Vladimir Timofeevich Grinev
THEORY OF PLASMA CRYSTALLIZATION.
PREFACE The mass
media regularly report on the next major fundamental discovery. Most readers
are already used to such publications and do not take them seriously. Certified
scientists simply remain silent or react to all this with undisguised
irritation. Nevertheless, publications appear and find their readers.
Subconsciously, at the level of intuition, most people believe that sooner or
later a really big discovery will happen, and this expectation of a miracle is
intensively exploited. Fundamental discoveries are not made every day,
therefore, the vast majority of these reports do not correspond to reality, and
professional scientists can understand that it is painful and thankless to
search for mistakes in an endless stream of obviously erroneous fantasies. But
if you discard everything in a row, without bothering to carefully study new
ideas, then the real discovery will surely be rejected, and sooner or later it
will appear. The paradox is that a real
fundamental discovery capable of initiating a firework of fantastic inventions
has long existed and is able to fully satisfy the wildest expectations, but
remains unnoticed. PC-based thermonuclear reactors are
relatively simple, reliable, inexpensive devices, completely unlike modern
installations, operating on a completely different principle, absolutely safe
in operation, not accumulating radioactive waste, providing direct conversion
of nuclear fusion energy into electrical energy and capable of using not only
deuterium and tritium as fuel, but also many other chemical elements.
Introduction The problem
of implementing controlled thermonuclear fusion has been well known for a long
time. The root of the problem is that
the effective cross-section of the nuclear fusion reaction has very small
dimensions. The nuclei of atoms should get closer to (10^- The modern
theory of controlled thermonuclear
fusion (CTF) sees a way out in the banal heating of thermonuclear fuel to a
temperature of tens and hundreds of millions of degrees, and its retention at
such a temperature until most of the nuclei, moving chaotically, collide and
react. In fact, plasma retention is the
organization of a very large number of core-to-core throws, hoping to accidentally
hit exactly the target. It is easy to calculate that only one out of a hundred
million particles will hit the nucleus, even if the accelerated nuclei are
directed exactly at the target atom.
The
guiding star of the CTF is the well-known Lawson condition, which gives a
quantitative ratio between the plasma density and its retention time. Lawson's
condition is both the foundation and the sacred cow, in the modern theory of
CTF
. It is based on the postulate that
particles in plasma move chaotically, and their velocities are distributed
according to Maxwell's law, and if you hold a bunch of particles long enough,
sooner or later, most particles will successfully collide and react. The higher
the particle density, the less time it takes to hold the plasma. Thus, the gas-kinetic properties of
plasma are postulated, and this is the root of all problems and failures with
the implementation of CTF. As
it turned out, at a temperature of tens of millions of degrees, plasma
particles can no longer move chaotically and randomly. Under the influence of their own
magnetic fields, particles gather into jets (into separate beams, streams), and
these jets interact with each other in such a way that focus points
(three-dimensional intersections of these beams) are formed. Crossing the focus
points, the particle beams are compressed (autofocused) and their diameter is
compared with the de Broglie wavelength. As a
result, plasma radically changes its properties. Its density becomes extremely
uneven, and at a low average density, it reaches fantastic values (neutron
density) at the focus points. In whatever
direction a particle moves in such a plasma, it will be pulled into the nearest
point of absolute focus, (whose dimensions are equal to the de Broglie
wavelength for positive particles) will pass it, will be pulled again into the
next closest point of focus, etc. Considering that the de Broglie wavelength
for positive particles (deuterium ions, for example) is comparable to the
radius of nuclear forces, and at each such point there may be several positive
nuclei at once, nuclear fusion reactions take place at these points. These
reactions are not due to random frontal collisions of positive particles in a
high-temperature plasma, as the modern theory of thermonuclear fusion claims,
but due to the ultra-high density of matter at these absolute focus points, and
the tunneling effect. The unintentional
realization of uncontrolled nuclear fusion during heating, a mixture of
deuterium and tritium, to a temperature of several tens of millions of degrees,
led the entire modern theory of plasma and thermonuclear fusion to a hopeless
dead end. Having received a thermonuclear explosion,
with the help of heating thermonuclear fuel, everyone was convinced of the
simplest, but in fact, grossly erroneous mechanism of the thermonuclear fusion
reaction. No one has a shadow of doubt that the
synthesis is due to random collisions of particles in high-temperature plasma,
with their chaotic thermal motion, and as a result - long, exhausting,
unsuccessful and completely hopeless attempts to implement controlled nuclear
fusion by heating and holding thermonuclear fuel.
