We study real-time dynamics of a charge carrier introduced into undoped Mott insulator propagating under a constant electric field F on the t-J ladder and square lattice. We calculate quasistationary current. In both systems adiabatic regime is observed followed by the positive differential resistivity (PDR) at moderate fields where carrier mobility is determined. Quantitative differences between ladder and 2-dimensional (2D) system emerge when at large fields both systems enter negative differential resistivity (NDR) regime. In the ladder system Bloch-like oscillations prevail, while in 2D the current remains finite, proportional to 1/F . The crossover between PDR and NDR regime in 2D is accompanied by a change of the spatial structure of the propagating spin polaron. [12,13] and the relaxation of correlated systems after the photoexcitations [14,15], represent the well-studied examples of nonequilibrium phenomena which are important both for fundamental understanding of strongly correlated systems as well as for their potential applications.Most of theoretical studies so far considered the breakdown of undoped MI, when threshold value of the electric field exceeds experimental value [9] by a few orders of magnitude (see discussion in Ref. [11]). It indicates that other transport mechanism becomes active at energies much lower than the Mott-Hubbard gap. In this Letter we inveqstigate a nonequilibrium response of a charge carrier doped into the insulator and driven by an uniform electric field F . Understanding of this subject on one hand widens our knowledge of a charge carrier doped into the antiferromagnetic (AFM) background [16,17], on the other, it represents a fundamental problem of a quantum particle moving in a dissipative medium [18].Having in mind strongly correlated systems, we investigate the t-J model where the particle driven by a constant electric field dissipates the energy by inelastic scattering on spin degrees of freedom. We use numerical approaches to treat t-J model at zero temperature on two different system geometries, i.e., a ladder with periodic boundary conditions and an infinite 2-dimensional (2D)