dynamic analysis with examples – seismic analysis

34
OpenSees Days in Portugal @FEUP p. 1 Dynamic Analysis Notes Dr. André R. Barbosa July 03, 2014 OpenSees Days in Portugal @Faculdade de Engenharia at Univ. do Porto DYNAMIC ANALYSIS (Seismic and Tsunami loadings) André R. Barbosa, Ph.D., P.E. July 03, 2014

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Presentation made by Dr André Barbosa @ University of Porto during the OpenSees Days Portugal 2014 workshop

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Page 1: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 1 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

OpenSees  Days  in  Portugal  @Faculdade  de  Engenharia  at  Univ.  do  Porto  

 

DYNAMIC  ANALYSIS  (Seismic  and  Tsunami  loadings)  

 André  R.  Barbosa,  Ph.D.,  P.E.  

July  03,  2014    

Page 2: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 2 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

2  

Outline  

•  Moment-­‐interac8on  diagrams  as  an  applica8on  of  sec8on  analysis  using  OpenSees.exe  

•  Modeling  a  1-­‐bay,  2-­‐story  RC  concrete  frame  – Nonlinear  material  and  nonlinear  geometry  

•  What  can  else  can  we  do  using  OpenSees?  – Building  example  – Bridge  example  – Soil-­‐structure-­‐fluid-­‐interac8on?  

Page 3: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 3 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Moment  interacOon  diagrams  RC  sec8on  behavior  under  Combined  

Bending  and  Axial  Load  

https://www.dropbox.com/s/evzcz6er3ep0jen/Ex1_MP_Interaction_Diagram.zip

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OpenSees Days in Portugal @FEUP

p. 4 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Development  of  M-­‐N  interac8on  diagrams  

Concrete crushes before steel yields

Steel yields before concrete crushes

Moment

Axia

l Loa

d, P

Failure Criterion: ecu = 0.003

Interaction Diagram

(Failure Envelope)

Page 5: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 5 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

General  Procedure  –  For  various  levels  of  axial  load,  increase  curvature  of  the  sec8on  un8l  a  concrete  strain  of  0.003  is  reached.  

   –  Files  used:  

• model.tcl  • Mp.tcl  

 – Output:  

• mp.out    

Moment = f(c)

Axia

l Loa

d, P

P

M

Page 6: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 6 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Zero  Length  Sec8on  Element  for  RC  Sec8on  Analysis  

y

z

y

x

1Lu uL

L

ε

θχ θ

≡Δ= = Δ

Δ= = Δ

Zero-Length Section

Page 7: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 7 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Concrete01

2*$fpc/$epsc0

$fpc $fpcu

$epsU $eps0

strain

stre

ss

$E0

$b*E0 $Fy

strain

stre

ss

$Fy $b*E0

As1 = 4 No. 8 bars

As2 = 4 No. 8 bars

y

z y1

-y1

-z1 z1

cover

Fiber sec8on  

Steel01  

Concrete01  

Core concrete

Cover concrete

Page 8: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 8 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Interac8on  Diagram    

c si1=

= +∑n

ni

P C F

( )c si12 =

⎛ ⎞= − + −⎜ ⎟⎝ ⎠∑n

n ii

aM C y F y d

Reinforced  Concrete:  Mechanics  and  Design  (4th  Edi8on)    by  James  G.  MacGregor,  James  K.  Wight  

1 11

0.003 ; where = 0.003

ε εε

⎛ ⎞= ⎜ ⎟−⎝ ⎠

s ys

c d Z

= 0.003ε −⎛ ⎞⎜ ⎟⎝ ⎠

isi

c dc

= ; ε ≤si si s si yf E f f

1 = 1.05 0.051000

β′⎛ ⎞

− ⎜ ⎟⎝ ⎠

cfpsi

( )( ) 1 = 0.85 ; β′ =c cC f ab a c

= (positive in compression)si si siF f A

( ) = 0.85 ′−si si c siF f f A

if < ia d

else

for symmetric sections2

= hy

Page 9: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 9 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Interac8on  Diagram    

Page 10: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 10 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Modeling  a  1-­‐bay,  2-­‐story  RC  frame  Beam  column  element  with  (elas8c)  RC  

fiber  sec8on  

https://www.dropbox.com/s/ove56qgu7dqg54r/Ex2_ElasticFrame.zip

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OpenSees Days in Portugal @FEUP

p. 11 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

P   P  

H/2  

1   2  

3   4  

5   6  H  

A   A  

P   P  

(1)   (2)  

