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 Levee formation by deposition from sediment-laden flows debouching into open waters has been conceptually and analytically linked to jet hydrodynamics since the middle of the 20th century. Despite this long-standing association between jets and levees, the morphodynamics controlling subaqueous levee development remain largely unquantified and poorly understood. Here we report the results of physical experiments on subaqueous levee development modeled on floodplain tie channel processes. In the laboratory, we created subaqueous levees from a sediment-laden jet entering a basin of still water. Levee formation occurred where the local shear velocity of the jet declined below the critical shear velocity for entrainment of sediment into suspension. The rate of levee deposition depended on the rate of lateral sediment transfer to the jet margins and the settling velocity of suspended sediment. In our friction-dominated flows, lateral sediment flux to the levees was primarily due to dispersive lateral transport driven by turbulence. High rates of sediment transfer from the jet core to the margins led to levee growth that outpaced deposition along the flow centerline. Under hypopycnal conditions, we failed to produce levees. We observed distinct differences in levee morphology due to changes in the size and density of suspended sediment under identical hydrodynamic conditions. Our experimental results and review of published data on hypopycnal river mouths suggest that suspended sediment characteristics, relative magnitude of bed friction, and channel outlet aspect ratios may have a more significant influence on river mouth morphology than the buoyancy of discharging waters as envisioned in existing conceptual models.
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 The formation of bounding levees by deposition from sediment-laden flows debouching into open water, and the resulting self channelization of these flows, is a fundamental geomorphological process that extends channel networks, builds deltas, and constructs sedimentary records in both lacustrine and coastal settings. In the middle of the last century, Bates  advanced the hydrodynamic analogy between debouching river effluent and the class of boundary layer flows known as jets. Relying on earlier observations [e.g., Leighly, 1934], Bates  hypothesized that levees should form on the margins of outflowing jets along “the threads of maximum turbulence.” Since then, the specifics of Bates  hypotheses regarding the characteristics of jets (axial versus plane) and resulting delta morphologies have been extensively discussed and the relative importance of inertia, density, friction and river outlet aspect ratio debated [Crickmay, 1955; Jopling, 1963; Axelsson, 1967; Kashiwamura and Yoshida, 1967; Wright and Coleman, 1974; Wright, 1977; Wellner et al., 2005]. Wright  presented conceptual models to relate river mouth morphologies to outflow hydrodynamics that remain in common use today [e.g., Bridge, 2003]. Specifically, Wright  suggested that flows in contact with the bed would be friction dominated, spread rapidly and therefore have rapidly diverging levees and prominent mouth bars. Buoyant outflows, in contrast, should be detached from the bed and subject to convergent secondary circulation near the bed which would produce narrow, parallel levees with straighter, longer channels that bifurcate less frequently than channels in frictional settings [Wright, 1977].
 To quantify the morphodynamics of levee formation by sediment-laden jets, we conducted scaled laboratory experiments modeled after of a class of floodplain channel that build into lakes known as “tie channels” (Figure 1). Tie channels are secondary channels that “tie” or link floodplain lakes to the main stem river and allow bidirectional flow to exchange between river and lake depending on the relative lake and river stages [Blake and Ollier, 1971; Dietrich et al., 1999]. These channels convey significant fractions of water and sediment from the main stem into lakes and the floodplain settings bordering the channels [Day et al., 2008, 2009]. Tie channels are characteristically narrow (width to depth ratio ∼5), single threaded (few channels exhibit bifurcations) and nonmeandering. Tie channels progressively extend into lakes through levee building and progradation [Rowland et al., 2009a].
 Tie channels possess a number of characteristics that make them a favorable prototype for the study of channel levee formation at the outlet of a river or stream into an open body of water. These channels form and prograde into floodplain lakes free of waves, tides and littoral currents which all modify depositional morphologies in coastal settings. Tie channels, additionally, are characterized by high flow velocities and boundary shear stresses that create a jet which transports sediment largely in suspension [Rowland et al., 2009a] limiting the influence of bed load sediment transport mechanics. Our modeling focused on the subaqueous deposition of sediment basinward of the channel outlet that is responsible for the initiation of levees and the advancement channels into receiving basins. Field data suggests that bidirectional flow through tie channels is critical for channel maintenance, once formed, but has limited influence on initial levee development or the subaqueous channel morphologies [Rowland et al., 2009a]; therefore, our experiments only explored the dynamics of unidirectional flows.
 We premised our initial experiments on the hypothesis that the suspension of sediment in a fully turbulent jet would be the critical condition necessary for levee formation. Given the ubiquitous occurrence of leveed self-formed channels in a wide range of natural settings, we were surprised by repeated failures to form levees in experiments with silica-based sediments, ranging in size from clay to medium sand and with size distributions ranging from homogeneous sized glass spheres to mixtures of sand, silt and clay. In all cases, sediment deposition from the jet was at a maximum along the core of the jet, rapidly outpacing deposition along the margins of the outflow; a condition antithetical to the development of bounding lateral deposits and eventual self channelization [Imran et al., 1998]. Preliminary tests using low-density ground walnuts shells led to the abandonment of silica-based sediments in favor of lower-density ground plastic particles (specific gravity 1.5 versus 2.65). When introduced into a turbulent jet these plastic sediments were suspendable at experimental velocities, rapidly deposited along the quiescent margins of the jet, but most importantly were readily reentrained into the flow along the high-velocity core of the jet.
 These observations led to revision of our working hypotheses for levee formation to include both conditions of sediment suspension and a distribution of boundary shear stresses that allows for greater net deposition to occur along the outflow margins than along the center. Since both the suspension and entrainment of sediment into suspension depend on the properties of the sediment, such as size, density and shape, we further hypothesized that sediments of different densities and sizes would likely lead to different depositional patterns under identical flow conditions.
 The majority of this paper presents the results from experiments with concurrent measurements of hydrodynamics, suspended sediments distributions, and morphologies. Based on these results we explore the relationship between bottom boundary shear stress distributions and levee development and quantify the relative contributions of advective versus dispersive sediment transport mechanics on levee deposition. From these results and observations of longer-duration experiments we explore the potential competition between levee development and mouth bar formation and its implications for channel bifurcation. Finally, based the morphological results of these experiments, our exploration of buoyant jets, and field observations of natural tie channels we undertake a reevaluation of the published data underlying the hypopycnal model for river mouth morphologies [Wright, 1977].
2. Experimental Setup
 We conducted our experiments in a basin with horizontal dimensions of 8 m × 3 m and a maximum depth of 0.6 m (Figure 2). An acrylic bed 2.4 m wide × 3.7 m long, supported by an adjustable aluminum frame, was submerged in the basin. A constant head tank supplied flow to the basin via 7.6 cm diameter pipe connected to a 0.54 m × 0.50 m stilling box. Flow exited the stilling box and entered the basin through a flow straightener that passed into a 1 m long outlet channel connected to the adjustable acrylic bed. At the opposite end of the basin, a pair of 7.6 cm diameter siphons extracted water to a sump where a pair of pumps recirculated the water back to the head tank. The siphons discharged water into the sump through a head cylinder mounted on a computer controlled linear positioner. Raising and lowering the head cylinder controlled both the flow rate through the siphons and the elevation of the water in the basin. Sustainable inflow rates to the basin ranged from 0.1 L/s to 10 L/s. Outflow rates achieved by the siphons fell within a similar range.
