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Introduction Modeling and Simulation Summary Modeling and Simulation of Earthquakes, Soils, Structures and their Interaction Boris Jeremi´ c Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence Berkeley National Laboratory, Berkeley, CA Best PSHANI Château de Cadarache, France Mai 2018 Jeremi´ c et al. MS-ESSI

Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

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Page 1: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Modeling and Simulation ofEarthquakes, Soils, Structures and

their Interaction

Boris JeremicHexiang Wang, Han Yang, Maxime Lacour, Yuan Feng

University of California, Davis, CALawrence Berkeley National Laboratory, Berkeley, CA

Best PSHANIChâteau de Cadarache, France

Mai 2018

Jeremic et al.

MS-ESSI

Page 2: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Outline

IntroductionMotivation

Modeling and SimulationSeismic MotionsInelasticity

Summary

Jeremic et al.

MS-ESSI

Page 3: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Motivation

Outline

IntroductionMotivation

Modeling and SimulationSeismic MotionsInelasticity

Summary

Jeremic et al.

MS-ESSI

Page 4: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Motivation

Motivation

I Improve safety and economy of infrastructure objects

I Improve numerical modeling and simulation forinfrastructure objects, nuclear installations

I Quality assurance, verification & validation

I Practical numerical modeling and simulation system

I Select level of sophistication numerical models to analyzeearthquake soil structure interaction of nuclear installations

Jeremic et al.

MS-ESSI

Page 5: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Motivation

Uncertainties

I Modeling uncertainty, introduced by simplifyingassumptions, need for capability to perform lower andhigher level of sophistication modeling and simulation

I Parametric uncertainty, propagation of uncertainty inmaterial K ep and loads F (t), through:Mui + Cui + K epui = F (t), resulting in PDFs and CDFs forσij , εij , ui , ui , ui

I Le doute n’est pas un état bien agréable, mais l’assuranceest un état ridicule. (François-Marie Arouet, Voltaire)

Jeremic et al.

MS-ESSI

Page 6: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Motivation

Flow of Seismic Energy

I Seismic energy input into the ESSI system

I Seismic energy dissipation outside of ESSI systemI Wave reflectionsI Structural oscillations, wave radiation

I Seismic energy dissipation within ESSI systemI Viscous effects (soil, fluid containers...)I Inelastic effects (soil, concrete, contacts, dissipators...)

I Numerical energy dissipation and production

Jeremic et al.

MS-ESSI

Page 7: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Outline

IntroductionMotivation

Modeling and SimulationSeismic MotionsInelasticity

Summary

Jeremic et al.

MS-ESSI

Page 8: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Stress Test Motions and Regional Scale Motions

I Stress test motionsI 3D - 6C, Haskel’s solution for plane harmonic wavesI 3D - 3×1CI 3D - 1CI 1D - 1C

I High fidelity (?) free field regional scale seismic motionsusing SW4, courtesy of Dr. Rodgers, Dr. Pitarka andDr. Petersson (LLNL)

I Knowledge of geology and the site is important

Jeremic et al.

MS-ESSI

Page 9: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Example Structure, a Small Modular Reactor (SMR)

Jeremic et al.

MS-ESSI

Page 10: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Stress Test Motions

I Variation in inclination, frequency, energy and durationI Try to "break" the system, shake-out strong and weak links

L oL w

L oL w

Jeremic et al.

MS-ESSI

Page 11: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Free Field, Variation in Input Wave Angle, f = 5Hz

(MP4)

Jeremic et al.

MS-ESSI

Page 12: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

SMR ESSI, Variation in Input Wave Angle, f = 5Hz

(MP4)

Jeremic et al.

MS-ESSI

Page 13: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Free Field, Variation in Input Frequency, θ = 60o

(MP4)

Jeremic et al.

MS-ESSI

Page 14: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

SMR ESSI, Variation in Input Frequency, θ = 60o

(MP4)

Jeremic et al.

MS-ESSI

Page 15: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

SMR ESSI, Variation in Input Frequency, REAL TIME

(MP4)

Jeremic et al.

MS-ESSI

Page 16: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Free Field vs ESSI - Different Frequencies

0.0 0.2 0.4 0.6 0.8 1.0Time [s]

0.50

0.25

0.00

0.25

0.50

Ax [

g]

SMR Free field

0.0 0.2 0.4 0.6 0.8 1.0Time [s]

60

30

0

30

60

Ax [

g]

SMR Free field

0.0 0.2 0.4 0.6 0.8 1.0Time [s]

60

30

0

30

60

Ax [

g]

SMR Free field

0.0 0.2 0.4 0.6 0.8 1.0Time [s]

0.50

0.25

0.00

0.25

0.50

Az [

g]

SMR Free field

0.0 0.2 0.4 0.6 0.8 1.0Time [s]

60

30

0

30

60

Az [

g]

SMR Free field

0.0 0.2 0.4 0.6 0.8 1.0Time [s]

60

30

0

30

60

Az [

g]

SMR Free field

AB

C

Jeremic et al.

