TY - JOUR
T1 - Piezoelectric Floating Element Shear Stress Sensor for the Wind Tunnel Flow Measurement
AU - Kim, Taeyang
AU - Saini, Aditya
AU - Kim, Jinwook
AU - Gopalarathnam, Ashok
AU - Zhu, Yong
AU - Palmieri, Frank L.
AU - Wohl, Christopher J.
AU - Jiang, Xiaoning
N1 - Publisher Copyright:
© 1982-2012 IEEE.
PY - 2017/9
Y1 - 2017/9
N2 - A piezoelectric (PE) sensor with a floating element was developed for direct measurement of flow induced shear stress. The PE sensor was designed to detect the pure shear stress while suppressing the effect of normal stress generated from the vortex lift up by applying opposite poling vectors to the PE elements. During the calibration stage, the prototyped sensor showed a high sensitivity to shear stress (91.3 ± 2.1 pC/Pa) due to the high PE coefficients (d{{31}}=-1330 pC/N) of the constituent 0.67Pb(Mg{1/3} Nb {2/3} )O3-0.33PbTiO3 (PMN-33%PT) single crystal. By contrast, the sensor showed almost no sensitivity to normal stress (less than 1.2 pC/Pa) because of the electromechanical symmetry of the sensing structure. The usable frequency range of the sensor is up to 800 Hz. In subsonic wind tunnel tests, an analytical model was proposed based on cantilever beam theory with an end-Tip-mass for verifying the resonance frequency shift in static stress measurements. For dynamic stress measurements, the signal-To-noise ratio (SNR) and ambient vibration-filtered pure shear stress sensitivity were obtained through signal processing. The developed PE shear stress sensor was found to have an SNR of 15.8 ± 2.2 dB and a sensitivity of 56.5 ± 4.6 pC/Pa in the turbulent flow.
AB - A piezoelectric (PE) sensor with a floating element was developed for direct measurement of flow induced shear stress. The PE sensor was designed to detect the pure shear stress while suppressing the effect of normal stress generated from the vortex lift up by applying opposite poling vectors to the PE elements. During the calibration stage, the prototyped sensor showed a high sensitivity to shear stress (91.3 ± 2.1 pC/Pa) due to the high PE coefficients (d{{31}}=-1330 pC/N) of the constituent 0.67Pb(Mg{1/3} Nb {2/3} )O3-0.33PbTiO3 (PMN-33%PT) single crystal. By contrast, the sensor showed almost no sensitivity to normal stress (less than 1.2 pC/Pa) because of the electromechanical symmetry of the sensing structure. The usable frequency range of the sensor is up to 800 Hz. In subsonic wind tunnel tests, an analytical model was proposed based on cantilever beam theory with an end-Tip-mass for verifying the resonance frequency shift in static stress measurements. For dynamic stress measurements, the signal-To-noise ratio (SNR) and ambient vibration-filtered pure shear stress sensitivity were obtained through signal processing. The developed PE shear stress sensor was found to have an SNR of 15.8 ± 2.2 dB and a sensitivity of 56.5 ± 4.6 pC/Pa in the turbulent flow.
KW - Bimorph piezoelectric (PE) structures
KW - electromechanical symmetry
KW - floating element (FE)
KW - PMN-33%PT crystal
KW - shear stress
UR - http://www.scopus.com/inward/record.url?scp=85029603417&partnerID=8YFLogxK
U2 - 10.1109/TIE.2016.2630670
DO - 10.1109/TIE.2016.2630670
M3 - Article
AN - SCOPUS:85029603417
SN - 0278-0046
VL - 64
SP - 7304
EP - 7312
JO - IEEE Transactions on Industrial Electronics
JF - IEEE Transactions on Industrial Electronics
IS - 9
M1 - 7748566
ER -