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UILU-ENG-2000-2016 CIVIL ENGINEERING STUDIES STRUCTURAL RESEARCH SERIES NO. 631 ISSN: 0069-4274 STRUCTURAL REDUNDANCY OF DUAL AND STEEL MOMENT FRAME SYSTEMS UNDER SEISMIC EXCITATION By SEUNG-HAN SONG and YI-KWEIWEN A Report on a Research Project Sponsored by the NATIONAL SCIENCE FOUNDATION (Under Grant NSF EEC-97-01785) DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN • I I URBANA; ILLINOIS NOVEMBER 2000

Transcript of CIVIL ENGINEERING STUDIES - COnnecting REpositories · CIVIL ENGINEERING STUDIES STRUCTURAL...

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UILU-ENG-2000-2016

CIVIL ENGINEERING STUDIES STRUCTURAL RESEARCH SERIES NO. 631

ISSN: 0069-4274

STRUCTURAL REDUNDANCY OF DUAL AND STEEL MOMENT FRAME SYSTEMS UNDER SEISMIC

EXCITATION

By SEUNG-HAN SONG and YI-KWEIWEN

A Report on a Research Project Sponsored by the NATIONAL SCIENCE FOUNDATION (Under Grant NSF EEC-97 -01785)

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN

• I I URBANA; ILLINOIS NOVEMBER 2000

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REPORT DOCUMENTATION PAGE

4. Title and Subtitle

1. REPORT NO.

UILU-ENG-2000-2016

2. 3. Recipient's Accession No.

5. Report Date

November 2000 Structural Redundancy of Dual and Steel Moment Frame Systems under Seismic

6. Excitation

7. Author(s)

S.-H. Song and Y. K. Wen

9. Performing Organization Name and Address

University of Illinois at Urbana-Champaign Department of Civil and Environmental Engineering 205 N. Mathews Avenue Urbana, Illinois 61801-2352

12. Sponsoring Organization Name and Address

National Science Foundation 4201 Wilson Boulevard Arlington, VA 22230

15. Supplementary Notes

16. Abstract (Limit: 200 words)

8. Performing Organization Report No.

SRS 631

10. Project/TaskIWork Unit No.

11. Contract(C) or Grant(G) No.

NSF EEC-97-01785

13. Type of Report & Period Covered

14.

The extensive investigation of structural failure after the Northridge and Kobe earthquakes showed poor structural performance due to brittle member behavior and improper design. The lack of ductility capacity and redundancy has become a serious concern. Most reliability and redundancy studies in the past have been limited to ideal simple systems. As a result, structural redundancy under stochastic loads such as earthquakes has not been well understood, which could lead to misunderstandings among structural engineers. In this study, the redundancy of dual systems and special moment resisting frames (S~.1P~) is investigated in terms of system reliability under SAC ground motions. Major factors considered include structural configuration (number and layout of shear walls and moment resistant frames), ductility capacity, uncertainty in demand and capacity including correlation of member strength. Dual systems of five and ten stories, equal lateral resistance, and different configurations are first investigated. Interaction between walls arid moment frames is considered. Ductile special moment resistant frames (S~T1P~) of tr...ree and nine stories, equal floor area and strength but different numbers of bays and different beam and column sizes are then analyzed. Furthermore, three SMRF systems of 1 x 1, 2 x 2, and 3 x 3 bay, equal strength, and brittle beam-column connections are investigated to examine the effect of ductility capacity and torsion. A uniform-risk redundancy factor is then proposed and compared with the redundancy factor (p) in the NEHRP-97, UBC-97, and IBC2000. The p factor is found to be inconsistent. It overestimates the effect of configuration and underestimates the effects of ductility and torsion.

17. Document Analysis a. Descriptors

redundancy, dual systems, moment frames, ductility, brittle failure, SAC ground motions, dynamic response, bi-axial motion, torsion, nonlinearity, uncertainty, risk and reliability, design factor.

b. Indentifiers/Open·Ended Terms

c. COSATI Field/Group

18. Availability Statement

Release Unlimited

(See ANSI-Z39.18)

19. Security Class (This Report)

UNCLASSIFIED

21. Security Class (This Page)

m..rCLASSIFIED

20. No. of Pages

162

22. Price

OPTIONAL FORM 272 (4-77) Department of Commerce

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ABSTRACT

STRUCTURAL REDUNDANCY OF DUAL AND STEEL MOMENT FRAME

SYSTEMS UNDER SEISMIC EXCITATION

Seung-Han Song and Y. K. Wen

The extensive investigation of structural failure after the Northridge and Kobe

earthquakes showed poor structural performance due to brittle member behavior and

improper design. The lack of ductility capacity and redundancy has become a serious

concern. Most reliability and redundancy studies in the past have been limited to ideal

simple systems. As a result, structural redundancy under stochastic loads such as

earthquakes has not been well understood, which could lead to misunderstandings among

structural engineers.

In this study, the redundancy of dual systems and special moment resisting frames

(SMRF) is investigated in terms of system reliability under SAC ground motions. Major

factors considered include structural configuration (number and layout of shear walls and

moment frames), ductility capacity, uncertainty in demand and capacity including

correlation of member strength. Dual systems of five and ten stories, equal lateral

resistance, and different configurations are first investigated. Interaction between walls

and moment frames is considered. Ductile special moment resistant frames(SMRF) of

three and nine stories, equal floor area and strength but different numbers of bays of

different beam and column sizes are then analyzed. Furthermore, three SMRF systems of

1 xl, 2 x 2, and 3 x 3 bay, equal strength, and brittle beam-column connections are

investigated to examine the effect of ductility capacity and torsion.

A uniform-risk redundancy factor is then proposed and compared with the

redundancy factor (p) in the NEHRP-97, UBC-97, and IBC2000. The p factor is found

to be inconsistent. It overestimates the effect of system configuration and underestimates

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the effects of ductility and torsion. Finally, the reliability of design based on the uniform­

risk redundancy factor is verified for a 5-story, one-way dual system.

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ACKNOWLEDGEMENTS

The authors would like to thank W. L. Gamble, D. A. Foutch, N. M. Hawkins, and

Y. M. A. Hashash for their valuable comments and suggestions.

This work was supported primarily by the Mid-America Earthquake Center of the

Earthquake Engineering Research Centers Program of the National Science Foundation

under Award Number EEC-970178S.

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TABLE OF CONTENTS

CHAPTER 1

INTRODUCTION ...................... '" .................................................................................. 1

1.1 Background .......................................................................................................... 1

1.2 Objective and Scope ............................................................................................. 2

1.3 Organization ........................................................................................................ 3

CHAPTER 2

PARAMETRIC STUDY OF SERlES AND PARALLEL SYSTEMS UNDER TTh1E

VARYING STOCHASTIC LOADS ................................................................................ 5

2.1 Introduction ......................................................................................................... 5

2.2 Effect of System Parameters on Redundancy ......................................................... 6

2.2.1 Effect of Number of Components ................................................................. 6

2.2.2 Effect of Ductility of Components ................................................................ 7

2.2.3 Effect of Correlation of Component Strength ................................................ 7

2.2.4 Effect of the Ratio of Load to Resistance Variability ..................................... 7

2.3 Conclusions and Remarks ..................................................................................... 8

CHAPTER 3

MODELING OF SHEAR WALL .................................................................................. 17

3.1 Introduction ....................................................................................................... 17

3.2 Previous Research on Analytical and Experimental Shear Wall ModeL ................ 18

3.3 ACI and UBC Provisions .................................................................................... 19

3.4 Equivalent Analytical Shear Wall Model.. ........................................................... 21

3.5 Yield and Ultimate Strength ............................................................................... 22

3.5.1 Yield Strength ..................................................................... ~ ..................... 22

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3.5.2 Ultimate Strength ...................................................................................... 23

3.6 Nonlinear Static Push-Over Analysis ................................................................. 25

3.7 Displacement-Based Design Methodology .......................................................... 25

3.8 Simulation of Ductility Capacity ......................................................................... 28

CHAPTER 4

MODELING AND DESIGN OF DUAL AND SMRF SySTEMS .................................. 43

4.1 Introduction ....................................................................................................... 43

4.2 Member Capacity Requirements ......................................................................... 44

4.3 Uncertainty in Material and Member Properties .................................................. 45

4.4 Design Issues of Secondary Steel Moment Resisting Frame (SJ\.1RF) System ....... 45

4.5 Design of Dual Systems ...................................................................................... 46

4.5.1 Five-Story, One-Way Dual Systems ........................................................... 46

4.5.2 Five-Story, Two-Way Dual Systems .......................................................... 47

4.5.3 Ten-Story, Two-Way Dual Systems ........................................................... 47

4.6 P-~ Effect ..................................................................................................... 48

4.7 Interaction between Shear Walls and SMRF Systems .......................................... 48

4.8 Design of S\tRF Systems ................................................................................... 49

4.8 I Thrt..x·-Story ~1oment Frame Systems with No Torsion ............................... 49

4 8 2 ~tne-Story ~1oment Frame Systems with No Torsion ................................. 49

4 8 3 Three-Story f\ioment Frame Systems with Torsion and Brittle Connection

Failure .............................................................................................. 50

CHAPTER 5

RESPONSE .-\..':\L YSIS AND PERFORMANCE EVALUATION ............................... 66

5.1 Introduction ..................................................................................................... 66

5.2 SAC-2 Ground Motions ..................................................................................... 66

5.3 Five-Story, One-Way Dual Systems .................................................................... 67

5.3.1 Effect of Number of Shear Walls .......................................... -...................... 67

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5.3.2 Effect of Ductility Capacity of Shear Walls ................................................ 69

5.3.3 Effect of Correlation of Shear Wall Strength .............................................. 69

5.3.4 Effect of the Ratio ofEQ Load to Shear Wall Resistance Variability ........... 70

5.4 Two-Way Dual Systems ..................................................................................... 70

5.4.1 Five-Story, Two-Way Dual Systems .......................................................... 70

5.4.2 Ten-Story, Two-Way Dual Systems ........................................................... 71

5.5 Steel Moment Frame Systems ............................................................................. 72

5.5.1 Three-Story Moment Frame Systems with No Torsion ............................... 72

5.5.2 Nine-Story Moment Frame Systems with No Torsion ................................. 73

5.5.3 Three-Story Moment Frame Systems with Torsion ..................................... 73

CHAPTER 6

RELIABILITY AND REDUNDANCY EV ALUATION .............................................. 109

6. 1 Introduction ..................................................................................................... 109

6.2 Background ...................................................................................................... 109

6.3 Redundancy Factor in Recent Codes and Standards ........................................... 112

6.4 Seismic Hazard Analysis .................................................................................. 114

6.4.1 Uniaxial Spectral Acceleration ................................................................. 114

6.4.2 Biaxial Spectral Acceleration ................................................................... 115

6.5 Probabilistic Perfonnance Analysis in tenns of SWDR and MCDR ................... 115

6.6 Dual Unifonn-Risk Redundancy Factor ............................................................ 117

6.7 Definition of Incipient Limit State for Shear Walls and Moment Frames ............ 120

6.8 Redundancy Evaluation of Dual Systems .......................................................... 121

6.8.1 Five-Story, One-Way Dual Systems ......................................................... 121

6.8.2 Five-Story, Two-Way Dual Systems ........................................................ 122

6.8.3 Ten-Story, Two-Way Dual Systems ......................................................... 122

6.9 Redundancy Evaluation of Steel SMRF Buildings ............................................. 123

6.9.1 Three-Story Buildings with No Torsion .................................................... 123

6.9.2 Nine-Story Buildings with No Torsion ................................. , ................... 123

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6.9.3 Three-Story Buildings with Torsion ......................................................... 124

6.10 Verification of Dual Uniform-Risk Redundancy Factor ................................... 125

CHAPTER 7

SUMMARY, CONCLUSIONS, AND REC O:MMEND AT IONS FOR FUTURE

RESEARCH ................................................................................................................ 146

7.1 Summary ......................................................................................................... 146

7.2 Conclusions..................................................................................................... 148

7.3 Recommendations for Future Research ............................................................. 149

APPENDIX

EARTHQUAKE RESPONSE ANALYSIS OF THREE DIMENSIONAL DUAL

SYSJEMS .................................................................................................................. 151

REFERENCES ............................................................................................................ 157

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LIST OF TABLES

Table 2.1 Parameters of Stochastic Load Process ........................................................... 9

Table 2.2 Resistance Random Variables of the Two-Component System ....................... 9

Table 2.3 Resistance Random Variables of the Three-Component System ..................... 9

Table 2.4 Resistance Random Variables of the Four-Component System ..................... 10

Table 2.5 The Ratio of Load to Resistance Variability in the Four-Component System. 10

Table 3.1 Material Properties of Concrete and Steel Reinforcement and Yield Strength

Parameters in One-Shear Wall System (Aspect Ratio: 1.67) ........................ 29

Table 3.2 Material Properties of Concrete and Steel Reinforcement and Ultimate

Strength Parameters in One-Shear Wall System (Aspect Ratio: 1.67) ........... 29

Table 3.3 Material Properties of Concrete and Steel Reinforcement and Yield Strength

Parameters in Two-Shear Wall System (Aspect Ratio : 1.67) ........................ 30

Table 3.4 Material Properties of Concrete and Steel Reinforcement and Ultimate

Strength Parameters in Two-Shear Wall System (Aspect Ratio: 1.67) .......... 30

Table 3.5 Material Properties of Concrete and Steel Reinforcement and Yield Strength

Parameters in Three-Shear Wall System (Aspect Ratio: 1.67) ...................... 31

Table 3.6 i\1aterial Properties of Concrete and Steel Reinforcement and Ultimate

Strength Parameters in Three-Shear Wall System (Aspect Ratio: 1.67) ........ 31

Table 3.7 !\1aterial Properties of Concrete and Steel Reinforcement and Yield Strength

Parameters in One-Shear Wall System (Aspect Ratio: 4.0) .......................... 32

Table 3.8 !\1aterial Properties of Concrete and Steel Reinforcement and Ultimate

Strength Parameters in One-Shear Wall System (Aspect Ratio: 4.0) ............. 32

Table 3.9 Material Properties of Concrete and Steel Reinforcement and Yield Strength

Parameters in Two-Shear Wall System (Aspect Ratio: 4.0) .......................... 33

Table 3.10 Material Properties of Concrete and Steel Reinforcement and Ultimate

Strength Parameters in Two-Shear Wall System (Aspect Ratio: 4.0) ............ 33

Table 3.11 Different Ductility Capacity of Shear Wall (Aspect Ratio: 1.67) .................. 34

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Table 3.12 Parameters Used in DRAIN3DX for Modeling Different Ductility Capacities

of Three-Shear Wall System ........................................................................ 35

Table 4.1 Design ofSMRF of5-Story, One-Way Dual System .................................... 51

Table 4.2 Design of SMRF of 5-Story, Two-Way Dual System ................................... 51

Table 4.3 Design ofSMRF of 10-Story, Two-Way Dual System ................................. 51

Table 4.4 Design of3-Story, 4 x 4 Bay SMRF System ................................................ 52

Table 4.5 Design of 3-Story, 6 x 6 Bay SMRF System ................................................ 52

Table 4.6 Design of9-Story, 5 x 5 Bay SMRF System ................................................ 52

Table 4.7 Design of 9-Story, 8 x 8 Bay SMRF System ................................................ 53

Table 4.8 Design of3-Story, 1 x 1 Bay SMRF System ................................................ 53

Table 4.9 Design of3-Story, 2 x 2 Bay SMRF System ................................................ 53

Table 4.10 Design of3-Story, 3 x 3 Bay SMRF System ................................................ 54

Table 5.1 Four Case Studies of5-Story One-Way Dual Systems .................................. 75

Table 5.2 Medians and Coefficient of Variation of Spectral Acceleration (5-Story, One-

Way Dual Systems) ..................................................................................... 76

Table 5.3 Medians and Coefficient of Variation of Spectral Acceleration (5-Story, Two-

Way Dual Systems) ..................................................................................... 77

Table 5.4 Medians and Coefficient of Variation of Spectral Acceleration (10-Story, Two-

Way Dual Systems) ..................................................................................... 78

Table 5.5 Medians and Coefficient of Variation of Spectral Acceleration (3-Story SMRF

Systems with No Torsion) ........................................................................... 79

Table 5.6 Medians and Coefficient of Variation of Spectral Acceleration (9-Story SMRF

Systems with No Torsion) ........................................................................... 80

Table 5.7 Medians and Coefficient of Variation of Spectral Acceleration (3-Story SMRF

Systems with Torsion) ................................................................................. 81

Table 5.8 Medians and Coefficient of Variation of Response Variables (5-Story, One-

Way Dual Systems of Different Number of Shear Walls) ............................. 82

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Table 5.9 Medians and Coefficient of Variation of Response Variables (5-StOIY, One-

Way Dual Systems of Different Shear Wall Ductility Capacity) .................... 83

Table 5.10 Medians and Coefficient of Variation of Response Variables (5-Story, One-

Way Dual Systems with Different Correlation of Shear Wall Strength) ......... 84

Table 5.11 Medians and Coefficient of Variation of Response Variables (5-Story, One-

Way Dual Systems and Different Ratios ofEQ to Strength Variability) ........ 85

Table 5.12 Medians and Coefficient of Variation of Response Variables (5-Story, Two-

Way Dual Systems) ..................................................................................... 86

Table 5.13 Medians and Coefficient of Variation of Response Variables (lO-Story, Two-

Way Dual Systems) ..................................................................................... 87

Table 5.14 Medians and Coefficient of Variation of Response Variables (3-Story SMRF

Systems with No Torsion) ........................................................................... 88

Table 5.15 Medians and Coefficient of Variation of Response Variables (9-Story SMRF

Systems with No Torsion) ........................................................................... 89

Tabie 5.16 Medians and Coefficient of Variation of Response Variables (3-Story s:rvfRF Systems with Ductile Connections and Torsion) ........................................... 90

Table 5.17 Medians and Coefficient of Variation of Response Variables (3-Story SMRF

Systems with Brittle Connections including Column Damage and Torsion) .. 90

Table 6.1 Definition of Incipient Limit State for Shear Walls and Moment Frames ..... 126

Table 6.2 50-Year Probability of Exceedance of Shear Wall (5-Story, One-Way Dual

Systems) ................................................................................................... 127

Table 6.3 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor (5-Story,

One-Way Dual Systems) ........................................................................... 128

Table 6.4 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor (5-Story,

Two-Way Dual Systems) ........................................................................... 129

Table 6.5 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor (10-Story,

Two-Way Dual Systems) ........................................................................... 129

Table 6.6 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor C3-Story

SMRF Systems with No Torsion) .......................................... ~ ................... 130

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Table 6.7 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor (9-Story

SJvfRF Systems with No Torsion) .............................................................. 130

Table 6.8 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor (3-Story

SJvfRF Systems with Torsion) .................................................................... 131

Table 6.9 Redesign of 5-Story, One-Way Dual Systems with One Shear Wall ............ 132

Table 6.10 Response/Redundancy of Redesigned 5-Story, One-Way Dual Systems with

One Shear Wall ......................................................................................... 132

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LIST OF FIGURES

Figure 2.1 (a) System Configuration (Parallel versus Series Systems) ............................. 11

Figure 2.1 (b) System Configuration (Parallel versus Series Systems: Moses, 1974) ...... 11

Figure 2.2 Restoring Force-Deformation Characteristics ............................................... 12

Figure 2.3 Different Number of Components in Parallel Balanced Systems ................... 13

Figure 2.4 Different Number of Components in Series Systems .................................... 13

Figure 2.5 Effect of Number of Components (parallel System) ..................................... 14

Figure 2.6 Effect of Number of Components (Series System) ........................................ 14

Figure 2.7 Effect of Component Post-Yielding Behavior .............................................. 15

Figure 2.8 Effect of the Correlation of Component Resistance ...................................... 15

Figure 2.9 Effect of the Ratio of Load to Resistance Variability .................................... 16

Figure 2.10 System Redundancy Factor by De and Cornell ............................................. 16

Figure 3.1 Rocking Motion and Outriggering Interaction (Bertero, 1991) ...................... 37

Figure 3.2 Hysteretic Curve of Shear Wall in Experiment (Paulay, 1982) ...................... 37

Figure 3.3 Equivalent Shear Wall Model ...................................................................... 38

Figure 3.4 Trilinear and Degradation Model of Fiber Beam Column Element (Parakash et

aI, 1994) ...................................................................................................... 39

Figure 3.5 Stress and Strain Diagram at Yield Strength ................................................. 40

Figure 3.6 Stress and Strain Diagram at Ultimate Strength ............................................ 40

Figure 3.7 Nonlinear Static Push-Over Analysis of Shear Wall in One-, Two-, and Three-

Shear Wall System ...................................................................................... 41

Figure 3.8 Curvature Diagram ...................................................................................... 41

Figure 3.9 Hysteretic Response of One-Shear Wall System (Aspect Ratio: 1.67, Ductility

: 6.4) ........................................................................................................... 42

Figure 3.10 Different Ductility Characteristics of Shear Walls ........................................ 42

Figure 4.1 Redundancy in Shear Wall Systems (ATC-19, 1995) ................................... 55

Figure 4.2 Design Requirement of Secondary SMRF System in a Dual System ............. 56

Figure 4.3 (a) Five-Story, One-Way Dual Systems with One Shear Wall ........................ 56

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Figure 4.3 (b) Five-Story, One-Way Dual Systems with Two Shear Walls ...................... 57

Figure 4.3 (c) Five-Story, One-Way Dual Systems with Three Shear Walls .................... 59

Figure 4.4 (a) Five-or Ten-Story, Two-Way Dual Systems with One Shear Wall ............ 58

Figure 4.4 (b) Five- or Ten-Story, Two-Way Dual Systems with Two Shear Walls ......... 58

Figure 4.4 (c) Five-Story, Two-Way Dual Systems with Three Shear Walls ................... 59

Figure 4.5 Interaction between Shear Walls and S:MRF Systems (5-Story, Two-Way Two-

Shear Wall System) ..................................................................................... 59

Figure 4.6 Nonlinear Static Push-Over Analysis of 5-Story, Two-Way Two-Shear Wall

System ........................................................................................................ 60

Figure 4.7 Three-Story, 4 x 4 Bay S11R.F System ......................................................... 60

Figure 4.8 Three-Story, 6 x 6 Bay S11R.F System ......................................................... 61

Figure 4.9 Nonlinear Static Push-Over Analysis of 4 x 4 and 6 x 6 Bay Systems ........... 61

Figure 4.10 Nine-Story, 5 x 5 Bay S11R.F System ........................................................... 62

Figure 4.11 Nine-Story, 8 x 8 Bay S11R.F System ........................................................... 62

Figure 4.12 Three-Story, 1 x 1 Bay S11R.F System ......................................................... 63

Figure 4.13 Three-Story, 2 x 2 Bay S11R.F System ......................................................... 63

Figure 4.14 Three-Story, 3 x 3 Bay S11R.F System ......................................................... 64

Figure 4.15 Nonlinear. Static Push-Over Analysis of 1 x 1 and 2 x 2 Bay Systems ........... 64

Figure 4.16 Brittle Fracture Model (Wang and Wen, 1998) ............................................. 65

Figure 5.1 A Pair of SAC-2 Earthquake Ground Motions (LA21 and LA22) ................. 91

Figure 5.2 Displacement of Top Mass Center of 5-Story, One-Way Dual Systems (One-

Shear Wall System) ..................................................................................... 92

Figure 5.3 Displacement Trajectory of Top Mass Center under LA21 and LA22 (5-Story,

One-Way Dual Systems with 5% Accidental Torsion) .................................. 94

Figure 5.4 Displacement Trajectory of Top Mass Center under LA21 and LA22 (No

Accidental Torsion) ..................................................................................... 95

Figure 5.5 Scatter of Spectral Acceleration (5-Story, Two-Way Dual Systems of One

Shear Wall: T1=0.61, T2=0.56, S=0.02) ................................. : ..................... 96

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Figure S.6 Scatter ofSWDR (S-Story, One-Way Dual Systems) ................................... 97

Figure S.7 Scatter of MCDR (S-Story, One-Way Dual Systems) ................................... 98

Figure S.8 Scatter of SWDR (S-Story, Two-Way Dual Systems) ................................. 100

Figure S.9 Scatter ofSWDR (10-Story, Two-Way Dual Systems) ............................... 102

Figure S.1 0 S 0-Year Probability of Exceedance of Median SWDR (S-Story, One-Way Dual

Systems) ................................................................................................... 104

Figure S.11 SO-Year Probability of Exceedance of Median SWDR (S-Story, Two-Way

Dual Systems) ........................................................................................... lOS

Figure S.12 SO-Year Probability of Exceedance of Median SWDR (10-Story, Two-Way

Dual Systems) ........................................................................................... 106

Figure S.13 SO-Year Probability of Exceedance of Median Story Drift Ratio (X Direction)

(3-Story SMRF Systems with No Torsion) ................................................. 106

Figure S.14 SO-Year Probability of Exceedance of Median Story Drift Ratio (X Direction)

(9-Story SMRF Systems with No Torsion) ................................................. 107

Figure S.IS SO-Year Probability of Exceedance of Median MCDR (3-Story S:MRF Systems

with Ductile Connections and Torsion) ...................................................... 107

Figure S.16 SO-Year Probability ofExceedance of Median MCDR (3-Story S:MRF Systems

with Brittle Connections including Column Damage and Torsion) .............. 108

Figure 6.1 Uniaxial Elastic Response Spectrum (Sa) ................................................... 133

Figure 6.2 Uniaxial Elastic Response Spectrum (Sd) ................................................... 134

Figure 6.3 Biaxial Elastic Response Spectrum ............................................................ 13S

Figure 6.4 Spectral Acceleration Hazard Curve (10-Story, Two-Way Dual Systems with

Two-Shear Wall System) ........................................................................... 138

Figure 6.S Dual Uniform-Risk Redundancy Factor, RR ............................................... 139

Figure 6.6 Relative Redundancy Ratio, RRR ................................................................ 139

Figure 6.7 Exceedance Probability (S-Story, One-Way Dual Systems) ........................ 140

Figure 6.8 Redundancy Factor (S-Story, One-Way Dual Systems) .............................. 140

Figure 6.9 Probabilistic Performance Curves of S-Story, One-Way Dual Systems (X

Direction) ............................................................................. : ................... 141

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Figure 6.10 Probabilistic Performance Curves of 10-Story, Two-Way Dual Systems ..... 142

Figure 6.11 Probabilistic Performance Curves of 3-Story SMRF Systems (X Direction and

No Torsion) ........ '" ................................................................................... 143

Figure 6.12 Probabilistic Performance Curves of 9-Story SMRF Systems (X Direction and

No Torsion) .............................................................................................. 143

Figure 6.13 Probabilistic Performance Curves of 3-Story SMRF Systems (Ductile

Connections and Torsion) .......................................................................... 144

Figure 6.14 Probabilistic Performance Curves of 3-Story SMRF Systems (Brittle

Connections and Torsion) .......................................................................... 144

Figure 6.15 Probabilistic Performance Curves of Redesigned 5-Story, One-Way Dual

Systems (X Direction) ............................................................................... 145

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CHAPTER 1

INTRODUCTION

1.1 Background

Structural system reliability and redundancy have been studied extensively in the

past. Most studies, however, have been limited to ideal simple systems under static loads.

