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

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Presentation on theme: "Radially Polarized Piezoelectric Transducer © 2013 COMSOL. All rights reserved."— Presentation transcript:

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

2 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 Introduction

3 Select Model Wizard and 3D Space Dimension

4 Structural Mechanics > Piezoelectric Devices

5 Select a Stationary Study

6 Geometry – Create a disk

7 Definitions > Coordinate Systems > Base Vector System

8 You can find the same in the ribbon

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

10 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 axisCylindrical coordinates x1φ (Azimuthal) x2z (Axial) x3r (Radial)

11 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.

12 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

13 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

14 Materials – PZT-5H

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

16 What happens to the material properties? d 33 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 d 33 = 5.93e-10[C/N]

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

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

19 Mesh and Compute The Normal Swept mesh creates 72 hexahedral elements

20 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

21 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

22 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

23 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

24 Strains in local coordinate system Plot on a radial section

25 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

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