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SIMPLIFIED ANALYSIS TO
PREDICT COLLAPSE
RESISTANCE
April 2017
Ramon Gilsanz
Akbar Mahvashmohammadi
Participants
•
2
Ramon Gilsanz
Karl Rubenacker
Akbar Mahvashmohammadi
Joshua Peng
John Abruzzo
Ross Cussen
Joe Gannon
Nabil A. Rahman
Sarah Orton
Min Liu
Contents
• 1- Introduction
• 2- Simplified Analysis to Components
• 3- Dynamic Effects on Collapse Capacity of Components
• 4- Simplified Analysis to Systems
1- Introduction
• The objective is to develop simplified formulas to predict
collapse capacity of structures:
 Steel and concrete moment frames
 Steel gravity frames
 Flat plates
• Wood, cold formed steel, and masonry are not considered in
this study
2.1- Steel Frame Structures
• Equilibrium:
• Material:
 Elastic perfectly plastic with effective yield stress 𝐹𝑦,𝑒𝑓𝑓 = (𝐹𝑦 + 𝐹𝑢)/2
 Assume yield surface below
F(𝛥)=
4𝑀(𝛥)
𝐿
𝑐𝑜𝑠2
𝜃 + 2𝑃(𝛥) · sin(𝜃)
𝑃
𝑃𝑦
+
𝑀
1.18𝑀 𝑝
= 1.0
𝑀 = 𝑀 𝑝
𝑃𝑦 = A𝐹𝑦,𝑒𝑓𝑓
𝑀 𝑝 = 𝑍𝐹𝑦,𝑒𝑓𝑓
2.1- Steel Frame Structures
• Assumption: The resistance at each point is the maximum
resistance achieved by using any pair of moment and axial
force on yield surface.
• 𝑙 𝑝 = 0.25𝑑 for WUF-B connections
• 𝑙 𝑝 = 0.6𝑑 for RBS connections
𝐹(𝛥) = ma x 4𝑀 𝛥
𝐿
𝐿2 + 𝛥2
+ 2𝑃𝑦 1 −
)𝑀(𝛥
1.18𝑀 𝑝
𝛥
𝐿2 + 𝛥2
𝐹(𝛥) =
4𝑀 𝑝
𝐿
𝐿2 + 𝛥2 + 0.3 · 𝑃𝑦
𝛥
𝐿2 + 𝛥2
, 𝛥 𝐿2 + 𝛥2 ≤ 2.353
𝑍𝐿
𝐴
2 · 𝑃𝑦
𝛥
𝐿2 + 𝛥2
, 2.353
𝑍𝐿
𝐴
< 𝛥 𝐿2 + 𝛥2 < 𝛥 𝑢
0 𝛥 ≥ 𝛥 𝑢
𝛥 𝑢 = 𝜃 𝑢
𝐿
2
= 𝜙 𝑢 𝑙 𝑝
L
2
=
ɛ 𝑢
0.5𝑑
𝑙 𝑝 𝐿
2.1- Steel Frame Component
• Experimental vs estimated results for WUF-B and RBS tests
WUF-B RBS
2.2 Concrete Frame Structures
• Following the research done by
Park:
• Deformation geometry:
 ℎ − 𝑐′
− 𝑐 = −
𝛥
2`
−
𝛽𝐿2
2𝛥
(ɛ +
2𝑡/𝐿)
• Equilibrium:
 𝐶𝑐
′
+ 𝐶𝑠
′
− 𝑇′
= 𝐶𝑐 + 𝐶𝑠 + 𝑇
• Leads to:
 𝑐′
=
ℎ
2
−
𝛥
4
−
𝛽𝑙2
4𝛥
ɛ +
2𝑡
𝑙
+
𝑇′−𝑇−𝐶 𝑠
′+𝐶 𝑠
1.7𝑓𝑐
′ 𝛽1
 𝑐 =
ℎ
2
−
𝛥
4
−
𝛽𝑙2
4𝛥
ɛ +
2𝑡
𝑙
+
𝑇′−𝑇−𝐶 𝑠
′+𝐶 𝑠
1.7𝑓𝑐
′ 𝛽1
Depth of beam available for arching
Formation of plastic hinges
C.G
Compressive
stress
Deformation diagram of AB yielded section
2.2 Concrete Frame Structures
𝛥 = 𝛥 𝑢𝛥 = ℎ − (𝑐′
+ 𝑐)/2
𝐹
𝛥
𝑀(𝛥) =
0.85𝑓𝑐
′
𝑏𝛽1 𝑐(0.5ℎ − 0.5𝛽1 𝑐) + 𝐶𝑠 (0.5ℎ − 𝑑′
) + 𝑇(𝑑 − 0.5ℎ) 𝛥 ≤ 𝑑 − (𝑐’ + 𝑐 ) 2
0 𝛥 > 𝑑 − (𝑐’ + 𝑐 ) 2
𝑃(𝛥) =
𝐶𝑐
′
+ 𝐶𝑠
′
− 𝑇′