 A composite screw feeder fed sediment into a standpipe tapped vertically into the main water line to the basin 2 m downstream of the head tank and 4 m upstream of the entrance box to the basin. Sediment feed rates could be varied from less than 1 g/s to 10 g/s. Sediment was entirely trapped within the basin and not recirculated.
 Over the course of our investigations into levee formation, we explored the influence of a range of entrance channel and basin slope configurations and sediment types and sizes. The majority of this paper, however, focuses primarily on one set of experiments conducted with a horizontal bed submerged by 5 cm of standing water. In this setup, the 1 m long entrance channel conveying flow into the basin partially confined the inflow. At the discharge point from the flow straightener the channel was 22 cm wide and the walls were 4 cm high (1 cm below the standing water height in the basin) (Figure 2c). Along the length of the channel, the sidewalls decreased in elevation to merge with the acrylic bed 1 m from the entrance to the basin. Over the same reach, the sidewall separation distance uniformly increased to 25.5 cm at the junction with the acrylic bed. This configuration was designed to simulate outlet conditions of our natural prototype channels in which the transition from full confinement to complete unconfinement typically occurs gradually as bounding levees progressively decrease in height and widen [Rowland and Dietrich, 2006; Rowland et al., 2009b].
 We conducted experiments with three different mixtures of plastic particles. Two of the plastics were composed of Type II urea for which the manufacturer reported a specific gravity of 1.47 to 1.52 and the third plastic was composed of acrylic with a specific gravity ranging from 1.1 to 1.2. We directly measured the settling velocity distributions using settling columns. These results are graphically presented in Figure 3; the median settling velocities were 1.9 and 2.6 cm/s for the two size distributions of urea and 1.0 cm/s for the acrylic. Based on the relationships determined by Dietrich , we calculated median grain diameters of 0.38 mm and 0.48 mm for the urea distributions and 0.41 mm for the acrylic. The three sediments will be referred to by the estimated median grain diameter/specific gravity for the remainder of this paper: 0.38/1.5, 0.48/1.5 and 0.41/1.2.
 The width of tie channels for a range of river systems has been observed to vary at their outlets into lakes from 10 to 50 m; however these channels are characteristically narrow relative to their depth with a mean width to depth ratio of about 5 [Rowland et al., 2009a]. Tie channels have high flow velocities and boundary shear stresses (relative to the stresses needed for initial motion criteria for their sediment load) and transport their sediment load in suspension [Day et al., 2008; Rowland et al., 2009a]. Based on the available field data, our primary scaling objectives were to approximate the aspect ratio observed at tie channel outlets and achieve suspended sediment conditions. The first scaling objective was motivated by the hypothesis that the relative balance of bed friction to lateral shear generated along the margins of the flow would influence jet hydrodynamics and hence sediment deposition. The motivation for the latter objective was the hypothesis that depositional levees form primarily from sediment deposited out of suspension onto the margins of the flow. Given these scaling objectives, outlet velocity and hence discharge were set by the flow conditions needed to achieve sediment suspension. Table 1 presents a comparison of prototype tie channel characteristics to those modeled in the flume. Despite similar aspect ratios, the experimental tie channel geometry was approximately rectangular compared to the distinctly “V”-shaped geometry observed in the field [Rowland et al., 2009a]. We did not quantify the effect of this variation in outlet geometry on flow dynamics.
Table 1. Comparison of Prototype and Model Scalinga
Here g is the acceleration due to gravity, ν is the kinematic viscosity of water, u* is the shear velocity, and Ws is the sediment settling velocity.
Outlet Width (Bo)
Outlet Depth (Ho)
Outlet Velocity (Uo)
Outlet Discharge (Qw)
Froude Number ()
Reynolds Number (UoHo/v)
2.8 × 104
 Mass concentrations of suspended sediment were set to values comparable to natural tie channels (200–800 mg/L [Rowland et al., 2009a]) to avoid introducing unrepresentative density effects into the experimental flows. Due to the lower density of plastic, experimental volumetric concentrations exceed those of natural systems by about a factor of two. In order to compare volumetric deposition rates between runs with sediment of differing densities, we ran each experiment with a volumetric concentration of 4.2 × 10−4 which is equivalent to 630 and 490 mg/L for the urea and acrylic sediments, respectively.
 Scaling the experiments based on a suspension criterion where the shear velocity exceeds the particle settling velocity (u*/Ws > 1) [Bagnold, 1966] failed to produce levee deposition using a broad range of sediment sizes and flow conditions. The success of lower-density particles in producing levees highlighted the need for an additional scaling criterion based on the threshold for entrainment of sediment from the bed into suspension. This suspension threshold differs from an initial motion threshold of particle movement along the bed [Shields, 1936] and has been quantified in the experimental work of Niño et al. .
Niño et al.  conducted a series of experiments and developed empirical criteria to predict the thresholds for sediment entrainment into suspension based on the shear velocity of the flow and a dimensionless particle diameter
where R is the submerged specific density defined by R = (ρs − ρ)/ρ and ρ and ρs are the density of water and the sediment, respectively, g is the acceleration due to gravity, dp is the representative median particle diameter, and ν is the kinematic viscosity of water. Niño et al.  found that for a bed covered with particles the same size as those in suspension the threshold or critical shear velocity for entrainment to settling velocity ratio was
while on a bed that was 80 to 85% free of sediment (termed smooth)
Values for Rp and u*ce calculated for both equations (2) and (3) are presented in Table 2. A plot with experimental and estimated field values of u*/Ws along with Niño et al.’s  threshold values of for entrainment into suspension is presented in Figure 4.
Table 2. Entrainment Scaling for Experimental Sedimentsa
Here Rp is the dimensionless particle number (equation (1)).
4. Data Collection Methods
 Data collection varied with our three primary experimental conditions: (1) early phase of levee development, (2) longer-term evolution of levees, and (3) buoyant jet test. Data collection for the early phase study included measuring flow velocities and turbulent characteristics, suspended sediment distributions, and levee morphology. These measurements could not be done simultaneously, however, because our instruments were too large and we had to measure the bed topography subaerially. We measured the velocity and turbulent structure of the flow under steady conditions, absent sediment. Following velocity profiling, suspended sediment concentration profiles were collected only over the first minute of sediment transport into the basin to minimize the effects of sediment deposition on the flow field. Finally, the experiment was run for 20 min with constant water and sediment discharge to allow sufficient deposition for topographic surveying. As a consequence of these experimental limitations our velocity and suspended sediment data record only the initial characteristics controlling levee formation. Evolution of either the flow field or suspended sediment distributions in response to developing levees could not be quantitatively assessed but continuous video of the experiments allowed qualitative characterizations.
 Data collection during the long duration and buoyant inflow experiments included overhead video, still photography, and topographic surveys of the resulting deposits. We also documented the vertical structure of the buoyant inflow from the side using a high-speed video camera submerged beneath the water surface within a watertight acrylic box.
