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

Book 2. The Bath School. Chapter 2. Physics of the Bath Taking Process 128 yourself. Everything is described as it is supposed to be, if something goes wrong. But if everything goes right , and you are not forgotten to be taken to the Bath, you can use "SvetL" Programs or, at the worst (depending on your resources), N. Levashov's Health Improving Sessions (from here – http://svetl.name/page/os ) and use them in strict accordance with the Instruction. As biologists have noticed, extraneous relationships do not lead to this effect. But where can we find these potentials in the conditions of a great number of relatives and the prohibition to stick out of the window? Then a little trick comes to the rescue. The wave, tightening the knot and changing the phase (so that it is not noticed), begins to walk next to the Diogenes barrel with the same angle of the Archimedes spiral (so as not to get lost). This is why I am writing about the Barrel and the Spiral in detail. Normally moving potential, naturally, encounters a lonely wave, changes it all that is possible – both the filling and the current parameters. Back in its home environment, the wave, as if nothing had happened, takes a FULL SUBSEQUENT TRANSFORMATION COURSE , having a number of innovations in stock. These innovations can only be discovered after 12 years of the new structure existence , when these innovations begin to get interested in their daddy. It remains only to guess what new properties can bring about, for example 23.5 . Since the wave does not care who will change its state, if only the potential is good; later it leads (especially after several generations) to the effect of automatic superposition, when any innovation ends only in the effect of decomposition. Isn’t it sad? But it's better to know about it than to "guess". An increase in the angle of Archimedes' spiral due to the INCREASE IN THE NUMBER OF CYCLICAL SHAPES ultimately leads to the normalization of the wave itself, when any potential can create an independent joint structure, taking such a wave as the ideal option for annihilation. Since the process of annihilation must take place under the cover of the web, this is where the process of automatic superposition takes place, in which not only properties of the potential disappear, but also the web, because the normalized wave can not be in the pit of the barrel, but only on the ledge that in time becomes connected with the web. When the necessary parameters of pressure are received from the