DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

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Delft, 3rd of November 2015 Frank Platzek (Deltares) Regina Patzwahl (BAW) mesoscale horizontal flow-field modelling at a channel-river junction Delft Software Days 2015 A behavioral study

Transcript of DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

Page 1: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

Delft, 3rd of November 2015

Frank Platzek (Deltares) Regina Patzwahl (BAW)

mesoscale horizontal flow-field modelling at a

channel-river junction

Delft Software Days 2015

A behavioral study

Page 2: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

Delft, 3rd of November 2015

Frank Platzek (Deltares) Regina Patzwahl (BAW)

more mesoscale horizontal flow-field modelling at a

channel-river junction

Delft Software Days 2015

A behavioral study

Page 3: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

Delft, 3rd of November 2015

Frank Platzek (Deltares) Regina Patzwahl (BAW)

Even more mesoscale horizontal flow-field modelling at

a channel-river junction

Delft Software Days 2015

A behavioral study

Page 4: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

Delft, 3rd of November 2015

Frank Platzek (Deltares) Regina Patzwahl (BAW)

Even more mesoscale horizontal flow-field modelling at

a (modified) channel-river junction

Delft Software Days 2015

A behavioral study

Page 5: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

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Outline

1. Geometrical setting

2. Field measurements

3. Scale model

4. Numerical model

5. Lessons learned 2013

6. Lessons learned 2014: Sheet pile wall modelling for beginners

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Introduction

1. Geometrical setting

2. Field measurements

3. Scale model

4. Numerical model

5. Lessons learned 2013

6. Lessons learned 2014: Sheet pile wall modelling for beginners

7. Another channel mouth geometry

8. Results from D-Flow FM

9. Lessons learned

So, what‘s new this

year?

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Geometrical setting

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Import of coarse AND fine material

into the channel mouth

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Geometrical setting

Topography in the vicinity of the channel mouth: groynes, dunes, sediment deposition on upstream side of the inlet, dregded fairway on the downstream side of the inlet

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Depth-averaged ADCP-measurements

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950 m³/s 1700 m³/s

1950 m³/s 840 m³/s

• Flow velocities increase with discharge

• Position of eddy is discharge independent

950 m³/s

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ADCP-cross profiles

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Source: Ing. Büro Schmid

• Horizontal eddy (2D-problem)

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Scale model

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4 km of river stretch = 67 m of model length

Length Scaling: 1:60

Height Scaling: 1:30

Stationary discharge conditions, non-movable gravel bed

Polystyrol tracer for investigation of transport processes

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Numerical model

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• 11 km long river model

• grid types:

• quadrilateral (dx=2m),

river axis aligned,

# of elements: ~ 800.000

• triangular (dx=1,5m),

# of elements: ~ 2.500 000

• discharge at inflow: 986 m³/s

• water level at outflow: 4.71 m

• const. hor. visc.0.0001 m²/s

• 1. and 2. order advection

• Smagorinsky off/ on

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Lessons learned 2013

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The modelled flow field in the junction domain is sensitive to:

advection scheme

Constant viscosity

Grid type

„Smagorinsky“

Lower velocities in

the eddy field

Numerical diffusion

„physically correct“?

Arguably improved?

Grid-dependent

results

advection scheme

= crucial choice!

Grid-dependent

results

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Lessons learned 2013

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Best modelling result

Quads, Hor. Visc.1.0*10-4

Perot 3, Smag Field measurements Scale model

• Excellent validation case for modelling mesoscale horizontal recirculation

• Unique combined set of field data, scale model and numerical model data

=> We follow the project with D-FLOW FM for studying purposes

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Lessons learned 2014

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Lessons learned 2014

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Lessons learned 2014

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/rough /smooth

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Lessons learned 2014

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Lessons learned 2014

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Lessons learned 2014

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Another channel mouth geometry

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1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river

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Another channel mouth geometry

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1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river 1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river

2. No bed load transport into channel mouth

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Another channel mouth geometry

Even more horizontal flow field modelling | Frank Platzek, Regina Patzwahl

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1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river 1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river

2. No bed load transport into channel mouth

3. No suspended load transport into channel mouth

Page 23: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

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Another channel mouth geometry

Even more horizontal flow field modelling | Frank Platzek, Regina Patzwahl

04/12/2015 Page 26

1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river 1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river

2. No bed load transport into channel mouth

3. No suspended load transport into channel mouth

Page 24: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

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Another channel mouth geometry

Even more horizontal flow field modelling | Frank Platzek, Regina Patzwahl

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1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river 1. Widening of cross-section in the main flow -> deposition of bed load and suspended load in the river

2. No bed load transport into channel mouth

3. No suspended load transport into channel mouth

Page 25: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

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1. Order advection 2. Order advection

Results from numerical model

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No stationarity observable Develops towards a

stable condition

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1. Order advection 2. Order advection 1. Order advection 2. Order advection

Results from numerical model

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No stationarity observable

Develops towards a

stable condition

Develops towards a

stable yet different

condition

Develops towards a

stable condition yet

different

+ Smagorinsky

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Results

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With the calibration of the current state we identified relevant dependencies of the

results on the model set-up

- the jokers helped to identify the „values“ of the „playing cards“

JOKER

measure

ments

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- the modified geometry led to

different dependencies…

Results

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JOKER

measure

ments

…and the values of the playing

cards are unknown

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Conclusion

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04/12/2015 Page 40

JOKER?

JOKER

Measure

ments

Very sensitive test case, on the border of model validity:

• point of flow separation

• location and orientation of the eddies

In particular for the modified geometry, where we also lack validation

data from the field.

=> a challenge for a numerical model(ler)

Page 30: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

Bundesanstalt für Wasserbau

76187 Karlsruhe, Germany

www.baw.de

Thank YOU for your attention

We want to thank for support:

The hydraulic lab (B. Hentschel) at BAW

Colleagues from W2 and W5 at BAW

Colleagues from Deltares

Page 31: DSD-INT 2015 - the next steps, horizontal flow field modelling using delft3 d fm

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A new channel mouth geometry

Even more horizontal flow field modelling | Frank Platzek, Regina Patzwahl

04/12/2015 Page 42

Analysis of As-is

state

Numerical model Scale model

Numerical model

Telemac3D

Investigation of possible

geometry variations:

Variant X

Fine-tuning of variant X

In respect to transport:

Xplus

Numerical model

Telemac2D

(J. Becker 2014)

Fine tuning of

variant Xplus in

respect to

hydraulic

matters:

Xplusplus

Xplus

Variant X

Xplusplus