The problems of life quality, health support, and longevity are related for all us, first of all, to the synchronism of the processes of vital activity running in human organism.

In healthy organisms, all processes are running synchronously. In the case of a disease, the synchronism of the processes in organism is broken. This occurs not only on the cellular level, but also touches the endocrinous, immune, and other controlling systems. If a disease becomes chronic, the degree of desynchronism increases, by causing the propagation of the disease onto other organs and systems.

The synchronism of the processes in organism is also broken during its ageing. Many researchers indicate that, with increase in the age, there occurs a slow dehydration of organism. In this case, cells are slagged, intracellular and exchange processes are desynchronized, the number of stem cells supplying young cells to organs decreases catastrophically, which deteriorates the protective properties of organism, etc.

The answer to the question “How can the synchronism of the functioning of systems of our organism be supported?” is related to our internal aqueous medium and the consumption of complementary coherent water.

Namely this water corresponds completely, by structure and state, to intracellular water.

Complementary coherent water

— causes no aberrations (breaks) of chromosomes,

— is not toxic,

— activates the production of interferon during 72 h up to 360 un.act./ml, whereas cells in the control group die in 24 h, by producing interferon in the amount of at most 128 un.act./ml,

— increases reliably the efficiency of inhibition of the vesicular stomatitis virus amounted to 2 lg ID50,

— increases reliably the protective properties of the immune system against the herpes infection (2 lg ID50),

— activates the inhibition of HIV/AIDS; as a result, the number of lymphocytes CD4+ in patient’s blood increases, and some opportunistic diseases of organism disappear.

 

Complementary of water

COMPLEMENTARY COHERENT WATER

 

V.G. Krasnobryzhev

 

In recent years, the medical statistics indicates a deterioration of population’s health. The high anxiety is caused by the fact that only 20% of children are healthy. Thus, the perspectives for future generations in our country give rise to the preoccupation and the alarm.

In this case, we observe the interconnection between the state of health and the qualitative composition and structural properties of drinking water.

Undoubtedly, the state of our health is connected with the quality of drinking water. Indeed, 70% of an adult and 80-85% of a child consist of water. It is worth noting that water in human organism possesses specific properties such as the presence of some structure and a negative redox potential, which significantly influence the intracellular metabolism.

Many researchers assert that the usage of structurized high-quality water improves the health and affects the longevity of people. It is necessary to completely agree with this viewpoint.

However, these studies did not answer the following quite actual question: To which extent does drinking structurized water correspond to intracellular water of human organism? We know that intracellular water is also structurized and, in addition, its molecules have left torsion. Why? The answer is simple. The structure of all protein molecules of human organism is characterized by left torsion. Hence, drinking water must have also a structure with left torsion. However, the structure of water is represented by R- and L-tetramers in identical concentrations. Therefore, only a half of used water with left torsion enters the cells of organism. Water with R-torsion remains in the intercellular region, since it is not complementary to the protein-based structure of the membranes of cells.

In health organism, all processes run synchronously. In this case on the cellular level, the cells perform the informational exchange in the ultraviolet range with wavelengths of 240-380 nm. Despite a significant width of this range, the exchange is realized with the same phase, i.e., coherently. This yields the coherence and, respectively, the synchronism of all processes in human organism.

At a disease, the synchronism of the processes in organism is broken. This happens not only on the cellular level, but influences the endocrine, immune, and other controlling systems. But if a disease acquires the chronic course, the degree of desynchronization of organism increases, by causing the extension of a disease onto other organs and systems.

The synchronism of the processes in organism is also violated in the process of ageing. The authors of a lot of works indicate the development of dehydration of ageing organisms. In this case, there occur the slagging of cells, the desynchronization of intracellular and exchange processes, the catastrophic drop of the number of stem cells, which are suppliers of young cells, the deterioration of protective properties of organism, etc.

The answer to the question “What shall we do?” is unique. It is necessary to drink complementary coherent water, which differs from ordinary one only by that the structure of the former possesses the L-torsion, and its molecules oscillate with identical frequency and phase, i.e., synchronously. In this case, one says that each molecule feels all molecules of its environment.

It is significant that, under the recovery of the synchronous state of cellular structures, we may expect the intensification of the intracellular informational exchange and biochemical reactions, increasing the selectivity of processes, self-purification of surfaces from catalytic slags, etc. Therefore, by using complementary coherent water, we return the synchronism and the vital force to our organism and, hence, make it more healthy.

 

Complementary coherent water can be produced with the help of a special unit “Synchronizer.”

“Synchronizer” is a spintronic device possessing a large spin potential, which is conserved for 1.5 yr. It can be glued to the wall (or the bottom) of a ceramic mug or a glass 250–300 ml in volume. If we fill up it with water, then water becomes coherent in 5 min. We recommend you to wait 1 h and then to pour off water. You now have a simple system for the production of complementary coherent water. In what follows, you can fill up the mug with water, and it will become complementary coherent in 5 min.

Scheme of the usage of water.

1.                     Complementary coherent water should be drink in the morning or in the evening prior to a sleep every day. The usage of water can be realized by the following scheme: in Your mug with “Synchronizer,” you fill up a portion of water 200-250 ml in volume and wait 5 min. Then, by holding the mug in your hand, you have to drink complementary coherent water during at least 5 min by small swallows. Due to the drinking of such water, the water medium of Your organism passes to the synchronized state, which causes the synchronization of all processes.

You should not expect the positive effect at once and forever. Miracles are met rarely and mainly in fairy tales. But the synchronism is a foundation of of the health of Your organism, which should be continuously supported.

Complementary coherent water will help You to counteract a wide spectrum of viral infections, which include, in the first term, herpes, vesicular stomatitis, HIV, hepatoinfections, etc.

The recovery of the synchronism of Your immunity will help You to resist the allergic diseases. Moreover, the synchronization of Your endocrine system will restore its regulatory functions. For example, You will be able to resist diabetes mellitus.

We do not promise the rejuvenation of Your organism without injection of stem cells, but Your health will become stronger.

 

Studies of the biological effiuciency of complementary coherent water

 

The ideology of studies is related to the following premises.

1.                     Diseases and the ageing of organism are conjugated with the desynchronization of intracellular processes.

2.                     The usage of complementary coherent water will initiate the synchronization of

intracellular processes, by supporting their intensity, will restore the correlations (interconnections and interrelations) between cells and their correlated behavior on the macrolevel, will improve the protective functions of organism, and will decelerate of the processes of ageing.

The studies of the efficiency of complementary coherent water were carried out by means of the determination of its influence on the operation of the immune system of infected organisms in vitro and in vivo.

The studies were performed at the Institute of Epidemiology and Infectious Diseases of the Academy of Medical Sciences.

                                      

1.                     Cytologic and cytogenetic investigation of complementary coherent water

 

The culture of cells was obtained from 8-9-week human embryos by the standard procedure of trypsinization of disintegrated pieces. Cells were grown in nutrient medium RPMI-1640+10% embryonic calf serum + antibiotics.

For the cytologic studies, cells were grown on cover glasses in ordinary bacteriological test tubes. Cells were treated by a fixative, dehydrated, and colored with hematoxylin-eosin. We determined the following indices: proliferative activity (‰) and the presence of pathological mitoses.

Cytogenetic preparations were produced by the method given in “Method of human chromosome aberration analysis,” edited by K. Backton and H. Evans (WHO, Geneva, 1976). While studying the metaphases, we counted the number of chromosomes and aberrations in them.

To study the influence of complementary coherent water on the cytologic and cytogenetic indices, we treated cHET cells in the phase of logarithmic growth by complementary coherent water and produced preparations in 24 h. The control group included cells, which were not undergone any actions.

 

Results and their discussion.

 

Results of cytologic studies of the preparations, which were obtained on cHET cells and treated with coherent water, are shown in Table 1.

 

Influence of complementary coherent water on the mitotic mode of cHET cells

 

Table 1

Influence

̳ (in ‰)

Normal, in mitosis, ‰

Abnormal, mitosis, ‰

Cells +coherent water

21,0

91,4

8,6

The control of cells

29,0

93,2

6,8

 

Table 1 indicates that complementary coherent water rendered no significant action on the mitotic mode of cHET cells, as compared with cells in control.

In Table 2, we show the results of cytogenetic studies of cHET cells processed with coherent water.

 

Cytogenetic indices of cHET cells processed with complementary coherent water

 

Table 2

 

Influence

Influence Cells with number of chromosomes (in %)

45

46

47

The control of cells

4,0

96,0

0

Cells +coherent water

2,0

96,0

2,0

 

The data presented in Table 2 testify that the action of complementary coherent water rendered no significant action on the karyotype of cells and induced no aberrations (breaks) of chromosomes.

 

2.                     Study of the interferonogenic activity of complementary coherent water

 

The interferonogenic activity of complementary coherent water was studied in experiments in vitro. For this purpose, we used leukocytes of donors. Into their 3-ml solution, we added 0.1 ml of coherent water, incubated the mixture at è 37îÑ for 18 h. Then we determined the activity of interferon in the supernatant fluid by the method of suppression of the cytopathogenous action of vesicular stomatitis virus in the homologous intertwined culture of cells L41 (human lymphoblast cells). The culture was grown in the medium consisting of nutrient medium RPMI-1640 + 10 % fetal serum + antibiotics.

To the monolayer of cells grown in dishes, we added the dilution of a cultural fluid containing complementary coherent water (after the incubation with leukocytes) and incubated. Then we remove the supernatant fluid and introduced vesicular stomatitis virus (VSV) in a dose of 100 TCD 50/0.1 ml. As control, we took the cultures of cells treated with VSV and cells undergone no treatment. Experimental and control cultures were incubated at 37îÑ for 24 and 72 h.

The determination of the activity of interferon was made in 24 and 72 h, when the introduced VSV caused the total degeneration of cells in control, whereas the intact culture of cells and the cells + complementary coherent water were not degenerated. As the titer of interferon, we took the quantity reciprocal to the dilution of coherent water, at which the culture in 50% of small cavities was completely protected from the cytopathogenous action of VSV.

The results of studies of the interferonogenous activity of complementary coherent water are given in Table 3.

 

Interferonogenous activity of complementary coherent water

 

Table 3

 

Influence

Interferon activity, units/ml

24 hour

72 hour

Spontaneous effect

4

4

The control of cells

128

Cells +coherent water

168

360

 

 

Thus, complementary coherent water activates the production of interferon and protects the culture of cells of leukocytes from the destruction.

           

3.                     Study of the influence of complementary coherent water on the

           reproduction of vesicular stomatitis virus (VSV).

 

The study of the influence of complementary coherent water on the reproduction of VSV was carried out in the intertwined culture of cells L41 (human lymphoblast cells). Cells were grown in medium RPMI-1640 + 10% fetal serum + antibiotics.

Vesicular stomatitis virus, Indiana strain, was obtained from the Museum of viruses at the D.I. Ivanovskii Institute of Virology (RAMS, Moscow). The infection titer of the culture of cells L41 was 4.0-4.5 lg ID50. A monolayer of cells L-41 was grown in test tubes. Then VSV was introduced into test tubes in a dose of 100 ID50, and cells were treated by complementary coherent water. As control, we took the cultures of cells treated only with VSV and cells undergone no treatment. The infection titer of VSV was determined in the cultural experimental and control media after the 24-h cultivation at 37°Ñ, when the full degeneration of the monolayer of cells in test tubes with VSV was observed. The results of studies of the influence of complementary coherent water on the reproduction of VSV are given in Table 4.

 

Influence of complementary coherent water on the reproduction of VSV

 

Table 4

 

Preparation

Credit of a virus in   lg ID50

Inhibition VVS in lgID50

 

Ð

Coherent water

3,0

3,0

<0,001

The control of cells

5,0

 

 

Thus, the studies performed indicate that, in the presence of complementary coherent water, the inhibition of the reproduction of vesicular stomatitis virus is equal to 2 lg ID50.

 

4.                     Study of the anti-HIV activity of complementary coherent water

 

The study of the influence of complementary coherent water on the reproduction of HIV was performed on a new model of HIV-infection in COS cells, which possess the universal sensitivity to RNA- and DNA-containing viruses, including HIV.

The monolayer of cells COS grown in dishes was infected by HIV in a dose of 100 ID50 and cultivated for 5-7 days. We took the cultural fluid and determined ð24 with the help of test-system Virognostica Organon in it. Then, by using 10-fold dilutions, we infected the culture of COS cells to determine the infectious titer. The results are presented in Table 5.

 

Characteristic of HIV-infection

 

Table 5

Processing of culture

Days cultivation

Level expression ð24 HIV

ð24, ng/mL

infectious titer in lg ID50

HIV

5

3,640

5,0

HIV

7

3,666

6,0

 

The ÑÎS model was used for the study of the influence of complementary coherent water on the reproduction of HIV. For this purpose, the monolayer of cells ÑÎS was infected by HIV in a dose of 100 ID50 and treated with coherent water by the scheme used in the previous studies. We incubated cells at 37°Ñ for 7 days and then determined the expression of ð24 of HIV and its infectious titer in samples.

 

The results of studies of the influence of complementary coherent water on the reproduction of HIV are presented in Table 6.

 

Influence of complementary coherent water on the reproduction of HIV

 

Table 6

Preparations

Expration, pg/ml

Infectious titre of a HIV in lg ID50

HIV+coherent water

630

4,0

The control of a HIV

650

5,6

 

As a result of studies, we have established that complementary coherent water inhibits the reproduction of HIV by 1.6 1g ID50, which was revealed in the inhibition of the expression of antigene ð24 of HIV-1 and in a decrease of the infectious titer by 1.6 1g ID50.

 

5. Study of the antiherpetic activity of complementary coherent water

 

To study the antiherpetic action of complementary coherent water, we used the model of herpetic meningoencephalitis. The given model is convenient for the estimation of the expression of symptoms, is characterized by the 100-% reproducibility, and requires no additional control. The development of clinic symptoms of the disease began in 5-6 days starting from the time moment of infection, attained the maximum in 13-14 days, and then was characterized by a decrease of the expression of symptoms with the subsequent recovery of survived animals. The presence of acute herpetic infection was corroborated by the method of immunofluorescence. For example, the most intense fluorescence was observed in tissues of brain (especially in trunk parts). It appeared in 6-7 days starting from the time moment of infection, which corresponds to the appearance of clinic signs of the disease. The less intense fluorescence (+ or ++) was observed in spleen and was absent in liver and lungs. Lethality of animals infected by herpes virus was 100%.

To model the experimental herpetic infection, we used simple 1-kind herpes virus. At the laboratory, virus made 28 passages through brain of white white. Prior to the experiment, virus was conserved in a 50% solution of glycerin in a phosphate buffer solution at a temperature of 10-15°Ñ .

In experiments, we used white mongrel white 14-16 g in weight. The virus-containing material 0.03 ml in volume was introduced in mouse’s brain. The magnitude of infecting dose in experiments was equal to 1-10 ID50 (lethal doses for mice).

Complementary coherent water was introduced one time in the amount of 0.2 ml intraperitoneally by the following schemes: before the infection — prophylactic scheme of introduction; in 24 h after the infection by herpes virus — therapeutic scheme.

Each experiment included 2 groups of mice:

1 – mice under the action of complementary coherent water + herpes virus,

2 – mice, to which a physiologic salt solution + herpes virus were introduced.

The estimation of the activity of complementary coherent water was executed by comparing the lethalities of mice in experimental and control groups. In this case, we took into account

—  the lethality of animals (%),

— protection ratio (PR) – the ratio of the number of died mice in the experimental group to that in the control group,

— efficiency index (EI) of the preparation was calculated by the formula

EI        protection ratio

On the first stage of studies, we investigated the activity of complementary coherent water. To the animals infected by herpes, we introduced coherent water every 24 h up to the end of the experiment. The results of studies of the antiherpetic activity of complementary coherent water under the prophylactic action on mice are given in Table 7.

 

Antiherpetic activity of complementary coherent water

the anti herpetic activity of coherent water

 

Table 7

 

Preparation

Quantity

of mice

From them were lost

Frequency rate of protection

Index of efficiency

In total

Percent

Coherent water

12

6

50

2,0

50,0

Placebo

14

14

100

 

 

 

As a result of studies, we have established that complementary coherent water activates the protective functions of the immune system against the herpetic infection.

 

6.                     Pilot experiment on the inhibition of HIV in vivo at the usage of

    complementary coherent water

 

THE EXPERIMENT WAS EXECUTED IN THE SAR WITH PATIENTS (VOLUNTEERS) INFECTED BY HIV WITH VARIOUS CONTENTS OF Ò-LYMPHOCYTES CD4+ IN BLOOD. IN THE EXPERIMENT INVOLVED  V.G. KRASNOBRYZHEV,               S.V. BRUKOVSKY, J.M. KEARNEY, E. KEARNEY

In the SAR, HIV-infected persons are divided into the following groups:

— group of patients ill with AIDS if the content of lymphocytes CD4+ <  200 un./µl in blood,

— group of HIV-carriers if the content of lymphocytes CD4+ > 200 un./µl in blood.

One part of patients used only complementary coherent water, whereas another part did complementary coherent water and antiretroviral drugs (ARVD). The results are presented in Table 8.

