Piezo materials. Actuators Sensors Generators Transducers. Piezoelectric materials may be used to produce e.g.: Piezo materials Ver1404

Similar documents
Addition 1. Shear Stack Piezoelectric Elements and Shear Effect Basics

PIEZOELECTRIC TECHNOLOGY PRIMER

Ferroelectric Ceramic Technology for Sensors. Jim McIntosh Ceramic Operations Manager PCB Piezotronics

Principles of Active Vibration Control: Piezoelectric materials

Classification of Dielectrics & Applications

Piezoelectric Resonators ME 2082

NUMERICAL EVALUATION OF A TEFLON BASED PIEZOELECTRIC SENSOR EFFECTIVITY FOR THE MONITORING OF EARLY AGE COCRETE STRENGTHING

VIBRATION CONTROL OF RECTANGULAR CROSS-PLY FRP PLATES USING PZT MATERIALS

1990. Temperature dependence of soft-doped / hard-doped PZT material properties under large signal excitation and impact on the design choice

Transduction Based on Changes in the Energy Stored in an Electrical Field

Dielectric Materials: Properties and Applications

SIMULATION AND OPTIMIZATION OF MEMS PIEZOELECTRIC ENERGY HARVESTER WITH A NON-TRADITIONAL GEOMETRY

Thickness Optimization of a Piezoelectric Converter for Energy Harvesting

FIELD MODELS OF POWER BAW RESONATORS

Micromechanical modeling and simulation of piezoceramic materials

Lecture 19. Measurement of Solid-Mechanical Quantities (Chapter 8) Measuring Strain Measuring Displacement Measuring Linear Velocity

COURSE OUTLINE. Introduction Signals and Noise Filtering Sensors: Piezoelectric Force Sensors. Sensors, Signals and Noise 1

MME 467: Ceramics for Advanced Applications

ANALYSIS AND NUMERICAL MODELLING OF CERAMIC PIEZOELECTRIC BEAM BEHAVIOR UNDER THE EFFECT OF EXTERNAL SOLICITATIONS

ESO 205 Nature and Properties of Materials

Electrical Properties

Exploring Piezoelectric Properties of Wood and Related Issues in Mathematical Description. Igor Dobovšek

STABILITY OF MECHANICAL AND DIELECTRIC PARAMETERS IN PZT BASED CERAMICS JAN ILCZUK, JUSTYNA BLUSZCZ, RADOSŁAW ZACHARIASZ

Finite Element Modeling of Ultrasonic Transducers for Polymer Characterization

Piezoactuators. Jiří Tůma

Creation of DIPOLE (two poles) (distortion of crystal structure by the small displacement of the ion in direction of electric field)

Piezoelectric sensing and actuation CEE575

Piezo Engineering Primer

Thermal Analysis of a piezo-disk ultrasound probe

Piezo Theory: Chapter 1 - Physics & Design

Temperature Dependence of the Dielectric, Elastic and Piezoelectric Material Constants of Lead Zirconate Titanate Ceramics

Intelligent Materials and their applications. Autors: Jana Pintea, Ionut Balan INCDIE ICPE-CA Bucharest, ROMANIA

TRANSDUCERS. An Introduction

Non-linear Properties of Piezoelectric Ceramics

I. INTRODUCTION II. SAMPLE PREPARATION JOURNAL OF APPLIED PHYSICS VOLUME 92, NUMBER 5 1 SEPTEMBER

ME 515 Mechatronics. Overview of Computer based Control System

ELECTRIC POWER GENERATION USING PIEZOELECTRIC DEVICES

Dielectric Properties of Solids

ELECTROMECHANICAL RESPONSE OF PIEZOELECTRIC FOAMS

Piezoelectric Materials and Devices

Piezoelectricity: Basics and applications. Friday Morning Meeting, Technical Talk Petar Jurcevic

Finite Element Analysis of Piezoelectric Cantilever

Supplementary Information

Laser Interferometric Displacement Measurements of Multi-Layer Actuators and PZT Ceramics

Testing and analysis of high frequency electroelastic characteristics of piezoelectric transformers

INF5490 RF MEMS. LN03: Modeling, design and analysis. Spring 2008, Oddvar Søråsen Department of Informatics, UoO

