Model help:Acronym1D: Difference between revisions

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| submerged specific density of sediment
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| τ<sub>g<sub>
| flow velocity
| shields number
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| water depth
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| u<sup>*</sup>
| shear velocity
| m / s
| m / s
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| τ<sub>sg</sub>
| Q<sub>wa</sub>
| shield stress
| mean annual water discharge
| kg / (m s)
| m<sup>3</sup> / s
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| D<sup>g</sup>
| geometric mean
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| σ<sup>g</sup>
| geometric standard deviation
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| D<sup>x</sup>
| diameter such that x% of the distribution is finer
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| Q<sup>wr</sup>
| mean water discharge for each range
| m<sup>3</sup> / s
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| pQ
| fraction of time in that range
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| u<sub>*</sub>
| shear velocity on the range
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Revision as of 15:48, 15 April 2011

The CSDMS Help System

Acronym1D

“Acronym1_D” combines the scheme of “Acronym1_R” with a flow duration curve. The bedload transport rate and bedload grain size distribution are computed for each flow of the curve, and then averaged to yield a mean bedload transport rate and a mean bedload grain size distribution.

Model introduction

“Acronym1_D” simply adds a flow duration curve to the algorithm of “Acronym1_R” in order to compute the average volume gravel bedload transport rate per unit width qbTa, as well as the average bedload grain size distribution (Db,i, paf,i), i = 1..N+1. In addition, it computes the values Qa, Ha, u∗a and τga∗ corresponding to annual mean values of the water discharge, depth, shear velocity and Shields stress based on surface geometric mean size. The values Dalg, σalg, Dal90, Dal70, Dal50 and Dal30 associated with the mean grain size distribution of the bedload are computed along with the corresponding values for the surface material, Dsg, σsg, Ds90, Ds70, Ds50 and Ds30. Finally, the program computes the volume gravel bedload transport rate per unit width qbT, the water discharge Qw, flow depth H, the shear velocity u and the Shields stress τg∗ associated with each range in the flow duration curve, along with the fraction of time pQ that the flow is in that range.

The flow duration curve is specified in terms of the pairs (Qwd,k, peQ,k), k = 1..M+1, where Qwd,k denotes the kth discharge and peQ,k denotes the percentage of time this flow is exceeded. Here k = 1 corresponds to the highest flow in the curve, with an exceedance percentage peQ of zero, and k = M+1 corresponds to the lowest flow in the curve, with an exceedance percentage peQ of 100. The lowest flow on the curve Qwd,M must exceed zero.

Model parameters

Parameter Description Unit
First parameter Description parameter [Units]
Parameter Description Unit
First parameter Description parameter [Units]

