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"THINKING OUT LOUD"
SCIENTIFIC ROMAN ON THE BASIS OF SCIENTIFIC THEORY
UNIVERSAL, NEUTRONIC PHYSICS AND NEUTRON CHEMISTRY
Valeriy Fedorovich Andrus
" Our task is to develop means of obtaining energy from stocks that are eternal and inexhaustible, to develop methods that do not use consumption and consumption of any" material "carriers. Now we are absolutely sure that the realization of this idea is not far off.: The opportunities for development This concept consists precisely in the fact that to use for the work of engines in any point of the planet the pure energy of the surrounding space ... "
(Tesla, 1897)
 To get started, download the conversion table for chemical elements
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PLASTICITY AND BRITICALITY OF BI AND Sb FROM THE POSITION OF NEUTRON PHYSICS
The following anomaly - Antimony and Bismuth do not possess a high plasticity and ductility characteristic of metals, that is, they are fragile.
Antimony Sb, silver-white. Metal, ρ = 6.684 g / cm 3 , m.p. = 630.5 ° C.
Bismuth Bi, silver-white. Metal, ρ = 9.8 g / cm 3 , m.p. = 271.4 & lt; 0 & gt; C.
In the powder state, both metals are gray, that is, vertically the needles are contracted and superconductivity conditions for light are created. Antimony in relation to Iron and Bismuth in relation to Osmium have lower material densities and melting temperatures, although they have higher order numbers in the element table, i.e. Longer needles.
The usual forms of these elements are characterized by the same layered structure of metals, that is, we have a sedimentary metal bond.
Antimony is an important part of some responsible alloys: typographical font, alloys for bearings, etc. The addition of 1% Sb to the Lead greatly increases its hardness, which is of great importance for the production of lead pipes.
The volume of Bismuth melts noticeably decreases, i.e. He (like water) behaves abnormally in this respect.
Telluride Bismuth (mp = 580 ° C) is used in some thermoelectric devices. Its crystals have a layered structure and exhibit sharply different electrical conductivities in directions parallel and perpendicular to the layers. With increasing pressure, their melting point first increases (to 610 ° C at 15,000 tons), and then decreases (to 535 ° C at 50,000 tons).
We represent the crystal lattices of Antimony and Bismuth, based on the available data. Docking elements occurs in them and as in Carbon, i.e. Vertical axes retain their position when docking.
The application of needles does not go along one another, but transversely, i.e. Rhombically. This suggests that the ends of the needles, as a minimum, have an alternating magnetic field (packets of fives rotate in opposite directions). Vertical needles have a metallic bond with longitudinal overlap. Why such confidence in the correctness of the lattice structure? Such a lattice structure follows from the properties of substances to conduct differently electricity in parallel planes and across them, create a thermal emf, and a sharp decrease in the melting temperatures for such large urchins having needles with a length of 40 fives Sb to 69- Bi. How is this all tied up?
Let's start, as always, from the very beginning. We said that heat is a stream of free heat carriers (neutrinos, neutrons, magnet charges). The direction of the flow of heat carriers is the movement from a place with a high density to a low side. We also asserted that if there is a flow and a sufficient density of carriers, their structuring begins, i. E. Formation of fives and ropes. Before entering the grid of magnets of needles, we did not consider the thermo-emf, now this moment has come.
Let's look at the side of the crystal lattice of Antimony or Bismuth, in which the planes of the elements are arranged horizontally, and between them there are vertical needles docked with an overlap, which, like spacers, hold a gap between the planes. It is more convenient for carriers of electricity and heat to move between planes where there are fewer needles and consequently less resistance. There are no magnets in the places of application of needles. However, the magnets Sb and Bi are large and strong. They create common magnetic fields of planes that have the same poles and try to push apart from each other. The least strained magnetic fields in the places where the needles are laid, where there are no magnets and in the middle between the needles. Suppose that in the gap between the planes on both sides the north poles and, for example, on the right side create a high density of magnetic charges, which must move forward and the north poles, how will they move?
Naturally, they will move in the middle of the needles, bumping into the places of their connection, under the action of the fields of planes - this is the central point of obtaining thermo-emf! Its essence lies in the fact that the scattered heat carriers here are forced into narrow passages, where their density increases sharply, and they begin to form the ropes of electricity, and the Light inside the lattice! This technique is used by all living beings for biogluc- tion!
As you can see, the ropes of electricity and Light can move, in the same corridors (passages) parallel to each other! (Crystals increase the electrical conductivity when illuminated).
Now we will concentrate on the fact that these ropes come across with partial destruction to the place of the butt joints of the needles and cause them a massive impact of the flow. As during the Second World War, tank wedges focused on a narrow section broke through the front, and the flow breaks the metal connection of the vertical needles. For this reason, the melting point of such substances sharply decreases. The determining factor for the appearance of such substances is the hedgehog needle, which has almost the entire length of a permanent magnet, and only at the end a small number of fives that rotate in different directions; Having an alternating magnetic field.
print version
Author: Valerii Fedorovich Andrus
PS The material is protected.
Date of publication 15.12.2003gg
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