Radially Polarized Piezoelectric Transducer

Slides:



Advertisements
Similar presentations
Curve Fitting using the Optimization Module in COMSOL
Advertisements

Finite Element Method CHAPTER 4: FEM FOR TRUSSES
Radially Polarized Spherical Piezoelectric Acoustic Transducer.
Common Variable Types in Elasticity
Common Variable Types in Elasticity
Capacitive Micromotor
FE analysis with shell and axisymmetric elements E. Tarallo, G. Mastinu POLITECNICO DI MILANO, Dipartimento di Meccanica.
Definition I. Beams 1. Definition
Parameterizing a Geometry using the COMSOL Moving Mesh Feature
Chapter 3 Stress and Equilibrium
Einzel Lens You can use the heading from the model documentation for the title. © 2012 COMSOL. All rights reserved.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
EE3321 ELECTROMAGENTIC FIELD THEORY
Beams and Frames.
Model: Shear Bender.
EM 388F Term Paper: Discussion of Fracture Criterions under Impermeable and Permeable Crack Surface of Piezoelectric Materials RONG JIAO April 27, 2008.
The relation between the induced charge density σ p and the polarisation, P is Where is a unit vector along the outward normal to the surface. P is along.
Chang Liu MASS UIUC Micromachined Piezoelectric Devices Chang Liu Micro Actuators, Sensors, Systems Group University of Illinois at Urbana-Champaign.
Mechanics of Materials – MAE 243 (Section 002) Spring 2008 Dr. Konstantinos A. Sierros.
FEA Simulations Usually based on energy minimum or virtual work Component of interest is divided into small parts – 1D elements for beam or truss structures.
Computational Fracture Mechanics
3-6. Conductors in Static Electric Field
Method to Use Conservations Laws in Fluid Flows…… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Mathematics of Reynolds Transport.
1-1 Engineering Electromagnetics Chapter 1: Vector Analysis.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
MA Day 45 – March 18, 2013 Section 9.7: Cylindrical Coordinates Section 12.8: Triple Integrals in Cylindrical Coordinates.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
Forces Due to Static Fluid
UNIVERSITI MALAYSIA PERLIS
S.S. Yang and J.K. Lee FEMLAB and its applications POSTEC H Plasma Application Modeling Lab. Oct. 25, 2005.
Department of Civil and Environmental Engineering, The University of Melbourne Finite Element Modelling – Element Types and Boundary Conditions (Notes.
Theories of Stress and Strain
ANSYS Fundamentals This document contains no technical data subject to the EAR or the ITAR.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
Copyright © Cengage Learning. All rights reserved. 12 Vectors and the Geometry of Space.
Piezoelectric Equations and Constants
Magnet Design for Neutron Interferometry By: Rob Milburn.
1 20-Oct-15 Last course Lecture plan and policies What is FEM? Brief history of the FEM Example of applications Discretization Example of FEM softwares.
1 ELEC 3105 Basic EM and Power Engineering Start Solutions to Poisson’s and/or Laplace’s.
Micro-Resistor Beam.
Transformations of Stress and Strain
Dr. Wang Xingbo Fall , 2005 Mathematical & Mechanical Method in Mechanical Engineering.
Example: Radially Polarized Tube. Introduction This is a 2D static axisymmetric piezoelectric benchmark problem A radially polarized piezoelectric tube.
Introduction to Seismology
Frame with Cutout Random Load Fatigue. Background and Motivation A thin frame with a cutout has been identified as the critical component in a structure.
Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0, the other
Stress and Strain ( , 3.14) MAE 316 – Strength of Mechanical Components NC State University Department of Mechanical & Aerospace Engineering Stress.
Abj 4.1: Introduction to Forces in Fluids: Surface Force: Shear/Viscous/Frictional Force Forces in Fluids Surface Force and Stress Surface.
1 Structural Geology Force and Stress - Mohr Diagrams, Mean and Deviatoric Stress, and the Stress Tensor Lecture 6 – Spring 2016.
Model: Thermally Induced Creep. Introduction This model computes the stress history over a long time for a material that exhibits creep behavior. The.
1 Non-Linear Piezoelectric Exact Geometry Solid-Shell Element Based on 9-Parameter Model Gennady M. Kulikov Department of Applied Mathematics & Mechanics.
Basic Geometric Nonlinearities Chapter Five - APPENDIX.
BME 315 – Biomechanics Chapter 4. Mechanical Properties of the Body Professor: Darryl Thelen University of Wisconsin-Madison Fall 2009.
Transformation methods - Examples
Bolt Pretension with Contact. Nonlinear Structural Analysis Goals Goal: – In this workshop our goal is to investigate the behavior of the pipe clamp assembly.
EXAMPLES OF SOLUTION OF LAPLACE’s EQUATION NAME: Akshay kiran E.NO.: SUBJECT: EEM GUIDED BY: PROF. SHAILESH SIR.
LINE,SURFACE & VOLUME CHARGES
Date of download: 10/10/2017 Copyright © ASME. All rights reserved.
Introduction to Seismology
Peter Uzunov Associate professor , PhD Bulgaria, Gabrovo , 5300 , Stramnina str. 2 s:
11 Vectors and the Geometry of Space
Continuum Mechanics for Hillslopes: Part IV
AE/ME 339 Computational Fluid Dynamics (CFD) K. M. Isaac 11/15/2018
FEA Simulations Boundary conditions are applied
ENE/EIE 325 Electromagnetic Fields and Waves
AE/ME 339 Computational Fluid Dynamics (CFD) K. M. Isaac 12/3/2018
11 Vectors and the Geometry of Space
Topic 6 NavierStokes Equations
Review Chapter 1-8 in Jackson
Evaluating Intramural Virtual Electrodes in the Myocardial Wedge Preparation: Simulations of Experimental Conditions  G. Plank, A. Prassl, E. Hofer, N.A.
Presentation transcript:

Radially Polarized Piezoelectric Transducer © 2013 COMSOL. All rights reserved.

Introduction This tutorial provides a step-by-step instruction on how to create a piezoelectric material that is radially polarized in a cylindrical coordinate system This model can be created using any of the Acoustics Module, MEMS Module or Structural Mechanics Module The method of visualizing stress and strain in the cylindrical coordinate system is shown

Select Model Wizard and 3D Space Dimension

Structural Mechanics > Piezoelectric Devices

Select a Stationary Study

Geometry – Create a disk

Definitions > Coordinate Systems > Base Vector System

You can find the same in the ribbon

Base Vector coordinate system By default, the local coordinate system is oriented along the global rectangular coordinate system

Cylindrical coordinate system In order to model radial polarization of the piezo disk, we need to define a cylindrical (local) coordinate system The cylindrical coordinate directions will correspond to the local coordinates in the following manner Local axis Cylindrical coordinates x1 φ (Azimuthal) x2 z (Axial) x3 r (Radial)

Related Technical Notes Why do we not use COMSOL’s predefined Cylindrical Coordinate System? COMSOL has a more automatic option for creating a cylindrical coordinate system but that option fixes the relation between the local axes and the axes of the cylindrical coordinate system using the following relation: x1 → r, x2 → φ, x3 → z which is not what we want Why do we use upper case X and Y instead of lower case x and y to define the base vectors? The coordinate system will be used to transform material properties. The material properties are defined in the Material Coordinate System (X,Y,Z) and not the Spatial Coordinate System (x,y,z). Hence the Base Vector Coordinate System needs to be defined in terms of the material coordinates. This is important especially when the material is expected to deform significantly and exhibit geometric nonlinearity.

How can we transform coordinates? In order to create a new local coordinate system (cylindrical), we need to define the unit vectors of the cylindrical coordinates in terms of the material coordinates (X,Y,Z) For that purpose we will use the relation between the material and cylindrical coordinates (r,φ,z) Relation between material and cylindrical coordinates

Unit vectors in cylindrical coordinate system A unit vector can be expressed as: where The cylindrical and material coordinate systems can be related using the following unit vectors This is the information we typed in as base vectors

Materials – PZT-5H

Change the coordinate system Piezoelectric Devices (pzd) > Piezoelectric Material 1 Change the Coordinate system from Global coordinate system to Base Vector System 2 (sys2)

What happens to the material properties? d33 denotes the polarization along the local z-direction By default this would correspond to the material’s z-direction In the newly defined cylindrical coordinate system this would correspond to the radial direction d33 = 5.93e-10[C/N]

Structural boundary conditions All other boundaries are free to deform Restrict normal displacement of inner surface Restrict vertical displacement of lower surface

Electrical boundary conditions All other boundaries are at zero charge Outer surfaces are at electrical ground (zero voltage) Inner surfaces are at 100 V

Mesh and Compute The Normal Swept mesh creates 72 hexahedral elements

Displacement, Electric Fields and Electric Potential The radial displacement produced by a radial electric field (black cones) shows that the piezo disk is radially polarized Voltage distribution in the piezo disk

Cylindrical coordinate system The blue arrows pointing radially within the disk indicates that the third axis (x3) of the Base Vector System is aligned with the radial direction

Stresses and Strains Stresses and Strains are available in the Local Coordinate System for postprocessing Stresses in the local coordinate system are named: Normal components: pzd.sl11, pzd.sl22, pzd.sl33 Shear components: pzd.sl12, pzd.sl13, pzd.sl23 Strains in the local coordinate system are named: Normal components: pzd.el11, pzd.el22, pzd.el33 Shear components: pzd.el12, pzd.el13, pzd.el23 For our example this notation can interpreted as: Index 1 → φ direction Index 2 → z direction Index 3 → r direction

Transformation into local coordinate sytem Turn on the Equation View to see how the components of the coordinate transformation tensor sys2.Tij (i,j = 1,2,3) influence the stress and strain computation

Strains in local coordinate system Plot on a radial section

Summary This tutorial showed how to setup a static analysis on a radially polarized piezoelectric disk The radial polarization was modeled by creating a custom cylindrical coordinate system The tutorial showed how to create plots to visualize the new coordinate system and stresses and strains in this coordinate system