Back in the thirties, (at the
dawn of the study of plasma) some scientists (for example, physicist
Vlasov) it was pointed out that gas laws
are absolutely not applicable to plasma, because all its particles simultaneously
interact with each other through magnetic and electric fields, therefore, the
movement of particles in a plasma cannot be considered separately from the
field, and the field from the motion. However, self-consistent mathematical
problems are not really solved even now, with the help of powerful computers,
and this, as it has now become clear, absolutely correct technique has been
discarded. The thermonuclear explosions finally discredited the correct idea,
put the seal of absolute truth on the primitive (in many places crudely
manipulated by experimental facts), the gas kinetic theory of C.T.F., and on
the grossly erroneous Lawson condition, and the authors of all this were turned
into celestials from science. Thus, all
progress in this very important and complex field of knowledge was frozen and
slowed down for decades. Plasma
crystallization. The ultra-high temperature only creates conditions for the formation of multiple plasma focus points. As soon as such points are formed in the plasma, its properties change dramatically. This is no longer chaos, but a strictly organized system of streams (beams) of charged particles with many three-dimensional intersections in three-dimensional space. The particles in these flows, then synchronously (all at the same time) slow down, then synchronously accelerate, while creating the most powerful spherical electric fields, and the most powerful magnetic fields. As a result, the entire space occupied by the plasma turns out to be filled with a complex and very harmonious structure of magnetic and electric fields. See (Fig. 3). As a
result, most of the time, positive particles spend outside the electron cluster
and the positive charge is concentrated around the negative cluster, in the
form of a positively charged sphere, where positive particles slow down and
have a minimum velocity. Negative particles, on the contrary, cross the
intersection area at minimum speed and fly through the area of positive spheres
at maximum speed. With a general quasi-neutrality, the
electron clumps tend to be distributed at the maximum distance from each other
and evenly throughout the plasma volume. Similarly, charged refractory dust
particles behave in well-known dust plasma crystals. There, charged and glowing
specks of dust spontaneously line up in ordered structures resembling crystal
lattices of a solid, and these structures are perfectly visible to the naked
eye. However, in full-fledged plasma
crystals (unlike dust crystals), giant electron currents flow between clumps of
negative charges. Currents of tens of thousands of amperes flow from one clot
to another, in the form of a stream of electrons, and form the most powerful
magnetic fields. In general, such a system of currents is mutually balanced,
and does not create a total external magnetic field. But each elementary
current flowing into the clot interacts with the currents flowing from the same
clot. What comes out of this is clearly seen in (Fig. 3). Electron fluxes form a rigid
three-dimensional framework throughout the volume occupied by the crystalline
plasma and turn it into a solid.
The guiding star and the foundation
of the modern theory of U.T.S., is the Lawson condition. According to this
condition, the thermonuclear fuel must be heated to the ignition temperature,
and held for some time until the thermonuclear energy is three times higher
than the energy spent on heating the fuel. This famous
condition assumes that the plasma, heated to the desired temperature, is held
in a hypothetical, sealed vessel. Lawson does not specify how and how to keep
such a plasma. No one knew
about tokamaks and magnetized plasma at that time. The creator of this popular
formula apparently meant that a kind of sealed box would be created, with walls
impervious to this plasma. Apparently, it was assumed that the plasma would
behave like an ordinary gas, i.e. electrons and ions would bounce elastically
off these walls. Suppose there is some hypothetical sphere
with a diameter of Mentally
fill it with a mixture of deuterium and tritium with a density of 10^20 pieces
per m3, heat it to a temperature of 100 million degrees and we will observe for
more than one second (finally, we will fulfill the Lawson condition). Heating
will require very little energy . According to modern theory (according to
the Lawson condition), more energy will be released in such a plasma only after
one second than was spent on its initial heating. Essentially, by heating up the plasma,
we accelerated all its particles by 10 keV and after one second we got the same
amount, i.e. 10 keV for each particle. Now let's see at what price these 10
keV per particle were obtained. The free path length of the particle is
about Even worse is the case with
electrons. Their speed is thirty times more. In the same second, each electron
will pass from wall to wall 60 million times, i.e. 60 million times it must be
slowed down and accelerated again to 10 keV, by our hypothetical sphere, and
then it will receive its 10 keV. Moreover,
6,000 times each particle must dramatically change direction when approaching
another particle, and this is at least a few electron volts for each collision
- radiation losses. A very depressing picture is emerging.
To get 1 watt of thermonuclear power, you need to reflect 60 MW of energy with
a loss of no more than 0.3 watts. It turns out that our sphere should have a
reflection loss coefficient of about one in a hundred million, and this is
without taking into account radiation losses. The value is completely unreal in technical
terms. Moreover, there is a direct
fundamental prohibition, according to the second law of thermodynamics. And any
attempt to create our hypothetical shell with the required reflection
coefficient is a hopeless attempt to make a perpetual motion machine of the
second kind, in the literal sense of these words. As is known from the second principle of
thermodynamics, a complete transition of thermal energy into mechanical (or
electrical) is impossible, it is limited by the ideal efficiency, which depends
on the temperature of the heater and the temperature of the refrigerator,
according to the famous Carnot cycle. In
our case, each electron within a second should be slowed down to zero 60
million times and accelerated again, to the original energy, with losses of no
more than one 60 millionth. That is, the
thermal energy of the electron flow must be converted into the energy of the
electric field, and then back, with the same high efficiency – (0.99999999)
eight nines. However, at our temperature (100 million degrees) and the refrigerator
temperature of 300 degrees, the ideal efficiency is only five nines 0.99999,
instead of the required eight nines 0.99999999, that is, a thousand times less
than Mr. Lawson requires. Consequently, Lawson's Condition has no
physical meaning, because it contradicts the second law of thermodynamics and
is a perpetual motion machine of the second kind. Simply put, it is impossible to keep the
plasma (that is, to keep the energy spent on the initial heating) for a
