Koppolu Sujeethraj, Chitnis Parag V, Mamou Jonathan, Allen John S, Ketterling Jeffrey A
IEEE Trans Ultrason Ferroelectr Freq Control. 2015 Mar;62(3):494-501. doi: 10.1109/tuffc.2014.006828.
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.
聚合物壳超声造影剂(UCAs)可能会因超声诱导的壳屈曲或破裂而排出其包裹的气体。这种气泡的非线性振荡会在超声背向散射中产生一个次谐波分量。本研究调查了这种气体释放机制与聚合物壳UCAs的壳厚度与半径比(STRRs)之间的关系。研究了三种STRRs分别为7.5、40和100 nm/μm的聚乳酸壳UCAs。每个UCAs群体的标称平均直径为2μm。在一个定制设计的测试腔中,UCAs在2小时内承受从2到330 kPa的逐渐增加的静态超压,同时使用200倍放大倍数的视频显微镜以5帧/秒的帧率进行成像。对数字化视频图像进行二值化处理,以获得单个UCAs的横截面积。将归一化横截面积在归一化时间上进行积分,定义为屈曲因子(Bf),提供了一个无量纲参数,用于量化和比较不同STRRs的UCAs在响应超压时的破裂前屈曲程度。STRR为7.5 nm/μm的UCAs在壳破裂前(Bf < 1)表现出明显的壳屈曲阶段,而STRRs较高(40和100 nm/μm)的UCAs则没有经历显著的破裂前屈曲(Bf ≈ 1)。超压响应的差异与这些UCAs产生的次谐波响应相关。当使用20 MHz超声激发时,未表现出屈曲阶段的群体中的单个UCAs(N = 3000)产生的次谐波响应比具有明显破裂前屈曲阶段的UCAs群体大一个数量级。这些结果表明,这些UCAs的气体排出机制可能是决定其对高频超声的次谐波响应水平的一个相关因素。