AgDegNormal
This module calculates a) the equilibrium sediment transport rate and b) the morphodynamic evolution of a reach due to a change in sediment input rate.
Model introduction
The module computes variation in river bed level η(x, t), where x denotes a streamwise coordinate and t denotes time, in a river with constant width B. The bed sediment is characterized in terms of a single grain size D and submerged specific gravity R. The reach under consideration has length L. Bed elevation at the downstream end is assumed to be fixed. The model is based on total bed material load. The model is 1D, assumes a rectangular channel and neglects wall effects.
By modifying the sediment feed rate (Gtf) at the upstream end, the river can be forced to aggrade or degrade to a new equilibrium. The module computes this evolution.
Model parameters
Uses ports
This component has no uses ports.
Provides ports
- Model: Provides IRF functionality.
Main equations
- Flow in the channel (using Manning-Strickler formulation)
[math]\displaystyle{ C_{z}={\frac{U}{u_{*}}}=\alpha _{r}\left ( \frac{H}{K_{c}} \right )^{\frac{1}{6}} }[/math] (1)
- grain roughness (Used as roughness height when bedforms are absent)
[math]\displaystyle{ k_{s} = n_{k} D }[/math] (2)
- water conservation for a quasi-steady flow
[math]\displaystyle{ Q = q\lt sub\gt w\lt /sub\gt B = U B H }[/math] (3)
- Boundary shear stress
[math]\displaystyle{ \tau _{b} = \rho u_{*} ^2 = \rho g H S }[/math] (4)
- Shields number (Shields stress)
[math]\displaystyle{ \tau ^* = {\frac{\tau _{b}}{\rho R g D}} = {\frac{H S}{R D}} }[/math] (5)
- Submerged specific gravity
[math]\displaystyle{ R = {\frac{\rho _{s}}{\rho}} - 1 }[/math] (6)
- Water depth
[math]\displaystyle{ H = [{\frac{\left (k_{c} \right ) ^{\frac{1}{3}} Q_{w}^2}{\alpha _{r} g B^2 S}}]^{\frac{3}{10}} }[/math] (7)
- Computation of the sediment transport (Meyer-Peter and Muller equation )
[math]\displaystyle{ q_{t} ^* =\left\{\begin{matrix} \alpha_{t} \left ( \varphi_{s} \tau ^2 - \tau_{c} ^* \right ) ^ \left ( n_{t} \right ) & \tau ^* \gt \tau_{c} ^* \\ 0 & \tau ^* \lt = \tau_{c} ^*\end{matrix}\right. }[/math] (8)
- Einstein number
[math]\displaystyle{ q_{t} ^* = {\frac {q_{t}}{\sqrt{R g D} D}} }[/math] (9)
- Cumulative time of the river has been in flood
[math]\displaystyle{ t_{f} = I_{f} t }[/math] (10)
- Equilibrium (graded) states
- Annual sediment yield with a graded state at this slope
[math]\displaystyle{ G_{t} = \rho_{s} q_{t} Bl_{f} t_{a} }[/math] (11)
- Volume sediment transport rate per unit width obtained at the graded state
[math]\displaystyle{ q_{t} = {\frac{G_{tf}}{\rho_{s}Bl_{f} t_{a}}} }[/math] (12)
- Computation of bed variation
- Exner equation of sediment continuity (assume that qt is zero for most of the time)
[math]\displaystyle{ \left ( 1 - \lambda_{p} \right ) {\frac{\partial\eta}{\partial t}} = - {\frac{\partial q_{t}}{\partial x}} }[/math] (13)
- Exner equation of sediment continuity (average over many floods)
[math]\displaystyle{ \left ( 1 - \lambda_{p} \right ) {\frac{\partial \eta}{\partial t}}= - {\frac{\partial l_{f} q_{t}}{\partial x}} }[/math] (14)
- Spatial derivative of the total bed material load per unit width
[math]\displaystyle{ \frac{\Delta q_{t,i}}{\Delta X}=a_{u}\frac{q_{t,i}-q_{t,i-1}}{\Delta X}+\left ( 1-a_{u} \right )\frac{q_{t,i+1}-q_{t,i}}{\Delta X} }[/math] (15)
- Bed slope computed in each node
[math]\displaystyle{ S=\left\{\begin{matrix} \frac{\eta _{1}-\eta _{2}} {\Delta x} & i=1\\ \frac{\eta _{i-1}- \eta _{i+1}} {2\Delta X} & i=2...M \\ \frac{\eta _{M} - \eta _{M+1}}{\Delta X} & i=M+1 \end{matrix}\right. }[/math] (16)
- Initial bed elevation
[math]\displaystyle{ \eta_{i}=S \left ( L - x_{i} \right ) }[/math] (17)
- non-dimensional total shear stress
[math]\displaystyle{ \tau _{b} ^* = {\frac{\tau _{b}}{\left ( \rho _{s} - \rho \right ) g D}} }[/math] (18)
Symbol | Description | Unit |
---|---|---|
X | Streamwise coordinate | m |
ΔX | Spatial step length | m |
t | Temporal coordinate | seconds |
Cf | Non-dimensional friction coefficient | - |
Qw | Flood discharge | m3/s |
If | Flood intermittency | - |
Bc | Channel width | m |
D | Characteristic grain size | mm |
λp | Bed porosity | - |
kc | Composite roughness height | mm |
SI | Ambient bed slope | - |
Gtf | Imposed annual sediment transport rate | tons/annum |
L | Length of reach | m |
Δt | Time step | year |
Ntoprint | number of time steps to printout | - |
Nprint | number of printouts | - |
M | Number of spatial intervals | - |
au | Upwinding coefficient (1 = full upwind, 0.5 = central difference) | - |
αr | Coefficient in Manning-Strickler | - |
αs | Coefficient in sediment transport relation | - |
ηt | Exponent in sediment transport relation | - |
τ*c | Reference Shields number in sediment transport relation | - |
φs | Fraction of bed shear stress due to skin friction | - |
R | Submerged specific gravity | - |
Cz | Non-dimensional Chézy friction coefficient | - |
Output
Symbol | Description | Unit |
---|---|---|
η | Bed surface elevation | m |
S | Bed slope | - |
H | Water depth | m |
τb | Total (skin friction + form drag) Shields number | - |
qt | total bed material load | m2/s |
Notes
- The maximum number of computational nodes, M, is 99 (this is the case for all of the AgDeg functions).
- The model calculates the water depth with a Chezy formulation, if only the Chézy coefficient is specified in the input file. The code uses a Manning-Strickler formulation, when only the roughness height, kc, and the coefficient αr are given in the input text file. If all these parameters are in the text file, the program will ask the user which formulation he would like to use
- The model prompts user whether he would like to append some of the characteristic values for the initial and final equilibrium state to the output file, or write them in a separate file.
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:
- Upload file: http://csdms.colorado.edu/wiki/Special:Upload
- Create link to the file on your page: [[Image:<file name>]].
See also: Help:Images or Help:Movies
Developer(s)
References
- Paola, C., Heller, P.L., and Angevine, C.L., 1992. The large-scale dynamics of grain-size variation in alluvial basins. 1: Theory. Basin Research, 4, 73-90.
- Meyer-Peter, E., and Müller, R., 1948. Formulas for bed-load transport Proceedings, 2nd Congress International Association for Hydraulic Research, Rotterdam, the Netherlands, 39-64.
Links
- Model:AgDegNormal
- http://vtchl.uiuc.edu/people/parkerg/word_files.htm (Chapter 14, "1D aggradation and degradation of rivers: normal flow assumption" of the e-book).