Uses ports

This will be something that the CSDMS facility will add

Provides ports

This will be something that the CSDMS facility will add

Main equations

  • Grain Size:
[math]\displaystyle{ \Psi= LN_{2}\left (D\right) = {\frac{log_{10}\left (D\right)}{log_{10}\left (2\right)}} }[/math] (1)
[math]\displaystyle{ \Psi_{i}= LN_{2}\left ( D_{i}\right) = {\frac{log_{10}\left (D_{i}\right)}{log_{10}\left (2\right)}} }[/math] (2)
[math]\displaystyle{ D_{i}= Sqrt \left (D_{b, i} D_{b, i+1} \right ) }[/math] (3)
[math]\displaystyle{ F_{i}= \left ( F_{f, i} - F_{f, i+1} \right ) / 100 }[/math] (4)
[math]\displaystyle{ D_{sg}=2^\Psi_{s} }[/math] (5)
[math]\displaystyle{ \Psi_{s}= \Sigma \Psi_{i} F{i} }[/math] (6)
[math]\displaystyle{ \sigma_{sg}= 2 ^\sigma }[/math] (7)
[math]\displaystyle{ \sigma ^2= \Sigma \left (\Psi_{i} - \Psi \right )^2 F_{i} }[/math] (8)
[math]\displaystyle{ W_{i}^*= {\frac{Rgq_{bi}}{F_{i}u_{*} ^3}}= 0.00218 G \left (\Phi \right ) }[/math] (9)
[math]\displaystyle{ \phi= \omega \phi_{sgo} \left ( {\frac{D_{i}} {D_{sg}}} \right )^ \left (-0.0951 \right ) }[/math] (10)
[math]\displaystyle{ \Phi= {\frac{\tau_{sg} ^*}{\tau_{ssrg} ^*}} }[/math] (11)
[math]\displaystyle{ \tau_{sg} ^*={\frac{u_{*} ^2}{Rg D_{sg}}} }[/math] (12)
  • φ> 1.59
[math]\displaystyle{ G \left ( \Phi \right )= 5474 \left ( 1 - {\frac{0.853}{\Phi}} \right ) ^ \left (4.5 \right ) }[/math] (13)
  • 1<=φ<=1.59
[math]\displaystyle{ G\left (\Phi \right )= exp\left ( 14.2\left ( \Phi - 1\right ) - 9.28 \left ( \Phi - 1 \right )^2 \right ) }[/math] (14)
  • φ< 1
[math]\displaystyle{ G\left (\Phi \right )= \Phi ^\left (14.2 \right ) }[/math] (15)
[math]\displaystyle{ \omega= 1 + {\frac{\sigma}{\sigma_{O} \left ( \Phi_{sgo} \right ) }} \left ( \omega_{O} \left ( \Phi_{sgo} \right ) - 1 \right ) }[/math] (16)
[math]\displaystyle{ q_{bT}= \Sigma q_{bi} }[/math] (17)
[math]\displaystyle{ p_{i}= {\frac{q_{bi}}{q_{bT}}} }[/math] (18)
[math]\displaystyle{ D_{lg}= 2 ^\left (\psi_{l} \right ) }[/math] (19)
[math]\displaystyle{ \Psi_{l}= \Sigma \Psi_{i} p_{i} }[/math] (20)
[math]\displaystyle{ \delta_{lg}= 2 ^\left ( \delta_{l} \right ) }[/math] (21)
[math]\displaystyle{ \delta_{l} ^2= \Sigma \left ( \Psi_{i} - \Psi_{l} \right )^2 p_{i} }[/math] (22)
[math]\displaystyle{ D_{lx}= 2 ^\left (\Psi_{lx} \right ) }[/math] (23)
[math]\displaystyle{ \Psi_{lx}= \Psi_{b, i+1} + {\frac{\Psi_{b, j} - \Psi_{b, i+1}}{p_{f, i} - p_{f, i+1}}}\left ( x - p_{f, i+1} \right ) }[/math] (24)
[math]\displaystyle{ \Psi_{b, i}= Ln_{2} \left ( D_{b, j} \right ) }[/math] (25)
[math]\displaystyle{ Q_{wr,k}= {/frac{1}{2}} \left ( Q_{wd,k} + Q_{wd, k+1} \right ) }[/math] (26)
[math]\displaystyle{ P_{Q,k}= {\frac{p_{eQ,k+1} - p_{eQ,k}}{100}} }[/math] (27)

Notes

  • Note on equations

In order to implement the equations 10~16, it is necessary to specify a) the surface grain size distribution (Df,i, Ff,i) and b) the shear velocity u. This results in a predicted values of qbi.

If the boundary shear stress at the bed includes a component of form drag, the component must be removed before computing u.

Once the parameters qbi are known the total volume bedload transport rate per unit width qbT and the fractions pi in the bedload can be calculated as equations 17, 18.

The results are presented in terms of qbT and the grain size distribution of the bedload, which is computed from the values of pi. These same fractions pi are used to compute the geometric mean and geometric standard deviation of the bedload Dlg and σlg, respectively, from the relations of equations 19, 20, 21, 22.

The percent finer in the bedload pf,i for the grain size Df,i is obtained from the fractions pi as follows: pf,1 = 100 pf,i = pf,i-1 - 100 pi-1 (i=2~N+1)

Let Dsx and Dlx denote sizes in the surface and bedload material, respectively, such that x percent of the material is finer. For example, if x = 50 then Ds50 and Dl50 denote the median sizes of the surface and bedload material, respectively. Once Ff,i is specified (pf,i is computed) the value Dsx (Dlx) can be computed by interpolation. The interpolation should be done using a logarithmic scale for grain size. For example, consider the computation of Dlx where pf,i ≤ x ≤ pf,i+1. Then we got equation 23, 24, using equation 25.

The characteristic flow Qwr,k in each range and fraction of time the flow is in that range pQ,k are computed with equation 26, 27, here k is ranged from 1 to M.

Let Yk be any parameter defined for each of the flow ranges k = 1..M. The mean value Ya averaged over the flow duration curve is then given as Y = /Sigma Yk pQ,k For example, if the fractions in the bedload in each grain size range within flow range k are given as pk,i then the average fractions of the bedload pai are given as pai = /Sigma pk,i pQ,k

Examples

An example run with input parameters, BLD files, as well as a figure / movie of the output

Follow the next steps to include images / movies of simulations:

See also: Help:Images or Help:Movies

Developer(s)

Gary Parker

References

  • Parker, G. 1990a Surface based bedload transport relation for gravel rivers. Journal of Hydraulic Research, 28(4), 417 436.
  • Parker, G. 1990b The "ACRONYM" series of Pascal programs for computing bedload transport in gravel rivers. External Memorandum M 220, St. Anthony Falls Hydraulic Laboratory, University of Minnesota.

Links