2015
DOI: 10.1002/2014wr016083
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Linking bed morphology changes of two sediment mixtures to sediment transport predictions in unsteady flows

Abstract: Flume experiments were conducted to measure bed morphology adjustments in sand/gravel and sand/silt sediment mixtures during repeated hydrographs and to link these changes to sediment transport patterns over multiple time scales. Sediment composition and hydrograph flow magnitude greatly influenced channel morphology, which impacted sediment yield, hysteresis, and transport predictions. Bed load yields were larger and more variable for the sand/silt mixture, as gravel in the sand/gravel sediment inhibited grai… Show more

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Cited by 44 publications
(80 citation statements)
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“…Further regression analysis on our data is used to develop a combined hydrograph parameter ξ that accounts for the relative influence of W k and Γ HG on measured sediment yields, similar to Waters and Curran () analysis (see section ). In our case, the most appropriate form of this parameter is ξ = W k Γ HG α , where exponent α = 0.2 provides the best overall correlation ( R 2 > 0.99) to the measured W t * values (Figure c), following the power law relationship: Wt*=968.09ξ1.0826,0.36em()R2=0.996.2em …”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Further regression analysis on our data is used to develop a combined hydrograph parameter ξ that accounts for the relative influence of W k and Γ HG on measured sediment yields, similar to Waters and Curran () analysis (see section ). In our case, the most appropriate form of this parameter is ξ = W k Γ HG α , where exponent α = 0.2 provides the best overall correlation ( R 2 > 0.99) to the measured W t * values (Figure c), following the power law relationship: Wt*=968.09ξ1.0826,0.36em()R2=0.996.2em …”
Section: Resultsmentioning
confidence: 99%
“…The observed temporal variability in bed load sediment transport in response to flow hydrographs and zero sediment supply at the upstream boundary is characterized by differential transport rates, hysteresis patterns, and bed load yields during the rising and falling limbs under a wide range of hydrograph conditions. To account for this variability, Waters and Curran () proposed a modeling approach whereby the bed load transport is predicted separately, under equivalent discharge conditions, on the rising and falling hydrograph limbs. This is obtained through evaluation of a dimensionless transport rate W * , using the Einstein‐Parker dimensionless reference shear stress approach (Parker, ; Parker et al, ), which can be written for uniform sediments in the general form: W*=m10.8351τbr*τb*n, where m and n are modified transport coefficients derived from nonlinear regression and τ br * is the critical Shields stress, corresponding to the dimensionless reference transport rate W r * = q b * /τ b *3/2 = 0.002 (e.g., Parker et al, ), with q b * being the Einstein () bed load parameter (equation ).…”
Section: Discussionmentioning
confidence: 99%
“…During floods a hysteresis loop often develops in sediment flux measurements, whereby different magnitudes of bedload flux are produced on the rising and falling limbs of hydrographs for the same flow magnitude (Reid et al, 1985;Church et al, 1998;Hassan et al, 2006;Waters and Curran, 2015;Mao, 2018). During floods a hysteresis loop often develops in sediment flux measurements, whereby different magnitudes of bedload flux are produced on the rising and falling limbs of hydrographs for the same flow magnitude (Reid et al, 1985;Church et al, 1998;Hassan et al, 2006;Waters and Curran, 2015;Mao, 2018).…”
Section: Effect Of Inter-flood Duration On Bed Stabilitymentioning
confidence: 99%
“…Excess shear (ratio of applied shear stress and critical shear stress: τ 0 / τ c ) for the hydrographs ranges between 1.7–2.9 and 1–1.8 for the D 50bulk and D 84bulk particle sizes, respectively. Each triangular hydrograph was approximated in a series of short steps, as has been done in previous experiments simulating unsteady flow (Hassan et al, ; Mao, ; Martin and Jerolmack, ; Waters and Curran, ). The Froude number in the experiments ranged from 0.4 to 0.8 (estimated based on measured flow depths and known discharges), which is within range of the prototype streams and previous experiments studying unsteady flow (Lee et al, ; Mao, ; Waters and Curran, ).…”
Section: Methodsmentioning
confidence: 99%
“…The bed was then slowly saturated and drained to promote initial settlement of the freshly placed sediment. A period of low flow, enough to mobilize sand fractions, with no sediment feed was then initialized to provide the channel with a flow history (Waters and Curran, ; Mao, ; Redolfi et al, ). This period lasted for approximately 8 h, and was considered complete when the sand particles had rearranged such that their mobility was limited in the channel (through visual observation) and there was negligible sediment appearing in the bedload trap.…”
Section: Methodsmentioning
confidence: 99%