Example26 Floating electrode

General

  • We will examine how the floating electrode works.

  • The piezoelectric material is deformed by force. The voltage generated by the deformation is analyzed.

  • The result is compared with the piezoelectric constant.

 

Show Results

Item

Setting

Solver

Piezoelectric analysis [Rayleigh]

Analysis Space

3D

Analysis Type

Static analysis

Unit

mm

Options

N/A

Model

The model is a rectangular solid body. The boundary condition is set on each of the faces.

 

 

Body Attributes and Materials

Body Number/Type

Body Attribute Name

Material Name

0/Solid

piezo

000_P-4 *

* Available from the material DB

 

Body Attribute Name

Tab

Setting

piezo

Direction

Specified by: Vector

Vector: X=Y=0.0, Z=1.0

 

Boundary Condition

Boundary Condition Name/Topology

Tab

Boundary Condition Type

Setting

UX0/Face

Electric

Magnetic wall

 

Mechanical

Displacement

Select UX and enter 0.0

UY0/Face

Electric

Magnetic wall

 

Mechanical

Displacement

Select UY and enter 0.0

UZ0/Face

Electric

Electric Wall

Voltage specified:

Voltage 0[V]

Mechanical

Displacement

Select UZ and enter 0.0

FLOAT/Face

Electric

Electric Wall

Floating electrode

Mechanical

Free

 

PULL/Face

Electric

Magnetic wall

 

Mechanical

Distributed Face Load

1[Pa]

 

Results

Fig (a) below shows the stress distribution. The stress of 1 [Pa] is exhibited in the X direction. It is generated by applying the face load of 1 [Pa].

We will study the electric field generated by the mechanical stress using the d-type piezoelectric equation.

 

D = dT+εE (1)

 

Only Tx of the X component of the stress exists. Of the D constants relating to the X component of the stress, the constant having the value other than 0 is d31. It means there is a possibility that DZ component exists. From the floating electrode with the charge of 0, DZ is 0.

0 = d31*Tx+εz*Ez is derived from the equation (1). The electric field Ez is obtained by inserting the stress (Tx) in this equation. The material used for this analysis is 000P-4 having d31=-0.7e-11[C/N] and εz=200ε0.

 

Ez = -d31*Tx/εz = -(-0.7e-11)*1.0/(200*8.854e-12) = 3.953e-3 [V/m] (2)

 

Fig (b) shows the calculation result of electric field. It matches with the result obtained by the equation (2). As the electric field in the piezoelectric material is constant, the potential is obtained from Ez and the thickness.

Fig (c) below shows the voltage distribution.