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8/10/2019 toptology optimixation
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Slide 4a.1Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Your specifications for a stiff structure
Distributed ramp force
Point forceFixed
FixedUse 40 % material that can fit intothis rectangle
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Slide 4a.2Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Stiff structure for your specifications
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Slide 4a.3Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Your specifications for thecompliant mechanism
Hole
Fixed
Fixed
Input force
Outputdeflection
Use 30 % material
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Slide 4a.4Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Compliant mechanismto your specifications
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Slide 4a.5Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Lecture 4aDesign parameterization instructural optimization
Various ways of defining design variables for size,shape, and topology optimization schemes.
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Slide 4a.6Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Contents Hierarchical description of the physical
form of a structure Topology Shape Size
Size (dimensional, parameter) optimization Shape optimization Topology optimization
Ground structure method
Homogenization method Power law, and SIMP methods Micro-structure based models peak function
Level-set methods
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7/35Slide 4a.7Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Hierarchical description of the physicalform of a structure Topology or layout
Connectivity among portions of interest
force
force
support
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8/35Slide 4a.8Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Topology or layout (contd.)Number of holes in the design domain
also determine the connectivityforce
force
support
Topology orlayout design
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9/35Slide 4a.9Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Hierarchical description of a physicalform of structure: Shape
Shape design
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10/35Slide 4a.10Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Hierarchical description of a physicalform of structure: Size
1R
1w
2R
1R
1R
2w
t = thickness
When the topology and shape are selected, one canoptimize by varying size related parameters such asdimensions.
Dimensional orparametric orsize design
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11/35Slide 4a.11Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Stiffest structure for thesespecifications for a given volume
60x40=2400
120x80=9600
30x20=600 elements
Results given by PennSyn program for
Volume = 40%
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12/35Slide 4a.12Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Design parameterization In order to optimize topology (layout), shape, or
size, we need to identify optimization variables.This is called the design parameterization.
Size optimization
Thickness, widths, lengths, radii, etc. Shape optimization Polynomials Splines
Bezier curves, etc. Topology optimization
We will discuss in detail
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13/35Slide 4a.13Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Ground structure with truss elementsDefine a grid of joint locations and connect them in allpossible ways with truss elements so that all the lementslie within the design region.
Associated with each truss element, define a c/s areavariable. This leads to N optimization variables.
Each variable has lower (almost zero) and upper bounds.
Ground structure A possible solution
Kirsch, U. (1989). Optmal Topologies of Structures. Applied Mechanics Reviews42(8):233-239.
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14/35Slide 4a.14Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Ground structures with beam elements
Overlapping beam elements are avoided because they createcomplications in practical realization of the designs.Realizable slopes are limited but it does not matter in most
cases.Again, each element has a design variable related to its cross-section.
Saxena, A., Ananthasuresh, G.K., On an optimal property of compliant topologies, Structural andMultidisciplinary Optimization, Vol. 19, 2000, pp. 36-49.
d l
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15/35Slide 4a.15Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Continuum modeling:the homogenization-based method
At each point, we need to interpolate the materialbetween 0 and 1 in order to do optimization.
Three optimizationvariables per element:a, b, and q.
ab
q
Each element is imagined to bemade of a composite materialwith microstructural voids.
Bendse, M.P., and Kikuchi, N. (1988). Generating optimal topologies in structural design using a
homogenization method. Computer Methods in Applied Mechanics and Engineering71:197-224.
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16/35Slide 4a.16Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Homogenization-based method (contd.)
Material with microstructure Homogeneous material withequivalent properties
Homogenization
a b q
Homogenizedpr
operty
Homogenizedpr
operty
Homogenizedpr
operty
Relevant homogenized properties are pre-computed andfitted to smooth polynomials for ready interpolation.
h i b d
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17/35Slide 4a.17Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Another microstructure basedmethodThe original homogenization-based method used three
variables to get some anisotropicy (orthotropy, inparticular). But practical considerations mostly needisotropic materials.
Assume isotropic (sphericalinclusions)
Volume fraction =
Gea, H. C., 1996, Topology Optimization: A New Micro-Structural Based Design Domain Method, Computers
and Structures, Vol. 61, No. 5, pp. 781 788.
02
EE
Youngs modulus =
Fi i i d i h d
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18/35Slide 4a.18Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Fictitious density method; powerlaw model
Fictitious density approach
10with0 EE
SIMP (Solid Isotropic Material with Penalty)
10with0 EE p
pis the penalty parameter to push densitiestoblack (1) andwhite (0).
For optimization, there will be as many as thenumber of elements in the discretized model.
s'
Rozvany, G.I.N. , Zhou, M., and Gollub, M. (1989). Continuum Type Optimality Criteria Methods for LargeFinite Element Systems with a Displacement Connstraint, Part 1. Structural Optimization1:47-72.