sufficient time in principle, and any attempts to do this are doomed to
failure. In other words, it is impossible to obtain a positive energy balance
by holding randomly moving charged particles. If the particles are reflected using a
magnetic field, when the particle does not lose kinetic energy at the moment of
reflection from the wall, but is wrapped back by the magnetic field, then 60
million such reversals will be required in one second, and (10 Kev) of energy
will be wasted due to braking radiation. At the same time, the braking radiation
immediately goes beyond the plasma and cannot be absorbed again. Energy losses will always be thousands of
times greater, even Lawson's condition requires, and this conclusion is in
excellent agreement with experimental results for half a century. As a result, we can state with full
confidence a stunning FACT - for more than half a century, humanity has been
struggling to create a perpetual motion machine, in the form of a thermonuclear
reactor. The
international ITER project is completely hopeless and will be a waste of
billions of dollars. Of course, in a modern tokamak, particles do
not bounce off the walls, but move in spirals in a magnetic field. However,
even in this case, the losses will always be greater than the energy output,
since there is no precise pointing of the particles at each other, and
therefore the number of unsuccessful attempts to get the nucleus into the
nucleus is too large. There is not and
cannot be a device capable of accelerating an electron 60 million times to
10,000 electron volts with an efficiency of nine nines. Controlled nuclear fusion with a positive
energy output can be realized only by artificially organizing, with the help of
super-powerful permanent electron beams crossed in space, just one point of
absolute plasma focus, while taking care of the energy recovery of electron
beams. THE
IGNITION TEMPERATURE OF A THERMONUCLEAR EXPLOSION . It is well
known that a mixture of deuterium and tritium has an ignition temperature in
the region of 40 million degrees, and deuterium 100 million, which corresponds
to 4 keV and 10 keV of the average energy of thermal motion of particles. At
the same time, the energy required to overcome the potential barrier, when the
nuclei approach to the distance of the nuclear forces, is in the region of 400
keV, i.e. 100 times more. 1) It is
determined that the plasma obeys gas laws and the Maxwell law of particle
velocity distribution is adopted; 2) The number of particles with a velocity
greater than the average is determined - 20% is obtained (the Maxwell tail is
clearly too short); 3) The probability of a tunnel transition is
calculated for particles approaching at an average speed - it turns out that
one of several tens of thousands of particles tunnels. Well, then
a logical error begins, or a fraud!!! 4) For example, a plasma of
Newsreel analysis of the thermonuclear explosion H BOMB On the documentary video of the thermonuclear explosion "HBOMB", the plasma crystal has been flaunting for more than a dozen years. The paradox is that this is a direct experimental confirmation of the new plasma theory, which reveals the most fantastic technologies vital to all mankind, constantly flashes on TV screens around the world, but remains unnoticed and misunderstood. (Fig. 1.) shows
several frames from this popular video, with an interval of about one second. It is well known that the duration of the glow
in the epicenter of a thermonuclear explosion lasts several seconds (up to 20
seconds). For the same few seconds, a powerful stream of neutron radiation
(penetrating radiation) comes from the epicenter of a thermonuclear explosion. At
the same time, the greater the power of the explosion, the longer the glow
lasts and the longer the neutron flux takes. All this clearly indicates that
intensive nuclear fusion is going on all this time, but not microseconds, as
the modern theory claims. There is a gigantic (millions of times) discrepancy
between theories and experiment. Further, it is even more interesting – for all
8 seconds (for an explosion, this is a gigantic time), the diameter of the
luminous hemisphere increased by no more than (20%), and it is clear that the
clear boundary of this hemisphere is not a shock wave. What kind of force keeps the incandescent
plasma so reliably and steadily within the strictly delineated boundaries of
the hemisphere, modern theory, not that it can explain, cannot hint!!! Moreover, the above frames show very clearly
that the internal structure of the plasma hemisphere has a highly uneven
structure, which is not at all like a bubble uniformly filled with incandescent
gas. Judging by the glow, the release of thermonuclear energy is also very
uneven. There are
bright spots, and there are vast darkened areas. It is easy to understand that
nuclear fusion takes place in these luminous points, and this one hundred
percent coincides with the new theory. Even more
surprising is the fact that the internal structure of the plasma hemisphere,
for all 8 seconds, does not change at all, and the question arises that can
immediately send the gas–kinetic theory of plasma to the landfill - if plasma
is at least a little gas, then why is there no hint of pressure and density
equalization during all 8 seconds. Where is the Maxwellian velocity
distribution, where is statistical physics, and other gas-kinetic and
hydrodynamic models. What is visible in these frames is a strictly
ordered system of charged particle flows that interacts with its own magnetic
and electric fields. This is the same self-consistent mathematical problem that
70 years ago they could not solve and now they cannot, but the logic of this
process is clear. As is known, during an atomic explosion, the heating of a thermonuclear charge (T1) is due to X-ray radiation and, first of all, the electrons are heated intensively. (See Fig. 2)
At the
first moment (T2), electrons heated to a gigantic temperature are held in this
area by an electrostatic field from heavy and slow positive ions, which can not
keep up with them, and as an anchor for some time they keep a swarm of light
and heated electrons from scattering. A ball
capacitor is formed for a short time. Each
electron manages to make thousands of attempts to leave the clot of heavy ions,
but each time it falls back, under the influence of an electrostatic field. As
long as the electrons fly out evenly and return back evenly, there are no
magnetic fields. However, such a situation is completely unstable and the
slightest fluctuation will lead to a very rapid and avalanche-like separation
of the electron flow into outgoing and incoming jets. Instability begins its
creative work. Incoming and outgoing flows form
closed trajectories of electrons, twisted into a dense tangle, that is, a
constant current is formed flowing along a closed trajectory. This trajectory
is closed to itself, but twisted into a chaotic and dense tangle. Over time and
very quickly, this current increases, due to all the new electrons that enter
synchronous trajectories. It is at this moment that crystallization takes
place, and a powerful electromagnetic pulse is formed. Part of the plasma
energy goes to the formation of the most powerful magnetic fields, and the
