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THIN PHYSICAL FIELDS. WHAT DO WE KNOW ABOUT THEM? METHODS OF MEASURING DTP. FINE PHYSICAL FIELDS

THIN PHYSICAL FIELDS. WHAT DO WE KNOW ABOUT THEM?

Subtle physical field

THIN PHYSICAL FIELDS. WHAT DO WE KNOW ABOUT THEM? FINE PHYSICAL FIELDS

Mark Greene, Ph.D.

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PART 2
METHODS OF DFT MEASUREMENT

Before considering the properties and characteristics of various sources of radiation and the DFT itself, it is necessary to dwell on methods for measuring their parameters, since only the latter allow one to determine certain properties and characteristics of these fields.

Unfortunately, until now classical methods and devices for direct measurement of DFT parameters are not known. This circumstance is due to the fact that the mechanism of interaction of DFT with substances and other physical fields is still unknown, which does not allow us to determine the object of measurement itself.

The main method of measurement, allowing to test the existence and some parameters of the TFT, is the radial (biolocation) method. In this regard, it is possible to anticipate the objections of a number of readers, since the statements that the method of biolocation is "illegitimate" and has poor convergence is not uncommon.

However, such objections are most often heard from those people who do not themselves own this method.

Therefore, it is useful to remind doubters that this method, known since the 8th millennium BC, has been tested by the centuries-old experience of many peoples. Currently, he received legal protection in the form of several international patents, including Russian patent No. 2021749 [6]. And not only.

Currently, Russia has a package of standards for energy and information well-being of the population, and in particular, the standard "Biolocation measurements, tests and studies" ES4.03.01-00 (A) .

The disadvantage of the biolocation method is that it is recognized as a method of measurement not in all countries but rather that it is not owned by every researcher of DFT .

It should be noted that the most informative detector of DFT , with an indirect method of measuring them, is the human body. But about this - below.

If we ponder the essence of the process of biolocation testing of DFT by means of a pendulum, we will see that it is the result of interaction of the operator's bio field with the DFT under test. In this case, the result of testing is manifested in certain movements of the pendulum. Of course, and not everything is clear up to the end ...

At first glance, the biolocation method makes it possible to test only the qualitative side of the process. But it is not so. Let us recall how the units of measurement of the basic physical quantities appeared, for example, such as length, mass, time, etc. In doing so, we find that they are nothing more than a contractual condition accepted by the participants in the measurement process. Such "contractual terms" are given in the table of basic units of the International System of Measurements ( SI ).

As a result, the process of measuring the basic physical quantities is reduced to comparing the measured quantity with its "contractual" standard.

In the same way, for convenience, when comparing the DFT of different sources, for the conventional unit of intensity ( veI ), until the nameless one, I accepted the intensity of the DFT obtained as a result of the so-called " "Information-wave" transfer to the "neutral carrier", in our case - metal (for example, aluminum foil), information properties of the wave component of the electric field of the power source - an AA- type element with a nominal voltage of 1.5 V (so-called "finger battery" "). Note that the state of this source, i.e. Its capacity (amperes) and the residual voltage on the result do not affect.

Having adopted this magnitude of intensity for 1 ye , a series of "working standards" was created, which now covers about a hundred units, and this series makes it possible to measure intensity within a few thousand yeU . Such a range is quite sufficient for measuring (comparing) the intensity of DFT of any substances and objects of the surrounding world, including man-made sources obtained as a result of the addition of fields.

As a "bank of standards" a set of CDs is used , each of which stores information identical to that of the primary source. Thus, each standard is an information copy - the IR (or information analogue - IA ) of the corresponding primary source of DFT .

The process of measuring the intensity of an unknown DFT is performed by a zero (compensating) measurement method, which is a particular case of the comparison method. This method, for example, measures the mass on conventional lever weights, where the measured mass is set on one cup, and on the other - one or several weights, respectively. When measuring the intensity of the TFT, I use "working standards" as the "dumbbells", and as the zero-body of the weights is a pendulum fixing the moment of equality of the intensity of the measured field and that of the corresponding set of digitized "working standards".

It is clear that such a parameter as the intensity makes it possible to compare different sources of radiation, but does not determine all the properties of the DFT .

As an example, below is a table containing the intensities of a number of substances, objects and bioobjects measured by the indicated method.

THIN PHYSICAL FIELDS. WHAT DO WE KNOW ABOUT THEM? METHODS OF MEASURING DTP. FINE PHYSICAL FIELDS

Other important parameters of the DFT are the frequency, and the phase, which results from the information-wave character of the DFT . In this case, all the above parameters are decisive in the interaction of DTP with the environment, for example, with the human body. Without dwelling in detail on these interactions, I will only point out that the main parameters in the selection of homeopathic medicines for therapeutic purposes are the frequency and intensity of the PH of the preparation. In this case, the choice of the drug determines the frequency (or spectrum of frequencies), and the magnitude of the potency - the intensity of the effect causing the optimal therapeutic effect, i.e. Resonance response (bioresonance) of the body.

