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==Overview==
 
==Overview==
−
Module Runoff allows the calculation of the overland surface runoff over a regular structured grid as function of the water column and terrain slope. The water column, namely the water located above the terrain, is given by the [[Module Basin]] where the precipitation is converting into a water column considering the losses due to the evapotranspiration and the infiltration processes. In particular the overland flow is evaluated by the Manning’s equation.
+
Module Runoff allows the calculation of the overland surface runoff over a grid as function of the water column slopes between adjacen cells (dynamic wave). The water column, namely the water located above the terrain, is given by the [[Module Basin]] after considering the precipitation input and the losses due to the evaporation and the infiltration.  
  
 
==Main Processes==
 
==Main Processes==
 +
The ModuleRunoff computes flow at cell faces using three different approaches (user option)
 +
#Full St. Venant Equation in 2D (shallow water equations)
 +
#Manning Equation with surface water gradient (diffuse wave)
 +
#Manning Equation with bottom gradient (kinematic wave)
  
−
The runoff is calculated by the Manning's equation.
+
===St. Venant Equations ===
 +
The St. Venant Equations are derived from the Newton's second law taking into account inertia effects. In this case a 2D approach is followed. [[Equations_in_Mohid_Land#2D_descritization_.28Runoff.29 | See equations description]].
  
 +
===Manning Equation===
  
−
:<math>\[Q=\frac{1}{n}\cdot A\cdot R_{h}^{2/3}\cdot s^{1/2}\]</math>
+
The overland surface runoff flow (m3/s) is calculated at the cell faces and it can be obtained by applying the Manning's equation.
 +
In this case inertia effects are neglected and forces balance bottom friction.
 +
 
 +
<ref>Gauckler, P. (1867), Etudes Théoriques et Pratiques sur l'Ecoulement et le Mouvement des Eaux, Comptes Rendues de l'Académie des Sciences, Paris, France, Tome 64, pp. 818–822</ref> :
 +
 
 +
:<math>Q_i=\frac{1}{n}\cdot A\cdot R_{h}^{2/3}\cdot s_i^{1/2}\,\,\,\,\,\,\,\,\,\,\,\,(1.1)</math>
 +
 
 +
where:
 +
:{|
 +
| ''Qi'' || is the overland flow in each direction (m<sup>3</sup>/s)
 +
|-
 +
| ''A'' || is the area of the cross-section (m<sup>2</sup>)
 +
|-
 +
| ''n'' || is the Manning coefficient (s/m<sup>1/3</sup>)
 +
|-
 +
| ''R<sub>h</sub>''|| is the hydraulic radius (m)
 +
|-
 +
| ''Si'' || is the slope of the water surface  (m/m)
 +
|}
 +
 
 +
 
 +
====Hydraulic radius====
 +
 
 +
In rectangular channels, the hydraulic radius is evaluated by the formula:
 +
 
 +
 
 +
:<math>R_{h}=\frac{w\cdot h}{w+2\cdot h}\,\,\,\,\,\,\,\,(1.2)</math> 
 +
 
 +
But in runoff the lateral cell face is open boundary (to the next cell) not exerting friction in a surface as the bottom boundary, and so hydraulic radius can be rewritten:
 +
 
 +
 
 +
:<math>R_{h}=\frac{w\cdot h}{w}\,\,\,\,\,\,\,\,(1.2)</math>
 +
 
 +
 
 +
and the hydraulic radius is R<sub>h</sub>=h. Therefore the Manning's equation can be rewritten as:
 +
 
 +
 
 +
:<math>Q=\frac{1}{n}\cdot w\cdot h^{5/3}\cdot s^{1/2}\,\,\,\,\,\,\,\,(1.3)</math>
 +
 
 +
====Slope====
 +
 
 +
The slope (s) is calculated by the difference of the water levels (H) at the extremities of the considered cell:
 +
 +
 
 +
:<math>H(i,j)= h(i,j)+T(i,j)\,\,\,\,\,\,\,\,\,\,\,\,(1.4)</math> 
 +
 
 +
 
 +
where:
 +
:{|
 +
|-
 +
|''H'' || is the water level (m)
 +
|-
 +
| ''h(i,j)'' || is the water column (m)
 +
|-
 +
| ''T(i,j)'' || is the Topography (m)
 +
|-
 +
| ''j'' || is X direction
 +
|-
 +
| ''i'' || is Y direction
 +
|}
 +
 