rapid increase in the magnetic field induces electromagnetic waves
(electromagnetic pulse). The fact
that this structure is not strictly symmetrical is explained by the fact that
even at the beginning of formation, the electron flows were distorted by
external random factors: contact with the elements of the charge structure,
with the earth's surface, with a metal truss, etc. However, once formed, they
already tend to retain their original shape. After the electronic component is
trapped in its own magnetic trap, the plasma acquires all the signs of a solid
body and holds itself. The most powerful streams of electrons, twisted into a
tight ball, with numerous points of mutual intersection, serve as a rigid
framework, and reliably preserve the shape of the plasma that was formed at the
first moment. After a while, the ions will fill the entire
volume occupied by the electronic component, and even try to go beyond it
(T4). All this happens at the first
moment and very quickly, then the events proceed slowly and calmly. The ionic
component weakly interacts with the magnetic field, since the ions are much
heavier and move at lower speeds. If you look at the above frames again, you
will notice that the luminous hemisphere has a very sharp and clear outer
surface. This surface is formed by an ionic component. At high speed, positive
ions try to jump out of the luminous hemisphere, but are slowed down by an
electric field, slow down and return back. It is the positive particles that
come into contact with the atmosphere and with the surface of the earth, but at
the moment of contact with the external environment their velocity is close to
zero, that is, they cannot significantly warm up those objects that are in
direct contact with the surface of the glowing ball. Simply put, the surface of
the luminous hemisphere is cold. The
tangle of electronic currents is surrounded on all sides by a layer of thermal
insulation made of ions and does not contact the outside world at all, and the
ions come into contact on the fly – cooled down. By the way, ball lightning also interacts with
the surrounding world in the same way, its surface temperature is close to
absolute zero, that is, only ions slowed down to zero speed (cooled down on the
fly) interact with the atmosphere, but if you pierce this layer of ion
insulation, then a ball lightning explosion will occur. The fact that energy escapes from the epicenter
of a thermonuclear explosion mainly due to electromagnetic radiation (energy
flashing) has long been a well-known experimental fact, but why a clot heated
to a gigantic temperature of matter has such a calm and clear boundary with the
atmosphere, and even for 8 seconds, can only be explained by the theory of
crystalline plasma. The effect
of a double flash in thermonuclear explosions fits very well into the new
theory. The first
flash is heating up due to a chain reaction of fission. Immediately begins the
formation of an electronic tangle and the generation of an electromagnetic
pulse. The end of the electromagnetic pulse means that the transients are
completed, that is, the electron current has reached its maximum and the plasma
crystal is fully formed. At this moment, the glow almost stops, but after a
while (after about one microsecond) neutron density points are formed, a
nuclear fusion reaction begins in them, and the glow increases dramatically. The
glow lasts until most of the thermonuclear fuel captured by the general round
dance burns out, even at the time of the formation of electronic flows.
Formation
of neutron density points. After the
crystallization is completed, the plasma begins the process of forming points
of extremely high density of matter. Very simple initial conditions are needed
for their formation. 1) there
should be no frequent paired collisions between particles in the plasma. 2) There
should be powerful counter electron flows in the plasma. The radius
of each cell is always equal to the Debye radius for a given plasma, it also
depends on the density and energy of particles (electrons). Each cell contains 4 electron beams and the
same number come out of it, but these outgoing beams immediately become part of
neighboring cells and so on. It is clearly seen that these elementary currents, 4 crossed
and combined common currents are formed, which do not create a total external
magnetic field. However, there is a magnetic field in each cell. The entire
volume occupied by this plasma is embroidered with a very harmonious and very
strong magnetic field. If we consider that at a plasma density (1.0 E + 20
pieces per cubic meter) and a temperature of 100 million degrees, the cell
diameter (Debye radius) is about 100 microns, and the current flowing into it
is 10,000 amperes, then the magnetic field strength at the cell surface reaches
a very decent value (1.0E +8) a/ m, and as it approaches the center, it grows
rapidly - inversely proportional to the distance to this center and the
diameter of the beam. Moreover,
this magnetic field has a maximum intensity on the surface of each elementary
current, but decreases to zero in the center of the same elementary current. As
a result, a very harmonious system of hollow tubes made of a magnetic field is
obtained, which expand at the cell boundary and narrow to an infinitesimal
diameter as they approach the center of the cell. Unfortunately, a two-dimensional drawing
does not allow you to fully show the beauty of this magnetic field pattern. And
the fact that this whole complex system is formed spontaneously is amazing. At the tips
of magnetic tubes, the magnetic field strength reaches gigantic, intracellular
values, and naturally it cannot reach the maximum instantly - induction
interferes. This process lasts approximately one millionth of a second. This is
the delay time between the heating of the thermonuclear fuel and the start of
the synthesis reaction. Such a delay was
noticed even during the first tests. It is very important to note that electrons
cannot pass through the center of the cell without changing directions, and if
you follow the trajectory of an individual electron, a random, broken
trajectory will come out, the break points of which will coincide with the
centers of the cells. This is due to the
fact that an electron can come arbitrarily close to the center of the cell, but
it cannot overcome this center and continue moving in a straight line. Moving along the incoming magnetic tube, the
electron flies up to the center, slows down in the electrostatic field and is
thrown back by the same field. But he can no longer move in the opposite
direction through the same magnetic tube. The magnetic field of the incoming
tube will immediately push it out and it will inevitably be trapped in one of
the three output tubes (there are two such tubes in the flat drawing). As a
result, a certain paradox comes out - electrons in a crystalline plasma move
along a broken and random trajectory, bouncing elastically from the centers of
cells, but the electron currents formed by them have a strictly ordered, stable
structure. The rebound
of an electron from the center of the cell, only at first glance, is random, in
fact it is a very subtle and precise system of homing the incoming flow of
electrons to the absolute center of the cell.
