Shojaaee Zahra, Roux Jean-Noël, Chevoir François, Wolf Dietrich E
Faculty of Physics, University of Duisburg-Essen, 47048 Duisburg, Germany.
Phys Rev E Stat Nonlin Soft Matter Phys. 2012 Jul;86(1 Pt 1):011301. doi: 10.1103/PhysRevE.86.011301. Epub 2012 Jul 6.
We report on a numerical study of the shear flow of a simple two-dimensional model of a granular material under controlled normal stress between two parallel smooth frictional walls moving with opposite velocities ± V. Discrete simulations, which are carried out with the contact dynamics method in dense assemblies of disks, reveal that, unlike rough walls made of strands of particles, smooth ones can lead to shear strain localization in the boundary layer. Specifically, we observe, for decreasing V, first a fluidlike regime (A), in which the whole granular layer is sheared, with a homogeneous strain rate except near the walls, then (B) a symmetric velocity profile with a solid block in the middle and strain localized near the walls, and finally (C) a state with broken symmetry in which the shear rate is confined to one boundary layer, while the bulk of the material moves together with the opposite wall. Both transitions are independent of system size and occur for specific values of V. Transient times are discussed. We show that the first transition, between regimes A and B, can be deduced from constitutive laws identified for the bulk material and the boundary layer, while the second one could be associated with an instability in the behavior of the boundary layer. The boundary zone constitutive law, however, is observed to depend on the state of the bulk material nearby.
我们报告了一项关于颗粒材料简单二维模型在两个以相反速度±V 移动的平行光滑摩擦壁之间受控法向应力下的剪切流的数值研究。在密集圆盘组件中使用接触动力学方法进行的离散模拟表明,与由颗粒链构成的粗糙壁不同,光滑壁会导致边界层中的剪切应变局部化。具体而言,随着 V 的减小,我们首先观察到一种类流体状态(A),其中整个颗粒层被剪切,除了靠近壁的区域外应变率均匀,然后是(B)一种对称速度分布,中间有一个固体块,应变集中在壁附近,最后是(C)一种对称性破缺的状态,其中剪切率局限于一个边界层,而大部分材料与相对的壁一起移动。这两种转变都与系统尺寸无关,并且在特定的 V 值下发生。文中讨论了瞬态时间。我们表明,A 态和 B 态之间的第一次转变可以从为主体材料和边界层确定的本构定律推导出来,而第二次转变可能与边界层行为的不稳定性有关。然而,观察到边界区域的本构定律取决于附近主体材料的状态。