Very little has been done on structures under stochastic loads primarily due to the

analytical difficulty. As a result, structural redundancy has not been clearly understood

and design for redundancy has been mostly based on judgement.

After the 1994 Northridge earthquake, extensive investigations of structural failure

showed poor structural performance due to brittle member behavior and improper design.

For instance. the brittle steel connection fractures were totally unexpected of the highly

regarded "ductile" systems. The lack of system ductile capacity and redundancy could

lead to system Instability and collapse. Since then, the design for redundancy has

attracted more attC:1tlOn of both researchers and practitioners.

Under ~e\ erc earthquake excitations, member failures particularly progreSSIve

failure in a buIldlrlf: ~: stem can change the dynamic properties of the structure and make

it less resistant tu ~el~nllC excitation and energy demand. Dual systems that is typically

composed of rnrna~ steel bracings or shear walls and secondary moment frames provide

many altematl\ e loadmg paths after member failures, and therefore, residual strength and

redundancy. The load-carrying capacity depends on the interaction of primary and

secondary subsystcm~. For special moment frames, the redundancy may be more

affected by the ductility capacity of the connections, the numbers of bays, and the column

and beam sizes. Also, biaxial interactions and torsion may become significant after

member failures. To incorporate these factors in evaluation of structural reudanccy,

analytical models for a three-dimensional structural analysis are required.

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In most recent building codes and documents for building design (e.g. A TC-19

(1995) and ICBO (1997)), the lack of redundancy is considered via a penalty factor in

conjunction with the response modification factor, R. The penalty is a function of

structural configuration (number of structural components, ground floor area, and

maximum element-story shear ratio). Other factors that may be important in assessing

the redundancy of a structures such as ductility capacity, loading and resistance

uncertainty, component interactions, biaxial and torsional motions have not been

considered. More research, therefore, is needed for a better understating of structural

redundancy and development of a rational design procedure.

1.2 Objective and Scope

The purpose of this study is to investigate the redundancy of dual systems and steel

moment frames under seismic excitations. The specific objectives are:

1. Develop an analytical model for hysteretic behavior of reinforced concrete shear

wall in dual systems. The model should reproduce the shear wall response

behavior observed in experiments

2. Develop a three-dimensional building model for dual systems and moment

frames under seismic excitations. Important 3-D structural behaviors such as

rocking motion of shear walls, interaction between primary and secondary

subsystem, biaxial interaction, and torsion are considered.

3. Evaluate structural reliability and redundancy of dual systems and moment

frames under stochastic excitations. Generalize the uniform-risk redundancy

factor proposed by Wang and Wen (1998) for moment frames to design and

performance evaluation of dual systems.

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1.3 Organization

In Chapter 2, a parametric study of simple series and parallel systems under time­

varying stochastic loads is perfonned via Monte-Carlo simulation. It is an extension of

studies under time-invariant static loads analyzed by Gollwitzer and Rackwitz (1990) and

De and Cornell (1989). The important factors affecting redundancy under time-invariant

static loads are found to be also valid under time-varying stochastic loads.

In Chapter 3, an analytical shear wall model is developed based on hysteresis

obtained from experimental results. Incipient yield and collapse are defined according to

the stress-strain relationship. A displacement-based design methodology is used. The

ductility capacity of a shear wall is given by a function of the ratio of maximum concrete

strain to neutral axis depth.

In Chapter 4 the modeling and design of dual and moment frame systems is

decribed. The seismic provisions of dual systems in current codes are reviewed. The

capaci ty of dual systems against lateral load is studied. A three-dimensional building

model is developed. Interaction between shear walls and moment frames is included in

the model. The modeling and design of steel moment frames is also investigated in this

chapter. Biaxial interaction -and P-Ll effects are also considered. Uncertainty in member

capacity and earthquake excitation is considered.

In Chapter 5, response analyses of 5-story, one-way and two-way dual systems and

10-story two-way dual systems subjected to SAC-2 ground motions are performed using

the structural models developed in Chapter 3 and 4. Shear wall damage is measured by

the shear wall drift ratio (SWDR) while system incipient collapse is measured by the

Maximum Column Drift Ratio (MCDR). Major factors affecting redundancy of dual

systems include number and layout of shear vvalls, ductility capacity, lateral resistance

variability, and correlation of shear wall strength. The effects of these factors on

structural response are investigated. The response analyses of 3-story moment frames and

9-story moment frames with either ductile or brittle connections and different numbers of

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bays are also carried out to examIne the effect of member behavior and system

configuration.

In Chapter 6, previous studies of system reliability and redundancy of building

systems are first reviewed. The redundancy of a building under earthquake excitations is

then quantified in terms of system reliability. The uncertainty in seismic loads is

incorporated in the analysis via the hazard curve of spectral acceleration. The median

value of nonlinear structural responses under SAC-2 ground motions is calculated and

multiplied by a correction factor to account for the resistance and modeling uncertainty.

The results are then fitted by a log-normal distribution. For design purpose, a uniform­

risk redundancy factor proposed by Wang and Wen (1998) is used. A comparison of the

risk-based factor and the reliability/redundancy factor of NEHRP is made and the

inconsistency of the latter is pointed out.

Chapter 7 summarizes the conclusions of this study and recommendations for

future research.

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CHAPTER 2

PARAMETRIC STUDY OF SERIES AND PARALLEL SYSTEMS UNDER TIME VARYING STOCHASTIC LOADS

2.1 Introduction

The reliability and redundancy of simple series and parallel systems (shown in

Figure 2.1) under stochastic loads are studied by Monte-Carlo simulation. The purpose of

this study is to identify the most important parameters affecting the redundancy of such

systems under stochastic loads. For simplicity, the following assumptions are made: 1)

The components have the same elastic modulus, area, and length; 2) The total mass is

equal to unity; 3) The system has equal load distribution; and 4) The component

resistance is modeled by Gaussian random variables with equal mean and standard

deviation. The stochastic excitations are modeled as Gaussian processes and simulated by

the spectral method (Shinozuka, 1991). For a stationary load process, a model of

summation of cosine functions with prescribed amplitudes and random phase shifts is

used,

f(t) =.fi i(2Sff(QJk)~W)l/2 cos(Wkt + <Pk) k=O

(2.1)

where Srr is the spectral density function of ground acceleration type of excitation and <Pk

is a uniform random number between 0 and 2IT. The parameters of the process are given

in Table 2.1.

Nonstationarity is introduced by multiplying the stationary Gaussian process by a

deterministic modulation function, aCt),

aCt) = 1- e- ilt (2.2)

where A is always larger than O.

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The simple series and parallel systems in this study consist of two, three, or four

members in order to investigate the effect of number of system components. It is assumed

that the mean resistance of the member is 20 for the two-member system, 13.33 for the

three-member system, and 10 for the four-member system (shown in Tables 2.2, 2.3, and

2.4, respectively). Therefore, systems with different numbers of members have the same

mean resistance for a fair comparison of the system performance. The coefficient of

variation of the resistance is assumed to be 20% for all members.

The effect of ductility is considered by varying the post-yielding member resistance

as illustrated by the restoring force-deformation relationship in Figure 2.2. The members

are categorized into three groups: 1) ductile-the member is perfectly plastic after

yielding; 2) semi-brittle-the post-yielding residual strength is half of that of the ductile

case; and 3) brittle-there is no residual strength after yielding. All members in a given

system are assumed to have the same post-yielding behavior.

2.2 Effect of System Parameters on Redundancy

2.2.1 Effect of Number of Components

In a building system, the number of vertical seismic framing systems and seismic

shear wall systems are the main concerns in redundancy evaluation in ATC-19 and 34

(1995). The effect of different numbers of system components shown in Figures 2.3 and

2.4 is investigated. Figures 2.5 and 2.6 show examples of simulation results for a system

of brittle components subjected to a nonstationary load over a period of 30 seconds. It is

evident that the reliability of the parallel system increases and that of the series system

decreases as the number of components increases. The results show that the trend is the

same for different correlations of component resistance and post-yielding behavior.

Gollwitzer and Rackwitz (1990) reached the same conclusion for such systems under

static loads.

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2.2.2 Effect of Ductility of Components

The effect of ductility capacity of members such as beam, columns and connections

in a moment frame and the shear walls in a dual system are other important. In view of

this, the effect of ductility capacity of parallel systems is investigated. Figure 2.7 shows

the simulation results for the parallel systems with different post-yielding behaviors. The

system of perfectly ductile components has the lowest failure probability. As expected,

the perfectly brittle components give the highest failure probability. The reliability of the

system of semi-brittle components is in between.

2.2.3 Effect of Correlation of Component Strength

The stochastic dependence is considered herein to examine the extent to which the

statistical correlation among components influences the reliability and redundancy of the

system. Components 1 & 4 and 2 & 3 in the four-member system are assumed to have a

correlation coefficient of 1, 0.5, or O. The ductile parallel components of perfectly plastic

behavior are simulated under nonstationary loads as shown in Figure 2.8. As can be seen,

the reliability drops as the correlation increases. The trend is the same for systems of

semi-brittle and brittle members.

2.2.4 Effect of the Ratio of Load to Resistance Variability

The effect of the relative magnitude of load to resistance variability on redundancy

is also investigated. Four different Gaussian load processes with the same mean value of

22, and standard deviations of 4.4, 8.8, 13.2, and 17.6, are applied to a system that has a

mean of 10 and a standard deviation of 2 for each component resistance. The ratio of load

to resistance variability in terms of the coefficient of variation, therefore, is 1,2,3, and 4,

respectively, as given in Table 2.5. Figure 2.9 shows that the failure probability of the

parallel system of semi-brittle members is very sensitive to the ratio. The trend is the

same for ductile and brittle systems. As the ratio increases, the benefit of redundancy

drastically reduced. The same has been found under static loads. In other words, for large

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ratio, the uncertainty in the demand dominates the reliability of the system. As a result,

the configuration and ductility of the members become less important.

2.3 Conclusions and Remarks

A simple parallel system can provide efficient extra reliability when subjected to

time varying stochastic loads if the system meets the following requirements:

1. Adequate number of components

2. At least moderate degree of component ductility

3. Low stochastic strength correlation among components

4. Low ratio of load to resistance variability

The conclusions of this study agree with those of Gollwitzer and Rackwitz under

time-invariant static loads (e.g. Gollwitzer, S. & R. Rackwitz, 1990; De, R.S., A.

Karamchandani and C.A. Cornell, 1989).

According to De, et al. (1989), a redundancy factor in terms of probability can be

defined as follows:

RR = P{system failure} P{any first member failure}

(2.3)

By definition. this factor is bounded between 0 and 1. Thus, higher redundancy of a

system is indicated by a smaller system redundancy factor. One example is given in

Figure 2.10 for the systems of parallel brittle components under stationary loads. Such a

factor may be useful in describing system redundancy.

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Table 2.1 Parameters of Stochastic Load Process.

Standard Load Process Mean COY

Deviation

Stationary

S or 22 4.4 0.2

Nonstationary

Table 2.2 Resistance Random Variables of the Two-Component System.

Resistance Standard Distribution Mean COY

Variables Deviation

Rl Gaussian 20 4 0.2

R2 Gaussian 20 4 0.2

Table 2.3 Resistance Random Variables of the Three-Component System.

Resistance Standard Distribution Mean COY

Variables Deviation

Rl Gaussian 13.33 2.67 0.2

R2 Gaussian 13.33 2.67 0.2

R3 Gaussian 13.33 2.67 0.2

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Table 2.4 Resistance Random Variables of the Four-Component System.

Resistance Standard Distribution Mean COV

Variables Deviation

Rl Gaussian 10 2 0.2

R2 Gaussian 10 2 0.2

R3 Gaussian 10 2 0.2

R4 Gaussian 10 2 0.2

Table 2.5 The Ratio of Load to Resistance Variability in the Four-Component System.

Standard Standard Ratio of

Mean of COVof Mean of Deviation COVof Deviation Load to

Load Load Resistance of Resistance of Load Resistance

Process Process Variables Resistance Variables Process Variability

Variables

22 4.4 0.2 10 2 0.2 1

22 8.8 0.4 10 2 0.2 2

22 13.2 0.6 10 2 0.2 3

22 17.6 0.8 10 2 0.2 4

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/ / / /

R 1 R2 R3 R4

Parallel ~ S(t)

Set)

t=U Rl 0 R2 a R3 o~ Series

Figure 2.1(a) System Configuration (Parallel versus Series Systems).

2

3

N

p Model

p-.".------,

Structure

Series System

-'. -'.-'.

1 2

~ p

Model'

'/

N

Structure

Parallel System

Figure 2.1 (b) System Configuration (Parallel versus Series Systems: Moses, 1974).

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Force Ductile

Semi-brittle

Brittle

Deformation

Figure 2.2 Restoring Force-Deformation Characteristics.

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/ / /

s s s

Figure 2.3 Different Number of Components in Parallel Balanced Systems.

s.j ••• ~s

Flfure ::. -l Different Number of Components in Series Systems.

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0.4

Q) en c.. ~ (5

0.3 U E Q)

en >-

Cf)

'0 0.2

g :0 co .0 2 0.1

Cl.

0.0 0

14

Brittle Parallel System under Nonstationary Load

• Two Member System ...... ............. Three Member System ._._._ .•. _._.- Four Member System

............ ,6 .•.•.. ................. ..... _ ..•. -~~ .

............... }f ............ . ...... .. ...... ",,' ......... .. .. ........

:.11 10 15 20 25 30

Time (sec)

Figure 2.5 Effect of Number of Components (Parallel System).

Q) en c.. ~ (5 U E Q)

en >­

Cf)

'0

1.0

0.9

0.8

0.7

0.6

0.5

Brittle Series System under Nonstationary Load

... ·_···-·I';'···~··- ... ··--II6-·-~·::=-=·-=~ .. __ ·-__ • ./ ........ .../,----e--

I- ( • •

/ g 0.4

:0 I

! Two Member System Three Member System Four Member System

co .0 o c:

Ii /

0.2 !.f" / 0.1 ,..: .... jl

.. .i.,.: ./" 0.0 ...... """-4-._--I. __ ~_-'-_----' __ -'--_______ ~_~_-'

0.3 .........•......... ._._._ .•. _._.-

o 4

Time (sec)

Figure 2.6 Effect of Number of Components (Series System).

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0.14

Q)

~ 0.12 3! (5 o 0.10 E Q)

~ 0.08 Cf)

'0 ~ 0.06

:0 ct1 .0 o 0:

15

Four Member Parallel System under Stationary Load

• ·········A··

Brittle Member Semi-Brittle Member

._._._ .•. -._.- Ductile Member

~·"".A··

.·A··: :· .... ·.··A·:

.·A·.· ... · .. · ....... ....• , ......

I ............. ~·· .. ·• ... · ..... · •• · ... · ....... ·IHI· .... ·

.:~ •. I

o.~~~--~--~---L--~--~--~--~--~--~--~--~--~ 10 15 20 25 30

Time (sec)

Figure 2.7 Effect of Component Post-Yielding Behavior.

0.05

Q)

Ductile Four Member Parallel System under Nonstationary Load

• Perfect Correlation ........ ·A········· Partial Correlation

~ 0.04 ._. __ .•. _._.- No Correlation ~ o ()

E Q)

Ul >.

Cf)

'0

0.03

~ 0.02

:0 ct1 .0 o 0: 0.01

: ........

; .•. : j ......

•· ....... ·.·.A • ~ i

:.~ .......... ..; : i

.......................... 1

i i • i

10 15 20 25 30

Time (sec)

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1.0

16

Semi-Brittle Four Member Parallel System under Stationary Load

................................. -.............. . ~ 0.9 *.~- ................... . 0... . ... 11' ....

~ 0.8 ." _ ........... ... 8 .: , ... 0.7: •

~ ~ ... , ~ 0.6 / ,_

~ 0.5 ,f ,.',J' ........................................ . ...... .... .............. . g 0.4 ~,. .......... • Variability Ratio = 1 :0. .............. ..... Variability Ratio = 2 ~ 0.31/ : •. , ._._._ .•. _._._ Variability Ratio = 3

!t 0.2 q .: .............. Variability Ratio = 4

• 0.1 ~.

~-OO~~--~--~--~--~--~~--~--~--~--~--~~

."""_.... --_ ........ a 10 15 20 25 30

Time (sec)

Figure 2.9 Effect of the Ratio of Load to Resistance Variability.

c:..

Brittle Four Member Parallel System under Stationary Load

.... ~· ..... ·.-II, ........ JI·' ............ , •.. : ,..... .

Ii •.

, .' c. ~,. ri-t:- ,

: 4 ~ ,

~ I' • Probability of Any First Member Failure

..... . Probability of System Collapse 1--·_· ... ·_·_·- Redundancy Factor defined by De and Cornell

.......... ~ " ., .. ~ ... ~ ....... -t ....... _.H.r' ......... ". ................. .. ..- ... ........................ .. .... . -.&------~--~~--~--~--~--~--~--~~--~--~

10 15 20 25 30

Time (sec)

Figure 2.10 System Redundancy Factor by De and Cornell.

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CHAPTER 3

MODELING OF SHEAR WALL

3.1 Introduction

Accurate modeling of reinforced concrete shear wall response behavior is most

important in the study of redundancy of dual systems. The yielding and collapse

capacities ofRC shear walls in terms of shear wall drift ratio are highly variable as shown

in experimental studies (Duffey, et aI, 1994). At the ultimate load, the drift is generally

larger for a shear wall of larger aspect ratio, but it is difficult to quantify the ultimate drift

capacity as a function of member geometric and material parameters.

Under cyclic loading, a shear wall may still have a useful seIsmIC energy

absorption capacity beyond the point of maximum (ultimate) load, until the resistance

drops to about 90 to 50% of the maximum. Nevertheless, the drift limit at the ultimate

load is still the most appropriate measure of incipient collapse because significant

damage to nonstructural components may have occurred when it is exceeded. Also, the

scatter of drift limit values beyond the maximum is known to increase significantly as the

residual resistance capacity decreases, indicating that beyond the ultimate load there is a

much larger uncertainty in the drift capacity.

Bertero, et al. (1991), suggest, as a guideline, a drift ratio of 0.06 to 0.6 % for

serviceability, and 1 to 3 % for safety (collapse), regardless of the type of structure and its

function. The drift limits suggested by Bertero, et al. are probably more appropriate for

medium- and high-rise structures but generally not appropriate for low aspect ratio shear

walls. In this study, the drift ratio at ultimate load is taken conservatively as a damage

level indicative of incipient collapse of a shear wall.

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3.2 Previous Research on Analytical and Experimental Shear Wall Model

There have been many studies of the modeling of RC shear walls based on either a

finite element (FE) or a macroscopic equivalent member approach. The macroscopic

member approach is frequently used for its simplicity. It includes the equivalent beam

model, the equivalent truss model, and the three vertical line element model (Vulcano

and Bertero, 1987). Although the FE approach is capable of modeling local behavior in

detail, the implementation is computationally cumbersome. For this reason, the

equivalent structural component approach is employed to model the overall behavior of

shear wall. In order to account for the three important failure modes, i.e. flexural, sliding

shear, and fixed end rotation failures including rocking motion and outriggering

interaction with the frame (Figure 3. 1), a realistic RC shear wall model is needed for this

study.

A secondary issue in the modeling of RC shear walls is the realization of the

softening region. The slope of the negative stiffness affects the interaction between shear

walls and between the shear wall and the special moment resisting frame (SMRF) after

the failure of any shear walls in a dual system, therefore, its load-carrying capacity. The

field studies of shear wall structures by Paulay (1986) (depicted in Figure 3.2) show that

stiffness and strength degradations and energy dissipation capacity are the most important

factors in the deterioration of lateral resistance capacity of shear walls. Therefore, the

shear wall model should also reproduce the stiffness and strength degradation

characteristics under dynamic loads.

The third important consideration is the uncertainty in structural material strength

and random stochastic loads. Important material parameters, such as yield strength and

plastic moduli of the member cross section, can be modeled as random variables

(Melchers, 1987). Based on a study of experiments of a total of 168 shear walls in Japan,

Y. J. Park (1995) suggested a coefficient of variation of ultimate shear wall strength of

23%. In this study, the uncertainty of shear wall is considered by modeling yield and

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collapse strength as random variables and incorporated into the response analysis via

Monte-Carlo simulation.

3.3 ACI and UBC Provisions

According to ACI318-95, distributed web reinforcement is selected to resist the

shear force. Nominal shear strength, V n, of structural walls and diaphragms in regions of

high seismic risk can be assumed not to exceed the shear force calculated from the

following equation:

(3.1)

in which Acv is the net area of concrete section bounded by web thickness and length of

section in the direction of shear force considered, f~ is specified compressive strength of

concrete and fy is a specified yield strength of reinforcement. Pn is ratio of distributed

shear reinforcement on a plane perpendicular to plane of Acv. For walls and wall

segments having a ratio of (hw/1w) larger than 2.0, U c is 2.0. U c increases to 3.0 for short

walls.

The minimum longitudinal steel reinforcement ratio is 0.0025 unless ¢Vn ~ AcvK

according to ACI318-95 and UBC97. Two curtains of steel are required if

Vu > 2 AcvK· Vn should be smaller than 8 AcvK. Note that Vn is nominal shear

strength, V u is factored shear force, and ¢V n is design shear strength.