This system
works as follows. See (Fig. 4) If the
tip of the incoming magnetic tube is directed exactly to the center, then all
the electrons that go through this tube will be divided into three equal parts
when bouncing and go through the three outgoing tubes. But if the tip is shifted from the center,
then the rebound of electrons will no longer be divided into equal parts. There
will be a redistribution in the outgoing flows and the magnetic field will
increase from the side where the axis of the incoming flow is shifted. The
resulting distortion in the magnetic field will correct the error and direct
the incoming flow exactly to the target. . M10B1 and
M10B2 show the case when several beams are directed to one point from all
sides. The scattering charge, in this case, is formed spontaneously from
delayed electrons. Each beam, under the influence of the above-described
regularity, tends to correct the direction of its movement so as to move more
accurately to the center of the system, and this leads to spontaneous centering
of the formed volumetric negative charge. At the first moment of time T1 (See
Fig. 6), negative volume charges from inhibited electrons form and hang
motionless in the cells. The figure shows one of the cells at different points
in time. At time (T1), a spherical volume charge appears in the cell (the first
stage of electron compression). Its
electric potential is approximately equal to the initial kinetic energy of the
electrons, and this equality is formed by means of a magnetic field that
counteracts the forces of electrostatic repulsion in the beam, and all the time
tends to direct (tuck) the kinetic energy vector of each electron to meet the
electrostatic braking force, and thus forces the electrons to completely expend
their kinetic energy. The greater the current, the stronger this effect (MHD
braking). (See Figure
5) However, it is necessary to pay special
attention to the fact that in this volumetric charge there are seals in those
places where electron flows come into contact with it. These seals are formed
by a magnetic field. Two forces act simultaneously on the electrons flying to
the center of the cell. One is magnetic, which presses the flow of electrons to
its own axis, the other is electric, which slows down the entire flow. At the
first stage, when the electrons have a maximum velocity, the magnetic force
acts as a collecting lens. At the second stage, when the electron velocity is
minimal, the main role is played by the force of electrostatic repulsion and a
scattering lens is formed. As a result, it turns out that the volume charge
formed by these flows has electrostatic scattering lenses evenly located on the
surface, located strictly in the center of the magnetic tubes. For electrons,
these are scattering lenses, but for ions, these are electrostatic collecting
lenses.
Of course, ions react to a negative volume charge. From all sides, positive particles with acceleration begin to move towards the negative charge, which hangs motionless in the center of the cell. Having reached it, they gain kinetic energy equal to its potential, and therefore energy equal to the initial energy of electrons. At the maximum speed, the ions pass through the electrostatic collecting lenses and continue moving towards the center already by inertia and are intensively inhibited by their own volumetric charge.. After passing about half of the remaining distance to the center, the moment of time (T2), the ions will almost completely lose speed and form a volumetric positive charge there (the first stage of ion compression). Its potential will be equal to, their (ions)the maximum kinetic energy, and therefore will be equal to both the maximum electron energy and the potential of the first negative volume charge. At the same time, the resulting positive electric charge will be much smaller than the first negative volumetric charge, and therefore will not be able to compensate for it. Thus, at time T2, a ball capacitor is formed in the cell, charged to a voltage equal to the kinetic energy of the part expressed in electron volts. Ions move much slower than electrons, and therefore, as soon as the first positive charge appears, the electrons immediately change their trajectories, and a system (T3) is formed. Now the electrons slow down on the first negative sphere, but they do not bounce off it, but with acceleration they continue to move even closer to the center of the cell. At maximum speed, they enter the first positive sphere, pass another half of the remaining path to the center, and form a second negative volumetric charge (the second stage of electron compression). In shape, it is an exact copy of the first, and has a similar set of electrostatic lenses, its potential is the same, but the radius is 4 times smaller than the radius of the first negative, and the electric field strength on its surface is 4 times higher. At the same 4 times, it has a high intensity and a magnetic field surrounding this new charge. It is very important that with the formation of the second negative charge, a new, even smaller, but much more intense structure of magnetic fields was formed. The magnetic tubes seemed to stretch out to the center and sharpened. The electrons still bounce off the center of the cell, but they approach this center by a much smaller (4 times) distance. At the moment of time (T4), a second positive volumetric charge is formed (the second stage of ion compression). Its size is even smaller than the new ball of electrons, and the electric field strength is doubled again. Then all this is repeated many times and spontaneously. Step by step, the streams of charged particles approach the absolute center of the cell. With each step, hollow magnetic tubes are sharpened and lengthened. With each step, new, smaller, volumetric charges are formed. The intensity of magnetic and electric fields is rapidly increasing. Each time, a new, even shorter-focus set of electrostatic lenses is formed, located even closer to the absolute center. At the same time, a set of scattering lenses alternates with a set of collecting lenses. Eventually, in the center of the crystal plasma cell, a focus point is formed, the size of an atomic nucleus, and through it pass: an electron current of tens of thousands of amperes, and an ion current of hundreds of amperes, simultaneously. Accordingly, at each moment of time, there are several ions and several electrons at this point. How they will behave there, no one can say. No accelerator can collide several ions at once, and even mixed with electrons. This requires fundamentally different devices.
