Technion Israel Institute of Technology

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1 Technion Israel Institute of Technology The Faculty of Civil Engineering Simultaneous Shape and Topology Optimization of Prestressed Concrete Beams Emad Shakour Oded Amir

2 Background and motivationTopology optimization has been rarely used in the field of civil engineering. The implementation of topology optimized concrete structures is a complex task comparing with traditional non optimal structures. Concrete is a highly non-linear material with almost no tensile strength. Manufacturing constraints. Economical issues. Motivation concrete … Ancient Greek building, small beam spans.

3 Background and motivationPre-stressed concrete advantages: Section remains un-cracked under service loads Increase in durability. The full section is utilized. High span-to-depth ratios. Reduction in self weight . More aesthetic appeal due to slender sections. More economical sections. Reinforced Concrete Prestressed concrete Dead load (self-weight) Prestressing cable pre-stressing force Service load 𝝈 𝒕 < 𝝈 𝒕, π’‚π’π’π’π’˜π’†π’… Reinforcing bars Un-cracked with likely small upwards deflection under dead load and pre-stress. Cracked beam. Deflection under dead and full service load. Service load = D.L + L.L Prestressed concrete concept. pre-stressing force pre-stressing force No tension β†’ No cracks. very small deflection.

4 Background and motivationπ‘ƒπ‘Ÿπ‘’π‘ π‘‘π‘Ÿπ‘’π‘ π‘ π‘–π‘›π‘” π‘π‘Žπ‘π‘™π‘’ Fig. 1 - The shape of the cable correlated to the moment diagram. Fig. 2 - The shape of the cable is restricted to a straight line in the bottom. Impossible cable shape. Possible cable shape. Topology optimization whitout prstress

5 Modeling the pre-stressed structureThe concrete domain is discretized into simple 4 node finite element with bi-linear shape functions. Linear elastic material model. 𝑻 𝒑𝒓𝒆 The continuous cable is divided into piecewise linear segments. 𝑻 𝒑𝒓𝒆 Boundary conditions Structural Model. The shape of the cable obtained by knowing the y coordinates at each junction between two adjacent segments. 𝑻 𝒑𝒓𝒆 βˆ’Cable tension force π‘·βˆ’Equivalent prestress forces, due to different inclination angle between two adjacent cable segments.

6 Pre-stressing forces (1) 𝑃 𝑖 - equivalent prestressing load.(2) 𝑃 𝑖,π‘₯ , P i,y calculated through equilibrium equation. 𝒅 𝟐 𝒅 𝟏 Structural Model. (3) The equivalent prestressing load is transferred to the joints through linear interpolation. 𝑻 𝒑𝒓𝒆 βˆ’Cable tension force π‘·βˆ’Equivalent prestress forces, due to different inclination angle between two adjacent cable segments.

7 Formulation – shape optimization for the cable only𝑃 𝑒π‘₯𝑑 Only for verification purposes min 𝑦 πœ™ 𝑦 = 𝒇 𝑒π‘₯𝑑 𝑇 𝒖 π‘‡π‘œπ‘‘π‘Žπ‘™ 𝑠.𝑑: 𝑦 𝑖 βˆ’β„Ž+𝑐≀ 𝑖=1,…, 𝑁 πΆπ‘Žπ‘π‘™π‘’ π‘›π‘œπ‘‘π‘’π‘  βˆ’ 𝑦 𝑖 +𝑐≀ 𝑖=1,…, 𝑁 πΆπ‘Žπ‘π‘™π‘’ π‘›π‘œπ‘‘π‘’π‘  π‘€π‘–π‘‘β„Ž: 𝑲 𝒖 π‘‡π‘œπ‘‘π‘Žπ‘™ = 𝒇 𝑒π‘₯𝑑 + 𝒇 π‘π‘Ÿπ‘’ 𝒖 π‘‡π‘œπ‘‘π‘Žπ‘™ = 𝒖 𝑓 𝑒π‘₯𝑑 + 𝒖 𝑓 π‘π‘Ÿπ‘’ β„Ž βˆ’π΅π‘’π‘Žπ‘š β„Žπ‘’π‘–π‘”β„Žπ‘‘ 𝑐 βˆ’πΆπ‘œπ‘›π‘π‘Ÿπ‘’π‘‘π‘’ π‘π‘œπ‘£π‘’π‘Ÿ Expected solution 𝑓 𝑒π‘₯𝑑 𝛿 + = 0 Expected solution 𝑐 Formulation for cable only. π‘­π’†π’‚π’”π’Šπ’ƒπ’π’† π’π’π’„π’‚π’•π’Šπ’π’ 𝒐𝒇 𝒕𝒉𝒆 𝒄𝒂𝒃𝒍𝒆 𝑦 𝑖 β„Žβˆ’2𝑐 𝑦 𝑐 π‘₯