The ACI 318-95 provisions based on a simple elastic model are easy to apply and

familiar to designers. Many experimental results, however, show that the ACI 318-95

provisions are rather conservative for the confined boundary elements of shear walls. The

provisions result in an excessive extension of boundary transverse reinforcement along

the height of the wall. Many researchers and engineers, therefore, have a negative opinion

on the ACI 318-95 steel reinforcement detailing. Confined boundary elements were

required in ACI318-95 to be designed according to following condition: -

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20

Structural walls not designed to the provisions mentioned above shall

have special boundary elements at boundaries and edges around openings

of structural walls where the maximum extreme fiber stress, caused by

Vu , exceeds 0.2f c. The special boundary element can be discontinued

where the calculated compressive stress is less than O.lSf c. Therefore,

according to the requirements for the extreme fiber stress suggested by

the above provision, stresses along the shear wall shall be calculated and

used for the factored forces using a linearly elastic model and cross­

section properties. In ACI318-99, the foregoing approach became an

alternate approach, but still permissible approach. The preferred

approach became the following:

(a) For walls continuous from base to top and having a single critical

section for flexure and axial loads at the base, compression zones shall be

reinforced with special boundary elements if

lw c ~

600 (bu / hw)

in which lw is wall length, hw is wall height, and 8u is design displacement

of wall. The quantity 8u / hw in equation shall not be less than 0.007.

(b) Where special boundary elements are required by the above equation

(3.2), the special boundary element reinforcement shall extend vertically

along the wall a distance not less than the larger of lw and Mu / 4Vu from

the critical section. (ACI318-99)

(3.2)

The above equation is based on a displacement-based approach which assumes that

special boundary elements are required to confine the concrete where the strain of the

extreme compression fiber of the wall exceeds a critical value when the wall reaches the

design displacement.

Another important change in ACI 318-99 provIsIons IS the adoption of a

displacement-based design approach for flexure-controlled walls. It is consistent with the

results of research to improve the design of shear walls in terms of both economy and

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21

safety. To accommodate this concern, the newly released provisions require wall design

using flexure and axial forces based on section analysis identical to the design for column

cross sections. It means that engineers are encouraged to use the entire wall cross section

to resist gravity loads and overturning moments, rather than use the design compression

and tension forces only from boundary elements.

3.4 Equivalent Analytical Shear Wall Model

In designing a shear wall, the primary concern is the determination of yield and

ultimate strength. The material properties of concrete and steel reinforcement and

performance parameters at incipient yielding and collapse are given in Tables 3.1 through

3.10. The material and geometric properties follow those ofUBC-97 (lCBO, 1997).

The equivalent shear wall model shown in Figure 3.3 is composed of multiple

columns and rigid beams. The computer software DRAIN3DX is used to model the shear

wall response behavior. Element 15 of the program, which is a fiber beam column

element, is used for simulating the global hysteretic behavior of a concrete shear wall by

adjusting the parameters. For computational efficiency, the elastic bars with end plastic

connection hinges are used based on the assumption that the lumped plasticity at the ends

of the bars is reasonable (Elwood and Wen, 1995). The pullout properties (skeleton

curve; see Figure 3.4) defined in DRAIN3DX for connection hinge fibers are selected to

allow the incorporation of stiffness, strength degradation, and pinching effect.

The softening region, which allows more energy dissipation capacity, IS

incorporated into the system by a hysteretic model with stiffness and strength

degradation. The load-carrying capacity of the dual systems is highly dependent on the

slope of the negative stiffness.

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22

3.5 Yield and Ultimate Strength

3.5.1 Yield Strength

Based on elastic section analysis, the yielding moment at the base of shear wall can

be easily calculated under force equilibrium. From the strain and stress diagrams shown

in Figure 3.5, taking the first moment of transformed areas about the neutral axis yields

the following equation if axial load, P, is neglected:

tw (kd)2 +(2n-1)As'(kd-d)= nAs(d-kd)+ nAs" (~-kd) (3.3) 2 2

in which n is the ealstic modulus ratio ofEJEe.

The tension and compression force equilibrium yields the following equation:

fe tw (kd) + (2n -1) fe (kd - d')As '= nfe(d - kd)As + nAs" fe(lw - 2(kd» + A lw twf e 2 kd kd 2(kd)

(3.4)

f (kd) in which fe is a specified concrete stress given by Y , tw is the thickness of wall,

ned - kd)

and (kd) is neutral axis depth. The axial load, P, is assumed to be 10% (A) of Aw fe'.

Solving the above equation for (kd) allows calculating the compression force induced by

concrete (Ce), the compression force induced by compressive steel reinforcement (C's),

and the tension force by tensile steel reinforcement (T s, T" s). Thus, the total compression

force (CTOT) is the sum ofCe and C's, and the total tension force (TToT) is the sum ofTs,

T" s, and P (axial load). The calculation of each force component is shown in the

following equations:

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23

fc Cc = - tw (kd)

2

CI = (2n - 1) f kd - dl

s c kd

Ts = Asfy

AI S

Til = nAil f [lw- 2(kd)]SAS"fy sse 2(kd)

P Alwtwfc

Cc + Cis-Ts-T"S=P

CTOT = Cc + CiS

(3.5)

Given these force components, the yield moment at the base of the shear wall is obtained

from the following equation:

X= CTOT

T d' + Til ~+P~ s s 2 2 (3.6)

y= TTOT

in which, X is the distance from the top of the wall to the effective point of application of

the total compression force and Y is the distance from the bottom of the wall to the

effective point of application of the total tension force.

3.5.2 Ultimate Strength

According to the ACI 318-99, maXImum concrete strain ranges from 0.003 to

0.004. In this study, the value is taken as 0.003 to be on the conservation side. Referring

to the strain and stress diagrams in Figure 3.6, equating the compression and tension

forces at equilibrium yields the following equation:

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24

0.85ftlfctwc + rAs'(fy-0.85fc) 1 /2 - c

a As fy + AAw f c + a As " EsE cu ( w ) C

(3.7)

in which a and yare the parameters to account for possible material overstrength and

strain hardening and c is the neutral axis depth. The last quantity in right hand side of the

equation is based on the assumption that the web steel reinforcement is lumped at the

center of shear wall.

The total compression force (CTOT) is the sum of compression force by concrete (Cc) and

steel reinforcement (C's), while the total tension force (TTOT) is the sum of tension force

by steel reinforcement (Ts, T" s) and axial load (P). Each component force is given by the

following equations:

Cc = 0.85 /31f c tw c

CiS = r A's (fy - 0.85f c)

Ts =aAsfy

T" A" E [lw /2- c] "f s = a s s&cu c :::; As y

P = Alwtwfc

C = /31 w (neutral axis depth)

CTOT = Cc + CiS

(3.8)

Calculation of above equations yields the neutral aXIS depth (c) and each force

component. The ultimate moment at the base of the shear wall is given by the following

equations:

X= C fJIC + C' d'

c 2 S

CTOT

T d' Til lw P lw s + s 2+ 2

(3.9)

y= TTOT

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25

This calculation usually requires an iteration procedure according to the state of

steel stress. Initially, assume that all steel reinforcements reach yield stress and then

check whether all steel strains are larger than yield strain. If not, a different assumption of

steel stress is tried, check steel strain, and then compare with the yield strain, and so on.

3.6 Nonlinear Static Push-Over Analysis

To determine the capacity of the RC shear walls, stress-strain relationships for

concrete and steel reinforcement are used. In a static analysis, the equivalent RC shear

wall under gravity loads should have a yielding and an ultimate strength either based on

stress-strain relaticnship or based on experimental results. To accomplish this, the

equivalent shear wall model based on DRAIN3DX is calibrated to reproduce the overall

behavior of a shear wall. Nonlinear static push-over analysis in the DRAIN program is a

step-by-step static analysis with an incremental load. Both force and displacement

controls are available in the program.

Consideration of gravity load is also important in nonlinear static cases SInce

stiffness and strength deterioration beyond incipient collapse are generally accelerated by

the p-~ effect The nonlinear static push-over result of an equivalent shear wall having an

aspect ratio of I (17 I" shov.n in Figure 3.7.

J. i Displacement-Based Design Methodology

Under the a"lO,umption of flexural deformation of a shear wall, the top displacement

responses for \Ieldlng and ultimate levels are easily calculated based on a curvature

diagram. This IS the w-called "displacement-based design methodology." However, the

accuracy of this methodology is dependent on the assumption of the curvature diagram.

There are two assumptions required. The plastic depth at the base of the shear wall is

approximately one-half of the wall length and yield curvature is assumed to be 0.0025 (

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26

or 0.003 in UBC-97) divided by the wall length (lw). Based on the curvature diagram, the

ultimate top displacement can be measured by the following equation:

5u = Oy + 8p (h w - ~) 2

= ~ ¢yhw 2 + (¢u - ¢yr) lp (hw - ~) 3 2

(3.10)

where lp is 0.51w and $y is 0.0025/lw. (ou is ultimate displacement, Oy is yield

displacement, 8p is plastic rotation, hw is wall height, $y is yield curvature, $u is ultimate

curvature, Ip is plastic length, and lw is wall length). Note that UBC-97 procedure has

yield displacement as ~ ¢Yhw 2.

40

According to the journal paper, "New methodology for seismic design of RC shear

walls" by John W. Wallace, the maximum concrete compressive strain can be calculated

by multiplying neutral axis depth index, p, by ¢ulw. In other words, the maximum

concrete compressive strain, Be, max, can be given by muitiplying neutral axis depth (c) by

ultimate curvature (<Pu). The value of ¢ulw can be given by a function of the wall aspect

ratio, (hw/lw), and ratio of wall to floor plan area, p. Also, the neutral axis depth index, p, is given by the following equation in the bracket in terms of many material properties.

This equation is derived for rectangular-shaped walls. In this equation for p, the

longitudinal tension and compression reinforcement is assumed to develop a stress of afy

and yfy, respectively, to account for possible material overstrength and strain hardening.

The a and y vary in the range of 1-1.5 and 1-1.25 respectively. (Wallace used a of 1.5

and y of 1.25.)

¢Ulw 0.0025 + hw ( 1 .JP - 0.00125) lw 2200 P

[

r afy P 1 (p+p" __ pI) _ +

j3 ¢u I w = a f c I wtwf c ¢Ul w = c ¢U (0.85j31 + 2p" afy)

fc

(3.11)

Ec, max

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27

where Ec, max = maximum concrete compressive strain

lw = wall length

p = ratio of wall to floor plan area

p = tension steel reinforcing ratio

pI = compression steel reinforcing ratio

pI! = distributed web steel reinforcing ratio

/31 = a factor defined in ACI 318 - 95

P = axial load

fy = nominal yield stress of the steel

f c = concrete compressive stress

tw = wall thickness

c = neutral axis depth

a, r = factors to account for possible material overstrength and strain hardening

In the above equation, the value of the ratio of wall to floor plan area, p, IS

suggested to be 0.5 - 1.0%, which are common. The results from his study show that the

ratio of wall to floor plan area plays a major role in the expected performance of shear

wall buildings. Small ratios less than 1 % indicate a substantial increase in extreme fiber

compression strain. In addition, where relatively few walls are used to resist lateral loads,

damage to one of the walls could potentially result in significant torsional effects.

Therefore, the effect of thickness of shear wall is important. In this study, p of 0.4% is

used. According to ACI318-89, the thickness of walls designed by empirical design

method (Sec. 14.5.3) shall not be less than 1/25 the supported height or length, whichever

is shorter, nor less than 100 mm (3.94 in). Walls designed as compression members can

have slenderness ratios of 40 (ACI318-99, Sec. 14.4) and even up to 70 (ACI318-99, Sec.

14.8).

Another curvature diagram model suggested in ACI 318-99 is a simplified model

that allows for the half of the plastic depth to extend into the wall foundation. This model

was initially proposed by Moehle in 1992. Based on this simple model, ultimate top

displacement response is calculated by following equation:

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28

Eie, max = rjJu C

= 2 ~ c hw lw

Ou 1 = -Ei hw 2/3 e,max

(3.12)

The ultimate drift ratio (8u/hw) is simply given by a function of both maximum concrete

compressive strain (cc, max) and neutral axis depth index (~ ) (Wallace, 1996).

Furthermore, the displacement ductility ratio (f...l) is a function of (cc, max/~) according to

the UBC-97 curvature diagram under the assumption of constant wall aspect ratio.

J1=

1.5(&c,max _ O.0025)(hw _ !) 1 + f3 lw 4

O.0025( hW)2 lw

(3.13)

where ~ is a ratio to account for neutral axis depth (c) in terms of lw. Thus, the different

ductility capacity of the shear wall is affected mainly by the value of maximum concrete

strain dependent on the system for confinement.

3.8. Simulation of Ductility Capacity

To investigate the effect of ductility capacity, the ultimate drift capacity of a shear

wall having an aspect ratio of 1.67 is assumed to be 0.75 % to 1.03 % (ductility ranging

from 5.4 to 7 ~, These values are close to those recommended by Bertero (1991). The

same yielding pomt IS used while different ductility capacities (displacement ductility

factor: 5 4, 6 4. and'" 4) are assumed (Table 3.11). The different ductility capacities of a

shear wall can be a..:hleved by adjusting the second strain hardening ratio, yield stress,

and ultimate stre~~ In DRAIN3DX. The hysteretic model of a shear wall having a

ductility of 64 is ShO\\l1 in Figure 3.9. Different ductility capacities of shear walls are

sketched in Figure 3.10. The ductility capacity parameters are summarized in Table 3.12.

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lw

b (tw)

d

d'

h .....

1 .....

b (tw)

d

d'

hw

29

Table 3.1 Material Properties of Concrete and Steel Reinforcement

and Yield Strength Parameters in One-Shear Wall System.

(Aspect Ratio : 1.67)

360 in As (A's) 10 in2 fy 60 ksi TToT

26.3 in A"s 47.3 in2 Seu 0.003 <py

352in Ee 4000 ksi Sy 0.002 8y

29000 8 in Es kd 89 in My

ksi

3620 600 in fe 4 ksi CTOT Py

kips

Table 3.2 Material Properties of Concrete and Steel Reinforcement

and Ultimate Strength Parameters in One-Shear Wall System.

(Aspect Ratio: 1.67)

360 in As (A's) 10 in2 fy 60 ksi TToT

26.3 in A"s 47.3 in2 Seu 0.003 I-l

352 in Ee 4000 ksi Sy 0.002 8u

29000 8in Es c 53.5 in Mu

ksi

4633 600 in fe 4 ksi CTOT Pu

kips

3620

kips

6.94E-06

0.83 in

742403

kips-in

1687

kips

4633

kips

6.4

5.34 in

946998

kips-in

2152

kips

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lw

b (tw)

d

d'

hw

lw

b (tw)

d

d'

hw

30

Table 3.3 Material Properties of Concrete and Steel Reinforcement

and Yield Strength Parameters in Two-Shear Wall System.

(Aspect Ratio: 1.67)

360in As (A's) 5 in2 fy 60 ksi TToT

13.15 in A"s 24 in2 Ecu 0.003 <py

352 in Ec 4000 ksi Ey 0.002 by

29000 8 in Es kd 89in My

ksi

1810 600 in fc 4 ksi CTOT Py

kips

Table 3.4 Material Properties of Concrete and Steel Reinforcement

and Ultimate Strength Parameters in Two-Shear Wall System.

(Aspect Ratio: 1.67)

360in As (A's) 5 in2 fy 60 ksi TToT

13.15 in A"s 24 in2 Ecu 0.003 J.l

352in Ec 4000 ksi Ey 0.002 bu

29000 8 in Es c 53.5 in Mu

ksi

2317 600 in fc 4 ksi CTOT Pu

kips

1810

kips

6.94E-06

0.83 in

371201

kips-in

844 kips

2317

kips

6.4

5.34 in

473499

kips-in

1076

kips

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lw

b (tw)

d

d'

hw

lw

b (tw)

d

d'

hw

31

Table 3.5 Material Properties of Concrete and Steel Reinforcement

and Yield Strength Parameters in Three-Shear Wall System.

(Aspect Ratio: 1.67)

360 in As (A's) 3.33 in2 fy 60 ksi TToT

8.8 in A"s 15.8 in2 Ecu 0.003 ~y

352 in Ee 4000 ksi Ey 0.002 by

29000 8in Es kd 89 in My

ksi

1207 600 in fe 4 ksi CTOT Py

kips

Tab I e 3.6 Material Properties of Concrete and Steel Reinforcement

and Ultimate Strength Parameters in Three-Shear Wall System.

(Aspect Ratio: l.67)

360 in As (A's) 3.33 in2 fy 60 ksi TToT

88 in Ails 15.8 in2 Ecu 0.003 ~

352 in Ee 4000 ksi Ey 0.002 bu

29000 8in Es c 53.5 in Mu

ksi

1544 600 in fe 4 ksi CTOT Pu

kips

1207

kips

6.94E-06

0.83 in

247468

kips-in

562 kips

1544

k-ln~ ---r-

6.4

5.34 in

315666

kips-in

717 kips

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lw

b (tw)

d

d'

hw

lw

b (tw)

d

d'

hw - -

32

Table 3.7 Material Properties of Concrete and Steel Reinforcement

and Yield Strength Parameters in One-Shear Wall System.

(Aspect Ratio: 4.0)

360 in As (A's) 100 in2 fy 60 ksi TToT

96 in A"s 69.1 in2 f:cu 0.003 ~y

352 in Ec 4000 ksi f:y 0.002 Oy

29000 8 in Es kd 87.6 in My

ksi

14887 1440 in fc 4 ksi CTOT Py

kips

Table 3.8 Material Properties of Concrete and Steel Reinforcement

and Ultimate Strength Parameters in One-Shear Wall System.

(Aspect Ratio: 4.0)

360 in As (A's) 100 in2 fy 60 ksi TTOT

96in A"s 69.1 in2 f:cu 0.003 ~

352in Ec 4000 ksi f:y 0.002 Ou

29000 8 in Es c 39.7 in Mu

ksi

16670 1440 in fc 4 ksi CTOT Pu

- - - - 1· -KIpS

14887

kips

6.94E-06

4.80 in

3475234

kips-in

3389

kips

16670

kips

4.5

21.48 in

3929948

kips-in

3832

- 1 • -KIpS

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lw

b (tw)

d

d'

33

Table 3.9 Material Properties of Concrete and Steel Reinforcement

and Yield Strength Parameters in Two-Shear Wall System.

(Aspect Ratio: 4.0)

360 in As (A's) 50 in2 fy 60 ksi TToT

48 in A"s 34.6 in2 Seu 0.003 Q>y

352in Ee 4000 ksi Sy 0.002 by

29000 8 in Es kd 87.6 in My

ksi ,

7443

hw ..11440 in I fe 4 ksi kips

lw

b (tw)

d

d'

hw

Table 3.10 Material Properties of Concrete and Steel Reinforcement

and Ultimate Strength Parameters in Two-Shear Wall System.

(Aspect Ratio: 4.0)

360 in As (A's) 50 in2 fy 60 ksi TToT

48in A"s 34.6 in2 Seu 0.003 J.l

352in Ee 4000 ksi Sy 0.002 bu

29000 8 in Es c 39.7 in Mu

ksi

8335 1440 in fe 4 ksi CTOT Pu

kips

7443

kips

6.94E-06

4.80 in

1737617

kips-in

1694

kips

8335

kips

4.5

21.48 in

1964974

kips-in

1916

kips

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34

Table 3.11 Different Ductility Capacity of Shear Wall (Aspect Ratio: 1.67).

Properties Ductility 5.4 Ductility 6.4 Ductility 7.4

lw 360 in 360 in 360 in

b (tw) 8.8 in 8.8 in 8.8 in

d 352 in 352 in 352 in

d' 8 in 8 in 8 in

hw 600 in 600 in 600 in

As (A's) 3.33 in2 3.33 in2 3.33 in2

A"s 15.8 in2 15.8 in2 15.8 in2

Ec 4000 ksi 4000 ksi 4000 ksi

Es 29000 ksi 29000 ksi 29000 ksi

Pc 4 ksi 4 ksi 4 ksi

fy 60 ksi 60 ksi 60 ksi

Sy 0.002 0.002 0.002

P 0.15 0.15 0.15

Eeu 0.00251 0.00300 0.00349

Eeu/P 0.0169 0.0202 0.0235

c 53.5 in 53.5 in 53.5 in

<h 6.94E-06 6.94E-06 6.94E-06

8y 0.83 in 0.83 in 0.83 in

8u (0/0) 4.51 in (0.75%) 5.34 in (0.89%) 6.18 in (1.03%)

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35

Table 3.12 Parameters Used in DRAlN3DX for Modeling Different Ductility Capacities

of Three-Shear Wall System.

Parameters Ductility 5.4 Ductility 6.4 Ductility 7.4

Modulus Kl 3.33E03 3.33E03 3.33E03

Modulus K2 4.700 4.600 1.200

Modulus K3 0.001 0.001 0.001

Yield Stress SIT in 3.167 3.167 3.167

Tension

Yield Stress S2T in 3.933 3.933 3.933

Tension

Yield Stress SIC in 3.167 3.167 3.167

Compression

Yield Stress S2C in 3.933 3.933 3.933

Compression

Stiffness 0.01 0.01 0.01

Degradation Factor

Tension Strength 0.30 0.30 0.30

Degradation Factor

Compression

Strength 0.30 0.30 0.30

Degradation Factor

Saturated Strain in 1.0 1.0 1.0

Compression

Saturated Strain in 1.0 1.0 1.0

Tension

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36

Pinch Factor 1.0 1.0 1.0

Pinch Strength 0.95 0.95 0.95

Factor

Pinch Plateau Factor 0.95 0.95 0.95

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37

Figure 3.1 R.ocking Motion and Outriggering Interaction (Bertero, 1991).

-Z .x -0 c{

0 ...J

800

600

400

200

0

-200

~OO -4 -2 0 2 4 6 8 10 12 14 16 18 20

DISPLACEMENT (mm)

Figure 3.2 Hysteretic Curve of Shear Wall in Experiment (Paulay, 1982).

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38

Rigid Floors

Plastic hinges at base

Figure 3.3 Equivalent Shear Wall Model.

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Stress

39

Basic , .... ------ curve

,__--- Comp. 1 ~--Comp.2

--------~~~~-------. Comp.3

Stress

(a) Basic trilinear curve is first decomposed into three parallel components

(b) Stiffness degradation factor applies to both elastic-plastic components

Stress

I

,

Strength loss factor = (b/SC)* STDF

(not less than SID F)

:' Strength loss factor -_/ W\ = «a+c)/Sll*SCDF

Strength loss factor = (alSn* SCDF

(c) Strength loss in each component depends on strength degradation factor (STDF or SCDF)

and ratio of accumulated plastic displacement to saturated displcement (ST or SC)

Stress

PF*ST1--------

_ (l-PSF)*PF*SC PPF*GL

--~·--tPF*SC

(d) Pinch factor (PF) divides each component into pinching and non-pinching

parts. Pinch strength factor (PSF) and plateau factor (PPF) are then applied.

Figure 3.4 Trilinear and Degradation Model of Fiber Beam Column Element.

(prakash et aI, 1994)

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40

:,:s······· .................................................... ~.:::.::::::::.~~:::t:: ............ . f' s

• • d • •

• •

d'

Strain Stress

Figure 3.5 Stress and Strain Diagram at Yield Strength.

O.85fc

f\'~: ••••••• .....................................

..... :::.:::::::l~:::: .................... ~ f' s

• • • • ..

• •

Strain Stress

Figure 3.6 Stress and Strain Diagram at Ultimate Strength.

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2200 2000 1800

(j) 1600 a. ;g. 1400

:E, 1200 c ~ ~.-

41

3·0 Nonlinear Static Push·Over Analyses

• One Shear Wall System .................. Two Shear Wall System ............... Three Shear Wall System

•.. ..-....................... -............................................... .... Ci5

:~~ f:.:~· .. · .. ··•··•··•··•· ... · .. · .. ········a ................. .

400 It 200 !f O--~~~~~~~~~~~~~~~~~

o 2 3 4 5 6 7 8 9 10 X Displacement (in)

Figure 3.7 Nonlinear Static Push-Over Analysis of Shear Wall in One-, Two-, and Three­

Shear Wall System.

