1/23 A. Giraudeau, F. Pierron - 2009 MPSVA conference Identification of local material damping in vibrating plates using full-field measurements Alain.

Slides:



Advertisements
Similar presentations
TWO STEP EQUATIONS 1. SOLVE FOR X 2. DO THE ADDITION STEP FIRST
Advertisements

Analysis and Design of Beams for Bending
Kapitel 21 Astronomie Autor: Bennett et al. Galaxienentwicklung Kapitel 21 Galaxienentwicklung © Pearson Studium 2010 Folie: 1.
Supplemental Web Fig. 2 mos10/mos10, grown on 100 mm plate SLAS27 medium, day 1.
Chapter 1 The Study of Body Function Image PowerPoint
Finite Element Method CHAPTER 4: FEM FOR TRUSSES
INTRODUCTION TO MECHANICS FOR SOLIDS AND STRUCTURES
SPECIAL PURPOSE ELEMENTS
Copyright © 2011, Elsevier Inc. All rights reserved. Chapter 5 Author: Julia Richards and R. Scott Hawley.
1 Copyright © 2010, Elsevier Inc. All rights Reserved Fig 2.1 Chapter 2.
By D. Fisher Geometric Transformations. Reflection, Rotation, or Translation 1.
Business Transaction Management Software for Application Coordination 1 Business Processes and Coordination.
MIT 2.71/2.710 Optics 10/25/04 wk8-a-1 The spatial frequency domain.
FIGURE 5.1 Potentiometric displacement sensor.
Jeopardy Q 1 Q 6 Q 11 Q 16 Q 21 Q 2 Q 7 Q 12 Q 17 Q 22 Q 3 Q 8 Q 13
Jeopardy Q 1 Q 6 Q 11 Q 16 Q 21 Q 2 Q 7 Q 12 Q 17 Q 22 Q 3 Q 8 Q 13
Title Subtitle.
0 - 0.
ALGEBRAIC EXPRESSIONS
DIVIDING INTEGERS 1. IF THE SIGNS ARE THE SAME THE ANSWER IS POSITIVE 2. IF THE SIGNS ARE DIFFERENT THE ANSWER IS NEGATIVE.
MULTIPLYING MONOMIALS TIMES POLYNOMIALS (DISTRIBUTIVE PROPERTY)
SUBTRACTING INTEGERS 1. CHANGE THE SUBTRACTION SIGN TO ADDITION
MULT. INTEGERS 1. IF THE SIGNS ARE THE SAME THE ANSWER IS POSITIVE 2. IF THE SIGNS ARE DIFFERENT THE ANSWER IS NEGATIVE.
Addition Facts
Year 6 mental test 5 second questions
Evolutionary Structural Optimisation
Two-Dimensional Unsteady Planing Elastic Plate Michael Makasyeyev Institute of Hydromechanics of NAS of Ukraine, Kyiv.
Around the World AdditionSubtraction MultiplicationDivision AdditionSubtraction MultiplicationDivision.
ZMQS ZMQS
Through-the-Thickness Mechanical Properties of Smart Composite Laminates Gang Zhou, L.M. Sim, P.A. Brewster and A.R. Giles Department of Aeronautical.
BT Wholesale October Creating your own telephone network WHOLESALE CALLS LINE ASSOCIATED.
FINAL FOCUS: COMBINATION OF PRE ISOLATOR AND ACTIVE STABILISATION K. Artoos, C. Collette, R. Leuxe, C.Eymin, P. Fernandez, S. Janssens * The research leading.
1/38 The virtual fields method for characterizing nonlinear behavior Dr. Stéphane AVRIL.
Aerospace Structures and Materials Lecture 22: Laminate Design.