= 𝐶 𝐶 + 𝐶𝑆 − 𝑇 𝛥 ≤ 𝑑 − (𝑐’ + 𝑐 ) 2
𝑇 + 𝑇′ 𝛥 > 𝑑 − (𝑐’ + 𝑐 ) 2
𝐹 𝛥 =
2 𝑀′ 𝛥 + 𝑀 𝛥 − 𝑃 𝛥 𝛥
𝛽𝐿
𝛥 ≤ 𝑑 − (𝑐′
+𝑐)/2
2 · 𝑃𝑦
𝛥 𝑢
𝐿2 + 𝛥 𝑢
2
𝛥 = 𝛥 𝑢
2.3 Concrete Frame Component
• Experimental vs estimated results for IMF and SMF tests
IMF SMF
2.3 Steel Gravity Frame Component
• Use Oosterhof and Driver (2016):
1- Localized deformation capacity: 𝛿 𝑚𝑎𝑥 = 0.7𝐿 𝑒
2- Calculate the rotation at initial failure, 𝜃 𝑢 using:
𝛿𝑠𝑝𝑟𝑖𝑛𝑔 = 𝛿 𝐶𝐿 + 𝑒𝑡𝑎𝑛(𝜃𝑐)
𝛿 𝐶𝐿 =
𝐿
2
(
1
cos 𝜃 𝑐
− 1)
3- Calculate the axial deformation at each bolt
location in the connection at initial failure
4- Determine the effective number of bolts in
catenary
𝑛 𝑒𝑓𝑓 =
𝐹𝑏𝑟
𝑅 𝑛
=
𝛿𝑠𝑝𝑟𝑖𝑛𝑔
𝛿 𝑦𝑖𝑒𝑙𝑑
5- Determine nominal resistance:
𝑅 𝑛 = min(0.6 2𝐿 𝑒 𝑡 𝜎 𝑦 + 𝜎 𝑢 2 , 3𝑡𝑑𝜎 𝑢,
1.5 𝐿 𝑒 −
𝑑
2
𝑡𝜎 𝑢, 0.6
𝜋𝑑2
4
𝜎 𝑢)
2.3 Steel Gravity Frame Component
6- Plot the resultant force versus rotation diagram
7- Plot force vs deformation
𝐹 = 2𝐹𝑅sin (𝛾)
Δ = L. tan(𝜃𝑐)
2.3 Steel Gravity Frame Component
• Component Example:
2.4 Flat Plates
Force
KA = Factor of two-way behavior
KB = Factor of cracking
KC = Factor of edge conditions
𝛥 = 𝐾𝐴 𝐾 𝐵 𝐾𝐶
𝜔𝑙 𝑛
4
𝐷
𝐷 =
𝐸𝑐ℎ3
12 1 − 𝜈2
1. End of elastic flexural response:
2
)(*3
l
mbcmtc 

mtc: moment capacity of
top steel in column strip
mbc: moment capacity of
bottom steel in column strip
2. End of plastic flexural response:
3. End of tensile membrane response:
𝜔 =
2𝑇𝑥 𝑠𝑖𝑛 6𝜀 𝑥
𝐿 𝑥
+
2𝑇𝑦 𝑠𝑖𝑛 6𝜀 𝑦
𝐿 𝑦
𝐿 𝑥, 𝐿 𝑦= clear span in short
and long direction
𝑇𝑥, 𝑇𝑦 = force in reinforcement
in short and long direction
𝜀 𝑥, 𝜀 𝑦= clear span in short and long direction
3 Dynamic Effects, Energy Balance
• 𝑊𝑒𝑥𝑡 = ∫ 𝐹𝑑𝑒𝑠𝑖𝑔𝑛 𝑑𝛥 =𝐹𝑑𝑒𝑠𝑖𝑔𝑛 𝛥
• 𝑊𝑖𝑛𝑡 = ∫ 𝑅 𝑛(𝛥)𝑑𝛥 =Area under pushover curve
• 𝐶𝑎𝑝𝑎𝑐𝑖𝑡𝑦 𝛥 = 𝑊𝑖𝑛𝑡 𝛥 /𝛥
3 Dynamic Effects, Energy Balance
• Steel Examples
WUF-B Subsystem RBS Subsystem
4 Simplified Analysis of Systems
• Lateral Load Resisting Column Removal in 10 Story Steel
Building
4 Simplified Analysis of Systems
• Gravity Column Removal in 10 Story Steel Building
4 Simplified Analysis of Systems
• Concrete Moment Frame-10 Story Frame or 4 Bay Slab
Conclusions
• Simple closed form formulas were presented for static force-
displacement behavior of steel and concrete moment resisting
systems and steel gravity systems.
