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Case study of applying Delft3D FM in the
Waal River, the Netherlands
Delft3D User Days 2017
Roy van Weerdenburg
30 October 2017
Objectives of this study
 Analysis of the differences between D-Flow FM and Delft3D-FLOW
 Analysis of the modelling results of D-Flow FM compared to Delft3D-FLOW
 Hydrodynamics
 Morphology
 Discover new possibilities in D-Flow FM
 Get experience with the new modelling suite
Most important differences
 Flexible mesh: no rows and columns in the grid anymore ((m,n) coordinates)
 Allows for local refinement or coarsening of the grid
 ADI-solver no longer applicable in D-Flow FM
 Dynamic time step reduction based on CFL-condition
 All geometric model input in model-independent coordinates
 Independent of the grid
 DeltaShell is the GUI of D-Flow FM
Model-independent coordinates
 Grid enclosure is replaced by defining dry areas
 Currently no opportunity to see how exactly the input files are projected onto
the grid
D-Flow FM:
Spatial coordinates (*.xyz)
Delft3D-FLOW:
Directly projected on the grid
Validation models
 Deltares made many validation models to assess the performance of several
functionalities
 These models are very simplified situations
 e.g. a rectangular gutter or one single bend
 Investigate what the combined effect is in a more
complex model of a lowland river
Model set-up
 Delft3D FM Suite 2017 HMWQ (1.3.2.37884): β-version
 Set-up similar models in Delft3D-FLOW and D-Flow FM
 The new models are based on the DVR-model of the Rhine branches
 The same curvilinear grid was used in both models
 Input files were generated by the newest available version of Baseline
Hydrodynamic modelling
 Constant discharge: Q = 1600 m3/s (Lobith 2350 m3/s)
Hydrodynamic modelling
 Difference in stationary water level at the observation points (Q = 1600 m3/s)
Hydrodynamic modelling
 These differences are caused by
 The information in input files from Baseline
 Differences in the numerical solver
 Matlab toolbox to convert a Delft3D-FLOW model into D-Flow FM input files
Hydrodynamic modelling
 dflowfmConverter.m
Hydrodynamic modelling
 Difference in stationary water level at the observation points (Q = 1600 m3/s)
 Converted input files
Hydrodynamic modelling: first conclusions
 Differences in water level are partially caused by differing input files from
Baseline
 The new numerical solver calculates different water levels and the maximum
difference is approximately 5 cm during average discharge
Hydrodynamic modelling
 Constant discharge: Q = 820 m3/s (Lobith 1020 m3/s)
 This discharge is exceeded 95% of time
 Flow limited to the conveyance channel
 No influence of weirs and flood plains
Hydrodynamic modelling
 Difference in stationary water level at the observation points (Q = 820 m3/s)
Hydrodynamic modelling
 Difference in water level is now approximately 4.5 cm
 Relates to the reduction in water depth
 We consider the water levels and the flow velocities in four cross sections
Hydrodynamic modelling
KM 880
KM 885KM 902KM 904
left bank right bank
Hydrodynamic modelling
 The differences in flow velocities also occur at the downstream end
Hydrodynamic modelling
 Flow velocity vectors: blue = Delft3D-FLOW red = D-Flow FM
Hydrodynamic modelling: some conclusions
 The water level profiles in the cross sections look very similar
 Near the edges of the conveyance channel we see some differences in the
flow velocities
Hydrodynamic modelling: secondary flow
 The secondary flow pattern is in both models based on the primary flow, using
the same equations
Morphology
 Hydrodynamics directly affects the morphologic development
 Same numerical procedure for sediment transport rates in both models
 Upwind approach (default option)
Conclusions
 The input files as generated by Baseline cause water level differences of a
few centimeters
 The new numerical solving method computes water depths that differ up to 5
centimeters compared to the ADI-solver (average discharge)
 The new numerical solving method computes a slightly different pattern of
flow velocities in the cross sections
 The differences in morphological development are directly linked to the
hydrodynamics, because the equations and the solving method are the same
Conclusions
 The DeltaShell GUI provides much insight into the model components and
input may be changed easily within the interface
 Next step: Use field measurements to calibrate D-Flow FM model
Any further questions?
Roy van Weerdenburg
Student Hydraulic Engineering at Delft University of Technology
Intern at Royal Haskoning DHV
email: roy.van.weerdenburg@rhdhv.com
r.j.a.vanweerdenburg@student.tudelft.nl
phone: +31 6 46505353
Please contact me!