4.1. Velocity Measurements
 We recorded flow velocity in three dimensions for a period of 120 s at each sampling location at an output frequency of 25 Hz using a side-looking Nortek Vectrino Acoustic Doppler Velocimeter (ADV). The ADV probe was affixed to a point gage mounted to an aluminum frame spanning the basin. The point gage had a minimum increment of vertical motion of 0.3 mm. We collected vertical velocity profiles every 2 cm across half of the jet beginning 2 cm beyond the midline of the flume bed (the inferred jet centerline) out to margin of the jet, ending where flow velocities and turbulence became too intermittent to be reliably measured. The cross sectional profiles were conducted at 14 cm spacing down the jet at distances between 76 cm and 300 cm downstream of the channel outlet. Each vertical profile consisted of measurements at 0.8, 1.02, 1.32, 2.78, and 4.25 cm above the mean bed elevation. The height of these sampling intervals relative to the total flow depth (H = 5 cm) were 0.16, 0.21, 0.26, 0.56, and 0.85. Detailed descriptions of ADV data processing and analysis were presented by Rowland et al. [2009b].
4.2. Suspended Sediment Measurements
 We measured the spatial distribution of suspended sediment concentrations for a flow with the 0.38/1.5 sediment in suspension. Similar to the velocity measurements, concentrations were recorded over half of the experimental flow, but at approximately half the total number of cross sections with measurements at: 76, 104, 132, 160, 174, 188, 216, 244, 272, and 300 cm downstream of the channel outlet. These concentration measurements were derived from high-speed digital video imagery of sediment particles illuminated by an infrared laser across 6 cm wide windows oriented orthogonal to the flume centerline. A 500 mW infrared laser, mounted on the aluminum instrument frame, vertically projected a sheet of light through a clear acrylic window and into the flow. The acrylic window served to remove surface waves and prevent distortion of the light sheet passing into the flow. The video camera, enclosed in a clear acrylic box, was immersed in the flow 30 cm downstream of the laser sheet. At each 6 cm wide window, the flow was imaged with a resolution of 0.138 mm per pixel at a rate of 10 frames/s for 1 min. The laser and camera were then stepped 4 cm laterally and another sequence of images recorded.
 To determine suspended sediment concentrations, the mean intensity recorded in each image pixel over the course of 1 min was calculated and then averaged across windows 2 cm wide and 0.4 cm high. These intensities were converted to suspended sediment concentrations using an intensity-sediment concentration calibration relationship determined from siphon samples of suspended sediment. To maintain a flow field identical to the sediment-free one measured with the ADV, we swept all sediment from the bed prior to recording each image sequence. Additional details regarding instrumentation setup, data collection and image calibration are given by Rowland .
4.3. Bed Topography Measurements
 We surveyed the depositional morphology associated with each experimental run using a Single-Lens Reflex (SLR) 35 mm digital camera and a 40 mW laser sheet. The laser sheet was projected vertically onto the bed such that the intersection of the laser sheet with the flume bed generated a line. The location of this line relative to an arbitrary but fixed reference frame was recorded in successive digital images of the bed. On a flat bed, the laser line occupied a set of parallel rows in the digital image. Variations in the bed topography resulted in a deflection of the laser line to higher or lower rows in the digital image. The location and magnitude of these variations were determined by digitally extracting the pixel locations of the line from the photographs. Based on a calibrated reference matrix, each pixel containing the laser line was assigned a horizontal and vertical location. By collecting a sequence of images at regular intervals along the flume, a complete survey of the bed was performed.
 The camera-laser setup we used surveyed a 114 cm wide section of the bed with pixel resolutions of 0.38 mm and 0.43 mm horizontally and vertically, respectively. The images were collected at 2 cm intervals down flume from 98 to 326 cm downstream of the channel outlet. Based on analysis of duplicate surveys, the system accurately determined elevation differences as small as 0.65 mm with a standard deviation of 0.11 mm.
 Bed elevations of the bare flume bed were subtracted from the topographic surveys to construct contour maps of the total deposition. Localized variations in bed deflections between runs resulted in deposit thickness measurement errors of approximately 1 mm. A complete description of the camera-laser setup and the methodology was presented by Rowland .
5. Experimental Results
5.1. Levee Development
 In all experimental runs, our jet developed a large-scale (width on the order of the jet width) meandering instability beginning less than a meter from the outlet into the basin. The amplitude of the meandering increased with distance into the basin. This meandering arises from a hydrodynamic instability driven by the shear along the margins of the outflow [Jirka, 2001; Socolofsky and Jirka, 2004]. Aerial photographs and satellite images of tie channel flow into lakes shows that a similar meandering instability is common in these natural systems (Figure 1a). Literature reports [Giger et al., 1991; Jirka, 1994] and aerial photos indicate that these large-scale turbulent features also occur in coastal settings where tidal inlets create jets into the ocean. Despite the meandering of the jet core and its visible influence on the trajectory of individual sediment particles, sedimentation along the margins of these experimental jets resulted in continuous linear deposits that appeared to reflect the time-averaged hydrodynamics of the jet rather than the persistent, but spatially transient meander.
 Subaqueous levee development over the course of a 20 min run is depicted in Figure 5. In this run, the experimental sediment was the 0.38/1.5 particles and the flume setup was as shown in Figure 2. Levee formation began immediately following introduction of sediment into the basin. In the first minute, levees began to develop between 100 and 200 cm downstream of channel outlet to the basin. Sediment traveled widely dispersed in the flow but locally clear patterns of transient sediment deposition and resuspension were observed in association with the passage of the meandering large-scale turbulence (the meander is visible in the trail of surface bubbles in Figure 5, also see Figure 1 and Rowland et al.’s [2009b] associated online video). Over time, the levees grew in height and progressively extended down the basin. The inner levee margins advanced inward toward the jet centerline as the levees captured more sediment (visible at distances greater than 200 cm (5 grid squares) from the outlet in Figure 5). This process occurred in an intermittent fashion as sediment stalled along the toe of the levee only to have a portion of the newly deposited sediment carried downstream by the passage of the meandering jet core. After extending down jet to 300 cm from the outlet, the inner margins formed a straight “channel” of uniform width along the centerline of the jet. The final levee morphology of this experimental run along with the morphologies of runs using the 0.48/1.5 and 0.41/1.2 sediment distributions are presented in Figure 6.
 In contrast to the short-duration experiments detailed above, we ran a set of experiments for a cumulative duration of 350 min to document the continued evolution of subaqueous levees. In this series of experiments, flow entered the basin from a straight walled entrance channel that abruptly transitioned into the basin. The basin floor sloped away from the entrance with a gradient of 0.03 and the sediment used was also the 0.38/1.5 urea-based particles. The experiment was run in ∼30 min intervals. Flow rate and sediment feed were held constant for the entire run but the water level in the basin was allowed to slowly rise to simulate the progressive infilling of a lake. This cycle of basin infilling was repeated over each experimental interval. Between experimental runs we sprayed a clay-silt mixture onto the subaerial levees and allowed it to dry. This procedure created interlayered deposits of plastic and mud that only eroded along the levee toes leading to near vertical inner banks but protected the levee crests from erosion. In the absence of bank cohesion, variations in the flow field associated with the rise and fall of the basin waters led to significant erosion of the developing levees.
 In these experiments, the rate of growth in levee height was initial rapid and then slowed with time (Figure 7). The levee growth largely ceased after reaching a relatively stable height that was approximately 3/4 of the mean water depth. Initially, no deposition occurred along the centerline of the flume, however, over time centerline deposition increased as levee growth slowed (Figure 7).
