“…It can be shown (see [13]) that the pole of every of these logarithmic spirals coincides with the common centre of the concentric spheres above. In the limit case when a = 0 these logarithmic spirals reduce to circles and then M 3 is a parallel orbit, namely the Segre orbit (see [13], [15] Recall that partial differential prolongation of this system leads to the equations (4.9) and (4.10), but by the further prolongation the following consequences can be obtained (see [11]): by differential prolongation (see [9], [11], [14]) dA = Bω …”