(3)  

(4)   (5)  

(6)  

Linear  Elas8c  

Steel  

Concrete  

Lbeam  =  42  _  

Lcol  =  36  _  

Lcol  =  36  _  

Cross-­‐sec8ons  

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OpenSees Days in Portugal @FEUP

p. 12 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Pushover Analysis

Linear geometry

PDelta

Corotational

Page 13: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 13 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

13  

Time-history Response Analysis Linear

geometry

PDelta

Corotational

Page 14: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 14 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Modeling  a  1-­‐bay,  2-­‐story  RC  frame  Beam-­‐column  element  with  RC  

nonlinear  fiber  sec8on  

https://www.dropbox.com/s/geigqdn3dsrvbyb/Ex3_NonlinearFrame.zip

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OpenSees Days in Portugal @FEUP

p. 15 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

e

P   P  

H/2  

1   2  

3   4  

5   6  H  

A   A  

P   P  

(1)   (2)  

(3)  

(4)   (5)  

(6)  

Lbeam  =  42  _  

Lcol  =  36  _  

Lcol  =  36  _  

Cross-­‐sec8ons  

s e s

Steel02   Concrete02  

Material  models  

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OpenSees Days in Portugal @FEUP

p. 16 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Pushover Analysis Time History Analysis

Page 17: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 17 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Concrete stress-strain response

Steel stress-strain response

z

y Fiber 2

Fiber 1

Pushover Analysis

Element 1 Section 5

Page 18: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 18 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

z

y Fiber 2

Time History Analysis Concrete stress-strain response

Steel stress-strain response

Element 1 Section 5

Page 19: Dynamic Analysis with Examples – Seismic Analysis

OpenSees Days in Portugal @FEUP

p. 19 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Building  Example  Barbosa, Conte, Restrepo (2011)

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OpenSees Days in Portugal @FEUP

p. 20 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

q  NEHRP  design  example  (FEMA  451)  

Ø  Demonstrate  the  design  procedures  (ASCE7-­‐05,  ACI318-­‐08)  Ø  Building  was  re-­‐designed  to  account  for  latest  Seismic  Design  Maps  and  

common  prac8ces  in  California  

Latitude: 37.87N

Longitude: -122.29W

Plan  View   Eleva,on   Loca,on  

Barbosa, Conte, Restrepo (2011)

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OpenSees Days in Portugal @FEUP

p. 21 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Elevation Location

Ø  Walls:  Nonlinear  truss  modeling  approach  Ø  Columns  and  beams:  Force-­‐based  beam-­‐column  elements    Ø  Diaphragms:  Flexible  diaphragms  allowing  for  plas8c  hinge  

elonga8on  

q First….  CHECK  AND  VALIDATE  YOUR  MODEL…  q The  model  

Barbosa, Conte, Restrepo (2011)

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p. 22 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

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p. 23 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Bridge  Example  Soil-structure interaction: Barbosa, Mason, Romney (2013)

Tsunami following earthquake: Carey, Mason, Barbosa, Scott (2014)

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p. 24 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Soil-­‐Founda8on-­‐Bridge  Model  q Type-­‐I  sha\  q California,  Oregon,  Washington,    USA  

boundary is modeled in OpenSees by specifying a horizontal “compliant bedrock” dashpot [7], as shown in Figure 1b. The dashpot coefficient, c, is calculated as c = ȡE Vs A, where ȡE is the mass density of the bedrock layer, Vs is the shear wave velocity of the bedrock layer, and A is the out-of-plane cross sectional area of the quadrilateral element. The earthquake motion is applied to the model as an equivalent force-time series, which is coupled with the dashpot. The equivalent force-time series, FE, is calculated as FE = 2ȡE Vs uլ g A, where uլ g is the velocity-time series of the input earthquake motion. Applying the force-time series at the soil-bedrock interface requires the soil column to have unconstrained horizontal degrees of freedom, which is accomplished by modeling soil column bedrock interface with rollers (i.e. the vertical degree-of-freedom is constrained).