 +
 
 +
:<math>s_{x}=\frac{H(i,j-1)-H(i,j)}{DZX}\,\,\,\,\,\,\,\,(1.5)</math> 
 +
 
 +
 
 +
where:
 +
:{|
 +
|-
 +
|''s<sub>x</sub>'' || is the slope in the X direction (m)
 +
|-
 +
| ''H(i,j-1)'' || is the water column at the left face of the cell (m)
 +
|-
 +
| ''H(i,j)'' || is the water column at the right face of the cell (m)
 +
|-
 +
| ''DZX'' || is width of the cell in the X direction (m)
 +
|}
 +
 
 +
 
 +
:<math>s_{y}=\frac{H(i-1,j)-H(i,j)}{DZY}\,\,\,\,\,\,\,\,(1.6)</math>  
  
  
 
where:
 
where:
 
:{|
 
:{|
−
| ''A'' || is the area of the cross-section (<math>\[m^{2}]</math>)
+
|''s<sub>y</sub>'' || is the slope in the Y direction (m)
 
|-
 
|-
−
| ''n'' || is the '''Manning coefficient''' ()
+
| ''H(i-1,j)'' || is the water column at the left face of the cell (m)
 
|-
 
|-
−
| ''R_{h}''|| is the hydraulic radius (m)
+
| ''H(i,j)'' || is the water column at the right face of the cell (m)
 
|-
 
|-
−
| ''S'' || is the slope of the water surface  (m/m)  
+
| ''DZY'' || is width of the cell in the X direction (m)
 
|}
 
|}
  
 +
In order to take in account the limitation given by the Manning's equation (1.1) that tends to overestimate the flow velocity when solpe > 0.04, the slope value obtained by the formulas (1.5) and (1.6) it  is subsequently adjusted by the following function:
 +
[http://www.hkh-friend.net.np/rhdc/training/lectures/HEGGEN/Tc_3.pdf Slope correction given by City of Albuquerque, 1997, p.22-26]
  
−
In order to apply it each cells of the grid are considered as a open channel as shown in the  scheme below.
 
  
−
[[Image:Example.jpg]]
+
 
 +
:<math>s= 0.05247 + 0.06363 \cdot s - 0.182\cdot e^{(-62.38\cdot s)}\,\,\,\,\,\,\,\,\,\,\,\,(1.7)</math>
 +
 
  
 
where:
 
where:
 
:{|
 
:{|
−
| ''H'' || is the water column (m)
+
|''s'' || is the slope (m)
 +
|}
 +
 
 +
===Manning cofficient===
 +
 
 +
The Manning coefficient is derived from the land use map. Indeed by using a GIS program it is possible to associate at each cell a land use class in order to obtain, by the support of an abacus or table, a Manning coefficent value. See the Other Features section.
 +
 
 +
===Connection with River===
 +
 
 +
 
 +
In the eventuality presence of a river it is possible to obtain two different configurations:
 +
 
 +
:{|
 +
* Flow to the river when the water level of the river is lower that soil one
 
|-
 
|-
−
| ''W'' || is the cell width (m)
+
 
 +
|-
 +
[[Image:Figure03.jpg|thumb|center|upright=2|Figure 3: Flow to the river]]
 +
|-
 +
|-
 +
* Flow from the river when the water level is higher than the soil one
 +
|-
 +
|-
 +
[[Image:Figure04.jpg|thumb|center|upright=2|Figure 4: Flow from the river]]
 +
 
 +
 
 +
The flow between river and runoff is computed using the same formulation as in runoff cells using the surface gradient between runoff and river.
 +
 
 
|}
 
|}
  
 +
==Boundary Conditions==
 +
In Runoff there is the option to define the boundary condition as a level or as a timeserie (tide). This level will be imposed at the boundary and if the user wishes a) the water will only exit if the water level is higher than the boundary level and no inflow is allowed or b) inflow is allowed if the boundary level is higher than water level.
 +
 +
===Computation===
 +
Boundary fluxes are computed after the flow computation iteration.
 +
 +
The boundary flux is computed with celerity in both directions (x and y) where boundary face exists.
 +
Qi = - cel  *  Li * min(dh,h)
  
 +
where cel is celerity = SQRT(g * h)
 +
where Li is cell length perpendicular to direction
 +
where dh is level difference, if negative, boundary level is higher than runoff level
 +
where h is water height
  
−
In order to apply this formula each cells is consider like a open channel where the water level is given by the water column and the slope in the two directions X,Y is given by the difference of the slopes' interfaces. The roughtness of the terrain is given by the manning coefficient ans it is obtained by the land use map by a gis process.
 
