Viscoplastic corner eddies

When viscous fluid in a corner is disturbed, eddies can form in the absence of inertia. Examples of flow configurations in which this motion occurs include flow through an abrupt contraction and over a cavity. Six decades ago, Moffatt (1964) calculated the slow viscous flow of Newtonian fluids in sharp corners, detailing his eponymous “Moffatt eddies”. In this study, we examine corner flows of viscoplastic materials, a class of non-Newtonian fluids which exhibit solid-like behaviour for stresses below a yield stress. Specifically we consider a Bingham fluid, for which the material is perfectly rigid at stresses below the yield-stress. While a static unyielded plug forms at the tip of the corner, eddies analogous to those found by Moffatt (1964) can also form. We examine these viscoplastic eddies numerically, by computing finite element solutions using the augmented-Lagrangian method, and analytically, by employing a viscoplastic boundary-layer formulation and scaling arguments. We measure the depth of the static plug as a function of Bingham number (dimensionless yield-stress), show that the process of a new eddy forming as the Bingham number is decreased is driven by the pressure in the yielded fluid adjacent to the static plug, and provide a heuristic argument for the critical Bingham number at which this occurs.