Measurement of local elastic modulus with CLUE

Size: px
Start display at page:

Download "Measurement of local elastic modulus with CLUE"

Transcription

1 Measurement of local elastic modulus with CLUE Alexander A.Karabutov 1, Alexander A.Karabutov (Jr.) 2, Elena V.Savateeva 3 1 International Laser Center of Moscow State University aak@ilc.edu.ru 2 Deptm.of Physics of Moscow State University, akarabutov@gmail.com 3 Institute for laser information technology RAS evsav73@mail.ru

2 Abstracts The problem of local elastic properties measurement at part of construction is of great importance for estimation of active stresses and life service, especially for composites. Contact Laser-Ultrasonic Evaluation (CLUE) makes it possible to measure acoustic wave velocity with high precision at short path. Comparison with theoretical model of the stiffness matrix enables one to measure the complete set of elastic modulus. We measure the elastic modulus of isotropic solids and 1-D carbon fiber reinforced composite. For isotropic medium the velocity of longitudinal and shear wave was measured simultaneously. For the samples with the thickness greater, then 2 mm the accuracy was as high as (0.1-1)%. The resolution in lateral direction was ~3mm. For orthotropic 1-D CFRC opto-acoustic transducers of different schemes were explored to measure the ultrasonic wave velocity, propagating at different angles to the fibers. The accuracy of 1% was provided for the measurements. The applications of elastic modulus measurement with CLUE are discussed.

3 Ultrasonic measurement of elastic modulus Modulus of elasticity E c 2 s 3c 4c 2 2 L s c c 2 2 L s Shear modulus G c 2 s Poisson ratio c 2c 2 2 L s 2 2 2( cl cs)

4 Precise time-resolved measurement of ultrasonic wave velocity Amplitude of signals, Volts 1.0 3t t Time-delay between echo signals can be measured with high accuracy 0.2 t = 2h/c , m

5 sample Contact Laser Ultrasound Evaluation. Optical fiber Laser DPSS Q-switched laser pulse is absorbed in optoacoustic generator/ Laser Irradiation exited wideband probe ultrasonic pulse propagates to a sample under investigation/ Data acquisition system Optoacoustic generator probe pulse is scattered at the sample structures/ wideband piezotransducer detects backscattered ultrasound waves/ Backscattered signals deliver the information about the sample, namely, on the acoustic properties of different structures of the sample.

6 Comparison of Laser and Piezo UT 1 0, s 0.58 s 0-0,5-1 z piezo >(6-7)z CLUE Laser UT Piezo UT 0 0,5 1 1,5 2 2,5 3 3,5 4 Time, s In-depth resolution of UT is determined by probe pulse duration. CLUE pulse duration is 6-7 times shorter then that for traditional UT at the same central frequency.

7 Advantages of CLUE Short duration of a probe ultrasonic pulse enhanced in-depth resolution for limited frequency band Smooth temporal shape of a probe ultrasonic pulse no deadzone, discrimination of soft and rigid impurities Small diameter of a probe ultrasonic beam enhanced sensitivity of small defect detection

8 Sensitivity, V/bar LASER-ULTRASONIC DEFECTOSCOPE UDL-2M Specific features Short UT pulses are excited in a course of laser pulse absorption in a Laser-Ultrasonic transducer. Back-scattered UT signals are detected with ultra wide-band piezo-receiver. It makes it possible to enhance spatial resolution and to reduce dead-zone. Probe Ultrasonic pulse Spectral sensitivity of detection ,8 50 0,6 0 0,4-50 0,2 4,2 4,4 4,6 4,8 5 5,2 5,4 Время (мкс) Time, s Частота (МГц) Frequency, MHz

9 Measurement of elastic modulus in echo-regime with CLUE Probe pulse Ultrasonic trace Time H/C S +H/C L 2H/C L 2H/C L OA-Generator L L L L S Sample

10 Measurement of Elastic Modulus with UDL-2M Longitudinal Pulses Sample thickness (1-20) mm, Beam diameter 2 mm, Relative error of C L 0.1% Relative error of C S 1% Scatter of C L 0.02% Sear Pulse

11 Ultrasonic wave velocity in stressed medium Stress-free medium Calculation of stresses Acousto-elastic effect ) ( ) 2 ( 2 yy xx zz z B A V ) 2 ( 2 0 V z z z z z zz yy z z z xz xx V V V B V V V A

12 Ultrasonic Velocity in Stressed Al y Width z x Base , dv 5 1 V velocity 0.8*10 d MPa 0,08 0, , deformation 0, Stress xx, MPa

13 Residual stress distribution in weld Stainless steel 250 MPa

14 Laser-Ultrasonic Tomography of Mechanical Modulus To measure the complete set of elastic modulus of anisotropic solid it s necessary to determine the velocity of all types of acoustic wave quasi-longitudinal, quasi-shear propagating in various directions. The optoacoustic transducer discussed above provides the excitation of longitudinal wave normal to the surface. So, it s necessary to design the transducers provided measurement of the velocity of acoustic wave of another types and directions of propagation. They are discussed below.

15 Rayleigh wave velocity measurement with CLUE Opto - electronic unit Laptop fiber signal cable power cable ОА- Transducer Specific features Short SAW pulse is excited in a course of laser pulse absorption at a metal surface under testing. SAW pulse is detected with point-like piezo-receiver. Laser excitation and piezo-detection of SAW pulse is combined in a Optoacoustic Transducer. Optical fiber fiber adapter preamplifier Optoacoustic transducer

16 Ultrasonic Trace detected by LUIT 6 4 U, mv Shear wave signal Rayleigh wave signal Time, s The base of measurement 15 mm, ultrasonic beam width 2 mm, relative error of SAW velocity measurement ~ 1%, scatter %

17 SAW Velocity in Stressed Metal Stainless steel 12X18H10T 0,025 y = -5,0768e ,019e-05x R= 0, ,02 0,015 0,01 velocity variation 0, Stress, MPa

18 z y x Width CLUE of Residual Stress in Al Base Sample #07 (Al-ST) Al7050 6,28 2,84 6,275 2,835 6,27 2,83 6,265 2,825 6,26 CLZ, mm/us CRX, mm/us X, mm 2,82 Homogeneous sample Sample with residual stress Distribution of C LZ and C RX along the sample.

19 Measurement of longitudinal wave velocity with inclined probe ultrasonic beam Base 30 mm Beam width 3 mm Relative error of C L 1% Scheme of optoacoustic transducer PLU-6H-02.

20 Stressed state of rail

21 CONCLUSIONS Contact Laser-Ultrasonic Evaluation (CLUE) makes it possible a measurement of elastic modulus locally. The accuracy is better then 1%. Investigation of stressed state of solid can be realized effectively with CLUE. 3-D distribution of stress with Laser-Ultrasonic Tomography is discussed.

MEASUREMENT OF LOCAL POROSITY OF PARTICLES REINFORCED COMPOSITES WITH THE LASER OPTOACOUSTIC METHOD

MEASUREMENT OF LOCAL POROSITY OF PARTICLES REINFORCED COMPOSITES WITH THE LASER OPTOACOUSTIC METHOD MEASUREMENT OF LOCAL POROSITY OF PARTICLES REINFORCED COMPOSITES WITH THE LASER OPTOACOUSTIC METHOD A.A. KARABUTOV, N.B. PODYMOVA, L.I. KOBELEVA*, T.A. CHERNYSHOVA* INTERNATIONAL LASER CENTER, M.V. LOMONOSOV

More information

6th NDT in Progress Lamb waves in an anisotropic plate of a single crystal silicon wafer

6th NDT in Progress Lamb waves in an anisotropic plate of a single crystal silicon wafer 6th NDT in Progress 2011 International Workshop of NDT Experts, Prague, 10-12 Oct 2011 Lamb waves in an anisotropic plate of a single crystal silicon wafer Young-Kyu PARK 1, Young H. KIM 1 1 Applied Acoustics

More information

NDT&E Methods: UT. VJ Technologies CAVITY INSPECTION. Nondestructive Testing & Evaluation TPU Lecture Course 2015/16.

NDT&E Methods: UT. VJ Technologies CAVITY INSPECTION. Nondestructive Testing & Evaluation TPU Lecture Course 2015/16. CAVITY INSPECTION NDT&E Methods: UT VJ Technologies NDT&E Methods: UT 6. NDT&E: Introduction to Methods 6.1. Ultrasonic Testing: Basics of Elasto-Dynamics 6.2. Principles of Measurement 6.3. The Pulse-Echo

More information

Measurement of acousto-elastic effect by using surface acoustic wave

Measurement of acousto-elastic effect by using surface acoustic wave Measurement of acousto-elastic effect by using surface acoustic wave Y. D. Shim¹, J. H. Jun¹, S. M. Kim¹, J. You², C. H. Lim², H. C. Hyun² and K. -Y. Jhang¹ 1 School of Mechanical Engineering, Hanyang

More information

Nanoacoustics II Lecture #2 More on generation and pick-up of phonons

Nanoacoustics II Lecture #2 More on generation and pick-up of phonons Nanoacoustics II Lecture #2 More on generation and pick-up of phonons Dr. Ari Salmi www.helsinki.fi/yliopisto 26.3.2018 1 Last lecture key points Coherent acoustic phonons = sound at nanoscale Incoherent

More information

A FEM STUDY ON THE INFLUENCE OF THE GEOMETRIC CHARACTERISTICS OF METALLIC FILMS IRRADIATED BY NANOSECOND LASER PULSES

A FEM STUDY ON THE INFLUENCE OF THE GEOMETRIC CHARACTERISTICS OF METALLIC FILMS IRRADIATED BY NANOSECOND LASER PULSES 8 th GRACM International Congress on Computational Mechanics Volos, 12 July 15 July 2015 A FEM STUDY ON THE INFLUENCE OF THE GEOMETRIC CHARACTERISTICS OF METALLIC FILMS IRRADIATED BY NANOSECOND LASER PULSES

More information

On the study of elastic wave scattering and Rayleigh wave velocity measurement of concrete with steel bar

On the study of elastic wave scattering and Rayleigh wave velocity measurement of concrete with steel bar NDT&E International 33 (2000) 401 407 www.elsevier.com/locate/ndteint On the study of elastic wave scattering and Rayleigh wave velocity measurement of concrete with steel bar T.-T. Wu*, J.-H. Sun, J.-H.

More information

Shear waves in solid-state materials

Shear waves in solid-state materials Shear waves in solid-state materials TEAS Related topics Ultrasonic transmission measurement, propagation of ultrasound waves, ultrasound wave modes, shear waves, longitudinal and transverse waves, modulus

More information

APPLICATION-DIRECTED MODELING OF RADIATION AND PROPAGATION OF ELASTIC WAVES IN ANISOTROPIC MEDIA: GPSS AND OPOSSM

APPLICATION-DIRECTED MODELING OF RADIATION AND PROPAGATION OF ELASTIC WAVES IN ANISOTROPIC MEDIA: GPSS AND OPOSSM APPLICATION-DIRECTED MODELING OF RADIATION AND PROPAGATION OF ELASTIC WAVES IN ANISOTROPIC MEDIA: GPSS AND OPOSSM M. Spies, F. Walte Fraunhofer-Institute for Nondestructive Testing (IzfP) 66123 Saarbriicken,

More information

Principle and application of ultrasonic wave

Principle and application of ultrasonic wave Topics on ultrasonic wave Principle and application of ultrasonic wave Writer Handong Li ( ) Emendator: Yabin Zhu ( ) 1 brief introduction to the special subject Ultrasonic wave is an acoustic wave whose

More information

Supplement (videos)

Supplement (videos) Supplement (videos) Ruben s tube (sound): http://www.youtube.com/watch?v=gpcquuwqayw Doppler US (diagnostic use): http://www.youtube.com/watch?v=fgxzg-j_hfw http://www.youtube.com/watch?v=upsmenyoju8 High

More information

Doppler echocardiography & Magnetic Resonance Imaging. Doppler echocardiography. History: - Langevin developed sonar.

Doppler echocardiography & Magnetic Resonance Imaging. Doppler echocardiography. History: - Langevin developed sonar. 1 Doppler echocardiography & Magnetic Resonance Imaging History: - Langevin developed sonar. - 1940s development of pulse-echo. - 1950s development of mode A and B. - 1957 development of continuous wave

More information

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich UNIVERSITY OF SASKATCHEWAN ME 313.3 MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich A CLOSED BOOK EXAMINATION TIME: 3 HOURS For Marker s Use Only LAST NAME (printed): FIRST

More information

EFIT SIMULATIONS FOR ULTRASONIC NDE

EFIT SIMULATIONS FOR ULTRASONIC NDE EFIT SIMULATIONS FOR ULTRASONIC NDE René Marklein, Karl-Jörg Langenberg, Klaus Mayer (University of Kassel, Department of Electrical and Computer Engineering, Electromagnetic Field Theory, Wilhelmshöher

More information

LECTURE NO. 4-5 INTRODUCTION ULTRASONIC * PULSE VELOCITY METHODS

LECTURE NO. 4-5 INTRODUCTION ULTRASONIC * PULSE VELOCITY METHODS LECTURE NO. 4-5 ULTRASONIC * PULSE VELOCITY METHODS Objectives: To introduce the UPV methods To briefly explain the theory of pulse propagation through concrete To explain equipments, procedures, calibrations,

More information

Tensile Stress Acoustic Constants of Unidirectional Graphite/Epoxy Composites

Tensile Stress Acoustic Constants of Unidirectional Graphite/Epoxy Composites Tensile Stress Acoustic Constants of Unidirectional Graphite/Epoxy Composites Journal of Reinforced Plastics and Composites, Vol. 9 (March, 1990) pp. 127-133 W. H. PROSSER NASA Langley Research Center

More information

Measurement of Elastic Constants Using Ultrasound

Measurement of Elastic Constants Using Ultrasound MCEN 3027 Updated 02/26/2001 Measurement of Elastic Constants Using Ultrasound Introduction Ultrasound uses very high frequency sound, higher than 20 khz (the limit of human hearing), to determine material

More information

SIMULATION OF ULTRASONIC NDT IN COMPOSITE RADIUS

SIMULATION OF ULTRASONIC NDT IN COMPOSITE RADIUS SIMULATION OF ULTRASONIC NDT IN COMPOSITE RADIUS N. Dominguez 1, O. Grellou 2, S. Van-der-Veen 2 1 European Aeronautic Defense and Space Company (EADS), Innovation Works Dept., 1 rue Marius Terce, 325

More information

Basic Equations of Elasticity

Basic Equations of Elasticity A Basic Equations of Elasticity A.1 STRESS The state of stress at any point in a loaded bo is defined completely in terms of the nine components of stress: σ xx,σ yy,σ zz,σ xy,σ yx,σ yz,σ zy,σ zx,andσ

More information

ULTRASONIC WAVE PROPAGATION IN DISSIMILAR METAL WELDS APPLICATION OF A RAY-BASED MODEL AND COMPARISON WITH EXPERIMENTAL RESULTS

ULTRASONIC WAVE PROPAGATION IN DISSIMILAR METAL WELDS APPLICATION OF A RAY-BASED MODEL AND COMPARISON WITH EXPERIMENTAL RESULTS ULTRASONIC WAVE PROPAGATION IN DISSIMILAR METAL WELDS APPLICATION OF A RAY-BASED MODEL AND COMPARISON WITH EXPERIMENTAL RESULTS Audrey GARDAHAUT 1, Hugues LOURME 1, Frédéric JENSON 1, Shan LIN 2, Masaki

More information

Evaluation of transverse elastic properties of fibers used in composite materials by laser resonant ultrasound spectroscopy

Evaluation of transverse elastic properties of fibers used in composite materials by laser resonant ultrasound spectroscopy Evaluation of transverse elastic properties of fibers used in composite materials by laser resonant ultrasound spectroscopy Denis Mounier, Christophe Poilâne, Cécile Bûcher, Pascal Picart To cite this

More information

Finite element simulation of the critically refracted longitudinal wave in a solid medium

Finite element simulation of the critically refracted longitudinal wave in a solid medium Finite element simulation of the critically refracted in a solid medium Weina Ke, Salim Chaki To cite this version: Weina Ke, Salim Chaki. Finite element simulation of the critically refracted in a solid

More information

SPECTRAL FINITE ELEMENT METHOD

SPECTRAL FINITE ELEMENT METHOD SPECTRAL FINITE ELEMENT METHOD Originally proposed by Patera in 1984 for problems in fluid dynamics Adopted for problems of propagation of acoustic and seismic waves Snapshot of the propagation of seismic

More information

The Relationship between the Applied Torque and Stresses in Post-Tension Structures

The Relationship between the Applied Torque and Stresses in Post-Tension Structures ECNDT 6 - Poster 218 The Relationship between the Applied Torque and Stresses in Post-Tension Structures Fui Kiew LIEW, Sinin HAMDAN * and Mohd. Shahril OSMAN, Faculty of Engineering, Universiti Malaysia

More information

IDENTIFICATION OF ELASTIC PROPERTIES OF MATERIALS OF LARGER BODIES. IDENTIFIKACE ELASTICKÝCH VLASTNOSTÍ MATERIÁLU ROZMĚRNĚJŠÍCH TĚLES.

IDENTIFICATION OF ELASTIC PROPERTIES OF MATERIALS OF LARGER BODIES. IDENTIFIKACE ELASTICKÝCH VLASTNOSTÍ MATERIÁLU ROZMĚRNĚJŠÍCH TĚLES. 40. MEZINÁRODNÍ KONFERENCE EXPERIMENTÁLNÍ ANALÝZY NAPĚTÍ 40 th INTERNATIONAL CONFERENCE EXPERIMENTAL STRESS ANALYSIS 3. 6. VI. 2002, PRAHA/PRAGUE, CZECH REPUBLIC IDENTIFICATION OF ELASTIC PROPERTIES OF

More information

Simulation of an Ultrasonic Immersion Test for the Characterization of Anisotropic Materials

Simulation of an Ultrasonic Immersion Test for the Characterization of Anisotropic Materials DIPARTIMENTO DI SCIENZE DELL INGEGNERIA CIVILE E DELL ARCHITETTURA POLITECNICO DI BARI Simulation of an Ultrasonic Immersion Test for the Characterization of Anisotropic Materials A. Castellano*, P. Foti,

More information

Graduate School of Engineering, Kyoto University, Kyoto daigaku-katsura, Nishikyo-ku, Kyoto, Japan.

