Surface model (Water Overlay): Difference between revisions

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__NOTOC__
__NOTOC__
The [[Water Module]]'s primary function is the simulation of the 2-dimensional flow of water on the surface. In order to simulate flowing water, the project area is discretized into x by y cells, based on the configured [[grid cell size]].  
==Computation==
 
The [[Water Module]]'s primary function is simulating two-dimensional flow of water along the surface. In order to do this, the project area is first discretized into ''x'' by ''y'' cells depending on the configured [[grid cell size]]. Secondly, a set of rules is required that describes the behavior of the flow. This is done through a second-order semi-discrete central-upwind scheme produced by Kurganov and Petrova (2007)<ref name="Kurganov2"/>, which is based on the 2-D Saint-Venant equations (a.k.a. shallow water equations):
Secondly a model is required which describes the rules that need to be followed. For this we use the two-dimensional Saint-Venant system, which reads:
[[File:2D-Saint-Venant_system.png|left]]
[[File:2D-Saint-Venant_system.png|left]]
where:
where
: h<sub>t</sub> = water depth at time t
: h<sub>t</sub> = water depth at time t
: u<sub>t</sub> = velocity in the x direction at time t
: u<sub>t</sub> = velocity in the x direction at time t
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: g = gravitational constant
: g = gravitational constant
{{clear|left}}
{{clear|left}}
In the {{software}} this model is implemented using the ''Well Balanced Positivity Preserving Central-Upwind Scheme'' described in Kurganov and Petrova (2007)<ref name="Kurganov2"/>.
For more information about the implementation, see [[Surface_flow_formula_(Water_Overlay)|Surface flow formula]].


[[File:Waterlevel_schematic.png|right|x200px|frame|For each grid cell:<br>B = bottom elevation<br>h = water depth<br>w = water surface elevation]]
[[File:Waterlevel_schematic.png|right|x200px|frame|For each grid cell:<br>B = bottom elevation<br>h = water depth<br>w = water surface elevation]]
The implemented method rewrites the '''h''' from the original Saint-Venant system to <code>w = h + B</code>. See the image on the right for clarification on the terms water level (w), surface (or bottom) elevation (B) and water depth(h).
This method deviates from the original Saint-Venant equations in that it approaches the system in terms of water surface elevation (''w = h + B'') and flux (''hu'' and ''hv''), rather than just the water depth (''h''). The image on the right aims to clarify on the various terms. More technical information on the {{software}}'s implementation of the ''Well-Balanced Positivity Preserving Central-Upwind Scheme'' can be found [[Surface_flow_formula_(Water_Overlay)|here]].


====Flowing water====
====Flowing water====
Based on variations in the surface elevation and water levels, which may cause unbalance, water will start flowing, until it eventually is balanced in terms of water level and fluxes ''hu'' and ''hv''.
Imbalances in the water surface elevation among grid cells drive the flow of water in the model until a state of equilibrium is reached in terms of ''w'' and flux.
 
{{clear|right}}


===Water level initialization===
===Water level initialization===
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The terrain height is defined by the [[terrain height]] in the project. The surface height is further influenced by the height of constructions present in the project (bounded by [[Design flood elevation m model attribute (Water Overlay)|DESIGN_FLOOD_ELEVATION_M]]) and by the [[Breach height (Water Overlay)|BREACH_HEIGHT]] of [[Breach (Water Overlay)|breaches]].
The terrain height is defined by the [[terrain height]] in the project. The surface height is further influenced by the height of constructions present in the project (bounded by [[Design flood elevation m model attribute (Water Overlay)|DESIGN_FLOOD_ELEVATION_M]]) and by the [[Breach height (Water Overlay)|BREACH_HEIGHT]] of [[Breach (Water Overlay)|breaches]].


==Notes==
===Notes===
* Water can be added to and removed from the described surface system by the [[Rain model (Water Overlay)|rain]], [[Evaporation model (Water Overlay)|evaporation]] and [[Infiltration model (Water Overlay)|infiltration model]], as well as certain [[Hydraulic structures (Water Overlay)|hydraulic structures]], [[Sewer model (Water Overlay)|sewer]]s and [[Breach (Water Overlay)|breach]]es.
* Water can be added to and removed from the described surface system by the [[Rain model (Water Overlay)|rain]], [[Evaporation model (Water Overlay)|evaporation]] and [[Infiltration model (Water Overlay)|infiltration model]], as well as certain [[Hydraulic structures (Water Overlay)|hydraulic structures]], [[Sewer model (Water Overlay)|sewer]]s and [[Breach (Water Overlay)|breach]]es.
* Underground flow uses a different flow system and formula's, described in [[Underground model (Water Overlay)|underground model]].
* Underground flow uses a different flow system and formula's, described in [[Underground model (Water Overlay)|underground model]].

Revision as of 10:06, 24 June 2019

Computation

The Water Module's primary function is simulating two-dimensional flow of water along the surface. In order to do this, the project area is first discretized into x by y cells depending on the configured grid cell size. Secondly, a set of rules is required that describes the behavior of the flow. This is done through a second-order semi-discrete central-upwind scheme produced by Kurganov and Petrova (2007)[1], which is based on the 2-D Saint-Venant equations (a.k.a. shallow water equations):

2D-Saint-Venant system.png

where

ht = water depth at time t
ut = velocity in the x direction at time t
vt = velocity in the y direction at time t
Bx = slope in the x direction
By = slope in the y direction
g = gravitational constant
For each grid cell:
B = bottom elevation
h = water depth
w = water surface elevation

This method deviates from the original Saint-Venant equations in that it approaches the system in terms of water surface elevation (w = h + B) and flux (hu and hv), rather than just the water depth (h). The image on the right aims to clarify on the various terms. More technical information on the Tygron Platform's implementation of the Well-Balanced Positivity Preserving Central-Upwind Scheme can be found here.

Flowing water

Imbalances in the water surface elevation among grid cells drive the flow of water in the model until a state of equilibrium is reached in terms of w and flux.

Water level initialization

In theory, each grid cell can have a unique water level and accompanying water depth. In practice though, water levels are often initialized for large groups of cells, since it is assumed that a particular area within the project area has a given water level. Therefore, the surface water level is initialized based on hydrological features. We make the following distinction:

For all water terrains, the amount of water set on the grid cell is such that the resulting water level in that location is equal to the WATER_LEVEL attribute provided by the Water level area. If no water level area is overlapping that grid cell, or the water level is below the surface elevation of the grid cell, the water depth is assumed to be 0 and the water level equal to the surface elevation.

For the second case, inundation areas have been added to the model. Water is placed in all grid cells which are covered by an inundated area, (regardless of the terrain type in that location, in contrast to the water level areas), such that the resulting water level is again equal to the inundation area's INUNDATION_LEVEL attribute. If no inundation area is overlapping that grid cell, or the inundation level is below the surface elevation of the grid cell, the water depth is assumed to be 0 and the water level equal to the surface elevation.

The terrain height is defined by the terrain height in the project. The surface height is further influenced by the height of constructions present in the project (bounded by DESIGN_FLOOD_ELEVATION_M) and by the BREACH_HEIGHT of breaches.

Notes

Related formulas

Related models

References

  1. Kurganov A, Petrova G (2007) ∙ A Second-Order Well-Balanced Positivity Preserving Central-Upwind Scheme for the Saint-Venant System ∙ found at: http://www.math.tamu.edu/~gpetrova/KPSV.pdf (last visited 2019-04-11)

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