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A state of the art review on mathematical modelling of flood propagation

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A state of the art review on mathematical modelling of flood propagation First IMPACT Workshop Wallingford, UK, 16-17 May 2002 F. Alcrudo University of Zaragoza – PowerPoint PPT presentation

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Title: A state of the art review on mathematical modelling of flood propagation


1
A state of the art review on mathematical
modelling offlood propagation
  • First IMPACT Workshop
  • Wallingford, UK,
  • 16-17 May 2002

F. Alcrudo University of Zaragoza Spain
2
Overview
  • The modelling process
  • Mathematical models of flood propagation
  • Solution of the Model equations
  • Validation

3
The modelling process
  • Understanding of flow characteristics
  • Formulation of mathematical laws
  • Numerical methods
  • Programming
  • Validation of model by comparison of results
    against real life data
  • Prediction Ability to FOREtell not to PASTtell

4
The modelling process
REALITY
Analisis
Computer Simulation Validation
Data uncertainties
Conceptual errors uncertainties
Discretization errors
MATHEMATICAL MODEL
COMPUTER MODEL
Numerics Implementation
5
The flow characteristics
  • 3-D
  • time dependent
  • incompresible
  • free surface
  • fixed bed
  • (no erosion deposition)
  • turbulent (very high Re)

6
Mathematical models
  • 3-D Navier-Stokes (DNS)
  • Chimerical
  • 3-D RANS
  • Turbulence models ?
  • Still too complex
  • Euler (inviscid)
  • Simpler, requires much less resolution
  • Could be an option soon

7
Mathematical models
  • Tracking of the free surface
  • VOF method (Hirt Nichols 1981)
  • MAC method (Welch et al. 1966)
  • Moving mesh methods

8
NS, RANS Euler
  • 2-D dam break and overturning waves
  • Zwart et al. 1999
  • Mohapatra et al. 1999
  • Stansby et al. (Potential) 1998
  • Stelling Busnelli 2001...
  • River flows
  • Casulli Stelling (Q-hydrostatic) 1998
  • Sinha et al. 1998, Ye McCorquodale 1998...

9
Simplified mathematical models
  • Shallow Water Equations (SWE)
  • Depth integrated NS
  • Mass and momentum conservation in horizontal
    plane
  • Pseudo compressibility

10
  • Inertial Pressure fluxes
  • Convective Momentum transport
  • Hydrostatic pressure distribution

11
  • Diffusive fluxes
  • Fluid viscosity
  • Turbulence
  • Velocity dispersion (non-uniformity)

Benqué et al. (1982)
12
  • Sources
  • Bed slope
  • Bed friction (empirical)
  • Infiltration / Aportation (Singh et al. 1998
    Fiedler et al. 2000)

13
  • 1-D SWE models

14
Issues in SWE models
  • Corrections for non-hydrostatic pressure,
    non-zero vertical movement
  • Boussinesq aproximation (Soares 2002)
  • Stansby and Zhou 1998 (in NS-2D-V)
  • Flow over vertical steps (Zhou et al. 2001)
  • (Exact solutions Alcrudo Benkhaldoun 2001)
  • Corrections for non-uniform horizontal velocity ?
  • (Dispersion effects)

15
Issues in SWE models (cont.)
  • Turbulence modelling in 2D-H
  • Nadaoka Yagi (1998) river flow
  • Gutting Hutter (1998) lake circulation (K-e)
  • Gelb Gleeson (2001) atmospheric SWE model
  • Bottom friction
  • Non-uniform unsteady friction laws ?
  • Distributed friction coefficients (Aronica et al.
    1998)
  • Bottom induced horizontal shear generation
    (Nadaoka Yagi 1998)

16
Simplified models
  • Kinematic diffusive models
  • Arónica et al. (1998)
  • Horrit and Bates (2001)
  • Flat Pond models
  • Tous dam break inundation (Estrela 1999)

17
Flat pond model of Rio Verde area (Estrela 1999)
18
Solution of the model equations(Restricted to
SWE models)
  • Discretization strategies
  • Mesh configurations
  • Numerical schemes
  • Space-Time discretizations
  • Front propagation
  • Source term integration
  • Wetting and drying

19
Discretization strategies
  • Finite differences
  • Decaying use (less flexible)
  • Usually structured grids
  • Scheme development/testing (Liska Wendroff
    1999, Glaister 2000 ...)
  • Practical appications (Bento-Franco 1996,
    Heinrich et al. 2000, Aureli et al. 2000)

20
  • Finite volumes
  • Both structured unstructured grids
  • Cell-centered or cell-vertex
  • Extremely flexible intuitive
  • Many practical applications (CADAM 1998-1999,
    Brufau et al. 2000, Soares et al. 1999, Zoppou
    1999)
  • Most popular

