BOOK 2. THE BATH SCHOOL. N. LEVASHOV'S «SVETL BROOM» IN A. KHATYBOV'S «BATH SCHOOL» AND A LABOUR SPADE

F. Shkrudnev N. Levashov's "SvetL Broom" in A. Khatybov's "Bath School" and A Labour Spade 117 The number of rotation angles of the charge agrees with the multiplicative relation for the symmetry system, or 108 (18 axes and 6 transmissions). This was also taken into account when developing "SvetL" Programs . But this is only in a complex space. Entering the function y=sinx , we change the coordinates and get a 36- multiplicative relation (12 axes and 3 transmissions) for the quaternion. Entering a sinusoidal function in a system of complete symmetry is a jump by an angle p /2 c with the continuation of the sign system from the preceding series. However, the entering of this function is a direct dependence on the value of the number p and, as will be shown below, ignorance of this number leads to a chaotic scattering of the capacity of the potential, and not to a directed action. The random formation of a stable vortex, even for a non- inertial mass, is impossible for a period of more than 0.1 sec. The next jump in the origin is made by exhausting the sign series of the quaternion – the transition to an octave. The jump is linear, but its value = p , for octaves we get 8 (8 symmetry axes and 1 transmission). Thus, the complete sign system is 152 signs – one triple revolution of the vector. NOW YOU SEE HOW IT IS ALL SIMPLE. The first sign of the complex expression must be the continuation of the sequence of the last sign of the octave, otherwise there will be a breakdown in sign and scattering of the potential. If this is considered regarding “ SvetL" Programs , then the potential scattering might not occur, because the last octave sign is controlled by the Brain in interaction with the Generator through the Programs. This could be understood and achieved only thanks to the calculations made by A. Khatybov in his monograph "Cold Nuclear Synthesis." The Coulomb law was not regarded as the law for the organization of a directed vortex process and was transferred to inertial masses as the basic law of "attraction" of inertial masses. Considering that the potential is not an abstract quantity, but strictly "tied" to the corresponding frequency, we get: = + , - ∗ , ∗ ( ) ) . ,/( Here j is the number of frequencies for the formation of a stable vortex; i – is the sign operator for potentials of a given frequency; r – is the radius of the vortex;