“…To compare the impact of the shear rate, the data are plotted as a function of dimensionless time (α⟨ G ⟩ tϕ ), − where the prefactor α is a function of primary particle’s Peclet number ( Pe ), through power-law dependency, α = Pe – n . The scaling parameter, n , is a function of the interparticle interactions, characterized with the ratio of the Hamaker constant and k B T and Pe , as n = 0.18 – (0.82 bPe 0.82 )/(1 – exp ( bPe 0.82 )) with b = 4( A H /12 k B T ) 0.18 . − As can be seen, the initial aggregation period was rather fast, and at the dimensionless time equal to two, all conditions already reached the steady state that is characterized by the dynamic equilibrium between aggregation and breakup. ,, When comparing the steady-state sizes, it can be seen that by increasing the vessel averaged shear rate, the size of aggregates becomes smaller as a result of a stronger impact of the breakup. This observation is in agreement with the available data in the literature. ,,,,,, Somehow surprising is the dramatic increase of the steady-state aggregate sizes when temperature rises from 5 to 25 °C, almost by 1 order of magnitude.…”