N. LEVASHOV'S «SVETL BROOM» IN A. KHATYBOV'S «BATH SCHOOL» AND A LABOUR SPADE. BOOK 4. THE PHYSICS OF THE REALITIES

F. Shkrudnev N. Levashov's "SvetL Broom" in A. Khatybov's "Bath School" and A Labour Spade 321 6.3. Medium of motion from the direction of the "SvetL" Programs It is expedient to consider the motion medium from different points of view – classical physics, as more or less understandable (the interaction of masses and certain gravitational fields), and physics that takes into account the energy features of the medium in relation to the working conditions of the " SvetL " Programs. All this have to be remembered when striving for taking the Bath, being in the medium of the motion in this direction. Laws of classical physics By the medium of motion is meant the spatial atmosphere in which bodies move. The basic law by which bodies move in a spatial atmosphere is Newton's law: P=m·g (1) On the other hand, Newton's law is used for bodies: , (2) where g is the acceleration of gravitation (m/sec 2 ). Through the coefficient k, the dependencies of free motion are established both in the atmosphere and in the Cosmos. According to modern concepts and terminology, in Newton's 1st and 2nd laws by the body it is necessary to understand the material point, and by the motion – the motion relative to the inertial reference system. The mathematical expression of the second law in classical mechanics is like this: d(mv)dt=F, (3) that is, the movement takes place in time. By the way, the standard of time is defined as the vibrations of cesium atom and, as can be pointed out, it has no relation to the concrete movement. According to the law of universal gravitation (non-relativistic mechanics), the law (2) describes the universal property of matter to create the gravitational field and experience the actions of gravitational fields. In the framework of the Newton law (2) the gravitational field can be described with the help of the scalar potential j , while force F acting on the test particle of mass m is equal to: F=-grad j (4) The potential j meets the Poisson condition: