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WP3' Adaptive Composite Modeling

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Title: WP3' Adaptive Composite Modeling


1
WP3. Adaptive Composite Modeling
  • FP6- STREP project contract N013517NMP3-CT-2005-
    013517
  • Paris, 12-13 December 2006
  • E. CARRERA - POLITO WPLeader

2
SUMMARY
  • 1 - WP3 Overview
  • 2 - Task 3.1 Modelling composites with
    piezoelectric
    sensors/actuators
    (POLITO, IST, LPMM)
  • 3 - Task 3.2 Modelling thermo-piezoelectric
    composites (POLITO,ISMEP)

3
WP3 Overview
  • Partecipants
  • LPMM(4) ISMEP (2) IST (8) POLITO(3),ULB(9)
  • WP Leader
  • POLITO
  • Start
  • 1 (4), End 21 (25)
  • Interaction
  • WP1,WP4,WP5

4
WP3 Overview
  • Description of work
  • Task 3.1 Modelling composites with piezoelectric
    sensors/actuators ( POLITO,
    IST,LPMM) ACTIVE (Complete)
  • Task 3.2 Modelling thermo-piezoelectric
    composite composites with piezoelectric
    sensors/actuators
    (POLITO, ISMEP) ACTIVE(In
    progress)
  • Task 3.3 Piezoceramic shunted damping concepts

    (ISMEP, ULB) NOT Active
  • Task 3.4 Models and concepts validation

    (ALL) NOT Active

5
WP3 Overview
  • Objectives
  • Analytical and numerical (finite element)
    modelling of sandwich and laminated composites
    with piezoelectric layers.
  • Analytical and numerical modelling of thermal and
    pyroelectric effects in piezoelectric composites
  • Finite element modelling and analysis of new
    passive damping concepts using shunted
    piezoceramics
  • Application and validation of the above advanced
    models and associated FE for various problems,
    such as vibration suppression of simple beams and
    plates due to mechanical or/and thermal loads by
    means piezoelectric sensors and actuators

6
Task 3.1 Declared Topics (POLITO,IST,LPMM)
Comprehensive coupled piezoelectric models for
beam, plate and shell geometries will be
developed. The model has hierarchic capabilities
in the sense that accuracy can be increased by
augmenting computational efforts.
  • The following main cases will be available
  • Classical model based on known theories for
    laminates, such as
    CLT (Classical Laminated
    Theories) and FSDT (First order Shear Deformation
    Theory)
  • Layer-wise models that have independent variables
    in each layer will be used to describe zig-zag
    fields for the displacement
  • Classical methods with only displacement
    variables and advanced methods based on Mixed
    Variational Theorem will be discussed to fulfil
    interlaminar continuity of normal stresses.

7
Task 3.1 Variational statements (POLITO)
Models have been developed in the framework of
the three following variational tools.
PVD Principle of Virtual Displacements
RMVT Reissner Mixed Variational Theorem
E RMVT Electric Reissner Mixed Variational
Theorem, four fields
The developments have been made according Unified
Formulation introduced by Carrera.
8
Task 3.1 Constitutive and geometric relaction
(POLITO)
Plates
Shells
9
Task 3.1 Formulation (POLITO)
Unified Formulation
Classic Formulation (PVD)
Mixed Formulation (RMVT)
Mixed formulation four field (RMVT)
10
Task 3.1 Different theories(POLITO)
Equivalent Single Layer (ESL)
Funzione di Murakami (zig-zag)
Layer Wise (LW)
11
Task 3.1 Acronyms (POLITO)
12
Task 3.1Examples (POLITO)
13
Task 3.1 Principle of virtual displacements
(PVD) (POLITO)
Constitutive relactions
Geometric relations
Thickness function
Shape function
Matrix product
FEM governing equations
14
Task 3.1 Constitutive relations RMVT(POLITO)
Constitutive relations PVD
Constitutive relations RMVT
15
Task 3.1 Reissner Mixed Variation Theory(RMVT)
(POLITO)
Substituting constitutive relations
Substituting geometric reltions
Substituting thickness functions
Substituting shape functions
16
Task 3.1 Constitutive relations RMVT four
field(POLITO)

Constitutive relations PVD
Constitutive relations RMVT four fields
17
Task 3.1 Reissner Mixed Variation Theory four
field(POLITO)
Substituting constitutive relations
Substituting geometric reltions
Substituting thickness functions
Substituting shape functions
18
Task 3.1 Assembling (POLITO)
Assemblaggio nodo-layer
Variazione indice k
Assemblaggio nodo-multilayer
Variazione indici i,j
Equivalent single layer
Lawer wise
Eliminazione gradi di libertà vincolati
Assemblaggio struttura
Applicazione Penalty
Applicazione dei vincoli
19
Task 3.1 Numerical Results (POLITO)
  • Modal Analysis of an adaptive plate by Mixed and
    Classical FEs
  • Static Analysis of an adaptive plate by Mixed and
    Classical FEs sensor
  • Static Analysis of an adaptive plate by Mixed and
    Classical models actuator
  • Analytic models for piezo-mechanics ring modal
    analysis

20
Task 3.1 Modal Analysis(POLITO)
6x6 Q9 Integrazione selettiva
21
Task 3.1Modal Analysis (POLITO)
  • Every order of LW theories is able to obtain the
    frequencies with a maximum error of 2
  • Mixed theories make us obtain better results
    using lower expansion order
  • Murakamis function improves an ESL theory

22
Task 3.1 Sensor (POLITO)
6x6 Q9 Integrazione selettiva
23
Task 3.1 Sensor (POLITO)
  • The exact value is 6.11 for a a/h4 plate
  • Mixed element obtains better result than classic
    elements using lower expansion order
  • ESL elements do not obtain correct values using
    low expansion order
  • Murakamis function improves ELS models
  • Mixed theories respect CZ0 requirements and
    obtain continuous normal stresses
  • To obtain the normal electric displacement
    continuous is necessary to use the RMVT four
    fields

24
Task 3.1 Actuator (POLITO)
25
Task 3.1 Actuator (POLITO)
  • The exact value is 0.4476 for a a/h4 plate
  • Mixed theories obtains better result than classic
    theories using lower expansion order
  • ESL theories do not obtain correct values using
    low expansion order
  • Murakamis function improves ELS models
  • Mixed theories respect CZ0 requirements and
    obtain continuous normal stresses
  • To obtain the normal electric displacement
    continuous is necessary to use the RMVT four
    fields

26
Task 3.1 Modal analysis for piezo-mechanic ring
(POLITO)
27
Task 3.1 Modal Analysis (POLITO)
  • Mixed theories obtains better result than classic
    theories using lower expansion order
  • ESL theories do not obtain correct values using
    low expansion order
  • Mixed theories respect CZ0 requirements and
    obtain continuous normal stresses
  • To obtain the normal electric displacement
    continuous is necessary to use the RMVT four
    fields

Frequencies Hz. Compare PVD and RMVT models
28
Task 3.2 Declared Topics (POLITO,IST,LPMM)
Development and implementation of computationally
finite elements of thermo-piezo-elastic model for
the analysis of smart structures. Accurate
hierarchical formulation based on classical
variational statement (PVD) and advanced
partial-mixed variational principles will be
proposed.
  • The following main cases will be available
  • Layer-wise models that have independent variables
    in each layer will be used to describe zig-zag
    fields for the displacement, electric potential,
    normal stresses, normal potential and
    temperature
  • Temperature can be modelled like a load and the
    coupling temperature-mechanic field will be
    neglected
  • Temperature can be considered like an unknown and
    the coupling temperature-mechanic field will be
    considered

29
Task 3.2 Variational statements(POLITO)
Models have been developed in the framework of
the three following variational tools.
  • PVD piezo-thermo-mechanic partially coupled
    (two fields u,E)
  • PVD piezo-thermo-mechanic fully coupled (three
    fields u,E,q)
  • RMVT piezo-thermo-mechanic partially coupled
    (three fields u,E,sn)
  • RMVT piezo-thermo-mechanic fully coupled (four
    fields u,E,sn,q)
  • ERMVT piezo-thermo-mechanic fully coupled (five
    fields u,E,sn, Dn,q)

Numerical results will be obtained soon. At the
moment just partially coupled methods have been
implemented.
30
Task 3 POLITO Research Work
  • Details can be read in
  • E. Carrera, M. Boscolo, C. Fagiano, A. Robaldo,
    Unified Formulation to Assess Multilayered Plate
    Analysis of Thermo-Mechanical Problems, XVIII
    CONGRESSO NAZIONALE AIDAA, Volterra(PI), Italy,
    September 19-22, 2005
  • E. Carrera, M. Boscolo, C. Fagiano, A. Robaldo,
    Mixed Finite Elements for Piezoelectric Plates
    based on Unified Formulation, XVII CONGRESSO
    AIMeTA DI MECCANICA TEORICA E APPLICATA,
    Florence, Italy, September 11-15, 2005
  • E. Carrera, M. Boscolo, C. Fagiano, A. Robaldo,
    Mixed Elements for Accurate Vibration of
    Piezo-electric Plates, II ECCOMAS THEMATIC
    CONFERENCE ON SMART STRUCTURES AND MATERIALS,
    Lisbon , Portugal, July18-21,2005

