• DocumentCode
    3091848
  • Title

    On the use of the Structure Factor Model to understand the measured backscatter coefficient from concentrated cell pellet biophantoms

  • Author

    Franceschini, Emilie ; Guillermin, R. ; Tourniaire, Franck ; Lamy, Edouard ; Roffino, Sandrine ; Landrier, Jean-Francois

  • Author_Institution
    Lab. de Mec. et d´Acoust. LMA, Univ. Aix-Marseille, Marseille, France
  • fYear
    2013
  • fDate
    21-25 July 2013
  • Firstpage
    1220
  • Lastpage
    1223
  • Abstract
    Quantitative ultrasound technique utilizes the amplitude and frequency dependence of the backscatter coefficient (BSC) to estimate the size and concentration of scatterers. QUS techniques rely on theoretical scattering models to fit the BSC from biological tissues to an estimated BSC using an appropriate model. Franceschini and Guillermin (J. Acoust. Soc. Am. 132(6) 3735-7347 2012) recently showed that the Structure Factor Model (SFM) was the more suitable theoretical scattering model for dealing with concentrated medium, such as densely packed cells in tumors. The aim of the present study is to use the SFM to understand and identify the scattering sites in concentrated cell pellet biophantoms. The biophantoms consisted of a suspension of human erythromyeloblastoid leukemia (K562) cells trapped in a mixture of plasma and thrombin. The biophantoms had identical cells (cell radius rc around 6.44 μm) but had different cell volume fractions φc of 0.03, 0.06, 0.18 and 0.30. Ultrasonic backscatter measurements were made from frequencies from 10 MHz to 42 MHz using an ultrasound scanner (Vevo 770, Visualsonics, Toronto, Canada) equipped with the RMV 710 and 703 probes. In order to understand these four measured BSC behaviors, one cell (composed of a nucleus and of a cytoplasm) was assumed to scatter as an effective and single fluid sphere. An optimization procedure was then performed to minimize a cost function, which is the average over frequency of the difference between the sum of four measured BSC and the sum of four estimated BSC using the SFM. Two parameters were estimated: the effective scatterer radius and the corresponding effective impedance contrast. The goodness of the fit for the cell concentration ranging from 0.03 to 0.18 shows that the SFM is sufficient to explain the frequency-dependance and amplitude of the measured BSC from concentrated cell pellet biophantoms. Using the SFM and K562 cell pellet biophantoms, we foun- that the main cellular structure responsive for scattering in the frequency range 10-42 MHz is the entire cell.
  • Keywords
    biomedical ultrasonics; cancer; cellular biophysics; optimisation; phantoms; suspensions; ultrasonic scattering; Franceschini model; Guillermin model; RMV 703 probes; RMV 710 probes; Visualsonics; amplitude dependence; backscatter coefficient; biological tissues; cell radius; cell volume fractions; concentrated cell pellet biophantoms; cytoplasm; densely packed cells; effective impedance contrast; effective scatterer radius; frequency 10 MHz to 42 MHz; frequency amplitude; frequency dependance; frequency dependence; human erythromyeloblastoid leukemia K562 cells; main cellular structure; measured backscatter coefficient; nucleus; optimization procedure; plasma-thrombin mixture; quantitative ultrasound technique; scatterer concentration estimation; scatterer size estimation; single fluid sphere; structure factor model; suspension; theoretical scattering models; ultrasonic backscatter measurements; ultrasound scanner Vevo 770; Acoustics; Backscatter; Biological system modeling; Frequency measurement; Scattering; System-on-chip; Ultrasonic imaging;
  • fLanguage
    English
  • Publisher
    ieee
  • Conference_Titel
    Ultrasonics Symposium (IUS), 2013 IEEE International
  • Conference_Location
    Prague
  • ISSN
    1948-5719
  • Print_ISBN
    978-1-4673-5684-8
  • Type

    conf

  • DOI
    10.1109/ULTSYM.2013.0312
  • Filename
    6724826