The properties of aggregated marine sediment, or flocs, exert an influence on numerous estuarine processes (Dyer, 1989). For example, suspended sediment settling fluxes are a strong function of both particle size and composition (Manning & Bass, 2006), and predicting these fluxes is critical as sea level rise drives unprecedented morphological changes along coastlines and within estuaries worldwide (Prandle & Lane, 2015). Additionally, the transport of contaminants that readily adhere to sediment aggregates is largely determined by the transport properties of the aggregates themselves (Lick, 2008;Mehta et al., 2014), necessitating a comprehensive understanding of how flocs move and evolve in wavy, turbulent flows. Rates of photosynthesis and the potential for algal blooms, too, are controlled by the vertical distribution of particles throughout the water column (Cloern, 1996), which itself depends on the interplay between hydrodynamic forcing and particle characteristics.Numerical models often simulate the transport of flocs by separating them into discrete size classes (James et al., 2010;Soulsby et al., 2013;Verney et al., 2009). Each size class is then treated as an Eulerian concentration field with a superimposed settling velocity, 𝐴𝐴 𝐴𝐴𝑠𝑠 , assumed to follow Stokes Law (Stokes, 1851), 𝑤𝑤𝑠𝑠 =