# Connections between resonance and nonlinearity in swimming performance of a flexible heaving plate

## TL;DR

This study clarifies how resonance influences the swimming performance of a flexible plate in viscous fluid, revealing the interplay of linear resonant effects and nonlinear behaviors at different amplitudes.

## Contribution

It provides an unambiguous definition of resonance in viscous fluid-structure systems and distinguishes linear resonant effects from nonlinear effects in finite-amplitude swimming.

## Key findings

- Resonance peaks occur near the linear stability frequency.
- Non-resonant mechanisms become significant at large amplitudes.
- Leading-edge separation affects performance at high amplitudes.

## Abstract

We investigate the role of resonance in finite-amplitude swimming of a flexible flat plate in a viscous fluid. The role of resonance in performance remains unclear for two reasons: i) a lack of definition of resonance for the fully-coupled fluid-structure interaction system in a viscous flow, and ii) the presence of nonlinear effects, which makes it difficult to disentangle resonant and non-resonant mechanisms in finite-amplitude swimming. We address point i) and provide an unambiguous definition for system resonance by computing global linear stability modes of the fully-coupled fluid-structure interaction system that account for the viscous fluid, the plate, and the coupling between them. We then resolve point ii) by considering high-fidelity nonlinear simulations of systematically increased amplitude. By comparing the results for different amplitudes with one another and with the linear stability modes, we separate linear and/or resonant effects from nonlinear and/or non-resonant effects. Resonant behavior is observed over a wide range of plate stiffnesses, with peaks in trailing-edge motion and thrust occurring near the resonant frequency defined by the global linear analysis. The peaks broaden and weaken with increasing heave amplitude, consistent with an increased damping effect from the fluid. At the same time, non-resonant mechanisms are present at large heave amplitudes. The input power exhibits qualitatively different dynamics at large heave amplitudes compared to smaller heave amplitudes, where resonance dominates. Moreover, leading-edge separation is present for stiff plates at large heave amplitudes, which can drastically alter the performance characteristics from what one would expect through linear predictions.