Abstract

The onset of monami – the synchronous waving of seagrass beds driven by a steady flow – is modelled as a linear instability of the flow. Unlike previous works, our model considers the drag exerted by the grass in establishing the steady flow profile, and in damping out perturbations to it. We find two distinct modes of instability, which we label modes 1 and 2. Mode 1 is closely related to Kelvin–Helmholtz instability modified by vegetation drag, whereas mode 2 is unrelated to Kelvin–Helmholtz instability and arises from an interaction between the flow in the vegetated and unvegetated layers. The vegetation damping, according to our model, leads to a finite threshold flow for both of these modes. Experimental observations for the onset and frequency of waving compare well with model predictions for the instability onset criteria and the imaginary part of the complex growth rate respectively, but experiments lie in a parameter regime where the two modes can not be distinguished.

Highlights

  • Seagrasses exhibit a rich set of dynamical behaviours due to their collective interaction with fluid flows

  • We present a linear hydrodynamic instability underlying the onset of these coherent oscillations

  • While some features of the instability are similar to KH instability, we find significant differences

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Summary

Introduction

Seagrasses exhibit a rich set of dynamical behaviours due to their collective interaction with fluid flows. The grass responds to these eddies by deforming, which leads to large-amplitude synchronous oscillations of the grass blades This picture can be used to derive a simple scaling dependence of the monami frequency on the flow speed and the shear layer thickness, and to understand transport in the seagrass bed (Nepf & Vivoni 2000; Ghisalberti & Nepf 2002, 2004; Okamoto, Nezu & Ikeda 2012). The velocity profile of the free shear layer is assumed ad hoc to be piecewise linear (Py, De Langre & Moulia 2006) or hyperbolic tangent (Raupach et al 1996; Ghisalberti & Nepf 2002), with parameters fitted using the experimental observations The origin of these profiles, the values of the fitted parameters, and their effect on monami remain unexplained.

Mathematical model
Linear stability analysis
Mode 1
Conclusion
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