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Intégration de modèles 3D réduits dans
le processus de conception vibratoire.
Exemples de différentes industries.
Etienne Balmes
SDTools
Arts et Métiers ParisTech
NAFEMS Simulation des systèmes
3 Juin 2015
• FEM simulations
• System models (model reduction, state-space, active control, SHM)
• Experimental modal analysis
• Test/analysis correlation, model updating
Activities
2
CAD/Meshing
FEM
Simulation
Testing
CATIA, Workbench, …
NASTRAN, ABAQUS, ANSYS,...
Adams, Simulink,...
LMS TestLab, ME-Scope, …
Simulation
Validation
SDT : MATLAB based toolbox
Commercial since 1995 > 700 licenses sold
Pantograph/catenary Modal test correlation Track dynamics
Outline
• Systems, models, dynamic models
• Tools for model reduction
– Variable separation
– Parametric models
– Domain decomposition
• Conclusion
3
A system = I/O representation
Prototype Virtual prototype
 All physics (no risk on validity)  limited physics (unknown & long CPU)
 in operation response  design loads
 limited test inputs  user chosen loads
 measurements only  all states known
 few designs  multiple (but 1 hour, 1 night,
several days, … thresholds)
 Cost : build and operate  Cost : setup, manipulate
In Out
Environment/Design point
System
Meta/reduced models
5
Full numerical
model
expensive
Meta-model
acceptable cost
Learning
points
Responses
Computation
points
LearningX LearningY
X
Estimations
Yˆ
Validity ?
• Regular relation
• Band-limited
• Spatial position
of inputs
• …
Predictive monitoring
of fuel circuit
Ph.D. of B. Lamoureux
~500 parameters
~100 indicators
~20 Inputs
Data from in
operation
measurements
System models of structural dynamics
Simple linear time invariant system
Extensions
• Coupling (structure, fluid,
control, multi-body, …)
• Optimization, variability,
damping, non linearity, …
When
Where
Sensors
Large/complex FEM
Historical keywords :
Modal analysis
Superelements, CMS, …
Ingredient 1 : variable separation
• General transient but
– limited bandwidth
– time invariant system
• Modal Analysis
response well approximated
in spatial sub-space
𝑞(𝑥, 𝑡) = 𝜙𝑗 𝑥 𝑎(𝑡)
𝑁𝑀
𝑗=1
• Space shapes =modes
• Time shapes =
generalized coordinates
7
SVD on the time response
• coincides with modes if
isolated resonances
• similar info for NL systems
8
Space / Time decomposition
Squeal limit cycle
PhD Vermot (Bosch)
NL system with impacts, PhD Thénint (EDF)
Data/model reduction
9
• SVD = data reduction through variable separation
– Extension to higher dimension variable separation see Chinesta (afternoon)
• Ritz analysis : build reduced dynamic models
– Reduced model = differential/analytic equation for qR(𝑡)/qR(𝑠)
– States qR allow restitution
– Assumptions on loading : band limited 𝑢 𝑡
restricted loads in space 𝑏𝑖 𝑥
F x,t = bi x u t
NA
i=1
– Learning = full FEM static & modes (McNeal, Craig-Bampton, …)
{q}N=
qR
Nx NR
T
𝑀𝑠2 + 𝐶𝑠 + 𝐾 𝑞(𝑠) = 𝑏 𝑢(𝑠)
𝑇 𝑇 𝑍(𝑠) 𝑇 𝑁𝑅×𝑁𝑅 𝑞 𝑅(𝑠) = 𝑇 𝑇 𝑏 𝑢(𝑠)
Validity of reduced system models
Test & FEM system models assume
• Input restrictions
– Frequency band (modes)
– Localization (residual terms)
• System
– Time invariant
– Linear
Implemented in all major FEM & Modal Testing software
10
In Out
Environment/Design point
System
qR
Nx NR
T
System=IO relation
System=modal series
Challenge :
account for environment/design change
Sample design changes
• Material changes (visco damping)
• Junctions (contact)
• Component/system
Mesh/geometry
11
12
Ingredient 2 : parametric matrices
•Viscoelastic damping
𝐾𝑣 = 𝐾 𝐸(𝜔, 𝑇)
•Rotation induced stiffening
𝐾 𝐺 = 𝐾 Ω
•Contact stiffness evolution with
operating pressure
𝐾 𝑁 = 𝐾 p(x, 𝐹𝐺𝑙𝑜𝑏𝑎𝑙)
Reduction basis T can be fixed
for range of parameters
Speedup : 10-1e5
13
• Multi-model
• Other + residue iteration
• Example : strong coupling
With heavy fluids : modes of structure & fluid give
poor coupled prediction
Bases for parametric studies
Example water filled tank
With residualWithout residual
[T(p1) T(p2) … ]
Orthogonalization
[T]
[Tk] Rd
k=K-1 R(q(Tk))
Orthog [Tk Rd
k]
1th vertical mode: Main frame and
bow moving in phase
2
Co-simulation
SDToos/OSCAR
MSC/Motion
(VSD 2014)
Ingredient 3 : domain decomposition
• 1D  models coupled by few in/out :
hydraulic circuits, shaft torsion
• 3D FEM : classical uses
– Component Mode Synthesis/ Craig-Bampton
– Multibody with flexible superelements
• For each component base assumptions
remain
– LTI, few band-limited I/O
