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Ultimate Strength Analysis of Arbitrary Cross Sections under Biaxial Bending and Axial Load by Fiber Model and Curvilinear Polygons Aristotelis Charalampakis.

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Presentation on theme: "Ultimate Strength Analysis of Arbitrary Cross Sections under Biaxial Bending and Axial Load by Fiber Model and Curvilinear Polygons Aristotelis Charalampakis."— Presentation transcript:

1 Ultimate Strength Analysis of Arbitrary Cross Sections under Biaxial Bending and Axial Load by Fiber Model and Curvilinear Polygons Aristotelis Charalampakis and Vlasis Koumousis National Technical University of Athens Institute of Structural Analysis and Aseismic Research

2 National Technical University of Athens
Problem definition Task: Analysis of arbitrary cross sections under biaxial bending and axial load Using a “fiber model” based on the Bernoulli – Euler assumption: Simple calculation of strains (plane sections remain plane) Used in Design Codes Close agreement with experimental results for monotonic / proportional loading Moment – curvature diagram, interaction curves and failure surfaces can be used in non-linear analyses

3 Cross Section Arbitrary Cross Section
National Technical University of Athens Cross Section Arbitrary Cross Section defined by curvilinear polygons (i.e. polygons with edges that may be straight lines or arcs) the polygons can be nested to any depth

4 Materials Custom material data Additional data: max or min strain, etc
National Technical University of Athens Materials Custom material data Stress - strain diagram composed of any number and any combination of consecutive linear, parabolic or cubic segments Additional data: max or min strain, etc

5 National Technical University of Athens
Materials Materials “Foreground” and “Background” materials for each curvilinear polygon. Positive “Foreground” / Negative “Background” material stresses

6 Calculations Deformed plane Angle θ Curvature k Strain ε0
National Technical University of Athens Calculations Deformed plane Angle θ Curvature k Strain ε0

7 Calculations Neutral axis is parallel to horizontal axis Y:
National Technical University of Athens Calculations Direction of neutral axis (angle θ) is imposed by the algorithm By rotating the cross section by this angle θ, strains (and stresses) vary only in vertical axis Z: Neutral axis is parallel to horizontal axis Y:

8 Calculations Trapezoidal decomposition of curvilinear polygons
National Technical University of Athens Calculations Trapezoidal decomposition of curvilinear polygons Basic set of curvilinear trapezoids calculated only once per angle θ

9 Calculations Basic integrals
National Technical University of Athens Calculations Basic integrals Basic integrals calculated only once per curvilinear trapezoid

10 Calculations Stress resultants for a curvilinear trapezoid
National Technical University of Athens Calculations Stress resultants for a curvilinear trapezoid Cubic stress – strain segment (αi material constants). Strain distribution in current deformed plane (θ fixed). Basic integrals Ij(m,n) have already been calculated. Independent of k, ε0. Summation over the trapezoids produces the overall stress resultants.

11 Moment – Curvature diagram (1)
National Technical University of Athens Moment – Curvature diagram (1) Initialization Pick neutral axis direction (angle θ) Pick initial curvature step Rotate cross section Decompose into curvilinear trapezoids Calculate basic integrals Ij(m,n)

12 Moment – Curvature diagram (2)
National Technical University of Athens Moment – Curvature diagram (2) Calculate initial ε0 for axial equilibrium with no curvature

13 Moment – Curvature diagram (3)
National Technical University of Athens Moment – Curvature diagram (3) Neutral Axis Δk In a loop, apply a small increase in curvature...

14 Moment – Curvature diagram (4)
National Technical University of Athens Moment – Curvature diagram (4) Neutral Axis … and find new ε0 using Van Wijngaarden – Dekker – Brent method

15 Moment – Curvature diagram (5)
National Technical University of Athens Moment – Curvature diagram (5) Decrease curvature step when necessary (close to failure) Continue up to failure to produce the full moment – curvature diagram

16 National Technical University of Athens
Interaction curve The interaction curve is produced by repeating the previous procedure for different directions of neutral axis (angle θ)

17 Calculation of Deformed Plane
National Technical University of Athens Calculation of Deformed Plane Calculation of deformed configuration of a cross section under given external loads N, MYc, MZc Trial-and-error procedure All paths of the analyses stem from (M0Yc, M0Zc ) (Bending moments for axial equilibrium with no curvature)

18 Example 1 EC2 design charts Equal reinforcement, top and bottom
National Technical University of Athens Example 1 EC2 design charts Rectangular cross section Equal reinforcement, top and bottom Steel grade S500 d1/h = 0.10 Calculations for : ω = 0.00, 0.50, 1.00, 1.50, and various axial load levels

19 Example 2 Analysis with MyBiAxial 2.0 Arbitrary cross section
National Technical University of Athens Example 2 Arbitrary cross section Analysis with MyBiAxial 2.0

20 Example 2 Interaction curve for N = -4120kN Complete failure surface
National Technical University of Athens Example 2 Interaction curve for N = -4120kN Complete failure surface

21 3D view of proposed connection
National Technical University of Athens Example 3 Bolted connection 3D view of proposed connection

22 Stress solids in CAD software
National Technical University of Athens Example 3 Bolted connection Example 3 in MyBiAxial 2.0 Stress solids in CAD software

23 Example 4 Moment capacity of rigid footing
National Technical University of Athens Example 4 Moment capacity of rigid footing

24 Example 4 Moment capacity of rigid footing
National Technical University of Athens Example 4 Moment capacity of rigid footing

25 Conclusions Custom material data
National Technical University of Athens Conclusions Generic algorithm for the analysis of arbitrary cross sections under biaxial bending and axial load Features: Custom material data Curved graphical objects with analytical expressions instead of approximations with simple polygons or dimensionless fibers for the reinforcement bars Construction of full bending moment – curvature diagram Fast, very stable algorithm Can be used for a variety of purposes as demonstrated in the examples


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