21
  • Finite elements
  • Variational formulation
  • Conceptually more complex
  • More difficult front capture operator (Ribeiro et
    al. 2001, Hauke 1998)
  • Practical applications
  • Hervouet 2000, Hervouet Petitjean 1999
  • Supercritical / subcritical, tidal flows, Heniche
    et al. 2000

22
Mesh configurations
  • Structured
  • Cartesian / Boundary fitted (mappings)
  • Less flexible / Easy interpolation
  • Unstructured
  • Flexible but Indexing / Bookkeeping overheads
  • More elaborated Interpolation (Sleigh 1998,
    Hubbard 1999)
  • Easy refining (Sleigh 1998, Soares 1999) and
    adaptation (Benkhaldoun 1994, Ivanenko et al.
    2000)
  • Quad-Tree

23
Mesh configurations
  • Quad-Tree
  • Cartesian with grid refining/adaptation
  • Hierarchical structure / Interpolation operators
  • Needs bookkeeping
  • Usually specific boundary treatments (Cartesian
    cut-cell approach Causon et al. 2000, 2001)
  • Practical applications (Borthwick et al. 2001)

24
Numerical schemes
  • Space Time discretization
  • Space discretizations
  • Time integration of resulting ODE
  • Time integration
  • Explicit usu 2-step, Runge-Kutta (Subject to CFL
    constraints)
  • Implicit (not frequent)

25
  • Front propagation
  • Shock capturing or through methods
  • Approximate Riemann solvers (Most popular Roe,
    WAF second)
  • Higher order interpolations limiters (either
    flux or variables), TVD, ENO
  • Mostly in FV FD but progressively incorporated
    into FE (Sheu Fhang 2001)
  • Plenty of methods (or publications)

26
  • Multidimensional upwind
  • Wave recognition schemes (opposed to classical
    dimensional splitting)
  • Consistent Higher resolution of wave patterns
  • Usually in unstructured (cell vertex) grids
    (mostly triangles)
  • Considerably more expensive
  • Hubbard Baines 1998, Brufau Garcianavarro
    2000 ...

27
  • Source term integration (bed slope)
  • Flow is source term dominated in most practical
    applications
  • Flux discretization must be compatible with
    source term
  • Source term upwinding (Bermudez Vazquez 1994)
  • Pressure splitting (Nujic 1995)
  • Flux lateralisation (Capart et al. 1996, Soares
    2002)
  • Surface gradient method (Zhou et al. 2001)
  • Discontinuous bed topography (Zhou et al. 2002)

28
  • Wetting-drying
  • Intrinsic to flood propagation scenarios
  • Instabilities due to coupling with friction
    formulae and to sloping bottom (Soares 2002)
  • Threshold technique (CADAM 1998), simple, widely
    used but no more than a trick
  • Fictitious negative depth (Soares 2002)
  • Boundary treatment at interface (Bento-Franco
    1996, Sleigh 1998), modification of bottom
    function (Brufau 2000)
  • Bottom function modification, ALE (Quecedo and
    Pastor (2002) in Taylor Galerkin FE

29
Validation
  • Model accuracy
  • Differences between model output real life
  • Determined with respect to experimental data
  • Accuracy loss
  • Uncertainty Due to lack of knowledge
  • Errors Recognizable defficiencies

30
  • Main losses of accuracy in flood propagation
    models
  • Errors in the math description (SWE or worse)
  • Uncertainties in data (topography, friction
    levels, initial flood characteristics)
  • Additional errors
  • Inaccurate solution of model equations (grid
    refining)

31
  • Much validation work of numerical methods against
    analytical /other numerical solutions
  • Chippada et al., Hu et al., Aral et al. 1998
  • Holdhal et al., Liska Wendroff , Zoppou
    Roberts etc ... 1999
  • Causon et al., Wang et al., Borthwick et al. etc
    ... 2001
  • Validation against data from laboratory
    experiments
  • CADAM work, Tseng et al. 2000, Sakarya Toykay
    2000 etc ...
  • Validation against true real flooding data
  • CADAM 1999, Hervouet Petitjean (1999), Hervouet
    (2000), Horritt (2000), Heinrich et al. (2001),
    Haider (2001)
  • Sensitiviy analysis (usually friction)
  • Urban flooding ?

32
Conlusions
  • Present feasible mathematical descriptions of
    flood propagation are known to be erroneous but
    ...
  • Better mathematical models are still far ahead
  • The level of accuracy of present models has not
    yet been thoroughly assessed
  • There are enough methods at hand to solve the
    mathematical models (most are good enough)
  • Exhaustive validation programs against real data
    are needed
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