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Frontiers of Structural and Civil Engineering

ISSN 2095-2430

ISSN 2095-2449(Online)

CN 10-1023/X

Postal Subscription Code 80-968

2018 Impact Factor: 1.272

Front. Struct. Civ. Eng.    2023, Vol. 17 Issue (2) : 165-178    https://doi.org/10.1007/s11709-022-0892-3
RESEARCH ARTICLE
Controlling interstory drift ratio profiles via topology optimization strategies
Wenjun GAO1,2(), Xilin LU1,2
1. Department of Disaster Mitigation for Structures, College of Civil Engineering, Tongji University, Shanghai 200092, China
2. State Key Laboratory of Disaster Reduction in Civil Engineering, Tongji University, Shanghai 200092, China
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Abstract

An approach to control the profiles of interstory drift ratios along the height of building structures via topology optimization is proposed herein. The theoretical foundation of the proposed approach involves solving a min–max optimization problem to suppress the maximum interstory drift ratio among all stories. Two formulations are suggested: one inherits the bound formulation and the other utilizes a p-norm function to aggregate all individual interstory drift ratios. The proposed methodology can shape the interstory drift ratio profiles into inverted triangular or quadratic patterns because it realizes profile control using a group of shape weight coefficients. The proposed formulations are validated via a series of numerical examples. The disparity between the two formulations is clear. The optimization results show the optimal structural features for controlling the interstory drift ratios under different requirements.