1 p

(a) UBC 97 Idealization (b) Simplified Idealization

Figure 3.8 Curvature Diagram.

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c ., r.J)

0.. ~

C Q)

E 0 ~ Q) r.J)

ro al

42

Hysteretic Response of Shearwall (Ductility=6.88)

1200000.0 1000000.0

800000.0 600000.0 400000.0 200000.0

0.0 -200000.0 -400000.0 -600000.0 -800000.0

-1000000.0 -1200000.0

-40 -30 -20 -10 0 10 20 Top Story Displacement (in)

30 40

Figure 3.9 Hysteretic Response of One-Shear Wall System.

(Aspect Ratio: 1.67, Ductility: 6.4)

Strength

Disp

Figure 3.10 Different Ductility Characteristics of Shear Walls.

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CHAPTER 4

MODELING AND DESIGN OF DUAL AND SMRF SYSTEMS

4.1 Introduction

During strong ground motions, well-engineered buildings may still undergo severe

damage. These buildings, however, have the potential to endure the motion and maintain

their integrity without collapse. Dual systems are one of these systems. They are typically

composed of a primary RC shear wall subsystem and a secondary special moment

resisting frame (SMRF) subsystem. Dual systems may survive during strong motions

because the secondary subsystem (SI\1RF) contributes in resisting lateral force, even after

the primary lateral system (RC shear wall) fails. The damaged dual system, therefore, is

still capable of resisting lateral loads due to the alternative load path provided by the

secondary system.

period of the system. Obviously, the secondary subsystem is much more flexible and, as a

result, the damaged structure has a much longer natural period. If the period of the peak

earthquake excitation is very close to the fundamental period of the dual system, much of

the energy will be absorbed by the system hysteresis and may cause the failure of the

primary subsystem After the failure of the primary subsystem, the natural period of the

damaged system lengthens and the earthquake energy at this period may drop

significantly and the damaged dual system now supported by the secondary subsystem

can survive. If the period corresponding to peak earthquake excitation is long, the dual

systems may survive without failure of any subsystem.

According to the principle of structural dynamics and past experience, high-rise

buildings and base-isolated buildings are vulnerable to earthquakes having long

predominant periods, while low-rise rigid buildings are vulnerable to earthquakes having

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short predominant periods. Dual systems are more earthquake-resistant because the

change in fundamental structural periods after damage may improve the chance of

surviving a given earthquake. In other words, the redundancy in the form of two lines of

defense in a dual system dramatically increases its reliability, especially under severe

earthquakes since the redundancy effect is more clearly seen in the fully nonlinear

behavior of building structure.

In reliability and redundancy evaluation of dual systems, a 3-dimensional structural

analysis is required to account for the interaction between the shear walls and the special

moment resisting frames. Therefore, the torsional motion and biaxial interaction in the

building structure need to be incorporated into the analysis. In addition, the rocking

motion of the shear wall under out-of-plane flexible diaphragm and outriggering

interaction with the frame should also be considered in the analysis.

4.2 Member Capacity Requirements

In ATC-34, the redundancy of a dual system is accounted for by the use of a

response modification factor (R factor) larger than that for a pure shear wall system. In

A TC-19, the redundancy of dual reinforced concrete shear walls with steel moment frame

systems was considered. As shown in Figure 4.1, a frame of three bays including one

flexural wall with a nominal plastic moment capacity of 1000 units is compared with

another frame of three bays including two flexural walls, each with a nominal plastic

moment capacity of 500 units. It is suggested by ATC-19 that the single shear wall

framing system needs to have 40 percent higher design lateral strength in order to achieve

the same level of reliability of the double shear wall framing system.

The NEHRP-97 provisions stipulate that the moment frame (in dual systems) shall

be capable of resisting at least 25 % of the design force. The total shear force resistance is

to be provided by the combination of the moment frame and the shear walls or braced

frames in proportion to their rigidities. In order for the moment frames to contribute

significantly to the resistance of the dual system, their stiffness and strength should be

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comparable to those of the shear walls. Both the shear walls and the back-up moment

frames resist the lateral force at the initial stages of loading. After the failure of the first

shear wall, the lateral force is redistributed through the damaged dual system according to

the load-carrying capacity of the system. Therefore, even though the total lateral

resistance of the shear walls is kept the same, the number of shear walls may still playa

significant role in system redundancy. Moreover, the ductility capacity of shear walls is

another factor affecting the load-carrying capacity of system and contributing to system

redundancy. In addition, the statistical correlation of yielding and ultimate strength

among shear walls, and the ratio of the earthquake excitation variability to that of the

lateral resistance of shear wall may also affect the redundancy of the system, as seen in

the parametric study of simple parallel systems under stochastic excitation in Chapter 2.

4.3 Uncertainty in Material and Member Properties

In response analysis of structures under earthquakes, a realistic consideration of the

material and member uncertainties is required. The Monte-Carlo method can be used to

take into account the effect of such uncertainty. For this purpose, the yield strength (Fy)

and ultimate strength (Fu) of shear walls are treated as random variables and assumed to

be nonnally distributed with a coefficient of variation of 10-20% (Y. J. Park, 1995). The

yield strength of A36 and Grade 50 steel (Fy) for both beams and columns in dual

systems is also assumed to have 15% uncertainty (Kennedy and Baker, 1984).

4.4 Design Issues of Secondary Steel Moment Resisting Frame (SMRF) System

The design philosophy of a SMRF as a secondary subsystem has not been made

clear in most seismic design guidelines and building codes. Because the SMRF is used as

a secondary system, over-design and cost have often been a concern. The stiffness and

strength of the SMRF after the collapse of the shear wall, however, will control the

response of the system and have important safety implications.

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The secondary SMRF system in this study is designed according to the requirement

ofNEHRP-97 as shown in Figure 4.2. The sum of base shear of the SMRF should exceed

25% of the design base shear. The design is that of a strong column and weak beam

(SCWB).

4.5 Design of Dual Systems

4.5.1 Five-Story, One-Way Dual Systems

Three five-story, one-way dual buildings were designed according to the

requirements ofNEHRP-97 and suggestions of ATC-19 (1995). The site of the structure

was assumed to be in Los Angeles, California. Each floor was assumed to weigh 3150

Kips, thus, the total weight of the structure was 15750 Kips. The site condition is

assumed to be stiff soil, which is Type D specified in NEHRP-97. The story height is 10

ft for all stories. The number of shear walls in the system varies from one to three. The

material properties of concrete and steel reinforcement in the one-, two-, and three-shear

wall systems are given in Chapter 3, Table 3.1 through 3.6.

As shown in Figure 4.3, the shear wall systems resist only the force in the East­

West direction. In the North-South principal direction, there are no shear walls and the

system is entirely resisted by the SMRF system. The member sizes of the SMRF systems

are given in Table 4.1. The total weight of the shear walls was 750 Kips, i.e. the same for

the one-, two-, and three-shear wall systems. The design base shears in the E-Wand N-S

directions were 2270 Kips and 2170 Kips respectively. The structural periods are 0.68

seconds in the E-\V direction, 0.93 seconds in the N-S direction, and 0.66 seconds in

rotation for the one-shear wall system, 0.67 seconds, 0.93 seconds, and 0.56 seconds for

the two-shear wall system, and 0.63 seconds, 0.93 seconds, and 0.46 seconds for the

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three-shear wall system. More details of these dual systems will be discussed in Chapter

5.

4.5.2 Five-Story, Two-Way Dual Systems

Three five-story, two-way dual systems of one, two, and three shear walls were

also considered. A shear wall having an aspect ratio of 1.67, as used in the above one­

way dual systems, was again used in both the E-W and N-S directions (Figure 4.4). The

secondary SMRF in the N-S direction was redesigned according to the provisions in

NEHRP-97. The member sizes of the S11RF systems are given in Table 4.2. The

fundamental structural periods are, 0.61 seconds in the E-W direction, 0.56 seconds in the

N-S direction, and 0.97 seconds in rotation for the one-shear wall system, 0.59 seconds,

0.57 seconds, and 0.51 seconds for the two-shear wall system, and 0.59 seconds, 0.56

seconds, and 0.56 seconds for the three-shear wall system. The same material properties

and performance parameters of shear walls are used.

4.5.3 Ten-Story, Two-Way Dual Systems

Two ten-story', two-way dual systems of one and two shear ·walls 'were designed .. AL

shear wall having an aspect ratio of 4 and displacement ductility of 4.5 was designed for

severe earthquakes in Los Angeles, California. The site condition is assumed to be stiff

soil, which is Type D specified in NEHRP-97. The story height is 12 ft for all stories.

Target yield and ultimate strengths were 3338.5 and 3832.8 Kips respectively. Target

yield and ultimate displacements of shear wall were 4.8 and 21.5 inches respectively. The

total weight of the dual systems was 31500 Kips and the design base shear was 3960

Kips. The same shear wall configurations used in 5-story, two-way dual systems were

used (Figure 4.4). The secondary SMRF subsystems (Table 4.3) for both directions were

designed such that the strengths of these subsystems meet the minimum strength of 990

Kips required in the guideline. The structural periods are 0.91 seconds in the E-W

direction, 0.90 seconds in the N-S direction, and 1.94 seconds in rotation for the one-

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shear wall system and 0.81 seconds, 0.73 seconds, and 0.94 seconds for the two-shear

wall sy stem.

The drift limit is suggested by seismic codes as a check of adequacy of preliminary

building design. For both dual and SMRF systems, an inelastic drift ratio of 2% is

recommended in NEHRP-97. It is noted that different deflection amplification factors are

assigned for different seismic systems in the calculation of inelastic drift ratio.

4.6 p-~ Effect

Second order effects resulting from decreases in flexural stiffness and lateral

stiffness due to drift are included in the nonlinear analyses of building structures. The

effect of decrease in flexural stiffness due to changes in geometric stiffness is usually

negligible compared to that from decrease in lateral stiffness. At each time increment, the

effect of secondary moments caused by story weights may amplify the lateral

displacement and, as a result, the structure may become unstable. Therefore, the P-,1.

effect cannot be ignored in the design. In low-rise buildings, the P-,1. effect is mainly due

to the changes of geometric stiffness. It is much larger in high-rise buildings because of

the possible large drift. The effect ofP-,1. is considered in the DRAIN3DX program.

4.7 Interaction between Shear Walls and SMRF Systems

Nonlinear push-over analysis of five-story, two-way dual systems of two shear

walls (Figure 4.4 (b)) was carried out. The mass at each diaphragm is pushed

incrementally by triangular-shaped lateral forces in the E-W direction. The lateral shear

forces are distributed through overall diaphragms. The interaction among two shear walls

and two SMRF systems is plotted in Figure 4.5. The figure shows the shear force transfer

within the system by interaction. In the initial stage of monotonic loading at the mass

center, the two SMRF systems carry only a small portion of the lateral loads. The portion

of the load resisted by the frame increases as the resistance of the shear wall reaches a

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plateau and decreases. It appears that the shear wall is acting as the active component and

the SIvlRF is acting as a standby component. In addition, the total story shear force, i.e.

sum of shear forces of shear walls and SMRF systems, of the dual systems is shown in

Figure 4.6.

4.8 Design of SMRF Systems

4.8.1 Three-Story Moment Frame Systems with No Torsion

The responses of two three-story short period moment frame systems without

accidental torsion will be investigated to examine the effect of different number of bays.

F or this purpose, a 4 x 4 bay SMRF system and a 6 x 6 bay SMRF system were designed

(Figure 4.7 and 4.8). The systems were designed for the same lateral resistance and

verified by push-over analyses (Figure 4.9). The beams and columns were carefully

designed by selecting larger sizes for the system of smaller number of bays (Table 4.4

and 4.5), and so on. The design base shear of the systems was 1148 Kips and the

fundamental periods were 0.76 sec in both E-W and N-S direction and 0.44 sec in

rotation.

4.8.2 Nine-Story Moment Frame Systems with No Torsion

Two equivalent nine-story moment frames located in LA, California were also

designed to consider the reliability and redundancy of SMRF structures with longer

periods. The site condition is assumed to be stiff soil, which is Type D specified in

NEHRP-97. Torsion was not considered. Two systems of different number of bays, a 5 x

5 bay and a 8 x 8 bay, were investigated (Figure 4.10 and 4.11). These systems were

designed as strong column weak beam (SCWB) systems according to NEHRP-97. Table

4.6 and 4.7 show the member sizes of the beams and columns. The same design base

shear of 1715 Kips was used for both systems. The method of selecti<?n for beams and

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columns was identical to that of three-story systems. The period in both E-Wand N-S

directions is l. 7 sec and the rotational period is 0.98 sec.

4.8.3 Three-Story Moment Frame Systems with Torsion and Brittle Connection

Failure

Three three-story moment frames of 1 x 1 bay, 2 x 2 bay, and 3 x 3 bay system

with 5% accidental torsion were designed (Figure 4.12, 4.13, 4.14, and 4.15, Table 4.8,

4.9, and 4.10). The systems were designed such that these three frames have the same

lateral resistance but brittle connections. The brittle connection failure has been a serious

concern after the Northridge earthquake, 1994 and may have a significant impact on the

redundancy. The connection fracture hysteresis model of Wang and Wen (1998, Figure

4.16) was employed to simulate test results by Anderson, et al (1995). The first three

vibration periods of the system are 0.85 (E-W direction), 0.85 (N-S direction), and 0.50

(torsion) seconds.

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Table 4.1 Design of S:rv1RF of 5-Story, One-Way Dual System.

E-W SMRF N-S SMRF Story

Column Beam coiumn Beam

5 W24x68 W24x55 W36x160 W36x135

3-4 W24x76 W24x62 W36x182 W36x150

1 W24x84 W24x68 W36x210 W36x160

Table 4.2 Design of S:MRF of 5-Story, Two-Way Dual System.

E-W SMRF N-S SMRF Story

Column Beam Column Beam

5 W24x68 W24x55 W24x131 W24x104

3-4 W24x76 W24x62 W24x146 W24xl17

1 W24x84 W24x68 W24x162 W24x131

Table 4.3 Design ofS:rv1RF of 10-Story, Two-Way Dual System.

E-W SMRF N-S SMRF Story

Column Beam Column Beam

9-10 W24x131 W24x104 W24x131 W24x104

5-8 W24x146 '"("1: T,.." A, .1 1 ,.., ,"("1:T,.."A,.1 AC W24xl17 W L.LtXll I W L.LtXILtO

1-4 W24x162 W24x131 W24x162 W24x131

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Table 4.4 Design of 3-Story, 4 x 4 Bay SJv1RF System.

E-W SMRF N-S SMRF Story

Column Beam Column Beam

3 W36x135 W33xl18 W36x135 W33xl18

2 W36x150 W33x130 W36x150 W33x130

1 W36x160 W33x141 W36x160 W33x141

Table 4.5 Design of3-Story, 6 x 6 Bay SJv1RF System.

E-W SMRF N-S SJ\1RF Story

Column Beam Column Beam

3 \V30xl16 W30x99 W30xl16 W30x99

2 \\'30x124 W30x108 W30x124 W30xlO8

1 \\'30x132 W30xlO8 W30x132 W30xlO8

Table 4 6 Design of9-Story, 5 x 5 Bay SJv1RF System.

E-W SMRF N-S SMRF Story

Column Beam Column Beam

7-9 \\"36x210 W36x170 W36x210 W36x170

4-6 \\'36x232 W36x182 W36x232 W36x182

1-3 \V36x256 W36x182 W36x256 W36x182

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Table 4.7 Design of 9-Story, 8 x 8 Bay SMRF System.

E-W SMRF N-S SMRF Story

Column Beam Column Beam

7-9 W30x148 W30x124 W30x148 W30x124

4-6 W30x173 W30x124 W30x173 W30x124

1-3 W30x191 W30x148 W30x191 W30x148

Table 4.8 Design of3-Story, 1 x 1 Bay SMRF System.

E-W SMRF N-S SMRF Story

Column Beam Column Beam

.., W14x193 W27x94 W14x193 W27x94 j

2 W14x193 W36x182 W14x193 W36x182

1 W14x193 W36x150 W14x193 W36x150

Table 4.9 Design of3-Story, 2 x 2 Bay SMRF System.

E-W SMRF N-S SMRF

Story Exterior Interior Exterior Interior Beam Beam

Column Column Column Column

3 W14xlO9 W14x193 W24x62 W14xlO9 W14x193 W24x62

2 W14xlO9 W14x193 W3Oxl16 W14xlO9 W14x193 W3Oxl16

1 W14xlO9 W14x193 W3Ox99 W14xlO9 W14x193 W3Ox99

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Table 4.10 Design of3-Story, 3 x 3 Bay SMRF System.

E-W SMRF N-S S:MRF

Story Exterior Interior Exterior Interior Beam Beam

Column Column Column Column

3 W14x132 W14x159 W21x57 W14x132 W14x159 W21x57

2 W14x132 W14x159 W27x84 W14x132 W14x159 W27x84

1 W14x132 W14x159 W24x76 W14x132 W14x159 W24x76

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(a) One-Shear Wall System (b) Two-Shear Wall System

Figure 4.1 Redundancy in Shear Wall Systems (ATC-19, 1995).

Base Shear

O.91V

( Dual system

--- -- -- p\ -Dual system "fails· at

'" deformation capacity of shear wall

Shear wall

( Back·up moment frame

Roof Drift Index (%)

(a) Force-Displacement Relationship for a Dual System (ATC-19, 1995)

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en 0..

1000 900 800 700

56

3-D Static Push-over analysis of X-Dir SMRF

g .!: 600 _________ _

0, 500 c ~

Ci5 400 300 200 100

Immm_m_- 25 % of Design Base shearl

O~~~~~~~~~~~~~~~~~~

o 2 4 6 8 10 12 14 16 x displacement(in)

(b) t.Jonlinear Static Analysis of Secondary S:r-v1RF System

Figure 4.2 Design Requirement of Secondary SMRF System in a Dual System.

5@30 ft

4@30 ft

Figure 4.3 Ca) Five-Story, One-Way Dual Systems with One Sht?ar Wall.

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5@30 ft

4@30 ft

Figure 4.3 (b) Five-Story, One-Way Dual Systems with Two Shear Walls.

5@30 ft

4@30 ft

Figure 4.3 (c) Five-Story, One-Way Dual Systems with Three Sh~ar Walls.

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5@30 ft

4@30 ft

Figure 4.4 (a) Five- or Ten-Story, Two-Way Dual Systems with One Shear Wall.

4@30 ft

I T

.I.

.!:

5@30 ft

. I. I ! I .L o!.

Figure 4.4 (b) Five- or Ten-Story, Two-Way Dual Systems with Two Shear Walls.

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5@30 ft

4@30 ft

Figure 4.4 (c) Five-Story, Two-Way Dual Systems with Three Shear Walls.

800

700 C;; .9- 600 ~ CD 500 u 0

LL 400 "§ CD 300 co

.-1

200

100

0 0 2

• 1 st Shear Wall -----.~.----- 2nd Shear Wall ._._._.-6-._._.- 1 st SMRF

--..5.}--- 2nd SMRF

3 4 Top story displacement (in)

Figure 4.5 Interaction between Shear Walls and SMRF Systems.

(5-Story, Two-Way, Two-Shear Wall System)

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5000

en 4000 a. g (J.)

3000 2 0 u..

Cti ID 2000 co -1

1000

0 0

60

Nonlinear Static Push-Over Analysis

10 20 30

- ...... - 1st Story '-'-0-'- 2nd Story ----4---- 3rd Story •••• 0() • • •• 4th Story

• 5th Story

40 Story displacement at mass center (in)

50

Figure 4.6 Nonlinear Static Push-Over Analysis of 5-Story, Two-Way, Two-Shear Wall

System.

4@30 ft = 120 ft

6@30 ft=180 ft

Figure 4.7 Three-Story, 4 x 4 Bay SMRF System.

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6@20 ft = 120 ft

61

9@20 ft=180 ft

Figure 4.8 Three-Story, 6 x 6 Bay SMRF System.

4000

__ 3000 en Cl..

g Q)

~ .2 2000 co Q; co -l

1000

Nonlinear Static Push-Over Analysis (Disp. Control)

.,...... .. .• --+ ........... ...

~,~,,'~~::. .. ~' .. ',-~ ........ .

I, i" /'i / . (

r f /' r ~ J l / I :' [ / . ~

- 4 x 4 bay system (3rd story) ....... ""...... 6 x 6 bay system (3rd story) ............ 4 x 4 bay system (2nd story) ..... +........ 6 x 6 bay system (2nd story) --... -- 4 x 4 bay system (1st story) ........ - ...... 6 x 6 bay system (1st story)

o~~--~--~--~~--~--~~~~--~---o 2 3 4 5 6 7 8 9 10

Story displacement at mass center (in)

Figure 4.9 Nonlinear Static Push-Over Analysis of 4 x 4 and 6 x 6 Bay Systems.

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6@25 ft = 150 ft

1O@ 15 ft = 150 ft

62

6@25 ft=150 ft

Figure 4.10 Nine-Story, 5 x 5 Bay SMRF System.

10@ 15 ft=150 ft

Figure 4.11 Nine-Story, 8 x 8 Bay SMRF System. -

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63

3@30 ft

I • • I I I · I

-I- -pooo

4@30 ft · ~ · '" · ~ - . -- --

I • • I

I • • I

Figure 4.12 Three-Story, 1 x 1 Bay SMRF System.

3@30 ft

• 1 I · ~ · ~

• l- • l-

· ~ · '" - l- • I--I- .~

1 I · · • • I

I • • . . I

Figure 4.13 Three-Story, 2 x 2 Bay SMRF System.

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64

3@30 ft

1@15 ft 1 I • --- • -'- I -' I I • I I . . • I

-~ --· '"' • l-

· '"' · "" • l- • I-

3@30 ft

-'" -. · '"

. . • I- -.

1@15ft I -- --I I I I I I I I I · . . . . . I

Figure 4.14 Three-Story, 3 x 3 Bay SMRF System.

1100

1000

900

en 800 Cl...

g 700

Q) 600 2

.2 500 CO CD 400

Ci:i .....J 300

200

100

0 0

Nonlinear Static Push-Over Analysis (Disp. Control)

._._._.",_._._.- 2 X 2 bay system (3rd story)

• 1 X 1 bay system (3rd story) .-.-.-.~-.-.-.- 2 X 2 bay system (2nd story)

1 X 1 bay system (2nd story) ._._._ ... -._.-.- 2 X 2 bay system (1 st story)

1 X 1 bay system (1 st story)

2 3 4 5 6 7 8 9 10 11 12 13 14 15

Story Displacement at mass center (in)

Figure 4.15 Nonlinear Static Push-Over Analysis of 1 x land 2 x 2 Bay Systems.

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65

100

-3 3

Figure 4.16 Brittle Fracture Model (Wang and Wen, 1998).

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66

CHAPTERS

RESPONSE ANALYSIS AND PERFORMANCE EVALUATION

5.1 Introduction

The nonlinear dynamic responses of dual systems under SAC phase-2 ground

motions are studied. Since the dual systems are composed of two subsystems, to measure

the performance of the system, at least one response variable for each subsystem is

required. The in-plane lateral resistance of a shear wall is the primary component in

resisting earthquake damage. The out-of-plane capacity of shear wall is usually ignored

in the design, e\'en though it still offers some resistance. Therefore, the in-plane

maximum shear wall drift ratio (SWDR) in a nonlinear analysis will be used as a

reasonable measure of shear wall performance. The maximum instantaneous vector sum

of two orthogonal column drift ratio (MCDR) in a nonlinear analysis will be used as a

measure of system overall performance. Due to the torsional motion in three-dimensional

analysis, t\1CDR l~ 2 better indicator of total system damage than the 2-dimensional story

drift ratio.

5.2 SAC-2 Ground Motions

To in\'estl~Jte pre·~orthridge steel connection behavior, SAC phase 2 ground

motions were generated by Somerville (1997) using existing records and broad-band

simulations, The ground motions were corresponding to 2%, 10%, and 50% exceedance

probability in 50 years. These ground motions were generated such that they are

compatible with the USGS uniform-hazard target response spectra. The use of SAC

ground motions provides a convenient way to calibrate building reliability covering a -

wide range of response, i.e. from linear to nonlinear behavior. The building response

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67

statistics can be easily determined for a given probability of exceedance. Another

advantage of using SAC motions is that a relatively small number of building response

simulations is required to determine the required response statistics. Redundancy

evaluation as well as probabilistic performance study is, therefore, carried out using these

ground motions. Examples of SAC phase-2 time history ground motions are given in

Figure 5.1. The ground motions shown in the figure, LA21 and 22, are based on Kobe

earthquake in 1995. LA21 is a fault-normal and LA22 is a fault-parallel ground motion.

