Piezoelectricity-Advanced Physics-Project Presentation, Slides of Physics

This is project presentation for Physics course. Instructor and project supervisor was Prof. Alpana Vishvajit at Aliah University. It includes: Piezoelectricity, Transducers, Coupled, Field, Material, Acoustic, Harmonic, Cantilever, Bimorph, Beam

Typology: Slides

2011/2012

Uploaded on 07/18/2012

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Presentation Layout
Project description
Historical Background
Piezoelectricity & Piezoelectric transducers
Coupled field analysis
Piezoelectric analysis
Material properties
Acoustic analysis
Harmonic analysis
Results of Single and multiple layers
Results of Cantilever bimorph beam
Conclusion
Future Work
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Presentation Layout

  • Project description
  • Historical Background
  • Piezoelectricity & Piezoelectric transducers
  • Coupled field analysis
  • Piezoelectric analysis
  • Material properties
  • Acoustic analysis
  • Harmonic analysis
  • Results of Single and multiple layers
  • Results of Cantilever bimorph beam
  • Conclusion
  • Future Work

Project Description

  • The project deals with the modeling of ultrasonic

(piezoelectric) transducer in ANSYS.

  • Piezoelectric transducer used in different application areas,

this thesis contains result for sonar (sound navigation and

ranging) application and some introduction to bimorph beam.

  • Modeling is done only for the sonar transmitter application

and for bimorph both actuation and sensing mode results are

obtained.

  • Material used is piezoceremic (PZT 5H, PZT 5R, PZT 5A), in

single and multilayer configurations.

Piezoelectricity

  • “Piezo” is a Greek word which means “to press”.
  • Piezoelectricity means the pressing of material by the

application of electricity (voltage).

  • Piezoelectricity is the property of materials possessing

piezoelectric effect.

  • Material produce an electric field when the material

dimensions are changed as a result of an imposed mechanical force and vice verse.

Piezoelectric Transducer

  • A vital part of the ultrasonic instrumentation system to be used for the generation and detection of the ultrasound.
  • Piezoelectric transducer are linear and low cost transducers.
  • Piezoelectric transducer are reversible in nature.
  • Piezoelectric sensors react on compression. It converts electrical pulses to pressure waves (Transmitter) and the conversion of returned pressure waves back into electrical energy (Receiver).
  • Piezoelectric sensors are used in many systems for actuation sensing, detection and energy harvesting.
  • used to measure force, torque, pressure, motion, surface roughness and sound.

Ultrasonic Transducer Applications

  • Ultrasonic Transducer main Application areas are
    • Biomedical imaging and therapy
    • Electronic devices
    • Industrial processing
    • Non-destructive testing (NDT)
    • Remote sensing
    • Micro electromechanical systems (MEMS)
    • Sound Navigation and Ranging (SONAR)

Why using ANSYS?

  • There are specialized software available for the modeling of

piezoelectric transducers like PZ flex is tailored for Piezo

analysis using FEM.

  • At PIEAS we do not have this software therefore ANSYS is

used to simulate the piezoelectric transducer.

  • Modeling in ANSYS is a tedious job, involves the coupled field

piezoelectric and coupled field acoustic analyses combined

even for a simplest working model.

Piezoelectric Analysis

  • Piezoelectric is the coupling of structural and electrical

fields which is a natural property of materials such as quartz and piezoceramic.

  • Possible piezoelectric analysis types are static, modal

harmonic, and transient.

  • Harmonic analysis is used to observe the characteristic

behaviour of transducer.

  • Transient analysis is performed to observe the travelling

wave in the medium.

Piezoelectric Analysis (Contd.)

  • The electric and mechanical behaviour of any piezoelectric

material can be described by following equations.

  • Where
    • {T} is the stress tensor
    • [c] is the material stiffness matrix under a constant electric field
    • {S} is the strain tensor
    • {D} is the electrical flux density vector
    • [] is the dielectric tensor at constant mechanical strain
    • {E} is the electric field vector
    • [e] is piezoelectric matrix

  T   c   S   e   E

  D   e T   S      E

Material Properties

  • Relative Permittivity [ε]
    • Ratio of the amount of stored electrical energy when a

voltage is applied, relative to the permittivity of a vacuum.

  • The permittivity values represent the diagonal components

ε 11 , ε 22 , and ε 33 respectively of the permittivity matrix.

Material Properties (Contd.)

  • Piezoelectric matrix
    • It relates the electric field to the stress or strain
    • One can define the piezoelectric matrix in [e] form

(piezoelectric stress matrix) or in [d] form (piezoelectric

strain matrix).

Acoustic Analysis

  • Acoustics is the study of the generation, propagation

absorption, and reflection of sound pressure waves in a fluid medium.

  • Involves modeling the fluid medium and the surrounding

structure.

  • A coupled acoustic analysis takes the fluid-structure

interaction into account.

  • Acoustic elements required density and speed of sound

as material properties.

Acoustic Analysis (Contd.)

  • Acoustic wave equations is:
  • Assumptions are:
    • pressure and density changes are small compared to their starting values
    • no mean fluid flow
    • fluid is inviscid
  • one-dimensional form of wave equation is:

2

2 2 2

2 x

P C t

P

P t

P v

2 2 2 2 

1 

Harmonic Analysis

  • The equation of motion governing the harmonic behavior of a structure is given by:
  • Where
    • F 0 is the maximum forcing amplitude
    • i denotes a complex operator
    •  denotes a phase angle, in radians.
  • After simplification we get the following equation
  • Where
    • U 1 & F 1 are real
    • U 2 & F 2 are imaginary

M    u    C   u^   K   uF 0 e i  ^ t^ 

  2  M   i  C   K  u 1  i u 2   F 1  i F 2 

Transducer Modeling

  • 3D model, interested only in thickness direction of the

model, therefore model known as 1D model.

  • Model lateral dimensions must be greater then thickness

to prominent thickness mode.

  • Results are taken for single and multiple active layers.
  • Voltage is applied at front, back and interacting faces
  • Acoustic fluid loading at front and back face