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Form-Finding of Long Span Bridges with Continuum Topology Optimization and a Buckling Criterion Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan (Adviser) Department of Civil and Environmental Engineering Center for Computer-Aided Design The University of Iowa

Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

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Page 1: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Form-Finding of Long Span Bridges with Continuum Topology Optimization

and a Buckling Criterion

Salam Rahmatalla (Graduate Student)Prof. Colby C. Swan (Adviser)

Department of Civil and Environmental EngineeringCenter for Computer-Aided Design

The University of Iowa

Page 2: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Objective Statement

To develop a continuum topology formulation capable of finding structural forms of maximum buckling stability.

Page 3: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Introduction Structural Optimization

. Size Optimization

. Shape Optimization

. Topology Optimization

Page 4: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Alternative Topology Optimization Formulations

Continuum topology optimizationDiscrete topology optimization(Ground structures)

Page 5: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Applied loads

SupportsStarting Design domain

Elements of Continuum topology optimization

numnp

i ii 1

( ) N ( )φ φ=

= ∑X X

( ) 0φ =X

0 ( ) 1.0φ≤ ≤X

Intermediate design

( ) 1.0φ =X

( )( ) rule] [mixing )( XX φEE =

Page 6: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Sparsity of Long-Span Bridges

Sunshine Skyway bridge cable-stayed bridge in Tampa, Florida

Akashi Bridge suspension bridge In Japan

Most long-span bridges occupy < 1% of their envelope volume.

Page 7: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

SPARSITY in Topology Optimization

• Fixed-mesh model of full envelope volume;• must capture the form of the structure with realistic sparsity• must capture mechanical performance of the structure

• Fine meshes are required;• Implies large computational expense;

50% Material constraint usage 10% Material constrain usage 3% Material constraint usage

40 elements 100 elements 224 elements

20 elements 50 elements 224 elements

Page 8: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

• Structure modeled as linearly elastic system

• Stability analysis performed via linearized buckling analysis

• Linear elastic problem:

• Eigenvalue problem:

• Objective function:

• Design sensitivity analysis:

tL

exfuK =⋅

0ψbuGψbKL =+ ),()( λ

)min(1),(λ

=buL

).()()1(bfu

bKuψ

bK

bGψ

bLL

∂∂

−∂∂

+∂∂

+∂∂

−=ext

TaT

ddL

λ

GψψψKψ L

T

T

−=λ

a T ∂=∂LGK u ψ ψu

Page 9: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Design Constraints

• Bounds on individual design variables

• Material usage constraint

J0 1 J 1,2, ,NUMNPφ≤ ≤ = K

( ) d

dC

φΩ

Ω

Ω≤

Ω

X

Page 10: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Gradient-basedOptimizationAlgorithm

Optimal?

Initialization Starting guess

Structural analysisFind u(b) and λ(b)

Sensitivity analysis (Linearization)

Optimization step(Linear programming sub-problem)

Stop

YesNo

Page 11: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Fix-end Beam Problem

Maximizing the min.critical buckling load,

nonlinear formulation.

Maximizing the min.critical buckling load,linearized buckling.

Minimizing thegeneral compliance.

d FF

Design domainwith 10% materialconstraint.

Resulting topology

First bucklingmode.

65.09*10Π =61.496*10Π =

10.0λ = 19.51λ =

Page 12: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Design domainWith material 2.5% Constraint

Minimizing structuralCompliance

Maximizing the min.critical buckling load,linearized buckling.

Circle Problem

Undeformed configuration

Deformed configuration

52.66*10Π =54.09*10Π =

91.57*10λ = 93.28*10λ =

Page 13: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

100m

300m

1000m

80 elements

200 elements 200 elements

80 elements

Canyon Bridge ProblemDesign domainWith 12.5% material Constraint and 10 kPaapplied load.

Minimizing the general compliance

Maximizing the min.critical buckling load,linearized buckling.

Maximizing the min.critical buckling load,linearized buckling.(Non-designable deck)

31.7*10Π =

41*10Π =

32.49*10Π =

34.84*10λ =

33.88*10λ =

36.98*10λ =

Page 14: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

50 elements

3000m

375m 375m

200m

(a)

200 elements

50 elements

(b)

(c)900 elements

60 elements

(d)200 elements

Long-Span Bridge Problem “2-Supports”

Design domain with 12.5% material constraintand 10 kPa applied load.

Compliance Minimization

Compliance Minimization(finer mesh)

Optimimum linearized bucklingstability

52.92*10Π =58.3λ =

412λ =

63.16*10Π =

Page 15: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

150m375m 375m

3000m

250m

200 elements

50 elements

200 elements

50 elements

Long-Span Bridge Problem “3-Supports”

51.52*10Π =

42.06*10Π =

35.15*10λ =

25.29*10λ =

Design domain with 12.5% material constraintand 10 kPa applied load.

Compliance Minimization

Optimimum linearized bucklingstability

Page 16: Salam Rahmatalla (Graduate Student) Prof. Colby C. Swan ...user.engineering.uiowa.edu/~swan/presentations/topo_buckling_Seattle.pdfSalam Rahmatalla (Graduate Student) Prof. Colby C

Summary & Conclusion

• A formulation has been developed and tested for form-finding of large-scale sparse structures;

• The formulation is based on linearized buckling analysis;

• The structural form and topology are optimized to achieve maximum buckling stability;

• The formulation yields “concept designs” that resemble existinglarge-scale bridge structures;