 

Influence of complementary coherent water on the content

of lymphocytes CD4+ in blood of HIV-infected patients

 

Table 8

 

The patient

 

Accepted preparations

Time of reception, days

 

Contents CD4 + in blood

 

Water

ÀRVM

 

Before experiment

After experiment

 

 

 

 

1/mcl

%

1/mcl

%

Michael Makhoba

+

10

20

3,2

207

9,06

Rachel Ngcayiya

+

10

90

6,96

154

11,05

Mercia Dube

+

10

419

21,0

597

21,65

Petrus Tshabalala

+

+

30

101

6,68

156

7,54

John Moroazwi

+

+

30

271

18,8

453

21,25

Alfred Zulu

+

+

60

448

20,19

642

20,77

 

As a result of the executed experiment on the inhibition of HIV in vivo, we have established that complementary coherent water inhibits the reproduction of HIV, which causes the increase of the content of lymphocytes CD4+ in blood of patients. In addition, already during 10 first days, we observed the purification of skin of patients from eczematous and herpetic exhibitions, enlightening of urine, improvement of a sleep, and an increase of body’s weight.

 

Properties of coherent water

Properties of Coherent Water

 

V.G. Krasnobryzhev a), M.V. Kurik b)

a)Sci.-Industr. Center “Priroda”. E-mail:vkentron@gmail.com

 

b)Institute of Physics of the NAS of Ukraine; Ukrainian Institute of Human Ecology,

Kiev, E-mail:kurik@iop.kiev.ua

 

We present the results of measurements of a number of physical characteristics

of packed (bottled) drinking waters transferred in the coherent state.

We show that it is possible to obtain two sorts of coherent water with the left (L)

and right (R) mainly spin polarizations with the help of the developed technology.

These waters possess different physical characteristics and render, respectively,

different influences on alive organisms.

 

Urgency of the problem

 

The phenomenon of coherence is widely applied to the description of physical states of matter, which are joined by such common features as the ordering and the coordination in a behavior of the great amount of elements of a substance. Superconductivity, superfluidity, laser beams, and other phenomena arise due to the coherence on macroscopic scales.

At the present time, the urgency of the problem concerning the creation of a coherent substance becomes so high that it is called the fifth state of matter. This is related to the fact that the macroscopic coherence causes the appearance of completely new physical properties of a substance, which allow one to use it in various forms and on “industrial scales”.

A distinctive property of the coherent substance is the not proportional response to an external action. For example, water starts to generate radiowaves under the action of a low-intensity laser radiation with a wavelength of 0.63 µm [1]. In this case, this wavelength is resonant with respect to water. The studies showed [2] that, under the action of an electromagnetic field 3 µW/min power on coherent water at the resonance frequency, the internal energy of such water increases by the value corresponding to the internal energy of water in the equilibrium state under the action of an electromagnetic field 100 µW/min power.

One of the authors proposed [3, 4] a means that allows one to transfer up to 500,000 tons of matter represented by coal in the coherent state. In this case, the activation energy of coal decreases by 57% [5]. In addition, a technology of transfer of metals in the coherent state, in which the energy consumption at their annealing is lower by 36-40%, was developed.

A significant peculiarity of the above-mentioned means to create a macroscopic coherence is the possibility for the distant interaction (teleportation) between the remote singlet pairs and, in such a way, the transfer of spin states from one material object to another one [5]. In this case, the distance between such pairs can be indeterminately large.

The interest in coherent properties of water is caused by the perspective to use such water in prophylactic and therapeutic purposes, since at least a half of molecules of the alive matter consists of molecules of water. At such huge number of molecules, water plays the defining role in biochemistry, biophysics, and the functioning of the alive matter itself. We can support the opinion of Prof. Del Giudice [6-9] that the role of water in organisms is crucial.

The studies in vitro and in vivo showed [10] that coherent water causes no aberrations (failures) of chromosomes; is not toxic; activates the production of interferon for 72 h up to 360 un. act./ml, whereas the cells in control group produced interferon in the amount of at most 128 un. act./ml and died in 24 h; increases reliably the efficiency of the inhibition of the vesicular stomatitis virus; improved the protective functions of the immune system relative to herpes infection; activates the inhibition of HIV/AIDS, which increases the amount of lymphocytes CD4+ in blood of patients and eliminates opportunist diseases;.

A particular role of water is also revealed in the quantum physics of alive matter. On the basis of quantum electrodynamics, it was first proved [11] that liquid water is a coalition or the totality of coherent domains. The size of each coherent domain corresponds to the wavelength of the quantum transition from the ground state to an excited one.

The results of calculations of the authors [6-9] testify that the difference in the energies of the ground state and the first excited one of a coherent domain of water is equal to 12.06 eV, which corresponds to the wavelength of photons of soft X-ray radiation (at room temperature, the size of a coherent domain of water is about 0.1 µm). In normal water, the separate coherent domains are independent of one another. Each coherent domain possesses a field extending outside the domain, and the fields of different domains overlap, by “gluing” them. Therefore, the domains form a conglomerate but do not form the common coherence with one another. This situation is characteristic of “normal” distilled water.

The basic peculiarity of water consists in that the excited-state energy of a coherent domain is very close to the ionization energy of a molecule of water: 12.06 eV and 12.60 eV, respectively. If a domain is in the ground state (the lowest energy), all electrons are tightly bound, so that water will be ionized, if it will receive the energy pulse of at least 12.60 eV, which corresponds to soft X-ray radiation. In the excited state, many electrons are almost free, and a low energy is required in order that the electrons become completely free. The molecules of water in the noncoherent state cannot be reducers or donors of electrons, whereas à coherent water is a good reducer.

Noncoherent water retains the electrons sufficiently firmly and can be considered as a weak oxidizer, and a molecule of water can be transformed in ion Í2Î. In the coherent state, water donates electrons easily, and ions Í2Î+ are formed.

In view of the above consideration, the studies of properties of coherent water seem to be urgent, because the data presented are not complete.

The investigations are carried out with the help of the developed system of quantum teleportation described in [4, 12], which allows one to create the coherent state of natural packed water at a distance of several kilometres. We measured its main physical characteristics and discovered its unusual properties as compared with those of ordinary noncoherent water. The results concerning some properties of coherent water are the subject of the present work.

 

Experimental procedure

 

The transformation of ordinary drinking water into coherent water consists in the following. A special chip [4], which is an element of the singlet pair with translational symmetry, was attached to the outer side of a glass vessel filled with natural packed drinking water. We chose the volume of water for studies to be 50 ml, though its value can be different. At the beginning, we activated water by an L-chip (left polarization of spins). Then another chip of the R-type was attached to the second vessel filled with the same packed water. Both vessels with water were positioned at a definite distance from each other (about 0.5 m).

After the pouring of initial water in the vessels, we measured the physical properties of water and observed the dynamics of the chip-induced appearance of the coherent state of water. All measurements were performed relative to the initial control packed water.

In studies, we used various packed drinking waters such as “Prozora”, “Goryanka”, and drinking additionally purified water of the Alpine type. Hence, the main difference between those waters consisted in different contents of controlled admixtures determining the specific features of their structures.

The measurement of physical characteristics consisted in the measurement of the acid-alkali equilibrium (ðÍ), specific conductivity (σ), redox potential (RP), concentration of dissolved admixtures or the salinity of water (TDS in mg/l), optical absorption spectra, and dielectric permittivity. All measurements were carried out at room temperature.

In studies, we used the following devices:

1.                     The acid-alkali equilibrium was measured with the help of two devices: a ðÍ–meter ÎÐ-261-1, of the “Radelkis” firm (Hungary) and a high-frequency device ðÍ-009 (M), of the “Kelilong Instruments” firm (China). The accuracy of measurements of ðÍ was equal to ± 0.02.

2.                     Specific conductivity was measured in μSm with a device ÑÎÌ-100, ÅÑ/TDS/temp COMBOMETR, the “Digital. Inc.” firm (USA). The accuracy was ±10%.

3.                     Redox potential was measured with a device ORP-169 of the “Kelilong Instruments” firm (China). The accuracy of measurements was equal to ±20%.

4.                     The total level of mineralization (content of salts) was measured in mg/l with a device ÑÎÌ-100, the “Digital. Inc.” firm (USA). The accuracy was ±10%.

5.                     Absorption spectra were measured with the help of a two-beam spectrometer.

The structure ordering of water was determined by the crystal-optical method, by studying a structure of the solid phase (the phase transition: water, solution – solid phase) with a universal optical microscope NU-2E, Zeiss, Germany.

 

Results of measurements

 

As is seen from Fig. 1A, the absorption spectra of coherent water with L- and R-polarizations are different significantly from each other and from those of water â the equilibrium state. These parts of the absorption spectrum of water represent the long-wave “tail” of the electron absorption of water, whose absorption band maximum is located in the region of vacuum ultraviolet light near 7 eV [13]. In the indicated spectral region, the absorption is formed by optical transitions with the participation of vibrations of a lattice (of water molecules), as well as by admixtures present in water under study. In this case, the shape of the electron absorption spectrum measured as the dependence of the coefficient of absorption on the wavelength of light (the photon energy) is described by the exponential function at a given temperature. In other words, the absorption spectrum shape obeys the Urbach rule [14].

 

The analytic processing of the results of measurements of the shapes of the absorption spectra of R- (curve 2) and L-water (curve 3) confirmed that, on a small part of the spectrum (200-240 nm), the absorption spectrum shape is described by the exponential function of the photon energy.

Analytically, these data are described by the function Y=A+BX, where where À=7.00 and Â=-0.03 for the L-polarization and À=3.49 and Â=-0.03 for the R-polarization.

Since À and  determine the steepness of absorption curves in the given coordinates, this means that the steepnesses of the absorption spectra on the given part differ by a factor of 2 for the L- and R-polarizations, which indicates the differences in structures and in degrees of coherence.

In Figs. 1 and 1Ñ, we present the data of measurements of the temporal variations of the parameters of water “Goryanka” in the equilibrium and coherent states: ðÍ of water and σ äëÿ L- and R- polarizations, by starting from the time moment of the attachment of a chip to the vessel with water. In both cases, the vessels with water were open.

At the same time, we observe a monotonic growth in ðÍ and conductivity σ for both L- and R- polarizations of coherent water. This testifies to the dynamic variation and the ordering of the cluster structure of water at the continuous “holding” of the coherence of water with the help of a chip. For water in the equilibrium state, the values of ðÍ and σ were practically constant during the experiment.

The dependences analogous to those shown in Fig. 1 are observed for all types of waters under study, which is a characteristic peculiarity of the influence of the coherence on a structure and properties of the waters.

In Fig. 2À, we show the trends of the relative variation of the differential resistance of samples of control water as compared with the R- and L-polarized coherent water (R0/RR,L). As is seen, the wide dispersion band in the region 2.5 — 10 Hz is observed for coherent water. The measured decrease in the differential resistance is analogous to that in negatronic systems.

It is worth also noting the closeness of this effect to Schumann’s resonances and to alpha-rhythms of a human brain.

Fig. 2. Electrophysical properties of coherent water:

 

À – relative differential resistance of water R0/RR,L vs the frequency, where R0 – resistance

of water in the equilibrium state, RR, RL –resistance of water in R- and L-polarized states;

 – relative variation of the capacity of water vs the frequency, where ÑR , CL – capacity of

water in R and L-polarized states, Ñ– capacity of water in the equilibrium state.

In Fig. 2Â, we present the trends of the relative variation of the capacity of samples of control water relative to those of R- and L-polarized coherent water (ÑR,L0). As is seen, coherent water possesses a wide dispersion band in the region about 100 Hz. Analogously to the properties of negatronic systems, we observe an increase of the capacity of water.

 

The described dependences are revealed by all types of the waters under study, which is a characteristic peculiarity of the influence of the coherence on the structure and the properties of water. For example, the L-polarized structure is more ordered as compared not only with the initial structure, but also with the R-polarized structure.

The above-presented peculiarities of the physical properties of L- and R-polarized coherent water are the reason for various manifestations of the action on alive structures, including men and women [10]. In this case, we note that the biological activity of L-coherent water must be more intense as compared with R-water. This is connected with the fact that L-water is complementary to protein structures of organisms possessing the L-spatial configuration.

 

Conclusions

 

For the first time, we have experimentally confirmed the fact of the production of coherent drinking water with the help of the Universal system of quantum teleportation and have shown that the coherent state of water can be held with the help of a special chip.

Coherent properties are determined by peculiarities of the structure of water, which is undergone to the coherentization.

The application of the basically new Universal system of quantum teleportation opens new possibilities in studies of the physics of macroscopic entangled states and, what is of fundamental importance, allows one to use the quantum and classical physical methods in parallel for the investigation of the phenomenon of teleportation.

By concluding, the authors thank A.V. Koval’chuk and A.P. Boiko for their help in a number of experiments.

 

References

 

1.                     I. Petrosyan, N.I. Sinitsyn, V.A. Elkin, O.V. Bashkatov, Interaction of hydrogen-containing media with electromagnetic fields // Biomedits. Radioelekt., 2000, No. 2, 10-17.

2.                     W. Smith. Quantum and Coherence Effects in Water and Living Systems / J. of Altern. and Complem. Medic., 2004, 10(1): 69-78.

3.                     Sposób i urządzenie do modyfikacji paliwa. Zgloszenie patentowe P-380566 od 05.09.2006 r. w Urzędu Patentowym RP. / Biuletyn Urzędu Patentowego ¹ 5, Warszawa, 2007, pp. 15.

4.                     The means and a device for the formation of the coherent material medium. Patent application No. 200803310 on03.2008 in the Ukrainian Institute of Industrial Property.

5.                     V.G. Krasnobryzhev, 500,000 tons of coherent matter. Reports on the Conference ”Foundations of Physical Interaction: Theory and Practice”. Kyiv 2008, p. 229.

6.                     Del Giudice, G. Preparata, M. Fleischmann, J. of Electroanal. Chem., 482, No. 2, 2000, 110-116.

7.                     Del Giudice, G. Preparata. J. Biol. Phys. 20, No. 1-4, 1995, 105-116.

8.                     Del Giudice. J. of Phys. Conference Series, 67, 2007, 012006 (7 pp.).

9.                     Del Giudice, A. Tedeschi. Water and Autocatalysis in Living Water // Electromagnetic Biology and Medicine 28 (1), 2009, 46-52.

10.                  V.G. Krasnobryzhev, System “Dipole,” Reports on the Conference ”Foundations of Physical Interaction ”, Dnepropetrovsk, 2006, p. 163.

11.                  Del Giudice, et al. Coherent Quantum Electrodynamics in Living Matter // Electromagnetic Biology and Medicine. 2005, Volume 24, pg 199-210.

12.                  V.G. Krasnobryzhev, Universal system of quantum teleportation. //Torsion Fields and Informatinal Interactions– 2009. Proceedings of the Sci. Conference. Sochi. 2009. 411-419.

1.                     I.P. Studenyak, M. Kranjčec, M.V. Kurik, Optics of Disordered Media, Radzha, Uzhgorod, 2009 (in Ukrainian).

14.                  Buhks, On Urbach rule theory for impurity light absorption. 1975 J. Phys. C: Solid State Phys. 8 1601-1606.

15.                  I. Doronin, Quantum Magic, Ves’, St.-Petersburg, 2007 (in Russian).

 

The effectiveness of a coherent water for HIV

Substantiation of the Efficiency of the Action of Coherent Water

under HIV—infection

 

1.                     V. G. Krasnobryzhev

 

Coherence is a state of matter, in which atoms or molecules oscillate at the same frequency with the same phase.

 

1.                     HIV can penetrate into Ò-lymphocytes CD4+, whose surfaces contain a special protein-receptor gð120. The virus binds with this protein with the help of chemokine ÑÕÑR-4 (reaction of polymerization) by the “key-lock” principle and easily penetrate into a lymphocyte.

The process of development of viral infections in organism is based on the biochemical reactions, whose rate is controlled not only by enzymes, but also by spin states of reagents.

As is known from spin chemistry, if molecules entering a chemical reaction have antiparallel spins (singlet state), the chemical bond can be formed. But if the interacting molecules have parallel spins (triplet state), then the chemical reactions in a triplet pair cannot run in most cases, because the prohibition of chemical reactions by spin is insuperable.

If a patient drinks coherent water, its organism passes to the coherent state (effect of synchronism). This state holds for 15 sec, and then the process of decoherentization is running for 12 h.

The decoherentization is accompanied by a decrease of the frequency of oscillations, but the phase is conserved. The decrease of the frequency affects the processes of spin exchange between HIV virus and Ò-lymphocytes CD4+ on the surface, which participate in the reaction of polymerization. This influence appears by two reasons. First, the orientation of the spin of one of the molecules related to the decoherentization changes many times during the formation of a chemical bond. Second, the spin state of molecules changes arbitrarily. As a result, the singlet pairs of molecules recombine in the triplet ones, and the efficiency of a chemical reaction of polymerization (HIV — ÑÕÑR-4 — lymphocyte CD-4) decreases sharply. In this connection, the replicative activity of HIV drops. The virus remains in the intercellular region, is recognized by cells of the immune system, and is destroyed.

 

The example of a laboratory study of the coherent and noncoherent states of water.

 

We have used L-polarized coherent water, which was caused by the fact that the structure of all protein molecules of human organism has L-torsion. Respectively, coherent water must be complementary to human organism.

We studied the dispersions of a disordering of spin structures of water in the initial and coherent states and in a state after the decoherentization.

To register such changes, we applied an apparatus-programmable complex “Oberon.” Its functioning is based on the principle of the amplification of an initiating signal at the decay of metastable spin systems by means of the action of an external magnetic field and low-frequency (up to 8.2 Hz) sound on them. Under the action of the magnetic field and sound, there occurs the disordering of the spin structures of delocalized electrons of water, which causes the appearance of unstable metastable states. The decay of these states plays the role of an amplifier of the initiating signal registered by “Oberon.”

