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Adaptive shunted piezoelectric metacomposite: a new integrated technology for vibroacoustic control
Dr M. Collet(1), Dr M. Ouisse(1), F. Tatéo, Pr M. Ichchou(2), T. Huang(2)
(1) Dept Applied MechanicsFEMTO-ST UMR 6174, Besançon, France (2) LTDS, Ecole Centrale de Lyon, Ecully, France
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université de technologieBelfort-Montbéliard dMEMS 2012 - Besançon
Motivations
2
Classical approaches of ANC or AVC is difficult to apply into real fully distributed applications :
Technological and Numerical complexity
Difficulties for integrating such technology into the Design Process (Robustness/Performances)
Energy Cost
Necessity to propose a new approach ….
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Active Control of Vibroacoustic interface by the synthesis of generalized Impedance operator
université de technologieBelfort-Montbéliard dMEMS 2012 - Besançon3
To Program the behavior relationship inside hybrid composite material by using a distributed set of smart cells including transducers, Computing capabilities and smart materials .
We have to Synthetize and integrate dedicated programmable vibroacoustic functionnalities inside structures for realizing adaptive interfaces.
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Motivations
université de technologieBelfort-Montbéliard dMEMS 2012 - Besançon4
The Targeted Application
Let us consider the elasto-dynamical wave control by means of shunted piezoelectric periodic patches :
The shunt impedance is complex Damped SystemWe obtain evanescent Bloch wave and damped scattering
By using WFE techniques => Optimization of the energy diffusion* for wave trap
* M. Collet, K.A. Cunefare, N.M. Ichchou, Wave Motion Optimization in Periodically Distributed Shunted Piezocomposite Beam Structures Journal of Intelligent Material Systems and Structures, 20(7), 787-808, 2009
université de technologieBelfort-Montbéliard dMEMS 2012 - Besançon5
Challenges and Contents
Fields of interest– Wave propagation in multiphysics and periodic systems : Smart Wave Guides– Structural Health Monitoring (Faults detection…)– Noise & Vibration Reduction in Complex Structures (Optimization of passive or active
systems) Available Techniques
– Floquet theorem in 1D waveguide (SAFE, WFE, TL techniques …)– Bloch theorem in 2D for undamped or weakly damped systems (WFE)
Challenges– To predict and analyze complex waves vectors of damped mechanical systems with
multiphysics coupling introduced by shunted piezoelectric patches Approach
– Formulate Bloch Expansion theorem for damped piezo-elastodynamic problems– Introduce a suitable criterion based on Waves Intensity vector
Contents - Outline– Mathematical methodology– Optimization of the shunted electric impedance – Acoustic induced control and 3D validations.
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard6
Part 1-
Mathematical Formulation
Part 1-
Mathematical Formulation
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard7
Bloch Expansion Theorem
‘Generic’ Elliptic PDE :
(Bloch Expansion)
where are the eigenvectors :
of the shifted cell operator :
Periodic System
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard8
Piezo-Elastodynamic Application
The Piezo-Elastodynamic equilibrium :
Boundary Conditions
With :
The weak formulation is also:
QEP
The shifted cell eigenvalue problem :
and :
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard9
Numerical Implementation
The proposed Weak formulation leads to a QEP:
When visco-elastic materials and adaptive metamaterials (shunted piezoelectric) are considered, we introduce frequency dependent piezo-elastodynamic operator i.e K, L and H depend on : w The problem is Non Linear, and non quadratic on w
We prefer to solve that QEP by fixing w and f and search k :
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard10
Part 2-
Electric Impedance Optimization
Part 2-
Electric Impedance Optimization
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard11
The Considered System
PZT-Aluminum Composite
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard12
Optimization of the shunted electric impedance
The Critera for Optimizing the Flexural Wave Propagation:Based on computing the Group Velocity :
Two vibroacoustic functions to minimize is (Nelder Mead algorithm):
(Transmission)
(Absorption)
The normal acoustic wave number is given by :
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard13
Transmission Optimization
Induced effects on Acoustic normal wave number Acoustic coincidence
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard14
Reactive Circuit
Quasi constant Cneg :
The Optimal Impedance
Transmission Optimization
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard15
Effect on Acoustic normal wave number Acoustic coincidence
Acoustic decay rate
Absorption Optimization
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard16
Dissipative Circuit
Quasi constant Cneg :
The Optimal Impedance
Absorption Optimization
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard17
Validation on a periodically semi-distributed adaptive cells
The considered System :
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard18
Validation on a periodically semi-distributed adaptive cells
dMEMS 2012, Besançonuniversité de technologieBelfort-Montbéliard19
Conclusions
Wave Dispersion in 2DWave Dispersion in 2D
Application of the Bloch TheoremApplication of the Bloch Theorem
Shunted Piezoelectric SystemShunted Piezoelectric System
Finite Element Approach (Multiphics)Finite Element Approach (Multiphics)
ConceptsConcepts
Whole 2D K-space computation with electric shuntWhole 2D K-space computation with electric shunt
Group Velocity based IndicatorGroup Velocity based Indicator
Impedance optimizationImpedance optimization
Vibroacoustic energy diffusion controlVibroacoustic energy diffusion control
ResultsResults
Periodic smart StructuresPeriodic smart Structures
Passive, semi-active or active controlPassive, semi-active or active control
Waves Diffusion at 2D Medium InterfaceWaves Diffusion at 2D Medium Interface
Wave Trap ConceptsWave Trap Concepts
FutureFuture