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- Authors : Souvik Sutradhar, E Paul Braineard
- Paper ID : IJERTCONV1IS06059
- Volume & Issue : ICSEM – 2013 (Volume 1 – Issue 06)
- Published (First Online): 30-07-2018
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Electro-Mechanical Analysis of Micro fabricated Piezoelectric Actuator
SOUVIK SUTRADHAR E PAUL BRAINEARD
Department of ICE, Department of ICE,
SRM University SRM University,
Chennai, India Chennai, India
Abstract This paper focuses on optimization of the geometry of piezoelectric actuator for maximization of output for applications such as micro-pump.The device structure consists of a piezoelectric disk/plate which is glued on the top of a silicon plate. Under various constraints the displacement or deflection of the silicon plate attached to the piezoelectric material plate is obtained from simulation and used for the analysis. For analysis purpose a circular and a square shaped silicon plate/membrane has been taken separately into consideration which are simulated under various size, shape and input excitations and the results are compared to determine the optimum dimension.For a 5 mm diameter/edge length silicon plate,the optimum diameter of circular PZT plate obtained is 4.6 mm, whereas, it is 4.1 mm edge length for square PZT plate.
KeywordsPZT, plate, displacement, actuator.
Piezoelectric effect was discovered in 1880 by Pierre Curie in quartz crystals. The word piezo originated from the Greek word piezen which means to press. Piezoelectric (PZT) materials when subjected to mechanical pressure produces electricity which is called piezoelectric effect, whereas mechanical deformation caused by application of electric potential across such materials is called inverse piezoelectric effect. This principle of inverse piezoelectric effect is used in PZT actuators for various applications. Piezoelectric actuation has stable driving compared with other actuations.MEMS (Micro-electro-mechanical Systems) technology is used in fabricating such piezoelectric actuators as it results in miniaturization, low power consumption and low expense when produced in bulk. Micropump is one of the most important devices where piezoelectric actuator is used for controlled drug delivery. The oscillation ofmembrane excited by the piezoelectric actuators attached to it propels thedrug flow. Hence analysis of the shape, size and material of the membrane as well as the PZT plate/disk is necessary in order to achieve high and desired performance. In order to obtain optimum geometry, the thickness of the plate/disk has been of major area of interest because a thicker plate would result in a reduced displacement which may result in less force to drive the liquid in micropump, whereas a much thinner plate mayresult inmechanical damage at increased potential. Apart from the thickness, the edge length or diameter of the
plate plays a major role in determining the efficiency of the PZT actuator. Hence, these parameters have been thoroughlyanalyzed in this paper to obtain maximum output for optimum geometry. The choice of material of the structure also adds to the maximization of the output. Silicon as a mechanical material is the favorite choice for most people as it has high tensile strength and Youngs modulus which makes it the most useful material for mechanical devices. There is wide range of PZT materials such as quartz, barium titanate, PZT- 5A, PZT-5H which has its own advantages. PZT-5H (Lead Zirconate Titanate) offers high sensitivity and good response. Analytical expressions forplate deflection in terms of maximum displacement are presented for a set of plate boundary conditions.
The PZT actuator has basically three layers, stacked and glued as shown in fig. 1 below .
Fig. 1. Schematic model of piezoelectric actuator
The silicon plate of the PZT actuator model is clamped at its circumference/edges. This layer can be termed as the interactive layer as this layer directly interacts with the fluid flow (in case ofmicropump). On the top of the silicon plate is the PZT layer made of PZT-5H (Lead Zirconate Titanate) glued by an intermediate layer of epoxy. The top two layers are free at its circumference. When an electric potential is applied to the PZT plate, the strain produced in the PZT plate causes it to expand or contract, resulting in actuation .The actuation does not only depends on the shape and size of the silicon plate, but also on the excitation voltage. The PZT materialconsidered in this paper is polarizedalong z-axis.The
different material properties  have been listed below. There are two particular shapes of the silicon membrane that has been analyzed here, namely, circular and square which in turn determines the shape of the actuator.
TABLE I. MATERIAL PROPERTIES OF DIFFERENT LAYERS OF THE DEVICE
E = Youngs Modulus of the plate material t3 = plate thickness
= Poissons ratio of the plate material
This flexural rigidity is a measure of stiffness of the plate.
