In the paper a feasibility study on the use of surface acoustic wave (SAW) vibration sensors for electronic warning systems is presented. The system is assembled from concatenated SAW vibration sensors based on a SAW delay line manufactured on a surface of a piezoelectric plate. Vibrations of the plate are transformed into electric signals that allow identification of the sensor and localization of a threat. The theoretical study of sensor vibrations leads us to the simple isotropic model with one degree of freedom. This model allowed an explicit description of the sensor plate movement and identification of the vibrating sensor. Analysis of frequency response of the ST-cut quartz sensor plate and a damping speed of its impulse response has been conducted. The analysis above was the basis to determine the ranges of parameters for vibrating plates to be useful in electronic warning systems. Generally, operation of electronic warning systems with SAW vibration sensors is based on the analysis of signal phase changes at the working frequency of delay line after being transmitted via two circuits of concatenated four-terminal networks. Frequencies of phase changes are equal to resonance frequencies of vibrating plates of sensors. The amplitude of these phase changes is proportional to the amplitude of vibrations of a sensor plate. Both pieces of information may be sent and recorded jointly by a simple electrical unit.
References
[1]
Wohltjen, H.; Dessy, R. Surface acoustic waves probe for chemical analysis I. Introductcion and instrument design. Anal. Chem 1979, 9, 1458–1475.
[2]
Nakamoto, T.; Nakamura, K.; Moriizumi, T. Study of oscillator-circuit behavior for QCM gas sensor. Proceedings of the Ultrasonics Symposium, San Antonio, TX, USA, 3–6 November 1996; 1, pp. 351–354.
[3]
Gizeli, E.; Liley, M.; Love, C.R.; Vogel, H. Antibody binding to a functionalized supported lipid layer: A direct acoustic immunosensor. Anal. Chem 1997, 69, 4808–4813.
[4]
Urbańczyk, M.; Jakubik, W.; Kochowski, S. Investigation of sensor properties of cooper phtalocyanine with the use of surface acoustic waves. Sens. Actuat. B 1994, 22, 133–137.
[5]
Cullen, C.; Reeder, T. Measurement of SAW velocity versus strain for YX and ST quartz. Proceedings of the Ultrasonics Symposium, Los Angeles, CA, USA, 22–24 September 1975; pp. 519–522.
[6]
Cullen, C.; Montress, T. Progress in the development of SAW resonator pressure transducers. Proceedings of the Ultrasonics Symposium, Boston, MA, USA, 5–7 November 1980; 2, pp. 519–522.
[7]
Pohl, A.; Ostermayer, G.; Reindl, L.; Seifert, F. Monitoring the tire pressure of cars using passsive SAW sensors. Proceedings of the Ultrasonics Symposium, Toronto, ON, Canada, 5–8 October 1997; 1, pp. 471–474.
Drafts, B. Acoustic Wave Technology Sensors, Available online: http://www.sensorsmag.com/sensors/acoustic-ultrasound/acoustic-wave-technology-sensors-936 (accessed on 5 November 2011).
[11]
Seifert, F.; Bulst, W.; Ruppel, C. Mechanical sensor based on surface acoustic waves. Sens. Actuat. A 1994, 44, 231–239.
[12]
Hauden, D. Elastic waves for miniaturized piezoelectric sensors: Applications to physical quantity measurements and chemical detection. Arch. Acoust 1991, 16, 91–106.
Mason, W.P. Physical Acoustics and the Properties of Solids; Van Nostrand: Princeton, NJ, USA, 1958.
[19]
Bogusz, W.; D?ygad?o, Z.; Rogula, D.; Sobczyk, K.; Solarz, L. Linear vibration of discrete systems. In Vibrations and Waves A; Kaliski, S., Solarz, L., Eds.; Elsevier: Amsterdam, The Netherlands, 1992.
[20]
Filipiak, J.; Solarz, L.; Zubko, K. Analysis of acceleration sensor by the discrete model. Mol. Quantum Acoust 2004, 25, 89–99.
[21]
Zubko, K. Applying of the Rayleigh Method to Determination of Elastic and Viscoelastic Parameters of Piezoelectric Crystals (in Polish)Ph.D. Thesis. Military University of Technology, Warsaw, Poland, 2006.
[22]
Filipiak, J.; Zubko, K. Determination of damping in piezoelectric crystals. Mol. Quantum Acoust 2005, 26, 75–80.
[23]
Kopycki, C. Effect of Substrates on the Parameters of Piezoelectric Vibration Sensor with a Surface Acoustic Wave (in Polish)Ph.D. Thesis. Military University of Technology, Warsaw, Poland, 1999.
[24]
Filipiak, J. Problems of Synthesis of Components of a Surface Acoustic Wave Signal Processing to Complex Type “Chirp” (in Polish)Ph.D. Thesis. Military University of Technology, Warsaw, Poland, 1993, 1–333.
[25]
Matthews, L. Surface Wave Filters; John Wiley & Sons: New York, NY, USA, 1997.
[26]
Morgan, P. Surface Wave Devices for Signal Processing; Elsevier: London, UK, 1985.
Ballantine, D.S.; White, R.M.; Martin, S.J.; Ricco, A.J.; Zellers, E.T.; Frye, G.C.; Wohltjen, H. Acoustic Wave Sensor—Theory, Design, and Physico-Chemical Applications; Academic Press: San Diego, CA, USA, 1997.
[29]
Filipiak, J.; Solarz, L.; Steczko, G. The analysis of electronics warning systems with surface acoustic wave sensors (in Polish). Electr. Rev 2010, 11a, 177–179.
[30]
Filipiak, J.; Kopycki, C.; Solarz, L.; Ostrowski, J. The SAW acceleration sensor. Proceedings European Frequency and Time Forum, Warszawa, Poland, March 1998; 1, pp. 229–232.
[31]
Filipiak, J.; Kopycki, C.; Solarz, L.; Ostrowski, J. Lithium niobiate as the substratum for the SAW acceleration sensor. Proc. SPIE 1997, 3179, 256–260.