In the present work, the effect of a fluid's yield stress is investigated on the hydroelastic instability in pressuredriven flow through a two-dimensional channel lined with a highly-compliant polymeric gel. Having assumed that the fluid obeys the Herschel-Bulkley model with the gel obeying the two-parameter Mooney-Rivlin model, analytical basic solutions were obtained for the fluid and solid sides at vanishingly-small Reynolds numbers. The stability of the basic solutions so-obtained was then investigated when subjected to infinitesimally-small, normal-mode perturbations. Having dropped all nonlinear perturbation terms, an eigenvalue problem was obtained which was numerically solved using the shooting method. The effect of the fluid's yield stress was then examined on the growth rate of the most unstable modes. Based on the numerical results obtained in this work, it is concluded that the yield stress has a destabilizing effect on pressure-driven flows of Bingham fluids in two-dimensional channels lined with compliant gels. For Herschel-Bulkley fluids, the effect of yield stress can be stabilizing or destabilizing depending on the power-law exponent (i.e., the degree of the fluid's shear-thinning). gel to obey the hyperelastic Mooney-Rivlin model, to the best of our knowledge, for the first time. This robust solid model better fits rheological data for soft polymeric gels, and so it is expected that more meaningful results could be obtained using this model. 12) Like Gkanis and Kumar 5) , we intend to focus on the creeping flow case only both because of its industrial implications in microfluidic field and also because it excludes complications which might arise through the rise of Tollmien-Schlichting (TS) waves. At this extreme, Gkanis and Kumar 5) have shown that for pressure-driven flow of Newtonian fluids in compliant channels, there are two types of instability for Re = 0: i) a finite-wavelength mode which becomes unstable for sufficiently thick solids, and (ii) a short-wavelength mode which arises due to the discontinuity of the first normal stress difference at the interface. It would be interesting to see how these modes are affected by a fluid's yield stress. To achieve its objectives, the work is organized as follows. In the next section we present the governing equations for the solid and the fluid side. We then proceed with obtaining the basic solution for each phase. The linearized equations governing the stability of the basic state are then introduced. The numerical method of solution is briefly described followed by presenting the numerical results. The work is summarized by highlighting its major findings.
GOVERNING EQUATIONSWe consider the pressure-driven flow of a viscoplastic fluid in planar Poiseuille flow, as shown in Fig. 1. As can be seen in this figure, the upper and lower plates are lined with a complaint layer made of a soft polymeric gel having a thickness of HR with 2R representing the height of the channel. Assuming that the width of the channel is much larger than its height, we w...