(a)

(b)

Figure 1. (a) Generalized elevation schematic of the bridge deck, column, pile, and interface springs, and (b) generalized view of the fair-field soil column modeled using 9-4 quadrilateral elements. The soil mesh is connected to the concrete pile with a series of interface springs, as

shown conceptually in Figure 1a. The interface springs – lateral (p-y), vertical (t-z), and end bearing (q-z) – capture the dynamic response of the surrounding soil and its interaction with the concrete pile foundation. The interface spring coefficients are calculated in accordance with API recommendations [20]. Each interface spring is defined by its depth varying ultimate resistance (pult, qult, and tult) and its expected displacement when 50% of the ultimate strength is mobilized. At larger depths, subgrade reaction moduli, which are used to define the shape of load-displacement curves (i.e., p-y, t-z, and q-z curves), are adjusted for overburden effects by the factor (50 kPa/ıүv)0.5, where ıүv is the effective vertical stress at the depth of interest, in accordance with Boulanger et al. [21]. In OpenSees, the interface springs are implemented using PySimple1, TzSimple1 and QzSimple1 [21] for the p-y, t-z, and q-z springs, respectively. More details about the spring coefficients are given in Barbosa et al. [13].

Barbosa, Mason, Romney (2013)

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p. 25 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Bridge  Deck  &  Abutments  •  Linear  elas8c  beam-­‐column  

•  10.36  m  W  x  1.67  m  T  x  63.4  m  L  •  Area  =  4.56  m2  

•  Ixx  =  5.98x1012  mm4  

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OpenSees Days in Portugal @FEUP

p. 26 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Bridge  Deck  &  Abutments  •  Abutment  (Shamsabadi  et  al.,  2007,  Caltrans  SDC)  

•  Silty  sand  •  S8ffness,  K  =  307  kN/cm/m  •  Yield  Force,  Fy  =  1397  kN  •  Ini8al  Gap  Opening  =  2.54  cm  

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p. 27 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

27

Pile  and  Column  •  Moment-­‐Curvature  Analysis  

•  f’ c  =  28  MPa  •  Fy  =  475  MPa  •  E  =  200  GPa  •  Long.  steel  ra8o  =  1.0%  

•  Fiber-­‐sec8on:  •  Varied  number  of  theta  wedges  and  

radial  rings  

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p. 28 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Analysis  Methodology  •  Development  of  SFB  Model  

•  Step  1:  Define  soil  •  Step  2:  Define  structural  nodes  and  elements  

the seismic resiliency of bridges is an important topic of investigation for earthquake engineers. To this end, a two-dimensional finite element model of a soil-bridge system was developed to evaluate the effects of earthquake motions from shallow crustal and subduction zone sources on the seismic response of bridges. Within the developed model, soil-bridge interaction is accounted for by connecting the soil to the bridge pile with soil-interface springs. Furthermore, the direct method [1] for analyzing soil-bridge interaction was employed. A thorough literature review is outside the scope of this study. Readers can consult Barbosa et al. [2] for more information about soil-bridge interaction. The works by Khosravifar [3], Chiaramonte et al. [4], Zhang et al. [5], Shamsabadi et al. [6], Chang [7], Brandenberg et al. [8] and Boulanger et al. [9] were instrumental for creating the soil-bridge models and informing the research work.

Methodology A two-dimensional (2-D) finite element model of a double-span reinforced concrete bridge and foundation connected to a nonlinear soil column by nonlinear soil springs was developed using the Open System for Earthquake Engineering Simulations (OpenSees) finite element framework [10]. The seismic response of the soil-bridge system was analyzed by subjecting the model to seven shallow crustal earthquake motions and seven subduction zone earthquake motions. Figure 1 shows a schematic of the overall soil-bridge system and a cross-section of the modeled pile and bridge column. Barbosa et al. [2] contains more details about the soil-bridge model, though some of the modeling details have changed, which are documented herein.

(a) (b)

Figure 1. (a) Soil-bridge system analyzed, and (b) cross-section of bridge pile and column (all dimensions are in meters) [2].

Earthquake Motion Selection In the United States, the Pacific Northwest (PNW) and Alaska are prone to subduction zone earthquakes. Traditionally, bridges have been designed to withstand shallow crustal earthquakes, because these bridges are predominant in California. However, the subduction zone earthquake

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Dr. André R. Barbosa July 03, 2014

Analysis  Methodology  •  Step  3:  Gravity  (self-­‐weight)  loads  

•  Soil  self-­‐weight  loading  •  Connect  pile  to  soil  column  •  Structural  self-­‐weight  loading  

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p. 30 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Analysis  Methodology  •  Step  4:  Nonlinear  dynamic  analysis  using  earthquake  mo8ons  