  
−
The runoff is calculated by the Manning's equation as follow:
+
the water height in celerity is water column (maximum column between inside and outside) and height for Area is the minimum between the difference between levels (dh) and the water column (if boundary level higher, height is dh, otherwise is also dh except if boundary level is lower than topography and in that case the minimum is the water column).
 +
 
 +
===Keywords===
 +
The keyword in Runoff_X.dat that connects the open boundary is:
 +
IMPOSE_BOUNDARY_VALUE    : 1
 +
 
 +
The keyword that defines the boundary level is:
 +
BOUNDARY_VALUE            : 100.
 +
 
 +
The open boundary computation can be limited to specific areas defining the maximum altimetry that the boundary will be open. This is specifically useful when one wants to open the surface water at flat areas where in fact the flux can go trough the boundaries of the watershed delimitation.
 +
MAX_DTM_FOR_BOUNDARY      : 1000.
 +
 
 +
Using a value of the latter keyword higher than the maximum altimetry found in the watershed will make the boundary open in all watershed.
 +
 
 +
 
 +
To allow water to flow in if the boundary level is higher use this keyword connected. Otherwise the boundary level will behave as a wall that if boundary level is higher than it does not allow water to exit but dos not also allow it to enter.
 +
ALLOW_BOUNDARY_INFLOW    : 1
 +
 
 +
If the user wants to use a timeserie for imposing level (tide) than use this block where Piezometer6.dat is a time serie with level in time in the second column that the user will impose.
 +
<begin_boundary>
 +
FILENAME                  : ..\General Data\Boundary Conditions\Piezometer6.dat
 +
DATA_COLUMN              : 2
 +
<end_boundary>
 +
 
 +
==Discharges==
 +
 
 +
In Runoff the discharges may be positive or negative (Runoff uses discharge flow) and are dealt with ModuleDischarges.
 +
 
 +
===Computation===
 +
The discharges are initialized in Construct phase reading its locations and checking if inside boundaries.
 +
 
 +
In Modification phase, the several discharges flows are accounted and water volume updated. The computation is inside the water column iteration process.
 +
And integration variable integrates this flow for RunoffProperties.
 +
 
 +
===Keywords===
 +
For discharges to be read in Discharges_X.dat the following keyword needs to exist in the Runoff_X.dat
 +
DISCHARGES : 1
 +
Without these keyword no matter what is inside Discharges_X.dat it will not be read!
  
−
In order to apply the manning formula
 
  
 
==Other Features==
 
==Other Features==
Line 47: Line 206:
 
Options:
 
Options:
 
* Use a constant value  
 
* Use a constant value  
−
* Define a Manning's grid: One possible option is to associate Manning with land use classes (shape file). In this case can use MOHID GIS going to menu [Tools]->[Shape to Grid Data] and provide: i) the grid (model grid), ii) the land use shape file and iii) the corespondence between land use codes and Manning.
+
* Define a Manning's grid: One possible option is to associate Manning with land use classes (shape file). In this case can use MOHID GIS going to menu [Tools] <math>\Longrightarrow </math> [Shape to Grid Data] and provide:
−
 
+
:{|
 +
|(i) the grid (model grid)
 +
|-
 +
|ii) the land use shape file  
 +
|-
 +
| iii) the corespondence between land use codes and Manning
 +
|}
 
Use Manning inicialization with [[Module_FillMatrix|Module FillMatrix]] standards in the block:
 
Use Manning inicialization with [[Module_FillMatrix|Module FillMatrix]] standards in the block:
 
  <BeginOverLandCoefficient>
 
  <BeginOverLandCoefficient>
Line 58: Line 223:
 