5.3 Five-Story, One-Way Dual Systems

A number of case studies are carried out. They are categorized according to number

of shear walls, shear wall ductility capacity, shear wall strength correlation, and ratio of

demand versus capacity uncertainty as shown in Table 5.1. The selection mark (./) in the

Table indicates the selected items to be analyzed for systems with properties marked by

"X". For example, for the case study of the effect of number of shear walls, systems of 1,

2, and 3 shear walls are examined with properties that include shear wall ductility

capacity of 6.4, zero correlation in shear wall strength, and a ratio of earthquake to

strength variability of 2.67, as shown in the third column of the Table.

5.3.1 Effect of Number of Shear Walls

As seen in the simulation study of parallel systems, keeping the mean total lateral

resistance constant allows a fair comparison of redundancy for the systems with different

numbers of lateral resistance components. Since a dual system is a parallel system, the

number of shear walls is one of the important factors affecting the redundancy of dual

systems. Also, the load-carrying capacity after the failure of any shear walls needs to be

carefully considered.

The configurations of dual systems with different number of shear walls were

illustrated in Chapter 4. The hysteretic response of a single shear wall under cyclic

loading was also shown in Chapter 3. The modeling of two- and three-shear wall systems

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68

is essentially the same as that of the one-shear wall system except that the dimension and

stiffness/strength of the shear walls are properly adjusted to maintain the same total

resistance, i.e. by varying the thickness and longitudinal and web steel reinforcement of

the shear wall. For instance, the thickness and longitudinal and web steel reinforcement

of each shear wall in the two-shear wall system are approximately half of those of the

one-shear wall system, etc. Nevertheless, different shear wall locations produce a

different torsional vibration period causing widely different building dynamic

characteristics.

The redundancy effect of a system of more than one shear wall resides in the

residual strength of the system. In a system of multiple shear walls, after the failure of

any first shear wall, the load is redistributed and transferred to the other walls and

moment frames, which may prevent sudden total collapse and allow time for occupants to

escape.

The seismic hazard to the shear wall can be expressed in terms of spectral

acceleration at the fundamental natural period. The statistics (median and coefficient of

variation, COY) of spectral acceleration at the fundamental period in the X direction for

the shear wall and the biaxial spectral acceleration for the total system corresponding to

three probability levels are given in Table 5.2.

The displacement time history at the top of the 5-story, one-way dual systems of a

single shear wall under LA21 and 22 excitations is shown in Figure 5.2. Because the

diaphragm of the building system has three degrees of freedom, i.e. X, Y and rotation

with respect to Z axis, the three displacements of lumped floor mass are displayed. As

expected, the 20/0 in 50 years SWDR responses are sensitive to the number of shear walls

since shear walls become highly nonlinear under the excitation. The SWDR responses are

observed to be 2.52% in one-shear wall system, 2.50% in two-shear wall system, and

2.43% in three-shear wall system, a reduction of approximately 3.7% from one to three

shear walls.

The displacement trajectory of the mass center under LA21 and 22 biaxial

excitations can be traced. The displacement trajectories of mass center for one-, two-, and

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69

three-shear wall systems under the same biaxial loadings are compared in Figure 5.3. The

response statistics are also summarized in Table 5.8 and the scatters of response variables

are shown in Figure 5.6 and 5.7.

5.3.2 Effect of Ductility Capacity of Shear Walls

A three-wall system with an aspect ratio of 1.67 and three different ductility

capacities of 5.4, 6.4, and 7.4 was selected and designed according to displacement-based

methodology explained in Chapter 3.

The response statistics are summarized in Table 5.9. It is seen that the median

SWDR responses of shear walls subject to 2% in 50 years earthquakes with or without

accidental torsion show that they are not sensitive to the variation of ductility capacity,

which has little effect on the load-carrying capacity, and therefore, on shear wall

response. The results are also shown in Figure 5.1 O-b. The failure probability of a shear

wall, however, may still depend on the ultimate drift capacity. The redundancy

implication will be discussed in Chapter 6.

5.3.3 Effect of Correlation of Shear Wall Strength

Since shear walls are made of the same concrete and steel reinforcement and

constructed by the same process, there is a statistical correlation between them by nature.

In the simulation study of parallel systems by Gollwitzer and Rackwitz (1990), the

correlation of components in the system was shown to have an important effect on

redundancy. Therefore, the effect of lateral resistance correlation among shear walls in

the dual systems was investigated. Two shear walls of ductility 6.4 were selected for this

purpose. Correlation coefficients of 0.0, 0.2, 0.6, and 1.0, were selected and the correlated

resistance random variables were generated through Monte-Carlo simulation.

While the SWDR responses for 50% in 50 years earthquakes appeared to be within

elastic range, the responses for 2% in 50 years earthquakes were definitely beyond the

elastic li1l1it. The results suggest that the effect of correlation does _ not significantly

contribute to the SWDR response. The lateral capacity by the secondary system absorbs

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70

some the effect of shear wall strength correlation. Table 5.10 summarizes the response

statistics.

5.3.4 Effect of the Ratio of Earthquake Load to Shear Wall Resistance Variability

It is well known that the response of a structure is highly dependent on the

characteristics of earthquake ground motions and the reliability of the structure is

sensitive to the uncertainties of earthquake loads. The demand versus capacity

uncertainty, therefore, is an important factor in the reliability of structure. Three shear

walls of a ductility capacity of 6.4 were selected to investigate this effect. Three

representative resistance uncertainties, 10%, 15%, and 20%, were used resulting in the

ratios of load to resistance variability of 5.33,3.55, and 2.67.

The analysis results show that the variation of the ratio does not significantly

influence the SWDR response. The 2% in 50 years shear wall responses for the three

ratios are observed to be 2.40%, 2.42%, and 2.43% respectively (Table 5.11). This

indicates that the demand uncertainty dominates and the strength correlation has little

effect on the system response and reliability. It can be partly attributed to the interaction

between shear walls and SMRF systems. The secondary SMRF system by providing

additional load-carrying capacity absorbs to some extent the shear wall resistance

uncertainty after the incipient collapse of the shear wall. This is in good agreement with

the results of the ideal parallel system examined in Chapter 2. A summary of response

statistics is shown in Table 5.11.

5.4 Two-Way Dual Systems

5.4.1 Five-Story, Two-Way Dual Systems

Five-story, two-way dual systems were constructed according to seismic codes to

evaluate their responses. The numbers and locations of shear walls were varied. The

configurations of one-, two-, and three-shear wall systems are given iii Chapter 4. The

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71

same material properties of shear walls in five-story, one-way dual systems were used,

which give, therefore, the same yield and ultimate strength of the shear walls. The

seismic hazard in terms of spectral acceleration was different for different systems as

shown in Table 5.3. The scatter of spectral acceleration of the SAC ground motion for the

three probability levels is shown in Figure 5.5. Structural responses for one-, two-, and

three-shear wall systems in each principal direction were calculated to determine their

system reliabilities. An approximately 6% response reduction in the X direction and a

2.4% response reduction in the Y direction under 2/50 earthquake levels were obtained

by replacing one with three shear walls (Table 5.12). Such response reductions in both

directions, under severe ground shaking, show the modest benefit of redundancy.

A comparison of the displacement trajectory between the one-way, one-shear wall

system and the two-way, one-shear wall system is illustrated in Figure 5.4 under LA21

and 22 excitations. The figure shows that the permanent displacement in the Y direction

of the two-way, one-shear wall system is larger than that of the one-way, one-shear wall

system. It is due to the failure of the shear wall in the Y direction in the two-way, one­

shear wall system. The reduction in MCDR response, from the one-shear wall to the

three-shear wall system, was 2.4% under 2/50 earthquakes (Table 5.12 and Figure 5.8

and5.11).

5.4.2 Ten-Story, Two Way Dual Systems

The redundancy of a long-period dual system was also investigated. It is evident

that total structural response of such a system is also dependent on the second or higher

modal responses. The responses of ten-story, two-way, one- and two-shear wall systems

were investigated. The fundamental structural periods of the one-shear wall system are

0.91 seconds in X direction, 0.90 seconds in Y direction, and 1.94 seconds in rotation.

The hysteretic model of shear wall and design of SMRF systems followed current code

(NEHRP-97), and an inelastic drift ratio limit was checked by a static analysis. The

ductility capacity of a shear wall was assumed to be 4.5. The fundamental structural

periods of the two-shear wall system are 0.81 seconds in X direction, 0.73 seconds in Y

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72

direction, and 0.94 seconds in rotation. The statistics of spectral acceleration

corresponding to the fundamental periods are given in Table 5.4. The same aspect ratio of

4 was used for modeling the two-shear wall system. The lateral capacity of the one-shear

wall system was the same as that of the two-shear wall system. Under 2/50 earthquakes in

the X direction, the shear wall drift ratio was 1.47% in the one-shear wall system and

1.42% in the two-shear wall system (Figure 5.12). Under 10/50 and 50/50 earthquakes,

there was also a small response reduction in the two-shear wall system when compared to

one-shear wall system. The biaxial MCDR responses of one- and two-shear wall systems

were all 2.4% under 2/50 earthquakes. The response statistics are summarized in Table

5.13 and the scatter of SWDR response is shown in Figure 5.9.

5.5 Steel Moment Frame Systems

5.5.1 Three-Story Moment Frame Systems with No Torsion

The response analyses of three-story ductile steel moment resisting frames under

SAC motions were performed. Two different configurations were considered for the

same floor area of 21600 ft2. A 4 x 4 bay SMRF system and a 6 x 6 bay SMRF system

were designed according to NEHRP and their responses were compared. The structural

drawings and member sizes are given in Chapter 4. The fundamental periods are 0.76 sec

in both X and Y directions and 0.44 sec in rotation. Basically, the median MCDR

responses of both systems under excitations at each probability level were almost the

same because the lateral strengths of the two systems were adjusted to be the same, i.e. a

larger size of beams and columns were used for system of smaller number of bays. For

instance, in the X direction, the MCDR responses of the 4 x 4 bay and 6 x 6 bay systems

against 2/50 levels were 2.6 and 2.7 % respectively (Figure 5.13). The response statistics

of the systems are given in Table 5.14. Also, the median and COY statistics of spectral

acceleration are shown in Table 5.5.

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73

5.5.2 Nine-Story Moment Frame Systems with No Torsion

Nine-story moment frame systems were also investigated as explained in Chapter 4.

Two different bay systems of 5 x 5 and 8 x 8 bays were designed according to NEHRP

and their structural responses were compared in Table 5.15. The median and COY

statistics of spectral acceleration are given in Table 5.6. The fundamental periods are 1.7

sec in both X and Y directions and 0.98 sec in rotation. The beam-column connection

behavior of these two systems was assumed to be perfectly ductile, i.e. no fracture failure.

In the X direction, maximum column drift ratios of the 5 x 5 bay and 8 x 8 bay systems

under 2/50 earthquakes were found to be 2.0 and 1.9 % respectively (Figure 5.14).

Therefore, there is practically no difference in responses between the two systems. The

redundancy implications will be discussed in Chapter 6.

5.5.3 Three-Story Moment Frame Systems with Torsion

Three moment frames with accidental torsion were considered. The structural

drawings and member sizes are given in Chapter 4. To model the irregularity of mass and

stiffness distribution of the diaphragm, a 5 % offset recommended by NEHRP was used in

this study. Mass center was assumed to deviate from stiffness center in both principal

directions. As stated in Chapter 4, two connection models, perfectly ductile and brittle,

were investigated. The brittle connection models included column fracture as well as top

or bottom flange fracture of the beam. The brittle connection fracture hysteresis model of

the system is also illustrated in Chapter 4 and included in the response analyses. To avoid

computational problems in nonlinear analyses of systems with a large number of bays, a

relatively small number of bays, 1 xl, 2 x 2, and 3 x 3 bays, were chosen. For all

systems, the seismic hazard of spectral acceleration was assumed to be the same (Table

5.7).

The MCDR responses of all systems with ductile connections are given in Table

5.16 (Figure 5.15). The median drift response of 1 x 1 bay SMRF under 2/50 earthquakes

was 6.63% and that of 3 x 3 bay SMRF was 5.14%. Thus, 22.5% response reduction was

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observed in the systems with ductile connections. The MCDR responses of all three

systems with brittle connections are also tabulated in Table 5.17 (Figure 5.16). The

median response of the systems with brittle fracture connections was higher than that of

the systems with ductile connections. However, the median response reduction from the 1

x 1 bay system to the 3 x 3 bay system at 2/50 hazard level was only 10.4%. It can be,

therefore, concluded that, when torsional motions are included into the consideration, the

response is clearly reduced by using larger number of bays and smaller member sizes if

the components are ductile.

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Table 5.1 Four Case Studies of 5-Story, One-Way Dual Systems.

Effect of Effect of the Effect of Effect of

5-Story, One-Way Correlation Ratio ofEQ Number of Ductility of

Dual Systems of Shear to Strength Shear Walls Shear Walls

Walls Variability

1 ./

Number of 2 ./ X

Shear Walls

3 ./ X X

5.4 ./

Ductility of 6.4 X ./ X X

Shear Walls

7.4 ./

0.0 X X ./ X

Correlation 0.2 ./

of Shear 0.6 ./

Walls

1.0 ./

Ratio of EQ 267 X X X ./

to Strength ) ~6 ./

VariabilItv ~ ., .. . J _'" ./

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Table 5.2 Medians and Coefficient of Variation of Spectral Acceleration.

(5-Story, One-Way Dual Systems)

5-Story 50/50 10/50

One-Way Median Median

Dual COY COV

Systems (g) (g)

X 0.685 0.621 1.073 0.301 One-

Shear y

Wall Bi 0.797 0.559 1.286 0.284

X 0.701 0.614 1.077 0.307 Two-

Shear y

Wall Bi 0.815 0.549 1.293 0.295

X 0.710 0.646 1.212 0.270 Three-

Shear Y

Wall Bi 0.835 0.541 1.379 0.292

x = Spectral Acceleration at Fundamental Period in the X direction

Y = Spectral Acceleration at Fundamental Period in the Y direction

Bi = Biaxial Spectral Acceleration

2/50

Median COV

(g)

2.064 0.425

2.419 0.414

2.097 0.436

2.412 0.430

2.152 0.310

2.442 0.377

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Table 5.3 Medians and Coefficient of Variation of Spectral Acceleration.

(5-Story, Two-Way Dual Systems)

5-Story 50/50 10/50

Two-Way Median Median

Dual COY COY

Systems (g) (g)

X 0.792 0.755 1.211 0.311 One-

Shear y 0.703 0.501 1.321 0.407

Wall Bi 0.978 0.642 1.537 0.334

X 0.794 0.701 1.195 0.341 Two-

Shear y 0.708 0.451 1.300 0.404

Wall Bi 0.955 0.589 1.620 0.327

X 0.794 0.701 1.195 0.341 Three-

Shear Y 0.703 0.501 1.321 0.407

Wall Bi 0.974 0.589 1.589 0.340

X = Spectral Acceleration at Fundamental Period in the X direction

Y = Spectral Acceleration at Fundamental Period in the Y direction

Bi = Biaxial Spectral Acceleration

2/50

Median COY

(g)

2.208 0.597

2.025 0.615

2.639 0.579

2.317 0.553

2.023 0.574

2.657 0.510

2.317 0.553

2.025 0.615

2.659 0.547

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Table 5.4 Medians and Coefficient of Variation of Spectral Acceleration.

(lO-Story, Two-Way Dual Systems)

10-Story 50/50 10/50

Two-Way Median Median

Dual COY COY

Systems (g) (g)

X 0.630 0.582 0.950 0.209 One-

Shear y 0.532 0.420 1.056 0.234

Wall Bi 0.770 0.498 1.227 0.226

X 0.650 0.728 1.136 0.281 Two-

Shear y 0.555 0.453 1.235 0.307

Wall Bi 0.772 0.653 1.481 0.263

X = Spectral Accckrarion at Fundamental Period in the X direction

Y = Spectral AcceleratIOn at Fundamental Period in the Y direction

Bi = Biaxial Spectr ~1 Acceleration

2/50

Median

(g)

1.913

1.749

2.231

2.155

1.969

2.523

COY

0.384

0.374

0.394

0.385

0.556

0.423

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Table 5.5 Medians and Coefficient of Variation of Spectral Acceleration.

(3-Story SMRF Systems with No Torsion)

3-Story 50/50 10/50

SMRF Median Median COY COY

Systems (g) (g)

X 0.655 0.834 1.083 0.270

4x4 Y 0.540 0.510 1.222 0.256

Bay

Bi 0.780 0.750 1.421 0.232

X 0.655 0.834 1.083 0.270

6x6 y 0.540 0.510 1.222 0.256

Bay

Bi 0.800 0.750 1.421 0.232

X = Spectral Acceleration at Fundamental Period in the X direction

Y = Spectral Acceleration at Fundamental Period in the Y direction

Bi = Biaxial Spectral Acceleration

2/50

Median

(g)

2.132

2.070

2.603

2.132

2.070

2.603

COY

0.352

0.562

0.444

0.352

0.562

0.444

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80

Table 5.6 Medians and Coefficient of Variation of Spectral Acceleration.

(9-Story SMRF Systems with No Torsion)

9-Story 50/50 10/50

SMRF Median Median

Systems COY COY

(g) (g)

X 0.264 0.552 0.568 0.529

5x5 Y 0.205 0.529 0.557 0.493

Bay

Bi 0.317 0.505 0.798 0.331

X 0.264 0.552 0.568 0.529

8x8 y 0.205 0.529 0.557 0.493

Bay

Bi 0.317 0.505 0.798 0.331

X = Spectral Acceleration at Fundamental Period in the X direction

Y = Spectral Acceleration at Fundamental Period in the Y direction

Bi = Biaxial Spectral Acceleration

2/50

Median

(g)

1.287

1.461

1.810

1.287

1.461

1.810

COY

0.586

0.447

0.437

0.586

0.447

0.437

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81

Table 5.7 Medians and Coefficient ofYariation of Spectral Acceleration.

(3-Story SMRF Systems with Torsion)

3-Story 50/50 10/50 2/50

SMRF Median Median Median

Systems COY COY

(g) (g) (g)

1 x 1 Bi 0.778 0.534 1.376 0.221 2.495

Bay

2x2 Bi 0.778 0.534 1.376 0.221 2.495

Bay

3x3 Bi 0.778 0.534 1.376 0.221 2.495

Bay

Bi = Biaxial Spectral Acceleration

COY

0.408

0.408

0.408

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82

Table 5.8 Medians and Coefficient of Variation of Response Variables.

(5-Story, One-Way Dual Systems of Different Number of Shear Walls)

50/50 10/50 2/50 Number of Shear

Median Median Median Walls COY COY

(%) (%) (%)

XSWDR 0.577 0.576 1.441 0.416 2.522 One-

Shear YSWDR

Wall MCDR 0.903 0.399 1.981 0.343 3.811

XSWDR 0.580 0.590 1.419 0.389 2.499 Two-

Shear YSWDR

Wall MCDR 0.905 0.400 1.963 0.337 3.785

XSWDR 0.563 0.593 1.381 0.375 2.428 Three-

Shear YSWDR

Wall MCDR 0.901 0.390 1.924 0.317 3.704

COY

0.502

,

0.426

0.495

0.422

0.489

0.436

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83

Table 5.9 Medians and Coefficient of Variation of Response Variables.

(5-Story, One-Way Dual Systems of Different Shear Wall Ductility Capacity)

50/50 10/50 2/50 Ductility of Shear

Median Median Median Walls COV COV COV

(%) (%) (0/0 )

XSWDR 0.565 0.593 1.385 0.375 2.442 0.498

5.4 YSWDR

MCDR 0.901 0.390 1.924 0.318 3.710 0.439

XSWDR 0.563 0.593 1.381 0.375 2.428 0.489

6.4 YSWDR

MCDR 0.901 0.390 1.924 0.317 3.704 0.436

XSWDR 0.590 0.578 1.412 0.374 2.447 0.500

7.4 YSWDR

MCDR 0.908 0.406 1.959 0.304 3.721 0.439

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I

84

Table 5.10 Medians and Coefficient of Variation of Response Variables.

(5-Story, One-Way Dual Systems with Different Correlation of Shear Wall Strength)

50/50 10/50 2/50 Correlation of

Median Median Median Shear Walls COY COY COY

(%) (0/0) (%)

XSWDR 0.580 0.590 1.419 0.389 2.499 0.495

0.0 YSWDR

MCDR 0.905 0.400 1.963 0.337 3.785 0.422

XSWDR 0.578 0.590 1.418 0.394 2.495 0.499

0.2 YSWDR

MCDR 0.905 0.400 1.964 0.342 3.793 0.419

XSWDR 0.576 0.590 1.401 0.397 2.507 0.501

0.6 YSWDR

MCDR 0.906 0.397 1.949 0.341 3.791 0.424

XSWDR 0.566 0.594 1.407 0.403 2.517 0.493

1.0 YSWDR

MCDR 0.908 0.396 1.962 0.342 3.775 0.427

...

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85

Table 5.11 Medians and Coefficient of Variation of Response Variables.

(5-Story, One-Way Dual Systems and Different Ratios ofEQ to Strength Variability)

Ratio of EQ to 50/50 10/50 2/50

Strength Median Median Median

Variability COY COY COY

(%) (%) (0/0 )

XSWDR 0.565 0.616 1.361 0.404 2.427 0.497

2.67 YSWDR

MCDR 0.899 0.398 1.898 0.337 3.696 0.441

XSWDR 0.561 0.600 1.353 0.389 2.423 0.498

3.55 YSWDR

MCDR 0.898 0.393 1.902 0.323 3.698 0.436

XSWDR 0.563 0.593 1.381 0.375 2.428 0.489

5.33 YSWDR

MCDR 0.901 0.390 1.924 0.317 3.704 0.436

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86

Table 5.12 Medians and Coefficient of Variation of Response Variables.

(5-Story, Two-Way Dual Systems)

5-Story Two- 50/50 10/50 2/50

Way Dual Median Median Median

Systems COY COY

(%) (%) (%)

XSWDR 0.555 0.592 1.397 0.422 2.578 One-

Shear YSWDR 0.425 0.557 1.100 0.557 2.610

Wall MCDR 0.747 0.460 1.922 0.386 3.857

XSWDR 0.555 0.589 1.384 0.402 2.452 Two-

Shear YSWDR 0.395 0.572 1.065 0.550 2.610

Wall MCDR 0.751 0.438 1.907 0.368 3.829

XSWDR 0.545 0.608 1.356 0.383 2.425 Three-

Shear YSWDR 0.391 0.568 1.057 0.567 2.554

Wall MCDR 0.760 0.432 1.872 0.369 3.766

COY

0.460

0.579

0.433

0.479

0.564

0.392

0.478

0.586

0.420

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87

Table 5.13 Medians and Coefficient of Variation of Response Variables.

(lO-Story, Two-Way Dual Systems)

10-Story Two- 50/50 10/50 2/50

Way Dual Median Median Median

Systems COY COY

(%) (%) (%)

XSWDR 0.346 0.380 0.769 0.347 1.470 One-

Shear YSWDR 0.244 0.432 0.674 0.394 1.936

Wall MCDR 0.402 0.353 0.999 0.210 2.431

X SWDR 0.324 0.468 0.753 0.344 1.415 Two-

Shear Y S\VDR 0.231 0.450 0.647 0.433 1.997

Wall ~1CDR 0.377 0.420 0.968 0.214 2.446

COY

0.465

0.323

0.328

0.453

0.336

0.322

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88

Table 5.14 Medians and Coefficient of Variation of Response Variables.

