This idea of rotating magnetic fields is the first successful application of our model based on the real relationships set up by nature. We assess them to be an indication of the accuracy of the model and will be looking meanwhile for other indications (before we try to answer the question about the cause of the electron's wobbling characteristics). We will use this method of thinking ahead just to check if the specified orbital model offers even more related signs, which would provide a clear, unrestrained picture of natural processes and, whether a further consideration makes sense at all. Thus, we raise the following question: How many electron orbits of this kind can we allow on such a spherical shell if the atomic number is correspondingly increased? We have assumed the electron to swim on its own magnetic field. Therefore, we must state now: only one second electron fits onto the spherical shell (Fig. 9). This second electron must be located opposite the first on each point of the orbit (it shall be hidden behind the nucleus in such a manner that the two electrons do not "see" each other). Every further electron that is added would terminate this nice game of hide-and-seek, and according to the magnetic field theorem, "notice" the magnetic fields of the other two electrons. The harmony would come to an end and the stationary orbit would be corrupted.

This is a illustrative interpretation of the Pauli exclusion principle. In spite of this, we still have to make up for something. We still owe a clear interpretation of the electron spin since without a spin we cannot explain the Pauli principle. After all, it is known that the introduced spin puts the electron into such a powerful rotation that it collides with the theory of relativity. However, the orbit introduced by us copes with lower speeds. Again we look toward the direction e - f and see a magnetic field generated by 4 orbiting lobes which is not in contradiction to our magnetic field theorem (Fig. 10). This is the spin.

Due to our theory of a hide-and-seek game for two electrons, this rosette surface is orbited by the two electrons in the opposite direction and we will obtain the correct result for the anti-parallel orientation of the spin magnets for the inert gas helium in its ground state.