Montellà E P, Toraldo M, Chareyre B, Sibille L
University Grenoble Alpes (UGA), 3SR, F-38000 Grenoble, France.
Phys Rev E. 2016 Nov;94(5-1):052905. doi: 10.1103/PhysRevE.94.052905. Epub 2016 Nov 10.
We present analytical and numerical results on localized fluidization within a granular layer subjected to a local injection of fluid. As the injection rate increases the three different regimes previously reported in the literature are recovered: homogeneous expansion of the bed, fluidized cavity in which fluidization starts developing above the injection area, and finally the chimney of fluidized grains when the fluidization zone reaches the free surface. The analytical approach is at the continuum scale, based on Darcy's law and Therzaghi's effective stress principle. It provides a good description of the phenomenon as long as the porosity of the granular assembly remains relatively homogeneous, i.e., for small injection rates. The numerical approach is at the particle scale based on the coupled discrete element method and a pore-scale finite volume method. It tackles the more heterogeneous situations which occur at larger injection rates. The results from both methods are in qualitative agreement with data published independently. A more quantitative agreement is achieved by the numerical model. A direct link is evidenced between the occurrence of the different regimes of fluidization and the injection aperture. While narrow apertures let the three different regimes be distinguished clearly, larger apertures tend to produce a single homogeneous fluidization regime. In the former case, it is found that the transition between the cavity regime and the chimney regime for an increasing injection rate coincides with a peak in the evolution of inlet pressure. Finally, the occurrence of the different regimes is defined in terms of the normalized flux and aperture.
我们给出了关于颗粒层内局部流化的分析和数值结果,该颗粒层受到局部流体注入。随着注入速率的增加,文献中先前报道的三种不同状态得以重现:床层的均匀膨胀、在注入区域上方开始发展流化的流化腔,以及当流化区域到达自由表面时最终形成的流化颗粒烟囱。分析方法基于达西定律和太沙基有效应力原理,处于连续介质尺度。只要颗粒集合体的孔隙率保持相对均匀,即对于小注入速率,它就能很好地描述该现象。数值方法基于耦合离散元法和孔隙尺度有限体积法,处于颗粒尺度。它处理在较大注入速率下出现的更不均匀的情况。两种方法的结果与独立发表的数据在定性上一致。数值模型实现了更定量的一致性。流化的不同状态的出现与注入孔径之间存在直接联系。窄孔径能清晰区分三种不同状态,而较大孔径倾向于产生单一的均匀流化状态。在前一种情况下,发现随着注入速率增加,腔态和烟囱态之间的转变与入口压力演变中的一个峰值相吻合。最后,根据归一化通量和孔径定义了不同状态的出现情况。