2) Square Plate:The maximum displacement  is given by, Wmax_s= 0.00126Pa4/D (3)
r 0 0 -6.62
I 0 0 -6.62l
I 0 0 23.24 I
I 0 0 0 I I
I 0 17.03 0 I
l17.03 0 0 J
3130 0 0
0 3130 0
0 0 3400
r 16.5 -4.78 -8.45 0 0 0 l
I-4.78 16.5 -8.45 0 0 0 I
I-8.45 -8.45 20.7 0 0 0 I*10-12
I 0 0 0 43.5 0 0 I
I 0 0 0 0 43.5 0 I
l 0 0 0 0 0 42.6J
Epoxy (glue/ bonder)
Youngsmodulu s [GPa]
Youngsmodulu s [GPa]
P = pressure applied
a = edge length of the plate D = flexural rigidity
B. Simulation Results
The circular and square plate having various dimensions is simulated under a fixed load on top surfaceand the results are plotted as shown below.
ANALYSIS OF THE SILICON MEMBRANE
A. Governing Equations
The maximum displacement/deflection determines the performance of an actuator. So, analysis of maximum displacement is of high importance while designing an actuator. For a clamped plate, laterally and uniformly loaded, the maximum displacement is at the centre of the plate.
1)Circular Plate: The maximum displacement  is given by, Wmax_c= Pa4/64D(1)
P = pressure applied a = radius of the plate
D = flexural rigidity and is given by,
D = Et3/12(1- 2) (2)
Fig. 2.Maximum displacement vs. thickness characteristics of (a) circular plate (b) square plate
The above two plots, i.e., fig 2 reveal that as the thickness of the plate is increased, the maximum displacement decreases for various diameter/edge length of the plate.From fig. 3 below  , it is evident that the centerline displacement decreases with increase in thickness of the plates for any particular diameter/edge length. When the thickness is doubled, the maximum deflection reduces by eight times which is also evident from the equations.
Fig. 3.Centerline displacement vs. membrane position characteristics of (a) circular plate (b) square plate
The following two plots show hat as the diameter of circular plate or the edge length of square plate is increased, the
maximum displacement also increases proportionally as shown in fig. 4.Apart from this, the graph also indicates that the maximum displacement decreases with increase in thickness of the plate.
Fig. 4.Maximum displacement vs. diameter/edge length characteristics of(a) circular plate (b) square plate
Fig. 3 also shows that the displacement/deflection at the circumference/edges is zero because the plate is clamped at its outer boundary. It is also observed from the plots that for same dimension the displacement of the square plate is always greater than the circular plate because in this case the surface area of the square plate is always greater than the circular plate. The maximum displacement obtained is for a plate thickness of 20 Âµm which is also rigid enough to sustain the stress generated. Since maximum displacement is of prime
importance for an actuator, so the silicon plate with 20 Âµ m is considered for actuator design in this paper.
ANALYSIS OF THE PIEZOELECTRIC ACTUATOR
CAD Model of the actuator
The CAD model of circular and square PZT actuator using COMSOL Multiphysics is shown below.
Fig. 5.CAD model of (a) circular(b) square PZT actuator
In Fig. 5 shown above, the silicon plate is under fixed constraint (clamped at its boundary), whereas the other two layers are free. These PZT models (circular and square) as per the schematic model of fig. 1are simulated subject to a constraint of 100 volt electric potential using different dimensions shown in Table II. The thicknesses of the different
layers have been kept constant while the diameter or the edge length has been varied. The dimension of the glue/bonder is varied equally with that of the PZT layer. The ratio of diameter or edge length, being calculated, is an important parameter which aids in determining the optimum dimension. TABLE II.DIMENSION OF DIFFERENT LAYERS OF PIEZOELECTRIC ACTUATOR
Diameter / Edge length (mm)
2.5, 3, 3.5, 4, 4.5, 5
2.5, 3, 3.5, 4, 4.5, 5
Circular PZT Actuator: Fig. 6shows  the plot of maximum displacement of the circular PZT actuator vs. the ratio of diameter between PZT disk (d) and silicon disk (D). It can be seen that the maximum displacement at first increases almost smoothly and then after a certain point (optimum value of ratio of diameter) the value tends to fall.