Graduate School of Engineering, Kyoto University, Kyoto daigaku-katsura, Nishikyo-ku, Kyoto, Japan. On relationship between contact surface rigidity and harmonic generation behavior in composite materials with mechanical nonlinearity at fiber-matrix interface (Singapore November 2017) N. Matsuda, K.

More information

Chapter 2 Surface Acoustic Wave Motor Modeling and Motion Control

Chapter 2 Surface Acoustic Wave Motor Modeling and Motion Control Chapter 2 Surface Acoustic Wave Motor Modeling and Motion Control 1 Abstract For miniaturization of ultrasonic transducers, a surface acoustic wave device has an advantage in rigid mounting and high-power-density

More information

6.730 Physics for Solid State Applications

6.730 Physics for Solid State Applications 6.730 Physics for Solid State Applications Lecture 5: Specific Heat of Lattice Waves Outline Review Lecture 4 3-D Elastic Continuum 3-D Lattice Waves Lattice Density of Modes Specific Heat of Lattice Specific

More information

Application of subsurface laser engraving in ultrasonic testing of materials

Application of subsurface laser engraving in ultrasonic testing of materials 11th European Conference on Non-Destructive Testing (ECNDT 2014), October 6-10, 2014, Prague, Czech Republic Application of subsurface laser engraving in ultrasonic testing of materials Jacek SZELĄŻEK

More information

Practical Results of Ultrasonic Imaging by Inverse Wave Field Extrapolation

Practical Results of Ultrasonic Imaging by Inverse Wave Field Extrapolation ECNDT 2006 - Th.2.3.1 Practical Results of Ultrasonic Imaging by Inverse Wave Field Extrapolation Niels PÖRTZGEN, RTD Group, Rotterdam, The Netherlands Abstract: Array technology in non-destructive inspection

More information

VISUALIZATION OF SOUND PROPAGATION WITH ELECTRODYNAMIC PROBES

VISUALIZATION OF SOUND PROPAGATION WITH ELECTRODYNAMIC PROBES VISUALIZATION OF SOUND PROPAGATION WITH ELECTRODYNAMIC PROBES Uwe VÖLZ, Heinz MRASEK, Klaus MATTHIES, Marc KREUTZBRUCK BAM Federal Institute for Materials Research and Testing, 12200 Berlin, Germany Abstract.

More information

For more information, please contact

For more information, please contact PhASE PhotoAcoustic Schlieren Elastography Design Team Hannah A. Gibson, Will A. Goth Briana J. Moretti, Zakary T. Smith Design Advisor Prof. Gregory Kowalski MIE Department Sponsor Prof. Charles DiMarzio

More information

Finite Element Modeling of Ultrasonic Transducers for Polymer Characterization

Finite Element Modeling of Ultrasonic Transducers for Polymer Characterization Excerpt from the Proceedings of the COMSOL Conference 2009 Milan Finite Element Modeling of Ultrasonic Transducers for Polymer Characterization Serena De Paolis *, Francesca Lionetto and Alfonso Maffezzoli

More information

FEA Based Simulation of Ultrasonic Wave Propagation in Isotropic and Orthotropic Media

FEA Based Simulation of Ultrasonic Wave Propagation in Isotropic and Orthotropic Media 19 th World Conference on Non-Destructive Testing 016 FEA Based Simulation of Ultrasonic Wave Propagation in Isotropic and Orthotropic Media Debasis DATTA 1 1 Indian Institute of Engineering Science and

More information

Riccardo M.G. Ferrari, PhD Danieli Automation S.p.A. (Buttrio, Italy)

Riccardo M.G. Ferrari, PhD Danieli Automation S.p.A. (Buttrio, Italy) Presented at the COMSOL Conference 2009 Milan Milan, October 14 th -16 th 2009 Riccardo M.G. Ferrari, PhD Danieli Automation S.p.A. (Buttrio, Italy) Introduction The [HK53, TB64] relates the change of

More information

SCSVMV UNIVERSITY,ENGINEERING PHYSICS

SCSVMV UNIVERSITY,ENGINEERING PHYSICS SCSVMV UNIVERSITY,ENGINEERING PHYSICS TWO MARK QUESTION BANK(Common to all branches) UNIT 1 PROPERTIES OF MATTER 1. Define Elasticity. 2. State Hooke s law. 3. What is meant by stress and strain? 4. Give

More information

ULTRASONIC TESTING OF RAILS INCLUDING VERTICAL CRACKS-

ULTRASONIC TESTING OF RAILS INCLUDING VERTICAL CRACKS- ULTRASONIC TESTING OF RAILS INCLUDING VERTICAL CRACKS- NUMERICAL MODELING AND EXPERIMENTAL RESULTS INTRODUCTION F. Schubert, B. Koehler Fraunhofer-IZFP, Branch Lab EADQ Kruegerstrasse 22 D-01326 Dresden

More information

Lamb Waves in Plate Girder Geometries

Lamb Waves in Plate Girder Geometries Lamb Waves in Plate Girder Geometries D.W. Greve, 1 N. L. Tyson 2, and I.J. Oppenheim 2 1 Electrical and Computer Engineering, Carnegie Mellon University, Pittsburgh, PA, 15213 2 Civil and Environmental

More information

PROPERTY STUDY ON EMATS WITH VISUALIZATION OF ULTRASONIC PROPAGATION

PROPERTY STUDY ON EMATS WITH VISUALIZATION OF ULTRASONIC PROPAGATION More Info at Open Access Database www.ndt.net/?id=18576 PROPERTY STUDY ON EMATS WITH VISUALIZATION OF ULTRASONIC PROPAGATION T. Yamamoto, T. Furukawa, I. Komura Japan Power Engineering and Inspection Corporation,

More information

Nanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems

Nanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems Nanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems Photonics group W. Claeys, S. Dilhair, S. Grauby, JM. Rampnoux, L. Patino Lopez,