On the plots in Fig. 1, we present the dispersions of a disordering of spin structures of water in the initial (1) and coherent (2) states and after the decoherentization (3).

 

It is seen that the dispersions of spin structures of water in the N- and S-th directions of the induction in the initial state and in the state after the decoherentization differ by 15%. This exceeds the measurement error equal to ± 10% and indicates that, in the process of decoherentization, the characteristic frequency of water is changed, which causes the conversion of singlet spin states and, on the other hand, hampers the desynchronization of water structures in the connection with the conservation of a phase.

 

2.                     In healthy organism, all processes are running synchronously. In this case, the cells exchange information with one another on the cellular level in the ultraviolet range with wavelengths of 240-380 nm. Despite a significant width of the range, where the exchange of information happens, this exchange is realized with the same phase, i.e., coherently. This yields the coherence and, respectively, the synchronism of all processes in human organism.

At a disease, the synchronism of processes in organism is broken. This occurs not only on the cellular level, but affects the endocrine, immune, and other controlling systems. But if a disease becomes chronic, the degree of desynchronization of organism increases, by causing the extension of the disease onto other organs and systems.

The consumption of L-polarized coherent water complementary to organism leads to the recovery of the synchronism of the processes in organism and, in particular, of systems such as the immune and endocrine ones.

 

It is of great importance that the recovery of the synchronous state of cellular structures is accompanied by an increase of the intensity of intracellular informational exchange and the selectivity of processes. Moreover, the surfaces are self-purified from catalytic slags, etc.

Therefore, the usage of L-polarized coherent water brings back the synchronism and the vital force to a sick human organism and, hence, sanitizes it.

 

 

 

 

 

Teleportation of properties of vaccines

Teleportation of Properties of Vaccines

 

V.G. Krasnobryzhev

In the last decade, the theme of quantum teleportation is firmly held on pages of purely scientific publications, and this scientific-fantastic term becomes truly scientific. At the same time, the reality of quantum teleportation remains to be one of the most disputable themes in the scientific world. In fine physical experiments, the transfer of information from one quantum particle to another one was successfully realized, though the distance between particles was huge as compared with their sizes. In this case, the transfer of information occurs instantly, without any fields, and is independent of the distance.

At the present time, at least three scientific communities – Austrian, Italian, and American – are carrying on the intense studies in this field and have reported on the successful teleportation of spin characteristics of photons and atoms of beryllium and calcium under laboratory conditions.

This qualitatively new trend was supported by the experiments including macroscopic objects. These experiments have demonstrated that a system by spin degrees of freedom is a single unit, and the quantum correlations not only determine the behavior of a macroscopic system, but also turn out stronger than the classical correlations [1, 2].

In this connection, it is actual to create a System, which would realize the teleportation of properties of drugs into organisms of animals and men/women at any distance, by inducing a therapeutic effect there.

In order to solve such a problem, it is necessary to consider the cellular structures of organisms. The studies by V. Yamskovaya and I. Yamskov [3] showed that the transfer of regulatory signals in organisms on the cellular level is ensured by small matrix (SM), whose composition includes low-molecular glycoproteins, for example, adhelon at a concentration of ~ 10-8 M and water. Adhelon and other glycoproteins separated from organism in the form of aqueous solutions possess a strongly manifested pharmacological effect at a concentration of ~ 10-8 M. The spatial structure of SM, whose state is described in terms of a liquid crystal, is permanently modified due to a change of properties and concentrations of its components, including the supermolecular ensembles of water (associates).

The state of supermolecular ensembles of water in SM determines its functional ability to induce and to hold a state, which ensures the reading, propagation, and annihilation of informational signals arrived from outside at cellular receptors.

1.                     M. Kurik considers that the carriers of controlling semantics on the histological and cellular levels are water associates or associates in aqueous solutions, as well as cluster and fractal structures [4]. In this case, the active cause of regulatory signals perceived by a cell or cellular organelles is a complicated geometric form of associates and the structure of physical fields adherent to an associate.

It was shown in [5] that if a molecule of some substance appears in water, the spatial spin configuration of the adjacent water environment is changed. This concerns the spins of protons (nuclei of hydrogen, water molecules) so that a new configuration makes copy of the characteristic structure of the spin configuration of this molecule. There are the experimental bases to believe that, due to a short-range character of the spin dynamics of molecules of a substance, only several layers of their spin proton copies are formed near such molecules.

By virtue of this fact, the spin proton copies of molecules of a substance render the same action on alive objects on the field level as the substance itself. On the level of the experimental phenomenology, it was known in homeopathy [6]. Then this phenomenon was studied in [7] on a extended biochemical material, rediscovered in [8] and [9], and developed in [10].

For example, works [11] and [12] have demonstrated the direct therapeutic effect of tocopherol and glycoprotein in various concentrations, down to superlow ones, though physics and biology forbid such a solution to possess a therapeutic effect in all cases.

The reality of the situation under discussion can be explained on the physical level with the use of spin models applied to the description of the mechanisms of activity of biological objects, which are involved in the dynamics of spin structures. The biochemical processes running in biological objects generate molecular structures, which play the role of spin nonseparable systems and realize the interaction between particles depending on some parameters.

A special interest in the system interconnections of the above-mentioned effects and states is caused by the spin coherent state, which means the spin coordination in a macroscopic system realized by means of nonlocal correlations. The experimental practice indicates that any biological object can be transferred in the coherent state, whose frequency is determined by the characteristic frequency of a molecular structure of water.

It was established with the use of the methods of experimental studies of the phase structure of liquid crystals that water with a characteristic ordered structure entering an organism is responsible for its coherent state. This assertion is of fundamental meaning, because an action with very low intensity on such a structure can induce a strong response of the system (of organism) [14].

Hence, by transferring an organism in the coherent state and by introducing some information in it, one can launch the intracellular processes directed to the production of own medicinal means (including the imaginary ones) with a certain pharmacological effect. Such therapy is referred to complementary medicine, whose methods are directed to the mobilization of protective mechanisms functioning by the principle of self-regulation in human organism.

In correspondence with the Program of teleportation of properties of drugs, the “Teleport” system was developed. This system has successfully realized the remote transfer of the properties of medicinal vaccines.

The principle of action of the System is based on the use of the effects of entangled quantum states between the translation block and a patient. The System realizes the teleportation of spin replicas (spatial configurations) of the protein fragments of vaccines onto an organism, being the object of vaccination, and induces the appropriate immune response in it.

The scheme of the System is presented in Fig. 1.

1 – generator of spin states, 2 – resonator, 3 – chip-translator of spin states,

3 – chip-inductor of spin states, 5 – vaccine, 6 – the object of action – Patient,

 

After the switching-on of generator of spin states 1, the spin coherence of water in resonator 2 is brought to the required level. Simultaneously, the entabgled chip-translator 3 and chip-inductor 4 are transferred in the coherent spin state at the characteristic frequency of water. Then we introduced a single dose of vaccine into the resonator and obtained 5 × 10-5 M solution.

After that, we mounted a chip-inducer onto the body of an object of vaccination. The System for the teleportation was positioned at a distance of 10 km from the objects under study. In all cases the duration of the continuous teleportation action was equal to 36 h.

For the teleportation, the following vaccines were used:

— vaccine “Influvac” for the prophylaxis of influenza, which was produced by “Solvay Pharma” (the Netherlands) and contained hemagglutinin and neuraminidase of viral strains À10/99(Í3N2), À20/99 (H1N1), and Â379/99;

— vaccine “Twinrix” for the prophylaxis of hepatitis À or Â, which was produced by “SmithKline Beecham Biologicals S.A.”.

The teleportation was realized onto human organisms (volunteers) and onto laboratory animals (rabbits):

1.                     a) vaccine “Influvac” — onto 5 rabbits,

2.                     b) vaccines “Influvac” and “Twinrix” — onto 5

The results of experiments were estimated by the presence of appropriate antibodies in biological objects and by the rate of formation of the relevant immune response (under normal conditions of vaccination the immune response is realized in 7-10 days).

In Table 1, we present the obtained results of titration of the analyzed samples of blood of the objects of the teleportational vaccination for the presence of specific antibodies.

 

Results of titration of blood samples under the teleportational vaccination of organisms

 

Table 1

 

Object of influence

 

Quantity of antibodies on an antigene (un / ml)

Vaccine «Influvac»

Vaccine «Twinrix»

H3N2

H1N1

B

HA

HbsAg

C

ÒV

C

ÒV

C

ÒV

C

ÒV

C

ÒV

the rabbits

in 36 hour

in 8 days

in 14 days

 

0

 

1024

8

256

 

0

 

 

 

16

10240

 

0

 

1024

256

256

 

 

 

 

the volunteers

in 36 hour

 

14

 

256

 

0

 

32

 

26

 

512

 

negative*

 

positive

 

0

 

0

 

C – control indices; TV – indices after the teleportational vaccination.

* — in the immunological practice, the immune response of organism to antigen ÍÀ is determined only in the form negative or positive.

 

The immune response of organisms was realized in 36 h instead of 7-10 days.

The reason for the absence of the immune response to protein fragment HbsAg is not known yet, but the practice of vaccination testifies that the full immunization of human organism occurs in 6 months after 3 injections.

The rapidity of the teleportational vaccination effect can be explained by the participation of the maximum pool of the organism’s lymphocytes in the realization of an immune response and by omitting the process of cloning. The spin replicas which are translated into the vaccination object play the role of a “master-key” intensifying the process of immunization.

 

Conclusions and perspective

 

As a result of these studies, we have established that the macroscopic quantum nonlocality is the objective reality and that the word ”quantum” indicates that the state of a system under study can be described by quantum methods, for example, with the density matrix method.

The main property of the resource of macroscopic quantum nonlocality consists in the fact that the teleportation of spin states onto a remote macroscopic object (located at infinity) creates a continuously supported coherent state in it. As a result, such an object can be used to enhance the efficiency of already available and also of future technologies.

We are convinced that the development of negatronic miniature devices aimed at the realization of teleportational communication at unlimited distances is possible.

The fabrication of highly efficient photochemical generators of hydrogen with the use of coherent water, catalysts and UV radiation in the interval 170-180 nm is promising.

Our study also opens the way for the teleportation of properties of medicinal preparations, including the teleportation of vaccines, which is especially important under conditions of space flight.

As a result of complex experiments executed on some heat and electric power plants we obtained a decrease of the consumption of coherent coal in the production of electric power of 16 % on average with the corresponding decrease in emissions of ÑÎ2 into the atmosphere. In this case, ~ 500,000 tons of coals were transferred into the continuously supported coherent state.

Also the consumption of energy at the recrystallization annealing steel of coherent state was decreased by 36-40%.

 

References

 

1.                     Joos E., Zeh H. D., Kiefer C., Giulini D., Kupsch J. and Stamatescu I. O. Decoherence and the Appearance of a Classical World in Quantum Theory, (Springer-Verlag 2003).

2.                     Zurek W. H. Decoherence, einselection and the quantum origins of the classical, Rev. Mod. Phys. 75, 715 (2003).

3.                     Quantum Mechanics on the Large Scale, Banff Center, Canada, Peter Wall Institute at UBC. A 5-day conference (April 12–17, 2003) and a 10-day workshop (April 17–27, 2003).

4.                     Calsamiglia J., Hartmann L., Dur W. Spin gases: quantum entanglement driven by classical kinematics // Phys. Rev. Lett. 2005. Vol. 95. — P. 1805021-4.

5.                     Dur W., Briegel H.-J. Stability of macroscopic entanglement under decoherence // Phys. Rev. Lett. 2004. Vol. 92. — P. 1804031–4.

6.                     Hein M., Dur W., Briegel H.-J. Entanglement properties of multipartite entangled states under infl uence of decoherence // Phys. Rev. A. 2005. Vol. 71. — P. 0323501-25.

7.                     Doronin S. I. Multiple quantum spin dynamics of entanglement Rev. A 68, 052306 (2003).

1.                     Chou C. W., de Riedmatten H., Felinto D., Polyakov S. V., van Enk S. J. and Kimble H. J. Measurement-induced entanglement for excitation stored in remote atomic ensembles, Nature 438, 828 (2005);

2.                     Chaneliere T., Matsukevich D. N., Jenkins S. D., Lan S.-Y., Kennedy T. A. B. and Kuzmich A. Storage and retrieval of single photons transmitted between remote quantum memories, Nature 438, 833 (2005);

3.                     Eisaman M. D., Andre A., Massou F., Fleischhauer M., Zibrov A. S. and Lukin M. D. Electromagnetically induced transparency with tunable single-photon pulses, Nature 438, 837 (2005).

11.                  J-W. Pan, D. Bouwmeester, M. Daniell, H. Weinfurter, and A. Zeilinger, Experimental test of quantum nonlocality in three-photon Greenberger-Horne-Zeilinger entanglement, Nature, 403, 515 (2000).

1.                     Ghosh, S., Rosenbaum, T. F., Aeppli, G. & Coppersmith, S. N. Entangled quantum state of magnetic dipoles. Nature 425:48-51 (2003).

13.                  Stodolsky L., in Quantum Coherence Proc. Intern. Conf. on Funda­mental Aspects of Quantum Theory, to Celebrate 30 Years of the Aharonov-Bohm Effect. USA, 1989 (Ed. J.S. Anandan) Singapore: World Scientific, 1990) p. 320.

14.                  Giulini D. et al. Decoherence and the Appearance of a Classical World in Quantum Theory (Berlin: Springer, 1996).

15.                  Mensky M.B. Quantum Measurements and Decoherence: Models and Phenomenology (Dordrecht: Kluwer Academic Publ., 2000).

16.                  Ê. Ì. Salikhov. 10 lectures on spin chemistry./ Chemistry and Computational Simulation. Butlerov Communications. 2001. Vol.1. No.4.

1.                     Doronin S.I. Qvantovaja magija. St.Peterburg, 2009, p. 336.

2.                     Krasnobryzhev V. Sposób I urządzenie do modyfikacji paliwa. Patent Nr. 207357 Rzeczypospolitej Polskiej.

19.                  Buhks On Urbach rule theory for impurity light absorption. 1975 J. Phys. C: Solid State Phys. 8 1601-1606.

1.                     Vyazovkin S, Sbirrazzuoli N.. Mechanism and kinetics of epoxy-amine cure studied by differential scanning calorimetry. Macromolecules, 1996, v. 29, N6, 1867 — 1873.

2.                      Vyazovkin S. Kinetic concepts of thermally stimulated reactions in solids: a view from a historical perspective.  Int. Rev. Phys. Chem., 2000, 19, 45.

 

The Global Resource of Macroscopic Quantum Nonlocality

The Global Resource of Macroscopic Quantum Nonlocality

 Krasnobryzhev1

 

We have shown experimentally that  the  macroscopic  quantum  nonlocality  is objective and can  be  determined  by  classical  methods  such as Nuclear Magnetic resonance spectrometry, the measurement of the absorption of light by water in the ultraviolet range and changes in the differential resistance and the electric  capacitance of  water as functions of the frequency of a current  passing through it, and  the  thermogravimetry  of  changes  in  the  activation  energy  due to the creation of a stable coherent state in a remote macroscopic object.

 

In recent years the achievements of experimental and theoretical studies of quantum nonlocality have transformed themselves into a completely new paradigm of reality. Already today one can assert that those achievements will gradually lead to profound changes in the comprehension of the physical reality.

Macroscopic quantum nonlocality, as a particular type of interaction, is a global intrinsic property of the classical world which arose, according to the cosmological theory of decoherence [1, 2], from a nonlocal source of reality.

This hypothesis has been confirmed by results of physical experiments carried out during the last few years, which convincingly prove the presence of a quantum entanglement in macroscopic systems. This fact allows for the far reaching conclusion that the entanglement of many various degrees of freedom in macroscopic systems has a significant fundamental and philosophical sense by challenging the basic ideas of the nature of the physical reality [3].

It is obvious that the time has come when the objective results of experimental studies help scientists to direct their efforts towards the practical use of a fundamentally new nonlocal resource, by opening a path from fundamental nonlocal reality to classical reality.

 

Entanglement in a macroscopic medium and suppression of decoherence

 

Macroscopic entanglement is based on quantum entanglement and manifests itself as a correlation of internal degrees of freedom without the intervention of local carriers of interaction.

Despite successes achieved in the development of the successive theory of entangled states [4, 5, 6, 7], the necessary condition for its application is the availability of a measuring tool allowing one to identify elements of it’s physical reality. This condition has focused the efforts of theoretical and experimental physicists on applied studies that means on the comprehension of the role of macroscopic entanglement in nature and on the use of this nonlocal resource [8, 9, 10].

Consistency, as a feature of quantum entanglement, has been confirmed by well-known experiments concerning macroscopic entanglement, which show that a system is the integral whole by spin degrees of freedom [11], and that quantum correlations not only determine the behavior of the macroscopic system but turn out stronger than the classical ones [12].

The results of studies presented hereafter are based on the fact that the states of entangled objects are independent of measurements performed on them, which allows one to manipulate the quantum entanglement of remote objects. At the beginning, these objects represent an integral system that is entangled by the internal spin degrees of freedom. After the division of the object into parts and their removal from one another, a certain part of subsystems of their common system belongs equally to these objects. The correlation of their spin degrees of freedom is conserved irrespective of the distance between the separated parts of the system, and the behaviors of spins in these parts are consistent.

The main reason preventing the use of the global resource of macroscopic entanglement is related to the problem of decoherence [13, 14, 15]. In order to solve this problem, the method of suppression of decoherence is being proposed here. It is based on the use of an anisotropic single crystal with oriented nuclei as a nonseparable system, where the behaviors of spin degrees of freedom are consistent.