(3-Story SMRF Systems with No Torsion)

50/50 10/50 2/50 3-Story SMRF

Median Median Median Systems COY COY

(%) (%) (%)

X CDR 0.769 0.518 1.475 0.299 2.588

4x4 YCDR 0.673 0.491 1.326 0.423 2.996

Bay

MCDR 0.870 0.480 1.756 0.381 3.489

X CDR 0.781 0.563 1.493 0.323 2.715

6x6 YCDR 0.656 0.500 1.348 0.447 3.136

Bay

MCDR 0.872 0.522 1.814 0.402 3.661

COY

0.415

0.373

0.430

0.431

0.391

0.452

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89

Table 5.15 Medians and Coefficient of Variation of Response Variables.

(9-Story SMRF Systems with No Torsion)

50/50 10/50 2/50 9-Story SMRF

Median Median Median Systems COY COY

(%) (%) (%)

X CDR 0.493 0.419 1.181 0.340 2.014

5x5 YCDR 0.413 0.366 0.970 0.336 2.838

Bay

MCDR 0.591 0.339 1.405 0.210 3.327

X CDR 0.452 0.439 1.091 0.331 1.941

8x8 YCDR 0.387 0.352 0.903 0.322 2.763

Bay

MCDR 0.548 0.355 1.282 0.196 3.255

COY

0.417

0.310

0.329

0.429

0.294

0.301

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90

Table 5.16 Medians and Coefficient of Variation of Response Variables.

(3-Story SMRF Systems with Ductile Connections and Torsion)

50/50 10/50 2/50 3-Story SMRF

Median Median Median Systems COY COY

(%) (%) (%)

1 x 1 MCDR 1.446 0.431 2.908 0.431 6.629

Bay

2x2 MCDR 1.485 0.398 2.808 0.398 5.881

Bay

3x3 MCDR 1.374 0.398 2.499 0.397 5.143

Bay

COY

0.501

0.486

0.466

Table 5.17 Medians and Coefficient of Variation of Response Variables.

(3-Story S~tRF Systems with Brittle Connections including Column Damage and

Torsion)

50/50 10/50 2/50 3-Story S~tRF

\1cdlan Median Median System~ COY COY COY

('t ) (%) (0/0 )

1 x 1 ~1CDR 1478 0.429 2.913 0.429 6.848 0.553

Bay

2x2 MCDR l.~ 13 0.410 2.832 0.383 6.604 0.547

Bay

3x3 MCDR 1.360 0.391 2.604 0.406 6.141 0.617

Bay

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§ 1.5

c 0 0.5 ~ ~

(])

-0.5 (j) (,) (,)

<{ -1.5

§ 1.5 c 0 0.5 ~ ~

(]) -0.5 (j)

(,) (,) <{ -1.5

0

0 2

2

4 6

91

8 1 0 12 14 1 6 1 8 20

Time (sec)

(a) Fault Normal (LA21)

4 6 8 1 0 1 2 14 1 6 18 20

Time (sec)

(b) Fault Parallel (LA22)

Figure 5.1 A Pair of SAC-2 Earthquake Ground Motions (LA21 and LA22).

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_ -0.0015 -0 (1j

..=.. -0.0005 c o

15 0.000 (5

3

3

5 7

5 7

92

9 11 13

(a) X-Direction

9 11 13

(b) Y-Direction

15 17 19 21 Time (sec)

15 17 19 21 Time (sec)

~ O.001~~--~----~--~~~~~----~--~~~--~----~---3 5 7 9 11 13 15 17 19 21 Time (sec)

(c) Z Rotation

Figure 5.2 Displacement of Top Mass Center of 5-Story, One-Way Dual Systems.

(One-Shear Wall System)

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93

-25 -15 -5 5 15 25 2o.-----~------~----~--~--~--~~20

10 10

C =-Q..

0 0 en (5

r

-10 -10

-20 '---~ __ ___'_ __ ~ __ ....l....._ ______ ____' ____ __'__ __ ____' -20

-25 -15 -5 5 15 25

X Disp (in)

(a) One-Shear Wall System

-25 -15 -5 5 15 25 20.----~----~---~------~----~20

10 10

C

~ =-Q.. 1/) r. 0 (5

v

r

-10 -10

-20 L.-__ ___'__~_....I.-__ __.....J'___~ _ __1.... __ ~__' -20 -25 -15 -5 5 15 25

X Disp (in)

(b) Two-Shear Wall System

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94

-25 -15 -5 5 15 25 20~~--~------~----~--~--~----~20

10 10

C ~

0-(j) 0 0 (5

>-

-10 -10

-20 L..-----'-_--.L.-_______ .l..----'-_--l-_______ .l..-______ --I -20

-25 -15 -5 5 15 25

X Disp (in)

(c) Three-Shear Wall System

Figure 5.3 Displacement Trajectory of Top Mass Center under LA21 and LA22.

(S-Story, One-Way Dual Systems with 5% Accidental Torsion)

-25 -15 -5 5 15 25 20~~--~~--~~--~i--~~I--~~j20

10 10

C

0- 0 0 CJ)

0 >-

-10 -10

-20~~--~~--~~--~~--~~~-20

-25 -15 -5 5 15 25 X Disp (in)

(a) S-Story, One-Way, One-Shear Wall System

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95

-25 -15 -5 5 15 25 20~~~--~~--~~~--~~~20

10 10

..-c - 0 0 0.. CJ)

£5 >- -10 -10

-20~--~--~~--~~~--~~~-20

-25 -15 -5 5 15 25

X Disp (in)

(b) 5-Story, Two-Way, One-Shear Wall System

Figure 5.4 Displacement Trajectory of Top Mass Center under LA21 and LA22.

(No Accidental Torsion)

1 ao.oog 6

~ •••• •• (J)

Co 3 CD >. 2

0 L.{)

10-1 .°°8 • ..... • ---CD 7 0

~ c ro "0 3 CD CD 2 • .. • w •• 0 x w 10-2 .°°8 '0 7 D ~ 0

0::: 3 2

10-3 .000

a 2 3 4 5 6 7

Uniaxial Sa (g)

(a) X Directional Uniaxial Spectral Acceleration

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~ Cd Cll >-0 l.()

---Cll u c Cd "0 Cll Cll u x w '0 .0 e

D...

~ Ctl Cll >-0 If)

--Cll u c Ctl

~ OJ u )(

w a .D e D...

96

100.00g 6

~ - .. 3 2

10-1.002 ..... -_ ... 7

~ 3 2

10-2.002 7

~ 3 2

10-3 .000

0 2 3 4 5 6

Uniaxial Sa (g)

(b) Y Directional Uniaxial Spectral Acceleration

10000~ I ~ ...... • 3 2

10-1 .002 ........... 7

~ 3 2 ..... ... • •

10.2 .002 7

~ 3 2

,0.3000

0 2 3 4 5 6 7 8

Biaxial Sa (g)

(c) Biaxial Spectral Acceleration

Figure 5.5 Scatter of Spectral Acceleration.

7

9

(5-Story, Two-Way Dual Systems of One Shear Wall: T1=0.61, T2=0.56, s= 0.02)

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97

- ..

234 5 Drift Ratio (%)

(a) One-Shear Wall System

3 4 5 Drift Ratio (%)

(b) Two-Shear Wall System

- ..

2

" T T

345 Drift Ratio (%)

(c) Three-Shear Wall System

6 7 8

6 7 8

6 7 8

Figure 5.6 Scatter of SWDR (5-Story, One-Way Dual Systems).

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Ul 100.roJ

ffi 5 >- 3

5S 2

10'1.roJ Q) 5 () 3 c -8 2

~ 10-2.roJ () 5 >< W 3

a 2

.g 10-3.roJ

c:

~ 10QroJ co

Q)

>- 5 0 3 L{)

2 Q) 10,1.0c0 () c 5 co

"t:l 3 Q) 2 Q) () 10-2.0c0 >< W

5 a 3 .ci 2 0 10-3.0c0 c:

Ul 10o.roJ Co 5 Q)

>- 3 0 2 L{) lO,1.roJ Q) 5 () c 3 co 2 "t:l Q) lO'2.roJ <l.J ()

5 >< W 3 a 2

.ci lO-3.roJ

2 CL

0

0

0

98

_ ..

2 3 4 5 678 Maximum Column Drift Ratio (%)

(a) One-Shear Wall System

_ ..

2 345 678 Maximum Column Drift Ratio (%)

(b) Two-Shear Wall System

_ .. .M .....

2 3 4 5 678 Maximum Column Drift Ratio (%)

(d) Three-Shear Wall System

Figure 5.7 Scatter of MCDR.

(5-Story, One-Way Dual Systems)

9 10

9 10

9 10

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99

(/) 4 - .. l 2 ~ 1O·1.(XX)

--. 4

i 1O-~~ Jj 4

'0 2 .g 10-3. (XX)

c: 0 234 5 Drift Ratio (%)

6 7 8

(a) X Directional SWDR (One-Shear Wall)

234 5 6 7 8 Drift Ratio (%)

(b) Y Directional SWDR (One-Shear Wall)

,~ :IT

4 - .. ",

~. .. ~

1::;'U .~~ A.

- 4 C.

~ ..., ~ W ~ ~ ).

~ 1::; .::0: i 'It u.

'" ~ 1a 3 :XX: -8 0 2 3 4 5 6 7 8 ct Drift Ratio (%)

(c) X Directional SWDR (Two-Shear Wall)

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rJ)

~ [is -... Q.l

j Jj 15 .g a:

100

• ........ A

2 345 6 7 Drift Ratio (%)

(d) Y Directional SWDR (Two-Shear Wall)

1dH )oo

4 - •• 2

1O-1.ClOO .......... A

4

2 ~ ,..,.. ~ W .... lO-2.ClOO

4 2

1o-3.ClOO

0 2 3 4 5 6 7 Drift Ratio (%)

(e) X Directional SWDR (Three-Shear Wall)

2

•••••

345 Drift Ratio (%)

6 7

(f) Y Directional SWDR (Three-Shear Wall)

8

8

8

Figure 5.8 Scatter of SWDR (5-Story, Two-Way Dual Systems).

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101

10°·000 CJ) 4 -l 2

SS 10-1.000 ~ - 4 CD

j 2 WW"" ~~ 10-2.000

J1 4

'0 2

-8 10-3.000

0: 0 2 3 4 5 6 7 8 Drift Ratio (%)

(a) X Directional SWDR (One-Shear Wall)

2 3 4 5 6 7 8 Drift Ratio (%)

(b) Y Directional S\VDR (One-Shear VI all)

1rPooo

4 --CJ)

l 2 SS 10-1.000 .......... -- 4

CD

i 2 WW~W~ ~ 10-2.000

J1 4

2 (5

10-3.000 -8 0 2 3 4 5 6 7 8 a:: Drift Ratio (%)

(c) X Directional SWDR (Two-Shear Wall)

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102

10'1000

4 .. CfJ >- 2

~ 10-1.000 ........ ~ - 4 Q) WW W ~

i 2

10-2.000

J5 4

2 '0 10-3.000 .g 0 2 3 4 5 6 7 8 0: Drift Ratio (%)

(d) Y Directional SWDR (Two-Shear Wall)

Figure 5.9 Scatter of SWDR (lO-Story, Two-Way Dual Systems).

~ ::r ~ I o t 1/") ,

04 r (tJ

~ ~ 03

i t v If

u;

c C 2'

\\.\\\ .....

\:.:-, \:\

\\

--- One-Shear Wall •. .J> .•..• Two-Shear Wall ---.. -- Three-Shear Wall

c C '--_____ ---1... ___ '--__ ....l.-__ ~ __ ___'

o 2 3

Drift Ratio (%) -------------------------------'

(a) Number of Shear Walls

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103

0.6

CJ)

co (l)

0.5 ~ Ductility 5.4 >. ._ . ."._ .. Ductility 6.4 0 ---.-- Ductility 7.4 LO

0.4 (l) u c co -0 (l)

0.3 (l) u x

W 0.2 '0 .0 2 0.1

0....

0.0 0 2 3

Drift Ratio (%)

(b) Ductility of Shear Wails

0.6

CJ) ~ Correlation Factor 0.0 co 0.5

\ Correlation Factor 0.2 (l) ._ . ."._ .. >.

Correlation Factor 0.6 0 ---.--LO .-... + ..... Correlation Factor 1.0 - 0.4 (l)

\ u c co -0 0.3 (l)

\ (l) u x W 0.2

~ '0 .0 0

0.1 0::

----------0.0 0 1 2 3

Drift Ratio (%)

(c) Correlation of Shear Wall Strength

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0.6

CIl

Co 0.5 Q) >.

0 L{)

0.4 Q) CJ C ctl

-.:l 0.3 Q) Q) CJ X ill 0.2 '0 .0 e 0.1 a..

0.0 0

104

----- Ratio 2.67 Ratio 3.55

---.-- Ratio 5.33

---------2

Drift Ratio (%)

(d) Ratio of EQ to Strength Variability

3

Figure 5.10 50-Year Probability of Exceedance of Median SWDR.

(5-Story, One-Way Dual Systems)

0.6

CIl

ro 0.5 \ Q) >.

----- One-Shear Wall -0&.-. Two-Shear Wall

0 ---.... Three-Shear Wall L{)

0.4 Q) CJ C ctl

-.:l 0.3 Q) Q) CJ X ill 0.2 '0 .0 2 0.1 a..

0.0 0 2 3

Drift Ratio (%)

(a) 5-Story, Two-Way Dual Systems eX Direction)

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0.6

en --- One-Shear Wall co 0.5

Q) Two-Shear Wall >-0 _ .... -- Three-Shear Wall L!)

0.4 Q) u c co "0 0.3 Q) Q) u x W 0.2 '0 -Ci 0

0.1 ct

---------------0.0 0 2 3

Drift Ratio (%)

(b) 5-Story, Two-Way Dual Systems (Y Direction)

Figure 5 .11 50-Year Probability of Exceedance of Median SWDR.

0.6

(J') --- One-Shear Wall Co 0.5 Q) ..... ..,(~ ... Two-Shear Wall >-

0 L!)

0.4 Q)

\ U c: co "0 0.3 Q)

'. Q) U \

X \

W 0.2 '0 .D 0

0' a:: ~

0.0 0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0

Drift Ratio (%)

(a) 10-Story, Two-Way Dual Systems (X Direction)

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0.6

C/)

03 0.5 (j) >. 0 L!)

0.4 (j) u c co

-0 0.3 (j) (j) u x ill 0.2 0 ..0 0

0.1 c::

0.0 0.0 0.5

106

1.0 1.5

Drift Ratio (%)

-- One-Shear Wall -4-.. Two-Shear Wall

2.0 2.5

(b) 10-Story, Two-Way Dual Systems (Y Direction)

Figure 5.12 50-Year Probability of Exceedance of Median SWDR.

0.6

~ co 0.5 (j)

>-0 L!)

0.4 (j) u c co -0 0.3 (j) (j) u x W 0.2 '0 ..0 e 0.1 a..

0.0 0

4 X4 Bay ...... - ........ _- 6X6Bay

1 2

Story Drift Ratio (%) 3

Figure 5 .13 50-Year Probability of Exceedance of Median Story Drift Ratio (X

Direction).

(3-Story SMRF Systems with No Torsion)

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~ co OJ >-0 I.!)

OJ () C co

"C OJ OJ () X w '0 .ci e a..

0.6

0.5

0.4

0.3

0.2

0.1

0.0 0

107

5 X5 Bay ------ 8 X 8 Bay

123

Story Drift Ratio (%)

Figure 5.1450-Year Probability of Exceedance of Median Story Drift Ratio (X

Direction) .

0.6

(/)

Co 0.5 OJ >-

0 I.!)

0.4 OJ ()

C co

"C 0.3 OJ OJ () X

W 0.2 '0 .n e 0.1 a..

0.0 0

(9-Story SMRF Systems with No Torsion)

Ductile Connection

~ ...

1 X 1 Bay ._._._-+_. __ .- 2 X 2 Bay .......•...... 3 X3 Bay

fv1aximum Column Drift Ratio (%)

Figure 5.15 50-Year Probability of Exceedance of Median MCDR.

C3-Story SMRF Systems with Ductile Connections and Torsion)

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0.6

(f)

Co 0.5 OJ >. o L.() ___ 0.4

OJ () C ct! "0 0.3 OJ OJ () X ill 0.2

'0 .!i o ct 0.1

108

Brittle Connection

• 1 X 1 Bay ._._.-.-+-._._.- 2 X 2 Bay

-------.------ 3 X 3 Bay

0.0 L-~-I-_ ___'__'__...l..-~_'_~____J'___~_'__ _ ___'_~___'

o

Maximum Column Drift Ratio (%)

Figure 5_16 50-Year Probability of Exceedance of Median MCDR.

(3-Story SMRF Systems with Brittle Connections including Column Damage and

Torsion)

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109

CHAPTER 6

RELIABILITY AND REDUNDANCY EVALUATION

6.1 Introduction

The redundancy of a structure primarily arises from the capacity to provide an

alternative load-carrying path after the collapse of the first primary load resisting system.

Some factors affecting redundancy were identified under static (Gollwitzer and Rackwitz,

1990) and stochastic (Wen, Wang and Song, 1998) loads. These factors included the

number of load resisting components, ductility capacity of the components, correlation

between member strengths, configuration of structural system, and the variability of the

demand versus that of the capacity. Since 1994 Northridge earthquake, the effect of

beam-column connection capacity in structural reliability and redundancy has been

investigated by Wang and Wen (1998) and Yun and Foutch (1998).

Quantification of structural redundancy is generally difficult, especially for

complex structures, due to the difficulty in describing the nonlinear member and system

response behavior and hence in evaluating the probability of local (member) and global

(system) limit states including collapse. Cornell (1989) and Frangopol (1994) have

proposed redundancy factors based on first member failure and system collapse

probabilities for simple parallel systems. Since SMRF or dual systems considered herein

are more complex and earthquake excitation is stochastic and dynamic in nature, the

quantification of the redundancy factor for such systems is even more challenging.

6.2 Background

The classical definition of redundancy has been the degree of indeterminacy. In

view of the large uncertainty in both capacity and demand, however, the definition,

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should be stated within a probabilistic framework. Redundancy of simple systems under

random static loads has been extensively studied in the past. Gollwitzer and Rackwitz

(1990) studied a parallel balanced system and identified several important factors

affecting the system redundancy. Hendawi and Frangopol (1994) investigated the four­

member parallel balanced system using a failure path approach. Grigoriu (1990, 1992)

carried out an analytical investigation redundancy of a parallel balanced system subject to

Gaussian load processes. For systems of some complexity such as a real structure,

simulation-based method, however, is generally preferred due the inherent analytical

difficulty (Wen and Chen, 1987; De, Karamchandani and Cornell, 1989).

Moses (1974) examined the effect of redundant wind framing systems. The degree

of indeterminacy of the structure was suggested to be a parameter to evaluate the degree

of redundancy of the structure, e.g. a weakest-link system (series system or statically

determinant structure) versus a parallel system (statically indeterminant structure). More

recently in ATC-19 (1995), it was suggested that the reliability of the framing system

against seismic load depends on the number of lateral load resistant components. Bertero,

et al. (1998), emphasized that the redundancy depends on structural over-strength and

plastic hinge capacity.

De and Cornell (1989), defined a redundancy factor as the conditional probability

of total system failure, given that at least one member has failed.

R _ _ P_( c_o_ll_a_p_se_) F - P(AFF)

0::; RF ::; 1, AFF: Any First member Failure

(6.1)

After any first-member failure, the load is redistributed according to the structural

configuration and the damaged structural system continues to carry the total load.

Hendawi and Frangopol (1994) introduced a probabilistic redundancy factor that was

defined as the difference in probabilities between any-first-member yielding and collapse

of the system normalized by the probability of collapse.

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P(yield) - P( collapse) R = ---------

F P( collapse) (6.2)

To define redundancy in earthquake resistant design, Bertero, et aI. (1998),

suggested the following: 1) If a pseudo static approach is used to analyze the structure,

the redundancy degree, n, of a structural system is the number of critical regions (plastic

hinges) of the structural system that must yield or fail to produce the impending collapse

of the structure under the action of monotonically increasing lateral deformations; and 2)

If a dynamic approach is used, the redundancy degree, n, of a structural system is the

number of critical regions or plastic hinges of the structural system that dissipate a

significant amount of plastic hysteretic energy before the structure collapse under the

earthquake ground motions.

In ATC-19 (1995) and ATC-34 (1995), it was proposed that a response

modification factor (R) can be divided into three factors: a period-dependent strength

factor (Rs), a period-dependent ductility factor (R)l), and a redundancy factor (RR).

(6.3)

Bertero, et aI. (1998), however, pointed out that the third component of the reduction

factor R, redundancy factor RR, can not be established independently of the over-strength

and ductility capacity of the structural system. The ductility can be simply explained as

an energy absorption capacity in plastic rotation. The over-strength can be defined as the

ratio of the mean resistance to demand (Bertero, et aI., 1998), which results mainly from

the strain hardening and the bias of the nominal yield stress compared to the actual yield

stress (Foutch, 1998) of the members. These three factors are interrelated and cannot be

easily separated. In view of this, Wang and Wen (1998) introduced a redundancy factor

based on uniform hazard spectra and reliability consideration. The uniform-risk

redundancy factor can be defined as the ratio of spectral acceleration causing incipient

collapse to the spectral acceleration corresponding to an allowable probability of

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incipient collapse. The redundancy factor is unity if the incipient collapse probability is

less than the allowable value.

h P < pall W en ip - ip

whenP > pall Ip Ip

~p = Probability of incipient collapse.

~I = Allowable probability of incipient collapse.

S: = Spectral acceleration corresponding to ~p.

S~I = Spectral acceleration corresponding to 1f!I.

S:es = Spectral accel. corresponding to design prob. level.

R = Response modification factor

R' = Revised response modification factor = R· RR

(6.4)

(6.5)

Then, the RR factor is applied to R (Response Modification Factor). The uniform-risk

redundancy factor, therefore, aims at achieving the same reliability for building systems

with different redundancies.

6.3 Redundancy Factor in Recent Codes and Standards

Bertero and Whittaker, et al. (1990), proposed that, as the minimum for adequate

redundancy, four lines of strength- and deformation-compatible vertical seismic framing

structures be included in each principal direction of a building. Their concept for

structural design for redundancy, in the form of a redundancy factor, requires a higher

seismic design force for less redundant structures. It is therefore a penalty factor.

Recently, UBC (lCBO, 1997), NEHRP (BSSC, 1997), and lBC 2000 (1998),

adopted a reliability/redundancy factor, p, which is a multiplier of design lateral

earthquake force defined as follows:

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in US customary,

or

p=2 6.1

in SI units,

1~p~1.5

P = Reliability / Redundancy Factor

rmax = Maximum element - story shear ratio

As = Ground floor area of the structure, fe (m2)

E = Earthquake load on an element of the structure

Eh = Earthquake load due to the base shear, V

E, = Load effect resulting from the vertical

component of the earthquake ground motion

(6.6)

The p factor is, therefore, a function of the system configuration and number of

seismic components. There has been some dissatisfaction with this factor. For example,

Whittaker, et al. ( 1999), were highly critical of the factor being based on the floor area

and component forces to describe the reliability and redundancy of the framing system.

It is pomted out that many important factors affecting redundancy have not been

considered in the p factor, such as ductility capacity and uncertainty in demand versus

capacity. bi-axlal mteraction and torsion, etc. Therefore, further research is needed on

redundancy factor that enables structural engineers to consider the effects of all the

important contnhuttnt; factors and quantity the redundancy in both evaluation and design.

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6.4 Seismic Hazard Analysis

6.4.1 Uniaxial Spectral Acceleration

Spectral acceleration at the fundamental structural vibration period is often used to

represent the seismic hazard to the structure. Examples of elastic response spectrum in

the fonn of spectral acceleration and spectral displacement are shown in Figure 6.1 and

6.2 respectively. The elastic spectral acceleration has been proposed by researchers (e.g.

Shome and Cornell, 1998) as a measure of ground shaking in predicting nonlinear

response of structure. However, when the first modal response does not dominate the

total response, the use of spectral accelerations at periods of second and higher modes in

addition to the fundamental mode is encouraged (Shome and Cornell, 1999), e.g. when

the shape of a structure is highly irregular such that torsional motion becomes important.

