Model:TopoFlow-Channels-Dynamic Wave: Difference between revisions
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|Spatial dimensions=2D | |Spatial dimensions=2D | ||
|Spatialscale=Landscape-Scale, Watershed-Scale | |Spatialscale=Landscape-Scale, Watershed-Scale | ||
|One-line model description=Dynamic Wave process component for a D8-based, spatial hydrologic model | |One-line model description=Dynamic Wave process component for a D8-based, spatial hydrologic model | ||
|Extended model description=This process component is part of a spatially-distributed hydrologic model called TopoFlow, but it can now be used as a stand-alone model. The dynamic wave method is the most complete and complex method for modeling flow in open channels. This method retains all of the terms in the full, 1D momentum equation, including the gravity, friction and pressure gradient terms (as used by the diffusive wave method) as well as local and convective acceleration (or momentum flux) terms. This full equation is known as the St. Venant equation. In the current version of TopoFlow it is assumed that the flow directions are static and given by a D8 flow grid. In this case, integral vs. differential forms of the conservation equations for mass and momentum can be used. | |Extended model description=This process component is part of a spatially-distributed hydrologic model called TopoFlow, but it can now be used as a stand-alone model. The dynamic wave method is the most complete and complex method for modeling flow in open channels. This method retains all of the terms in the full, 1D momentum equation, including the gravity, friction and pressure gradient terms (as used by the diffusive wave method) as well as local and convective acceleration (or momentum flux) terms. This full equation is known as the St. Venant equation. In the current version of TopoFlow it is assumed that the flow directions are static and given by a D8 flow grid. In this case, integral vs. differential forms of the conservation equations for mass and momentum can be used. | ||
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{{Model technical information | {{Model technical information | ||
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{{Input - Output description | {{Input - Output description | ||
|Describe input parameters=The input variables used for the Dynamic Wave method of routing flow in channels are defined as follows. These inputs must be provided as grids: | |Describe input parameters=The input variables used for the Dynamic Wave method of routing flow in channels are defined as follows. These inputs must be provided as grids: | ||
*flow_codes = D8 flow codes (Jenson convention) | *flow_codes = D8 flow codes (Jenson convention), (NE,E,SE,S,SW,W,NW,N) → (1,2,4,8,16,32,64,128) | ||
*bed_slope = slope of the channel bed or hillslope (m / m) | *bed_slope = slope of the channel bed or hillslope (m / m) | ||
*Manning_n = Manning roughness parameter (s / m1/3) | *Manning_n = Manning roughness parameter (s / m1/3) | ||
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These inputs can be provided as scalars or grids: | These inputs can be provided as scalars or grids: | ||
*sinuosity = channel sinuosity (m/m) (along-channel / straight length) | |||
*init_depth = initial water depth (m) (See HTML help) | |||
Grids must be saved in binary files with no header. All variables should be stored as 4-byte, floating-point numbers (IEEE standard) except flow codes, which are unsigned, 1-byte integers. | Grids must be saved in binary files with no header. All variables should be stored as 4-byte, floating-point numbers (IEEE standard) except flow codes, which are unsigned, 1-byte integers. | ||
The behavior of this component is controlled with a configuration (CFG) file, which may point to other files that contain input data. Here is a sample configuration (CFG) file for this component: | The behavior of this component is controlled with a configuration (CFG) file, which may point to other files that contain input data. Here is a sample configuration (CFG) file for this component: | ||
|Pre-processing software needed?= | |||
|Post-processing software needed?= | Method code: 3 | ||
|Visualization software needed?= | Method name: Dynamic_Wave | ||
Manning flag: 1 | |||
Law of Wall flag: 0 | |||
Time step: Scalar 6.00000000 (sec) | |||
D8 flow code: Grid Treynor_flow.rtg (none) | |||
D8 slope: Grid Treynor_slope.rtg (m/m) | |||
Manning N: Grid Treynor_chan-n.rtg (s/m^(1/3)) | |||
Bed width: Grid Treynor_chan-w.rtg (m) | |||
Bank angle: Grid Treynor_chan-a.rtg (deg) | |||