More information

Available online at ScienceDirect. Physics Procedia 63 (2015 ) 54 60

Available online at   ScienceDirect. Physics Procedia 63 (2015 ) 54 60 Available online at www.sciencedirect.com ScienceDirect Physics Procedia 63 (2015 ) 54 60 43 rd Annual Symposium of the Ultrasonic Industry Association, UIA Symposium 2014 Phase velocity method for guided

More information

Measuring vibration characteristics at large amplitude region of materials for high power ultrasonic vibration system

Measuring vibration characteristics at large amplitude region of materials for high power ultrasonic vibration system Ultrasonics 38 (2000) 122 126 www.elsevier.nl/locate/ultras Measuring vibration characteristics at large amplitude region of materials for high power ultrasonic vibration system Kentaro Nakamura *, Kiyotsugu

More information

CRACK-TIP DIFFRACTION IN A TRANSVERSELY ISOTROPIC SOLID. A.N. Norris and J.D. Achenbach

CRACK-TIP DIFFRACTION IN A TRANSVERSELY ISOTROPIC SOLID. A.N. Norris and J.D. Achenbach CRACK-TIP DIFFRACTION IN A TRANSVERSELY ISOTROPIC SOLID A.N. Norris and J.D. Achenbach The Technological Institute Northwestern University Evanston, IL 60201 ABSTRACT Crack diffraction in a transversely

More information

Application of Ultra-Sonic Pulse Velocity Techniques for Concrete Quality Measurements

Application of Ultra-Sonic Pulse Velocity Techniques for Concrete Quality Measurements Application of Ultra-Sonic Pulse Velocity Techniques for Concrete Quality Measurements Uday Bhise, Engineer. NDT; Durocrete Engineering Services Pvt. Ltd. Introduction This method of testing was originally

More information

Research on sound absorbing mechanism and the preparation of new backing material for ultrasound transducers

Research on sound absorbing mechanism and the preparation of new backing material for ultrasound transducers Research on sound absorbing mechanism and the preparation of new backing material for ultrasound transducers Guofeng Bai a) Xiujuan Zhang b) Fusheng Sui c) Jun Yang d) Key Laboratory of Noise and Vibration

More information

FROM NEAR FIELD TO FAR FIELD AND BEYOND

FROM NEAR FIELD TO FAR FIELD AND BEYOND More info about this article: h Czech Society for Nondestructive Testing 32 nd European Conference on Acoustic Emission Testing Prague, Czech Republic, September 07-09, 2016 FROM NEAR FIELD TO FAR FIELD

More information

MECH 5312 Solid Mechanics II. Dr. Calvin M. Stewart Department of Mechanical Engineering The University of Texas at El Paso

MECH 5312 Solid Mechanics II. Dr. Calvin M. Stewart Department of Mechanical Engineering The University of Texas at El Paso MECH 5312 Solid Mechanics II Dr. Calvin M. Stewart Department of Mechanical Engineering The University of Texas at El Paso Table of Contents Thermodynamics Derivation Hooke s Law: Anisotropic Elasticity

More information

Nonlinear effects in ultrasound fields of diagnostic-type transducers used for kidney stone propulsion: characterization in water

Nonlinear effects in ultrasound fields of diagnostic-type transducers used for kidney stone propulsion: characterization in water The 2th International Symposium on Nonlinear Acoustics, Lyon, June 29 th, 21 Nonlinear effects in ultrasound fields of diagnostic-type transducers used for kidney stone propulsion: characterization in

More information

Sub. Code:

Sub. Code: Important Instructions to examiners: ) The answers should be examined by key words and not as word-to-word as given in the model answer scheme. ) The model answer and the answer written by candidate may

More information

MEASUREMENT OF ACOUSTOELASTIC EFFECT OF RAYLEIGH SURFACE WAVES USING LASER ULTRASONICS

MEASUREMENT OF ACOUSTOELASTIC EFFECT OF RAYLEIGH SURFACE WAVES USING LASER ULTRASONICS MEASUREMENT OF ACOUSTOELASTIC EFFECT OF RAYLEIGH SURFACE WAVES USING LASER ULTRASONICS INTRODUCTION W-Y Lu and L. W. Peng Materials and Engineering Sciences Center Sandia National Laboratories Livermore,

More information

Sound Propagation through Media. Nachiketa Tiwari Indian Institute of Technology Kanpur

Sound Propagation through Media. Nachiketa Tiwari Indian Institute of Technology Kanpur Sound Propagation through Media Nachiketa Tiwari Indian Institute of Technology Kanpur LECTURE-13 WAVE PROPAGATION IN SOLIDS Longitudinal Vibrations In Thin Plates Unlike 3-D solids, thin plates have surfaces

More information

PHASED-ARRAY FOCUSING WITH LONGITUDINAL GUIDED WAVES IN A VISCOELASTIC COATED HOLLOW CYLINDER

PHASED-ARRAY FOCUSING WITH LONGITUDINAL GUIDED WAVES IN A VISCOELASTIC COATED HOLLOW CYLINDER PHASED-ARRAY FOCUSING WITH LONGITUDINAL GUIDED WAVES IN A VISCOELASTIC COATED HOLLOW CYLINDER W. Luo, J. L. Rose, J. K. Van Velsor, J. Mu Department of Engineering Science & Mechanics, The Pennsylvania

More information

SUBSURFACE WAVES IN SOLIDS WITH CURVED SURFACE AND ACOUSTICAL IMPEDANCE ON IT

SUBSURFACE WAVES IN SOLIDS WITH CURVED SURFACE AND ACOUSTICAL IMPEDANCE ON IT SUBSURFACE WAVES IN SOLIDS WITH CURVED SURFACE AND ACOUSTICAL IMPEDANCE ON IT A. Baev, P. Prokhorenko, and M. Asadchaya Institute of Applied Physics, Minsk, Belarus Abstract: This paper presents the results

More information

Recurrent scattering and memory effect at the Anderson transition

Recurrent scattering and memory effect at the Anderson transition Recurrent scattering and memory effect at the Anderson transition Alexandre Aubry Institut Langevin CNRS UMR 7587, ESPCI ParisTech Paris, France Collaborators: John Page, Laura Cobus (University of Manitoba,

More information

Introduction to SAWAVE. A 3D-Based Surface Acoustic Wave (SAWAVE) Device Simulator

Introduction to SAWAVE. A 3D-Based Surface Acoustic Wave (SAWAVE) Device Simulator Introduction to SAWAVE A 3D-Based Surface Acoustic Wave (SAWAVE) Device Simulator SAWAVE FV Data Structure Unstructured Finite Volume (FV) mesh allows unparalleled flexibility in 3D structure definition.

More information

Extensional and Flexural Waves in a Thin-Walled Graphite/Epoxy Tube * William H. Prosser NASA Langley Research Center Hampton, VA 23665

Extensional and Flexural Waves in a Thin-Walled Graphite/Epoxy Tube * William H. Prosser NASA Langley Research Center Hampton, VA 23665 Extensional and Flexural Waves in a Thin-Walled Graphite/Epoxy Tube * William H. Prosser NASA Langley Research Center Hampton, VA 23665 Michael R. Gorman Aeronautics and Astronautics Naval Postgraduate

More information

TABLE OF CONTENTS. Mechanics of Composite Materials, Second Edition Autar K Kaw University of South Florida, Tampa, USA

TABLE OF CONTENTS. Mechanics of Composite Materials, Second Edition Autar K Kaw University of South Florida, Tampa, USA Mechanics of Composite Materials, Second Edition Autar K Kaw University of South Florida, Tampa, USA TABLE OF CONTENTS 1. INTRODUCTION TO COMPOSITE MATERIALS 1.1 Introduction... 1.2 Classification... 1.2.1

More information

Lamb Wave Behavior in Bridge Girder Geometries

Lamb Wave Behavior in Bridge Girder Geometries Lamb Wave Behavior in Bridge Girder Geometries I. J. Oppenheim a*, D. W. Greve b, N. L. Tyson a a Dept. of Civil and Environmental Engineering, Carnegie Mellon University, Pittsburgh, PA 15213 b Dept.

More information

Module III - Macro-mechanics of Lamina. Lecture 23. Macro-Mechanics of Lamina

Module III - Macro-mechanics of Lamina. Lecture 23. Macro-Mechanics of Lamina Module III - Macro-mechanics of Lamina Lecture 23 Macro-Mechanics of Lamina For better understanding of the macromechanics of lamina, the knowledge of the material properties in essential. Therefore, the

More information

Optimisation using measured Green s function for improving spatial coherence in acoustic measurements

Optimisation using measured Green s function for improving spatial coherence in acoustic measurements Ultrasonics 42 (2004) 205 212 www.elsevier.com/locate/ultras Optimisation using measured Green s function for improving spatial coherence in acoustic measurements Matthew Clark *, Steve D. Sharples, Mike

More information

Problem " Â F y = 0. ) R A + 2R B + R C = 200 kn ) 2R A + 2R B = 200 kn [using symmetry R A = R C ] ) R A + R B = 100 kn

Problem  Â F y = 0. ) R A + 2R B + R C = 200 kn ) 2R A + 2R B = 200 kn [using symmetry R A = R C ] ) R A + R B = 100 kn Problem 0. Three cables are attached as shown. Determine the reactions in the supports. Assume R B as redundant. Also, L AD L CD cos 60 m m. uation of uilibrium: + " Â F y 0 ) R A cos 60 + R B + R C cos

More information

Lecture 8. Stress Strain in Multi-dimension

Lecture 8. Stress Strain in Multi-dimension Lecture 8. Stress Strain in Multi-dimension Module. General Field Equations General Field Equations [] Equilibrium Equations in Elastic bodies xx x y z yx zx f x 0, etc [2] Kinematics xx u x x,etc. [3]

More information

Fig. 1. Circular fiber and interphase between the fiber and the matrix.

Fig. 1. Circular fiber and interphase between the fiber and the matrix. Finite element unit cell model based on ABAQUS for fiber reinforced composites Tian Tang Composites Manufacturing & Simulation Center, Purdue University West Lafayette, IN 47906 1. Problem Statement In

More information

Nondestructive Determination of Elastic Constants of Thin Plates Based on PVDF Focusing Ultrasound Transducers and Lamb Wave Measurements

Nondestructive Determination of Elastic Constants of Thin Plates Based on PVDF Focusing Ultrasound Transducers and Lamb Wave Measurements 17th World Conference on Nondestructive Testing, 25-28 Oct 2008, Shanghai, China Nondestructive Determination of Elastic Constants of Thin Plates Based on PVDF Focusing Ultrasound Transducers and Lamb

More information

ULTRASONIC INVESTIGATION OF THE STIFFNESS OF GRAPHITE-

ULTRASONIC INVESTIGATION OF THE STIFFNESS OF GRAPHITE- ULTRASONIC INVESTIGATION OF THE STIFFNESS OF GRAPHITE- GRAPHITE INTERFACES A. M. Robinson, B. W. Drinkwater Department of Mechanical Engineering, Queen's Building, University Walk, University of Bristol,

More information

Signal Loss. A1 A L[Neper] = ln or L[dB] = 20log 1. Proportional loss of signal amplitude with increasing propagation distance: = α d

Signal Loss. A1 A L[Neper] = ln or L[dB] = 20log 1. Proportional loss of signal amplitude with increasing propagation distance: = α d Part 6 ATTENUATION Signal Loss Loss of signal amplitude: A1 A L[Neper] = ln or L[dB] = 0log 1 A A A 1 is the amplitude without loss A is the amplitude with loss Proportional loss of signal amplitude with

More information

Modeling of Acoustic Wave Propagation in Layered Solids and Its Application in Heat Assisted Magnetic Recording

Modeling of Acoustic Wave Propagation in Layered Solids and Its Application in Heat Assisted Magnetic Recording Modeling of Acoustic Wave Propagation in Layered Solids and Its Application in Heat Assisted Magnetic Recording Wei Peng, Yiao-Tee Hsia, Julius Hohlfeld Seagate Technology Abstract In multi-layered solids,

More information

ELASTICITY (MDM 10203)

ELASTICITY (MDM 10203) LASTICITY (MDM 10203) Lecture Module 5: 3D Constitutive Relations Dr. Waluyo Adi Siswanto University Tun Hussein Onn Malaysia Generalised Hooke's Law In one dimensional system: = (basic Hooke's law) Considering

More information

Stress and Energy Transmission by Inhomogeneous Plane Waves into Dissipative Media

