A FEM Study of displacement sensor based on L-L ......OOO H Properties PMN–28PT ρ, kg m-3 8060...

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Qingwei Lau, PhD candidate

School of ME, SJTU

A FEM Study of displacement sensor based on

L-L Magnetostrictive/Piezoelectric block

magnetoelectric composite material

Excerpt from the Proceedings of the 2016 COMSOL Conference in Shanghai

Contents

1 Introduction

2 Modelling of ME effect

3 Implementation with COMSOL

4 Simulation

5 Results

β–ͺ Magnetoelectric effect (ME) is the phenomenon of inducing magnetic

(electric) polarization by applying an external electric (magnetic) field.

Introduction

Single Phase

MaterialCr2O3

Composite Material

Mech.

Strain

Magneti-

zation

Polarization

0-3 Type

2-2 Type

1-3 Type

0 for particle

1 for fiber

2 for layer

3 for matrix

H

magnetic mechanicalME effect

mechanical electric

E

electric mechanicalME effect

mechanical magnetic

Product Property:

β–ͺ Magnetostrictive effect is a property of

ferromagnetic materials that causes them

to change their shape or dimensions during

the process of magnetization.

β–ͺ Piezoelectric effect is the ability of certain

materials to generate an electric charge in

response to applied mechanical stress.

H

l

zΞ” z

Magnetostrictive

layer

Piezoelectric

layer

Magnetostrictive

rod

Piezoelectric

plate

Ξ” z Fixed boundary with

rigid frame

M

M

P

M P

0

l 1 l 2

r

β–ͺ Magnetostrictive nonlinear constitutive equation

Modelling

2m3 1(( ) )

2 3

ii s

iM

2 2( ) , ( )2

ss

s s

M M

M M

eH H M H

( ,H)E

0 0 ( ,H)B H M

2 2 2( ) , ( ) , ( )2 2

ys x s zx y z s

s s s

MM M

M M M

β–ͺ Piezoelectric linear constitutive equation

Modelling

e e ec eE

T

eD e E

Implementation with COMSOL

Implementation with COMSOL

β–ͺ Geometry

Implementation with COMSOL

Air block

NdFeB magnet

Magnetic pole

pieces

MS rod

PMN-PT plate

β–ͺ Realization of PZT material model

β–ͺ The linear constitutive equations for piezoelectric material

β–ͺ For solid mechanics, the elastic relations

β–ͺ For electrostatics, the electrical relations:

Implementation with COMSOL

0 0( ) eT

Es S c E

0( )rD D e E

1[( u) u]

2

T

s

VF

VD

E V

β–ͺ Realization of magnetostrictive material model

β–ͺ The elastic relations

Implementation with COMSOL

0( )Ec

0 ( , , )2 2 2

diag

Properties PMN–28PT

ρ, kg m-3 8060π’„πŸπŸπ‘¬ ,GPa 115.4π’„πŸπŸπ‘¬ ,GPa 103.4π’„πŸπŸ‘π‘¬ ,GPa 102.6π’„πŸ‘πŸ‘π‘¬ ,GPa 114.1π’„πŸ’πŸ’π‘¬ ,GPa 68.9π’„πŸ”πŸ”π‘¬ ,GPa 65.8πœΊπŸπŸπ‘Ί /𝜺𝟎 925πœΊπŸ‘πŸ‘π‘Ί /𝜺𝟎 813

π’†πŸπŸ‘,C m-2 -3.4π’†πŸπŸ“,C m-2 10.1π’†πŸ‘πŸ‘,C m-2 20.5

β–ͺ Boundary conditions & Mesh

Implementation with COMSOL

Results

Thanks.

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