Assuming that the out-of-plane capacity of a shear wall in a dual system is

negligible, the in-plane capacity in each principal direction is of primary concern. The

seismic hazard in each principal direction for a given shear wall system can be assessed

by using uniaxial spectral acceleration at the fundamental period of the principal

direction. A uniaxial spectral acceleration exceedance probability for a specific damping

ratio and over a given time period can be used as the seismic hazard. Median values of

spectral acceleration of SAC-2 ground motions were selected to match USGS target

hazard levels at given probability levels (50%, 10%, and 2% in 50 years). Assuming the

scatter of uniaxial spectral accelerations of the SAC motions at a given probability level

follows a log-normal distribution, the median value is then the geometric mean, which is

given by

Sa.m = exp[;; t1n(Sa.;)] (6.7)

where Sa,i is the spectral acceleration of the i-th ground motion, Sa m is the median

estimate, and n is the sample size.

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Assuming again that median spectral acceleration over a given period follows a

log-nonnal distribution, the exceedance probability in 50 years is then given by

InS -A H (S) = 1- <1>( a,m ) ~ a ,

(6.8)

where A and , are log-normal distribution parameters determined by least squares

fitting of the median spectral accelerations at the three probability levels. (<1> is the

standard normal distribution function.) As an example, the seismic hazard in terms of the

spectral acceleration for la-story, two way dual systems is shown in Figure 6.4.

6.4.2 Biaxial Spectral Acceleration

F or biaxial excitations, the maximum of the vector sum of the spectral accelerations

at fundamental periods in the two principal directions can be used as a measure of

seismic hazard. Since structural members of a structure, i.e. columns in S:MRF, are

designed to resist loading in both directions at the same time, biaxial spectral acceleration

is a better measure of seismic hazard. Biaxial elastic response spectrum can be

constructed from the time history response analysis of a simple oscillator under biaxial

excitations. Examples of the biaxial elastic response spectrum are shown in Figure 6.3 (a)

(spectral acceleration) and Figure 6.3 (b) (spectral displacement). The biaxial elastic

response spectrum was based on 900 combinations of structural periods in the two

principal directions. It is seen that, as in uni-directional spectra, the peak acceleration

occurs in the short period range, whereas peak displacement occurs in the long period

range.

6.5 Probabilistic Performance Analysis in terms of SWDR and MCDR

The performance of a system can be described in terms of exceedance probability

of response threshold at three levels, 2%, 10%, and 50% in 50 years. The probabilistic

performance curve of the structural system can be obtained by a log-normal fitting of the

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probability of median response. In order to account for system capacity uncertainty, a

systematic demand analysis is needed (Shome and Cornell, 1999).

Denote the inherent uncertainty in the system drift capacity (in terms of either

SWDR or MCDR) against a given limit state by Deap and the capacity uncertainty due to

seismic ground motions for a given level of spectral acceleration by DISa' Assuming that

all uncertainties follow a log-normal distribution, then the variance of In Y, ()~y, where

Y is the total system capacity, can be estimated by

()~y = ()~Dls + ()~D (6.9) a cap

In which the conditional variance, ()~DISa' is determined from response results of

analyses under SAC-2 ground motions as,

2 1 ~( )2 () InDISa = --LJ InDi -lnDm

N-2 i=l

(6.10)

where Di is the calculated drift ratio, Dm is the median drift ratio for a given probability

level of SAC ground motions, and N is the sample size. The variance of InDeap may be

estimated by

()~D = In(1 + o~ ) cap cap

(6.11 )

in which 0 D is the coefficient of variation of Dcarp. cap

If the uncertainty in Y does not dominate the reliability problem, as is the situation in this

study, its effect on the reliability can be represented by a correction factor (Maes, 1996).

The correction factor is defined as the ratio of the limit state probability with

consideration of the uncertainty to that in which the uncertainty has been ignored (Wen

and Foutch, 1997). It can be shown that the correction factor for the probability of failure

for the case of a single uncertain parameter (Maes, 1996) is

(6.12) 1

in which Oy is the coefficient of variation of the system capacity, Oy = [exp( ()~y) _1]2,

and S is the sensitivity coefficient (Wen and Foutch, 1997) calculated from

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InSam -A, S= '

1;2 (6.13)

in which A and ~ are the log-normal distribution parameters in the spectral acceleration

hazard curve and Sa,m is the median obtained from Equation (6.7). The median drift ratio

including total system uncertainty (Dm c ) can be estimated as , F

(6.14)

Then, the probabilistic performance curve can be constructed by fitting all three median

drift ratios Dm, Cp

by a log-normal curve. It will be used as basis in the calculation of the

redundancy factor.

6.6 Dual Uniform-Risk Redundancy Factor

Based on the results of nonlinear analyses, a redundancy factor can be defined and

evaluated considering all important contributing factors. A dual redundancy factor is

introduced to consider component versus system redundancy following the approach used

in the uniform-risk redundancy factor by Wang and Wen (1998). For dual systems

properly designed according to code requirements such as those in NEHRP or UBC, the

first shear wall failure (expressed in terms of Shear Wall Drift Ratio - SWDR) generally

occurs before the incipient collapse of the system (expressed in terms of maximum

instantaneous column drift ratio - MCDR). Two levels of limit states are, therefore,

considered: the first shear wall failure and the incipient collapse of the whole system. To

check the performance, the probabilities of first shear wall failure and the incipient

collapse of the system are evaluated and compared with the allowable values. Hence, a

total of four cases are possible:

1) P~~R < pall - SWDR and pip

MCDR < pall - MCDR

2) P~~R > pall SWDR and pip

MCDR pall

< MCDR

3) P~~R < pall SWDR and pip

MCDR > pall

MCDR

4) P~~R > pall SWDR and pip

MCDR > pall

MCDR

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P~~R = Probability of first shear wall failure

in terms of Shear Wall Drift Ratio (SWDR)

P;~R = Allowable probability of first shear wall

failure in terms of SWDR

P~CDR = Probability of incipient collapse of dual systems

in tenns of Maximum Column Drift Ratio (MCDR)

P~~DR = Allowable probability of incipient collapse of dual

systems in tenns of MCDR

Among these four cases, the second case is usually considered in practice.

The basic principles of dual redundancy factors given above are:

1) If the probabilities of the first shear wall failure and the incipient system

coilapse are lower than the allowable values, then the dual system is redundant

enough, and no increase in design force is necessary, and therefore, the design

n~rllln(1::Inr.v f::lr.t()r R D =1 -----------J ------, --.1'\.. _w

2) If the probability of the first shear wall failure exceeds the allowable value and

the probability of incipient system collapse does not, then the first shear wall

failure dominates and can be compensated by a design redundancy factor, RR,

which is the ratio of uniaxial spectral accelerations corresponding to the two

probabilities for the shear wall. The design redundancy factor (RR) for the

second case can be defined as follows:

Sip

Design redundancy factor, R R = S ~lSWDR a, SWDR

(Redundancy lacking in local (shear wall) system,

increase in design seismic force necessary)

st SWDR = Uniaxial spectral acceleration corresponding to P~\vDR

S~IsWDR = Uniaxial spectral acceleration corresponding to P;~DR

(6.15)

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3) If the probability of the incipient system collapse exceeds the allowable value

and the probability of the first shear wall failure does not, then the system is

compensated by a design redundancy factor, RR, which is the ratio of biaxial

spectral accelerations corresponding to the two probabilities for the system. The

design redundancy factor (RR) for the third case can be defined as follows :

Sip . d d.c. a, MCDR DesIgn re un ancy lactor, RR = --'-all--

Sa,MCDR

(Redundancy lacking in global (column) system,

increase in design seismic force necessary)

S~ MCDR = Biaxial spectral acceleration corresponding to P~CDR

S:~lMCDR Biaxial spectral acceleration corresponding to P~~DR

(6.16)

4) If both the probabilities of the first shear wall failure and the incipient system

collapse exceed the allowable values, RRR (Figure 6.6), defined as the ratio of

the difference between the probability and its allowable probability for the

system collapse and to that of the first shear wall failure, is calculated.

pip pall R = MCDR - MCDR

RR pip pall SWDR - SWDR

(6.17)

When RRR is less than 1, shear wall failures dominate; RR is then given by as the

ratio of uniaxial spectral accelerations corresponding to first shear wall failure

to the allowable value. Otherwise, system failure dominates; RR is then given by

the ratio of biaxial spectral accelerations corresponding to incipient system

collapse to the allowable value.

The graphical representation of dual redundancy factor is shown in Figure 6.5. The

allowable probabilities for both the first shear wall failure and the incipient system

collapse may be expressed in terms of exceedance probability depending on the desirable

levels of reliability required of the system. In most design code provisions such as

NEHRP the design earthquake is specified to be approximately corresponding to 10%

probability of exceedance in 50 years. Following SAC-2 (Foutch, 2000), the allowable

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probability of incipient system collapse is specified as 2% in 50 years. Since target design

force of a shear wall is usually less than design base shear, e.g. 91 % of design base shear

in ATC-19, the allowable probability of shear wall failure is assumed to be 10% in 50

years in this study.

The design redundancy factor is thus bounded by 0 and 1, which modifies the

required design seismic force in order to maintain the same reliability for systems with

different redundancies. The structural modification factor (R') may be defined as the

multiplication of the design redundancy factor (RR) by the traditional structural

modification factor (R) as follows:

R'=RR· R (6.18)

6.7 Definition of Incipient Limit State for Shear Walls and Moment Frames

Following Seo et al. (1998), the ultimate drift capacity of shear wall IS

approximated by following equation as a function of the wall aspect ratio:

(6.19)

The wall aspect ratios of 1.67 and 4 used in this study lead to ultimate drift capacities of

1.640/0 and 3% respectively. The drift capacity is further refined according to the shear

wall ductility capacity. For example, for an aspect ratio of 1.67, the drift capacity for

shear walls is from 1.52 % for a ductility capacity of 5.4 to 1.74 % for a ductility capacity

of 7.4. To establish the displacement threshold of incipient system collapse, repeated

dynamic response analyses under a suite of ground motions with a wide range of intensity

are necessary. According to dynamic push-over analyses (Incremental Dynamic Analysis

(IDA)) of SMRF buildings by Yun and Foutch (1998), the drift ratio capacity against the

collapse ranges from 70/0 to 10% with ductile connections. In the following reliability

evaluation, the drift ratio capacity of the incipient collapse of the SMRF system is

assumed to be 8% for ductile and 5% for brittle connection. Table 6.1 is used for the

definition of incipient limit state for shear walls and moment frames in this study.

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6.8 Redundancy Evaluation of Dual Systems

6.8.1 Five-Story, One-Way Dual Systems

The reliability and redundancy evaluation of 5-story, one-way dual systems under

biaxial motions were carried out. Based on seismic hazard and probabilistic performance

analyses, a dual uniform-risk redundancy factor (RR) was calculated and compared with

the reliability/redundancy factor (p) (Tables 6.2 and 6.3). Note that the uniform-risk

redundancy factors were obtained based on the nonlinear structural response analyses.

The effect of number of shear walls, ranging from one to three, was clearly shown

in tenns of both RR and p factor. According to the p factor, the change of configuration

and number of shear walls from one to three caused a 50% increase in system

redundancy, therefore, a 50% reduction in design earthquake force was obtained for the

three-shear wall system. On the other hand, according to the uniform-risk redundancy

factor, RR, there was only 17% reduction in design force. The probabilistic performance

curves of the dual systems of one, two, and three shear walls are given in Figure 6.9. It is

noted that the 50~~ reduction in design earthquake force according to the p factor grossly

overestimates the benefit of redundancy for the three-shear wall system.

The benefit of redundancy due to shear wall ductility capacity was also

investigated. The capacity change from 5.4 to 7.4 of ductility led to 12% reduction in

design earthquake force according to the RR factor because the exceedance probability in

50 years decreases as the ultimate drift capacity of shear wall increases. On the other

hand, the ultimate drift capacity is not considered in the p factor, therefore, design

earthquake force remains the same.

The effect of both the uncertainty and the correlation of shear wall strengths was

considered. It was found to have no significant contribution to the system redundancy.

This result can be partly attributed to the interaction between the shear walls and the

SMRF systems, which generally absorbs the effect of small variatien in shear wall

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strength variability. Also, a major contributing factor is that the variability in strength is

small compared with that in the ground excitation. In other words, the uncertainty in the

excitation dominates the reliability evaluation. The exceedance probabilities in 50 years

and redundancy factors of 5-story, one-way dual systems as functions of number of shear

walls, shear wall ductility capacity, shear wall strength correlation, and the ratio of

earthquake to strength variability are compared in Figure 6.7 and 6.8 respectively.

6.8.2 Five-Story, Two-Way Dual Systems

Two-way dual systems under biaxial motions were considered. The biaxial

interaction effect may be amplified if the fundamental periods of the two principal

directions are close to each other. The in-plane capacity of a shear wall for a given

principal direction can deteriorate due to the lateral force from the other direction.

Therefore, the biaxial interaction usually amplifies the structural response. The results

show that approximately 8% design force reduction in the X direction and 0.1 % reduction

in the Y direction were obtained by replacing one wall with three walls according to the

uniform-risk redundancy factor (RR)' Meanwhile, a 50% design force reduction in the X

direction and a 46% design force reduction in the Y direction were obtained according to

the reliability/redundancy factor (p) (Table 6.4).

6.8.3 Ten-Story, Two-Way Dual Systems

The redundancy of longer-period dual systems with different number of shear walls

was studied under biaxial motions. Owing to the large ultimate drift capacity of the shear

wall, i. e. 1.5 % drift capacity of shear wall with an aspect ratio of 4, for such systems, the

failure probability of the shear wall was less than the allowable probability of 10% in 50

years. Hence, the uniform-risk redundancy factor (RR) was unity for both one- and two­

shear wall systems. It follows that the ductility capacity of a shear wall with a large

aspect ratio, as is usually found in such buildings, can be an important parameter by

which to judge the reliability of a shear wall structure. The nonlinear responses of the

dual systems with one and two shear walls were all within allowable values and the

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reliabilities of shear walls for both systems are satisfactory. In contrast, as seen in Table

6.5, according to the p factor, approximately 48% of redundancy deficiency in one-shear

wall and 40% in two-shear wall system were obtained. The probabilistic performance

curves of the dual systems including one and two shear walls are given in Figure 6.10. In

summary, the above results show that the risk-based redundancy factor based on

structural responses assures uniform reliability for systems with different number of shear

walls, while the results according to the p factor considering system configuration only

could lead to erroneous evaluation of the required design force.

6.9 Redundancy Evaluation of Steel SMRF Buildings

6.9.1 Three-Story Buildings with No Torsion

Two three-story ductile steel moment resisting frames under biaxial excitations

were considered. They were a 4 x 4 bay and a 6 x 6 bay SMRF system. Responses of

these two systems under SAC motions were calculated and compared. Nonlinear static

push-over analysis was performed to verify that the two systems have equal lateral

resistance. The median values of the dynamic responses of both systems under SAC-2

excitations were almost the same at all probability levels and satisfy the performance

requirements as shown in the probabilistic performance curve of Figure 6.11. The RR

factor is, therefore, unity for both systems. The p factor, however, drops from 1.24 for the

4 x 4 bay frame to 1 for the 6 x 6 bay frame, indicating an increase of 24% in design

earthquake force required of the 4 x 4 bay system (Table 6.6).

6.9.2 Nine-Story Buildings with No Torsion

Two nine-story SMRF structures of longer period and ductile connections were

also studied. The responses of these two systems, 5 x 5 and 8 x 8 bay S:MRF, were

calculated and compared. The beams and columns were chosen so that the total lateral

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resistances of the two systems were the same. As a result, the median story drift ratios of

the two systems are close under biaxial excitations. It is found that the larger number of

bays does not necessarily reduce the structural response, as long as the total lateral

resistance remains the same. The probabilistic performance analyses of these two

buildings are given in Figure 6.12. The NEHRP factor (p) calculation based on column

shear force gives a 25% increase required of design force for the 5 x 5 bay system

(Maximum for a SMRF in NEHRP, 1997), whereas the same RR factor of 1 is found for

the two systems (Table 6.7). The p factor, therefore, overstates the lack of redundancy in

the 5 x 5 bay system in comparison with the 8 x 8 bay system. In view of two systems

that have the same performance verified by reliability analysis, the 25% increase in

design force appears to be unnecessary.

6.9.3 Three-Story Buildings with Torsion

The three moment frames of 1 xl, 2 x 2, and 3 x 3 bays with 5% accidental torsion

and either ductile or brittle connections under biaxial excitations underwent severe

nonlinear responses at the 2/50 hazard level. For systems with ductile connections, the RR

factor was 1.0 for the 2 x 2 bay and 3 x 3 bay systems and 0.94 for the 1 x 1 bay system

(Table 6.8). A 6% increase is, therefore, required of the design force for the 1 x 1 bay

system. On the other hand, for systems with brittle connections, the required increase of

design force was 370/0 in the 1 x 1 bay and 31 % in the 3 x 3 bay system. In contrast, the p

factor is calculated to be 1.25 for the 1 x 1 bay and 2 x 2 bay systems, and 1.24 for the 3

x 3 bay system, indicating a increase of about 25% required of all systems, regardless of

connection behavior, which is not considered. The probabilistic performance curves of

the systems with ductile and brittle connections are given in Figure 6.13 and 6.14

respectively. The benefit of redundancy is more evident for the moment frames with large

drift capacity. Also, the benefit of large number of bays is more evident for the moment

frames with ductile connections. There is a little difference in probabilistic performances

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of the three systems with brittle connections. This finding also agrees with the results of

simple parallel systems.

6.10 Verification of Dual Uniform-Risk Redundancy Factor

To verify the adequacy of the dual uniform-risk redundancy factor, RR, the

reliability of the foregoing 5-story, one-way dual systems was re-evaluated after redesign.

To achieve a target reliability given by that of the three-shear wall system, the one-shear

wall system is redesigned in accordance with RR. The RR factor was 0.83 for the one­

shear wall and 0.97 for the three-shear wall systems. Therefore, the one-shear wall

system should be strengthened by 20%. As illustrated in Table 6.9, the new design base

shear was 2646 Kips compared to 2165 Kips of the original design. The redesigned shear

wall was made 5 in thicker with 5 in2 more reinforcement in longitudinal steel, As and

As'. The yield and ultimate strength of the shear wall was enhanced as shown in the

Table 6.9. The redesigned dual systems with one-shear wall system were then subjected

to SAC-2 motions The median SWDR responses corresponding to the three probability

levels were 247°0. 1300/0, and 0.51% respectively, which were comparable to those of

the three-shear wall system. The RR factor is 1.0 for the redesigned system as compared

with 0.97 for the three-shear wall system (Table 6.10). The comparison of probabilistic

performance CUf"\ es is also shown in Figure 6.15. The probabilistic performance curve of

the redesigned one-shear wall system closely matches that of the three-shear wall system.

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Table 6.1 Definition of Incipient Limit State for Shear Walls and Moment Frames.

Allowable

Systems Drift Capacity Probability of

Incipient Collapse

Aspect Ratio : 1.67 1.64% (SWDC) 10% in 50 years

(5-Story Dual Systems) Shear Walls

Aspect Ratio: 4.0 3% (SWDC) 10% in 50 years

(1 O-Story Dual Systems)

With Ductile Connections 8% (MCDC) 2% in 50 years Moment Frames

With Brittle Connections 5% (MCDC) 2% in 50 years

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Number of

Shear Walls

Ductility of

Shear Walls

127

Table 6.2 50-Year Probability ofExceedance of Shear Wall.

(5-Story, One-Way Dual Systems)

System Exceedance Probability in 50 years

1 0.18

2 0.17

3 0.11

5.4 0.15

6.4 0.12

7.4 0.10

0 0.17

Correlation of 0.2 0.17

Shear Walls 0.6 0.16

1.0 0.17

Ratio ofEQ 2.67 0.11

Load to 3.56 0.11 Strength

Variability 5.33 0.11

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Table 6.3 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor.

(5-Story, One-Way Dual Systems)

System RR P

1 0.83 1.50 Number of

2 0.85 1.02 Shear Walls

3 0.97 1.00

5.4 0.88 1.00 Ductility of

6.4 0.97 1.00 Shear Walls

7.4 1.00 1.00

0 0.85 1.02

Correlation of 0.2 0.85 1.02

Shear Walls 0.6 0.86 1.02

1.0 0.85 1.02

Ratio ofEQ 2.67 0.97 1.00

Load to Strength 3.56 0.97 1.00

V ari a b iii t \ 5.33 0.97 1.00

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Table 6.4 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor.

(S-Story, Two-Way Dual Systems)

RR P System

X y X Y

1 0.86 0.69 1.S0 1.46

Number of 2 0.92 0.71 1.02 1.00

Shear Walls 3 0.93 0.69 1.00 1.00

Table 6.S Comparison of Uniform-Risk Redundancy Factor (RR) and p factor.

(10-Story, Two-Way Dual Systems)

RR P System

X y X Y

Number of 1 1.00 1.00 1.48 1.47

Shear Walls 2 1.00 1.00 1.41 1.39

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Table 6.6 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor.

(3-Story SMRF Systems with No Torsion)

System RR P

4 x 4 Bay 1.00 1.24

6 x 6 Bay 1.00 1.00

Table 6.7 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor.

(9-Story SMRF Systems with No Torsion)

System RR P

5 x 5 Bay 1.00 1.25

8 x 8 Bay 1.00 1.00

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131

Table 6.8 Comparison of Uniform-Risk Redundancy Factor (RR) and p factor.

(3-Story S:MRF Systems with Torsion)

System RR P

Ductile 0.94 l.25

Connection 1 x 1 Bay

Brittle 0.63 l.25

Connection

Ductile 1.0 l.25

Connection 2 x 2 Bay

Brittle 0.64 l.25

Connection

Ductile l.0 l.24

Connection 3 x 3 Bay

Brittle 0.69 l.24

Connection

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Table 6.9 Redesign of 5-Story Dual Systems with One Shear Wall.

System Original System Redesigned System

Design Base Shear 2165 Kips 2646 Kips

Wall Reinforcement 10 in2 15 in2

(As, As')

Wall Thickness (tw) 26.3 in 31.3 in

Wall Yield Displacement 0.83 in, 1687 Kips 0.83 in, 2146 Kips

and Force( ~y, Fy)

Wall Ultimate Displacement 5.33 in, 2152 Kips 5.33 in, 2706 Kips

and F orce( ~u, F u)

Table 6.10 ResponselRedundancy of Redesigned 5-Story Dual Systems

System

Response 2/50

(SWDR~ 10/50

%) 50/50

Exceedance Probability :_ t:.f"'I v~~_~ 1l1..JV lC;a.l~

Dual Uniform-Risk

Redundancy Factor, RR

.

with One Shear Wall.

Original One- Redesigned One- Original Three-

Shear Wall Shear Wall Shear Wall

2.52 2.47 2.43

1.44 1.30 1.38

0.58 0.51 0.56

0.18 0.10 0.11

0.83 1.00 0.97

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133

5

en 4 c

0 m :..... 3 (])

(]) ()

~ "'ffi

2 :..... +-'

~ 1 (f)

0 0 1 2 3

Structural Periocf (sec)

(a) LA21

5

.-. en

5 4

m :..... 3 (])

(]) () ()

<! "'ffi

2 :..... +-'

~ 1 (f)

0 0 1 2 3

Structural periocf (sec)

(b) LA22

Figure 6.1 Uniaxial Elastic Response Spectrum (Sa).

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134

50 ..-c -- 40 C ~ Q)

30 ~ 0-CJ)

0 20 "'ffi ~

+-'

~ 10 (f)

0 0 1 2 3

Period (sec)

(a) LA21

50 ..-c -- 40 C ~ Q)

30 ~ 0-CJ)

0 20 "'ffi ~

+-'

~ 10 (f)

0 0 1 2 3

Period (sec)

(b) LA22

Figure 6.2 Uniaxial Elastic Response Spectrum (Sd).

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135

(a) Biaxial Spectral Acceleration (LA21 and LA22)

(B) Biaxial Spectral Displacement (LA21 and LA22)

Figure 6.3 Biaxial Elastic Response Spectrum.

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136

\ ................................................... . .. ...

0.1 , .:::::: .... ::::::~ ......

...... :::: ... :: ... : ... ~.;>.. ............. , ............................................ · .. ; ...... · ............ · .. · .. · .... · ............ · .. ·1 U\.. ;

0.01 " .. ".

