Spontaneous capillary imbibition in liquid–liquid systems with a shear-thinning wetting phase is crucial in natural and industrial processes yet remains underexplored. Shear-thinning fluids exhibit a continuous transition between power law and Newtonian behavior as the shear rate varies. To capture this rheological evolution during imbibition, we propose a Carreau–Yasuda-based transition function that quantitatively characterizes the relationship between wall shear rate and imbibition rate. Based on this function, we derive a governing equation, termed the transition model, to describe the capillary rise dynamics when Carreau–Yasuda fluid displaces a viscous liquid. The model is validated through multi-relaxation-time color-gradient lattice Boltzmann simulations. In parallel, capillary rise experiments using xanthan gum solutions and silicone oil are conducted to provide physical observations. The proposed transition function accurately captures the dynamic wall shear rate–imbibition rate relationship as Carreau–Yasuda fluids transition between power law and Newtonian behavior. Numerical solutions of the transition model closely align with experimental observation and lattice Boltzmann method simulation, whereas traditional power law model deviates at lower imbibition rates. Scaling analysis showed that, different from power law fluid, Carreau–Yasuda fluid imbibition in late viscous stage still obeys the classic square-root law when the imbibition rate falls below the critical value defined by the model and otherwise follows a power law scaling. This work provides new insights in shear-thinning fluids liquid–liquid imbibition and offers a robust framework for advancing the studies of non-Newtonian fluid imbibition in complex geometries.
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