• Dynamic effects were considered using energy balance
method.
• Building examples were analyzed using the proposed
formulas.
References
• Lew, H.S., Main, J. A., Robert, S.D., Sadek, F., Chiarito, V.P, (2013) “Performance of Steel
Moment Connections under a Column Removal Scenario. I: Experiments”, Journal of
Structural Engieering, 139:98-107.
• Oosterhof, S.A. and Driver, R.G. (2014). “Behavior of steel shear connections under
column-removal demands.” J. Struct. Eng., 141(4), 10.1061/(ASCE)ST.1943-541X.0001073,
04014126.
• Oosterhof, S.A. and Driver, R.G. (2016). “Shear connection modelling for column removal
analysis.” J. Constr.Steel Res., 117 (2), 227-242, doi:10.1016/j.jcsr.2015.10.015.
• Park, R., and Gamble, W.L., Reinforced Concrete Slabs, second edition, John Wiley & Sons,
2000, 716pp. `
• Sadek, F., Main, J.A., Lew, H.S., El-Tawil, Sh., “Performance of Steel Moment
Connections under a Column Removal Scenario. II: Analysis” , Journal of Structural
Engieering, 139:98-107.
• Sadek, F., Main, J.A., Lew, Robert, S.D., Chiarito, V.P, El-Tawil, Sh., “An Experimental
and Computational Study of Steel Moment Connections under a Column Removal
Scenario”, NIST Technical Note 1669.
• Lew, H.S., Bao, Y., Sadek, F., Main, J.A., Pujol, S., Mete, A.S., “An Experimental and
Computtaional Study of Reinforced Concrete Assemblies under a Column Removal
Scenario”, NIST Technical Note 1720.
• Uang, C.M, Ozkula, G., (2015) “Beam Plastic Hinge Length” University of California, San
Diego

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Simplified Analysis to Predict Collapse Resistance

  • 1. SIMPLIFIED ANALYSIS TO PREDICT COLLAPSE RESISTANCE April 2017 Ramon Gilsanz Akbar Mahvashmohammadi
  • 2. Participants • 2 Ramon Gilsanz Karl Rubenacker Akbar Mahvashmohammadi Joshua Peng John Abruzzo Ross Cussen Joe Gannon Nabil A. Rahman Sarah Orton Min Liu
  • 3. Contents • 1- Introduction • 2- Simplified Analysis to Components • 3- Dynamic Effects on Collapse Capacity of Components • 4- Simplified Analysis to Systems
  • 4. 1- Introduction • The objective is to develop simplified formulas to predict collapse capacity of structures:  Steel and concrete moment frames  Steel gravity frames  Flat plates • Wood, cold formed steel, and masonry are not considered in this study
  • 5. 2.1- Steel Frame Structures • Equilibrium: • Material:  Elastic perfectly plastic with effective yield stress 𝐹𝑦,𝑒𝑓𝑓 = (𝐹𝑦 + 𝐹𝑢)/2  Assume yield surface below F(𝛥)= 4𝑀(𝛥) 𝐿 𝑐𝑜𝑠2 𝜃 + 2𝑃(𝛥) · sin(𝜃) 𝑃 𝑃𝑦 + 𝑀 1.18𝑀 𝑝 = 1.0 𝑀 = 𝑀 𝑝 𝑃𝑦 = A𝐹𝑦,𝑒𝑓𝑓 𝑀 𝑝 = 𝑍𝐹𝑦,𝑒𝑓𝑓