  <EndOverLandCoefficient>
 
  <EndOverLandCoefficient>
  
−
==Outputs==
+
== Outputs==
  
−
==References ==
+
== References ==
 +
* Hubert Chanson|Chanson, H. (2004), The Hydraulics of Open Channel Flow, Butterworth-Heinemann, Oxford, UK, 2nd edition, 630 pages
 +
*http://www.hkh-friend.net.np/rhdc/training/lectures/HEGGEN/Tc_3.pdf
  
 
==Data File ==
 
==Data File ==

Latest revision as of 16:02, 18 May 2017

Overview

Module Runoff allows the calculation of the overland surface runoff over a grid as function of the water column slopes between adjacen cells (dynamic wave). The water column, namely the water located above the terrain, is given by the Module Basin after considering the precipitation input and the losses due to the evaporation and the infiltration.

Main Processes

The ModuleRunoff computes flow at cell faces using three different approaches (user option)

  1. Full St. Venant Equation in 2D (shallow water equations)
  2. Manning Equation with surface water gradient (diffuse wave)
  3. Manning Equation with bottom gradient (kinematic wave)

St. Venant Equations

The St. Venant Equations are derived from the Newton's second law taking into account inertia effects. In this case a 2D approach is followed. See equations description.

Manning Equation

The overland surface runoff flow (m3/s) is calculated at the cell faces and it can be obtained by applying the Manning's equation. In this case inertia effects are neglected and forces balance bottom friction.

<ref>Gauckler, P. (1867), Etudes Théoriques et Pratiques sur l'Ecoulement et le Mouvement des Eaux, Comptes Rendues de l'Académie des Sciences, Paris, France, Tome 64, pp. 818–822</ref> :

Q_i=\frac{1}{n}\cdot A\cdot R_{h}^{2/3}\cdot s_i^{1/2}\,\,\,\,\,\,\,\,\,\,\,\,(1.1)

where:

Qi is the overland flow in each direction (m3/s)
A is the area of the cross-section (m2)
n is the Manning coefficient (s/m1/3)
Rh is the hydraulic radius (m)
Si is the slope of the water surface (m/m)


Hydraulic radius

In rectangular channels, the hydraulic radius is evaluated by the formula:


R_{h}=\frac{w\cdot h}{w+2\cdot h}\,\,\,\,\,\,\,\,(1.2)

But in runoff the lateral cell face is open boundary (to the next cell) not exerting friction in a surface as the bottom boundary, and so hydraulic radius can be rewritten:


R_{h}=\frac{w\cdot h}{w}\,\,\,\,\,\,\,\,(1.2)


and the hydraulic radius is Rh=h. Therefore the Manning's equation can be rewritten as:


Q=\frac{1}{n}\cdot w\cdot h^{5/3}\cdot s^{1/2}\,\,\,\,\,\,\,\,(1.3)

Slope

The slope (s) is calculated by the difference of the water levels (H) at the extremities of the considered cell:


H(i,j)= h(i,j)+T(i,j)\,\,\,\,\,\,\,\,\,\,\,\,(1.4)


where:

H is the water level (m)
h(i,j) is the water column (m)
T(i,j) is the Topography (m)
j is X direction
i is Y direction


s_{x}=\frac{H(i,j-1)-H(i,j)}{DZX}\,\,\,\,\,\,\,\,(1.5)


where:

sx is the slope in the X direction (m)
H(i,j-1) is the water column at the left face of the cell (m)
H(i,j) is the water column at the right face of the cell (m)
DZX is width of the cell in the X direction (m)


s_{y}=\frac{H(i-1,j)-H(i,j)}{DZY}\,\,\,\,\,\,\,\,(1.6)


where:

sy is the slope in the Y direction (m)
H(i-1,j) is the water column at the left face of the cell (m)
H(i,j) is the water column at the right face of the cell (m)
DZY is width of the cell in the X direction (m)

In order to take in account the limitation given by the Manning's equation (1.1) that tends to overestimate the flow velocity when solpe > 0.04, the slope value obtained by the formulas (1.5) and (1.6) it is subsequently adjusted by the following function: Slope correction given by City of Albuquerque, 1997, p.22-26


s= 0.05247 + 0.06363 \cdot s - 0.182\cdot e^{(-62.38\cdot s)}\,\,\,\,\,\,\,\,\,\,\,\,(1.7)


where:

s is the slope (m)

Manning cofficient

The Manning coefficient is derived from the land use map. Indeed by using a GIS program it is possible to associate at each cell a land use class in order to obtain, by the support of an abacus or table, a Manning coefficent value. See the Other Features section.