Stress and Energy Transmission by Inhomogeneous Plane Waves into Dissipative Media Purdue University Purdue e-pubs Publications of the Ray W. Herrick Laboratories School of Mechanical Engineering 11-6-2015 Stress and Energy Transmission by Inhomogeneous Plane Waves into Dissipative Media

More information

Lecture #2 Nanoultrasonic imaging

Lecture #2 Nanoultrasonic imaging Lecture #2 Nanoultrasonic imaging Dr. Ari Salmi www.helsinki.fi/yliopisto 24.1.2014 1 Background Matemaattis-luonnontieteellinen tiedekunta / Henkilön nimi / Esityksen nimi www.helsinki.fi/yliopisto 24.1.2014

More information

Nondestructive Monitoring of Setting and Hardening of Portland Cement Mortar with Sonic Methods

Nondestructive Monitoring of Setting and Hardening of Portland Cement Mortar with Sonic Methods Nondestructive Monitoring of Setting and Hardening of Portland Cement Mortar ith Sonic Methods Thomas Voigt, Northestern University, Evanston, USA Surendra P. Shah, Northestern University, Evanston, USA

More information

Ultra-High Spatial Resolution in Distributed Fibre Sensing

Ultra-High Spatial Resolution in Distributed Fibre Sensing Presentation of EPFL-Group for Fibre Optics: Ultra-High Spatial Resolution in Distributed Fibre Sensing Prof. Luc THEVENAZ & co-workers 2 Postdoc, 4 PhD students, 3 visiting students 1/5 Adm. Assistant

More information

MEASUREMENT OF REFLECTANCE FUNCTION FOR LAYERED STRUCTURES USING FOCUSED ACOUSTIC WAVES INTRODUCTION

MEASUREMENT OF REFLECTANCE FUNCTION FOR LAYERED STRUCTURES USING FOCUSED ACOUSTIC WAVES INTRODUCTION MEASUREMENT OF REFLECTANCE FUNCTION FOR LAYERED STRUCTURES USING FOCUSED ACOUSTIC WAVES w.-j. Xu and M. Ourak Institut d'electronique et de Microelectronique du Nord Departement Opto-Acousto-Electronique

More information

INCREASING RUPTURE PREDICTABILITY FOR ALUMINUM

INCREASING RUPTURE PREDICTABILITY FOR ALUMINUM 1 INCREASING RUPTURE PREDICTABILITY FOR ALUMINUM Influence of anisotropy Daniel Riemensperger, Adam Opel AG Paul Du Bois, PDB 2 www.opel.com CONTENT Introduction/motivation Isotropic & anisotropic material

More information

3.22 Mechanical Properties of Materials Spring 2008

3.22 Mechanical Properties of Materials Spring 2008 MIT OpenCourseWare http://ocw.mit.edu 3.22 Mechanical Properties of Materials Spring 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. Quiz #1 Example

More information

Nonlinear surface acoustic wave pulses in solids: Laser excitation, propagation, interactions invited

Nonlinear surface acoustic wave pulses in solids: Laser excitation, propagation, interactions invited REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 74, NUMBER 1 JANUARY 2003 Nonlinear surface acoustic wave pulses in solids: Laser excitation, propagation, interactions invited Al. A. Kolomenskii, a) V. A. Lioubimov,

More information

Orientation of Piezoelectric Crystals and Acoustic Wave Propagation

Orientation of Piezoelectric Crystals and Acoustic Wave Propagation Orientation of Piezoelectric Crystals and Acoustic Wave Propagation Guigen Zhang Department of Bioengineering Department of Electrical and Computer Engineering Institute for Biological Interfaces of Engineering

More information

Absolute Nonlinear Parameter Estimation using Relative Nonlinear Parameter measured from Surface Acoustic Wave

Absolute Nonlinear Parameter Estimation using Relative Nonlinear Parameter measured from Surface Acoustic Wave Absolute Nonlinear Parameter Estimation using Relative Nonlinear Parameter measured from Surface Acoustic Wave J. H. Jun 1, H. G. Seo 1, Y. D. Shim 1 and K. Y. Jhang 1, School of Mechanical Engineering,

More information

Methods Based on the Phenomenon of Elastic Wave Propagation (Guided Waves) Interaction with Damage

Methods Based on the Phenomenon of Elastic Wave Propagation (Guided Waves) Interaction with Damage Propagation (Guided Waves) Interaction with Damage Wieslaw Ostachowicz Polish Academy of Sciences Institute of Fluid Flow Machinery Department of Mechanics of Intelligent Structures 14 Fiszera Street 80231

More information

MANY BILLS OF CONCERN TO PUBLIC

MANY BILLS OF CONCERN TO PUBLIC - 6 8 9-6 8 9 6 9 XXX 4 > -? - 8 9 x 4 z ) - -! x - x - - X - - - - - x 00 - - - - - x z - - - x x - x - - - - - ) x - - - - - - 0 > - 000-90 - - 4 0 x 00 - -? z 8 & x - - 8? > 9 - - - - 64 49 9 x - -

More information

We briefly discuss two examples for solving wave propagation type problems with finite differences, the acoustic and the seismic problem.

We briefly discuss two examples for solving wave propagation type problems with finite differences, the acoustic and the seismic problem. Excerpt from GEOL557 Numerical Modeling of Earth Systems by Becker and Kaus 2016 1 Wave propagation Figure 1: Finite difference discretization of the 2D acoustic problem. We briefly discuss two examples

More information

MATERIAL PROPERTIES. Material Properties Must Be Evaluated By Laboratory or Field Tests 1.1 INTRODUCTION 1.2 ANISOTROPIC MATERIALS

MATERIAL PROPERTIES. Material Properties Must Be Evaluated By Laboratory or Field Tests 1.1 INTRODUCTION 1.2 ANISOTROPIC MATERIALS . MARIAL PROPRIS Material Properties Must Be valuated By Laboratory or Field ests. INRODUCION he fundamental equations of structural mechanics can be placed in three categories[]. First, the stress-strain

More information

Attenuation and dispersion

Attenuation and dispersion Attenuation and dispersion! Mechanisms: Absorption (inelastic); Scattering (elastic).! Mathematical descriptions! Measurement! Frequency dependence! Dispersion, its relation to attenuation Reading: Sheriff