 In a separate set of experiments we explored the influence of buoyancy on the morphodynamics of a sediment-laden discharge. These experiments were conducted as a complement to a series of experiments exploring the morphodynamics of sediment-laden density currents [Rowland et al., 2010]. In these experiments flow was introduced into the basin through a slot 20 cm wide and 2 cm high. The basin floor sloped away from the outlet with a gradient of 0.006 and the basin water depth at the outlet was 2 cm. An inflow of fresh water (ρ = 1000 g/cm3) carrying the 0.41/1.2 sediment particles was introduced into a basin containing water with a density of 1016 g/cm3. The higher-density basin waters resulted from the mixing of dense inflows into a basin of fresh water. We generated the higher-density fluid by mixing table salt with tap water and measured the fluid density using a hydrometer demarcated every 2 g/cm3. As expressed as a density ratio (γ = 1 − ρf/ρs, where ρf and ρs are the fluid densities of the outflow and receiving water, respectively) the density contrast in our experiment had a value of 0.016. While somewhat arbitrarily selected, this ratio does fall within the 0.0109 to 0.0168 range of density ratios Wright and Coleman  reported for ebb and flood discharge conditions at the South Pass of the Mississippi River delta, the field location that served as the prototype for the conceptual hypopycnal model for river mouths [Wright, 1977].
 Using this experimental setup, we ran a “baseline” experiment in which in the inflow and receiving water densities were equal (excluding minor influence of the low-density sediment particles in suspension). The baseline experimental configuration resulted in distinct subaqueous levees similar to those observed in our other experiments (Figure 8a). The buoyant inflow, however, resulted in nascent levee formation only over the first 15 cm of the bed downstream of the outlet (Figure 8b). Downstream of this region, the buoyant outflow spread laterally near the water surface and sediment accumulated across the width of the flow with maximum deposit thicknesses occurring under the center of the outflow. Side-looking video beneath the water surface revealed that with increasing lateral spreading, the inflow separated from the flume bed and sediment deposited on the bed was not reentrained back into the flow.
Section 5.2 presents the detailed hydrodynamic data, suspended sediment profiling, and morphological data conducted in the series of experiments designed to quantify the initial morphodynamic controls on subaqueous levee formation.
 Detailed analysis of the hydrodynamics of our experimental flows was presented by Rowland et al. [2009b], therefore, here we limit our focus to the velocity and turbulent characteristics relevant to understanding the controls on levee formation.
5.2.1. Time-Averaged Velocity Structure
 The time-averaged velocity structure of our experimental jet (Figure 9) may be divided into two general regions that correspond to the standard jet classifications of a Zone of Flow Establishment (ZOFE) and a Zone of Established Flow (ZOEF) [Bates, 1953]. In the ZOEF of our jet, distances >190 cm or 8.5 channel widths downstream of the outlet from the stilling box, the time-averaged velocity structure of the flow was consistent with that previously reported for experimental plane (two-dimensional) jets [Albertson et al., 1950; Bates, 1953; Schlichting, 1968; Tennekes and Lumley, 1972]. In this region, the normalized centerline velocity in our jet decreased with a −1/2 dependence with distance such that
where c is the local streamwise velocity on the centerline, ois the streamwise velocity at the outlet (the overbars indicate time averaging), x is distance from the outlet in the streamwise direction, and B is the outlet width. In this region, the cross-stream distribution of the streamwise velocity exhibited a self-similar distribution with downstream distance characterized by a normal or Gaussian lateral distribution
where (y) is the streamwise velocity at any cross-stream location y, and η = y/b(x). b(x) is the cross-stream location where (y) = 1/2 c (the velocity half-width).
 In contrast to the ZOEF, across the ZOFE of our jet (measured from 76 to 190 cm downstream of the outlet), the centerline velocity decreased with a −1/6 dependence with distance. In this region of the jet, the cross-stream distribution of streamwise velocities deviated from a Gaussian distribution, exhibiting less of a lateral decrease in magnitude than would be predicted by equation (5) in the jet core. Because of the lack of reported data from other experimental jets in the ZOFE, we cannot determine how unique the velocity decay rate and cross-stream structure were to our particular experimental setup.
 The magnitude of the measured time-averaged cross-stream velocity rarely exceeded 5% of the local streamwise velocity. On the distal edges of the jet (only captured to a downstream distance of 174 cm in Figure 9), however, where still basin waters were entrained into the jet, the time-averaged cross-stream velocity ranged from 25 to 45% the local time-averaged streamwise velocity and was directed inward toward the jet core.
5.2.2. Turbulence Structure
 In a separate paper, we performed detailed analysis of the turbulence characteristics of our experimental jet absent suspended sediment [Rowland et al., 2009b]. Here we summarize the main findings of that paper and report new data of relevance to sediment transport and levee formation. Rowland et al. [2009b] found that a key control on turbulence intensities and lateral momentum transfer across the jet was the generation of a meandering instability in the jet, a feature also observed in natural tie channels [Rowland et al., 2009a, 2009b]. Although the large-scale quasiperiodic meandering turbulent structure had limited influence on the time-averaged structure of the jet, Rowland et al. [2009b] found that it dominated turbulence characteristics.
Figure 10 shows 20 s of velocity time series of the streamwise and cross-stream velocity components at the transition from the jet core to the margin (20 cm from the centerline) at a location 160 cm downstream of the flow outlet. At this location, the time-averaged cross-stream velocity was −0.01 m/s (minus indicating flow away from the jet centerline toward the margin), however, the instantaneous cross-stream velocity ranged from +0.09 to −0.14 m/s. The streamwise velocity ranged from 0.06 to 0.32 m/s about a time-averaged value of 0.17 m/s. Also visible in Figure 10 is a distinct asymmetry in the cross-stream velocity with the magnitude of outward directed velocities exceeding inward directed ones. Outward velocities on average exceeded inward velocities by a factor of 1.35 over the complete 2 min time series at this location. The negative excursions in the cross-stream velocities also corresponded to the highest streamwise velocities, highlighting the association between outward directed turbulence bursts with the periodic passage of the large-scale meander. At this sampling location, outward directed velocity excursions persisted for ∼2 s; the duration of this time scale increased downjet as the jet widened and the size of the meandering structure increased [Rowland, 2007].
5.2.3. Bottom Boundary Shear Stress Distributions
Rowland et al. [2009b] showed that the vertical profiles of streamwise velocity exhibited a log linear dependence on flow depth (increasing in magnitude with distance from the bed) out to a distance of ∼190 cm from the channel outlet. Beyond that distance, the vertical distribution of velocity became more uniform with depth. Over the same region of the jet, the vertical distributions of Reynolds stresses exhibited a linear distribution with depth (increasing with proximity to the bed), but no clear vertical structure was recorded across the margins (lateral distances > 10 cm from the centerline) or downstream of 190 cm. This suggests that in the ZOFE, the vertical distribution of velocity and bottom boundary shear stresses were similar to those typically observed in open channel flow.
 In regions of the flow with log linear vertical streamwise velocity profiles we estimated the shear stresses at the bottom boundary (τbx) from the friction or shear velocity (u*) [Tennekes and Lumley, 1972]
that is in turn related to the vertical distribution of time-averaged streamwise velocity by the following:
where (z) is the streamwise velocity at depth z, zo is a roughness height, and k is the von Karman constant (taken to be 0.40). In the regions of the experimental jet exhibiting log linear velocity profiles it is possible to use equations (6) and (7) to calculate bottom boundary streamwise shear stresses. However, across the remaining portions of the flow (locations downstream of 190 cm from the outlet and across the flow margins) this approach fails to yield meaningful estimates for u* since u is not a function of z over the portion of the flow depth that we were able to record velocity (z/H ≥ 0.16).