PIEZOELECTRIC MATERIALS USED FOR PORTABLE

Modelling and design analyses of a piezoelectric cymbal transducer (PCT) structure for energy harvesting application

ScienceDirect. Effect of Heat on the Performance of Novel Energy Harvester by using PZT-5H Transducers

Advanced. piezoelectric. materials. Science and technology. Edited by. Kenji Uchino WOODHEAD PUBLISHING. Oxford Cambridge Philadelphia New Delhi

NDT&E Methods: UT Ultrasound Generation

The Pennsylvania State University. The Graduate School. College of Engineering ON THE IMPACT OF ELECTRODE GEOMETRY ON THE PIEZOELECTRIC

Piezoelectric Vibration Energy Harvesting. Characteristics of Barium Titanate Laminates

UNIVERSITY OF BOLTON SCHOOL OF ENGINEERING MSC SYSTEMS ENGINEERING AND ENGINEERING MANAGEMENT SEMESTER 2 EXAMINATION 2015/20016

THERMAL DEGRADATION AND AGING OF HIGH TEMPERATURE PIEZOELECTRIC CERAMICS

UNIVERSITY OF CALGARY. Seyed Abdolali Zareian Jahromi A THESIS SUBMITTED TO THE FACULTY OF GRADUATE STUDIES

NON-CONVENTIONAL ENERGY SOURCE USING PIEZOELECTRIC MATERIALS

MODELING AND SIMULATION OF PIEZOCERAMIC MATERIALS USING MICROMECHANICAL APPROACH

DEVELOPMENT OF HIGH-STRAIN LOW-HYSTERESIS ACTUATORS USING ELECTROSTRICTIVE LEAD MAGNESIUM NIOBATE (PMN)

SENSORS and TRANSDUCERS

Ferroelectric Materials and Their Applications

Modeling, Simulation and Optimization of Piezoelectric Bimorph Transducer for Broadband Vibration Energy Harvesting

Smart elastomers a touch of robotics

Electrical material properties

INVESTIGATION OF TEMPERATURE DEPENDENCES OF ELECTROMECHANICAL PROPERTIES OF PLZT CERAMICS

Ferroelectricity. Phase transition. Material properties. 4/12/2011 Physics 403 Spring

INTRODUCTION TO PIEZO TRANSDUCERS

EE 5344 Introduction to MEMS CHAPTER 6 Mechanical Sensors. 1. Position Displacement x, θ 2. Velocity, speed Kinematic

BENCHMARKING OF PIEZOCERAMIC MATERIALS FOR GENERATOR APPLICATION

Piezoelectric Ceramic Products

Monika DUKAT, Aldona ZARYCKA

BIASED PZT MATERIALS FOR ACOUSTIC TRANSDUCERS

Piezoelectric Multilayer Beam Bending Actuators

APPENDIX A: MATHEMATICAL RELATIONS

The Pennsylvania State University. The Graduate School. Department of Materials Science and Engineering

5. Building Blocks I: Ferroelectric inorganic micro- and nano(shell) tubes

An Approach to Designing a Dual Frequency Piezoelectric Ultrasonic Transducer

TDS PIEZOTECH FILMS. Fluorinated Plectroactive Polymers

B) Single module (monolithic) but nested (serial) X and Y. Better response than A) but X and Y still work without "knowledge" of each other.

Appendix A Glossary of Mathematical Symbols

Enhancement of buckling load of thin plates using Piezoelectric actuators

User s Manual. STUDY OF DIELECTRIC CONSTANT Model: DEC-01

Effect of Domain Wall Motion and Phase Transformations on Nonlinear Hysteretic Constitutive Behavior in Ferroelectric Materials

Lecture 6: Piezoelectricity & Piezoresistivity

1106. Numerical investigation of dynamical properties of vibroactive pad during hot imprint process

Validation of High Displacement Piezoelectric Actuator Finite Element Models

Structural Health Monitoring Using Smart Piezoelectric Material

Single-phase driven ultrasonic motor using two orthogonal bending modes of sandwiching. piezo-ceramic plates

e453.eps 1 Change (or the absolute value) in the measured physical variable 2 Change in the sensor property is translated into low-power-level

7.Piezoelectric, Accelerometer and Laser Sensors

SPEED OF SOUND MEASUREMENT IN SOLIDS USING POLYVINYLIDENE FLUORIDE (PVDF) SENSORS

Measuring Properties of Piezoelectric Ceramics

Ferroelectric materials contain one or more polar axes along which a spontaneous

Determination of the lead titanate zirconate phase diagram by the measurements of the internal friction and Young s modulus

The Pennsylvania State University. The Graduate School. Mechanical and Nuclear Engineering

Ferroelectrics and ferroelectric domains

PERFORMANCE OF HYDROTHERMAL PZT FILM ON HIGH INTENSITY OPERATION

Bridging to the Continuum Scale for Ferroelectric Applications

CHAPTER 5 SIMULATION OF A PAYLOAD FAIRING

PVP CHARACTERIZATION OF PIEZO ELECTRIC WAFER ACTIVE SENSORS AFTER EXPOSURE TO HIGH TEMPERATURE

Transcription:

Noliac Group develops and manufactures piezoelectric materials based on modified lead zirconate titanate (PZT) of high quality and tailored for custom specifications. Piezoelectric materials may be used to produce e.g.: Actuators Sensors Generators Transducers www.noliac.com Piezo materials Ver1404

Piezo materials specifications Properties Symbol & unit NCE40 NCE41 NCE46 * NCE51 NCE53 NCE55 NCE56 NCE57 * NCE59 * NCE80 DIELECTRIC PROPERTIES (tolerances +/- 10 %) Relative Dielectric Constant ε T 33 ε 0 1250 1350 1300 1900 1600 5000 2900 1800 2900 1050 Dielectric Loss Factor tgδ [10-4 ] 25 40 30 150 130 220 140 170 190 20 Dielectric Loss Factor at 400V/mm tgδ [10-4 ] 140 200 100 ELECTROMECHANICAL PROPERTIES (tolerances +/- 5 %) Coupling Factors** k p 0.58 0.57 0.57 0.65 0.56 0.62 0.64 0.59 0.64 0.55 k 31 0.34 0.33 0.33 0.38 0.32 0.39 0.37 0.33 0.37 0.30 k 33 0.70 0.68 0.68 0.74 0.65 0.72 0.74 0.70 0.75 0.68 k t 0.50 0.50 0.47 0.50 0.47 0.50 0.50 0.47 0.52 0.48 Piezoelectric Charge Constants -d 31 [10-12 C/N] 140 130 130 195 150 260 250 170 240 100 d 33 [10-12 C/N] 320 310 290 443 360 670 580 425 575 240 Piezoelectric Voltage Constants -g 31 [10-3 Vm/N] 11 11 11 13 9 9 9 11 10 11 g 33 [10-3 Vm/N] 27 25 28 26 23 19 20 27 23 27 Frequency Constants N E p [m/s] 2160 2280 2230 1925 2180 1970 2000 2010 1970 2270 N D t [m/s] 1980 2000 2040 2000 2040 1990 2030 1950 1960 2050 N E 1 [m/s] 1470 1600 1500 1370 1530 1400 1410 1610 N D 3 [m/s] 1340 1500 1800 1320 1400 1500 1500 1500 PHYSICAL PROPERTIES (tolerances +/- 5 %) Mechanical Quality Factor Q m 700 1400 >1000 80 80 70 80 80 90 1000 Density ρ [10 3 kg/m 3 ] 7.75 7.90 7.70 7.85 7.60 8.00 7.65 7.70 7.45 7.80 Elastic Compliances s E 11 [10-12 m 2 /N] 13 13 13 16 16 17 18 17 17 11 s E 33 [10-12 m 2 /N] 17 16 20 19 18 21 20 23 23 14 Curie Temperature T c [ C] 318 284 330 360 340 159 242 350 235 307 *) For multilayer components only. **) Measured in accordance with standard EN 50324. The values listed above are for reference purposes only and cannot be applied unconditionally to other shapes and dimensions. Values vary depending on the components' actual shape, surface finish, shaping process and post-processing. www.noliac.com Piezo materials Ver1404 2