Keywords interstory drift ratio      aggregation function      bound formulation      min–max problem      topology optimization     
Corresponding Author(s): Wenjun GAO   
Just Accepted Date: 25 November 2022   Online First Date: 16 January 2023    Issue Date: 03 April 2023
 Cite this article:   
Wenjun GAO,Xilin LU. Controlling interstory drift ratio profiles via topology optimization strategies[J]. Front. Struct. Civ. Eng., 2023, 17(2): 165-178.
 URL:  
https://academic.hep.com.cn/fsce/EN/10.1007/s11709-022-0892-3
https://academic.hep.com.cn/fsce/EN/Y2023/V17/I2/165
Fig.1  Numerical model of the plane frame structure with a design domain for topological design. (a) Elevation view; (b) load distribution.
floor numberexterior columnsinterior columnsgirders
1W14 × 370W14 × 500W36 × 150
2W14 × 370W14 × 500W36 × 150
3W14 × 370W14 × 455W33 × 141
4W14 × 370W14 × 455W33 × 141
5W14 × 283W14 × 370W33 × 141
6W14 × 283W14 × 370W33 × 130
7W14 × 257W14 × 283W27 × 102
8W14 × 257W14 × 283W27 × 94
9W14 × 233W14 × 257W24 × 62
Tab.1  Shape information of the columns and beams used in the testing frame
shapessection area (m2)section depth (m)web thickness (m)flange width (m)flange thickness (m)
W14 × 2330.04420.40640.02720.40390.0437
W14 × 2570.04880.41660.03000.40640.0480
W14 × 2830.05370.42420.03280.40890.0526
W14 × 3700.07030.45470.04220.41910.0676
W14 × 4550.08650.48260.05130.42670.0815
W14 × 5000.09480.49780.05560.43180.0889
W24 × 620.011740.60200.01090.17880.0150
W27 × 940.017870.68330.01240.25400.0189
W27 × 1020.019350.68830.01310.25400.0211
W33 × 1300.024710.84070.01470.29210.0217
W33 × 1410.026840.84580.01540.29210.0244
W36 × 1500.028520.91190.01590.30480.0239
Tab.2  Geometry information of the beam and column shapes
Fig.2  Projected physical density fields of optimization results with flexible diaphragms under uniform profile control. (a) p =1; (b) p = 2; (c) p = 4; (d) p = 6; (e) p = 8; (f) p = 10; (g) p = 12; (h) p = 14; (i) p = 16; (j) p = 18; (k) p = 20; (l) p = 22; (m) p = 24; (n) bound formulation.
Fig.3  Projected physical density fields of optimization results with rigid diaphragms under uniform profile control. (a) p =1; (b) p = 2; (c) p = 4; (d) p = 6; (e) p = 8; (f) p = 10; (g) p = 12; (h) p = 14; (i) p = 16; (j) p = 18; (k) p = 20; (l) p = 22; (m) p = 24; (n) bound formulation.
Fig.4  Convergence histories of interstory drift ratio profiles under uniform profile control (f. d.: flexible diaphragm; r. d.: rigid diaphragm; B. F.: bound formulation). (a) f. d., p = 1; (b) f. d., p = 4; (c) f. d., p = 10; (d) f. d., p = 24; (e) f. d., B. F.; (f) r. d., p = 1; (g) r. d., p = 4; (h) r. d., p = 10; (i) r. d., p = 24; (j) r. d., B. F..
Fig.5  Iteration histories of maximum interstory drift ratio (B. F.: bound formulation). (a) Flexible diaphragm model; (b) rigid diaphragm model.
storyf. d.r. d.
13.2357353.1001
23.2357373.100101
33.2357363.100097
43.2357353.100098
53.2357363.100102
63.2357323.100103
73.2357343.100096
83.2357273.100105
93.235723.100096
Tab.3  Converged interstory drift ratios generated by bound formulation under uniform profile control (units: × 10?3)
Fig.6  Comparison of converged interstory drift ratios under uniform profile control (B. F.: bound formulation). (a) Flexible diaphragm model; (b) rigid diaphragm model.
Fig.7  Maximum interstory drift ratios achieved under different aggregation parameters (Agg. F.: aggregation formulation; B. F.: bound formulation). (a) Flexible diaphragm model; (b) rigid diaphragm model.
storytriangularquadratic
111
21.06251.2656
31.1251.5625
41.18751.8906
51.252.25
61.31252.6406
71.3753.0625
81.43753.5156
91.54
Tab.4  Shape weight coefficients for inverted triangular and quadratic distributions
Fig.8  Projected physical density fields of optimization results under inverted triangular and quadratic profile controls (f. d.: flexible diaphragm; r. d.: rigid diaphragm; T.: triangular; Q.: quadratic; B. F.: bound formulation). (a) f. d., T., p = 24; (b) f. d., T., B. F.; (c) f. d., Q., p = 24; (d) f. d., Q., B. F. (e) r. d., T., p = 24; (f) r. d., T., B. F.; (g) r. d., Q., p = 24; (h) r. d., Q., B. F..
Fig.9  Convergence histories of interstory drift profiles under inverted triangular and quadratic profile control (f. d.: flexible diaphragm; r. d.: rigid diaphragm; T.: triangular; Q.: quadratic; B. F.: bound formulation). (a) f. d., T., p = 24; (b) f. d., T., B. F.; (c) f. d., Q., p = 24; (d) f. d., Q., B. F.; (e) r. d., T., p = 24; (f) r. d., T., B. F.; (g) r. d., Q., p = 24; (h) r. d., Q., B. F..
Fig.10  Interstory drift profiles under triangular and quadratic profile control (f. d.: flexible diaphragm; r. d.: rigid diaphragm; T.: triangular; Q.: quadratic; B. F.: bound formulation; Agg.: aggregation formulation). (a) f. d., T.; (b) f. d., Q.; (c) r. d., T.; (d) r. d., Q.
profile shapeformulationprojected physical density fieldsinterstory drift ratio profiles
flexible diaphragmrigid diaphragmflexible diaphragmrigid diaphragm
uniformAgg. a)Fig.2(m)Fig.3(m)Fig.6(a)Fig.6(b)
B. F. b)Fig.2(n)Fig.3(n)
inverted triangularAgg.Fig.8(a)Fig.8(e)Fig.10(a)Fig.10(c)
B. F.Fig.8(b)Fig.8(f)
quadraticAgg.Fig.8(c)Fig.8(g)Fig.10(b)Fig.10(d)
B. F.Fig.8(d)Fig.8(h)
Tab.5  Comparison between two diaphragm models
Fig.11  Re-evaluation of optimized results using both flexible and rigid diaphragm models: (a) and (b) are based on the aggregation formulation; (c) and (d) are based on the bound formulation.
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