This work seeks to develop a theory for predicting microstructure of colloidal suspensions as a function of dimensionless quantities: Pe =6¹ηγ.a3/kbT and particle volume fraction, ϕ, where γ. is the shear rate, a is the particle radius, η is the viscosity of the fluid matrix and kbT is the thermal energy. This problem was pursued by conditionally averaging probability distribution function conservation equation (Smoluchowski equation) for two particles. Many-body effects in the averaged hydrodynamic and thermodynamic coefficients of the conservation equation were then formulated self-consistently through probabilistic third-particle integrals. The resulting differential-integral conservation equation was solved using an iterative method. Comparison between the theory predictions and simulation results showed that the theory was able to predict the well-known near equilibrium (Pe << 1) and dilute suspensions (ϕ <<1) results. In addition this theory was capable of predicting the details of microstructure at Pe >1 and concentrated regime, which differentiates it from the previous theoretical works in the field. The important rheological quantities such as shear stress, τ, first and second normal stress differences, N1 and N2 were calculated based on the obtained microstructure and were compared with simulation results. The results of this work suggest that the proposed self-consistent approach is able to capture the many-body hydrodynamic interactions in colloidal suspensions.
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