P l i h SIMP
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19/35Slide 4a.19Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Penalty parameter in the SIMPmethod: some justification
230
0
E
E
23
00
EEp
Therefore,
3 p
Hashin-Shtrikman bounds
Bendse, M.P. and Sigmund, O., Material Interpolation Schemes in Topology
Optimization, Archives in Applied Mechanics, Vol. 69, (9-10), 1999, pp. 635-654.
Mi t t f i t di t
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20/35Slide 4a.20Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Microstructure for intermediatedensities
Bendse, M.P. and Sigmund, O., Material Interpolation Schemes in Topology
Optimization, Archives in Applied Mechanics, Vol. 69, (9-10), 1999, pp. 635-654.
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21/35Slide 4a.21Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Multiple-material interpolation
22
22
21
21
2
2
2
1
eEeEE
0E
E
0 0.5 1 0 0.5 1 0 0.5 1
21112 )1( EEE For two-materials, in the SIMP method, two variables are needed.
Alternativelywith just one variable, manymaterials can be interpolated.
Yin, L. and Ananthasuresh, G.K., Topology Optimization of Compliant Mechanisms with Multiple MaterialsUsing a Peak Function Material Interpolation Scheme, Structural and Multidisciplinary Optimization, Vol.
23, No. 1, 2001, pp. 49-62.
Ad t f th k f ti b d
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22/35Slide 4a.22Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Advantages of the peak function basedprobabilistic material interpolation
22
22
21
21
2
2
2
1
eEeEE
1E
2E
E
1
1
Begin with large s and graduallydecrease to get peaks eventually.
voidi
N
i
EeEE ii
2
2
2
1
No bounds on the variables!
P k f ti th d f b ddi
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Slide 4a.23Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Peak function method for embeddingobjects
Embedded
objects
Connecting structure
Traction forceson GT
Fixedboundary
W
G
n
iiEEyxE
10
),(
i
i
ii
ii
i
i
yi
i
xi
iii
yy
xx
y
x
yxEE
EE
cossin
sincos
~
~
~~exp
exp
22
2
2
00
Z. Qian and G. K. Ananthasuresh, Optimal Embedding inTopology Optimization, CD-ROM proc. of the IDETC-2002,
Montreal, CA, Sep. 29-Oct. 2, 2002, paper #DAC-34148.
Contours (level set curves)
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Slide 4a.24Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Level-set method
A very powerful method for topology optimization.The boundary defined as the level set of a surface definedon the domain of interest. Zero level set curve definesthe boundary, while positive surface values define the
interior of the region.
W
GW
WW
\0)(
0)(
\0)(
Dxx
dxx
dxx
Interior
Boundary
Exterior
D W
M. Y. Wang, X. M. Wang, and D. M. Guo, A Level Set Method for Structural Topology Optimization,
Computer Methods in Applied Mechanics and Engineering, 192 (1), pp. 227-246, 2003.
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Slide 4a.25Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Level set method for multiple materials
Multiple materials can be dealt with more level set surfaces.
n n2With level set surfaces, materials can be exclusivelychosen.
Two level sets and four materials Three level sets and eight materials
M. Y. Wang, personal communication, 2003.
312
4
56
78
2
34
1
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Slide 4a.26Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Main points
Topology, shape, and size provide ahierarchical description of the geometry ofa structure.
Different smooth interpolations
techniques for topology optimization SIMP is widely used Peak function based probabilistic
interpolation method can easily handle
multiple materials with few variables Level-set method provides a larger design
space
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Slide 4a.27Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Your specifications for a stiff structure
Distributed ramp force
Point forceFixed
FixedUse 40 % material that can fit intothis rectangle
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Slide 4a.28Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Stiff structure for your specifications
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Slide 4a.29Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Optimal synthesis solution
Solved with 96x48 = 4608variables in the optimization problem.
Actual time taken on this laptop = ~10 minutes
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Slide 4a.30Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Designs with different mesh sizes
96x48 = 4608 elements
72x36 = 2592 elements
48x24 = 1152 elements
24x12 = 288 elements
Your specifications for the
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Slide 4a.31Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Your specifications for thecompliant mechanism
Hole
Fixed
Fixed
Input force
Outputdeflection
Use 30 % material
Compliant mechanism
8/10/2019 toptology optimixation
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Slide 4a.32Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Compliant mechanismto your specifications
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Slide 4a.33Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
A rigid-body mechanism (if you want)
Optimal compliant mechanism
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Slide 4a.34Stiff Structures, Compliant Mechanisms, and MEMS: A short course offered at IISc, Bangalore, India. Aug.-Sep., 2003. G. K. Ananthasuresh
Optimal compliant mechanismto your specifications
Compliant designs for different
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Compliant designs for differentmesh sizes
Rough mesh Medium mesh
Fine mesh