Let us consider the system of oriented nuclei in an anisotropic single crystal. By Ή, we denote the energy operator of this system. The stationary (eigen-) states ψk  and the energy levels of these stationary states Ek can be found by solving the Schrödinger equation [16].

According to quantum mechanics, the system can be in a state characterized by a linear superposition of stationary states

The measured quantity is the squared modulus of the wave function

This quantity consists of two parts. The first part of the equation characterizes the populations |ck|2 of stationary states ψk in a linear superposition. The second part indicates that the contributions of different stationary states to the observed value interfere with one another and the quantities c*nck (n ¹ k) characterize a coherent state of the quantum system.

The energy of an anisotropic single crystal can be expressed in terms of an analog of the “spin excess” [17]. In particular, we assign the maximum value of energy of the single crystal to the state denoted by |111…1ñ. If the single crystal interacts with a local object, whose energy state is |000…00ñ, and then the energy gradient between them will be at a maximum. In this case, the energy is redistributed between the single crystal with energy Å1 and the local object with energy Å2, so that the total energy Å is invariable [17]. As a result, the energy flow drives the “single crystal – object” system into the superpositional nonseparable state  In this case, decoherence does not occur.

 

Composition and the principle of action of a system of the teleportation of spin states

 

While developing the idea of the creation of the global resource of macroscopic quantum nonlocality, a System of Teleportation of Spin States was constructed. This system allows for the production of a continuously supported coherent state in a remote macroscopic object [18]. Moreover, the attainment of the coherence is represented as the limiting spin saturation of the remote object, which corresponds to its characteristic frequency and is attained due to the resonance exchange by energy between the spin and nuclear systems.

In Fig. 1, we give the scheme of the System of the Teleportation of Spin States (below, we will write the System). The System includes:

1.                     A Generator of Spin States (GSS), which is a unit on the basis of a single crystal with a preferred orientation of nuclear spins.

2.                     A Resonator, which ensures the spin saturation and the long-term conservation of spin coherence.

3.                     A Chip-translator and a chip-inducer, which form a macroscopic singlet couple made of a material with translational symmetry.

4.                     A Remote object of teleportation action.

 

Action principle of the System:

1.                     In the resonator, one places a material analogous to the material of the object of action. For example, if the object of action is water, coal, or steel, one places water, coal, or steel respectively in the resonator.

2.                     A chip-inducer is fixed on the object of action. A chip-translator is constantly present in the resonator.

When the GSS is switched on, spin saturation of the material medium in the resonator happens. The limiting level of saturation corresponds to the spin coherent state of the material medium. Simultaneously spin saturation in the “chip-translator – chip-inducer – object of action” chain occurs. This results in the coupling of the resonator and the object of action, so that the remote object transits in the coherent state. After this procedure, the remote object can be subjected to a target application.

 

In what follows, we describe the following themes:

1.                     NMR spectrometry of macroscopic nonlocality.

2.                     Properties of water in the state of macroscopic nonlocality.

3.                     Activation energy of coal in the state of macroscopic nonlocality.

4.                     Teleportation of properties of vaccines.

 

NMR studies of macroscopic nonlocality

 

The experiment was carried out with the use of a System for the Teleportation of Spin States (Fig. 1) and an NMR-spectrometer. During the experiment, we measured the time of relaxation of the transverse component Ò1 (spin-lattice relaxation). As an object of study, we choose hydrogen-containing samples such as gasoline and Diesel fuel. Prior to the experiment, we had measured the relaxation time of the transverse component Ò1 of the samples in the equilibrium state. Then, in agreement with the scheme shown in Fig. 1, the substance under study was filled in flasks with chip-inducers attached to them. The generator of spin states, a resonator, and a chip-translator were at a distance of 40 km from an NMR-spectrometer. After switching on the GSS, the samples in the flasks were transferred into the coherent state during 12 h. Then a sample of the substance was filled in a test tube and placed in an NMR-spectrometer to measure the time Ò1.

The processing of the results of measurements was made with the software PeakFitÒÌ. The experimental results are presented in Table 1.

 

Table 1| The results of measurements of the relaxation time of the transverse component Ò1

 

Studied samples

the relaxation time, ms

the equilibrium state

the coheren state

T1

T11

T12

 

T1

T11

T12

Diesel fuel

672±72

514±22

1410±81

 

805±12

441±35

999±79

gasoline

2197±33

 

 

 

2946±15

 

 

The experimental results indicate:

1.                     The relaxation time of the transverse component Ò1 of samples in the coherent state is different from that of a sample in the equilibrium state and exceeds the systematic error of measurements.

2.                     The teleportation of spin states at a distance of 40 km is realized.

 

Properties of water in the state of macroscopic nonlocality

 

As is known, an external electric field polarizes a medium, where an additional electric field compensating the external one arises. In other words, if a light beam passes through water, water actively interacts with light by nonlinearly absorbing it. In this case, the maximum absorption is observed in the ultraviolet range. In our studies, we used drinking water, which was transferred into the coherent state with the help of the system of the teleportation of spin states (Fig. 1). The transition time in the coherent state for water was equal to 12 h. The generator of spin states, a resonator, and a chip-translator were at a distance of 10 km from the object of studies.

Characteristics of water: Acid-base balance (ðÍ) = 7.8, Electric conductivity σ = 1020 (μSm), Total dissolved solids (TDS) = 1150 (mg/liter), The oxidation/reduction potential (ORP) = +142 (mV)

We studied the absorption spectra of coherent or noncoherent water in the ultraviolet (UV) range with the help of a spectrophotometer Libra S22 UV/Vis (Biochrom Ltd.) and relative variations of the differential resistance and the electric capacitance of samples of water as functions of the frequency.

 

All measurements were executed relative to the control sample of water at a temperature of 293 K. The results of these studies are presented in Fig. 2.

 

Figure 2 | Influence of the teleportation of spin states on the properties of watera – change in the absorption of UV radiation by water (1 – water in the equilibrium state,  2 – water in the coherent state),  b – relative differential resistance of water R0/Rc versus the frequency of a current passing through water, where R– resistance of water in the equilibrium state, Rc – resistance of water in the coherent state; c –relative variation in the electric capacitance of water versus the frequency, where Ñ– capacitance of water in the equilibrium state, Cc – capacitance of water in the coherent state.

 

Fig. 2a shows that the absorption spectra of coherent water differ significantly from those of noncoherent water. These UV spectral sections of the absorption of water occupy the interval of wavelengths 200 – 240 nm. The absorption in this spectral interval is formed by the optical transitions with participation of oscillations of molecules of water and admixtures. The absorption spectrum, like the dependence of the coefficient of absorption on the light wavelength (the energy of photons), is described by the exponential dependence at the given temperature, i.e. the shape of the absorption spectrum obeys the Urbach rule [19].

In Fig. 2b we show the variation of the differential resistance of samples of noncoherent water relative to that for coherent water (R0/Rc) as a function of the frequency of a current passing through water. As one can see, coherent water manifests a wide dispersion band for R0/Rc in the interval 2.7 – 10.2 Hz. The registered decrease of the differential resistance is analogous to the property of negatronic systems.

In Fig. 2c, we present the variation of the electric capacitance of samples of coherent water relative to that of water in the equilibrium state (Ñc0) as a function of the frequency. Remark the wide dispersion band with a maximum at 100 Hz.

The performed studies indicate that water transits in the coherent state due to the teleportation of spin states. This increases the nonlinear absorption of water in the UV range and causes both the appearance of the negative differential resistance and an increase in the electric capacitance, which can be measured by classical methods.

 

Activation energy of coal in the state of macroscopic nonlocality

 

In our studies, we used brown coal, which was transferred in the coherent state with the help of the System of the teleportation of spin states (Fig. 1). The GSS, a resonator, and a chip-translator were at a distance of 70 km from a laboratory. The duration of the transition in the coherent state for coal was    12 h. The size of coal grains was 1 – 1.2 mm. The content of the organic component was 80.3%, and the hygroscopic humidity was 4.1%.

We studied the variation of the coal activation energy at its transition in the coherent state. The value of activation energy was determined with the help of the “Free Kinetics” model, which allows one to carry out exact calculations for such complicated reaction as combustion.

The model is based on the theory by S. Vyazovkin [20, 21], in which the conversion function f(a) and the activation energy are constants under conditions where some other parameters vary. In calculations within this model, three dynamical curves with different rates of cooling (b) are required.

The determination of the activation energy was performed with the help of a thermogravimeter TGA/SDTA/851of the Mettler Toledo firm.

As a result of the transit of coal into the coherent state, we obtained a decrease of the activation energy by 56.7% relative to that in the equilibrium state (Table 2). This testifies to a decrease of the energy barrier that should be overcome in the case where coal burns in the coherent state.

 

Table 2 | The values of coal activation energy in the equilibrium and coherent states

 

State of coal

 

Activation energy

Decreasing of

activation energy

the equilibrium state

378 kJ/mol

0%

the coheren state

164 kJ/mol

56,6%

 

In order to confirm the correctness of the determination of the activation energy, we carried out the thermogravimetric (TG) analysis which reveals a decrease in the mass of a specimen of burning coal as a function of the temperature increment. The results of this analysis are shown in Table 3.

 

Table 3| Results of the TG analysis

 

The rate of heating,

oC/min

Temperature of full burning out of test of coal, ÎC

Difference

temperatures, OC

 

the equilibrium state

 

the coheren state

5

540

540

0

10

580

540

40

15

630

560

70

 

As is seen in Table 3, coal burns identically in both states at the rate of heating equal to 5oC/min (Ò ~540oC). At the rates of combustion equal to 10oC/min and 15oC/min, we observed a decrease in the burning temperature of coherent coal by 40îÑ and 70îÑ, respectively, relative to that of coal in the equilibrium state. An increase in the coal combustion rate at the lower temperature testifies to a growth of the reactivity of fuel in the coherent state and to its greater chemical activity to oxygen, which is related to a decrease in the activation energy.

 

A system of quantum communication

 

The quantum (teleportation) communication is realized instantly irrespective of the distance between the transmitting and receiving Systems. The main elements of these Systems are a chip-translator (transmitter) and a chip-inductor (receiver), which are quantum-mechanically entangled by spin and are formed from a macroscopic matrix of spin-entangled nuclei.

When the spin state of the nuclei of atoms of the chip-translator is changed, the spin states of the nuclei of atoms of the chip-inductor are also simultaneously changed. In this case, the exchange by spin states (information) between the chip-translator and the chip-inductor occurs instantly without any field carriers and is independent of the distance..

Such a type of communication is considered to be trivial, since the entangled nuclei of atoms of the chip-translator and the chip-inductor have the common wave function.

In Fig. 1, we show the scheme of the experimental System of quantum communication. In this system, we used the universal system of teleportation of spin states similarly to other technologies.

1 – generator of spin states (GSS), 2 – resonator, 3 – chip-translator À,

4 – chip-translator Â, 5 – chip-inductor, 6 – spectral analyzer, 7 – generator.

 

The System of quantum communication includes:

GSS 1, resonator 2, chip-translator À 3, chip-translator  4, which is a dielectric of capacitor Ñ1, chip-inductor 5, which is a dielectric of capacitor Ñ, spectral analyzer 6, whose input is connected with capacitor Ñ2, generator 7 connected with capacitor Ñ1, In this case, chip-translator 3, chip-translator 4,  and chip-inductor 5 are entangled by spin.

As a dielectric material, we used: a) water. b) textolite, c) ceramics.                                                                        

The details of the experiments are as follows:

1.                     The spectral analyzer, whose input is connected with capacitor Ñ2, was positioned at a distance of 10 km from the generator connected with capacitor Ñ1 and from GSS and the resonator.

2.                     In the resonator, we placed a dielectric material (e.g., ceramics) and mounted chip-translator À 3.

3.                     After the switching-on of GSS, the resonator, chip-translators 3 and 4, and chip-inductor 5 were transferred in the coherent state.

4.                     The sequence of the action of the generator on capacitor Ñ1:

 

2.                     a) dielectric material is water – the high-voltage generator is switched-on in 5 sec after the spectral analyzer. The action was high-voltage discrete for 5 sec. The spectra are given in 2.

style='box-sizing: inherit;font-style:inherit;font-weight:inherit;outline: 0px; box-sizing: inherit;font-style:inherit;outline: 0px' class="alignnone size-full wp-image-96" srcset="https://web.archive.org/web/20210517230938im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_131648.png 605w, https://web.archive.org/web/20210517230938im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_131648-300x56.png 300w" sizes="(max-width: 605px) 100vw, 605px" v:shapes="_x0000_i1036">

Fig. 2.

3.                     b) dielectric material is textolite – the high-voltage generator is switched-on in 5 sec after the spectral analyzer. The high-voltage action was of the Morse-code type. The spectra are given in 3.

4.                     a) the dielectric material was ceramics; the generator was switched-on in 5 sec after the spectral analyzer. We used the vocal and musical actions for 5 sec. The spectra are presented in 4.

style='box-sizing: inherit;font-style:inherit;font-weight:inherit;outline: 0px; box-sizing: inherit;font-style:inherit;outline: 0px' class="alignnone size-full wp-image-98" srcset="https://web.archive.org/web/20210517230938im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_131745.png 626w, https://web.archive.org/web/20210517230938im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_131745-300x262.png 300w" sizes="(max-width: 626px) 100vw, 626px" v:shapes="_x0000_i1038">

Fig. 4.

 

 

Macroscopic nonlocality and teleportation of properties of vaccines

 

The principle of action of the System is based on the teleportation of spin spatial configurations (replicas) of protein fragments of vaccines to the organism of an object of vaccination (a percipient) by inducing the appropriate immune response in it. In this case, the body of a percipient is transferred in the coherent state at a characteristic frequency of water, because 70% of the body consists of water.

The teleported information (state) interacts in the body of a percipient with a supermolecular water ensemble in the near-cell “small matrix” containing also glycoproteins in a concentration of        ~10-8Ì. This ensemble determines the functional ability of the “small matrix” to receive and to propagate the information signals coming from the outside to cell receptors. This results in the fabrication of appropriate antibodies by immunocompetent cells.

We then introduced the following changes in the sequence of applications of the System for the teleportation shown in Fig. 1: we poured water in the resonator with a chip-translator and transfered it into the coherent state, then we introduced a single dose of vaccine into the water and obtained a 5×10-Ì solution. After that, we mounted a chip-inducer onto the body of an object of vaccination. The System for the teleportation was positioned at a distance of 10 km from the objects under study. In all cases the duration of the continuous teleportation action was equal to 36 h.

For the teleportation, the following vaccines were used:

— vaccine “Influvac” for the prophylaxis of influenza, which was produced by “Solvay Pharma” (the Netherlands) and contained hemagglutinin and neuraminidase of viral strains À10/99(Í3N2), À20/99 (H1N1), and Â379/99;

— vaccine “Twinrix” for the prophylaxis of hepatitis À or Â, which was produced by “SmithKline Beecham Biologicals S.A.”.

The teleportation was realized onto human organisms (volunteers) and onto laboratory animals (rabbits):

1.                     a) vaccine “Influvac” — onto 5 rabbits,

2.                     b) vaccines “Influvac” and “Twinrix” — onto 5

The results of experiments were estimated by the presence of appropriate antibodies in biological objects and by the rate of formation of the relevant immune response (under normal conditions of vaccination the immune response is realized in 7-10 days).

In Table 4, we present the obtained results of titration of the analyzed samples of blood of the objects of the teleportational vaccination for the presence of specific antibodies.

 

Table 5| Results of titration of blood samples under the teleportational vaccination of organisms

 

Object of influence

 

Quantity of antibodies on an antigene (un / ml)

Vaccine «Influvac»

Vaccine «Twinrix»

H3N2

H1N1

B

HA

HbsAg

C

ÒV

C

ÒV

C

ÒV

C

ÒV

C

ÒV

the rabbits

in 36 hour

in 8 days

in 14 days

 

0

 

1024

8

256

 

0

 

 

 

16

10240

 

0

 

1024

256

256

 

 

 

 

the volunteers

in 36 hour

 

14

 

256

 

0

 

32

 

26

 

512

 

negative*

 

positive

 

0

 

0

C – control indices; TV – indices after the teleportational vaccination.

* — in the immunological practice, the immune response of organism to antigen ÍÀ is determined only in the form negative or positive.

 

The immune response of organisms was realized in 36 h instead of 7-10 days.

The reason for the absence of the immune response to protein fragment HbsAg is not known yet, but the practice of vaccination testifies that the full immunization of human organism occurs in 6 months after 3 injections.

The rapidity of the teleportational vaccination effect can be explained by the participation of the maximum pool of the organism’s lymphocytes in the realization of an immune response and by omitting the process of cloning. The spin replicas which are translated into the vaccination object play the role of a “master-key” intensifying the process of immunization.

 

Conclusions and perspective

 

As a result of these studies, we have established that the macroscopic quantum nonlocality is the objective reality and that the word ”quantum” indicates that the state of a system under study can be described by quantum methods, for example, with the density matrix method.

The main property of the resource of macroscopic quantum nonlocality consists in the fact that the teleportation of spin states onto a remote macroscopic object (located at infinity) creates a continuously supported coherent state in it. As a result, such an object can be used to enhance the efficiency of already available and also of future technologies.

We are convinced that the development of negatronic miniature devices aimed at the realization of teleportational communication at unlimited distances is possible.

The fabrication of highly efficient photochemical generators of hydrogen with the use of coherent water, catalysts and UV radiation in the interval 170-180 nm is promising.

