When a circularly-symmetric light beam with optical vortex (OV) diffracts at an opaque screen with the sharp edge, the OV core is displaced from the beam axis and, in case of the mcharged incident OV, decomposed into |m| single-charged ones. By means of numerical simulations and based on examples of incident beams with topological charges |m| =1, 2, 3 we show that, while the screen edge monotonously advances towards the beam axis, the OVs in the diffracted beam cross section move away from the incident beam axis along spiral-like trajectories. The trajectories contain fine structure details that reflect the nature and peculiar spatial configuration of the diffracting beam. For the Kummer beams' diffraction, the trajectories contain self-crossings and regions of "backward" rotation (loops); in case of Laguerre-Gaussian beams, the trajectories are smoother. The numerical results are supported by analytical approximations and conform with experiment The general shape of the trajectories and their local behavior show high sensitivity to the diffraction conditions (spatial structure of the diffracting beam, its disposition with respect to the screen edge, etc.), which can be used in diverse metrological applications. Besides the rich and impressive physical contents, including the phase singularities, internal energy circulation, specific features of the linear and angular momentum distributions [4][5][6], such beams offer a wide range of perspective applications in the micromanipulation techniques [7][8][9][10], information transfer and processing [11,12], sensitivity and resolution enhancement in optical observations and measurements [13][14][15][16][17][18][19].Among diverse manifestations of the specific "circulational" properties of optical vortices, an important place belongs to the edge diffraction phenomena [20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. A series of experimental and theoretical researches has demonstrated that diffraction "reveals" the internal energy circulation, normally "hidden" in circular OV beams, and induces the essential transformation of their phase profile. In particular, even at weak screening (when the opaque obstacle covers only a far periphery of the beam cross section and induces no visible deformation of the intensity profile), the axial OV of the incident beam changes its position and, if its absolute topological charge |m| > 1, splits into a set of |m| single-charged "secondary" vortices. As a result, a complicated pattern of singular points ("singular skeleton") is formed in the diffracted beam cross section that is highly sensitive to the diffraction conditions, especially to the screen edge position with respect to the incident beam axis.