Two challenges
• Performance problems for large interfaces
• Component/system relation
14
Concept
Requirements &
architecture
Component design
System
operation
AVL Hydsim
Basic component coupling
Start : disjoint component models
Coupling relation between disjoint states
• Continuity 𝑞𝐼1 − 𝑞𝐼2 = 0
• Energy
+
16
Coupling + reduction
Classical CMS
• Reduced independently
• All interface motion (or interface modes)
• Assembly by continuity
Difficulties
• Mesh incompatibility
• Large interfaces
• Strong coupling (reduction requires knowledge of coupling)
Physical interface coupling
• Assembly by computation of interface energy
(example Arlequin)
Difficulties
• Use better bases than independent reduction
17
Squeal example : trace of system modes
CMS with trace of system modes
• No reduction of DOFs internal to contact area
• Reduction : trace of full brake modes on
reduced area & dependent DOFs (no need for
static response at interface)
Reduced model with exact system modes
Very sparse matrix for faster for time
integration
Component mode tuning method
• Reduced model is sparse
• Component mode amplitudes are DOFs
• Reduced model has exact nominal modes
(interest 1980 : large linear solution, 2015 : enhanced
coupling)
• Change component mode frequency  change the diagonal
terms of Kel
Disc
OuterPad
Inner Pad
Anchor
Caliper
Piston
Knuckle
Hub
wj
21
[M] [Kel] [KintS] [KintU]
CMT & design studies
• One reduced model /
multiple designs
Examples
• impact of modulus change
• damping real system or component mode
19
Component redesign
Sensitivity
energy analysis
Nom
.
+10
%
+20
%
-
20%
20
Conclusion
Reduced 3D models combine
• Variable separation
• Solve using generalized/reduced DOFs
–u(t) just assumed band-limited
–Restitution is possible
• Parametric matrices
• Domain decomposition
– Craig-Bampton is very costly
– Generalized coordinates can make sense
Challenges
• Engineering time to manage experiments
• Control data volume (>1e3 of NL runs)
• Control accuracy : develop software / train
engineers
In
Out
Environment
Design point
System
qR
Nx NR
T
www.sdtools.com/publications
Ritz

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Nafems15 systeme

  • 1. 1 Intégration de modèles 3D réduits dans le processus de conception vibratoire. Exemples de différentes industries. Etienne Balmes SDTools Arts et Métiers ParisTech NAFEMS Simulation des systèmes 3 Juin 2015
  • 2. • FEM simulations • System models (model reduction, state-space, active control, SHM) • Experimental modal analysis • Test/analysis correlation, model updating Activities 2 CAD/Meshing FEM Simulation Testing CATIA, Workbench, … NASTRAN, ABAQUS, ANSYS,... Adams, Simulink,... LMS TestLab, ME-Scope, … Simulation Validation SDT : MATLAB based toolbox Commercial since 1995 > 700 licenses sold Pantograph/catenary Modal test correlation Track dynamics
  • 3. Outline • Systems, models, dynamic models • Tools for model reduction – Variable separation – Parametric models – Domain decomposition • Conclusion 3
  • 4. A system = I/O representation Prototype Virtual prototype  All physics (no risk on validity)  limited physics (unknown & long CPU)  in operation response  design loads  limited test inputs  user chosen loads  measurements only  all states known  few designs  multiple (but 1 hour, 1 night, several days, … thresholds)  Cost : build and operate  Cost : setup, manipulate In Out Environment/Design point System
  • 5. Meta/reduced models 5 Full numerical model expensive Meta-model acceptable cost Learning points Responses Computation points LearningX LearningY X Estimations Yˆ Validity ? • Regular relation • Band-limited • Spatial position of inputs • … Predictive monitoring of fuel circuit Ph.D. of B. Lamoureux ~500 parameters ~100 indicators ~20 Inputs Data from in operation measurements
  • 6. System models of structural dynamics Simple linear time invariant system Extensions • Coupling (structure, fluid, control, multi-body, …) • Optimization, variability, damping, non linearity, … When Where Sensors Large/complex FEM Historical keywords : Modal analysis Superelements, CMS, …
  • 7. Ingredient 1 : variable separation • General transient but – limited bandwidth – time invariant system • Modal Analysis response well approximated in spatial sub-space 𝑞(𝑥, 𝑡) = 𝜙𝑗 𝑥 𝑎(𝑡) 𝑁𝑀 𝑗=1 • Space shapes =modes • Time shapes = generalized coordinates 7
