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Hydrodynamic modeling reveals non-monotonic drag instabilities over rough seafloors in non-zonal ocean flows, highlighting novel mechanisms driving mesoscale eddy and jet formation.
Topographic roughness, defined as irregular variability of ocean depth on lateral scales of 1–10 km, has recently been shown to substantially impact the dynamics of large-scale and mesoscale ocean flows, including eddies, Rossby waves and baroclinic instability. This suggests that accurate modelling of roughness-induced forcing is critical for representing large-scale ocean behaviour. A recent multi-scale analysis of flows affected by small-scale bathymetry has produced the ‘sandpaper theory’, an explicit parametrisation of the roughness-induced bottom drag. This model accurately captures the impact of small-scale topography on large-scale flows without the need to resolve it in general circulation models. A peculiar facet of the sandpaper theory is that the drag is a non-monotonic function of the flow speed above the bottom boundary layer, which results in an instability. We characterise this non-monotonic drag instability for a series of barotropic and baroclinic systems, and explore a dynamically rich variety of scenarios that can produce stable jets, overstable Rossby waves, mesoscale eddy streets and self-amplifying hetons. We describe and quantify the properties of each flow type as they pertain to this non-monotonic drag regime.
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Brown et al. (2026) studied this question.
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