  In this paper we propose a generalized model for the motion of a two-species
self-driven objects ranging from a scenario of a completely random environment
of particles of negligible excluded volume to a more deterministic regime of
rigid objects in an environment. Each cell of the system has a maximum
occupation level called $\sigma _{\max }$. Both species move in opposite
directions. The probability of any given particle to move to a neighboring cell
depends on the occupation of this cell according to a Fermi-Dirac like
distribution, considering a parameter $\alpha $ that controls the system
randomness. We show that for a certain $\alpha =\alpha _{c}$ the system
abruptly transits from a mobile scenario to a clogged state which is
characterized by condensates. We numerically describe the details of this
transition by coupled partial differential equations (PDE) and Monte Carlo (MC)
simulations that are in good agreement.