Our study also opens the way for the teleportation of properties of medicinal preparations, including the teleportation of vaccines, which is especially important under conditions of space flight.

As a result of complex experiments executed on some heat and electric power plants we obtained a decrease of the consumption of coherent coal in the production of electric power of 16 % on average with the corresponding decrease in emissions of ÑÎ2 into the atmosphere. In this case, ~ 500,000 tons of coals were transferred into the continuously supported coherent state.

Also the consumption of energy at the recrystallization annealing steel of coherent state was decreased by 36-40%.

 

 

1.                     Joos E., Zeh H. D., Kiefer C., Giulini D., Kupsch J. and Stamatescu I. O. Decoherence and the Appearance of a Classical World in Quantum Theory, (Springer-Verlag 2003).

2.                     Zurek W. H. Decoherence, einselection and the quantum origins of the classical, Rev. Mod. Phys. 75, 715 (2003).

3.                     Quantum Mechanics on the Large Scale, Banff Center, Canada, Peter Wall Institute at UBC. A 5-day conference (April 12–17, 2003) and a 10-day workshop (April 17–27, 2003).

4.                     Calsamiglia J., Hartmann L., Dur W. Spin gases: quantum entanglement driven by classical kinematics // Phys. Rev. Lett. 2005. Vol. 95. — P. 1805021-4.

5.                     Dur W., Briegel H.-J. Stability of macroscopic entanglement under decoherence // Phys. Rev. Lett. 2004. Vol. 92. — P. 1804031–4.

6.                     Hein M., Dur W., Briegel H.-J. Entanglement properties of multipartite entangled states under infl uence of decoherence // Phys. Rev. A. 2005. Vol. 71. — P. 0323501-25.

7.                     Doronin S. I. Multiple quantum spin dynamics of entanglement Rev. A 68, 052306 (2003).

1.                     Chou C. W., de Riedmatten H., Felinto D., Polyakov S. V., van Enk S. J. and Kimble H. J. Measurement-induced entanglement for excitation stored in remote atomic ensembles, Nature 438, 828 (2005);

2.                     Chaneliere T., Matsukevich D. N., Jenkins S. D., Lan S.-Y., Kennedy T. A. B. and Kuzmich A. Storage and retrieval of single photons transmitted between remote quantum memories, Nature 438, 833 (2005);

3.                     Eisaman M. D., Andre A., Massou F., Fleischhauer M., Zibrov A. S. and Lukin M. D. Electromagnetically induced transparency with tunable single-photon pulses, Nature 438, 837 (2005).

11.                  J-W. Pan, D. Bouwmeester, M. Daniell, H. Weinfurter, and A. Zeilinger, Experimental test of quantum nonlocality in three-photon Greenberger-Horne-Zeilinger entanglement, Nature, 403, 515 (2000).

1.                     Ghosh, S., Rosenbaum, T. F., Aeppli, G. & Coppersmith, S. N. Entangled quantum state of magnetic dipoles. Nature 425:48-51 (2003).

13.                  Stodolsky L., in Quantum Coherence Proc. Intern. Conf. on Funda­mental Aspects of Quantum Theory, to Celebrate 30 Years of the Aharonov-Bohm Effect. USA, 1989 (Ed. J.S. Anandan) Singapore: World Scientific, 1990) p. 320.

14.                  Giulini D. et al. Decoherence and the Appearance of a Classical World in Quantum Theory (Berlin: Springer, 1996).

15.                  Ê. Ì. Salikhov. 10 lectures on spin chemistry./ Chemistry and Computational Simulation. Butlerov Communications. 2001. Vol.1. No.4.

1.                     Doronin S.I. Qvantovaja magija. St.Peterburg, 2009, p. 336.

17.                  Buhks On Urbach rule theory for impurity light absorption. 1975 J. Phys. C: Solid State Phys. 8 1601-1606

Properties of a Coherent Coal

Properties of a Coherent Coal

 

Viktor Krasnobryzhev

 

The method is developed for the creation of coherent coal and carried out of experiments on studying the change of properties of coherent coal. After coal transition to coherent state the decrease of activation energy being in twice took place.

 

The coherence phenomenon is widely practiced for the description of physical states of a substance joined by the common feature being   the ranking and coordination of the behavior of great number of substance elements. The coherent of collective quantum interactions of a physical structure can cause the appearance of absolutely new physical properties of a substance which make it possible to use it in various forms and on a commercial scale.

It can be expected the increase of reaction yields, selectivity of processes, self-purification of surfaces from catalyst poisons, diffusion processes acceleration etc. And these expectations have been confirmed especially in the case of chemical oscillators with forced oscillations [1-3]. The realizing of the fact that macroscopic coherence is a fundamental property has appeared not long ago and it has stimulated the actively progressing interest.

 

Thermogravimetric Investigation of Coherent Matter

 

Not only molecular but also spin dynamics playing a double part in elementary chemical acts is of great importance in combustion reactions. On the one hand it affects actively the reaction mechanism and kinetics by activation energy. On the other hand spin dynamics reacts very sensitively to the molecular dynamics of an elementary chemical act.

In order to explain the issue of the possibility of coherent control over chemical reactions, passing between two states should be analyzed. By the motion along the reaction coordinate from initial state to final one molecular system will pass through superposition of state [4]. Let at initial time T = 0 a system is in the state 1 of energy E1 and let there is the state 2 of energy E2 equal to E1 i.e. EE1, while the state E2, corresponds to the coherent state (Fig. 1).

Fig. 1. The distribution of molecular energy systems, according to Maxwell-Boltzmann:

where E1 — energy of the system (integral area) in the equilibrium state,  E2 — energy of

the system (the integral of the square) in a coherent state.

 

Let us assume that these two states are connected with transition matrix equal to V by some interaction. We shall consider the probability p(t) to find the system in the state at any instant of time. This probability time dependence depends strongly upon coherence. If the transition from initial state to final state occurs in an incoherent way in the course of time the equalizing of these states population takes place. After the achievement at p = 1/2 in the future these states populations conserve value 1/2. In the case of coherent motion unknown probability is equal to

P = sin(Vt / ž).                                                                                             

 

The following two conditions are absolutely remarkable:

1.                     This probability oscillates i.e. it does not change monotonically as it is expected in the case of coherent motion.

2.                     This probability achieves the value at some instants of time. When this probability becomes equal to 1/2 by Vt / ž = π/4 the two states turn out to be equipopulated. The transition from initial state to final one continues as if from force of inertia until the system complete transition to the state and so on. This example demonstrates that quantum coherence can play very important role in transition processes, chemical reaction and combustion processes.

A fuel coherent state can effect actively the kinetics of combustion processes. In the same time activation energy plays an important role in combustion processes. Its value can be determined by means of the “Free Kinetics” model, which makes it possible to carry out exact calculations for complex reactions such as combustion process.

The model is based on the theory of dr. S. Vyazovkin claiming that conversion function f(α) and activation energy are constants for some variables. Three dynamic curves with various heating rates (β) are required for the “Free Kinetics” model calculation.

The experiments on the influence of the coherent state of fuel on its activation energy was carried out on powdered brown coal with a grain size of 1 — 1.2 mm. Organic component content was 84,4%, hydroscopic humidity – 4,1%. The determination of activation energy value was carried out by means of the termogravimeter GA/SDTA/851of the Mettler Toledo firm.

The results of the measurements of brown coal activation energy in coherent state (the graph left side) and decoherization state (the graph right side) are given in Fig. 1a. Maximum value of activation energy has been determined for coal being in equilibrium state. After coal transition to coherent state the decrease of activation energy from 378 kJ/mol down to 163,6 kJ/mol being 56,7% took place. It demonstrates the decrease of energy  barrier  which  must  be surmounted  by coal combustion in coherent state. The following measurement were carried out in two days after the beginning of the process of coal decoherence. In spite of this process beginning the following decrease of coal energy activation for 16,6% (with respect to coherent state level) is noted.

The measurement carried out on the 7-th day of decoherence process demonstrated for the first time the increase of the value of activation energy but its level was close to the value of corresponding coherent state. This parameter considerable increase was observed only in 10 days after the beginning of decoherence process. In spite of so long decoherence time the return to equilibrium state level did not take place.

Odd behavior of activation energy caused by decoherence can be a consequence of the following processes. The coherent state of coal grains causes solitons forming and is necessary for their stable existence. Decoherence process is accompanied not only by dissipation but useful power conversion.

Internal work being done in this case causes maintaining temporary order in the system. Here, the rate of solitons energy exchange with medium exceeds the rate of energy dissipation in medium. This causes observed activation energy decrease. Further decoherence causes the decrease of the rate of energy exchange of solution with medium, their dissipation and activation energy increase.

Besides the determination of activation energy value the additional analyses of TG (thermogravimetric) curves is carried out. These curves represent the decrease of sample mass (mass ~ 0,3 g) (Y axis is left) corresponding to the level of coal conversion as a function of temperature increase (Y axis is right). The sequence of the process under investigation has been realized by three heating rates 5ºC/min (black line), 10ºC/min (red line) and 15 º C/min (blue line) both for coal being in equilibrium state and in coherent state and given in Fig. 1b.

From the given dependences it is obvious that the temperatures under which coal conversion process ceases are different by variable heating rates. Under heating rate α = 5ºC/min the coal sample total burn out takes place under 540ºC approximately.

Higher temperature (~580ºC) of total coal sample burn out was required by the process under heating rate α = 10ºC/min. Under heating rate α = 15ºC/min the temperature of coal conversion was 630ºC approximately.

Such regularity was not observed during the tests being carried out with coal in coherent state. Total burn out of the given coal portions in this place occurred under low temperature independently of the given sample heating rate.

Under heating rate α = 10ºC/min it is obvious that total coal conversion in equilibrium state takes place under ~580ºC whereas in the case of coal being in coherent state conversion temperature is 40ºC below (~540ºC).

The similar dependence can be observed under heating rate α = 15ºC/min. Maximum degree of coal burn out in equilibrium state is achieved under 630ºC, whereas for coal in coherent state this temperature is 560 ºC (Δt = 70 ºC). This tendency is connected without doubt with the decrease of activation energy determined for coal coherent state.

In addition to the TG analyses we shall trace the trend of DTG (differential thermogravimetric) curves  being  the  first  derivative in  the equations describing the describing the decrease of coal samples mass as a function of temperature. Temperature values corresponding to the function sequential extremes determine here the amplitudes characterized by the highest rate of physical and chemical changes taking place. In the used system X axis corresponds to temperature and the Y axis – process rate which corresponds to the tilt angle of TG curves.

The DTG curves represented in Fig. 1c respond directly the represented above trend of the TG curves for the process of coal combustion in equilibrium and coherent states for three heating rates – 5ºC/min (black line), 10ºC/min (red line), 15 º C/min (blue line).

The first minima demonstrated in Fig. 1c within temperature range 67-96ºC correspond to the process of moisture (hygroscopic) evaporation and will not be taken into account in the following analysis because they do not contribute to the information concerning the influence of coal coherent state upon the process of its burning up.

The behavior chemically decontaminated coke forming by coal sample degassing during its burning up. In this case it is necessary to note that for the coal being in equilibrium state temperature values corresponding to extremes (corresponding to coke burning up) are within wide enough range 395-467ºC    (ΔT = 72ºC) in contrast to narrow range 380-397ºC (ΔT = 17ºC) characterizing the samples of coal in coherent state.

In demonstrates the increase of coal reactivity above 300ºC to be exact. These transfers are obvious  however on the X axis only where ordinate values corresponding to curve maxima for equal heating rates                                                                                                                                       in these states come together i.e. about 0,1 mg/ºC for α = 15ºC/min, 0,13 mg/ºC for α = 10ºC/min,  0,17 mg/ºC for α = 5ºC/min.  It follows from the fact that maximum rates of the process of burning up achieved for these two states of coal are comparable but for coal being in coherent state they are realized under lower temperatures.

As previously by the TG curves analyses for low heating rate (α = 15ºC/min) temperature difference is not observed for the extremes of the curves describing the process of coal burning up in equilibrium and coherent states. In this case the ΔT value takes on a value ~13ºC as temperature difference 381-394ºC. The great difference takes place under heating rate α = 10ºC/min — 41ºC (424-383ºC). The greatest difference is observed under α = 15ºC/min when ΔT achieved the value of 70ºC (467-397ºC).

 

Conclusions

 

As a result of the carried out experiments the confirmation is obtained concerning the opportunity to create coherent state of matter and keep this state up during unlimited time. After coal transition to coherent state the decrease of activation energy being ~57% took place. The system of “industrial resources” of coherent matter is created. The important feature of the created system is a decrease of energy carriers consumption and reduction of greenhouse effect gas emission into the atmosphere. The use of a coherent state of matter in the complex of other measures of wildlife preservation can reduce effectively environmental impact of greenhouse effect gases and oppose global getting warmer.

           

References and Notes

 

1.                     G. Kothe, M. Bechtold, G. Link, E. Ohmes, J. -U. Weidne. // Chem. Phys. Lett.283, 51 (1998)

2.                     W. Hohmann, D. Lebender, J. Muller, N. Schinor, F. Schneider. // J. Phys. Chem. A101, 9132 (1997)

3.                     A.L. Buchachenko. // Coherent chemistry. Moscow, 2002.

4.                     Ê. Ì. Salikhov. 10 lectures on spin chemistry./ Chemistry and Computational Simulation. Butlerov Communications.  2001. Vol.1. No.4.

 

NEW TECHNOLOGY FOR POWER PLANTS

NEW TECHNOLOGY FOR POWER PLANTS

 

“Technology of a Coherent Modification of Coal”

 

V.G. Krasnobryzhev

 

The deficiency of technical achievements, which would allow one to increase of the production of electric energy, is undoubtedly related to the huge volumes of burned coal and to the emission of ÑÎ2 in the atmosphere. This makes the introduction of efficient technologies of combustion of fuels to be a priority actual task of the power industry.

The process of combustion is one of the most complicated known phenomena. During this process, it is necessary to continuously supply a certain amount of energy needed for overcoming an energy barrier called the activation energy to the combustion zone. This energy is transferred from the combustion core to the supplied fuel. As a result, the ideal energy, which would be released under the burning of coal, is decreased by the value of activation energy.

The proposed technology of modification of coal is characterized by that fuel is transferred in the coherent state prior to the combustion. In the coherent state, the activation energy coal is decreased. As a result, the amount of energy, which would be continuously supplied to the combustion zone, is decreased, and this unused part is utilized directly in the process of heating of a heat-carrying agent.

The coherency is a coordinated running of several oscillatory or wave processes in space and in time, in which the phase difference of oscillations of the atoms composing a specific physical structure remains invariable.

 

Studies of the activation energy of coherent coal

 

The large body of thermogravimetric studies of coal showed that the transfer of coal in the coherent state leads to a decrease of the activation energy relative to that in the equilibrium state (Table 1). This testify that the energy barrier, which should be overcome, is decreased in the case where coal is burned in the coherent state, and, respectively, we can economize burned coal.

 

table 1

State of coal

Activation energy

Decreasing activation energy

the equilibrium state

378 kJ/mol

0%

the coherent state 1

260 kJ/mol

31,2%

the coherent state 2

164 kJ/mol

56,7%

 

Besides the determination of the value of activation energy, we carried out the thermogravimetric (TG) analysis to find a decrease of the mass of a probe of burned coal as a function of the increment of the temperature. The results of the analysis are shown in Table 2.

 

TG-analysis

 

table 2

The rate of heating,

oC/min

Temperature of full burning out of test of coal, ÎC

Difference

temperatures, OC

 

the equilibrium state

 

the coherent state

5

540

540

0

10

580

540

40

15

630

560

70

 

As is seen from Table 2, no difference for the full combustion of coal probes at Ò~540oC is observed at a heating rate of 5oC/min. But, at the burning rates of 10oC/ min and 15oC/ min, the burning temperature of coherent coal decreases by 40 îÑ and 70 îÑ, respectively, as compared with that for coal in the equilibrium state.

The increase of the burning rate of coal at a lower temperature testifies to an increase of the reactivity of fuel in the coherent state and to a higher chemical activity of fuel components relative to oxygen.

The coherent state of matter is characterized by a frequency and a phase. One of the characteristics of the process of combustion is the electromagnetic emission frequency. During the process of combustion, the electromagnetic emission interacts with the atoms of fuel in the combustion zone. If the emission frequency coincides with that characteristic of the coherent state of fuel in the combustion zone (or with the frequency of one of the principal harmonics), we have a resonance, and the energy of the process of combustion increases.

In this case, the internal energy of fuel is released. This is seen from the following equation:

Er = E/  {1 /[1 – (ω0 / ωr)2]1/2}

 

Here, År and ωr are the energy and the frequency of oscillations in the resonance state, and Å0 and ω0 are the energy and the frequency of oscillations outside the of oscillations.

The less the structural distinctions of coherent coal (the coal mark, sizes of burned particles, ash content, humiodity, etc…), the higher the coherent emission energy.

Under real conditons, the interaction intensity will be significantly less due to the instability of the frequency spectrum of electromagnetic emission, which is caused by the instability of the structure and the quality of coal, fluctuations of the activation energy, etc. The less the structural difference of coherent coal depending on the coal mark, fragmentation, ash content, and humidity, the higher the coherent emission energy for burned particles of coal.

Therefore, a correction of the frequency of the coherent state of coal can lead to an enhancement of the coal burning efficiency and to a decrease of its consumption.

The determination of the burning efficiency of coherent coal in boilers of various types allowed us to find the spectra of coherent states of coal and to create a configuration of the System of coherentization of coal and to clarify the conditions of its application.