Piezo materials characteristics Piezoelectric materials have the property of developing an electric charge when mechanical stress is exerted on them. In these materials, an applied electric field produces a proportional strain. The electrical response to mechanical stimulation is called the direct piezoelectric effect, and the mechanical response to electrical stimulation is called the converse piezoelectric effect. Piezoelectric materials are usually divided into two groups. The antonyms hard and soft doped piezoelectric materials refer to the ferroelectric properties, i.e. the mobility of the dipoles or domains and hence also to the polarization/depolarization behaviour. Hard doped piezoelectric materials Hard doped PZT materials can be exposed to high electrical and mechanical stresses. The stability of their properties makes them ideal for high-power applications. Piezoelectric materials NCE41 and NCE40 are low loss materials for high power applications. The low dielectric and mechanical losses (tan(δ), Qm) combined with high piezoelectric charge constant (d 33 ) make them suitable for high-performance ultrasonic applications. Furthermore NCE41 and NCE40 can be exposed to high repetitive quasi-static and dynamic loads for ignition applications. NCE41 and NCE40 differ from each other in permittivity and mechanical quality factor values. This variability enables to fulfil all specific requirements. Piezoceramic material NCE80 is intended for power transducers with highest electric drive. Its low dielectric and mechanical losses at extremely high electric drive and high coupling factors make it suitable for high-power applications. Soft doped piezoelectric materials Soft doped piezoelectric materials are distinguished by a comparatively high domain mobility and thus ferro electrically soft behaviour, i.e. relatively easy polarization. These materials are characterized by high relative permittivity, large electromechanical coupling factors, large piezoelectric constants and low mechanical quality factors. They are particularly suitable for sensing applications, receivers, actuators and low power transducers. www.noliac.com Piezo materials Ver1404 3

Piezo material specifications Piezoelectric materials NCE51 and NCE57 are standard soft materials, particularly suitable for actuators and low power nonresonant applications in which high coupling factor and /or high charge sensitivity are requested. Piezoceramic material NCE53 has slightly lower electro-mechanical coupling factor, but has the advantage of higher temperature stability, and it is suitable especially for shear mode vibration sensors. Piezoelectric materials NCE55 and NCE56 are very high sensitivity materials featuring extremely high permittivity, large coupling factor and piezoelectric constant. They have a relatively low Curie temperature. These materials are suitable for a wide range of high sensitivity applications with limited temperature range of operation. Navy types - equivalences Hard materials Soft materials Material NCE40 NCE41 NCE46 NCE80 NCE51 NCE53 NCE55 NCE56 NCE57 NCE59 Navy Type I I I III II II VI V II V European standard EN 50324-1 100 100 100 100 200 200 600 600 200 600 www.noliac.com Piezo materials Ver1404 4

Technical piezo ceramics description Piezoelectricity is the property of nearly all materials that have a non-centrosymmetric crystal structure. Some naturally occurring crystalline materials that possess these properties are quartz and tourmaline. Some artificially produced piezoelectric crystals are Rochelle salt, ammonium dihydrogen phosphate and lithium sulphate. Another class of materials possessing these properties is polarized piezoelectric ceramic. In contrast to the naturally occurring piezoelectric crystals, piezoelectric materials have a polycrystalline structure. The most commonly produced piezoelectric materials are lead zirconate titanate (PZT), barium titanate and lead titanate. Ceramic materials have several advantages over single crystals, especially the ease of fabrication into a variety of shapes and sizes. In contrast, single crystals must be cut along certain crystallographic directions, limiting the possible geometric shapes. PZT (and many other piezoelectric materials) have crystal structures belonging to the perovskite family with the general formula AB0 3. In the following figure the ideal, cubic perovskite structure (centrosymme tric) and tetragonal (ferroelectric) structure are shown. A piezoelectric ceramic material consists of small grains (crystallites), each containing domains in which the polar direction of the unit cells are aligned. Before poling, these grains and domains are randomly oriented; hence the net polari zation of the material is zero, i.e. the ceramic does not exhibit piezoelectric properties. The application of a sufficiently high DC field (called poling process) will orient the domains in the field direction and lead to a remanent polarization of the material. Pb 0 Ti, Zr + The perovskite structure is very tolerant to element substitution (doping) by formation of solid solutions. The possibilities of doping in these materials lead to an unlimited number of possible perovskite-type oxides. Even small amounts of a dopant may cause huge changes in the properties of a material. Fig.1 The Perovskite crystal structure. The coupling of electrical and mechanical energy makes piezoelectric materials useful in a wide range of applications. www.noliac.com Piezo materials Ver1404 5

