Abstract
AbstractMany water quality and ecosystem functions performed by streams occur in the benthic biolayer, the biologically active upper (~5 cm) layer of the streambed. Solute transport through the benthic biolayer is facilitated by bedform pumping, a physical process in which dynamic and static pressure variations over the surface of stationary bedforms (e.g., ripples and dunes) drive flow across the sediment‐water interface. In this paper we derive two predictive modeling frameworks, one advective and the other diffusive, for solute transport through the benthic biolayer by bedform pumping. Both frameworks closely reproduce patterns and rates of bedform pumping previously measured in the laboratory, provided that the diffusion model's dispersion coefficient declines exponentially with depth. They are also functionally equivalent, such that parameter sets inferred from the 2D advective model can be applied to the 1D diffusive model, and vice versa. The functional equivalence and complementary strengths of these two models expand the range of questions that can be answered, for example, by adopting the 2D advective model to study the effects of geomorphic processes (such as bedform adjustments to land use change) on flow‐dependent processes and the 1D diffusive model to study problems where multiple transport mechanisms combine (such as bedform pumping and turbulent diffusion). By unifying 2D advective and 1D diffusive descriptions of bedform pumping, our analytical results provide a straightforward and computationally efficient approach for predicting, and better understanding, solute transport in the benthic biolayer of streams and coastal sediments.
Highlights
The movement of water into and out of the hyporheic zone, or “hyporheic exchange,” occurs over a wide range of spatial scales, from >10 km (>1 year) to
Values of the effective water depth inferred from the advective model are similar to values estimated from reported flume water volume and streambed area (Table S2)
When applied to previously published measurements of bedform pumping in a recirculating flume (Elliott & Brooks, 1997a), we find that both analytical frameworks closely reproduce average patterns and rates of hyporheic exchange, provided that the 1D diffusion model's diffusivity declines exponentially with depth
Summary
The movement of water into and out of the hyporheic zone, or “hyporheic exchange,” occurs over a wide range of spatial (and temporal) scales, from >10 km (>1 year) to
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