8 Formulation – shape optimization combined with topology optimizationmin 𝜌,𝑦 πœ™ 𝜌,𝑦 = 𝒇 𝑒π‘₯𝑑 𝑇 𝒖 π‘‡π‘œπ‘‘π‘Žπ‘™ 𝑠.𝑑: 𝑒=1 𝑁 π‘’π‘™π‘’π‘š 𝜌 𝑑 (𝜌) 𝑁 π‘’π‘™π‘’π‘š βˆ’ 𝑉 βˆ— ≀0 (Concrete volume fraction) 0< 𝜌 π‘šπ‘–π‘› β‰€πœŒβ‰€1 𝑦 𝑖 βˆ’β„Ž+𝑐≀ 𝑖=1,…, 𝑁 πΆπ‘Žπ‘π‘™π‘’ π‘›π‘œπ‘‘π‘’π‘  βˆ’ 𝑦 𝑖 +𝑐≀ 𝑖=1,…, 𝑁 πΆπ‘Žπ‘π‘™π‘’ π‘›π‘œπ‘‘π‘’π‘  π‘€π‘–π‘‘β„Ž: 𝑲 ( 𝜌 𝑒 , 𝑦 𝑖 )𝒖 π‘‡π‘œπ‘‘π‘Žπ‘™ = 𝒇 𝑒π‘₯𝑑 + 𝒇 π‘π‘Ÿπ‘’ Design variables: 𝒖 π‘‡π‘œπ‘‘π‘Žπ‘™ = 𝒖 𝑓 π‘π‘Ÿπ‘’ + 𝒖 𝑓 𝑒π‘₯𝑑 β„Ž βˆ’π΅π‘’π‘Žπ‘š β„Žπ‘’π‘–π‘”β„Žπ‘‘ 𝑐 βˆ’πΆπ‘œπ‘›π‘π‘Ÿπ‘’π‘‘π‘’ π‘π‘œπ‘£π‘’π‘Ÿ Concrete element densities according to SIMP. Y coordinates of the cable. The volume constraint is added. Formulation for cable an concrete. π‘­π’†π’‚π’”π’Šπ’ƒπ’π’† π’π’π’„π’‚π’•π’Šπ’π’ 𝒐𝒇 𝒕𝒉𝒆 𝒄𝒂𝒃𝒍𝒆 𝑐 β„Žβˆ’2𝑐 π‘₯ 𝑦 𝑦 𝑖 ? ? (BendsΓΈe 1989, Sigmund and Torquato 1997)

9 Filters and projections (1)β†’ 𝜌 𝜌 𝑒 𝜌 𝑑 Density filter Cable filter Dilated/Eroded Design variable 1. Density filter 𝜌 𝑖 = π‘—βˆˆ 𝑁 𝑖 𝑀 𝜌 𝑗 𝜌 𝑖 π‘—βˆˆ 𝑁 𝑖 𝑀 𝜌 𝑗 2. Cable filter - filter that insures covering the cable. 𝜌 𝑖 = 𝜌 𝑖 + 1βˆ’ 𝜌 𝑖 𝑒 βˆ’ 𝑑 𝑒𝑗 𝛽 𝑓𝑖𝑙 6 If an element is close enough to the cable his density is modified to 1. If not, the density remains the same. 2 𝛽 𝑓𝑖𝑙 𝑑 𝑒𝑗 𝜌 𝜌 =0.8 𝛽 𝑓𝑖𝑙 =4 Filters. To decrease the font size. To prepare beautiful graphs in MATLAB. Finish this slide. (Bruns and Tortorelli 2001; Bourdin 2001; Guest et al. 2004; Xu et al. 2010)

