The transverse beam pattern, usually observed in experiment, is a result of averaging the optical-frequency oscillations of the electromagnetic field distributed over the beam cross section. An analytical criterion is derived that these oscillations are coupled with a sort of rotation around the beam axis. This criterion appears to be in direct relation with the usual definition of the beam orbital angular momentum.OCIS codes: 070.2580, 080.4865, 140.3295, 260.6042 Light beams carrying the mechanical orbital angular momentum (OAM) with respect to the propagation axis attract great attention due to their unique physical properties and promising applications [1][2][3][4]. The question of physical origin of the vortex properties of such beams is interesting and insistent [3][4][5][6][7][8][9][10][11][12]. In attempts to answer it, researchers have employed the momentary patterns of the light field behaviour during a cycle of oscillation [3,4]. It was found that, in contrast to usual (non-vortex) beams where the evolution of the momentary transverse field distribution consists in periodical change of the field strength synchronously over the whole beam cross section, in the "classical" vortex beams (circular Laguerre-Gaussian modes) the momentary distribution of the electric field rotates with the field oscillation frequency (see Fig. 1a which illustrates the same behaviour as Fig. 10 of [3]).