Constitutive equations The piezoelectric effect depends on directions. The reference axis, called axis 3, is taken parallel to the direction of poling. Axes 1 and 2 are defined arbitrarily in order to form a direct coordinate system with axis 3. 4, 5 and 6 represent shear movements around axes 1, 2 and 3 respectively. Piezoelectric coefficients Based on this coordinate system, the piezoelectric effect can be described in a simplified way by matrix coefficients. The coefficients d (piezoelectric change constant 3 6 matrix) and s E (elastic compliance 6 6 matrix) are commonly used. Fig.2 Electric dipoles in piezoelectric materials before, during and after poling. + Basic piezoelectric equations These coefficients are used to relate the strain S (6-components tensor) to the stress T (6-components tensor) and electrical field E (3-components vector). 3 6 S = s E.T + d.e Polarization In this equation, the s E.T term describes the mechanical compliance of the component, similarly to any mechanical component. The d.e term describes the piezoelectric effect, i.e. strain generated by electrical field. The above equations are useful for designing a piezoelectric application. However, it must be kept in mind that they represent an approximation. 5 4 1 Fig.3 Designation of axes in piezoelectric materials. 2 www.noliac.com Piezo materials Ver1404 6

Definition of piezoelectric properties Properties Symbol / Definition Dimension ELECTRICAL PROPERTIES Relative Dielectric Constant (at 1V/1kHz) Dielectric Loss Factor K T = εt ε with 0 ε T = permittivity (F/m) ε 0 = permittivity of free space (8.854 10-12 F/m) K T 3 All stresses on material are constant or no external forces tan(δ) = Effective series resistance Effective series reactance 1 ELECTROMECHANICAL PROPERTIES Electromechanical Coupling Factors k = Mechanical energy stored Electrical energy applied = Electrical energy stored Mechanical energy applied k 31 1 Applied stress, or the piezoelectrically induced strain, is in 1 direction k 33 1 Applied stress, or piezoelectrically induced strain, is in 3 direction Piezoelectric Charge Constants d = Strain developed Applied field = Charge density Applied stress d 31 C/N Applied stress, or the piezoelectrically induced strain, is in 1 direction d 33 C/N Applied stress, or piezoelectrically induced strain, is in 3 direction Piezoelectric Voltage Constants g = Strain developed Applied charge density = Field developed Applied mechanical stress g 31 g 33 Applied stress, or the piezoelectrically induced strain, is in 1 direction Applied stress, or piezoelectrically induced strain, is in 3 direction Vm/N Vm/N continues on next page www.noliac.com Piezo materials Ver1404 7

Properties Symbol / Definition Dimension Frequency Constants N = F.X With F = resonance frequency (Hz) X = dimension governing the resonance (m) m/s N E p Planar mode, disc Measured with closed circuit m/s N E l Transverse mode, thin bar Measured with closed circuit m/s N D 3 Longitudinal mode, cylindar Measured with closed circuit m/s Elastic Compliances s = 1 Y = Strain Stress with Y = Young modulus s E 10-12 m 2 /N 11 Compliance is measured with closed circuit Stress or strain is in 1 direction Strain or stress is in 1 direction s E 10-12 m 2 /N 33 Compliance is measured with closed circuit Strain or stress is in 3 direction Stress or strain is in 3 direction Curie Temperature T c C www.noliac.com Piezo materials Ver1404 8

NCE51 extended specification 1. The presented data are determined on standardized specimens in the form of small-signal measurements according to European Standard EN 50324 and IEC Publication 483. 2. The standardized specimens are manufactured using a standard production powder and a standard production technology. 3. The data given represents nominal values which were determined 24 hours after poling process at an ambient temperature 23 C + - 2 C. 4. Standard Tolerances: Electrical properties ± 10 %. Mechanical Properties ± 5 %. Piezoelectric properties ± 5 %. Properties Symbol Unit ELECTRICAL PROPERTIES Dielectric dissipation factor tan δ [10-4 ] 150 Relative permittivity εt 33 ε 0 εs 33 ε 0 εt 11 ε 0 εs 11 ε 0 [1] [1] [1] [1] 1900 823 1940 906 Curie Temperature T c [ C] 360 Mechanical Properties Poisson s ratio σ E [1] 0.32 Density ρ [kg.m -3 ] 7850 Piezoelectric Properties Frequency Constants Planar N P [Hz.m] 1925 Thickness shear N 15 [Hz.m] 1180 Transverse N 31 [Hz.m] 1370 Longitudinal N 33 [Hz.m] 1320 Thickness N t [Hz.m] 2000 Coupling Factors Planar k p [1] 0.650 Thickness shear k 15 [1] 0.730 Transverse k 31 [1] 0.380 Longitudinal k 33 [1] 0.740 Thickness k t [1] 0.500 Charge Constant d 33 [10-12 C/N] 443 Voltage Constant g 33 [10-3 V.m/N] 26.3 Mechanical Quality Factor Q m [1] 80 Stability Temperature Coefficient Range 20 80 C α permittivity [10-6 K -1 ] 4000 α kp [K -1 ] 0 Aging Rates c ε [%] per decade -1.40 c Np [%] per decade 0.25 c kp [%] per decade 0.10 www.noliac.com Piezo materials Ver1404 9

