Homogenization in Electrostatic and Piezoelectric Transducers DFG - - PowerPoint PPT Presentation

homogenization in electrostatic and piezoelectric
SMART_READER_LITE
LIVE PREVIEW

Homogenization in Electrostatic and Piezoelectric Transducers DFG - - PowerPoint PPT Presentation

Homogenization in Electrostatic and Piezoelectric Transducers DFG Junior Research Group Inverse Problems in Piezoelectricity Tom Lahmer * Joachim Schberl ** *) Department of Sensor Technology, University of Erlangen **) CCES, RWTH Aachen


slide-1
SLIDE 1

DD 17, 2006, Page 1/24

Homogenization in Electrostatic and Piezoelectric Transducers

DFG Junior Research Group Inverse Problems in Piezoelectricity Tom Lahmer * Joachim Schöberl ** *) Department of Sensor Technology, University of Erlangen **) CCES, RWTH Aachen

slide-2
SLIDE 2

DD 17, 2006, Page 2/24

Overview

  • Motivation
  • Electrostatic Interdigital Sensors and
  • Piezoelectric Stack Actuators - Forward Problem (FEM)
  • Homogenization – 2 Scale Approach
  • Micro Model - Unit Cell Problem
  • Macro Model – Homogenized Structure
  • Numerical results
  • Summary and Outlook
slide-3
SLIDE 3

DD 17, 2006, Page 3/24

TASK

Find efficient solution method for electro and piezoelectric transducers with periodic structures

slide-4
SLIDE 4

DD 17, 2006, Page 4/24

Homogenization in Composites / Piezoelectricity

  • Calculation of effective piezoelectric material

parameters: (Berger, Gabbert, Köppe, Rodriguez - Ramos, Bravo -

Castillero, Guinovart-Diaz, Otero, Maugin, …)

  • Classical homogenization: (double scale asymptotic expansion)

(Sanchez – Palencia, Levy, … )

  • Bloch approximation:

Elliptic operators: (Conca, Natesan, Vanninathan, …) PDEs with periodic coefficients: (Bensoussan, Lions, Papanicoloaou) Piezoelectricity: (Turbé, Maugin) SAW – Filters: (Zaglmayr, Schöberl, Langer)

  • Generalized FEM for homogenization problems:

(A. M. Matache, C. Schwab, …)

slide-5
SLIDE 5

DD 17, 2006, Page 5/24

First Application: Electrostatic Sensor

Application areas: Force and acceleration sensors Airbag deployment Rotary capacitor

Source: http://www.semiconductors.bosch.de/ Sensor reacts with a change in capacitance while the electric field is changed by some outer impact

slide-6
SLIDE 6

DD 17, 2006, Page 6/24

Two Scale Homogenization (Electrostatics)

2 scale series expansion:

slide-7
SLIDE 7

DD 17, 2006, Page 7/24

The Quasi Periodic Electrostatic Eigenvalue Problem

Series expansion: Unit cell problem:

slide-8
SLIDE 8

DD 17, 2006, Page 8/24

Numerical Results Electrostatics (quadratic elements)

slide-9
SLIDE 9

DD 17, 2006, Page 9/24

Second application: Piezoelectric Stack - Actuator

Actuator reacts with a deformation in longitudinal direction by application of an electric field Application areas: Injection valves (common – rail) Optics, Laser Tuning General: High mechanical precision steering High frequency driving

c) Siemens

slide-10
SLIDE 10

DD 17, 2006, Page 10/24

Piezoelectric Effect

slide-11
SLIDE 11

DD 17, 2006, Page 11/24

Piezoelectric PDEs (Fourier Transformed)

Boundary conditions:

slide-12
SLIDE 12

DD 17, 2006, Page 12/24

Heterogeneous (scale resolving) 3D Model (computing times)

  • Stack 200 Layers - one frequency step ~ 5 min
  • Calculation of impedance curve –

100 frequency steps ~ 7.13 hrs

  • Simulation based parameter identification for composite

(evaluation at 15 frequencies x 10 parameters x 10 Newton steps) ~ 1 week

slide-13
SLIDE 13

DD 17, 2006, Page 13/24

Two Scale Homogenization

2 scale series expansion:

slide-14
SLIDE 14

DD 17, 2006, Page 14/24

Piezoelectric Eigenvalue Problem

slide-15
SLIDE 15

DD 17, 2006, Page 15/24

Piezoelectric Eigenvalue Problem (discretized)

slide-16
SLIDE 16

DD 17, 2006, Page 16/24

Piezoelectric Eigenvalue Problem

Solution of the eigenvalue problem by ARPACK using the implicitly restarted Arnoldi iteration With (shift of spectrum) we have a form amenable to the Lanczos algorithm

(eigenvectors are invariant under spectral transformation, eigenvalues might be recovered as )

slide-17
SLIDE 17

DD 17, 2006, Page 17/24

Eigensolutions

1 2 3 4 5 6

Scaled material parameters: (Electric potential) (Mechanical displacement)

slide-18
SLIDE 18

DD 17, 2006, Page 18/24

Weak form homogenized Piezo PDE

slide-19
SLIDE 19

DD 17, 2006, Page 19/24

Treatment of boundary

O O O O O O

...

Scale resolution close to boundary

slide-20
SLIDE 20

DD 17, 2006, Page 20/24

Visualization of Homogenized Solution

  • f Piezoelectric Stack Actuator

Electric Potential (V):

(thickness of each cell 0.2 mm)

Mechanical Displacement (m):

slide-21
SLIDE 21

DD 17, 2006, Page 21/24

Mechanical Displacement (50 cells)

slide-22
SLIDE 22

DD 17, 2006, Page 22/24

CPU Times (50 cells, calculation of one frequency step)

58.4 144840 50030 Heterogeneous 9.65 5454 (N=6) 408 4.64 3636 (N=4) 408 2.85 1818 (N=2) 408 Homogeneous 17.7 7272 (N=8) 408 20.23 22621 7701 Unit Cell (EV Pb.)

(calculation of 12 EVs)

CPU Times Number of Equations Number of Nodes Model

slide-23
SLIDE 23

DD 17, 2006, Page 23/24

Summary and Outlook

Implemented a scheme which effectively resolves

  • scillatory behavior of a periodic structure

Analyzed corresponding eigenvalue problems Homogenization scheme works with electrostatics and

piezoelectricity

Improve convergence with hp-FEM Extend model to 3D case Consider boundary conditions, e.g. pre-stressed stack Embed homogenized calculation in parameter identification

method

slide-24
SLIDE 24

DD 17, 2006, Page 24/24

Selected References:

slide-25
SLIDE 25

DD 17, 2006, Page 25/24

Have we seen a movie yet?