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The impact of turbulence on flying insects in tethered and free flight: high-resolution numerical experiments

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arxiv 1901.10350 v1 pith:KFSXZ22G submitted 2019-01-29 physics.flu-dyn

The impact of turbulence on flying insects in tethered and free flight: high-resolution numerical experiments

classification physics.flu-dyn
keywords turbulentturbulenceintensityinflowinsectsadaptedchangingcontrol
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Flapping insects are remarkably agile fliers, adapted to a highly turbulent environment. We present a series of high resolution numerical simulations of a bumblebee interacting with turbulent inflow. We consider both tethered and free flight, the latter with all six degrees of freedom coupled to the Navier--Stokes equations. To this end we vary the characteristics of the turbulent inflow, either changing the turbulence intensity or the spectral distribution of turbulent kinetic energy. Active control is excluded in order to quantify the passive response real animals exhibit during their reaction time delay, before the wing beat can be adapted. Modifying the turbulence intensity shows no significant impact on the cycle-averaged aerodynamical forces, moments and power, compared to laminar inflow conditions. The fluctuations of aerodynamic observables, however, significantly grow with increasing turbulence intensity. Changing the integral scale of turbulent perturbations, while keeping the turbulence intensity fixed, shows that the fluctuation level of forces and moments is significantly reduced if the integral scale is smaller than the wing length. Our study shows that the scale-dependent energy distribution in the surrounding turbulent flow is a relevant factor conditioning how flying insects control their body orientation.

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  1. Turbulence-based parametrization of animal flight

    physics.flu-dyn 2026-06 unverdicted novelty 7.0

    Empirical scaling analysis of flight parameters from 400+ species recovers the turbulence energy exponent -5/3 for the proxy E_sp = b^3 f^2.