We consider the laminar flow of a vortex crystal in the Corbino disk geometry. Laminar flow can be induced by thermal fluctuations melting the crystal, but also by shear stress after applying a large current at zero temperature. While the velocity profile is the same in the two cases, the underlying vortex structure is completely different. A vortex crystal in this geometry can flow in a laminar fashion whenever the appropriate curvature is established in the vortex lattice. This curvature requires the presence of geometrically necessary disclinations, which here migrate from the boundary to the bulk of the crystal in the form of current-induced grain boundary scars in flat geometry. We provide an estimate of the characteristic current needed to initiate such a laminar flow regime in the vortex crystal and show that the result is in good agreement with simulations. Under small shear stress, most liquids exhibit a laminar flow response: the local fluid velocity is proportional to the local force and they flow orderly in layers. Conversely, crystals do not flow at small stress, but deform elastically until the stress is large enough to cause plastic or irreversible flow. Notwithstanding, at very high loads crystals are sometimes observed to shear melt [1], which leads again to a laminar flow regime. To understand any microstructural differences between laminar flow in liquid and crystal phases it is necessary to observe atomic arrangements and the microscopic topological structure of the system while it is sheared. In this respect, self-assembled structures of artificial atoms [2], such as synthetic nanocrystals, magnetic colloids, charged particles in Coulomb crystals, proteins and surfactants, or vortices in type II superconductors and in Bose-Einstein condensates, represent ideal systems for this purpose. In particular, experiments and numerical simulations have suggested that shear-melting occurs in driven colloidal crystals [1,3] and superconducting vortex lattices [4].Experiments of superconducting vortex flow in the Corbino geometry display intriguing dynamic phases as a function of temperature and applied current. López et al.[5] have evaluated the vortex velocity profiles after measuring the voltage drop across a series of contacts placed radially on a superconducting disk. For low currents and temperatures, vortices move as a rigid solid. When the current exceeds a threshold value I 0 , the vortex crystal cannot sustain the shear stress induced by the resulting inhomogeneous Lorentz force and the response becomes plastic. Finally, at higher currents the flow is laminar. Theoretical [6,7] and numerical [8] studies have clarified the role played by topological defects in these transitions, revealing that when the flow is laminar dislocations are arranged into long radial grain boundary (GB) scars [8]. Similar dislocation scars have received much attention in recent years in the study of crystalline materials on curved manifolds. In these systems, the interplay of crystalline order and the curvature of the ...