 A commonly adopted approach for estimating bottom boundary shear stresses is to use a quadratic relationship between the depth- and time-averaged streamwise velocity and a nondimensional friction coefficient (Cd)
Estimates of jet-wide distributions of using equation (8) showed extremely poor agreement with sediment deposition patterns (i.e., large portions of the basin without deposition were in regions with predicted u* << u*ce). We attributed this disagreement to the influence of the large-scale meandering structure that is not accounted for in equation (8). In order to capture the potential influence of the meandering structure on , we adopted an approach to quantify the resultant magnitude of that includes the influence of both the time-averaged streamwise and cross-stream components of the horizontal flow vector and a measure of the influence of the meandering structure on the near bed turbulence. Conceptually this approach is similar to the approach used by Grant and Madsen  to determine instantaneous boundary shear stress in wave-influenced settings that incorporated both the mean current velocity and wave velocity fields in the formulation of the quadratic friction law. We incorporated the influence of the meander-driven cross-stream velocity excursions on by using both the depth- (capital letters) and time-averaged (indicated by overbars) horizontal velocity components ( and ) and the depth-averaged fluctuating velocity components (U′ (t)and V′ (t)), such that
Rather than calculating equation (10) for each individual velocity measurement (25 s−1 for each 2 min time series) and then averaging, we replaced the U′ (t) and V′ (t) terms in equation (10) with the root mean square values (rms) for U′ (t) and V′ (t) such that equation (10) was estimated in the following manner:
In the region of the flow field that exhibited log linear velocity profiles, equations (6) and (7) were used to calculate the bottom stress. Equating that result with equation (11) defines a drag coefficient (Cd = 0.0016 +/− 0.00019), which we assumed to be applicable over the entire flow domain. This drag coefficient and equation (11) were used to calculate shear velocities across the entire flow domain (Figure 11).
 At an individual downstream cross section, u* magnitudes were relatively constant out to a lateral distance of 10 cm followed by a rapid decrease across the jet margins. At a lateral distance of 12 cm from the centerline, u* values were relatively constant at all downstream cross sections. This location also marks a transition in the downstream trend in u* between the jet core and margin. At lateral distances < 12 cm from the centerline there was a steady decrease in u* with distance from the channel outlet. In contrast, at distances > 12 cm u* steadily increased with distance downstream.
5.3. Suspended Sediment Distributions
 We measured the distribution of suspended sediment using the 0.38/1.5 sediment in flow field identical to that presented in the preceding sections. Suspended sediment entered the experimental basin from the stilling box with an approximately uniform spatial distribution and a time-averaged concentration of the 630 mg/L. By the first measurement cross section 76 cm downstream of the outlet, the time-averaged suspended sediment distribution established a strong vertical gradient (Figure 12) and began to disperse laterally to the jet margins (Figure 13). With distance from the outlet the concentration of suspended sediment steadily decreased in the core of the jet while maintaining a relative constant time-averaged vertical structure. The downstream decrease in suspended sediment concentrations was also reflected in the decrease in the mass flux of suspended sediment at each measurement section (Figure 14).
 The downstream increases in sediment mass flux from 76 cm to 104 and 132 cm (Figure 14) were mostly likely related to the temporary deposition and subsequent resuspension of sediment along the inside margins of the entrance channel. We lack a clear explanation for the drop in sediment concentrations and total flux observed at the 188 cm measurement section.
 Similar to the time-averaged velocity structure of the jet, the time-averaged suspended sediment distributions do not capture the short time scale dynamics associated with the large-scale meandering turbulence and its influence on sediment transport. Within the meandering portion of the jet, the trajectory of suspended sediment closely matched the instantaneous flow pattern with sediment particles traveling back and forth across the core region of the jet and exiting the core along with detached vortices (Figure 5). For the 0.38/1.5 and 0.48/1.5 sediments the time scale for the sediment to fall through the water column (H/Ws) and deposit on the bed was equal to or less than the duration that the large-scale turbulent structures persisted on the jet margins [Rowland, 2007]. Therefore, by the time the fluid in these vortices was reentrained back into the core of the jet the majority of the sediment had been removed from suspension. For the 0.41/1.2 sediments, the settling time scale was typically greater than the persistence time scale for large-scale turbulent structures on the margins.
5.4. Levee Morphology
 Three separate experimental runs were conducted to document the depositional morphology associated with each of the three experimental sediments: 0.38/1.5, 0.48/1.5 and 0.41/1.2. The results of these runs are depicted in Figures 6 and 15. Increasing the settling velocity of the sediment in suspension (from 1.0 to 1.9 to 2.6 cm/s) resulted in decreases in three planform morphological levee attributes: (1) the width of the individual levees, (2) the distance between the paired levees (across the jet core), and (3) divergence angle (downstream increase in distance between levees) of the two levees crests. In general, the rate of change in the lateral positions of the levee crestlines was less than the spreading rate of the velocity half width (b(x)) [Rowland et al., 2009b]. The levees composed of the higher settling velocity particles (1.9 and 2.6 cm/s) reach peak elevations between 154 and 176 cm downstream of the outlet, whereas the levees composed of 0.41/1.2 (1 cm/s) sediment continue to grow in height with downstream distance. We observed that for both the 0.41/1.2 and the 0.38/1.5 sediments, the maximum lateral extent of sediment dispersal corresponded to the location of the jet margin, while the 0.48/1.5 sediments did not reach the outer jet margins.
 Comparison of levee cross sections for each of the sediment types highlight three morphological trends of the deposits (Figure 15): (1) the 0.38/1.5 and the 0.48/1.5 sediments both have well defined crests and steep inner margins, (2) locations of the crests and inner margins of the levees fall further from the flume centerline as the settling velocity of sediments decreases, and (3) both the 0.38/1.5 and 0.41/1.2 sediments have the same maximum lateral extent of deposition, which is greater than of the 0.48/1.5 levees.
6. Spatial Variations in Sediment Transport Mechanics
6.1. Entrainment Into Suspension
 Comparison of the distribution of u* with the observed bed topography indicates that the levees developed in regions where u* < u*ce (Figure 16). The inner margin of the 0.48/1.5 sediment (Figure 16b) corresponded to the location of the u*ce as determined for a sediment-covered bed (equation (2)), while the margin of the 0.41/1.2 sediments fell on the u*ce value for a largely sediment-free bed (equation (3)). The inner margin of the 0.38/1.5 deposit corresponded to sediment-free conditions to a downstream distance of 180 cm and was located between the two u*ce estimates (Table 2) downstream of this point. The results suggest that for our experiments the critical shear velocities for entrainment into suspension presented by Niño et al.  provided a good predictor for the spatial patterns of levee deposition.
