raise the electric voltage on cell walls up to several times, as can be experimentally proved. People are also endangered by EZ of overhead high-voltage power lines which may reach to great distances. Distance does not reduce their aggressiveness, there are many of them and they are conductive interconnected. They can be readily identified in the field according to the almost constant spacing of EZ. Places where EZ of power lines intersect are even more dangerous because the increase in voltage on cell membranes is faster there.
The size of the energy space in diagram No. 10, which represents a 0.4 kV power distribution line, will probably draw attention by its disproportion to high-voltage power lines. However, all is in order, the system functions as a watercourse. In the 0.4 kV distribution line there are currents of the order of hundreds amperes, unlike the high-voltage lines passed by only tens of amperes. In addition to this, the 0.4 kV line usually interacts with the P-charge of the building.
Ten graphs, which I note, are only the sample. They can be constructed in unlimited quantity for every material and would be differentiated only by their distances of EZ and interzones. I have obtained the piece of knowledge that in the distances of EZ and interzones every substance has its specific code by which can be identified. The other codes come up by the combination of two or more substances, which are differentiated from the original codes. I suppose however that the software would be able the codes of individual substances differentiate. In such case would be very easy to identify the sought substance even at extensive distance. At the security of airports or other important objects the PC would at once designate the person, which has along any forbidden substance. In the same way the police could check the vehicles driving through. Directors of schools would be informed, which pupil has used any drug or drink, or has along these substances. The pocket detectors would unfailingly designate drug dealers. The post sending could be examined very easy. This is only the scantling of exploitation the codes of substances, it would find much better use in industry.