The ideology of this technical achievement is based on the macroscopic quantum nonlocality opening a way to the controlled creation of coherent states of matter and to their use in various processes and in industrial technologies. One of the distinctive features of the proposed approach consists in that the coherentization of material media can be performed without participation of local carriers of any interaction. In this case, the attainment of the coherence is represented as the limiting spin saturation of a remote object corresponding to its characteristic resonance. This coherent state is created due to the resonance energy exchange between the spin and nuclear systems.

In Fig. 1, we present the universal System of coherentization, which allows one to create the continuously supported coherent state of great volumes of coal [Patent Nr. 207357 Rzeczypospolitej Polskiej – V. Krasnobryzhev. Sposób I urządzenie do modyfikacji paliwa]. The System includes

1 – generator of spin states (GSS) – unit for the spin saturation of coal;

2 – resonator, which ensures the long-term holding of the spin coherence;

3, 4 — chip-translator and chip-inductor, a macroscopic singlet pair;

5 —    object of the coherentization – coal on the store.

 

Prior to the switching-on of the System:

1.                     In the resonator, one places a material analogous to the material of the object of action. For example, if the object of action is water, the resonator is filled with water; coal – coal; steel – steel; etc.

2.                     On the object of action, one mounts a chip-inductor. The chip-translator is permanently positioned in the resonator.

If the GSS is switched-on, the material medium in the resonator becomes spin-saturated. The limiting level of saturation corresponds to the spin coherent state of the material medium. Simultaneously, there occurs the spin saturation in the “chip-translator – chip-inductor – object of action” chain. As a result, the coal present at the store is transferred in the coherent state.

The GSS of the System of coherentization is technologically manufactured as a collection of modules each consisting of six (see Fig. 2). Chip-inductors (receivers-activators) are digged-in at a depth of about 1 m near the coal store (Fig. 3).

In 36 h after the switching-on of the GSS, the receivers-activators transfer coal into the coherent state.

The technology requires no operational technical or technological changes.

Experiments with the burning of coherent coal

in boilers of an electric power plant

 

1.                     The first experiment was carried out at the electric power plant N1*, where about 10 mln tons of brown coal are burned for a year in 3 dust boilers and 7 fluidized-bed boilers with a power of 220-250 MW-h.

With the purpose to confirm the efficiency of the burning of coherent brown coal, we carried out the following experiments at a dust boiler of block No. 8:

à) in the equilibrium state – 04-12.02.2006;

á) in the nonstabilized coherent state– 13-16.02.2006;

â) in the stabilized coherent state– 17-20.02.2006.

In the course of experiments, about 220,000 tons of coherent coal were burned. The experimental data concerning the experiment were taken from the computer controlling system of the electric power plant and are shown in Figs. 4 and 5.

In Fig. 4, we present the plots of a variation of the emissions of ÑÎ2 and SOX as functions of the generated power.

The analysis of these plots indicates that the emission of ÑÎ2 decreased from 15% to 14.5% in the period since 17 till 20.02.2006, and the dispersion of values decreased sharply.

 

2.                     The second experiment was carried out at the electric power plant N2* (Poland), where about 4 mln tons of mineral coal for a year were burned in dust boilers. The experiment was performed in two stages: in April–June of 2007 and in September–October of 2007.

The complexity of the experiment was determined by the energetic and qualitative characteristics of coal supplied to the electric power plant from 15 mines.

In this connection, on the first stage, we made a correction of the frequencies of coherent states of coal, which determine an increase of the flame emission intensity (respectively, an increase of the efficiency of the burning of coherent coal) and a decrease of its consumption.

To this end, we chose boiler No. 7, which was equipped with photoelements in its upper and lower parts for the measurement of the flame emission intensity.

In Fig. 6, we present the trend of variations of the flame luminosity in boiler No. 7 (index G) under the burning of noncoherent (01-20.04.07) and coherent coal (20.04-05.06.07). The lower curves show a variation of the flame luminosity – index G12BB03A (upper photoelement), index G12BC03A (lower photoelement). The upper curve indicates a variation of the active power of the generator – index G41N001A).

Fig. 6. The trend of variations of the flame luminosity in boiler No. 7

 

The variations of the flame luminosity shown in Fig. 6 indicate its increase under the burning of coherent coal and, respectively, a higher level of the energy release.

In addition to the above-mentioned measurements, we detected the flame temperatures in boiler No. 7 of the electric power plant under the burning of noncoherent and coherent coals. The measurements of temperatures were performed on various levels of the combustion chambers of boilers with an optical pyrometer ST-8859. The range of variations of the temperature measured by a pyrometer was from -50ÎÑ to 1600ÎC at an optical resolving power of 50:1 and the controlled emissivity from 0.1 to 1.

The data of measurements are presented in Fig. 7.

Fig. 7. Distribution of temperatures in the combustion chamber of boiler No. 7 under the burning

of noncoherent and coherent coals.

 

As a result of measurements, we found an increase of the temperature in the upper zone of a combustion chamber (26.2 m) under the burning of coherent coal as compared with that for noncoherent coal.

After the determination of the mean value of effective frequency of the coherent state, we carried out the second stage of the experiment. During the experiment, the coherent state of coal on the shores was held by chip-inductors positioned along the perimeter of the stores near their bases.

The efficiency of combustion of coherent coal on the electric power plant N2* was estimated for the dust-coal blocks Nos. 1 and 4 with a power of 250 MW since September till October of 2007. For comparison, we took the operation parameters of the blocks in August of 2007 such as the electric power yield (MWh), turns of the suppliers of coal (%) , the supply of air to boilers (%), injections of cooling water on superheaters (ton / h). The results of estimations of the efficiency are given in Tables 3 and 4.

The experimental data were taken from the computerized control systems of these blocks.

 

Comparing the results presented in Tables 3 and 4 with those related to the operation of the blocks in August (coal in the equilibrium state), we may estimate the former as positive. The decrease of the index of turns for the mills on block No. 1 was 10.8% in September and 9% in October. On block No. 4, this index decreased by 9.2% in September and by 4.2% in October.

In this case, it should be taken into account that the caloricity of coal decreased by 1.5% in September and by 3.9% in October as compared with that in August.

The coal energy consumption for the production of electric power was calculated for blocks Nos. 1 and 4. In this case, the turns of the suppliers of coal were recalculated with regard for the weight of coal supplied to a boiler.

For this purpose, we took the following files from the computerized control system of the blocks for August, September, and October: block No. 1 – À41N001A (power, MW-h — scale 250), À03Z064O (coal consumption, ton/h — scale 110); block No. 4 – D41N001A (power, MW-h — scale 250), D44Z064O (coal consumption, ton/h – scale 110).

The calculations of qualitative indices of the caloricity of burned coal (Table 5) were performed with regard for the coal supply, laboratory data on the caloricity of supplied coal, and the laboratory data on samples taken from the feed belts supplying coal to blocks of the 1-st and 2-nd groups. The difference between the 1-st and 2-nd groups consists in the addition of biofuel to coal burned in blocks of the 2-nd group.

 

The caloricity of coal supplied to the blocks of the electric power plant

 

 

Groups

power blocks

Caloric content of coal, GJ / t

 

August

September

Octobe

1 (blocks 1 – 4)

20,877

20,563

20,055

2 (blocks 5 – 8)

20,862

20,354

19,931

 

 

 

 

 

 

Then we determined the consumption of the chemical energy of coal on blocks Nos. 1 and 4 in the case where the generated power is >200 MW-h. The results of processing of the data obtained are given in Tables 6-8.

On the basis of averaged data on the operation of blocks No. 1 and 4, we constructed the plots of the coal energy [GJ] consumed for the production of electric energy [MW-h] (see Fig. 7). They characterize the operation of the blocks in August-October of 2007 at the generated power ≥200 MW-h. This value of power was chosen with regard for the fact that the efficiency of boilers is decreased in this case.

The analysis of the results obtained at a generated power ≥200 MW shows that the coal energy consumption for the production of electric power by block No. 1 decreased by 15.9% in September and by 12.9% in October. As for block No. 4, this diminution was 10.4% in September and 7.4% in October.

At the same time, the decrease of the supply of air to a boiler causes an increase of the coal energy consumption. On block No. 1, the former decreased by 3% in September and by 5.2% in October.

In order to compare the results of calculations given in Tables 6-8 and presented in Fig. 8, we show the characteristic dependences of the coal consumption on the generated power (files À  À41N001A, À03Z064O and À  D41N001A, D44Z064O) in the period from 01.08 till 30.09.2007 in Figs. 9-10 (block No. 1) and 11-12 (block No. 4). The data in Fig. 9-12 indicate the tendencies in the coal energy consumption under the production of electric power analogous to those in Fig. 8.

style='box-sizing: inherit;font-size:2.7rem;font-style:inherit;outline: 0px' class="alignnone size-full wp-image-114" srcset="https://web.archive.org/web/20210517234025im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_132802.png 582w, https://web.archive.org/web/20210517234025im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_132802-300x256.png 300w" sizes="(max-width: 582px) 100vw, 582px" v:shapes="_x0000_i1053">

Besides blocks Nos. 1 and 4, we carried out the evaluation of the efficiency of the burning of coherent coal in September- October relative to that in August in boilers of the 2-nd groups — blocks Nos. 5 and 7. To this end, we determined the consumption of the energy of burned coal at the generated power >200 MW-h, by using the amount of burned coal, ton/month; caloricity of coal, GJ/ton; the amount of burned biomass, ton/month; caloricity of biomass, GJ/ton; the energy of fuel, GJ; and the production of electric power, MW.

The calculations were performed in the following sequence: the energy of fuel (GJ) = caloricity of coal (GJ/ton) × amount of burned coal (tons) + caloricity of biofuel (GJ/ton) × amount of burned biofuel (tons); the monthly consumption of the fuel energy (MJ/MW) = energy of fuel (GJ) / production of electric power, MW

In Table 9, we present the generalized data on the monthly consumption of the fuel energy multiplied by the generated power on blocks Nos. 5 and 7.

 

Table 9

 

Parameter

Month

August

September

Octobe

 

Consumption of coal, in tons

104218

92028

166191

 

Caloric content of coal, GJ / t

20,856

20,248

20,125

 

Consumption of biomass, tonnes

8190

7865

14871

 

Caloric content of biomass, GJ / t

14,715

11,87

10,47

 

The energy of the fuel, GJ

2294201

1956753

3299851

 

Production of electricity, MW

236580

211592

375727

 

The energy consumption of fuel, GJ/MWh

9,7

9,25

9,3

 

Efficiency,%

 

4,9

4,3

 

 

Table 9 indicates that a decrease of the energy consumption for coherent coal under the joint burning with biomass is insignificant. First of all this is connected with a decrease of the amount of air supplied in the process of combustion. In Fig. 13, we present the variations of the air supply (m3/MW-h ) to boilers of blocks Nos. 5 and 7. The comparison of the variations of these characteristics shows that, starting from August, their value decreased continuously and attained the minimum in September.

On the whole, the decrease of the air supply in September relative to August was 4.3% for block No. 5 and 2.6% for block No. 7. In this case, the content of oxygen in exhaust gases of a boiler of block No. 7 decreased by 8.4% in September and by 7% in October.

 

CONCLUSIONS

 

1.                     By performing the experiments on the burning of coherent coal in boilers of the electric power plants, we obtained the following results:

2.                     In the pilot experiment on the burning of coherent brown coal on the electric power plant N1* in the period from 13 till 20.02.06, the emissions of ÑÎ2, NOX, and SOX were decreased by 13%, 16%, and 16%, respectively.

3.                     The experiment on the burning of coherent mineral coal in the period from 01 till 30.10.2007 on the electric power plant N2* is characterized by the following efficiency:

— about 500 thou. tons of mineral coal were transferred in the coherent state on the stores of the electric power plant;

— the coal energy consumption at the production of electric power on blocks Nos. 1 and 4 decreased by ~16% in September relative to August and by 12.1% and 8.4%, respectively, in October at the generated power >200 MW-h. At the same time, the decrease of the supply of air to a boiler causes an increase of the coal energy consumption. On block No. 1, the former decreased by 3% in September and by 5.2% in October.

— the coal energy consumption on blocks Nos. 5 — 7 decreased by 4.9% in September and by 4.3 % in October relative to August.

4.                     The estimation of the experimental results shows that the consumption of coal can be really decreased by 25%. For this purpose, it is necessary:

— to develop an algorithm of the control over the functioning of the suppliers of coal to boilers with regard for variations of the temperature in the flame core;

— to mount the photoelements in boilers for the registration of variations of the temperature in the flame core;

— to use coal with a caloricity of 20-20.5 GJ /ton in the process of combustion.

 

Information sources:

1.                     Data on the supply of coal to blocks – the Department of coal preparation.

2.                     Reports on the supply of coal to blocks Nos. 1-4 and the data on the amount of burned coal — the Department of coal preparation and the dispatching offices of blocks Nos. 1 and 4.

3.                     Data on the caloricity of supplied coal and the caloricity of coal on stores — Laboratory and the Department of coal preparation.

4.                     Data on the mean hourly generated power, supply rate, air supply, amount of oxygen in exhaust gases from boilers, injected cooling water at the control over the temperature of superheated steam, reports on the production of electric power at the electric power plant N2*, the Departments of control over the exploitation and environment protection.

 

References

 

1.                     N.I. Davydov, Study of a system of regulation of the temperature of steam with two advancing high-speed signals, Teploenerg., No. 10, 2002, 17-21.

2 N.M. Kalinina, V.I. Nifad’ev. Procesy  samoorganizacii v detonacionnoy

volne nizkoplotnyh vzryvchatyh veschestv.  http://spkurdyumov.narod.ru/Kalinina10/Kalinina.htm

3.                     Cyril W. Smith, Quanta and Coherence Effects in Water and Living Systems, J. of Altern. and Complement. Medic., 2004, 10(1), 69-78.

4.                     A.L. Buchachenko, Chemistry as Music, Tambov: Nobelistika, 2004. 6.

 

Viktor Krasnobryzhev,

Efficient Decrease of the Toxicity of Diesel Engines

Efficient Decrease of the Toxicity of Diesel Engines

V.G. Krasnobryzhev

 

All types of the modern transport cause a great damage to the biosphere, most dangerous being the automotive one. In the global balance of the contamination of the atmosphere, the share of the automotive transport is 13.3%. But it is as high as 80% in cities.

 

The contamination of the environment due to the functioning of conventional internal-combustion engines consists in the blow-out of the oxides of nitrogen, carbon, and sulphur, as well as aldehydes, hydrocarbons, and suspended particles such as aerosols. The basic principles of a decrease of the amount of dangerous exhausts from internal-combustion engines are given in work [1]. Among them, it is worth noting the improvement of constructional parameters and operation modes (deboosting of a Diesel engine, decrease of the fuel injection advance angle, throttling on the air suction, enrichment of fuel with combustible gases and water vapor, etc.).

 

Diesel engines are widely used in the automotive industry. Their advantages are the high efficiency (up to 35%) and the possibility to use a cheaper fuel. However, the exhaust gases from Diesel engines are toxic and contain such cancer-producing substances as black and complex cyclic and aromatic hydrocarbons.

 

The results of studies performed by Swedish scientists and published in American Journal of Epidemiology indicate that exhaust gases from Diesel engines increase significantly the probability of cancer of lungs. The fuel combustion products for Diesel engines are so cancerogenic as asbestos.

 

The American researchers of the Cincinnati University have established that the exhaust gases from Diesel engines disturb the functioning of the immune system, by damping the activity of a number of substances determining the proper timely reaction of the immune system to the penetration of infectious agents.

 

In exhaust gases, hydrocarbons include the initial and reacted molecules of fuel. Of particular meaning are the exhausts of benzene, toluene, polycyclic aromatic hydrocarbons, and, in the first turn, benzpyrene. All they enter the group of cancerogenic substances, are not removed from the human organism, and promote the formation of malignant tumors.

 

Being stimulated by the legislations of Europe, the USA, and Asia, the producers of cars and trucks over the world make efforts aimed at a decrease of the toxicity of exhaust gases. A lot of ideas are known, but the most promising directions are reduced to three technologies: “fuel cells” (see «ABC» N2/1997)), electric motors, and hybrid engines.

 

Most researchers try to influence the processes of combustion, by varying the chemical composition of fuel, the amount of free radicals in it, and their energy state [2].

Combustion is one of the most complicated phenomena known to scientists. As is known, the combustion is a chain reaction with successive fragmentation of fuel particles into smaller charged ones with creation of radicals. The combustion involves the physico-chemical processes of transformation of the chemical energy of intermolecular bonds, the physical processes of transformation of the energy on the molecular and atomic levels into heat and light, and many other processes running simultaneously.

 

The reaction rate of combustion can be determined from the relation [3, 4]

 

K = (kT/ž) exp(F*/F) exp(-ΔÍ/kT) ,                                                        (1)                                                      

 

where   k  is the Boltzmann constant; T is the temperature; ν is the oscillator frequency; ž  is the Planck’s constant; F* is the statistical sum of singlet spin states per unit volume; is the statistical sum of triplet spin states per unit volume; and ΔÍ is the activation enthalpy, J/g-mole.

 

Any chemical reaction is related to displacements of the nuclei of atoms, which compose the molecules of reagents, and to the rearrangement of their electron environment. The potential energy of a system of atoms is determined by the locations of electrons and nuclei.  Since the distribution of electrons is set by the mutual position of nuclei, any such position corresponds to a single value of potential energy of a system. Any nuclear configuration corresponds to some point on the surface of the potential energy. The transition of a molecule from one surface of the potential energy onto another one is connected with a change of the electron state and/or the spin state of a molecule [5, 6].