10 Filters and projections (2)β†’ 𝜌 𝜌 𝑒 𝜌 𝑑 Density filter Cable filter Dilated/Eroded Design variable 3. Projection function: 0.5 𝜌 𝑖,𝑒 = π‘‘π‘Žπ‘›β„Ž 𝛽 πœ‚ 𝑒 + π‘‘π‘Žπ‘›β„Ž 𝛽 𝜌 𝑖 βˆ’ πœ‚ 𝑒 π‘‘π‘Žπ‘›β„Ž 𝛽 πœ‚ 𝑒 + π‘‘π‘Žπ‘›β„Ž 𝛽 1βˆ’ πœ‚ 𝑒 𝜌 𝑖,𝑑 = π‘‘π‘Žπ‘›β„Ž 𝛽 πœ‚ 𝑑 + π‘‘π‘Žπ‘›β„Ž 𝛽 𝜌 𝑖 βˆ’ πœ‚ 𝑑 π‘‘π‘Žπ‘›β„Ž 𝛽 πœ‚ 𝑑 + π‘‘π‘Žπ‘›β„Ž 𝛽 1βˆ’ πœ‚ 𝑑 πœ‚ 𝑒 =0.6 πœ‚ 𝑑 =0.4 Using the dilated/eroded formulation, allows determining a minimum length scale in the optimal design. Filters. To decrease the font size. To prepare beautiful graphs in MATLAB. Finish this slide. (Wang et al. 2011; Lazarov et al. 2016)

11 πœ™ = 𝑓 𝑒π‘₯𝑑 𝑇 𝑒 2 +πœ† π‘²π’–βˆ’ 𝒇 𝑒π‘₯𝑑 βˆ’ 𝒇 π‘π‘Ÿπ‘’ =πœ™Sensitivity analysis πœ™ 𝜌,𝑦 = 𝒇 𝑒π‘₯𝑑 𝑇 𝒖 π‘‡π‘œπ‘‘π‘Žπ‘™ 2 𝑔 π‘₯ = 𝑒=1 𝑁 π‘’π‘™π‘’π‘š 𝜌 𝑑 (𝜌) 𝑁 π‘’π‘™π‘’π‘š βˆ’ 𝑉 βˆ— ≀0 β†’ 𝑑𝑔 π‘‘πœŒ , 𝑑𝑔 𝑑𝑦 The derivatives of volume constraint are straightforward using the chain rule. The derivatives of the objective function πœ™ are computed using the adjoint method. πœ™ = 𝑓 𝑒π‘₯𝑑 𝑇 𝑒 2 +πœ† π‘²π’–βˆ’ 𝒇 𝑒π‘₯𝑑 βˆ’ 𝒇 π‘π‘Ÿπ‘’ =πœ™ β†’ 𝑑 πœ™ π‘‘πœŒ , 𝑑 πœ™ 𝑑𝑦 𝑋 𝐢𝑀 , π‘Œ 𝐢𝑀 𝑦 𝑗,2 𝑦 𝑗,1 𝑗 𝑑 𝑒𝑗 𝜌 𝑖 = 𝜌 𝑖 + 1βˆ’ 𝜌 𝑖 𝑒 βˆ’ 𝑑 𝑒𝑗 𝛽 𝑓𝑖𝑙 6 𝑑 𝑒𝑗 =𝑑𝑖𝑠𝑑 𝑋 𝐢𝑀 , π‘Œ 𝐢𝑀 , 𝑦 𝑗,1 , 𝑦 𝑗,2 𝑑 𝜌 𝑖 𝑑 𝑦 𝑗,π‘˜ = 𝑑 𝜌 𝑖 𝑑 𝑑 𝑒𝑗 𝑑 𝑒𝑗 𝑑 𝑦 𝑗,π‘˜ Topology design variables Shape design variables The derivative of the topology according to the distance The derivative of the distance according to the shape β†’ 𝜌 𝜌 𝑒 𝜌 𝑑 Density filter Cable filter Dilated/Eroded Design variable 𝜌 𝑖 Here because of the cable filter, we have a correlation between the topology and the shape design variables trough the distance dej which is a function of the concrete element centroid and the y coordinates of the cable. An then we can calculate the derivative of the topology according to the shape by the chain rule using this expression.

12 Examples – Shape Optimization OnlySimply supported beam Nelx=416; Nely=40; 52 Cable segments Prestressing force 𝑇 π‘π‘Ÿπ‘’ = 𝑇 π‘π‘Ÿπ‘’ ( 𝜎 𝑑 =0); 𝑃 𝑒π‘₯𝑑 π‘ƒπ‘œπ‘–π‘›π‘‘ π‘™π‘œπ‘Žπ‘‘ 𝑓 𝑒π‘₯𝑑 π·π‘–π‘ π‘‘π‘Ÿπ‘–π‘π‘’π‘‘π‘’π‘‘ π‘™π‘œπ‘Žπ‘‘ πΌπ‘‘π‘’π‘Ÿ. 𝑂𝑏𝑗𝑒𝑐𝑑𝑖𝑣𝑒 𝑃 𝑒π‘₯𝑑 π‘ƒπ‘œπ‘–π‘›π‘‘ π‘™π‘œπ‘Žπ‘‘ 𝑓 𝑒π‘₯𝑑 π·π‘–π‘ π‘‘π‘Ÿπ‘–π‘π‘’π‘‘π‘’π‘‘ π‘™π‘œπ‘Žπ‘‘ 25-30 Iterations to zero displacement Parabolic Nelx=416; Nely=40; Linear Nelx=416; Nely=40;