How to measure the frequency of FIs ?

There are all grounds to believe, and this is confirmed by a number of experiments, that the frequency of a specific DFT can be determined by a substitution method.

Substitutions, the method of measurement , one of the methods of comparison with the measure, consists in replacing the measured quantity by a measure selected or adjusted so that the readings of the measuring device remain unchanged; While the value of the measured quantity is equal to the nominal value. (Large Encyclopedic Dictionary)

In our case, using the diagnostic complex, the frequency parameters of the measured DFT , which change the functional state of the organism in a certain way, are replaced by an electric or electromagnetic signal of a special shape so that the effect on the body of the generated therapeutic signal of a known frequency is adequate to that obtained from the effect of DFT with Unknown frequency parameters.
Of course, this technique is only available to specialists in reflexology who have appropriate methods of working on diagnostic AIC .

A simpler way is a biolocation method for measuring the wavelengths of FIs .

For the first time, this method was proposed by the French pharmacist G. Lessour and published in 1934 . Lessour has developed a classification of pathogens along the wavelengths of their own radiations.

Why wavelengths? In principle, knowing the wavelength, you can determine and the frequency of radiation. But for this it is necessary to know the speed of propagation of a particular radiation in a vacuum. And for FI it is unknown. Therefore, in a particular case, we can only talk about the wavelengths of different radiations and compare the DFT only in terms of relative intensity and wavelength.

Determination of the wavelengths of FIs is carried out with the help of information analogs ( IA ) of radiation sources, which is an aluminum or other foil glued to the substrate with the information-wave properties of these sources transferred to them, as appropriate.

The measurement is carried out in the manner described below.

On the table there is a digitized wooden meter line in the direction from North to South (the beginning of the ruler is to the North) .. A millimeter scale is placed on the ruler. At the mark "0", IA is placed in such a way that its end is perpendicular to the digitized part of the ruler. It is convenient to install the EA in a wooden stand with a slot. Then the pendulum moves slowly along the digitized side of the ruler. In this case, the pendulum starts to make rotational movements, in accordance with the polarity of the radiation wave. For the positive half-wave, the right increase and vice versa. At some point, the rotational motion of the pendulum becomes transverse. At this point, the amplitude of the wave radiation of the IA becomes zero.

This point fixes the length of the half-wave FI . At very large and very small values ​​of the measured value scale scaling is used.

LITERATURE

  1. Patent of the Russian Federation No. 2021749 . A method for determining the type of interaction between a person and a plant.

  2. Announcements VN, Perevozchikov NF, Influence of the non-light component of laser radiation on water and aqueous solutions of organic compounds, "Reports of the International Forum on Problems of Science, Engineering and Education", vol.2, Moscow, December 4-8 2000.

  3. Garyaev PP, The Wave Genome, Http://lib.walla.ru/?a_id=6144

  4. Karafinka MM, Levitsky EF, Tereshchenko A.Yu., On the Background Radiation, Abstracts of the International Congress "Resortology, Physiotherapy, Restorative Medicine of the XXI Century", p. 96-97, Perm, 2000.

  5. Kvartalnov VV, Experimental emission of components of unknown physical nature from laser radiation, "Laser-Inform" No. 12 (219), 2001.

  6. Levitsky EF, Karafinka MM, Tereshchenko, A.Yu., The review of patents on the problem of transfer of information properties of the initial medical factors. "Questions of balneology, physiotherapy and physiotherapy", No. 3, 2000

  7. Puchko L.G. Multidimensional medicine, M., ANS, 2003

  8. Puchko, LG, Biolocation for all, M., Shark, 1996

  9. Rogozhkin V.Yu., Eniology, Rostov-on-Don, "ENIO" Publishing House, 2002

  10. Samokhin, A.V., Gotovsky Yu.V. Electropuncture diagnostics and therapy by the method of R. Foll, M., "Imedis", 1995

  11. Shipov GI, Theory of Physical Vacuum. Theory, Experiments and Technologies, Moscow: Nauka, 1997

  12. Shumov IV To the question of transferring information properties of medications used in electropuncture diagnostics and therapy according to R.Foll, homeopathy and other methods of diagnosis and treatment,
    Http://www.strannik.infomsk.ru/

  13. Etkin VA, Physical manifestations of energy-information interactions, 2005, http://zhurnal.lib.ru/e/etkin_w/

print version
Author: Mark Green, Ph.D.
PS The material is protected.
Date of publication 10.11.2006гг