 The discrepancies between the location of u*ce and the observed levee margins likely resulted from uncertainties in the estimation of u*ce due to imprecision in the determination of grain diameters and density (section 3) and the simplifying assumptions in calculating u* (section 5.2.3). Additionally, levee boundaries after 20 min of deposition may not have had the same hydrodynamic conditions captured under sediment-free conditions. Ongoing deposition likely altered the flow field locally and changed the roughness of the bed. The latter effect may account for the variation in which estimate of u*ce (equation (2) versus (3)) was most appropriate between runs with the 0.48/1.5 sediment (significant levee deposition) and 0.41/1.2 sediment (thin levee deposition).
6.2. Mechanics of Sediment Transport at the Margins
 Spatial patterns of u*ce appear to have controlled the location of the inner levee margins. The rate of levee development, however, should have been controlled by the combined rates of lateral sediment transfer to the margins and deposition on the bed at the margins. To quantify the mechanics of the lateral transfer of sediment at the margins we combined the data on the distribution and magnitudes of suspended sediment with the velocity and turbulence data. Here, we used a time- and depth-averaged formulation for the advection and lateral diffusion of sediment (modified from Parker et al.  and van Rijn ) to explore the controls on sediment transport at the margins of our experimental jet
where x, and y denote the streamwise, and cross-stream coordinate directions; t time; , , and the time-averaged values of u, v, and C; Fs represents the flux of sediment resuspended from the bed; and kysed is the lateral dispersivity of sediment. kysed = βky, where ky is the lateral diffusivity of momentum, also referred to as the eddy viscosity, and β is a constant to account for increased dispersivity of sediment relative to momentum. We calculated the lateral diffusivity of momentum from the measured values of lateral shear stress (τuv = −ρ) and the lateral gradient in the time-averaged streamwise velocity (∂/∂y) such that
 Because levee development appears to reflect time-averaged sediment transport, and we cannot calculate equation (12) for intervals less than 120s (due to the point by point collection of velocity data), we apply equation (12) using time- and depth-averaged values of velocity, sediment concentration and momentum diffusivity. Since the time-averaged value of the cross-stream velocity component () is approximately zero [Rowland et al., 2009b] the short time scale cross stream excursions in sediment transport are not captured in the time-averaged formulation, therefore we adjust β so that the influence of the meandering flow structure on sediment transport is represented as a dispersive process.
 To evaluate the control of advective sediment transport (terms two and three on the left had side of equation (12)) relative to dispersive sediment transport across the regions of levee development at the jet margins we make two simplifying assumptions. First we assume that at the margins on the short time scales of our measurements (∼1 min), the loss of sediment to the bed across the margin was balanced by the flux of sediment to the margin such that the sediment concentration was relatively steady and the first term in equation (12) may be approximated as zero. Second, given u* < u*ce at the jet margins (Section 6.1) we assume that the flux of sediment from the bed into the flow (Fs) was zero. Therefore, net deposition to the bed was equal to and total deposition rate (Dtot) may be calculated as
From the topographic survey of the bed we have a measure of the net deposition over the course of the 20 min experimental run. To compare observed and predicted deposition, we converted the mass fluxes (mg/L/s) obtained from equation (14) into deposit thickness (mm)
where 6.67 × 10−7 is the conversion factor from mass concentration to volumetric concentration, t is time (1200 s), H is total water column thickness (50 mm) and n is the deposit porosity that we assumed was 0.30.
Table 3. Relative Advective and Dispersive Contributions to Deposition on the Levee Crestsa
Cross Section Location (cm Downstream of Outlet)
Total Deposition (%)
Combined percentages of Dadv total and Ddis may not equal 100% due to rounding.
 The high β values arose in part from the relatively fast time scale for sediment to settle from suspension (H/ Ws) compared to the time scale for the meandering turbulence to change direction from outward to inward [Rowland, 2007]. Conservative tracers, such as temperature or dissolved solute, remain in the flow and experience the combined effect of both the outward and inward fluctuations in the cross stream velocity. In our experiment, a significant fraction of suspended sediment, however, settled to the bed over the course of a single outward or inward fluctuation. At the jet margins, where this sediment was not reentrained, much of the sediment only experienced the outward directed cross-stream velocity and thus did not experience the averaging effect of reversing cross-streamflow directions. For sediment with settling time scales significantly greater than the meandering time scale this effect should decrease. Under these conditions β values would be expected to decrease, potentially approaching previously reported values (∼2). In regions of the jet where sediment was readily reentrained we expect β values also to be less than those we predicted at the margins, rendering β values spatially variable across the jet.
 To quantify the relative roles of dispersive and advective sediment transport mechanics we separated equation (14) into its individual components
We further divided the advective components into streamwise (x) and cross-stream contributions (y)
The relative predicted deposition (in percent of the total) at the levee crests using equations (16), (18), and (19) for six cross sections is presented in Table 3. At the levee crests, our analysis suggests that between 70 and 100% of the deposition arose from the divergence in the lateral dispersive flux of sediment (equation (16)) with the relative contribution generally decreasing with distance downstream of the outlet.
 At upstream cross sections (160 and 174 cm) the ∂/∂y component of the lateral advective flux reduced (negative values) the net deposition to the bed. This resulted from inward directed flow (entrained into the jet from the basin waters), impinging on the levee and counteracting the outward diffusion of sediment. Further downstream, the total width of the jet increased while the inner levee margin and the levee crest positions remained approximately the same distance from the centerline. This change in jet width effectively separated the levee crests from the inward directed cross streamflow and removed its influence on levee deposition. Despite an increase in the lateral divergence of the horizontal velocity vectors with distance downstream (Figure 9) the role of jet spreading and flow divergence had a limited (<15%) influence on sediment transport across the jet margins and levee deposition.
7.1. Morphodynamic Competition Between Levee and Centerline Deposition
 In a sediment-laden jet entering a standing body of water where bed load and suspended bed material load play minor roles,(our experiments and natural tie channels) the deceleration and divergence of horizontal velocity vectors will not necessarily result in deposition of sediment onto the bed or stagnation of bed load transport. Instead the pattern of deposition will be set by the distribution of bottom boundary shear stresses above a critical value of sediment entrainment into suspension. The rate at which sediment is extracted from the core to the depositional zones at the margins will control the downstream flux of sediment in the debouching jet (Figure 14). If the rate of lateral sediment extraction is sufficient to extract the majority of sediment in the upstream reaches then little or no deposition will occur at downstream locations even where u* < u*ce. However, data from our longer-duration experiments (Figure 7) suggest that as the rate of lateral sediment extraction decreased in response to reduced levee development, deposition along the core of the jet increased and the bed became increasing alluviated. It is likely that even in systems where there is a strong interaction with the bed material load, the rate of lateral extraction of sediment to the flow margins will also influence the rate of centerline deposition.
 The results of our experiments combined with the modeling study of Edmonds and Slingerland  on mouth bar dynamics provide a number of insights into the potential coupled dynamics between levee and mouth bar development. In the results of Edmonds and Slingerland  there is a clear morphodynamic feedback between the developing mouth bar and the upstream levees. These simulations showed that as the mouth bar grew it deflected more of the flow around it and caused an increase in the divergence of horizontal flow vectors upstream of the bar. This flow divergence in turn resulted in a divergence of the tips of the developing levees around the growing mouth bar. We hypothesize, however, that levee growth may have an equally important morphodynamic feedback on mouth bar development through an evolution of the jet flow field.