More information

LAMB WAVES GENERATION USING A TRANSDUCER EMBEDDED IN A COMPOSITE PLATE

LAMB WAVES GENERATION USING A TRANSDUCER EMBEDDED IN A COMPOSITE PLATE LAMB WAVES GENERATION USING A TRANSDUCER EMBEDDED IN A COMPOSITE PLATE Emmanuel Moulin 1, Jamal Assaad 1, Christophe Delebarre 1 and Daniel Osmont 2 1 IEMN, UMR CNRS 9929, OAE Department, Université de

More information

Part 7. Nonlinearity

Part 7. Nonlinearity Part 7 Nonlinearity Linear System Superposition, Convolution re ( ) re ( ) = r 1 1 = r re ( 1 + e) = r1 + r e excitation r = r() e response In the time domain: t rt () = et () ht () = e( τ) ht ( τ) dτ

More information

Detection of laser generated ultrasonic waves in ablation regime by plane and confocal Fabry- Perot interferometers: Simulation

Detection of laser generated ultrasonic waves in ablation regime by plane and confocal Fabry- Perot interferometers: Simulation INDT6 Proceedings of the 3 rd Iranian International NDT onference Feb -, 6, Olympic Hotel, Tehran, Iran INDT 6-T3 More Info at Open Access Database www.ndt.net/?id=946 Detection of laser generated ultrasonic

More information

Nondestructive Evaluation of Pavements Ð Ultrasonic Tomography

Nondestructive Evaluation of Pavements Ð Ultrasonic Tomography Nondestructive Evaluation of Pavements Ð Ultrasonic Tomography Kyle Hoegh, Graduate Student Dr. Lev Khazanovich, Associate Professor Civil Engineering Department University of Minnesota Ð Twin Cities Outline!

More information

Supplementary Table 1. Parameters for estimating minimum thermal conductivity in MoS2

Supplementary Table 1. Parameters for estimating minimum thermal conductivity in MoS2 Supplementary Table 1. Parameters for estimating minimum thermal conductivity in MoS2 crystal. The three polarizations (TL1 TL2 and TA) are named following the isoenergydecomposition process described

More information

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 FREQUENCY DEPENDENCY AND ANISOTROPY OF THE ELASTIC CONSTANTS OF (NON-)POROUS MATERIALS AND THEIR INFLUENCE ON THE USAGE IN BUILDING

More information

6298 Stress induced azimuthally anisotropic reservoir - AVO modeling

6298 Stress induced azimuthally anisotropic reservoir - AVO modeling 6298 Stress induced azimuthally anisotropic reservoir - AVO modeling M. Brajanovski* (Curtin University of Technology), B. Gurevich (Curtin University of Technology), D. Nadri (CSIRO) & M. Urosevic (Curtin

More information

Mechanics PhD Preliminary Spring 2017

Mechanics PhD Preliminary Spring 2017 Mechanics PhD Preliminary Spring 2017 1. (10 points) Consider a body Ω that is assembled by gluing together two separate bodies along a flat interface. The normal vector to the interface is given by n

More information

Finite Element and Plate Theory Modeling of Acoustic Emission Waveforms. NASA Langley Research Center. Hampton, VA *University of Denver

Finite Element and Plate Theory Modeling of Acoustic Emission Waveforms. NASA Langley Research Center. Hampton, VA *University of Denver Finite Element and Plate Theory Modeling of Acoustic Emission Waveforms W. H. Prosser, M. A. Hamstad + *, J. Gary +, and A. O Gallagher + NASA Langley Research Center Hampton, VA 23681-1 *University of

More information

Limits on the Time Delay Induced by Slow-Light Propagation

Limits on the Time Delay Induced by Slow-Light Propagation Limits on the Time Delay Induced by Slow-Light Propagation Robert W. Boyd Institute of Optics, University of Rochester Daniel J. Gauthier Department of Physics, Duke University Alexander L. Gaeta Applied

More information

Characterization of ultrathin films by laser-induced sub-picosecond photoacoustics with coherent extreme ultraviolet detection

Characterization of ultrathin films by laser-induced sub-picosecond photoacoustics with coherent extreme ultraviolet detection Characterization of ultrathin films by laser-induced sub-picosecond photoacoustics with coherent extreme ultraviolet detection Qing Li 1, Kathleen Hoogeboom-Pot 1, Damiano Nardi 1, Chris Deeb 2, Sean King

More information

AN ANALYSIS OF ULTRASONIC WAVE GENERATED BY OBLIQUE INCIDENCE OF LASER

AN ANALYSIS OF ULTRASONIC WAVE GENERATED BY OBLIQUE INCIDENCE OF LASER International Symposium on Structural Health Monitoring and Nondestructive Testing 4-5 October 2018, Saarbruecken, Germany More info about this article: http://www.ndt.net/?id=23511 http://www.ndt.net/?id=23551

More information

Ultrasonic Non-destructive Testing and in Situ Regulation of Residual Stress

Ultrasonic Non-destructive Testing and in Situ Regulation of Residual Stress Ultrasonic Non-destructive Testing and in Situ Regulation of Residual Stress Chunguang Xu 1, a *, Haibing Tian 2,b, Wentao Song 3,c and Jianfeng Song 4,d 1,2,3,4 School of Mechanical Engineering, Beijing

More information

A TWO-LAYER MODEL FOR THE LASER GENERATION OF ULTRASOUND IN

A TWO-LAYER MODEL FOR THE LASER GENERATION OF ULTRASOUND IN A TWO-LAYER MODEL FOR THE LASER GENERATION OF ULTRASOUND IN GRAPHITE-EPOXY LAMINATES M. Dubois, F. Enguehard, L. Bertrand Ecole Polytechnique de Montreal, Departement de Genie Physique c.p. 6079, succ.

More information

Contents. Associated Editors and Contributors...XXIII

Contents. Associated Editors and Contributors...XXIII Contents Associated Editors and Contributors...XXIII 1 Fundamentals of Piezoelectricity...1 1.1 Introduction...1 1.2 The Piezoelectric Effect...2 1.3 Mathematical Formulation of the Piezoelectric Effect.

More information