1 Damage State Awareness in Composite Laminates Via Ultrasonic Guided Waves Cliff Lissenden Joseph Rose Engineering Science & Mechanics The Pennsylvania.
WAL Rail Damper for Track Noise Reduction
ABC Technology Project
Imperial College London 1 3. Beam extraction 3. Extraction of particle beams 3.1 The space charge limit and Child-Langmuirs law 3.2 External and internal.
High Frequency Distortion in Power Grids due to Electronic Equipment Anders Larsson Luleå University of Technology.
2 |SharePoint Saturday New York City
© S Haughton more than 3?
VOORBLAD.
Squares and Square Root WALK. Solve each problem REVIEW:
Lets play bingo!!. Calculate: MEAN Calculate: MEDIAN
Chapter 5 Test Review Sections 5-1 through 5-4.
SIMOCODE-DP Software.
GG Consulting, LLC I-SUITE. Source: TEA SHARS Frequently asked questions 2.
1 First EMRAS II Technical Meeting IAEA Headquarters, Vienna, 19–23 January 2009.
1 Anisotropic characteristics of wood dynamic viscoelastic properties Jianxiong Lu, Fucheng Bao and Jiali Jiang Key Laboratory of Wood Science and Technology.
Addition 1’s to 20.
25 seconds left…...
Test B, 100 Subtraction Facts
Week 1.
We will resume in: 25 Minutes.
©Brooks/Cole, 2001 Chapter 12 Derived Types-- Enumerated, Structure and Union.
1 Department of Civil and Environmental Engineering Sungkyunkwan University 비대칭 박벽보의 개선된 해석이론 및 방법 An Improved Theory and Analysis Procedures of Nonsymmetric.
1 Unit 1 Kinematics Chapter 1 Day
PSSA Preparation.
How Cells Obtain Energy from Food
Chapter 30 Induction and Inductance In this chapter we will study the following topics: -Faraday’s law of induction -Lenz’s rule -Electric field induced.
CompTest 2003 : ENSAM-Châlons en Champagne, January 2003 DIRECT IDENTIFICATION OF THE DAMAGED BEHAVIOUR OF COMPOSITE MATERIALS USING THE VIRTUAL.
1 /16 M.Chrzanowski: Strength of Materials SM1-10: Continuum Mechanics: Constitutive equations CONTINUUM MECHANICS (CONSTITUTIVE EQUATIONS - - HOOKE LAW)
Professor Fabrice PIERRON LMPF Research Group, ENSAM Châlons en Champagne, France THE VIRTUAL FIELDS METHOD Application to linear elasticity Paris Châlons.
Identification of material properties using full field measurements on vibrating plates Mr Baoqiao GUO, Dr Alain GIRAUDEAU, Prof. Fabrice PIERRON LMPF.
Identification of stiffness and damping properties of composites from full field measurements Theory and simulations A. Giraudeau, F. Pierron L.M.P.F.
Moulart, Pierron, Hallett, Wisnom - SEM 2009 Albuquerque 1 High strain rate photomechanics on composites: use of a ultra high speed camera and the virtual.
Professor Fabrice PIERRON LMPF Research Group, ENSAM Châlons en Champagne, France THE VIRTUAL FIELDS METHOD The principle of virtual work Paris Châlons.
Presentation transcript:

1/23 A. Giraudeau, F. Pierron MPSVA conference Identification of local material damping in vibrating plates using full-field measurements Alain Giraudeau, Fabrice PIERRON LMPF research group Arts et Métiers ParisTech Châlons en Champagne - France 7 th International Conference on Modern Practice in Stress and Vibration Analysis, 8-10 th September 2009, Cambridge

2/23 A. Giraudeau, F. Pierron MPSVA conference Motivation / Objectives  Material damping  Difficult to measure  Problem with connections/joints  Most of the standard techniques rely on beams  Difficult (but important) to get both complex stiffnesses on same test N.W. Tschoegl, W.G. Knauss, and I. Emri. Poisson's ratio in linear viscoelasticity - a critical review. Mechanics of Time-Dependent Materials, 6:3-51,  Objectives  Simultaneous identification of both complex stiffnesses (isotropy) on single test  Method to cancel the effect of connections  Explore the use of full-field measurements

3/23 A. Giraudeau, F. Pierron MPSVA conference Identification of material properties : Stiffness Damping  Thin plate specimens  Dynamic loading Attachements :Parasistic effects Unknown energy loss Equilibrium of forces No energy consideration F(t) Principle

4/23 A. Giraudeau, F. Pierron MPSVA conference Dynamic equilibrium :  Point M :  Observed area Internal f. Boundary f.Volumic f. Inertial f. Principle of Virtual Work (P V W) - Continuous - Differentiable ui*ui* ui*ui*ui*ui* Principle F(t) M

5/23 A. Giraudeau, F. Pierron MPSVA conference Considered case  Rectangular thin plate  Sine driving movement  Inertial excitation  Full field measurements  Data processing using Virtual Fields Method (V.F.M.)  Clamped on small area Principle

6/23 A. Giraudeau, F. Pierron MPSVA conference Principle of Virtual Work u*u* Thin plates Sine vibrating response  *=  ( u *) Constitutive law Unknown Thin plates  k SelectedMeasured Virtual Fields Method

7/23 A. Giraudeau, F. Pierron MPSVA conference along  V. F. Selection : = 0  Virtual Fields Method

8/23 A. Giraudeau, F. Pierron MPSVA conference P V W Measured ( w(x,y), k(x,y)) Selected k*(x,y), w*(x,y) (w(x,y),w*(x,y)) Two selected virtuals fields : VF1, VF2 Direct resolution of an inverse problem Virtual Fields Method

9/23 A. Giraudeau, F. Pierron MPSVA conference Deflectometry CCD O M P Q Deflection fields Curvature fields Slope fields In phase  /2 lag  dd . d  Experimental arrangement

10/23 A. Giraudeau, F. Pierron MPSVA conference Image Processing Grid Images At restDeformed Phases xx y y - Slopes x - y Spatial phase evaluation Experimental arrangement

11/23 A. Giraudeau, F. Pierron MPSVA conference Experimental set-up Experimental arrangement

12/23 A. Giraudeau, F. Pierron MPSVA conference Deflection 34  m / col. 80Hz (out of resonance) Images (examples) Results

13/23 A. Giraudeau, F. Pierron MPSVA conference Piecewise virtual fields (Toussaint et al., IJMS, 2006) w*(x,y) = 0  *(x,y) = 0  Virtual fields selection Results

14/23 A. Giraudeau, F. Pierron MPSVA conference Reference values Coupons: polycarbonate beams h = 4mm, l = 10mm, L= mm Clamped-free conditions Free vibrations, first bending mode E (GPa)  ( = tan(  ) ) Means C. variation 2.4%5.2% DMTA Results

15/23 A. Giraudeau, F. Pierron MPSVA conference Results 80 Hz 100 Hz reference (Beams, DMTA) (non res.) (res.) Poisson rat. loss factor GPa

16/23 A. Giraudeau, F. Pierron MPSVA conference Boundary condition effects Rubber washers 2 nd accelerometer  = 34° tan(  )= nd accel. Driving mvt. 100 Hz Results

17/23 A. Giraudeau, F. Pierron MPSVA conference GPa Poisson rat. loss factor Initial clampingWith rubber washers Boundary condition effects (2) 100 Hz tan(  )=0.67 Results

18/23 A. Giraudeau, F. Pierron MPSVA conference Additional damping effect Viscoelastic patch at back surface  w*(x,y) = 0  *(x,y) = 0 Results

19/23 A. Giraudeau, F. Pierron MPSVA conference GPa Poisson rat. loss factor Initial clampingWith rubber washers Additional damping effect (2) 100 Hz Results

20/23 A. Giraudeau, F. Pierron MPSVA conference Conclusion  Simultaneous identification of stiffness and damping  Material damping  Resonant or non resonant response  Information on localization phenomena  Low sensitivity to boundary conditions  Could be applied to in-plane vibrations  Plate of any shape  Part of a component

21/23 A. Giraudeau, F. Pierron MPSVA conference Conclusion Soundboard of a guitar Local damping

22/23 A. Giraudeau, F. Pierron MPSVA conference Conclusion  Improvements  Time synchronization: high speed camera  Better fixture (sweep over large frequency range)  Future work  Apply to composite plates (anisotropy)  Test on more complex structures

23/23 A. Giraudeau, F. Pierron MPSVA conference Thank you for your attention Sponsored by the Champagne-Ardenne Regional Council