Init. depth: Scalar 0.00000000 (m) | |||
Sinuosity: Scalar 1.00000000 (m/m) | |||
Save grid timestep: Scalar 60.00000000 (sec) | |||
Save Q grids: 1 Case5_2D-Q.rts (m^3/s) | |||
Save u grids: 0 Case5_2D-u.rts (m/s) | |||
Save d grids: 0 Case5_2D-d.rts (m) | |||
Save f grids: 0 Case5_2D-f.rts (none) | |||
Save pixels timestep: Scalar 60.00000000 (sec) | |||
Save Q pixels: 1 Case5_0D-Q.txt (m^3/s) | |||
Save u pixels: 0 Case5_0D-u.txt (m/s) | |||
Save d pixels: 0 Case5_0D-d.txt (m) | |||
Save f pixels: 0 Case5_0D-f.txt (none) | |||
|Input format=ASCII, Binary | |||
|Describe output parameters=This component computes the following variables, as grids: | |||
Q = discharge (m^3/s) | |||
u = flow velocity (m/s) | |||
d = flow depth (m) | |||
f = friction factor (none) | |||
Rh = hydraulic radius (m) | |||
S_free = free-surface slope (m/m) | |||
The user can choose which, if any, of these to save. Each may be saved as a grid sequence, indexed by time, in a netCDF file, at a specified sampling rate. Each may also be saved for a set of "monitored" grid cells, each specified as a (row,column) pair in a file with the name: <case_prefix>_outlets.txt. With this option, computed values are saved in a multi-column text file at a specified sampling rate. Each column in this file corresponds to a time series of values for a particular grid cell. For both options the sampling rate must no smaller than the process timestep. | |||
|Output format=ASCII, Binary | |||
|Pre-processing software needed?=Yes | |||
|Describe pre-processing software=Another program must be used to create the input grids. This includes a D8 flow grid derived from a DEM for the region to be modeled. The earlier, IDL version of TopoFlow can be used to create some of these. | |||
|Post-processing software needed?=Yes | |||
|Describe post-processing software=None, except visualization software. Grid sequences saved in netCDF files can be viewed as animations and saved as movies using VisIt. | |||
|Visualization software needed?=Yes | |||
|Other visualization software=VisIt | |||
}} | |||
{{Process description model | |||
|Describe processes represented by the model=The dynamic wave method for flow routing in the channels of a D8-based river network. | |||
|Describe key physical parameters and equations=Main equations used by this component: | |||
ΔV(i,t) = Δt * [ R(i,t) Δx Δy - Q(i,t) + Σk Q(k,t) ] = change in water volume [m3] (mass cons.) | |||
d = {[ w2 + 4 tan(θ) V / L]1/2 - w } / [2 tan(θ)] = mean water depth in channel segment [m] (if θ > 0) | |||
d = V / [w * L] = mean water depth in channel segment [m] (if θ = 0) | |||
Δv(i,t) = Δt * (T1 + T2 + T3 + T4 + T5) / [ d(i,t) * Aw ] = change in mean velocity [m / s] (mom. cons.) | |||
T1 = v(i,t) * Q(i,t) * (C - 1) = efflux term in equation for Δv | |||
T2 = Σk [v(k,t) - v(i,t) * C] * Q(k,t) = influx term in equation for Δv | |||
T3 = -v(i,t) * C * R(i,t) * Δx * Δy = "new mass" momentum term in equation for Δv | |||
T4 = Aw * [g * d(i,t) * S(i,t)] = gravity term in equation for Δv | |||
T5 = -Aw * [f(i,t) * v(i,t)2] = friction term in equation for Δv | |||
Q = v * Aw = discharge of water [m3 / s] | |||
f(i,t) = [ κ / LN ( a * d(i,t) / z0) ]2 = friction factor [unitless] (for law of the wall) | |||
f(i,t) = g * n2 / Rh(i,t)1/3 = friction factor [unitless] (for Manning's equation) | |||
C = Aw / At = area ratio appearing in equation for Δv | |||
At = wt * L = top surface area of a channel segment [m2] (L = length) | |||
wt = w + [ 2 * d * tan(θ) ] = top width of a wetted trapezoidal cross-section [m] | |||
Rh = Aw / Pw = hydraulic radius [m] | |||
Aw = d * [w + (d * tan(θ))] = wetted cross-sectional area of a trapezoid [m2] | |||
Pw = w + [2 * d / cos(θ)] = wetted perimeter of a trapezoid [m] | |||
Vw = d2 * [ L * tan(θ) ] + d * [L * w] = wetted volume of a trapezoidal channel [m] | |||
}} | }} | ||
{{Model testing}} | {{Model testing}} | ||
{{Users groups model}} | {{Users groups model}} |
Revision as of 13:09, 16 February 2010
Contact
Name | Scott Peckham |
Type of contact | Model developer |
Institute / Organization | CSDMS, INSTAAR, University of Colorado |
Postal address 1 | 1560 30th street |
Postal address 2 | |
Town / City | Boulder |
Postal code | 80305 |
State | Colorado |
Country | USA"USA" is not in the list (Afghanistan, Albania, Algeria, Andorra, Angola, Antigua and Barbuda, Argentina, Armenia, Australia, Austria, ...) of allowed values for the "Country" property. |
Email address | Scott.Peckham@colorado.edu |
Phone | 303-492-6752 |
Fax |
TopoFlow-Channels-Dynamic Wave
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