 In our experiments we observed feedbacks between subaqueous levee development and the jet flow field (Figures 5 and 7). We, however, were unable to document the influence of subaerial levee development. In natural systems, variations in both river stage and receiving basin water levels allow levees to aggrade to elevations above all but the most extreme water surface elevations. The transition from confined to unconfined flow at the channel outlet results in a rapid dissipation of the water surface slope that drives flow and bottom boundary shear stresses in the channel upstream of the outlet [Bates, 1953; Rowland, 2007; Rowland et al., 2009b]. Subaerial emergence of developing levees allows this water surface slope to be reestablished and over time propagated further into the receiving basin. This flow confinement and reestablishment of a driving water surface slope should increase flow velocities and sediment transport potential down gradient of the initial jet outlet, across regions that were previously depositional.
 We propose that the relative rate that levees grow vertically and reconfine the flow compared to the rate at which mouth bars grow may be a critical factor in the length of channelized segments between bifurcation points. In systems where levee growth is slow relative to mouth bar growth, mouth bars may become stabilized (in the sense of Edmonds and Slingerland ) leading to levee divergence and bifurcation of the channel. However, in systems where levee growth and subaerial development outpace mouth bar deposition, high sediment extraction rates and flow reconfinement by the levees may greatly slow the growth of mouth bars and significantly delay or prevent bar stagnation and stabilization. Recent modeling by Edmonds and Slingerland  also suggests that the ability of levees to resist erosion, due to cohesiveness, may influence the dynamics controlling the relative rates of levee and mouth bar development. We argue that tie channels with limited mouth bar development and long single-thread (nonbifurcating) channels fall into a levee-dominated mode. Between two extremes of levee-dominated and mouth bar-dominated systems there is likely a spectrum of systems where there is a dynamical morphodynamic interaction between levees and mouth bar.
7.2. Reexamination of Existing Conceptual Models
 Both our field observations of tie channels and experimental results appear inconsistent with levee morphologies that would be predicted by the long-standing conceptual models of Wright . In these conceptual models, still in common use today, river mouth settings dominated by frictional processes at the bed are associated with rapidly divergent levees and prominent mouth bar growth. In contrast, channels with straight parallel banks, low width to depth ratios and infrequent bifurcations are associated with river mouth settings characterized by buoyant or hypopycnal outflows (ρf < ρs). In order to resolve the apparent contradiction between our results and these models, we compared our results to these models and revisited the data on which the hypopycnal model was originally based to examine the universality of the mechanistic explanations for the type-levee morphologies presented in the models.
 Our experiments did not vary the amount bed friction between experimental runs in a controlled manner so we are unable to examine directly the relative influence of bed friction on river mouth morphodynamics and levee morphology. The jets explored here, however, were clearly frictional in the sense of the Wright  models in that the flow remained in contact with the bed and the shear generated from the no-slip condition at the base of the flow strongly influenced the dynamics of the jet. The influence of bed friction on the jet hydrodynamics and momentum was quantified and discussed by Rowland et al. [2009b]. The morphological results of our experiments (Figure 6), however, show that under identical flow conditions, significant variations in levee morphology and divergence angles (from nearly parallel to widely divergent) arose from variations in the settling velocities and entrainment thresholds for the sediment in suspension alone. In multiple experiments, three of which are shown in Figures 6 and 8a, we produced narrow approximately parallel levees under frictional conditions with minimal density contrast between the discharging jet and receiving basin waters.
 Our field observations further appear to contradict the explicit coupling of levee morphologies to either frictional or buoyant settings. Tie channels exhibit straight, parallel banks (Figure 1) with even lower width to depth ratios (∼5) [Rowland et al., 2009a] than the Mississippi River distributary channels that served at the prototypes for the hypopycnal river mouths models (W/D = 22 to 33) [Wright and Coleman, 1971]. In terms of density contrast, tie channel discharge is either of equal density as the receiving lake waters (homopycnal) or slightly denser due the suspended sediment content of the inflowing waters (hyperpycnal) (for additional images of tie channels see Figure 1 of Rowland et al. [2009a]). In these natural settings well-developed levees form and extend great distances into their receiving lakes without bifurcating.
 Finally, under experimental hypopycnal flow conditions, the jet rapidly detached from the bed and the deposition along the centerline of the jet greatly exceeded deposition on the margins. The resulting morphology was bar like with limited levee deposition restricted to the zone in which the jet remained in contact with the bed.
 The South Pass of the Mississippi River delta which is characterized by long nearly parallel levees [Wright and Coleman, 1974] served as the basis for the hypopycnal conceptual model presented by Wright . The development of the observed levee morphology was inferred to arise from lateral flow convergence (from the margins to the center) beneath a debouching buoyant effluent. The flow convergence in turn restricted lateral divergence of sediment. This convergent flow was attributed to the combined influence of salt-water entrainment into the base of the discharging flow and the development of paired helical flow cells within effluent in response to buoyant spreading (outward at the water surface and inward near the bottom) [Wright and Coleman, 1974]. The model presents these hydrodynamic conditions as the typical if not dominant conditions prevailing at hypopycnal river mouth settings. The data from the South Pass presented by Wright and Coleman [1971, 1974] suggests, however, that near the channel outlet the relative roles of entrainment and buoyancy driven spreading varied significantly depending on the magnitude of river discharge.
 During flood stages, river discharge at the South Pass of the Mississippi River delta was strong enough to force the wedge of denser salt water out of the river channel and the discharging river flow remained in contact with the bed over most if not all of the region of subaqueous levee development [Wright and Coleman, 1974]. At low and normal river stages, when salt wedge intrusion forced a flow separation from the bed, the densimetric Froude numbers (,where h' is the depth to the density interface from the upper free surface) of the river effluent were typically < 1 (subcritical) and entrainment of salt water into the buoyant discharge was limited [Wright and Coleman [1971, 1974]. Therefore, it is uncertain how large a role entrainment of underlying salt water into discharging river effluent can have on the morphodynamics of subaqueous levees during periods of low to normal river discharge conditions.
 Field observations of dye trajectories in discharge from the South Pass of the Mississippi River delta [Wright and Coleman, 1974] and the results of numerical model simulations [Waldrop and Farmer, 1973] provided the basis for the proposed helical flow mechanism. However, in at least one instance that dye releases were cited as showing the development of helical flow cells the Mississippi River was in flood stage. Under these conditions the outflowing river discharge was reported to be attached to the bed over the entire region characterized by subaqueous levees and flow dynamics were dominated by turbulent mixing (graphically shown occurring at the lateral margins), inertia, bed friction, and head-induced superelevation with limited influence from buoyant forces [Wright and Coleman, 1974].
 In all of our experimental runs the presence of friction between the jet outflow and the bed of the receiving basin was a critical factor in the formation of subaqueous levees. Under buoyant conditions, when bed friction was absent, levees failed to form. The relative magnitude of bed friction, rather than its strict presence or absence, may have a controlling influence of levee morphodynamics.
 A number of analytical predications of river mouth hydrodynamics have suggested that increasing bed friction will increase the rate of momentum extraction from the flow, increase the rate of flow deceleration and increase the lateral spreading of the outflow [e.g., Borichansky and Mikhailov, 1966; Ozsoy, 1977, 1986; Ozsoy and Unluata, 1982; Wang, 1984; Izumi et al., 1999]. All of these feedbacks may in turn influence the spatial patterns of sediment transport and deposition. In natural systems, it may be difficult to separate the relative influence of sediment size variations from bed friction on levee morphology since bed friction is likely to be strongly dependent on channel bed roughness which will in turn vary with bed load sediment size and the presence and size of mobile bed forms such as dunes.