NCE51 complete coefficient matrix Elastic Properties Piezoelectric Properties Elastic Compliance Matrix E s E [10-12 m 2 N] 17.0-5.36-8.69 0 0 0-5.36 17.0-8.69 0 0 0-8.69-8.69 21.3 0 0 0 0 0 0 48.9 0 0 0 0 0 0 48.9 0 0 0 0 0 0 44.6 Elastic Compliance Matrix D s D [10-12 m 2 N] 14.5-7.81-3.22 0 0 0-7.81 14.5-3.22 0 0 0-3.22-3.22 9.64 0 0 0 0 0 0 22.9 0 0 0 0 0 0 22.9 0 0 0 0 0 0 44.6 Elastic stiffness Matrix E c E [10 10 N m 2 ] 13.4 8.89 9.09 0 0 0 8.89 13.4 9.09 0 0 0 9.09 9.09 12.1 0 0 0 0 0 0 2.05 0 0 0 0 0 0 2.05 0 0 0 0 0 0 2.24 Charge Constant Matrix d [10-12 C N] 0 0 0 0 669 0 0 0 0 669 0 0-208 -208 443 0 0 0 e [C m²] 0 0 0 0 13.7 0 0 0 0 13.7 0 0-6.06-6.06 17.2 0 0 0 Voltage Constant Matrix g [10-3 Vm N] 0 0 0 0 38.9 0 0 0 0 38.9 0 0-12.4-12.4 26.3 0 0 0 Constant Matrix h [10 8 V m] 0 0 0 0 17.0 0 0 0 0 17.0 0 0-8.31-8.31 23.5 0 0 0 0 0 0 38.9 0 0-12.4-12.4 26.3 0 0 0 Elastic stiffness Matrix D c D [10 10 N m 2 ] 13.2 8.76 7.34 0 0 0 8.76 13.2 7.34 0 0 0 7.34 7.34 16.2 0 0 0 0 0 0 4.37 0 0 0 0 0 0 4.37 0 0 0 0 0 0 2.24 www.noliac.com Piezo materials Ver1404 10

Dielectric properties Matrix Permittivities [10-8 F m] ε T 11 1.72 ε S 11 0.802 ε T 22 1.72 ε S 22 0.802 ε T 33 1.68 ε S 33 0.729 Relative Permittivities [1] ε T 11r 1940 ε S 11r 906 ε T 22r 1940 ε S 22r 906 ε T 33r 1900 ε S 33r 823 Z ab Z - Property a - direction b - direction 1 2 3 4 1 Z 11 Z 12 Z 13 èb 2 Z 21 Z 22 Z 23 3 Z 31 Z 32 Z 33 4 a Young Modulus Matrix Y E [10 10 N m 2 ] 5.9-18.6-11.5 0 0 0-18.6 5.9-11.5 0 0 0-11.5-11.5 4.69 0 0 0 0 0 0 2.05 0 0 0 0 0 0 2.05 0 0 0 0 0 0 2.24 Young Modulus Matrix Y D [10 10 N m 2 ] 6.9-12.8-31.1 0 0 0-12.8 6.9-31.1 0 0 0-31.1-31.1 10.4 0 0 0 0 0 0 4.37 0 0 0 0 0 0 4.37 0 0 0 0 0 0 2.24 www.noliac.com Piezo materials Ver1404 11

www.noliac.com Piezo materials Ver1404 12