In the reactions of combustion, the essential role is played by both molecular and spin dynamics. In elementary chemical acts, the spin dynamics influences, on the one hand, the mechanism and kinetics of a reaction. On the other hand, the spin dynamics is very sensitive to the molecular dynamics of an elementary chemical act.

 

It is known from the spin chemistry [7] that chemical reactions are controlled by two fundamental factors: energy and spin. In this case, the prohibition of chemical reactions by spin is insurmountable. If the molecules colliding in a chemical reaction have antiparallel spins (singlet state), the chemical bond is formed. If the interacting molecules have parallel spins (triplet state), then the reaction product can be formed only in the triplet excited state. Since such states have, as usual, high energies, the chemical reactions for triplet pairs are impossible in the majority of cases.

 

By the Wigner rule, the statistical weights for the coupling of two molecules in the singlet and triplet states are equal to 1/4 and 3/4, respectively. In most cases, the ground state of products of a chemical reaction is the singlet one. Therefore, it should be expected that only one quarter of collisions will lead to the reaction product. As a rule, such processes require no activation, i.e., the activation energy of the reaction is close to zero. The formed molecule will be in the ground electron state. The reaction is running rapidly and efficiently, if the molecule-product can transfer the energy releasing at the formation of a bond to other particles, or this energy can be redistributed over many vibrational modes.

 

As a special feature of the spin dynamics, we mention the possibility of a coherent control over the chemical reactions [8, 9, 10]. In coherent modes, we can expect the high yields of reactions, the selectivity of processes, the self-purification of surfaces from catalytic poisons, etc. due to an increase of the statistical weight of singlet states of colliding molecules up to 1/2. These expectations are realized, in particular, in the chemical oscillators with forced vibrations.

 

Let us return to Eq. (1). It is seen that the reaction rate of combustion can be enhanced due to an increase of the temperature and a decrease of the activation energy. But since the combustion temperature is practically invariable, the single possibility for the control is presented by the activation entropy Sa /k = F*/F.in the form

 

K = À·exp(F*/F),

 

where      À = (kT/2πνž)·exp(-ΔÍ/kT). 

 

We now calculate the reaction rates of combustion in unit volume under conditions of the thermodynamic equilibrium for two spin states which are determined by the Wigner rule with F* = 250000; F = 750000:

 

K1 = À·exp(250000/750000) = 1.39 À.

 

For the coherent state of rteagents, we have F* = 500000; F = 500000, and

 

K2 = À·exp(500000/500000) = 2.73 À.

 

As is seen, the reaction rate of combustion increases by a factor of 2. In this case, it should be considered that this example bears the ideal character.

 

The specificity of spin interactions is revealed in the transfer of an ordered orientation from one system of spins to another one and in the spontaneous establishment of a single “weighted-mean” orientation of spins, which are oriented in various directions (including the case of opposite orientations). In view of the directed character of an orientational action and the possibility of the accumulation of the effect (as distinct from the chaotic perturbations), it can be sufficient for the ordering of not only micro- but also macrosystems [11].

 

This interaction is recognized by quantum mechanics, according to which the main role in the establishment of a spin-spin equilibrium is played by some specific (field) interaction of identical particles. This idea agrees with the conception of “A-fields” by R. Utiyama [12] asserting that each conserved independent parameter of a particle ài is asociated with the own material field Ài, which is the carrier of the interparticle interaction corresponding to the given parameter.

 

In practice, the coherent spin state of systems participating in chemical reactions can be attained by means of the use of a generator of spin states created on the basis of a specially organized ensemble of classical spins, where the maximal interaction energy is realized between not only adjacent spins, but also between remote spins. In this case, the system of interacting spins is a distinctive amplifier of small effects from each individual spin.

 

One of the methods of creation of the spin coherent state in engine fuel (EF) can be realized in the following way (Fig. 1).

style='box-sizing: inherit;font-style:inherit;font-weight:inherit;outline: 0px; box-sizing: inherit;font-style:inherit;outline: 0px' class="alignnone size-full wp-image-128 aligncenter" srcset="https://web.archive.org/web/20210517231331im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_133615.png 516w, https://web.archive.org/web/20210517231331im_/http://entron.com.ua/wp-content/uploads/2017/11/2017-11-08_133615-300x112.png 300w" sizes="(max-width: 516px) 100vw, 516px" v:shapes="_x0000_i1056">

1 — generator of spin states (GSS), 2 – resonator of spin states, 3 — chip-translator,  

 4 –fuel tank of a car,  5 – chip-inductor

 

In tank 4, we mounted chip-inductor 5 connected with chip-translator 3 by a quantum-coupling channel, which is formed on the basis of the physics of entangled quantum states states. The chip-translator was positioned in the resonator of spin states 2, which was connected with GSS 1. After the switching-on of GSS 1, the resonator of spin states 2 is excited to the required level. Simultaneously, there occurs the excitation of chip-translator 3, which realizes the translation of a spin excitation onto chip-inductor 5 by virtue of the effect of entangled quantum states. The chip-inductor makes the spin pumping of fuel in tank 4 and transfers it in the continuously supported spin coherent state.

 

The studies of the influence of the spin coherent state of Diesel fuel on the composition of exhaust gases were carried out on a testing stand at the Laboratory of internal-combustion engines of the Poznan Polytechnic Institute. The parameters of a stand engine are given in Table 1.

 

Parameters of the used engine

Table 1

The engine, type

Andoria 4TC90, diesel with a turbo-supercharging

The maximal capacity [kW/KM]

66/90 at 4100 rev/min

The maximal moment [Nm]

195 at 2500 rev/min

Diameter / course of the piston [mm]

90/95

Working volume of the engine [cm3]

2417

Degree of compression

21,1:1

Sequence of ignition

1-3-4-2

Direction of revolutions

Left

The fuel pump

The private soldier

Regulator of revolutions

Mechanical

Cooling of the engine

Flowing

Fuel

Diesel it agrees PN-EN 590:1999

Motor oil

Lotos Diesel API CG-4/SH SAE 15W/40

Climatic parameters of a premise

T = 26,50C, p = 1004 hPa

 

The results of studies of the influence of the spin coherent state of Diesel fuel on the composition of exhaust gases are presented in Table 2.

 

Results of measurements

Table 2

 

Test

No

Engine speed, l/min

Effective power, kW

Torsion moment,

Nm

Fuel consumption

Emissions, mg/m3

 

g/s

 

g/kWh

 

C

 

CxHy,

 

PM,

fuel in equilibrium state

2500

0,27

2,6

182

72

2500

5,18

19,3

0,95

660

3,5

103

40

2500

12,43

47,5

1,33

385

5,4

133

53

2500

24,62

195

2,07

302

7,2

60

26

fuel in coherent state

1b

2500

0,25

0,3

96

34

2b

2500

5,10

19,0

0,94

653

0,9

70

24

3b

2500

12,43

47,5

1,36

393

2,3

94

35

4b

2500

24,62

190

2,16

315

3,3

33

13

percentage altaration*

-7,40

-88,46

-47,25

-52,77

-1,05

-1,06

-74,28

-32,03

-40,00

2,25

2,07

-57,40

-29,32

-33,96

4,34

4,30

-54,16

-45,00

-50,00

 

— C — – soot, CxHy — hydrocarbons, PM- solid particles

— the sign “minus” indicates a decrease of emitted products in per cent

 

By using the data of Table 2, we constructed a plot (Fig. 2) demonstrating a decrease of the contents of black, hydrocarbons, and solid particles in exhaust gases from burned coherent Diesel fuel at various torque moments of an engine as compared with those from noncoherent Diesel fuel.

On the same stand, we carried out the studies of the influence of the spin coherent state of Diesel fuel on the composition of exhaust gases, according to tests ECE R-49 and Euro II. By performing the statistical analysis of the results of this complex of measurements, we constructed the plots presented in Figs. 3 and 4. They show the decrease of the contents of black, hydrocarbons, solid particles in exhaust gases from burned Diesel fuel. As 100%, we took the indices accepted in tests ECE R-49 and Euro II.

As a result of the performed studies, we draw the following conclusions:

1.                     The coherent state of Diesel fuel enhances the efficiency of its combustion, decreases the toxicity of exhaust gases, and increases the environmental safety of Diesel engines.

2.                     The same is true in view of the results of studies by tests ECE R-49 and Euro II.

3.                     The use of coherent Diesel fuel can be recommended for the traffic under urban conditions, since the engines of cars and trucks operate mainly in the idle mode or in the acceleration mode.

4.                     Because the contents of NOx, CO, Ñ, CxHy, and PM in exhaust gases of a Diesel engine operating on coherent fuel are lower than the normative requirements by ECE R-49 and Euro II, we recommend to reject the installation of filters-afterburners on engines for exhaust gases. In this case, we may expect an increase of the power of engines and a decrease of the Diesel fuel consumption.

 

References

 

1.                     Äâèãàòåëè âíóòðåííåãî ñãîðàíèÿ è ýêîëîãèÿ, ðåäàêöèîííàÿ ñòàòüÿ //Äâèãàòåëåñòðîåíèå, 1999, N2, ñ.43-44.

2.                     Ãåðàñèìîâ À.Ò., Ñíèæåíèå âûáðîñîâ âðåäíûõ âåùåñòâ ñ îòðàáîòàííûìè ãàçàìè àâòîìîáèëåé ñ äèçåëüíûìè äâèãàòåëÿìè// êàíä. äèññ. ÑÏ á, 1993, ñ.190.

3.                     Íèêîëàåâ Ë.À., Òóëóïîâ Â.À. Ôèçè÷åñêàÿ õèìèÿ. Ì., Âûñøàÿ øêîëà, 1964.

4.                     Ëåéäëåð Ê. Êèíåòèêà îðãàíè÷åñêèõ ðåàêöèé. Ì., 1966.

5.                     Áó÷à÷åíêî ÀË., Ñàëèõîâ Ê.Ì., Ìîëèí Þ.Í., Ñàãäååâ Ð.Ç. Ìàãíèòíûå è ñïèíîâûå ýôôåêòû â õèìè÷åñêèõ ðåàêöèÿõ. Íîâîñèáèðñê: Íàóêà, 1978.

6.                     Buchachenko A.L., Frankevich E.L. Chemical generation and reception of microvawes. N.Y., 1994.

7.                     Áó÷à÷åíêî ÀË. Õèìèÿ íà ðóáåæå âåêîâ: ñâåðøåíèÿ è ïðîãíîçû // Óñïåõè õèìèè. Ò. 68. Ñ. 85-102.

8.                     Kothe, M. Bechtold, G. Link, E. Ohmes, J. -U. Weidner Chem Phys Lett, 283, 51 (1998).

9.                     Hohmann, D. Lebender, J. Muller, N. Schinor, F. Schneider J.Phys Chem A, 101,9132(1997).

10.                  Jakubith, H. H. Rotermund, W.Engel, A. von Oertzen, G. Ertl. Phys. Rev. Lett, 65, 3013(1990).

11.                  Ýòêèí Â.À. Î ñïåöèôèêå ñïèí- ñïèíîâûõ âçàèìîäåéñòâèé. // Ýëåêòðîííûé æóðíàë “Íàóêà è òåõíèêà”, 2.02. 2002.

12.                  Óòèÿìà Ð. Ê ÷åìó ïðèøëà ôèçèêà. (Îò òåîðèè îòíîñèòåëüíîñòè ê òåîðèè êàëèáðîâî÷íûõ ïîëåé). Ì., Çíàíèå, 1986, 224 ñ.

 

 

 

The Global Resource of Macroscopic Quantum Nonlocality

The Global Resource of Macroscopic Quantum Nonlocality

 Krasnobryzhev1

 

We have shown experimentally that  the  macroscopic  quantum  nonlocality  is objective and can  be  determined  by  classical  methods  such as Nuclear Magnetic resonance spectrometry, the measurement of the absorption of light by water in the ultraviolet range and changes in the differential resistance and the electric  capacitance of  water as functions of the frequency of a current  passing through it, and  the  thermogravimetry  of  changes  in  the  activation  energy  due to the creation of a stable coherent state in a remote macroscopic object.

 

In recent years the achievements of experimental and theoretical studies of quantum nonlocality have transformed themselves into a completely new paradigm of reality. Already today one can assert that those achievements will gradually lead to profound changes in the comprehension of the physical reality.

Macroscopic quantum nonlocality, as a particular type of interaction, is a global intrinsic property of the classical world which arose, according to the cosmological theory of decoherence [1, 2], from a nonlocal source of reality.

This hypothesis has been confirmed by results of physical experiments carried out during the last few years, which convincingly prove the presence of a quantum entanglement in macroscopic systems. This fact allows for the far reaching conclusion that the entanglement of many various degrees of freedom in macroscopic systems has a significant fundamental and philosophical sense by challenging the basic ideas of the nature of the physical reality [3].

It is obvious that the time has come when the objective results of experimental studies help scientists to direct their efforts towards the practical use of a fundamentally new nonlocal resource, by opening a path from fundamental nonlocal reality to classical reality.

 

Entanglement in a macroscopic medium and suppression of decoherence

 

Macroscopic entanglement is based on quantum entanglement and manifests itself as a correlation of internal degrees of freedom without the intervention of local carriers of interaction.

Despite successes achieved in the development of the successive theory of entangled states [4, 5, 6, 7], the necessary condition for its application is the availability of a measuring tool allowing one to identify elements of it’s physical reality. This condition has focused the efforts of theoretical and experimental physicists on applied studies that means on the comprehension of the role of macroscopic entanglement in nature and on the use of this nonlocal resource [8, 9, 10].

Consistency, as a feature of quantum entanglement, has been confirmed by well-known experiments concerning macroscopic entanglement, which show that a system is the integral whole by spin degrees of freedom [11], and that quantum correlations not only determine the behavior of the macroscopic system but turn out stronger than the classical ones [12].

The results of studies presented hereafter are based on the fact that the states of entangled objects are independent of measurements performed on them, which allows one to manipulate the quantum entanglement of remote objects. At the beginning, these objects represent an integral system that is entangled by the internal spin degrees of freedom. After the division of the object into parts and their removal from one another, a certain part of subsystems of their common system belongs equally to these objects. The correlation of their spin degrees of freedom is conserved irrespective of the distance between the separated parts of the system, and the behaviors of spins in these parts are consistent.

The main reason preventing the use of the global resource of macroscopic entanglement is related to the problem of decoherence [13, 14, 15]. In order to solve this problem, the method of suppression of decoherence is being proposed here. It is based on the use of an anisotropic single crystal with oriented nuclei as a nonseparable system, where the behaviors of spin degrees of freedom are consistent.

Let us consider the system of oriented nuclei in an anisotropic single crystal. By Ή, we denote the energy operator of this system. The stationary (eigen-) states ψk  and the energy levels of these stationary states Ek can be found by solving the Schrödinger equation [16].

According to quantum mechanics, the system can be in a state characterized by a linear superposition of stationary states

The measured quantity is the squared modulus of the wave function

This quantity consists of two parts. The first part of the equation characterizes the populations |ck|2 of stationary states ψk in a linear superposition. The second part indicates that the contributions of different stationary states to the observed value interfere with one another and the quantities c*nck (n ¹ k) characterize a coherent state of the quantum system.

The energy of an anisotropic single crystal can be expressed in terms of an analog of the “spin excess” [17]. In particular, we assign the maximum value of energy of the single crystal to the state denoted by |111…1ñ. If the single crystal interacts with a local object, whose energy state is |000…00ñ, and then the energy gradient between them will be at a maximum. In this case, the energy is redistributed between the single crystal with energy Å1 and the local object with energy Å2, so that the total energy Å is invariable [17]. As a result, the energy flow drives the “single crystal – object” system into the superpositional nonseparable state  In this case, decoherence does not occur.

 

Composition and the principle of action of a system of the teleportation of spin states

 

While developing the idea of the creation of the global resource of macroscopic quantum nonlocality, a System of Teleportation of Spin States was constructed. This system allows for the production of a continuously supported coherent state in a remote macroscopic object [18]. Moreover, the attainment of the coherence is represented as the limiting spin saturation of the remote object, which corresponds to its characteristic frequency and is attained due to the resonance exchange by energy between the spin and nuclear systems.

In Fig. 1, we give the scheme of the System of the Teleportation of Spin States (below, we will write the System). The System includes:

1.                     A Generator of Spin States (GSS), which is a unit on the basis of a single crystal with a preferred orientation of nuclear spins.

2.                     A Resonator, which ensures the spin saturation and the long-term conservation of spin coherence.

3.                     A Chip-translator and a chip-inducer, which form a macroscopic singlet couple made of a material with translational symmetry.

4.                     A Remote object of teleportation action.

 

Action principle of the System:

1.                     In the resonator, one places a material analogous to the material of the object of action. For example, if the object of action is water, coal, or steel, one places water, coal, or steel respectively in the resonator.

2.                     A chip-inducer is fixed on the object of action. A chip-translator is constantly present in the resonator.

When the GSS is switched on, spin saturation of the material medium in the resonator happens. The limiting level of saturation corresponds to the spin coherent state of the material medium. Simultaneously spin saturation in the “chip-translator – chip-inducer – object of action” chain occurs. This results in the coupling of the resonator and the object of action, so that the remote object transits in the coherent state. After this procedure, the remote object can be subjected to a target application.