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p. 31 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

column, and accordingly, the out-of-plane contact width for the tsunami wave impact is 31.7 m, which is equal to the span length in the longitudinal direction of the bridge. Within the PFEM procedure, the mass and body forces are increased to represent the out-of-plane contact width. For numerical stability, the column contact width (1.1 m) is not considered. Neglecting the column width when considering tsunami impact is acceptable, because the soil-bridge system response will be dominated by tsunami impact on the much larger deck width. The length of the tsunami bore is set as twice the open length (defined in Figure 3). The accuracy and stability of the PFEM solution depends on the mesh density of the fluid and structure under consideration [9]. To ensure accuracy and stability, the mesh size for the tsunami bore simulation was selected as 175 mm x 175 mm.

Figure 3. Schematic of the tsunami bore simulation (Note: pile and soil column are not shown).

Analysis Framework

The soil-bridge model analysis framework is divided into three stages. The stages simulate the earthquake and tsunami wave loading. Furthermore, each stage is divided into sub-stages for analytical and conceptual reasons. The sub-stages presented for the seismic analysis were adapted from Barbosa et al. [13], and the tsunami stages from Zhu and Scott [9]. Figure 4 shows a flow chart of the stages and sub-stages described below. Stage 1: Earthquake Simulation x Stage 1.1: The global geometry (nodes, connectivity, and boundary conditions) of the soil-

bridge model is established. The bridge column, bridge pile, and soil mesh are created. Additionally, the 9-4 quadrilateral elements and soil interface springs are created. The interface-springs are connected to the soil column, but not to the bridge pile.

x Stage 1.2: The bridge pile and bridge column fiber sections are defined. The bridge pile and column is created using nonlinear beam column elements. The self-mass of the pile and column elements is lumped at the end nodes.

x Stage 1.3: The linear elastic rigid bridge deck is created and attached to the bridge column created in stage 1.2. The bridge deck elements are discretized to the same dimension as the

Tsunami  following  Earthquake  Modeling  q Type-­‐I  sha\  q California,  Oregon,  Washington,    USA  q  In  OpenSees,  use  PFEM:  

v  Zhu and Scott (2014)  

Carey, Mason, Barbosa, Scott (2014)

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p. 32 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Tsunami-­‐Bridge  Interac8on  Model  

PFEM procedure. At the conclusion of each time step, the fluid, wall, flume and bridge column were re-meshed for the subsequent time steps. Figure 5 shows a schematic of the tsunami simulation.

Figure 4. Flow Chart of the three stages comprising the analysis framework.

(a)

(b)

Figure 5. (a) Tsunami bore at the end of Step 3.1, and (b) tsunami bore during Step 3.2.

−20 −15 −10 −5 0 5 10−5

0

5

10

15

20

25

30Initial Bore Time 0

−20 −15 −10 −5 0 5 10−5

0

5

10

15

20

25

30Analysis at 0.575 Sec

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p. 33 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

Tsunami-­‐Bridge  Interac8on  Model  q Type-­‐I  sha\  q California,  Oregon,  Washington,    USA  

Carey, Mason, Barbosa, Scott (2014)

PFEM procedure. At the conclusion of each time step, the fluid, wall, flume and bridge column were re-meshed for the subsequent time steps. Figure 5 shows a schematic of the tsunami simulation.

Figure 4. Flow Chart of the three stages comprising the analysis framework.

(a)

(b)

Figure 5. (a) Tsunami bore at the end of Step 3.1, and (b) tsunami bore during Step 3.2.

−20 −15 −10 −5 0 5 10−5

0

5

10

15

20

25

30Initial Bore Time 0

−20 −15 −10 −5 0 5 10−5

0

5

10

15

20

25

30Analysis at 0.575 Sec

PFEM procedure. At the conclusion of each time step, the fluid, wall, flume and bridge column were re-meshed for the subsequent time steps. Figure 5 shows a schematic of the tsunami simulation.

Figure 4. Flow Chart of the three stages comprising the analysis framework.

(a)

(b)

Figure 5. (a) Tsunami bore at the end of Step 3.1, and (b) tsunami bore during Step 3.2.

−20 −15 −10 −5 0 5 10−5

0

5

10

15

20

25

30Initial Bore Time 0

−20 −15 −10 −5 0 5 10−5

0

5

10

15

20

25

30Analysis at 0.575 Sec

Units in meters

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p. 34 Dynamic Analysis Notes

Dr. André R. Barbosa July 03, 2014

[email protected]