........

c: 1-10-3 ..D

2

. .......... (,

~ ..... .

0....

~ 1"10-4

I .... · ...... · .......... · ........ · ........ · .... ·, .. · .... · .. · .. · ...... · .... · ........ · ............. ; .......................... :.""' ..... ""'~ .. ..

c: c:

<C

..

00 Medians Regression Line

.. .. ....... .. ; ................ .

, ....

Sa (T1=O.81, T2=O.73, c;=O.02) (g)

(a) Annual Probability of Exceedance (X Direction)

e 0.01 ::: ~

"§ :..;

1-10-3 x ~ '-

.g 6: 1-10-4 §

~ 1-10-5

a 2

00 Medians Sa Cf1=D.81, T2=D.73, g=O.02) (g) Regression Line

(b) Annual Probability of Exceedance (Y Direction)

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137

....... ::.:.: ........ . ...............................

........................ ~, ......... " .................................................... ; .............................................. ·····i

0.1 E···7····7····7·····7·····7····7·····S.~7· .. ~S .... 7 ... r\~·····7····~~222T22~·7 ·······2·······7······2·· ···7·······~···· ••••• H .................. • ••• ~,."\.' ••••••••••• .; •••••••••••••••••••••••••••••••••••••••••••••••• ~ ....................... "-Z

0.01 /==:::-=::-=::::=::::==..::::,==:::-=::-::::.== .:::-=::-~.=::::.. .~,=:::: ..... := ..... ::::. --==1 ., "'

I········································ .. ".·········· ......................................•................................ '-.. "' ....... .-.-.-.-.. .-.-. , ....

o

00 Medians Regression Line

2

Sa (TI=O.81, T2=O.73, <;=0.02) (g)

(c) 50-Year Probability of Exceedance (X Direction)

;..

~ .... (j I r t:: ..

..".

.(;

..:: "(II 2! "-~ -J!

.> - 1

00 \1cdlans Regression Line

2

Sa (TI=O.81, T2=O.73, ~.02) (g)

(d) 50-Year Probability of Exceedance (Y Direction)

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138

1 ~\d' ................. d..; . " .........

'\ \ ...... '. \ ............................................•.............................................. ~ .................... ····························i

0.1 :::::::::::::::\d \

.. .....

. ................. .

....

om . . ....... d ••••••••••••••••••• "

.................... ~"' .............•................................................... , •................... ·····························i "&.

.' . ....... ,

........

'-'........ . '"a -3 ........

j'lO p·S····· ·52····3377~T·~ ···7······33·····fFf~jSS;S33.(;t; .... 2 .... R .. J4 ~ .....

.

o 2

00 Medians - Regression Line

Sa <TJ=O.81, T2=O.73, g=O.02) (g)

(e) Annual Probability of Exceedance (Bi-Directions)

o 2

00 Medians Sa <TJ=O.81, T2=O.73, ~=O.02) (g) - Regression Lin

(f) 50-Year Probability of Exceedance (Bi-Directions)

Figure 6.4 Spectral Acceleration Hazard Curve.

(la-Story, Two-Way Dual Systems with Two-Shear Wall System)

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piP MCDR

p all

MCDR

1 : RR = 1 Sip

2 : RR = a,SWDR Sail

a, SWDR

S~ iviCDR

sail a, MCDR

139

3

p all

SWDR

4

2

piP SWDR

Sip = a, SWDR £ R < 1

~~11 or RR - , for RRR > 1 Sip

a, MCDR

nall :S~:'SWDR ~;, MCDR

Figure 6.5 Dual Uniform-Risk Redundancy Factor, RR.

pip paIl MCDR - MCDR

MCDR CONTROL

RRR < 0

MCDR R > 0 ~ONTROL RR

"\ RRR=l

~ SWDR ~ CONTROL

pip SWDR

SWDR CONTROL

RRR < 0

pall SWDR

Figure 6.6 Relative Redundancy Ratio, RRR.

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U) a: ~ 0.18 L()

~ ai 0.16 o a: 0-UJ 0.14 o z « fa 0.12 UJ o x UJ

U)

~ 0.20 a 0.18 L()

~ 0.16 ai 0.14 2 0.12 0- 0.10 ~ 0.08 ~ 0.06 fa 0.04

EFFECT OF NUMBER OF SHEARWALL

1.0 1.5 2.0 2.5 3.0 NUMBER OF SHEARWALL

EFFECT OF CORRELATION

• ---e •

~ 0.02 x 000 ... ' ---'-----'-------'---'-----' UJ -0 , 0.1 0.3 0.5 0.7 0.9 1.1

CORRELATION COEFFICIENT

140

U) a: ~0.15 L()

~ ai 20.13 0-UJ o z C§ 0.11 UJ UJ o X UJ

U)

~ 0.20 gO.18 zO.16 ~0.14 20.12 0- 0.10 ~0.08 ~0.06 fa 0.04

EFFECT OF DUCTILITY OF SHEARWALL

5.5 6.0 6.5 7.0 7.5 DUCTILITY OF SHEARWALL

EFFECT OF THE RATIO OF VARIABILITY

~0.02 ~ 0.00 L..-_--'-__ ---' ___ -'--__ __'__

3 4 5 6 THE RATIO OF VARIABILITY

Figure 6.7 Exceedance Probability (5-Story, One-Way Dual Systems).

a: o L.' 09: r < ~

>-l,..-, 09( t :i c ~

EFFECT OF NUMBER OF SHEARWALL

, .'- _, 2.0 2.5 3.0 ~ .,·VBER OF SHEARWALL

E""r:~ 'Y CORRELATION COEFFICIENT

• • • •

C f i.

o r; ~ - I 0.4 l.-' ---'---~--'---'-----'----'

·0 , o 1 0.3 0.5 0.7 0.9 CORRELATION COEFFICIENT

1.1

~ 1.00 I­o « LL

t; 0.95 z « o z 50.90 UJ a:

~ 1.0 I-

~ 0.9

t; 0.8 z « o z ~ o UJ a:

EFFECT OF DUCTILITY OF SHEARWALL

5.5 6.0 6.5 7.0 7.5 DUCTILITY OF SHEARWALL

EFFECT OF THE RATIO OF VARIABILITY

• • •

0.7 f 0.6 _ 0.5 L..-_--'-___ '--__ -'-__ ---'-_

345 6 THE RATIO OF VARIABILITY

Figure 6.8 Redundancy Factor (5-Story, One-Way Dual Systems).

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141

rJj

~ .......... ::~. . ...... .

Il.) "\~. ~f'."'·,~~<············································ ..................................................... ~

~ 0.1 f==Eg~.~, ... = ...... = ..... = ...... = ..... = ......... = ..... = ...... = ......... = .......... = ...... = ...... =1 .... . ~ I····················································;.11., ..... ''310.: ................... .

~ .~~.......

.g 0.01 r7272IIS·····S······72······I72~~~~~~~~ Il.) " ~--s;,: ...... . 8 ...................................................... ···················· .. ·,····.·.,;.:···~: ... ·,·~···· ... ··· .. ··I ~ '.~ ~-3 "~ 1-10

a 2 3 4 5

Drift Ratio (%)

1 shear wall system 2 shear wall system 3 shear wall system

Figure 6.9 Probabilistic Performance Curves of 5-Story, One-Way Dual Systems (X

Direction).

3

Drift Ratio (%)

00 Median values (l Shear Wall) Lognonnal Fitting (1 Shear Wall)

X X X Structural Responses (1 Shear Wall)

no Median values (2 Shear Walls) Lognonnal Fitting (2 Shear Walls)

;-. -+- 'r' Structural Responses (2 Shear Walls) 1 Shear Wall with system uncertainty 2 Shear Walls with system uncertainty

(a) X Direction

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142

....

.. :~~~, .. , ., .•...... , .................................................................... ; ............................ ····1

~~ ..

0.1 F .. ~S.::~·::~·::.:~~.:?::-.~:::.~:;.~~:r~?~~-,~~ •• ,,@~2 .... ?~.:2 .. ~2 ... ~, .... G .. 27 .27~8.~GG27q **~6L~(.+

.""~ ... ~ .. . 0.01 r=-:::=:::::::: ... ::::.:::::::;.:-.-:::=-:::=-:::=::::::::::::::::-:::==.::-... ~ ... ~ ... ,.,r:;;: •. .'!!'o:::::::.;:::::".= .... ~ ..... ~.

. ::' ... ...

1_10-3

Drift Ratio (%)

99 Median values (1 Shear Wall) Lognonnal Fitting (1 Shear Wall)

XXX Structural Responses (l Shear Wall)

DO Median values (2 Shear Walls) Lognonnal Fitting (2 Shear Walls)

+++ Structural Responses (2 Shear Walls) 1 Shear Wall with system uncertainty 2 Shear Walls with system uncertainty

(b) Y Direction

.\ ..

~ C'j Q) >-.

0 0.1

!!2 .0 0 I-

0... Q) u c:: C'j

'"0 0.01 0 .•....... ,.:~. (!) u """t • ... ><

u.:J .~!'OIo' .... """ ... ~

1-10- 3

Maximum Column Drift Ratio (%)

00 Median values (l Shear Wall)

XXX Lognonnal Fitting (1 Shear Wall) Structural Responses (1 Shear Wall)

DO Median values (2 Shear Walls)

+++ Lognonnal Fitting (2 Shear Walls) Structural Responses (2 Shear Walls) 1 Shear Wall with system uncertainty 2 Shear Walls with svstem uncertain tv

(C) Bi -Directions

Figure 6.10 Probabilistic Performance Curves of 10-Story, Two-Way-Dual Systems.

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·::::::§ik~~ .......... :~:x:.:.::.: ......................... ~ ....... . 'i\ ......................•. ~~~ ..... . ......................... +......... . .....

o.! t--------lJe~_~~~-----------------_I

:::r::·::::·:?::~~~,:::::::::::: : ........... :::::::.: .......................... . ...................... , ........................ " •........ : ..................... + ........................................ .

8 .. H';H-<I( Q~Qx-«>¢«>~ § . ,\:,'.. :

] (J.(J! 1-. --....,-.. -..•. -..•• -... -.""'" .. - .. -... -.... -.... -.... ""'" .• ;.,.:.:~:,.r::,,~ ....• -.~-;-t-.:::-.... -.-------; >( ....................•. ,... ....•..........•....•.•.•.••.••.. ..! .. ,~.~~........ . ....

UJ:"I~~~·~.,:~<

00 Q

00 xxx

. '. ~[~~:~~: 4

Maximum Column Drift Ratio (%)

Median values (4x4 Bay) Lognormal Fitting (4x4 Bay) Structural Responses (4x4 Bay)

Median values (6x6 Bay) Lognormal Fitting (6x6 Bay) Structural Responses (6x6 Bay) 4X4 Bay with system uncertainty 6X6 Bay with system uncertainty

Figure 6.11 Probabilistic Performance Curves of 3-Story SMRF Systems eX Direction

and No Torsion).

-, 1-10 .

i~:;~mmm \\ '\ .. ,

Maximum Column Drift Ratio (%)

00 Median values (5x5 Bay) Lognormal Fitting (5x5 Bay)

Q Structural Responses (5x5 Bay)

00 Median values (8x8 Bay) Lognormal Fitting (8x8 Bay)

X X X Structural Responses (8x8 Bay) 5X5 Bay with system uncertainty 8X8 Bav with svstem uncertain tv

Figure 6.12 Probabilistic Performance Curves of 9-Story SMRF Systems eX Direction

a..'1d :t'-Jo Torsion).

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1 I uQuuu .. uu .. uu.uuuuu u .............. '.·.·.: .... :.· ... · ... ·:.:.u .. u. u .. u uuuul

F··:::·~~······~~:=;~~··········~··· ~~~ ... . O.1··'="~3·-:.r, .. :~~: .... ·~ ...... :: ... ······· .. . u.................. _ ~ ..... ~.::~

0.0 1 p.:s: .... ¥J.7DS:77:'F7E7J7'271S7'F)~~t::~ ,., .....

. ,.

.. . ..

a 2 4 6 8 10

Maximum Column Drift Ratio (%)

IXI Bay 2X2 Bay '1V'1 Dn" .J~.J vay

Figure 6.13 Probabilistic Performance Curves of 3-Story SMRF Systems (Ductile

Connection and Torsion).

0.01 !--------......,....------...,.....j

a 2 4 6 8 10

Maximum Column Drift Ratio (%)

IXI Bay 2X2 Bay 3X3 Bay

Figure 6.14 Probabilistic Performance Curves of 3-Story SMRF Systems (Brittle

Connection and Torsion).

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rJ) ..... ro o >.

145

o !C: 0.1 r====~~=~=====i .0 o .....

0... o U t: ro

a3 0.01 ........................ " .. ::.:~.:::::: .. o ...... . . ................ , ::::::::~:\:~::': .. : .......... ·····1 u

>< ~

o

............................................................... , ....................•.....

." ......................... ~.~.; ..... . ".

2 3 4 5

Drift Ratio (%)

1 shear wall system redesigned 1 shear wall system 3 shear wall system

Figure 6.15 Probabilistic Performance Curves of Redesigned 5-Story , One-Way Dual

Systems (X Direction).

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CHAPTER 7

SUMMARY, CONCLUSIONS, AND RECOMMENDATIONS FOR FUTURE RESEARCH

7.1 Summary

The extensive investigation of structural failure after the Northridge earthquake

revealed the lack of system ductility capacity and redundancy as one of the most

important causes of such failures. The concept and definition of redundancy, however,

have not been clearly understood by structural engineers.

The redundancy of simple structural systems under random static loads has been

studied extensively in the past. Very little has been done on structural redundancy under

dynamic and stochastic loads due to the analytical difficulty of such problems. Provisions

in some recent codes and building design documents (e.g. ATC-19 1995; ICBO, 1997)

include a reliability/redundancy factor based on a penalty factor applied to the response

modification factor, R. The factor is dependent on structural configuration (number of

structural components, ground floor area, and maximum element-story shear ratio) based

mostly on engineering judgement. There has been dissatisfaction with this approach (e.g.

Whittaker et al. 1999). Further research is needed for a better knowledge of redundancy

that will enable engIneers to design and evaluate for the effect of redundancy in a

systematic way.

In this study the system reliability and redundancy of building structures is

investigated by response and reliability analyses of dual systems and steel moment

frames. Major factors affecting redundancy such as structural configuration (number and

layout of structural components), loading path change after partial failure, structural

member ductility capacity, and uncertainty in the capacity versus demand, are examined.

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147

Three-dimensional models were developed for the building systems. The building

structures were assumed to have rigid diaphragm in-plane but flexible diaphragm out-of­

plane. Interaction between shear walls and moment frames was included in the analysis.

Biaxial interaction and P-L1 effect were also considered. An equivalent shear wall model

based on DRAIN-3DX was proposed to simulate the global hysteretic behavior observed

in experiments. The model was intended to capture the essential hysteretic behaviors such

as stiffness/strength degradation and pinching effect. The hysteretic curve of the model

compared well with the test results. To achieve a target ductility capacity of shear wall, a

displacement-based design methodology was used. Two response variables, shear wall

drift ratio (SWDR) and maximum column drift ratio (MCDR) , were used for local and

global damage measures respectively. Factors affecting redundancy of dual systems, i.e.

number and layout of shear walls, ductility capacity and lateral resistance variability,

uncertainty and correlation of shear wall strength, were considered in the response

analyses and the redundancy evaluations. Three dimensional steel moment frame

buildings of different number of bays and column and beam sizes were also considered.

The effect of beam-column connection behavior (ductile or brittle) was included in the

response analyses following Wang and Wen (1998). The MCDR response variable was

used for the evaluation of moment frame redundancy.

The systematic analysis of seismic demand (Shome and Cornell, 1998, 1999) and

the framework for evaluation of structural reliability (Wen and Foutch, 1998) were used

to evaluate the probabilistic performance and redundancy. The uncertainty in seismic

loads was incorporated via the seismic hazard curve of spectral acceleration. Based on

results of nonlinear structural response analyses, probabilistic performance analyses were

carried out. The median response under SAC-2 ground motions was calculated and

multiplied by a correction factor to account for the resistance and modeling uncertainty.

A log-normal distribution was then used to describe the system performance. Three

exceedance probability levels, 2%, 10%, and 50% in 50 years, were used for this purpose.

The uniform-risk based redundancy factor proposed by Wang and Wen (1998) for special

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148

moment frames was extended to the dual systems. Finally, a comparison of the risk-based

factor and the recently proposed reliability/redundancy factor in NEHRP-97 was made.

7.2 Conclusions

The following conclusions are drawn from the results of this study:

1. The hysteretic behavior and energy dissipation capacity of a shear wall are

described satisfactorily by the proposed analytical shear wall model. The target

ductility capacity of the shear wall is achieved by the use of a displacement­

based design methodology.

2. The interaction between the shear walls and moment frames plays an important

role in making the dual systems robust, i.e. increasing the energy dissipation

capacity under seismic excitation. It is a significant factor in the load-carrying

capacity of the system after partial failure, and thus, has a strong influence on

the structural response and redundancy.

3. Everything else being equal, more shear walls and larger ductility capacity of

shear walls provides more redundancy in the dual systems. For example,

replacing one wall with three walls results in 17% reduction in design force.

Likewise, larger ductility capacity, i.e. from 5.4 to 7.4, of the shear wall results

in a reduction of 12%.

4. Without torsion, the two equivalent three-story moment frames of 4 x 4 bay

versus 6 x 6 bay with ductile connections give the same performance under

SAC-2 ground motions. The uniform-risk redundancy factor is, therefore, the

same and equal to 1 for both systems. The same is true for the two nine-story

moment frames of 5 x 5 bay and 8 x 8 bay. On the other hand, the benefit of

larger number of bays is seen when torsion is considered. The comparison of

three-story moment frames with 5% torsion shows 6% reduction in design

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149

force from 1 x 1 bay system to 3 x 3 bay system with ductile connections. The

reduction is 9% if the connections are brittle.

5. Comparison of the results based on the uniform-risk redundancy factor and the

NEHRP redundancy factor, p, shows that p over estimates the effect of system

configuration and underestimate effects of ductility capacity and biaxial and

torsional motion. The uniform-risk redundancy factor, on the other hand,

considers these factors and addresses the uncertainty in demand and capacity

and as a result gives more consistent results.

6. The adequacy of the proposed uniform-risk redundancy factor in achieving a

target reliability is demonstrated by a re-evaluation of the reliability of a 5-

story dual system after redesign according to the proposed procedure. The

results show that, after redesign, the one-shear wall system has the same

reliability as the three-shear wall system.

7.3 Recommendations for Future Research

The following is suggested for further investigations in the future:

1. On ft capacity corresponding to allowable probability of incipient collapse

suggested hy incremental dynamic push-over analyses shows wide scatter. The

drift capacity for incipient collapse should be defined with a proper

conSideratIOn of the uncertainty.

2. The ~tud~ of dual systems of primary bracing and secondary moment frames is

needed

3. The tn-plane flexible diaphragm is more appropriate in low-rise buildings. The

effect of flexible diaphragm should be considered in the performance analysis.

4. The out-of-plane buckling capacity of a shear wall under biaxial excitations is

ignored by assuming an adequate thickness of shear wall in this study. The

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150

instability problem, however, exists in nature. It needs to be included in the

response analysis.

5. Considerations of nonstructural components are excluded in this study. The

effect of nonstructural components is significant in the dynamic analysis of

building. Further research is needed taking the non structural components into

consideration.

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APPENDIX

EARTHQUAKE RESPONSE ANALYSIS OF THREE DIMENSIONAL DUAL SYSTEMS

1-Story Dual Systems

yKx, Y Ky Kx, Ky 3 DOFs SYSTEM

y

i ~ b >:=::}::<,,:,,::::,:"::::, x

l C.M. • C.S

Consider Ksx' KSY ' Kse for shear wall

Uy

{u} = l~:) Kx, Ky Kx, Ky

a ~ ~

Neglect the mass of shear wall at a given floor level.

[M] = [~ \v'here, Ie = °

The stiffness matrix is assembled by assuming unit displacement in each DOF.

yKx

+----0------ Kyx

Kx

,

~9xj ,

Ksx : , ,

Kx

Kx

LFx = 0, Kxx = (3+y)K x + Ksx

LFy=O, Kyx=O

b LM = 0, K{h( = "2 Kx (l-y)

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yKy

Kyy

---------f-----Kay------::::",.,:>::, ... :.:. Kxy

Ksy

I I

152

Ky

LFx = 0, Kxy = ° LFy = 0, Kyy = (3+ y) Ky + Ksy

a LM = 0, KOj = "2 Ky (l-y) r------------------------l

Ky ... uy=l ... Ky

yKx (b/2)

Kx (b'2) Ky(al2)

k·~.~ • yKy .. \_.~= ____ /_--. _. ___ _ (a

/2) / ...

~ Kx(b!2)

K~ (a.:1 J u . .=l

Thus, the stifTness matrix is

Ky (al2)

a LFy = 0, Kye = (l-y) Ky 2

Kx(b/2) LM = 0, Kee = (3 + y).

r K (~12 + Kv (~121 L x 2) J \2) J

+ Kse

ify = I, that IS. center of mass is equal to center of stiffness and Ksy = 0,

f4K + K i )< SX

I ° I

l ° °

° °

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153

In design point of view, suppose that the stiffness of shear wall in X direction is a

times higher than total stiffness of columns and the stiffness of shear wall in rotation is ~

times higher than total stiffness of columns (proportional rigidity), that is,

then,

4Kx(1+a) 0 0

[K] 0 4Ky 0

0 0 4( (~J Kx + (~J Ky J .[I+,8J

where, Kx 12E Iy 12Elx

3 Ky h3 h

Thus, the stiffness matrix can be expressed in terms of only stiffness of column. a

and ~ can be assumed by the design purpose. This stiffness matrix is the same as that of 2

or 3 shear wall systems in the dual systems.

Equation of motion

[M] {ii t} + [C] {u} + [K] {u} { 0 }

When considering 3 dimensional response, the direction of earthquake motion must

be considered. For earthquake motion in X direction only,

jii \ I liix + ii g

) •• t •• U y = liy •. t •. U () lie

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In general,

{iit} = {ii} + {s} iig

[M] {ii} + [c] {u} + [K] {u} = - [M] {s} iig

let {u} = [<l>] {q}, and premultiply [<l> f by both sides

[<l>JT [M] [<l>] {Ci} + [<l>Y [C] [<l>] {ci} + [<l>]T [K] [<l>] {q} = - [<l>f [M] {S} iig

Normalize as [<l>]T [M] [<l>] = [I],

In terms of generalized coordinates,

where, ri { tp i } T [M] S i

{ tp i } T [M] {tp i } parti ci pati on factor

= {tp i } T [M] S i

q" = r q" = r Sd" I I 10 I I

{u} = [<l>] {q}

5-Story Dual Systems

Model the structure with 3 degrees of freedom (DOF) each floor and assume rigid

floors. The global mass, stiffness, and displacement matrices are expanded to reflect the

increased number ofDOF.

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155

U SX

USy

USB

U 4x

U 4y

U 4B

U 3x

{U} = U 3y [M]lS xIS, [K]lS x 15

U 3B

U 2x

U 2y

U 2B

U 1x

U 1y

U w 15 x 1

Equation of Motion

[M] {U} + [C] {u} + [K] {U} = - [M] {S} Ug

let {u} = [<1>] {q}, and premultiply [<I>]T by both sides

[<Dr [M] [<1>] {Ci} + [<I>Y [C] [<I>] {q} + [<I>Y [K] [<I>] {q} = - [<I>]T [M] {s} ug

Nonnalize as [<1>Y [M] [<I>] = [1],

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156

In tenns of generalized coordinates,

{lPi} T [M] Si

where, ri = {q>if [M] {q>J

= {lP i } T [M] S i

participation factor

q. = r q. = r Sd· 1 I 10 I I

{u} = [<I>] {q}

In order to calculate the frequency and mode shape of the dual systems,

LtvI] {u} + [K] {u} = 0

Assume ui = Ai· eimt , hannonic solution

u. = _OJ2 u·

1 I

-OJ 2 [M] {u} + [K] {u} = 0

[_OJ2 [M] + [K]] {u} = 0, eigenvalue problem

solve for OJ, ¢

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