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The influence of the surface load exerted by a piezoelectric contact sensor on testing results: I. The displacement field in the solid

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Języki publikacji
EN
Abstrakty
EN
The influence of a strong discontinuity wave on its measurement with a piezoelectric sensor was analysed analytically. The one-dimensional model of the mechanical contact between the ultrasonic sensor and the solid medium was developed. The displacement field was calculated with the d'Alambert's method. The evaluation was made locally at the front of the distortion. It was found that the relative difference of a displacements between the free and loaded surfaces ranges from 10% to 72% and the mass M has no influence on it in the first time interval. It is affected not only by the wave impedances but also by surfaces of the sensor and sample. After a long period of time (depending on the mass M) the influence of the surface loading becomes much smaller. Part I of the paper contains the discussion of the displacement field in the solid, the electricaltransients generated by the piezoelectic sensor are given in Part II.
Słowa kluczowe
Rocznik
Strony
71--91
Opis fizyczny
Bibliogr. 13 poz., rys., tab., wykr.
Twórcy
  • Kielce University of Technology, 25-314 Kielce, Al. 1000-lecia P.P. 7, Poland
Bibliografia
  • [1] Z. WESOŁOWSKI, Akustyka ciała sprężystego [in Polish], PWN, Warszawa 1989.
  • [2] F. Lanza di Scalea, R. E. Green Jr., Experimental observation of the intrusive effect of a contact transducer on ultrasound propagation. Ultrasonics, 37, 179-183 (1999).
  • [3] D. M. NORRIS Jr., W. C. YOUNG, Complex modulus measurement by longitudinal vibration testing, Experimental Mechanics, 10, 93-96 (1970).
  • [4] T. PRITZ, Transfer function method for investigating the complex modulus of acoustical materials: rod like specimen, Journal of Sound and Vibration 81, 359-376 (1982).
  • [5] S. ÖDEEN, B. LUNDBERG, Determination of complex modulus from measured end-point acceleration of an impacted rod specimen, J. of Sound and Vibration, 165 (1), 1-8 (1993).
  • [6] C. BACON, J-L. LATAILLADE, Development of the Kolsky-Hopkinson technics and applications for non-conventional testing, 1-58, [in:] New experimental methods in material dynamics and impact, W. K. Nowacki, J. R. KLEPACZKO [Eds.], IPPT PAN, 2001.
  • [7] C. BACON, B. HOSTEN, Acoustic wave generation in viscoelastic rods by time-gated microwaves, JASA, 106, 1, 195-201 (1999).
  • [8] C. BACON, E. GUILLIORIT, B. HOSTEN, D. E. CHIMENTI, Acoustic wave generated by pulsed microwaves in viscoelastic rods: Modeling and experimental verification, JASA, 110, 3, 1398-1407 (2001).
  • [9] B. POUET, N. RASOLOFOSAON, Measurement of broadband intrinsic ultrasonic attenuation and dispersion in solids with laser techniques, JASA 93, 1286-1292 (1993).
  • [10] H. KWUN, J. J. HANLEY, C. M. TELLER, Performance of a noncontact magnetostrictive AE sensor on a steel rod, J. of Acoustic Emission 11, 1, 27-32 (1993).
  • [11] J. OSIECKI, Reflection of a plane stress wave in a non-homogeneous solid medium, Proceedings of Vibration Problems, 2, 7, 155-178 (1961).
  • [12] A. VARY, Ultrasonic measurement of material properties, [in:] Research Techniques in NDT vol. IV, R. S. SHARPE [Ed.], 159-204 (1980).
  • [13] G. ŁYPACEWICZ, Piezoelektryczne uklady nadawczo-odbiorcze dla celów ultrasonografii [in Polish], Prace IPPT PAN, 22/1995.
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-article-BAT3-0004-0015
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