Oscillatory laminar shear flow over a compliant viscoelastic layer on a rigid base

Abstract

We present an analytical study of oscillatory laminar shear flow over a compliant viscoelastic layer on a rigid base. This problem relates to oscillating blood flow in viscoelastic vessels. The deeper motivation for this study, however, is the possible use of compliant coatings for turbulent drag reduction. An analytical solution of the fluid and solid velocity is presented, and five dimensionless parameters emerge. The interaction between fluid and solid appears to be determined by a single combined dimensionless parameter, which we call the shear interaction parameter χ. The fluid satisfies a no-slip boundary condition when |χ| → 0, which occurs when the solid is heavy, stiff and/or thin. In contrast, the fluid obeys a free-slip boundary condition when |χ| → ∞, which corresponds to a lightweight and/or soft solid. Three types of resonance modes are identified for an elastic solid. Two modes (odd and even) are specific to the solid. The third mode results from the coupling with the fluid. The three modes are less pronounced or even absent for a viscoelastic solid. These findings have a twofold use. First, they help to understand the fluid and solid dynamics when shear coupling is important. Second, the presented analytical solution is very useful for validation of numerical fluid-structure-interaction solvers. Future work might include the extension of the theory to multiple viscoelastic layers and the dynamic coupling of normal stresses.

Analytical solutions of incompressible laminar channel and pipe flows driven by in-plane wall oscillations

“…34 Despite this, under certain technical conditions, it is possible to derive novel linear analytical solutions as it has been recently demonstrated. [35][36][37] Here, special cases of incompressible confined flows are considered for which exact linear analytical solutions can be derived. The present work aims at providing a comprehensive description of laminar channel and pipe flows driven by uniform and traveling wave wall motions.…”