  • 6. 2.1- Steel Frame Structures • Assumption: The resistance at each point is the maximum resistance achieved by using any pair of moment and axial force on yield surface. • 𝑙 𝑝 = 0.25𝑑 for WUF-B connections • 𝑙 𝑝 = 0.6𝑑 for RBS connections 𝐹(𝛥) = ma x 4𝑀 𝛥 𝐿 𝐿2 + 𝛥2 + 2𝑃𝑦 1 − )𝑀(𝛥 1.18𝑀 𝑝 𝛥 𝐿2 + 𝛥2 𝐹(𝛥) = 4𝑀 𝑝 𝐿 𝐿2 + 𝛥2 + 0.3 · 𝑃𝑦 𝛥 𝐿2 + 𝛥2 , 𝛥 𝐿2 + 𝛥2 ≤ 2.353 𝑍𝐿 𝐴 2 · 𝑃𝑦 𝛥 𝐿2 + 𝛥2 , 2.353 𝑍𝐿 𝐴 < 𝛥 𝐿2 + 𝛥2 < 𝛥 𝑢 0 𝛥 ≥ 𝛥 𝑢 𝛥 𝑢 = 𝜃 𝑢 𝐿 2 = 𝜙 𝑢 𝑙 𝑝 L 2 = ɛ 𝑢 0.5𝑑 𝑙 𝑝 𝐿
  • 7. 2.1- Steel Frame Component • Experimental vs estimated results for WUF-B and RBS tests WUF-B RBS
  • 8. 2.2 Concrete Frame Structures • Following the research done by Park: • Deformation geometry:  ℎ − 𝑐′ − 𝑐 = − 𝛥 2` − 𝛽𝐿2 2𝛥 (ɛ + 2𝑡/𝐿) • Equilibrium:  𝐶𝑐 ′ + 𝐶𝑠 ′ − 𝑇′ = 𝐶𝑐 + 𝐶𝑠 + 𝑇 • Leads to:  𝑐′ = ℎ 2 − 𝛥 4 − 𝛽𝑙2 4𝛥 ɛ + 2𝑡 𝑙 + 𝑇′−𝑇−𝐶 𝑠 ′+𝐶 𝑠 1.7𝑓𝑐 ′ 𝛽1  𝑐 = ℎ 2 − 𝛥 4 − 𝛽𝑙2 4𝛥 ɛ + 2𝑡 𝑙 + 𝑇′−𝑇−𝐶 𝑠 ′+𝐶 𝑠 1.7𝑓𝑐 ′ 𝛽1 Depth of beam available for arching Formation of plastic hinges C.G Compressive stress Deformation diagram of AB yielded section
  • 9. 2.2 Concrete Frame Structures 𝛥 = 𝛥 𝑢𝛥 = ℎ − (𝑐′ + 𝑐)/2 𝐹 𝛥 𝑀(𝛥) = 0.85𝑓𝑐 ′ 𝑏𝛽1 𝑐(0.5ℎ − 0.5𝛽1 𝑐) + 𝐶𝑠 (0.5ℎ − 𝑑′ ) + 𝑇(𝑑 − 0.5ℎ) 𝛥 ≤ 𝑑 − (𝑐’ + 𝑐 ) 2 0 𝛥 > 𝑑 − (𝑐’ + 𝑐 ) 2 𝑃(𝛥) = 𝐶𝑐 ′ + 𝐶𝑠 ′ − 𝑇′ = 𝐶 𝐶 + 𝐶𝑆 − 𝑇 𝛥 ≤ 𝑑 − (𝑐’ + 𝑐 ) 2 𝑇 + 𝑇′ 𝛥 > 𝑑 − (𝑐’ + 𝑐 ) 2 𝐹 𝛥 = 2 𝑀′ 𝛥 + 𝑀 𝛥 − 𝑃 𝛥 𝛥 𝛽𝐿 𝛥 ≤ 𝑑 − (𝑐′ +𝑐)/2 2 · 𝑃𝑦 𝛥 𝑢 𝐿2 + 𝛥 𝑢 2 𝛥 = 𝛥 𝑢
  • 10. 2.3 Concrete Frame Component • Experimental vs estimated results for IMF and SMF tests IMF SMF
  • 11. 2.3 Steel Gravity Frame Component • Use Oosterhof and Driver (2016): 1- Localized deformation capacity: 𝛿 𝑚𝑎𝑥 = 0.7𝐿 𝑒 2- Calculate the rotation at initial failure, 𝜃 𝑢 using: 𝛿𝑠𝑝𝑟𝑖𝑛𝑔 = 𝛿 𝐶𝐿 + 𝑒𝑡𝑎𝑛(𝜃𝑐) 𝛿 𝐶𝐿 = 𝐿 2 ( 1 cos 𝜃 𝑐 − 1) 3- Calculate the axial deformation at each bolt location in the connection at initial failure 4- Determine the effective number of bolts in catenary 𝑛 𝑒𝑓𝑓 = 𝐹𝑏𝑟 𝑅 𝑛 = 𝛿𝑠𝑝𝑟𝑖𝑛𝑔 𝛿 𝑦𝑖𝑒𝑙𝑑 5- Determine nominal resistance: 𝑅 𝑛 = min(0.6 2𝐿 𝑒 𝑡 𝜎 𝑦 + 𝜎 𝑢 2 , 3𝑡𝑑𝜎 𝑢, 1.5 𝐿 𝑒 − 𝑑 2 𝑡𝜎 𝑢, 0.6 𝜋𝑑2 4 𝜎 𝑢)
  • 12. 2.3 Steel Gravity Frame Component 6- Plot the resultant force versus rotation diagram 7- Plot force vs deformation 𝐹 = 2𝐹𝑅sin (𝛾) Δ = L. tan(𝜃𝑐)
  • 13. 2.3 Steel Gravity Frame Component • Component Example:
  • 14. 2.4 Flat Plates Force KA = Factor of two-way behavior KB = Factor of cracking KC = Factor of edge conditions 𝛥 = 𝐾𝐴 𝐾 𝐵 𝐾𝐶 𝜔𝑙 𝑛 4 𝐷 𝐷 = 𝐸𝑐ℎ3 12 1 − 𝜈2 1. End of elastic flexural response: 2 )(*3 l mbcmtc   mtc: moment capacity of top steel in column strip mbc: moment capacity of bottom steel in column strip 2. End of plastic flexural response: 3. End of tensile membrane response: 𝜔 = 2𝑇𝑥 𝑠𝑖𝑛 6𝜀 𝑥 𝐿 𝑥 + 2𝑇𝑦 𝑠𝑖𝑛 6𝜀 𝑦 𝐿 𝑦 𝐿 𝑥, 𝐿 𝑦= clear span in short and long direction 𝑇𝑥, 𝑇𝑦 = force in reinforcement in short and long direction 𝜀 𝑥, 𝜀 𝑦= clear span in short and long direction
  • 15. 3 Dynamic Effects, Energy Balance • 𝑊𝑒𝑥𝑡 = ∫ 𝐹𝑑𝑒𝑠𝑖𝑔𝑛 𝑑𝛥 =𝐹𝑑𝑒𝑠𝑖𝑔𝑛 𝛥 • 𝑊𝑖𝑛𝑡 = ∫ 𝑅 𝑛(𝛥)𝑑𝛥 =Area under pushover curve • 𝐶𝑎𝑝𝑎𝑐𝑖𝑡𝑦 𝛥 = 𝑊𝑖𝑛𝑡 𝛥 /𝛥
  • 16. 3 Dynamic Effects, Energy Balance • Steel Examples WUF-B Subsystem RBS Subsystem
  • 17. 4 Simplified Analysis of Systems • Lateral Load Resisting Column Removal in 10 Story Steel Building
  • 18. 4 Simplified Analysis of Systems • Gravity Column Removal in 10 Story Steel Building
  • 19. 4 Simplified Analysis of Systems • Concrete Moment Frame-10 Story Frame or 4 Bay Slab
  • 20. Conclusions • Simple closed form formulas were presented for static force- displacement behavior of steel and concrete moment resisting systems and steel gravity systems. • Dynamic effects were considered using energy balance method. • Building examples were analyzed using the proposed formulas.
  • 21. References • Lew, H.S., Main, J. A., Robert, S.D., Sadek, F., Chiarito, V.P, (2013) “Performance of Steel Moment Connections under a Column Removal Scenario. I: Experiments”, Journal of Structural Engieering, 139:98-107. • Oosterhof, S.A. and Driver, R.G. (2014). “Behavior of steel shear connections under column-removal demands.” J. Struct. Eng., 141(4), 10.1061/(ASCE)ST.1943-541X.0001073, 04014126. • Oosterhof, S.A. and Driver, R.G. (2016). “Shear connection modelling for column removal analysis.” J. Constr.Steel Res., 117 (2), 227-242, doi:10.1016/j.jcsr.2015.10.015. • Park, R., and Gamble, W.L., Reinforced Concrete Slabs, second edition, John Wiley & Sons, 2000, 716pp. ` • Sadek, F., Main, J.A., Lew, H.S., El-Tawil, Sh., “Performance of Steel Moment Connections under a Column Removal Scenario. II: Analysis” , Journal of Structural Engieering, 139:98-107. • Sadek, F., Main, J.A., Lew, Robert, S.D., Chiarito, V.P, El-Tawil, Sh., “An Experimental and Computational Study of Steel Moment Connections under a Column Removal Scenario”, NIST Technical Note 1669. • Lew, H.S., Bao, Y., Sadek, F., Main, J.A., Pujol, S., Mete, A.S., “An Experimental and Computtaional Study of Reinforced Concrete Assemblies under a Column Removal Scenario”, NIST Technical Note 1720. • Uang, C.M, Ozkula, G., (2015) “Beam Plastic Hinge Length” University of California, San Diego