Fig. 6.Maximum displacement vs. ratio of diameter characteristic of circular PZT actuator
Peak value of ratio of diameter (from the plot):
d/D = 0.92
d = diameter of the PZT disk
D = diameter of the silicon disk = 5 mm
Or, d = 0.92*5 mm
Or, d = 4.6 mm
Hence, optimum diameter of the circular PZT disk is 4.6 mm for obtaining maximum displacement for a 5 mm diameter
l/L = 0.82
silicon disk. The maximumdisplacement obtained after simulation is 3.9069 Âµm. With the above obtained PZT diameter, the following plot is obtained for various potential applied across the PZT layer.
Fig. 7. Centerline displacement vs. membrane position characteristics of circular PZT actuator for various voltages
Square PZT Actuator:Fig. 8 below shows the plot of maximum displacement of the square PZT actuator vs. ratio of edge length between PZT plate (l) and silicon plate (L).
Fig. 8.Maximum displacement vs. ratio of edge lengthcharacteristic of square PZT actuator
Peak value of ratio of edge length (from the plot):
l = edge length of the PZT plate
L = edge length of the silicon plate= 5 mm
Or, l = 0.82*5 mm
Or, l = 4.1 mm
Hence, optimum edge length of the PZT plate should be
mm for obtaining maximum displacement for a 5 mm edge length silicon plate. The maximum displacement obtained after simulation is 4.3235 Âµm. With the above obtained PZT edge length, the following plot is obtained for various potential applied across the PZT layer.
Fig. 9. Centerline displacement vs. membrane position characteristics of square PZT actuator for various voltages
Fig. 7and fig. 9 certainly shows that the displacement increases proportionally with increase in electric potential. It should be taken care that an optimum value of potential is maintained so that the membrane structure is not affected.
comments and suggestions, which helped to improve the paper. The authors would also like to acknowledge the faculties of Instrumentation and Control Engineering department of SRM University for their support in fulfillment of the project.
S. Timoshenko and S. Woinosky-Krieger, Theory of Plates and Shells, Tata McGraw Hill Edition 2010.
HeikoFettig and James Wylde,Thermo-MechanicalAnalysis of a Multi- Layer MEMS Membrane, NortelNetworks – Optical Components, 2002.
Qifeng Cui,Chengliang Liu and Xuan F. Zha, Study on apiezoelectric micropump for the controlled drug delivery system, 2007.
Il-Han Hwang, Sung-Kil Lee, Sang-Mo Shin, Yong-Gu Lee, Jong-Hyun Lee, Flow characterization of valvelessmicropump using driving equivalent moment: theory andexperiments, 2008.
Fig. 10.Displacement along diagonal vs. membrane position characteristic of square PZT actuator
Fig. 10 (above) reveals an interesting fact of square PZT actuator. The structure is simulated with optimum dimensions obtained above,with an electric potential of 90 volt as a constraint. It is seen that near the extremes of the diagonal the deformation is in the opposite direction. This is due to the fact that when the PZT layer actuates in the downward direction (negative z-axis), as per fig. 5, then the stress generated at the corners of it causes the silicon plate to deform on the reverse direction along the extreme diagonal ends.
The sensitivity of the PZT actuator can be easily found in terms of maximum displacement when the input excitation is a dc potential. The sensitivity is 0.04021Âµm/V for a circular PZT actuator whereas it is 0.04323Âµm/V for a square PZT actuator as obtained from Fig. 7 and Fig. 9 respectively. This sensitivity in terms of maximum displacement is found to be same in both the cases if a sinusoidal signal of 50 Hz frequency is used as the input excitation of the actuator.
We can easily observe that while the displacement of the square PZT actuator is more for same dimension but for same surface area of the silicon plate, circular PZT actuator proves to be more efficient in terms of maximum displacement.This can be proved from the governing equations also. One major concern of the square PZT actuator is that the corners along the diagonal get deformed in the reverse direction. But, the sensitivity of square PZT actuator is more than the circular PZT actuator for same dimension which results in high displacement for a certain voltage.
The authors would like to express their gratitude to anonymous reviewers of this paper for theirinsightful
Baowei Wang, Xiangcheng Chu, Enzhu Li, Longtu Li,Simulations and analysis of a piezoelectric micropump, June 2006.