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SAW sensor for detection of hydrocarbons. Numerical analysis and experimental results

Treść / Zawartość
Identyfikatory
Warianty tytułu
Języki publikacji
EN
Abstrakty
EN
The paper presents the results of numerical analyses of the SAW gas sensor in the steady and non-steady state. The effect of SAW velocity changes vs. the surface electrical conductivity of the sensing layer is predicted. The conductivity of the porous sensing layer above the piezoelectric waveguide depends on the profile of the diffused gas molecule concentration inside the layer. Knudsen's model of gas diffusion was used. Numerical results for the gases CH4, C2H4, C3H8, C6H6 in the steady state and CH4 in the non-steady state in the WO3 sensing layer have been shown. The results of numerical analyzes allow to select the sensor design conditions, including the morphology of the sensor layer, its thickness and operating temperature. Some numerical results were verified in experimental studies concerning methane.
Rocznik
Strony
589--595
Opis fizyczny
Bibliogr. 15 poz., rys., tab.
Twórcy
autor
autor
autor
  • ENTE Ltd, limited liability company, 7 Gaudiego St., 44-100 Gliwice, Poland
Bibliografia
  • [1] E. Maciak and Z. Opilski, “Transition metal oxides covered Pd film for optical H2 gas detection”, Thin Solid Films 515, 8351-8355 (2007).
  • [2] T. Pustelny, J. Ignac-Nowicka, and Z. Opilski, “Optical investigations on layered metalphthalocyanine nanostructures affected by NO2 applying the surface plasmon resonance method”, OpticaApplicata 34 (4), 563-572 (2004).
  • [3] W. Jakubik, M. Urbańczyk, E. Maciak, and T. Pustelny, “Surface acoustic wave hydrogen sensor based on layered structure of palladium/metal - free phthalocyanine”, Bull. Pol. Ac.: Tech. 56 (2), 133-138 (2011).
  • [4] M. Urbańczyk , E. Maciak, K. Gut, T. Pustelny, and W. Jakubik, “Layered thin film nanostructures of Pd /WO3-x as resistance gas sensors”, Bull. Pol. Ac.: Tech. 59 (4), 401-408 (2011).
  • [5] T. Hejczyk, M. Urbańczyk, and W. Jakubik, “Analytical model of semiconductor sensor layers in SAW gas sensors”, ActaPhysica Polonica A 118 (6), 1148-1152 (2010).
  • [6] T. Hejczyk and M. Urbańczyk, “Analysis of non-steady state in SAW gas sensors with semiconducting sensor layers”, ActaPhysica Polonica A 120 (4), 789-793 (2011).
  • [7] T. Hejczyk, M. Urbańczyk, and W. Jakubik, “Semiconductor sensor layer in SAW gas sensors configuration”, Acta PhysicaPolonica A 118 (6), 1153-1157 (2010).
  • [8] M.Urbańczyk, Gas Sensors with Surface Acoustic wave, Publishing House of Silesian University of Technology, Gliwice, 2011, (in Polish).
  • [9] M. Urbańczyk “Analytical model of a SAW gas sensor”, WITTrans. on Computational Methods and Experimental Measurements,Proc. CMEM11 48, 229-239 (2011).
  • [10] G.S. Kino, “A normal mode theory for the Rayleigh wave amplifier”, IEEE Trans. on Electron Devices Ed-18 (10), CDROM (1971).
  • [11] B.A. Auld, Acoustic Fields and Waves, vol. 2, John Willey and Sons, New York, 1973.
  • [12] J. Crank, The Mathematics of Diffusion, Oxford University Press, London, 1956.
  • [13] G. Sakai, N. Matsunaga, E.Shimanoe, and N. Yamazone, “Theory of gas-diffusion controlled sensitivity for thin film semiconductor gas sensor”, Sensors and Actuators B 80, 125-131 (2001).
  • [14] N. Matsunga, G. Sakai, K. Shimanoe, and N. Yamazoe, “Diffusion equation-based study of thin film semiconductor gas sensor-response transient”, Sensors and Actuators B 83, 216- 221 (2001).
  • [15] T. Hejczyk and M. Urbańczyk, “WO3-Pd structure in SAW sensor for hydrogen detection”, Acta Physica Polonica A 120 (4), 616-620 (2011)
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-article-BPG8-0096-0020
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