A model with both Rashba and Dresselhaus spin orbit (SO) couplings and Hubbard electronelectron interaction is studied on planar strips at quarter filling at zero temperature in the clean limit. In the absence of Hubbard repulsion and at equilibrium, within linear response theory, a nonmonotonic behavior of the spin Hall conductivity as a function of the ratio of the Rashba (α) and Dresselhaus (β) strengths was found for large enough SO strengths. This behavior is signalled by a peak or a cusp, depending on the strip width, at intermediate values of β/α in the interval [0, 1]. This behavior of the spin Hall conductivity was correlated with the one for the longitudinal spin conductivity. This study was then extended to the out-of-equilibrium regime that arises by imposing a finite voltage bias between the two ends of an open strip. This system, in the presence of a Hubbard term with coupling U , was treated with the density matrix renormalization group technique and with the Landauer-Buttiker formalism. It was found that relevant properties to the spin Hall effect, such as the transversal spin current and the spin accumulation, present a similar nonmonotonic behavior as the one found for the spin conductivities. More importantly, it was also found that these properties are enhanced by the repulsive Hubbard interaction up to a moderate value of U .