13 Examples – Shape Optimization Onlyoptimal shapes for different prestressing force 𝑇 π‘π‘Ÿπ‘’ 0 =1.0 𝑇 π‘π‘Ÿπ‘’ ( 𝜎 𝑑 =0); 1.5 𝑇 π‘π‘Ÿπ‘’ 0 1.0 𝑇 π‘π‘Ÿπ‘’ 0 0.75 𝑇 π‘π‘Ÿπ‘’ 0 0.5 𝑇 π‘π‘Ÿπ‘’ 0 𝑇 π‘π‘Ÿπ‘’ =1.5 𝑇 π‘π‘Ÿπ‘’ ( 𝜎 𝑑 =0); 𝑇 π‘π‘Ÿπ‘’ =1.0 𝑇 π‘π‘Ÿπ‘’ ( 𝜎 𝑑 =0); 𝑇 π‘π‘Ÿπ‘’ =0.75 𝑇 π‘π‘Ÿπ‘’ ( 𝜎 𝑑 =0); 𝑇 π‘π‘Ÿπ‘’ =0.5 𝑇 π‘π‘Ÿπ‘’ ( 𝜎 𝑑 =0);

14 Examples – Shape and topology Optimization𝑓 𝑒π‘₯𝑑 π‘ƒπ‘Ÿπ‘’π‘ π‘‘π‘Ÿπ‘’π‘ π‘ π‘’π‘–π‘›π‘” π‘π‘Žπ‘π‘™π‘’ 𝑛𝑒𝑙𝑦=40 𝑛𝑒𝑙π‘₯=416 𝑛𝑒𝑙𝑦 𝑛𝑒𝑙π‘₯ β‰…1:10 πΌπ‘‘π‘’π‘Ÿ. 𝑂𝑏𝑗𝑒𝑐𝑑𝑖𝑣𝑒 Cons. convergence Implemented Continuation Schemes π‘‰π‘œπ‘™π‘“π‘Ÿπ‘Žπ‘.=0.55 Iter. 𝛽 𝛽 𝑓𝑖𝑙𝑙 𝑝 𝐸 1-40 1 40-70 2 70-110 4 3 𝑇 π‘π‘Ÿπ‘’ 0.55 =0.2 𝑇 π‘π‘Ÿπ‘’ 1 ( 𝜎 π‘‘π‘’π‘›π‘ π‘–π‘œπ‘› =0); 𝑇 π‘π‘Ÿπ‘’ π‘‰π‘œπ‘™π‘“π‘Ÿπ‘Žπ‘

15 Examples – Shape and topology Optimizationoptimal prestressing design Fig. 1 normal stresses distribution only 𝑓 𝑒π‘₯𝑑 is applied 𝑓 𝑒π‘₯𝑑 + 𝑓 π‘π‘Ÿπ‘’ is applied – final design Compression normal stress Tensile normal stress Fig. 2 No tension stress Fig. 3

16 Prestressed Concrete – More ExamplesStatically indetermined structures ` 𝑛𝑒𝑙π‘₯1=208 𝑛𝑒𝑙𝑦=40

17 Prestressed Concrete – More ExamplesMulti-span bridge ` Distributed load Design domain Covered pre-stressing cable Volfrac=0.55 Zero deflection 𝑛𝑒𝑙π‘₯1=300 𝑛𝑒𝑙π‘₯2=370 𝑛𝑒𝑙π‘₯3=340 𝑛𝑒𝑙π‘₯2=370 𝑛𝑒𝑙π‘₯1=300 𝑛𝑒𝑙𝑦=50

18 Summary An new procedure for top. opt. of prestressed concrete structures is proposed. Simultaneous shape optimization of the cable and topology optimization of the concrete. Special filter is developed to insure cover of the prestressing cable with concrete. Focus on prestressed concrete allows the use of linear-elastic modelling. The obtained designs represent efficient and aesthetic structures, which can be used for conceptual design by architects and engineers. Possible practical applications: prestressed concrete bridges, slabs, bracing systems. Future work: Extend to 3-D Constrain tensile cracking stresses Embed code requirements: interaction, relaxation, creep

19 Acknowledgments Thank youThis research was funded by the European Commission Research Executive Agency, grant agreement PCIG12-GA Thank you