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DSD-INT 2017 Delft3D FM hydrodynamic and morphological modelling, Waal River, The Netherlands - van Weerdenburg

  • 1. Case study of applying Delft3D FM in the Waal River, the Netherlands Delft3D User Days 2017 Roy van Weerdenburg 30 October 2017
  • 2. Objectives of this study  Analysis of the differences between D-Flow FM and Delft3D-FLOW  Analysis of the modelling results of D-Flow FM compared to Delft3D-FLOW  Hydrodynamics  Morphology  Discover new possibilities in D-Flow FM  Get experience with the new modelling suite
  • 3. Most important differences  Flexible mesh: no rows and columns in the grid anymore ((m,n) coordinates)  Allows for local refinement or coarsening of the grid  ADI-solver no longer applicable in D-Flow FM  Dynamic time step reduction based on CFL-condition  All geometric model input in model-independent coordinates  Independent of the grid  DeltaShell is the GUI of D-Flow FM
  • 4. Model-independent coordinates  Grid enclosure is replaced by defining dry areas  Currently no opportunity to see how exactly the input files are projected onto the grid D-Flow FM: Spatial coordinates (*.xyz) Delft3D-FLOW: Directly projected on the grid
  • 5. Validation models  Deltares made many validation models to assess the performance of several functionalities  These models are very simplified situations  e.g. a rectangular gutter or one single bend  Investigate what the combined effect is in a more complex model of a lowland river
  • 6. Model set-up  Delft3D FM Suite 2017 HMWQ (1.3.2.37884): β-version  Set-up similar models in Delft3D-FLOW and D-Flow FM  The new models are based on the DVR-model of the Rhine branches  The same curvilinear grid was used in both models  Input files were generated by the newest available version of Baseline
  • 7. Hydrodynamic modelling  Constant discharge: Q = 1600 m3/s (Lobith 2350 m3/s)
  • 8. Hydrodynamic modelling  Difference in stationary water level at the observation points (Q = 1600 m3/s)
  • 9. Hydrodynamic modelling  These differences are caused by  The information in input files from Baseline  Differences in the numerical solver  Matlab toolbox to convert a Delft3D-FLOW model into D-Flow FM input files
  • 11. Hydrodynamic modelling  Difference in stationary water level at the observation points (Q = 1600 m3/s)  Converted input files
  • 12.
  • 13. Hydrodynamic modelling: first conclusions  Differences in water level are partially caused by differing input files from Baseline  The new numerical solver calculates different water levels and the maximum difference is approximately 5 cm during average discharge
  • 14. Hydrodynamic modelling  Constant discharge: Q = 820 m3/s (Lobith 1020 m3/s)  This discharge is exceeded 95% of time  Flow limited to the conveyance channel  No influence of weirs and flood plains
  • 15. Hydrodynamic modelling  Difference in stationary water level at the observation points (Q = 820 m3/s)
  • 16. Hydrodynamic modelling  Difference in water level is now approximately 4.5 cm  Relates to the reduction in water depth  We consider the water levels and the flow velocities in four cross sections
  • 19.
  • 20. Hydrodynamic modelling  The differences in flow velocities also occur at the downstream end
  • 21. Hydrodynamic modelling  Flow velocity vectors: blue = Delft3D-FLOW red = D-Flow FM
  • 22. Hydrodynamic modelling: some conclusions  The water level profiles in the cross sections look very similar  Near the edges of the conveyance channel we see some differences in the flow velocities
  • 23. Hydrodynamic modelling: secondary flow  The secondary flow pattern is in both models based on the primary flow, using the same equations
  • 24. Morphology  Hydrodynamics directly affects the morphologic development  Same numerical procedure for sediment transport rates in both models  Upwind approach (default option)
  • 25. Conclusions  The input files as generated by Baseline cause water level differences of a few centimeters  The new numerical solving method computes water depths that differ up to 5 centimeters compared to the ADI-solver (average discharge)  The new numerical solving method computes a slightly different pattern of flow velocities in the cross sections  The differences in morphological development are directly linked to the hydrodynamics, because the equations and the solving method are the same
  • 26. Conclusions  The DeltaShell GUI provides much insight into the model components and input may be changed easily within the interface  Next step: Use field measurements to calibrate D-Flow FM model
  • 27. Any further questions? Roy van Weerdenburg Student Hydraulic Engineering at Delft University of Technology Intern at Royal Haskoning DHV email: roy.van.weerdenburg@rhdhv.com r.j.a.vanweerdenburg@student.tudelft.nl phone: +31 6 46505353 Please contact me!