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Determination of the Effective Viscosity of Non-newtonian Fluids Flowing Through Porous Media

机译:通过多孔介质流动的非牛顿流体的有效粘度的测定

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摘要

When non-Newtonian fluids flow through porous media, the topology of the pore space leads to a broad range of flow velocities and shear rates. Consequently, the local viscosity of the fluid also varies in space with a non-linear dependence on the Darcy velocity. Therefore, an effective viscosity μeff is usually used to describe the flow at the Darcy scale. For most non-Newtonian flows the rheology of the fluid can be described by a (non linear) function of the shear rate. Current approaches estimate the effective viscosity by first calculating an effective shear rate mainly by adopting a power-law model for the rheology and including an empirical correction factor. In a second step this averaged shear rate is used together with the real rheology of the fluid to calculate μeff. In this work, we derive a semi-analytical expression for the local viscosity profile using a Carreau type fluid, which is a more broadly applicable model than the power-law model. By solving the flow equations in a circular cross section of a capillary we are able to calculate the average viscous resistance 〈μ〉 directly as a spatial average of the local viscosity. This approach circumvents the use of classical capillary bundle models and allows to upscale the viscosity distribution in a pore with a mean pore size to the Darcy scale. Different from commonly used capillary bundle models, the presented approach does neither require tortuosity nor permeability as input parameters. Consequently, our model only uses the characteristic length scale of the porous media and does not require empirical coefficients. The comparison of the proposed model with flow cell experiments conducted in a packed bed of monodisperse spherical beads shows, that our approach performs well by only using the physical rheology of the fluid, the porosity and the estimated mean pore size, without the need to determine an effective shear rate. The good agreement of our model with flow experiments and existing models suggests that the mean viscosity 〈μ〉 is a good estimate for the effective Darcy viscosity μeff providing physical insight into upscaling of non-Newtonian flows in porous media.
机译:当非牛顿流体通过多孔介质流动时,孔隙空间的拓扑导致宽范围的流速和剪切速率。因此,流体的局部粘度也在空间内变化,具有对达西速度的非线性依赖性。因此,通常使用有效粘度μEFF来描述达西规模处的流动。对于大多数非牛顿流程,可以通过剪切速率的(非线性)函数来描述流体的流变学。目前的方法通过首先计算有效的剪切速率来估计有效的粘度,主要通过采用流变学和包括经验校正因子来计算有效的剪切速率。在第二步骤中,这种平均剪切速率与流体的实际流变学相同使用以计算μEFF。在这项工作中,我们使用古老的型流体来得出用于局部粘度曲线的半分析表达,这是比电力法模型更广泛适用的模型。通过求解毛细管的圆形横截面中的流动方程,我们能够将平均粘性电阻与局部粘度的空间平均值计算。这种方法避免了经典毛细管束模型的使用,并允许在达西秤上以平均孔径尺寸的孔中的粘度分布上升。与常用的毛细管束模型不同,所提出的方法既不需要曲折性也不是输入参数。因此,我们的模型仅使用多孔介质的特征长度,并且不需要经验系数。在单分散球形珠子的填充床中进行流动细胞实验的所提出模型的比较显示,我们的方法仅通过使用流体的物理流变,孔隙率和估计的平均孔径进行良好,而无需确定有效的剪切速率。我们的模型与流动实验和现有模型的良好一致性表明,平均粘度<μ>是对有效达西粘度μEFF提供物理洞察多孔介质中的非牛顿流动的升高的良好估计。

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