 In settings characterized by large-scale meandering turbulence structures, stability analysis indicates that the observed meandering should be suppressed as the outlet aspect ratio (B/H) and/or the bed friction (Cd) increase [Jirka, 2001; van Prooijen and Uijttewaal, 2002; Socolofsky and Jirka, 2004]. Suppression of the meander would in turn reduce the lateral transport of momentum [Rowland et al., 2009b] and sediment, potentially slowing levee development and facilitating mouth bar growth.
7.3. Is There an Effective Discharge(s) for Levee Formation?
 From our limited experiments on the morphodynamics of a buoyant jet we can neither confirm nor refute the flow dynamics and inferred sediment transport dynamics presented by Wright and Coleman  for hypopycnal river mouths settings. However, their data and observations (that served as the basis for this model) suggest that there was considerable spatial and temporal variability in the processes thought to drive the hydrodynamics at hypopycnal river mouths. This variability raises a fundamental question: Is there an effective discharge for levee formation? Wright and Coleman  observed mouth bar growth primarily occurred during flood conditions when frictional conditions prevailed. Even though they also stated that “…development of subaqueous levees appears to be perennial and is partly a function of the convergent flows which occur near the bottom in the saltwater layer during low and normal stages” [Wright and Coleman, 1974], there are no data from their studies of the Mississippi River delta, or any other studies to our knowledge, that documents the rates or timing of levee development in relation to the relative magnitude of river discharges. Conditions at normal or low flow discharges (during which hypopycnal versus frictional flow are noted) may not be relevant.
 Exploration of the relationship between levee growth rates and discharge conditions represents a critical and to date unexplored aspect of river mouth and delta dynamics. We also suggest that to date the dominant focus placed on relative outflow densities in relation to levee morphology may incorrectly deemphasize other more important morphological controls. Such controls may include: sediment size distributions of suspended load [Orton and Reading, 1993], the relative importance of suspended versus bed load transport [Izumi et al., 1999], bed friction, aspect ratio, the relative influence of suspended bed material, flood magnitudes and frequencies, upstream channel morphology controls on jet dynamics, and the role of sediment cohesiveness and vegetation [Edmonds and Slingerland, 2010].
 Our experiments suggest that cohesive sediment is not a prerequisite for subaqueous levee formation. Based on our experiments and the simulations of Edmonds and Slingerland , however, it appears that cohesion is important for protecting levees from erosion and facilitating channel development and progradation. Cohesion will arise when fine silt and clay settle on levees and become consolidated (or dewatered during low water levels). The added bank strength provided by cohesive sediments may also help maintain narrower deeper channels that in turn control the hydrodynamics of the discharging jet. Attempts by us to incorporate vegetation into our experiments failed; however, field observations suggest that vegetation rapidly colonizes newly emergent levees in tie channel settings [Rowland et al., 2009a]. Depending on the size of the tie channel and the rooting depth of the vegetation, the vegetation may provide added bank cohesion. On tie channels vegetation appears to significantly increase the roughness of the levee tops which in turn could increase sediment deposition and levee growth.
 In both our experiments and natural tie channels the jet outflow from a channel into a standing body of water exhibited a large-scale meandering instability. Despite the influence this instability has on the turbulence and short time scale sediment transport dynamics, our experimental levees showed no morphological imprint of the meandering flow structure. Sediments with varying ratios of entrainment shear velocity (u*ce) to settling velocities (Ws) led to varying levee morphology under identical flow conditions. The two sediment types with the highest Ws and u*ce values developed levees with distinct levee crest lines that exhibited minimal divergence. Levees formed by a third experimental sediment with lower Ws and u*ce values were thinner, had less pronounced crests and were more widely divergent.
 Analysis of bottom boundary shear stress distributions across the jet showed that the spatial pattern of u* controlled the location of levee formation. Levees formed in regions of the jet where u* < u*ce. The rate of levee deposition was controlled by the rate at which sediment was transferred from the jet core to the margins and the rate it settled from suspension at the margins. A comparison of the relative influences of advective versus dispersive sediment transport mechanisms showed that dispersive transport-dominated sediment delivery to the levee crests. Advective transport arising from the divergence of horizontal velocity vectors in response to jet expansion played a minimal role in sediment delivery. This result suggests that models relying solely on the time-averaged velocity structure of jets and neglecting the turbulent dynamics that control the lateral dispersion of momentum and scalars will dramatically under predict levee deposition rates.
 In our experiments, with high lateral sediment extraction rates, deposition of sediment onto levees in the upstream reaches of the flow removed the majority of sediment from the flow effectively limiting deposition along the jet centerline at downstream locations where u* < u*ce. From these observations we suggest that a dynamic competition may exist between levee development and mouth bar deposition in natural systems. In systems with high rates of levee development, and where subaerial levee development arises, levees will serve to reestablish upstream, channelized water surface slopes in regions downstream of the initial channel outlet. This would in turn lead to increased sediment transport across the developing mouth bar, delaying its stabilization and postponing channel bifurcation. In contrast, in systems with relatively low levee deposition rates, mouth bar growth and stabilization may force developing levees to diverge around them and channels may bifurcate more frequently.
 The observed variations in levee morphology under identical experimental hydrodynamic conditions; the development of narrow, parallel levees without hypopycnal flows in both the experimental and natural tie channels; and our failure to develop subaqueous levees under hypopycnal conditions caused us to reexamine long-standing conceptual models relating river mouth levee morphologies to either frictional or hypopycnal conditions. Our experimental results and review of published data on hypopycnal river mouths lead us to conclude that sediment settling velocities and suspension entrainment thresholds, relative magnitude of bed friction, and channel outlet aspect ratios may be more significant controls on levee morphologies at river mouth outlets than the influence of hypopycnal conditions as envisioned in the models of Wright .
 This work was supported by funding from the American Chemical Society Petroleum Research Fund and the National Center for Earth-Surface Dynamics (NCED). Additional support for experiments involving buoyant outflows was provided by Chevron ETC and the Terman Fellowship to George E. Hilley at Stanford University. We gratefully acknowledge the support of the U.S. Department of Energy through the LANL/LDRD Program to J.C.R. Jeremy Venditti, Kathleen Mai, Ken Ferrier, Leslie Hsu, Claire LeGall, and Timothy Greib assisted in data collection and analysis. Stuart Foster, John Potter, Neto Santana, Johnny Sanders, and Taylor Perron all provided critical assistance in flume construction. Mark Schmeeckle provided the infrared laser used in the suspended sediment profiling. The Coastal and Marine Geology Team at the U.S. Geological Survey provided the use of their Particle Size Analysis Laboratory at Menlo Park for the determination of settling velocities. We also thank Chris Ellis at the Saint Anthony Falls Laboratory, University of Minnesota, who freely gave his insights and advice on experimental design and provided advice critical for the development of the laser surveying technique for bed topography. Federico Falcini reviewed an early version of this manuscript and provided many valuable improvements to the analysis presented. Finally we thank Chris Paola, Maarten Kleinhans, and an anonymous reviewer for their thoughtful and detailed reviews of this manuscript.