  • 8. SVD on the time response • coincides with modes if isolated resonances • similar info for NL systems 8 Space / Time decomposition Squeal limit cycle PhD Vermot (Bosch) NL system with impacts, PhD Thénint (EDF)
  • 9. Data/model reduction 9 • SVD = data reduction through variable separation – Extension to higher dimension variable separation see Chinesta (afternoon) • Ritz analysis : build reduced dynamic models – Reduced model = differential/analytic equation for qR(𝑡)/qR(𝑠) – States qR allow restitution – Assumptions on loading : band limited 𝑢 𝑡 restricted loads in space 𝑏𝑖 𝑥 F x,t = bi x u t NA i=1 – Learning = full FEM static & modes (McNeal, Craig-Bampton, …) {q}N= qR Nx NR T 𝑀𝑠2 + 𝐶𝑠 + 𝐾 𝑞(𝑠) = 𝑏 𝑢(𝑠) 𝑇 𝑇 𝑍(𝑠) 𝑇 𝑁𝑅×𝑁𝑅 𝑞 𝑅(𝑠) = 𝑇 𝑇 𝑏 𝑢(𝑠)
  • 10. Validity of reduced system models Test & FEM system models assume • Input restrictions – Frequency band (modes) – Localization (residual terms) • System – Time invariant – Linear Implemented in all major FEM & Modal Testing software 10 In Out Environment/Design point System qR Nx NR T System=IO relation System=modal series Challenge : account for environment/design change
  • 11. Sample design changes • Material changes (visco damping) • Junctions (contact) • Component/system Mesh/geometry 11
  • 12. 12 Ingredient 2 : parametric matrices •Viscoelastic damping 𝐾𝑣 = 𝐾 𝐸(𝜔, 𝑇) •Rotation induced stiffening 𝐾 𝐺 = 𝐾 Ω •Contact stiffness evolution with operating pressure 𝐾 𝑁 = 𝐾 p(x, 𝐹𝐺𝑙𝑜𝑏𝑎𝑙) Reduction basis T can be fixed for range of parameters Speedup : 10-1e5
  • 13. 13 • Multi-model • Other + residue iteration • Example : strong coupling With heavy fluids : modes of structure & fluid give poor coupled prediction Bases for parametric studies Example water filled tank With residualWithout residual [T(p1) T(p2) … ] Orthogonalization [T] [Tk] Rd k=K-1 R(q(Tk)) Orthog [Tk Rd k]
  • 14. 1th vertical mode: Main frame and bow moving in phase 2 Co-simulation SDToos/OSCAR MSC/Motion (VSD 2014) Ingredient 3 : domain decomposition • 1D  models coupled by few in/out : hydraulic circuits, shaft torsion • 3D FEM : classical uses – Component Mode Synthesis/ Craig-Bampton – Multibody with flexible superelements • For each component base assumptions remain – LTI, few band-limited I/O Two challenges • Performance problems for large interfaces • Component/system relation 14 Concept Requirements & architecture Component design System operation AVL Hydsim
  • 15. Basic component coupling Start : disjoint component models Coupling relation between disjoint states • Continuity 𝑞𝐼1 − 𝑞𝐼2 = 0 • Energy +
  • 16. 16 Coupling + reduction Classical CMS • Reduced independently • All interface motion (or interface modes) • Assembly by continuity Difficulties • Mesh incompatibility • Large interfaces • Strong coupling (reduction requires knowledge of coupling) Physical interface coupling • Assembly by computation of interface energy (example Arlequin) Difficulties • Use better bases than independent reduction
  • 17. 17 Squeal example : trace of system modes CMS with trace of system modes • No reduction of DOFs internal to contact area • Reduction : trace of full brake modes on reduced area & dependent DOFs (no need for static response at interface) Reduced model with exact system modes Very sparse matrix for faster for time integration
  • 18. Component mode tuning method • Reduced model is sparse • Component mode amplitudes are DOFs • Reduced model has exact nominal modes (interest 1980 : large linear solution, 2015 : enhanced coupling) • Change component mode frequency  change the diagonal terms of Kel Disc OuterPad Inner Pad Anchor Caliper Piston Knuckle Hub wj 21 [M] [Kel] [KintS] [KintU]
  • 19. CMT & design studies • One reduced model / multiple designs Examples • impact of modulus change • damping real system or component mode 19 Component redesign Sensitivity energy analysis Nom . +10 % +20 % - 20%
  • 20. 20 Conclusion Reduced 3D models combine • Variable separation • Solve using generalized/reduced DOFs –u(t) just assumed band-limited –Restitution is possible • Parametric matrices • Domain decomposition – Craig-Bampton is very costly – Generalized coordinates can make sense Challenges • Engineering time to manage experiments • Control data volume (>1e3 of NL runs) • Control accuracy : develop software / train engineers In Out Environment Design point System qR Nx NR T www.sdtools.com/publications Ritz