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Estimation and measurements of resonance scattering on the gas filled polymer microspheres

Treść / Zawartość
Identyfikatory
Warianty tytułu
Języki publikacji
EN
Abstrakty
EN
The gas filled polymer spheres are used either as an ultrasonic contrast agents or controlled drug delivery microcapsules. The power spectrum of the ultrasonic backscattered signal was calculated from the resonance scattering theory for the gas bubbles surrounded by elastic shield. The size distribution of the measured microspheres was included in the calculations. In experiment, the backscattered power spectrum of measured sample was recorded by Siemens Antares ultrasonic scanner. Radio frequency (RF) data was recorded for 2.5 - 6.7 MHz transmitted ultrasonic frequencies. The backscattered spectra were calculated by Matlab software and subtracted from the transmitter spectrum, recorded as an echo from the perfect reflector. The particle size in measured sample was 12 µm mean š 8 µm sd. The resonance frequency, measured under the microscope, was 0.60 MHz for 45 µm diameter microsphere which corresponds to 2.25 MHz for 12 µm sphere. The sample volume was 10cm? and the mean quantity of scatterers was 6ź103/cm?. In conclusion, measured spectra matched those calculated from theory. The use of ultrasonic scanner with RF data output and the high sensitivity, wide bandwidth ultrasonic transducer allows to measure backscattered signal from the very small quantity of resonance scatterers with satisfactory results at 40 dB signal to noise ratio.
Słowa kluczowe
Czasopismo
Rocznik
Tom
Strony
201--208
Opis fizyczny
Bibliogr. 12 poz., rys., wykr.
Twórcy
autor
autor
  • Department of Ultrasound Institute of Fundamental Technological Research, Polish Academy of Sciences, Świętokrzyska 21, 00-049 Warsaw, Poland, wsecom@ippt.gov.pl
Bibliografia
  • [1] D. Chatterjee et al., On the suitability of broadband attenuation measurement for characterizing contrast microbubbles, Ultrasound in Med. Biol., Vol. 31, 781-786, 2005.
  • [2] C. Church, The effect of an elastic solid surface layer on the radial pulsations of gas bubbles, J. Acoust. Soc. Am., Vol. 97, 1510-1521, 1995.
  • [3] J. Fowlkes, C. Holland, Mechanical bioeffects in the presence of gas-carrier ultrasound contrast agents, J. Ultrasound Med., 120-168, 2000.
  • [4] D. Goertz et al., High frequency attenuation measurements of lipid encapsulated contrast agents, Ultrasonics, Vol. 44, e131-e134, 2006.
  • [5] D. Goertz et al., High frequency nonlinear scattering from a micrometer to submicrometersized lipid encapsulated contrast agent, Ultrasound in Med. Biol., Vol. 32, 569-577, 2006.
  • [6] L. Hoff et al., Oscillations of polymeric microbubbles: Effect of the encapsulating shell, J.Acoust. Soc. Am., Vol. 107, 2272-2280, 2000.
  • [7] N. de Jong et al., Absorption and scatter of encapsulated gas filled microspheres: theoreticalconsiderations and some measurements, Ultrasonics, Vol. 30, 95-103, 1992.
  • [8] N. de Jong, L. Hoff, Ultrasound scattering properties of Albunex microspheres, Ultrasonics,Vol. 31, 175-181, 1993.
  • [9] N. de Jong et al., Contrast harmonic imaging, Ultrasonics, Vol. 40, 567-573, 2002.
  • [10] K. Kooiman et al., Oil –filled polymer microcapsules for ultrasound-mediated delivery oflipophilic drugs, J. Control. Release, Vol. 133, 109-118, 2009.
  • [11] H. Medwin, Counting bubbles acoustically: a review, Ultrasonics, Vol. 15, 7-13, 1977.
  • [12] J. Wu, J. Tong, Measurements of the nonlinearity parameter B/A of contrast agents,Ultrasound in Med. Biol., Vol. 24, 153-159, 1997.
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-article-BWMA-0017-0024
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