31
Task 3 POLITO Research Work
  • The following experiments could be of POLITO
    interest
  • The considered multilayered (any configuration
    with piezo-electric layers and pathces)
    structures can be beams or flat or curved panels
    with any geometrical boundary conditions (simply
    supported is the favorite one).
  • 1. Vibration testing
  • 1.1 Closed circuit - Open Circuit.
  • 1.2 Calculation of the first 1-5
    frequencies.
  • 2. Static Electromechanical testing
    Actuators/Sensors
  • 2.1 Case of applied potential
  • 2.2 Case of applied pressure
  • 2.3 Case of applied charge
  • Measurements of displacements, some
    stresses, Electrical variables (potentential,
    charge, displacements)

32
Task 3 POLITO Research Work
3. Thermo-Electromechanical testing
Actuators/Sensors 3.1 Case of applied
potential 3.2 Case od applied pressure
3.3 Case of applied charge 3.4 Case of
Uniform heating (temperature is the same in the
top and bootm surface) 3.5 Case of
non-uniform heating (temperature is different in
the top and bottom surface). 4. Control,
closed loop experiments 4.1
piezo-mechanical 4.2 thermo-electro-mechanica
l
33
IST Contribution to CASSEM Project
  • FP6 STREP Project Contract N 013517NMP3 - CT
    - 2005 - 013517
  • Paris, 12-13 December 2005
  • IST Lisbon Technical University, Portugal
  • Participant nr. 8

34
IST contribution to WP 3 WP 3 Adaptive
composites modelling (Leader TUT / Italy)
  • Task 3.1 Modelling composites with
    piezoelectric sensors/actuators
  • (TL TUT, IST, LPMM)
  • Higher Order Shear Deformation Theory and First
    Order Shear Deformation Theory coupled
    piezoelectric F.E. models for plate and shell
    geometries (based on displacement approach).
  • Mixed layerwise theory F.E. model for plate
    structures which includes piezoelectric behavior
    of layers or patches.
  • Mixed FE formulation based on least-squares
    variational principles, which is an alternate
    approach to the mixed weak form FE models.

35
WP3 cont.HSDT and FSDT coupled piezoelectric
FE models
  • Higher Order Shear Deformation Theory and First
    Order Shear Deformation Theory coupled
    piezoelectric F.E. models for plate and shell
    geometries, based on the generic displacement
    field

Among the IST research team, there are a few
published articles devoted to the development and
validation of these models for the analysis and
optimization of plate structures with
piezoelectric layers or patches.
36
WP3 cont.HSDT and FSDT coupled piezoelectric
FE models
  • since the beginning of the project
  • J.M. Moita, C.M. Mota Soares, C.A. Mota Soares,
    Active Control of Forced Vibrations in Adaptive
    Structures Using a Higher Order Model, Composite
    Structures, Elsevier, UK, Vol.71, pp. 349-355,
    2005.
  • J.M. Moita, P.G. Martins, C.M. Mota Soares, C.A.
    Mota Soares, Optimal Dynamic Control of
    Laminated Adaptive Structures Using a Higher
    Order Model and a Genetic Algorithm, Computers
    and Structures, (submitted in 2005).
  • J.M. Moita, V.M. Franco Correia, P.G. Martins,
    C.M. Mota Soares, C.A. Mota Soares, Optimal
    Design in Vibration Control of Adaptive Stuctures
    Using a Simulated Annealing Algorithm, Composite
    Structures, (submitted in 2005).

37
WP3 cont.Mixed layerwise FE model
  • Mixed layerwise theory for laminated plate
    structures which includes piezoelectric materials
    (layers or patches).
  • Due to the mixed formulation, transverse stresses
    (?zz, ?xz, ?yz), displacements (u, v, w) and
    electric potential (?) are considered as degrees
    of freedom, and are calculated without the need
    of post-processing. The model guarantees the
    continuity requirements for these quantities.
    The in-plane stress (?xx, ?yy, ?xy) and
    electric displacement (Dx, Dy, Dz) are calculated
    by post-processing of the obtained solution.
  • R.M. Garcia Lage, C.M. Mota Soares, C.A. Mota
    Soares, Static and Free Vibration Analysis of
    Magneto-Elastic Laminated Plates by a Layerwise
    Partial Mixed Finite Element Model, The 3rd
    International Conference on Structural Stability
    and Dynamics, June 19-22, 2005, Kissimmee,
    Florida, USA.

