Acoustic Response of Piezoelectric Membranes A.S. Wixom, D.F. Bahr, M.J. Anderson WSU REU 2010 – Materials Science and Engineering • Total Harmonic Distortion (THD) PRE-STRESS EFFECT The acoustic response of piezoelectric membranes has been shown to improve when bulged by a differential pressure. Research to this point has been focused on transducers using lead zirconate titanate (PZT) as the piezoelectric layer. •Pressure-deflection Curve is regressed to the equation P o w w 3 o d1 t a Et d2 4 (1 )a 2 OBJECTIVES f fR f fB f_bar = Normalized frequency f = Frequency of interest fR = Resonant frequency fB = Lower half-bandwidth of resonance An example of these values is shown below for both PVDF and PZT transducers. t = Membrane thickness d1, d2 = Geometry constants E = Young’s Modulus ν = Poisson’s Ratio σ = Initial stress in membrane PVDF – 2C •Results for several PVDF membranes and a PZT membrane for comparison PZT fR Displacement (μm/V) where P = Applied pressure w = Center displacement of membrane γo = Initial edge tension δ = Sheet stiffness a = Membrane span (radius) •Develop transducers using the piezoelectric polymer polyvinylidene flouride (PVDF) THD has a strong dependence on resonance, so in order to compare different transducers, a normalized frequency was defined. fR Displacement (μm/V) INTRODUCTION fB fB Frequency (Hz) •Investigate the effect of pre-stress in the membrane on acoustic response Trans. ID γo (kPa/μm) δ (mPa/μm^3) σ (Mpa) E (Gpa) 2A 0.0062 0.484 3.85 5.29 2B 0.0116 0.473 7.24 5.18 2C 0.0215 0.447 13.4 4.89 PZT 0.2968 64.6 90.0 102 •Compare PZT and PVDF transducers Frequency (Hz) Restricting measurements to negative normalized frequencies, those between -1 and 0 are within the resonance band with full resonance occurring at 0. THD measurements for both PZT and PVDF transducers at different normalized frequencies and pressures were gathered. •Silver ink painted onto the film is patterned to form electrodes and leads •Transducers are stretched to stress the membrane Pre-Stress Peak - 500 Hz 0.016 0.014 0.012 0.01 0.008 0.006 0.004 0.002 0 2A 2B 2C -10 Cut and patterned transducer being stretched to produce uniform biaxial stress in the active area. -5 0 Pressure (kPa) 5 Reduced pre-stress results in an increasing peak in response due to a smaller levels of pressure differential 10 THD Comparison - 3 kPa 100 10 10 PVDF-2C 1 PZT THD (%) 100 0.1 PVDF-2C 1 PZT 0.1 -2.5 -2 -1.5 -1 -0.5 0 -2.5 Normalized Frequency -2 -1.5 -1 -0.5 0 Normalized Frequency THD Comparison - 5 kPa 1000 THD (%) •Sheets of 28 μm think PVDF film are cut into transducer blanks •Response to a harmonic input was measured at differing pressurization levels Displacement (μm/V) TRANSDUCER CONSTRUCTION THD (%) THD Comparison - 1 kPa 100 PVDF-2C 10 PZT 1 -2.5 -2 -1.5 -1 -0.5 The PVDF transducer tends to have slightly lower levels of THD. The peak in the PZT THD is due to the smaller resonance region below the main resonant frequency. 0 Normalized Frequency PVDF vs. PZT •Frequency Response Frequency (Hz) •Testing is completed using the bulge testing apparatus to pressurize the transducers Frequency (Hz) Pressure (kPa) Frequency (Hz) Pressure (kPa) Pressure (kPa) Pressure (kPa) Mounted transducer being tested on bulge testing set-up. Displacement (μm/V) •A two part puck is used to mount and clamp the active area of the transducer CONCLUSION PZT Displacement (μm/V) PVDF – 2C Frequency (Hz) PVDF has a lower resonant frequency as well as a lower overall response when compared to PZT. The symmetry of layers in PVDF results in zero bending actuation causing the dead spot to occur at zero pressure differential where the PZT occurs at a slight negative pressure due to non-symmetrical layers. Reduction of pre-stress in piezoelectric membranes produces a peak in acoustic response for low levels of differential pressure. When comparing PVDF and PZT transducers, we see that PVDF has a smaller response but it also has less THD and therefore produces a cleaner signal. Future work can be done examining the power required to operate piezoelectric acoustic transducers. Also, the sensitivity of piezoelectric membranes acting as free field microphones should be investigated. Thanks to Bruce Chang for getting me started on the bulge testing equipment and to everyone in the MEMS lab who were there to bounce ideas off of. This work was supported by the National Science Foundation’s REU program under grant number DMR-0755055.