B. Noël, Soares S., Y. Zech Université catholique de Louvain

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WP3 : Flood Propagation WP3 : Flood Propagation Computation On The ‘Isolated Computation On The ‘Isolated Building Test Case’ And The Building Test Case’ And The Model City Flooding Model City Flooding Experiment Experiment B. Noël, Soares S., Y. Zech Université catholique de Louvain

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WP3 : Flood Propagation Computation On The ‘Isolated Building Test Case’ And The ‘ Model City Flooding Experiment ’. B. Noël, Soares S., Y. Zech Université catholique de Louvain. Overview. Numerical Model The ‘Isolated Building Benchmark’ Numerical modelling Numerical results - PowerPoint PPT Presentation

Transcript of B. Noël, Soares S., Y. Zech Université catholique de Louvain

Page 1: B. Noël, Soares S., Y. Zech Université catholique de Louvain

WP3 : Flood PropagationWP3 : Flood PropagationComputation On The ‘Isolated Computation On The ‘Isolated

Building Test Case’ And The ‘Building Test Case’ And The ‘Model Model City Flooding Experiment City Flooding Experiment ’’

B. Noël, Soares S., Y. ZechUniversité catholique de Louvain

Page 2: B. Noël, Soares S., Y. Zech Université catholique de Louvain

IMPACT - 3rd Workshop Novembre 2003

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OverviewOverview

• Numerical Model• The ‘Isolated Building Benchmark’

– Numerical modelling– Numerical results– Sensitivity analysis

• The ‘Model City Benchmark’– Numerical modelling– Numerical results– Sensitivity analysis

Page 3: B. Noël, Soares S., Y. Zech Université catholique de Louvain

IMPACT - 3rd Workshop Novembre 2003

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OverviewOverview

• Numerical Model• The ‘Isolated Building Benchmark’

– Numerical modelling– Numerical results– Sensitivity analysis

• The ‘Model City Benchmark’– Numerical modelling– Numerical results– Sensitivity analysis

Page 4: B. Noël, Soares S., Y. Zech Université catholique de Louvain

IMPACT - 3rd Workshop Novembre 2003

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Numerical ModelNumerical Model

• 2D finite-volume method• First-order scheme• Flux evaluated by Roe’s scheme• Non-Cartesian grids allowed

‘Soares Frazão S., 2002 PHD Thesis ’

Page 5: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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OverviewOverview

• Numerical Model• The ‘Isolated Building Benchmark’

– Numerical modelling– Numerical results– Sensitivity analysis

• The ‘Model City Benchmark’– Numerical modelling– Numerical results– Sensitivity analysis

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical modelling (2-mesh grid)– Grid :

Square meshes

Quadrangular meshes

Page 7: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical modelling– Building neighbouring

Page 8: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical modelling– Grid mean size : 5 x 5 cm– CFL number : 0.9–Time duration : ± 2 h– CPU : AMD XP1800+ (128Mb)

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical results

Page 10: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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0

0.05

0.1

0.15

0 5 10 15 20 25 30t [s]

Zw

ate

r [m

]

G1 - experimentG1 - numerical

The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical results– Water level :

Page 11: B. Noël, Soares S., Y. Zech Université catholique de Louvain

IMPACT - 3rd Workshop Novembre 2003

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical results– Water level (t = 10 s) :

Page 12: B. Noël, Soares S., Y. Zech Université catholique de Louvain

IMPACT - 3rd Workshop Novembre 2003

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical results– Velocity field (t = 5 s) :

Numerical ExperimentalNoël, Spinewine 2003 - UCL

Page 13: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Numerical results– Velocity Intensity (t = 5 s) :

Numerical ExperimentalNoël, Spinewine 2003 - UCL

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Water Level at G2

0

0.02

0.04

0.06

0.08

0.1

0.12

0.14

0 5 10 15 20 25 30

t [s]

h [

m]

Experimentn = 0.008n = 0.01n = 0.012

The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Sensitivity analysis– Manning roughness coefficient

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The ‘Isolated Building The ‘Isolated Building Benchmark’Benchmark’

• Sensitivity analysis– Initial downstream water-depth

Water Level at G2

0

0.02

0.04

0.06

0.08

0.1

0.12

0.14

0 5 10 15 20 25 30

t [s]

h [

m]

Experimenth0 = 0.0mh0 = 0.01mh0 = 0.02m

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OverviewOverview

• Numerical Model• The ‘Isolated Building Benchmark’

– Numerical modelling– Numerical results– Sensitivity analysis

• The ‘Model City Benchmark’– Numerical modelling– Numerical results– Sensitivity analysis

Page 17: B. Noël, Soares S., Y. Zech Université catholique de Louvain

IMPACT - 3rd Workshop Novembre 2003

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling (channelled)

Mesh XXX

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling (10-mesh grid)

Mesh XXX

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling (original)

Mesh XXX

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling (10-mesh grid)

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling– Topography reconstruction

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling– Upstream reservoir

• Dimensions : unknown but seen on picture

about 1 meter of longitudinal length

lateral bed level similar to the bed level of upstream end of channel

• Best way to model : decrease bed level of feeding tank and fill it with water at rest

numerical crash at corner of reservoir

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling– Upstream reservoir

• bed level of the upstream end of channel• Inlet introduced at the upstream end of the

prolonged channel

Inlet

Walls

Walls

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical modelling– Grid mean size : 2.5 x 2.5 cm– CFL number : 0.1– Time duration : ± 5h.– Computer : AMD XP1800+ (128Mb)

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical results– Test cases 1a & 1b (t = 20 s) :

Staggered layer :

- velocity decreased

- water level increased in the building layer

Page 26: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical results– Test cases 2a & 2b (t = 20 s) :

Staggered layer :

- velocity decreased

- water level increased in the building layer

Page 27: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical results– Test cases 3a & 3b (t = 20 s) :

Low inflow :

60 l/s

High inflow :

100 l/s

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical results– Test cases 4a & 4b (t = 20 s) :

Buildings as bed elevation (15 cm):

Page 29: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Numerical results– Test cases 4a & 4c (t = 20 s) :

High friction

(n = 10 s/m1/3):

- water lost in buildings

- maximum water level moves downstream and is a few decreased

Page 30: B. Noël, Soares S., Y. Zech Université catholique de Louvain

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The ‘Model City Benchmark’The ‘Model City Benchmark’

• Sensitivity analysis– Downstream boundary condition

Water Level at G10

0

0.005

0.01

0.015

0.02

0.025

0 10 20 30 40 50 60

t [s]

h [

m]

average slopezero slope

Page 31: B. Noël, Soares S., Y. Zech Université catholique de Louvain

WP3 : Flood PropagationWP3 : Flood PropagationComputation On The ‘Isolated Computation On The ‘Isolated

Building Test Case’ And The ‘Building Test Case’ And The ‘Model Model City Flooding Experiment City Flooding Experiment ’’

B. Noël, Soares S., Y. ZechUniversité catholique de Louvain