38
WP3 cont.Mixed layerwise FE model(cont. 2)
  • The problem fields, for each layer , are
  • The shape functions F(z) describe the plate
    behaviour in the thickness direction, which can
    be linear, quadratic or cubic.
  • The functions szz, sxz, syz, U, V, W, ? denote
    the nodal values of primary variables.


39
WP3 cont.Mixed layerwise FE model(cont. 3)
Numerical example 1
  • Ilustrative numerical example 1 simply supported
    PVDF piezolaminated plate with square shape (a?a)
    and thickness h.
  • Plate lay up is taken to be 0º/90º/0º and the
    PVDF layers properties are
  • Three geometric configurations with
    side-to-thickness ratios a/h4 10 50 (with
    h0.01m) and two load cases are analysed

LC1 LC2
40
WP3 cont.Mixed layerwise FE model(cont.
4)Transverse stresses and transversal electrical
displacement LC1
41
WP3 cont.Mixed layerwise FE model(cont.
5)Mechanical displacements and electric
potential LC1
42
WP3 cont.Mixed layerwise FE model(cont.
6)Transverse stresses and transversal electrical
displacement LC2
43
WP3 cont.Mixed layerwise FE model(cont. 7)
Mechanical displacements and electric potential
LC2
44
WP3 cont.Mixed layerwise FE model(cont. 8)
Numerical example 2
  • Ilustrative numerical example 2 simply supported
    piezolaminated single layer plate with square
    shape (a?a) and thickness (h0.01m). The plate is
    made of PZT-4 with stiffness and piezoelectric
    properties as follows
  • Typical results, for free vibration problems, are
    presented below

Ref.1 Heyliger Saravanos, J. Acoust. Soc.
Am., 98 (1995) 1547-1557.
45
WP3 cont.Mixed layerwise FE model(cont. 8)
Cross thickness modal distributions
46
Mixed Least-Squares FE Model
  • A mixed FE formulation based on least-squares
    variational principles, which is an alternate
    approach to the mixed weak form FE models, is
    being developed.
  • The least-squares-based FE model is being
    developed for the static and dynamic analysis of
    laminated composite plates using the FSDT, with
    the generalized displacements and stress
    resultants as independent variables.

47
Mixed Least-Squares FE Model Governing Equations
  • Equilibrium Equations and Laminate Constitutive
    Equations

48
Mixed Least-Squares FE Model Least-Squares
Formulation (1)
  • In a more compact notation the governing
    equations become

where,
  • Then, the associated least-squares functional is
    given by

49
Mixed Least-Squares FE Model Least-Squares
Formulation (2)
  • Leading to the following variational problem

50
Mixed Least-Squares FE Model Numerical Examples
(1)
  • Results for the static analysis of the square
    composite laminates (0/90), (0/90/0/90/0) and
    (-45/45)4 under uniformly distributed load, with
    different boundary conditions and
    side-to-thickness ratios.

Analytic solutions using FSDT by Navier series
(mn1,,30) and Lévy series (n1,,30).
51
Mixed Least-Squares FE Model Numerical Examples
(2)
  • Normalized deflections of the previous laminates
    with all boundaries simply supported (SSSS-1 or
    SSSS-2 as tabled).

52
Mixed Least-Squares FE Model Numerical Examples
(3)
  • Normalized deflections of the previous laminates
    with two opposite boundaries free and two simply
    supported (FFSS-1 or FFSS-2 as tabled).

53
IST contribution to WP 7WP 7 Dissemination and
innovation related activities(Leader CRPHT)
  • Publishing of Articles in selected Scientific
    International Journals
  • Composite Structures
  • Computers Structures
  • Journal of Inverse Problems in Science and
    Engineering
  • Participation in International Conferences
  • ICCS-13th Intern. Conf. of Composite Structures
    (Australia)
  • CST-8 (Tenerife)
  • ECCM-2006 (Lisbon)
  • SPIE - Smart Structures Materials/NDE 2006
    (San Diego, CA)
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