Now we come to the announced construction of various elementary particles. Initially, we will deal with the construction of the singly-charged elementary particles by having the charge run on the proposed guessed orbits as follows.

We start with the circumscribed tetrahedron. Fig. 25 shows the found solution which is only possible for a circumscribed tetrahedron if our conditions are satisfied. Initially, let us call this particle Tu. Each of the four small circular segments is parallel to one polyhedron edge (1,2); here four of the tetrahedron edges are “skipped” and only two opposite edges are each used twice for this parallelism. Thus, the spatial direction that is perpendicular to these preferred edges is distinguished with respect to the other directions which are shown in Fig. 26. We have to recognize that these four ellipses that continuously merge into each other represent a new kind of “spin rosette”, since now these ellipses do not meet each other in the center but overlap each other so that our “forward spin with reverse gear” has vanished. We do not want to suggest more at this point because in this phase of the examination of our models we are not yet able to calculate the “spin” as we did in the former procedure. The reason is that we have to specify masses for the mean angular momentum around such an axis. But we have just realized that rest mass and self-interaction energy are directly interdependent so that we can achieve precise data of the spin only if we know more about the rest masses of our particles. Thus, we will use the term “forward spin with reverse gear” (instead of “spin”) in order to identify our particles later more easily, and we expect that the behavior in this distinguished direction can be considered spin compensation. Fig. 27 shows one of the four directions of self-interaction.