 

In what follows, we describe the following themes:

1.                     NMR spectrometry of macroscopic nonlocality.

2.                     Properties of water in the state of macroscopic nonlocality.

3.                     Activation energy of coal in the state of macroscopic nonlocality.

4.                     Teleportation of properties of vaccines.

 

NMR studies of macroscopic nonlocality

 

The experiment was carried out with the use of a System for the Teleportation of Spin States (Fig. 1) and an NMR-spectrometer. During the experiment, we measured the time of relaxation of the transverse component Ò1 (spin-lattice relaxation). As an object of study, we choose hydrogen-containing samples such as gasoline and Diesel fuel. Prior to the experiment, we had measured the relaxation time of the transverse component Ò1 of the samples in the equilibrium state. Then, in agreement with the scheme shown in Fig. 1, the substance under study was filled in flasks with chip-inducers attached to them. The generator of spin states, a resonator, and a chip-translator were at a distance of 40 km from an NMR-spectrometer. After switching on the GSS, the samples in the flasks were transferred into the coherent state during 12 h. Then a sample of the substance was filled in a test tube and placed in an NMR-spectrometer to measure the time Ò1.

The processing of the results of measurements was made with the software PeakFitÒÌ. The experimental results are presented in Table 1.

 

Table 1| The results of measurements of the relaxation time of the transverse component Ò1

 

Studied samples

the relaxation time, ms

the equilibrium state

the coheren state

T1

T11

T12

 

T1

T11

T12

Diesel fuel

672±72

514±22

1410±81

 

805±12

441±35

999±79

gasoline

2197±33

 

 

 

2946±15

 

 

The experimental results indicate:

1.                     The relaxation time of the transverse component Ò1 of samples in the coherent state is different from that of a sample in the equilibrium state and exceeds the systematic error of measurements.

2.                     The teleportation of spin states at a distance of 40 km is realized.

 

Properties of water in the state of macroscopic nonlocality

 

As is known, an external electric field polarizes a medium, where an additional electric field compensating the external one arises. In other words, if a light beam passes through water, water actively interacts with light by nonlinearly absorbing it. In this case, the maximum absorption is observed in the ultraviolet range. In our studies, we used drinking water, which was transferred into the coherent state with the help of the system of the teleportation of spin states (Fig. 1). The transition time in the coherent state for water was equal to 12 h. The generator of spin states, a resonator, and a chip-translator were at a distance of 10 km from the object of studies.

Characteristics of water: Acid-base balance (ðÍ) = 7.8, Electric conductivity σ = 1020 (μSm), Total dissolved solids (TDS) = 1150 (mg/liter), The oxidation/reduction potential (ORP) = +142 (mV)

We studied the absorption spectra of coherent or noncoherent water in the ultraviolet (UV) range with the help of a spectrophotometer Libra S22 UV/Vis (Biochrom Ltd.) and relative variations of the differential resistance and the electric capacitance of samples of water as functions of the frequency.

 

All measurements were executed relative to the control sample of water at a temperature of 293 K. The results of these studies are presented in Fig. 2.

 

Figure 2 | Influence of the teleportation of spin states on the properties of watera – change in the absorption of UV radiation by water (1 – water in the equilibrium state,  2 – water in the coherent state),  b – relative differential resistance of water R0/Rc versus the frequency of a current passing through water, where R– resistance of water in the equilibrium state, Rc – resistance of water in the coherent state; c –relative variation in the electric capacitance of water versus the frequency, where Ñ– capacitance of water in the equilibrium state, Cc – capacitance of water in the coherent state.

 

Fig. 2a shows that the absorption spectra of coherent water differ significantly from those of noncoherent water. These UV spectral sections of the absorption of water occupy the interval of wavelengths 200 – 240 nm. The absorption in this spectral interval is formed by the optical transitions with participation of oscillations of molecules of water and admixtures. The absorption spectrum, like the dependence of the coefficient of absorption on the light wavelength (the energy of photons), is described by the exponential dependence at the given temperature, i.e. the shape of the absorption spectrum obeys the Urbach rule [19].

In Fig. 2b we show the variation of the differential resistance of samples of noncoherent water relative to that for coherent water (R0/Rc) as a function of the frequency of a current passing through water. As one can see, coherent water manifests a wide dispersion band for R0/Rc in the interval 2.7 – 10.2 Hz. The registered decrease of the differential resistance is analogous to the property of negatronic systems.

In Fig. 2c, we present the variation of the electric capacitance of samples of coherent water relative to that of water in the equilibrium state (Ñc0) as a function of the frequency. Remark the wide dispersion band with a maximum at 100 Hz.

The performed studies indicate that water transits in the coherent state due to the teleportation of spin states. This increases the nonlinear absorption of water in the UV range and causes both the appearance of the negative differential resistance and an increase in the electric capacitance, which can be measured by classical methods.

 

Activation energy of coal in the state of macroscopic nonlocality

 

In our studies, we used brown coal, which was transferred in the coherent state with the help of the System of the teleportation of spin states (Fig. 1). The GSS, a resonator, and a chip-translator were at a distance of 70 km from a laboratory. The duration of the transition in the coherent state for coal was    12 h. The size of coal grains was 1 – 1.2 mm. The content of the organic component was 80.3%, and the hygroscopic humidity was 4.1%.

We studied the variation of the coal activation energy at its transition in the coherent state. The value of activation energy was determined with the help of the “Free Kinetics” model, which allows one to carry out exact calculations for such complicated reaction as combustion.

The model is based on the theory by S. Vyazovkin [20, 21], in which the conversion function f(a) and the activation energy are constants under conditions where some other parameters vary. In calculations within this model, three dynamical curves with different rates of cooling (b) are required.

The determination of the activation energy was performed with the help of a thermogravimeter TGA/SDTA/851of the Mettler Toledo firm.

As a result of the transit of coal into the coherent state, we obtained a decrease of the activation energy by 56.7% relative to that in the equilibrium state (Table 2). This testifies to a decrease of the energy barrier that should be overcome in the case where coal burns in the coherent state.

 

Table 2 | The values of coal activation energy in the equilibrium and coherent states

 

State of coal

 

Activation energy

Decreasing of

activation energy

the equilibrium state

378 kJ/mol

0%

the coheren state

164 kJ/mol

56,6%

 

In order to confirm the correctness of the determination of the activation energy, we carried out the thermogravimetric (TG) analysis which reveals a decrease in the mass of a specimen of burning coal as a function of the temperature increment. The results of this analysis are shown in Table 3.

 

Table 3| Results of the TG analysis

 

The rate of heating,

oC/min

Temperature of full burning out of test of coal, ÎC

Difference

temperatures, OC

 

the equilibrium state

 

the coheren state

5

540

540

0

10

580

540

40

15

630

560

70

 

As is seen in Table 3, coal burns identically in both states at the rate of heating equal to 5oC/min (Ò ~540oC). At the rates of combustion equal to 10oC/min and 15oC/min, we observed a decrease in the burning temperature of coherent coal by 40îÑ and 70îÑ, respectively, relative to that of coal in the equilibrium state. An increase in the coal combustion rate at the lower temperature testifies to a growth of the reactivity of fuel in the coherent state and to its greater chemical activity to oxygen, which is related to a decrease in the activation energy.

 

A system of quantum communication

 

The quantum (teleportation) communication is realized instantly irrespective of the distance between the transmitting and receiving Systems. The main elements of these Systems are a chip-translator (transmitter) and a chip-inductor (receiver), which are quantum-mechanically entangled by spin and are formed from a macroscopic matrix of spin-entangled nuclei.

When the spin state of the nuclei of atoms of the chip-translator is changed, the spin states of the nuclei of atoms of the chip-inductor are also simultaneously changed. In this case, the exchange by spin states (information) between the chip-translator and the chip-inductor occurs instantly without any field carriers and is independent of the distance..

Such a type of communication is considered to be trivial, since the entangled nuclei of atoms of the chip-translator and the chip-inductor have the common wave function.

In Fig. 1, we show the scheme of the experimental System of quantum communication. In this system, we used the universal system of teleportation of spin states similarly to other technologies.

1 – generator of spin states (GSS), 2 – resonator, 3 – chip-translator À,

4 – chip-translator Â, 5 – chip-inductor, 6 – spectral analyzer, 7 – generator.

 

The System of quantum communication includes:

GSS 1, resonator 2, chip-translator À 3, chip-translator  4, which is a dielectric of capacitor Ñ1, chip-inductor 5, which is a dielectric of capacitor Ñ, spectral analyzer 6, whose input is connected with capacitor Ñ2, generator 7 connected with capacitor Ñ1, In this case, chip-translator 3, chip-translator 4,  and chip-inductor 5 are entangled by spin.

As a dielectric material, we used: a) water. b) textolite, c) ceramics.                                                                        

The details of the experiments are as follows:

1.                     The spectral analyzer, whose input is connected with capacitor Ñ2, was positioned at a distance of 10 km from the generator connected with capacitor Ñ1 and from GSS and the resonator.

2.                     In the resonator, we placed a dielectric material (e.g., ceramics) and mounted chip-translator À 3.

3.                     After the switching-on of GSS, the resonator, chip-translators 3 and 4, and chip-inductor 5 were transferred in the coherent state.

4.                     The sequence of the action of the generator on capacitor Ñ1:

 

2.                     a) dielectric material is water – the high-voltage generator is switched-on in 5 sec after the spectral analyzer. The action was high-voltage discrete for 5 sec. The spectra are given in 2.

Fig. 2.

3.                     b) dielectric material is textolite – the high-voltage generator is switched-on in 5 sec after the spectral analyzer. The high-voltage action was of the Morse-code type. The spectra are given in 3.

4.                     a) the dielectric material was ceramics; the generator was switched-on in 5 sec after the spectral analyzer. We used the vocal and musical actions for 5 sec. The spectra are presented in 4.

Fig. 4.

 

 

Macroscopic nonlocality and teleportation of properties of vaccines

 

The principle of action of the System is based on the teleportation of spin spatial configurations (replicas) of protein fragments of vaccines to the organism of an object of vaccination (a percipient) by inducing the appropriate immune response in it. In this case, the body of a percipient is transferred in the coherent state at a characteristic frequency of water, because 70% of the body consists of water.

The teleported information (state) interacts in the body of a percipient with a supermolecular water ensemble in the near-cell “small matrix” containing also glycoproteins in a concentration of        ~10-8Ì. This ensemble determines the functional ability of the “small matrix” to receive and to propagate the information signals coming from the outside to cell receptors. This results in the fabrication of appropriate antibodies by immunocompetent cells.

We then introduced the following changes in the sequence of applications of the System for the teleportation shown in Fig. 1: we poured water in the resonator with a chip-translator and transfered it into the coherent state, then we introduced a single dose of vaccine into the water and obtained a 5×10-Ì solution. After that, we mounted a chip-inducer onto the body of an object of vaccination. The System for the teleportation was positioned at a distance of 10 km from the objects under study. In all cases the duration of the continuous teleportation action was equal to 36 h.

For the teleportation, the following vaccines were used:

— vaccine “Influvac” for the prophylaxis of influenza, which was produced by “Solvay Pharma” (the Netherlands) and contained hemagglutinin and neuraminidase of viral strains À10/99(Í3N2), À20/99 (H1N1), and Â379/99;

— vaccine “Twinrix” for the prophylaxis of hepatitis À or Â, which was produced by “SmithKline Beecham Biologicals S.A.”.

The teleportation was realized onto human organisms (volunteers) and onto laboratory animals (rabbits):

1.                     a) vaccine “Influvac” — onto 5 rabbits,

2.                     b) vaccines “Influvac” and “Twinrix” — onto 5

The results of experiments were estimated by the presence of appropriate antibodies in biological objects and by the rate of formation of the relevant immune response (under normal conditions of vaccination the immune response is realized in 7-10 days).

In Table 4, we present the obtained results of titration of the analyzed samples of blood of the objects of the teleportational vaccination for the presence of specific antibodies.

 

Table 5| Results of titration of blood samples under the teleportational vaccination of organisms

 

Object of influence

 

Quantity of antibodies on an antigene (un / ml)

Vaccine «Influvac»

Vaccine «Twinrix»

H3N2

H1N1

B

HA

HbsAg

C

ÒV

C

ÒV

C

ÒV

C

ÒV

C

ÒV

the rabbits

in 36 hour

in 8 days

in 14 days

 

0

 

1024

8

256

 

0

 

 

 

16

10240

 

0

 

1024

256

256

 

 

 

 

the volunteers

in 36 hour

 

14

 

256

 

0

 

32

 

26

 

512

 

negative*

 

positive

 

0

 

0

C – control indices; TV – indices after the teleportational vaccination.

* — in the immunological practice, the immune response of organism to antigen ÍÀ is determined only in the form negative or positive.

 

The immune response of organisms was realized in 36 h instead of 7-10 days.

The reason for the absence of the immune response to protein fragment HbsAg is not known yet, but the practice of vaccination testifies that the full immunization of human organism occurs in 6 months after 3 injections.

The rapidity of the teleportational vaccination effect can be explained by the participation of the maximum pool of the organism’s lymphocytes in the realization of an immune response and by omitting the process of cloning. The spin replicas which are translated into the vaccination object play the role of a “master-key” intensifying the process of immunization.

 

Conclusions and perspective

 

As a result of these studies, we have established that the macroscopic quantum nonlocality is the objective reality and that the word ”quantum” indicates that the state of a system under study can be described by quantum methods, for example, with the density matrix method.

The main property of the resource of macroscopic quantum nonlocality consists in the fact that the teleportation of spin states onto a remote macroscopic object (located at infinity) creates a continuously supported coherent state in it. As a result, such an object can be used to enhance the efficiency of already available and also of future technologies.

We are convinced that the development of negatronic miniature devices aimed at the realization of teleportational communication at unlimited distances is possible.

The fabrication of highly efficient photochemical generators of hydrogen with the use of coherent water, catalysts and UV radiation in the interval 170-180 nm is promising.

Our study also opens the way for the teleportation of properties of medicinal preparations, including the teleportation of vaccines, which is especially important under conditions of space flight.

As a result of complex experiments executed on some heat and electric power plants we obtained a decrease of the consumption of coherent coal in the production of electric power of 16 % on average with the corresponding decrease in emissions of ÑÎ2 into the atmosphere. In this case, ~ 500,000 tons of coals were transferred into the continuously supported coherent state.

Also the consumption of energy at the recrystallization annealing steel of coherent state was decreased by 36-40%.

 

 

1.                     Joos E., Zeh H. D., Kiefer C., Giulini D., Kupsch J. and Stamatescu I. O. Decoherence and the Appearance of a Classical World in Quantum Theory, (Springer-Verlag 2003).

2.                     Zurek W. H. Decoherence, einselection and the quantum origins of the classical, Rev. Mod. Phys. 75, 715 (2003).

3.                     Quantum Mechanics on the Large Scale, Banff Center, Canada, Peter Wall Institute at UBC. A 5-day conference (April 12–17, 2003) and a 10-day workshop (April 17–27, 2003).

4.                     Calsamiglia J., Hartmann L., Dur W. Spin gases: quantum entanglement driven by classical kinematics // Phys. Rev. Lett. 2005. Vol. 95. — P. 1805021-4.

5.                     Dur W., Briegel H.-J. Stability of macroscopic entanglement under decoherence // Phys. Rev. Lett. 2004. Vol. 92. — P. 1804031–4.

6.                     Hein M., Dur W., Briegel H.-J. Entanglement properties of multipartite entangled states under infl uence of decoherence // Phys. Rev. A. 2005. Vol. 71. — P. 0323501-25.

7.                     Doronin S. I. Multiple quantum spin dynamics of entanglement Rev. A 68, 052306 (2003).

1.                     Chou C. W., de Riedmatten H., Felinto D., Polyakov S. V., van Enk S. J. and Kimble H. J. Measurement-induced entanglement for excitation stored in remote atomic ensembles, Nature 438, 828 (2005);

2.                     Chaneliere T., Matsukevich D. N., Jenkins S. D., Lan S.-Y., Kennedy T. A. B. and Kuzmich A. Storage and retrieval of single photons transmitted between remote quantum memories, Nature 438, 833 (2005);

3.                     Eisaman M. D., Andre A., Massou F., Fleischhauer M., Zibrov A. S. and Lukin M. D. Electromagnetically induced transparency with tunable single-photon pulses, Nature 438, 837 (2005).

11.                  J-W. Pan, D. Bouwmeester, M. Daniell, H. Weinfurter, and A. Zeilinger, Experimental test of quantum nonlocality in three-photon Greenberger-Horne-Zeilinger entanglement, Nature, 403, 515 (2000).

1.                     Ghosh, S., Rosenbaum, T. F., Aeppli, G. & Coppersmith, S. N. Entangled quantum state of magnetic dipoles. Nature 425:48-51 (2003).

13.                  Stodolsky L., in Quantum Coherence Proc. Intern. Conf. on Funda­mental Aspects of Quantum Theory, to Celebrate 30 Years of the Aharonov-Bohm Effect. USA, 1989 (Ed. J.S. Anandan) Singapore: World Scientific, 1990) p. 320.

14.                  Giulini D. et al. Decoherence and the Appearance of a Classical World in Quantum Theory (Berlin: Springer, 1996).

15.                  Ê. Ì. Salikhov. 10 lectures on spin chemistry./ Chemistry and Computational Simulation. Butlerov Communications. 2001. Vol.1. No.4.

1.                     Doronin S.I. Qvantovaja magija. St.Peterburg, 2009, p. 336.

17.                  Buhks On Urbach rule theory for impurity light absorption. 1975 J. Phys. C: Solid State Phys. 8 1601-1606.