Spontaneous
alignment of the elementary current system. The flows of electrons and ions entering the
crystal plasma cell do not have an initial exact direction but a neutron point.
Flying into the next cell of the crystalline plasma, each particle carries with
it a whole set of all possible errors, in vector, and in speed. Particle flows
have an even larger set of errors. For example, the flow of electrons going to
the center may have a non–zero total moment of rotation, and if this moment is
not removed, then when the flow narrows, its promotion will occur. In other words, electrons moving along a
magnetic tube can simultaneously rotate around the central axis of this
tube.
However, when studying this problem, it turned
out that there is a mechanism for equalizing the moment of rotation between
electrons moving along a common magnetic tube, that is, the moments of rotation
of all electrons in one tube are spontaneously aligned, and the total total
moment of rotation is transmitted through a common magnetic field to
neighboring outgoing electron flows. In this case, the exchange of the total
momentum of rotation occurs constantly, as the electron flow approaches the
point of absolute focus.
When
studying many other errors, a very important general pattern emerged – all
possible errors and errors carried by particles going to the center of the cell
are given over to particles coming out of the same absolute center. Figuratively speaking, the particles moving
towards the center, as it were, find out from the oncoming parts where this
center is, and correct (clarify) their trajectory. This dialogue is especially
intense in the area of electrostatic lenses located at the same compression
stage (in a common orbit). Figure 8 shows the structure of the distribution of electrostatic bulk charges in a crystal plasma cell. Positive volumetric charges are highlighted in red, and negative ones in blue. The figure clearly shows that in the first orbit (at an equal distance from the center), 8 electron bunches are evenly spaced - 4 are formed by incoming electron flows, 4 more are formed by outgoing ones. In the flat drawing, only 6 blobs are visible (3 incoming and 3 outgoing). These clumps consist of moving electrons, but they hang motionless in space and interact with each other as solid bodies, that is, they spontaneously tend to be evenly distributed over their sphere (along orbit No. 1). One of the mechanisms of automatic beam reduction, and works by using the tendency of the charge to fill the sphere evenly. If, for example, one of the incoming streams is directed slightly past the center, then the clot that it forms will shift slightly along sphere No. 1, and will shift slightly the near outgoing beam to which it is mistakenly displaced. As a result of this interaction, the incoming flow will go to the center more accurately, and the outgoing flow will deviate in the other direction and forget the exact direction to the center. The error energy will be exchanged. See (Fig. 9).
In the end, all charges will react to a slight shift from the center of the flow No. 2, their displacement will occur, a small general distortion of their total electric field will occur. This precos and will direct flow No. 2 to the common center. The clumps of electrons will remain in this slightly skewed state while a stream of electrons with an error vector will fly into this cell. As we approach the center, many more similar acts of direction refinement will occur (at each compression cycle). The closer to the center this exchange takes place, the more precisely the direction is determined. The multi-step nature of the process ensures fantastic accuracy of this mechanism. Figure 10
shows two more mechanisms for transmitting errors from incoming flows to
outgoing ones. In the first case, current #2 has a current greater than the
others. Then, at the moment of stopping in the first orbit, its excess volume
charge will transfer to the nearest outgoing streams. This additional current
will not pass to the center, but will be thrown back, along with the outgoing
flows, and will be divided into three parts.
Outgoing flows (in the flat picture, these are the first and third) will
take these surpluses and enter neighboring cells with them. There they will be
divided again, in the same way (into three parts) between other threads and so
on. Thus, the excess current will be divided into an infinite number of parts
and will be evenly distributed throughout all cells of the crystalline
plasma. How the total torque of rotation
is transmitted is clearly visible and without explanation.
Spherical symmetry and the cone of equilibrium. Option (a)
– electron flows evenly fill the ball, and there is no gap between the leading
and outgoing flows. In this case, the electrostatic field has a central
symmetry and an electric force directed strictly along the radius acts on each
electron. At the same time, the
electrons are affected by the force from their own magnetic field. Each
electron stream creates its own magnetic field, which tends to press its own
electrons to the centerline. On the axial lines of the flows, the magnetic
field is zero, but as it approaches the periphery of the flow, it increases and
reaches a maximum on the surface. At the same time, the intensity of the
magnetic fields synchronously and rapidly increases as they approach the
center, that is, as the flows narrow. It is clear that in this variant, the
magnetic forces remain uncompensated, and under their action, the flows will
narrow. It is important to note the fact that the farther the electron is from
the centerline of the beam, the stronger the magnetic field, and the steeper
its trajectory will bend, and this is the main law of the collecting lens.