Connection with River

In the eventuality presence of a river it is possible to obtain two different configurations:

  • Flow to the river when the water level of the river is lower that soil one
Figure 3: Flow to the river


  • Flow from the river when the water level is higher than the soil one


Figure 4: Flow from the river


The flow between river and runoff is computed using the same formulation as in runoff cells using the surface gradient between runoff and river.

Boundary Conditions

In Runoff there is the option to define the boundary condition as a level or as a timeserie (tide). This level will be imposed at the boundary and if the user wishes a) the water will only exit if the water level is higher than the boundary level and no inflow is allowed or b) inflow is allowed if the boundary level is higher than water level.

Computation

Boundary fluxes are computed after the flow computation iteration.

The boundary flux is computed with celerity in both directions (x and y) where boundary face exists. 

Qi = - cel  *  Li * min(dh,h)

where cel is celerity = SQRT(g * h) where Li is cell length perpendicular to direction where dh is level difference, if negative, boundary level is higher than runoff level where h is water height


the water height in celerity is water column (maximum column between inside and outside) and height for Area is the minimum between the difference between levels (dh) and the water column (if boundary level higher, height is dh, otherwise is also dh except if boundary level is lower than topography and in that case the minimum is the water column).

Keywords

The keyword in Runoff_X.dat that connects the open boundary is: 

IMPOSE_BOUNDARY_VALUE     : 1

The keyword that defines the boundary level is: 

BOUNDARY_VALUE            : 100.

The open boundary computation can be limited to specific areas defining the maximum altimetry that the boundary will be open. This is specifically useful when one wants to open the surface water at flat areas where in fact the flux can go trough the boundaries of the watershed delimitation. 

MAX_DTM_FOR_BOUNDARY      : 1000.

Using a value of the latter keyword higher than the maximum altimetry found in the watershed will make the boundary open in all watershed.


To allow water to flow in if the boundary level is higher use this keyword connected. Otherwise the boundary level will behave as a wall that if boundary level is higher than it does not allow water to exit but dos not also allow it to enter. 

ALLOW_BOUNDARY_INFLOW     : 1

If the user wants to use a timeserie for imposing level (tide) than use this block where Piezometer6.dat is a time serie with level in time in the second column that the user will impose. 

<begin_boundary>
FILENAME                  : ..\General Data\Boundary Conditions\Piezometer6.dat
DATA_COLUMN               : 2
<end_boundary>

Discharges

In Runoff the discharges may be positive or negative (Runoff uses discharge flow) and are dealt with ModuleDischarges.

Computation

The discharges are initialized in Construct phase reading its locations and checking if inside boundaries.

In Modification phase, the several discharges flows are accounted and water volume updated. The computation is inside the water column iteration process. And integration variable integrates this flow for RunoffProperties.

Keywords

For discharges to be read in Discharges_X.dat the following keyword needs to exist in the Runoff_X.dat 

DISCHARGES : 1

Without these keyword no matter what is inside Discharges_X.dat it will not be read!


Other Features

How To Generate Manning Coefficients

Manning coefficients must be provided in runoff data file.

Options:

  • Use a constant value
  • Define a Manning's grid: One possible option is to associate Manning with land use classes (shape file). In this case can use MOHID GIS going to menu [Tools] \Longrightarrow [Shape to Grid Data] and provide:
(i) the grid (model grid)
ii) the land use shape file
iii) the corespondence between land use codes and Manning

Use Manning inicialization with Module FillMatrix standards in the block: 

<BeginOverLandCoefficient>
FILE_IN_TIME           : NONE
INITIALIZATION_METHOD  : ASCII_FILE
REMAIN_CONSTANT        : 1
DEFAULTVALUE           : 0.08
FILENAME               : ..\..\GeneralData\Runoff\Mannings200m_v2.dat 
<EndOverLandCoefficient>

Outputs

References

Data File

Keywords

Sample

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