Title :
Correlation of rupture dynamics to the nonlinear backscatter response from polymer-shelled ultrasound contrast agents
Author :
Koppolu, Sujeethraj ; Chitnis, Parag ; Mamou, Jonathan ; Allen, John ; Ketterling, Jeffrey
Author_Institution :
F.L. Lizzi Center for Biomed. Eng., Riverside Res., New York, NY, USA
Abstract :
Polymer-shelled ultrasound contrast agents (UCAs) may expel their encapsulated gas subject to ultrasound- induced shell buckling or rupture. Nonlinear oscillations of this gas bubble can produce a subharmonic component in the ultrasound backscatter. This study investigated the relationship between this gas-release mechanism and shell-thickness- to-radius ratios (STRRs) of polymer-shelled UCAs. Three types of polylactide-shelled UCAs with STRRs of 7.5, 40, and 100 nm/μm were studied. Each UCA population had a nominal mean diameter of 2 μm. UCAs were subjected to increasing static overpressure ranging from 2 to 330 kPa over a duration of 2 h in a custom-designed test chamber while being imaged using a 200× magnification video microscope at a frame rate of 5 frames/s. Digitized video images were binarized and processed to obtain the cross-sectional area of individual UCAs. Integration of the normalized cross-sectional area over normalized time, defined as buckling factor (Bf), provided a dimensionless parameter for quantifying and comparing the degree of pre-rupture buckling exhibited by the UCAs of different STRRs in response to overpressure. The UCAs with an STRR of 7.5 nm/μm exhibited a distinct shell-buckling phase before shell rupture (Bf <; 1), whereas the UCAs with higher STRRs (40 and 100 nm/μm) did not undergo significant prerupture buckling (Bf ≈ 1). The difference in the overpressure response was correlated with the subharmonic response produced by these UCAs. When excited using 20-MHz ultrasound, individual UCAs (N = 3000) in populations that did not exhibit a buckling phase produced a subharmonic response that was an order of magnitude greater than the UCA population with a prominent pre-rupture buckling phase. These results indicate the mechanism of gas expulsion from these UCAs might be a relevant factor in determining the level of subharmonic response in response to high-frequency ultrasound.
Keywords :
backscatter; bending; biomedical ultrasonics; buckling; harmonics; nonlinear acoustics; optical microscopes; oscillations; polymer films; pressure sensors; video cameras; UCA gas expulsion mechanism; UCA population nominal mean diameter; UCA-exhibited prerupture buckling degree; UCA-produced subharmonic response; buckling factor; custom-designed test chamber; digitized video images; encapsulated gas subject; gas-release mechanism; high-frequency ultrasound; magnification video microscope frame rate; nonlinear backscatter response; nonlinear gas bubble oscillations; overpressure response; polylactide-shelled UCA type; polymer-shelled UCA STRR; polymer-shelled ultrasound contrast agents; rupture dynamics-backscatter response correlation; shell-buckling phase; shell-thickness-to-radius ratios; static overpressure-subjected UCA; subharmonic response level determination; ultrasound backscatter subharmonic component; ultrasound- induced shell buckling; ultrasound-induced shell rupture; Acoustics; Backscatter; Microscopy; Polymers; Sociology; Statistics; Ultrasonic imaging;
Journal_Title :
Ultrasonics, Ferroelectrics, and Frequency Control, IEEE Transactions on
DOI :
10.1109/TUFFC.2014.006828