Fig. (11b)
shows a variant when the solid angle of the electron beams is selected so that
the magnetic compression forces are balanced by a transverse electrostatic
force. In this case, only the braking force for incoming beams and the
acceleration force for outgoing beams will act on the electrons. It is
important to note that the transverse electrostatic force will be zero on the
axial lines, will increase to the surface of the beams and as it approaches the
center, that is, its shape completely coincides with the shape of the forces
from the magnetic field. With the right solid angle of the flows, the magnetic
forces are evenly compensated throughout the entire volume of the beams. In a
real situation, converging electron beams search for this equilibrium angle
spontaneously. If this angle becomes larger, then magnetic forces squeeze it,
but if it is smaller, then electrostatic forces inflate the particle
beam . Thus, the
converging flows are automatically guided to the common center and their solid
angle of narrowing is automatically selected. If we consider the current
structure of the fields from the point of view of a single moving charged
particle, then this is a system of collecting and scattering lenses tuned to a
common center. (See Fig. 8) The
trajectories of ions are shown in red. There are a
lot of such automatic self-adjusting systems in plasma crystals, and there are
very complex ones. For example, there is a system operating on the braking
radiation of particles, when a charged particle that has violated the general
order, resets the error energy in the form of braking radiation, thanks to this
it returns to the general system and ceases to emit. There is no way to study
all these systems in detail and quickly. They are also infinitely diverse and
complex, like plasma instability. However,
all these systems solve one single problem - they ensure that all charged
particles fall into the common absolute center of the cell, with an accuracy
the size of an atomic nucleus. All of
them are formed spontaneously, do not require any external adjustment and
adjustment. In order for them to appear and work, it is only necessary to
create the simplest initial conditions – to organize powerful counter
electronic flows in the plasma. Therefore, there is no need to describe in
detail and prove how all these complex systems of auto-guidance and autofocus
are formed and work. Firstly, it is simply impossible, and secondly, it is not
necessary. There is a great deal of
indirect and direct evidence that neutron density points exist. What initial
conditions are needed is now known for sure, and they can be organized in
laboratory conditions.
Conditions for the formation of a neutron density point. All these
conditions can be formed by simply heating the substance to a critical
temperature. Then converging (counter) electron flows and all additional
conditions will form spontaneously and inevitably. This principle is
implemented in thermonuclear explosions. However,
all the necessary conditions can be organized artificially. For example, it is
possible not to bring the temperature to critical, but to organize all
third-party compression (implosion) of the thermonuclear charge and neutron
density points will form at a much lower temperature. This principle is also
implemented in thermonuclear explosions. It is possible to bombard a
low-temperature plasma with a radially converging flow of electrons. This
option is implemented in "Plasma Focus" installations. The case when
a low-temperature plasma is fired by an electron stream of very high power and
neutron dots are formed due to this has a lot of practically implemented
examples: 1) Rosary
lightning – an electron beam formed at the moment of the main current breakage
passes through a positive thunderstorm cloud and forms a chain of neutron dots
(rosaries). 2) In Urutskoev's experiments
http://model.exponenta.ru/transmutation/0007.htm at the moment after melting the wire and
breaking the current, powerful electron flows are formed going through low-temperature plasma (foil
melting zone). collapsing bubbles form electron
flows going to the common center. There are
at least two known cases when neutron dots are formed in the crystal lattice of
a solid body: This is a well-known experiment with neutron radiation during the
electrolysis of heavy water, and experiments on the Proton 21 installation
http://www.proton21.com.ua/about.html
The
mechanism of transfer of nuclear fusion energy to electrons. Nuclear
fusion reactions take place in the center of an electrically neutral bunch of
electrons and ions of fantastic density. The energy of nuclear fusion is
released in the form of kinetic energy of neutrons and positively charged
nuclei. However, the density of particles surrounding the reaction zone is
prohibitively high (neutron density), and all particles move there along
strictly defined trajectories (super fluidity and super conductivity). Therefore,
any charged particle that tries to leave the reaction zone, along an
unauthorized trajectory and at an unresolved speed, will experience the full
power of the response from the ordered system of particles surrounding the
reaction zone, and will be intensively inhibited, transferring its kinetic
energy to the entire dance of particles. Yes, neutral neutrons, leaving the
reaction zone, will experience many collisions with ions, and will lose most of
the kinetic energy. A clot of particles in this case will play the role of a
moderator. Given that the strand in the system is supported by electrons, it is
the electronic component that will absorb the excess energy. The mechanism of
capturing excess energy by electrons is as follows: Electrons and ions enter
the reaction zone and exit it with equal energy. However, with equal energy,
electrons have about the speed of light, and ions have a speed much less. Consequently,
to leave the reaction zone and not violate its quasi-neutrality, and electrons
and ions have the right to enter at the same speed as they entered. Any attempt
by the ionic component to leave the reaction zone at an increased rate will
lead to the formation of an excess of electrons at this point. The electric
field formed in this case will begin to intensively push out electrons and slow
down the departing ions. However, the speed of the outgoing electrons is
already about light, and no matter how hard the outgoing heated and heavy ions
try to pull the electrons with them, their rate of exit from the reaction zone
can no longer increase (gaining energy, the electrons only get heavier), but
the ions themselves are intensively inhibited, that is, they lose both speed
and energy. Thus, any release of energy at the point of neutron density will
lead to the appearance of an excessive negative charge, which will slow down
the departure of the positive parts and weigh down the outgoing relativistic
electrons. Consequently, the energy from the positive component will be
transferred to the electrons. It is this
relativistic mechanism that makes it possible to create a reactor with a direct
conversion of nuclear fusion energy into electrical energy.