MS-ESSI

Acceleration response - Surface center point A

X direction

Z direction

(a) f = 1Hz θ = 60o (b) f = 5Hz θ = 60o (c) f = 10Hz θ = 60o

Page 17: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Example Regional Model (Rodgers et al, LLNL)

(MP4)

Jeremic et al.

MS-ESSI

Page 18: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Seismic Motions

Seismic Motions: SW4 to MS-ESSI

ESSI nodes

SW42ESSI

1 2 31 2 3 , ,( ), , ,u u u

72m×72m×56m36m embedded

300m ×300m ×100mGrid spacing ~ 5m

ESSI Box

30km × 14km ×5 km

Jeremic et al.

MS-ESSI

Page 19: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Inelasticity

Outline

IntroductionMotivation

Modeling and SimulationSeismic MotionsInelasticity

Summary

Jeremic et al.

MS-ESSI

Page 20: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Inelasticity

Inelastic Modeling for Components

I Soil elastic-plasticI Dry, single phaseI Unsaturated (partially saturated)I Fully saturated

I Contact, inelastic, soil/rock – foundationI Dry, single phase, normal/axial (hard and soft, gap

open/close), friction/shear (inelastic)I Fully saturated, suction and excess pressure (dynamic

buoyant force)I Structural inelasticity/damage

I Nonlinear/inelastic fiber beamI Nonlinear/inelastic fiber wall element

Jeremic et al.

MS-ESSI

Page 21: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Inelasticity

SMR: Inelastic ESSI Effects, Top Center

5 10 15 20Time [s]

1.00.50.00.51.0

A x [g

]

Elastic Inelastic

5 10 15 20Time [s]

1.00.50.00.51.0

A y [g

]

Elastic Inelastic

5 10 15 20Time [s]

1.00.50.00.51.0

A z [g

]

Elastic Inelastic

0 5 10 15 20Frequency [Hz]

0.00

0.05

0.10

FFT

A x [g

]

Elastic Inelastic

0 5 10 15 20Frequency [Hz]

0.00

0.05

0.10

FFT

A y [g

]

Elastic Inelastic

0 5 10 15 20Frequency [Hz]

0.00

0.05

0.10

FFT

A z [g

]

Elastic Inelastic

23

1

4(8)

5(9)6(10)

7(11)

12(13)

Jeremic et al.

MS-ESSI

Page 22: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Inelasticity

SMR: Accelerations Along Depth

40 30 20 10 0 10 20 30 40Width [m]

50

40

30

20

10

0

10

Dept

h [m

]

X=15

A

B

C

D

E

1g

0.0

2.5

5.0

7.5

10.0

12.5

15.0

17.5

20.0

Time [s]

40 30 20 10 0 10 20 30 40Width [m]

50

40

30

20

10

0

10

Dept

h [m

]

X=15

A

B

C

D

E

1g

0.0

2.5

5.0

7.5

10.0

12.5

15.0

17.5

20.0Tim

e [s]

40 30 20 10 0 10 20 30 40Width [m]

50

40

30

20

10

0

10

Dept

h [m

]

A

B

C

D

E

1g

0.0

2.5

5.0

7.5

10.0

12.5

15.0

17.5

20.0

Time [s]

40 30 20 10 0 10 20 30 40Width [m]

50

40

30

20

10

0

10

Dept

h [m

]

A

B

C

D

E

1g

0.0

2.5

5.0

7.5

10.0

12.5

15.0

17.5

20.0

Time [s]

Nonlinearsiteeffects

NonlinearESSIeffects

Jeremic et al.

MS-ESSI

Page 23: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Inelasticity

Energy Dissipation for an SMR

(MP4)

Jeremic et al.

MS-ESSI

Page 24: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Inelasticity

Stochastic Elastic-Plastic Finite Element MethodMui + Cui + K epui = F

(MP4)

Jeremic et al.

MS-ESSI

Page 25: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Outline

IntroductionMotivation

Modeling and SimulationSeismic MotionsInelasticity

Summary

Jeremic et al.

MS-ESSI

Page 26: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

Summary

I Seismic wave fields, 3C/6C, 3×1C and 1C, for ESSIbehavior

I Inelastic ESSI behavior, soil, contact and structure

I MS-ESSI Simulator: http://ms-essi.info

I Funding from and collaboration with the DOE, NRC,CNSC-CCSN, NSF and IAEA is greatly appreciated

I Collaborators: Feng, Han, Wang, Sinha, Lacour, Abell,Pisanò, Orbovic, McCallen, Petrone, McKenna

Jeremic et al.

MS-ESSI

Page 27: Modeling and Simulation of Earthquakes, Soils, …sokocalo.engr.ucdavis.edu/~jeremic/...Hexiang Wang, Han Yang, Maxime Lacour, Yuan Feng University of California, Davis, CA Lawrence

Introduction Modeling and Simulation Summary

US-DOE: ESSI of Nuclear Installations

The MS-ESSI Simulator: http://ms-essi.info

High Quality Validation test (UNR/UCD/LBNL)

Jeremic et al.

MS-ESSI