Abstract

Understanding the dynamics of fluid-driven sediment transport remains challenging, as it is an intermediate region between a granular material and a fluid flow. Boyer \textit{et al.}\citep{Boyer2011} proposed a local rheology unifying dense dry-granular and viscous-suspension flows, but it has been validated only for neutrally-buoyant particles in a confined system. Here we generalize the Boyer \textit{et al.}\citep{Boyer2011} model to account for the weight of a particle by addition of a pressure P0P_0, and test the ability of this model to describe sediment transport in an idealized laboratory river. We subject a bed of settling plastic particles to a laminar-shear flow from above, and use Refractive-Index-Matching to track particles' motion and determine local rheology --- from the fluid-granular interface to deep in the granular bed. Data from all experiments collapse onto a single curve of friction μμ as a function of the viscous number IvI_v over the range 10−5≤Iv≤110^{-5} \leq I_v \leq 1, validating the local rheology model. For Iv<10−5I_v < 10^{-5}, however, data do not collapse. Instead of undergoing a jamming transition with μ→μsμ\rightarrow μ_s as expected, particles transition to a creeping regime where we observe a continuous decay of the friction coefficient μ≤μsμ\leq μ_s as IvI_v decreases. The rheology of this creep regime cannot be described by the local model, and more work is needed to determine whether a non-local rheology model can be modified to account for our findings.

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