PLASMA FOCUS EFFECT Isn't the density too high for randomly
combined beams, without any adjustment and alignment of the shape of the
electrodes? All attempts to get something like this
forcibly, firing micro-targets from all sides with laser beams, were
unsuccessful. At the same time, the firing system of this target was specially
designed and tuned for a long time, and here, without any preparation,
adjustment, adjustment, only due to the randomly and roughly guessed shape of
the electrodes - on the first attempt – a powerful and stable nuclear
reaction. Any arguments about
gas-kinetic collisions of plasma flows are unconvincing. At this temperature,
the oncoming streams of particles will not even notice each other. The free
path length of their particles is so great. Only spontaneous formation of
information and autofocus systems can explain "Plasma focus". Hence
"Plasma focus", direct experimental confirmation of spontaneous
autofocus of converging streams of charged particles.
EXPLANATION
OF THE PLASMA FOCUS It is thanks to the spherical symmetry that the radially converging flow, under the influence of a magnetic field, is flattened (thinned), and the outgoing electrons are clamped into two beams. It can be noted that this is a well-known mechanism of plasma instability of the "overstretch" type, when an accidental narrowing of the plasma cord leads to an increase in the magnetic field in the same place and to a further narrowing of the cord diameter to a current break. In the
above example, as the radially converging flow approaches the center and
flattens, the magnetic field also increases, but the electrons, in this case,
are intensively inhibited by their own electrostatic field and, at a certain
moment, when their velocity decreases to a minimum, the force of electrostatic
repulsion will exceed the force of magnetic compression. Then, under the
influence of an electrostatic field, the electrons scatter in all directions
and accelerate again. But, as their speed increases, the magnetic force that
collects them into bundles also increases. In whatever direction the electron
tries to escape from the central point, the magnetic field will direct it into
one of the outgoing beams and will not allow it to move towards the converging
flow. In the case
under consideration, electrons are inhibited and transfer their kinetic energy
to an electric field, and positive particles accelerate, taking energy from the
same field and energy transfer occurs without direct contact between the
particles. Stationary
electrostatic waves arise by themselves in the focus area. Electrostatic
oscillations in plasma have been known for a long time, but the described
spherical system is something unique and unknown until now. Its peculiarity is
that electric fields are formed, hanging motionless in space. There can be
nothing like this in any other medium except plasma. It is very difficult to
detect such a structure experimentally, since it does not create external
electric and magnetic fields. Particles with an energy greater than the average
cross it unhindered, and its characteristic dimensions range from millimeters
to fractions of a micron. EFFICIENCY
OF THE PLASMA FOCUS As is
known, installations based on the principle of "Plasma Focus" provide
a very intense nuclear reaction (up to 100 MW per pulse), but do not give a
positive energy balance, and modern theory explains this by the fact that the
Lawson condition is not fulfilled. But this condition itself is an annoying
misunderstanding, and the real reason is that in order to form an absolute
focus point, a converging flow of electrons with a current of up to 10,000
amperes and with an energy of tens and hundreds of keV is needed, and this is a
power of thousands of megawatts. With equal energy, the velocity of positive
ions is one hundred times less than the velocity of electrons, therefore, the
ion current through the focus point is one hundred times less than the electron
current through the same point. In addition, not every ion that passes the
focus point will react, but about one in ten. As a result, with an electron
current of 10,000 amperes and a power of several thousand megawatts expended,
the nuclear reaction power at this point is only 100 megawatts, i.e. much less
than it is expended. Simply put, it turns out that for one act of fusion of two
nuclei, it is necessary to accelerate several thousand electrons to an energy
of tens of keV and, therefore, it is necessary to expend more energy than is
obtained as a result of the synthesis of the same two nuclei. There are
only two ways to resolve this contradiction: There are
currently no such accelerators, but the principle of their implementation has
already been found, reliably calculated and their feasibility is beyond doubt
(see M6B5). The cartoon shows a simplified diagram of an electron beam
flywheel. This principle is based on the spherical symmetry of the
accelerator-anti–accelerator system and the general, complementary structure of
magnetic and electric fields, accelerating and braking systems. This allows the
energy taken during deceleration of electron beams leaving the plasma focus to
be immediately transferred to accelerated beams and thus achieve an
exceptionally high recovery efficiency. The flow of energy goes directly
through the general electrostatic field, in which the particles entering the
reaction zone are accelerated, and the particles leaving this zone are slowed
down.
BALL
LIGHTNING
NEUTRON
RADIATION DURING HEAVY WATER ELECTROLYSIS
TRANSMUTATION
OF CHEMICAL ELEMENTS IN ELECTRICAL DISCHARGES
Epilogue Author: Grinev V.T. 12.09.2006
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