So, maybe the enormous nuclear energies consequently are self-interaction energies? Nevertheless let us return to our task which is to discover one or more free self-interaction processes. As a result of this examination we expect one or more elementary particles. For this purpose, we will compile the material that we have incidentally collected until now. Let us recall a sentence that we have formulated at the beginning of our explanations. We had found that the wobbling orbit on which the electron moves on the spherical shell has flat segments. This is also true for the wobbling orbit on the ellipsoid if we disregard the slight relativistic perihelion precession (calculated by quantum theory). Consequently, we will try to use an orbit model that shall also be partially flat. Such an orbit should be continuous and closed. We further demand the orbit to be kink-free at every point. In addition, there should be spatial directions – analogous to the previous model – that are surrounded by continuous orbital segments with a continuous spatial derivative , whereby at least segments of the orbit in this spatial direction appear parallel to the paths travelled previously . We must even demand that the entire space curve we are looking for is completely composed of such self-interacting segments. Otherwise our “particle” would immediately “burst”. Thirdly, under certain conditions a spin rosette should also be identifiable in a spatial direction that must not be identical with a direction of self-interaction. This spin rosette would correspond to the gyromagnetic ratio of the spin which analogous to our model is a “forward spin with reverse gear” since some elementary particles have a spin. There are still more expectations that we have with respect to such a model: namely, we expect, as already mentioned, that not only one such model exists, also due to the fact that our conditions are too general. Further, we hope that our model’s space curves are composed of segments of circles because we assume that nature has behaved rationally and optimally in building its elementary units. (Of course behind this expectation is the author’s hope not to come across insolvable elliptic integrals again.) In spite of this, we can hope for more: we expect that free self-interaction can only occur on space curves that are located on spherical surfaces (or, if necessary, on ellipsoid surfaces) because we want the constancy of the absolute value of the angular momentum (as confirmed in the calculation of h) to be valid also in the range of free self-interaction. We still have no reason to assume the contrar.