Chen Wen-Shiang, Matula Thomas J, Brayman Andrew A, Crum Lawrence A
Center for Industrial and Medical Ultrasound, Applied Physics Laboratory, University of Washington, Seattle, Washington 98105, USA.
J Acoust Soc Am. 2003 Jan;113(1):643-51. doi: 10.1121/1.1529667.
Contrast bubble destruction is important in several new diagnostic and therapeutic applications. The pressure threshold of destruction is determined by the shell material, while the propensity for of the bubbles to undergo inertial cavitation (IC) depends both on the gas and shell properties of the ultrasound contrast agent (UCA). The ultrasonic fragmentation thresholds of three specific UCAs (Optison, Sonazoid, and biSpheres), each with different shell and gas properties, were determined under various acoustic conditions. The acoustic emissions generated by the agents, or their derivatives, characteristic of IC after fragmentation, was also compared, using cumulated broadband-noise emissions (IC "dose"). Albumin-shelled Optison and surfactant-shelled Sonazoid had low fragmentation thresholds (mean = 0.13 and 0.15 MPa at 1.1 MHz, 0.48 and 0.58 MPa at 3.5 MHz, respectively), while polymer-shelled biSpheres had a significant higher threshold (mean = 0.19 and 0.23 MPa at 1.1 MHz, 0.73 and 0.96 MPa for thin- and thick-shell biSpheres at 3.5 MHz, respectively, p<0.01). At comparable initial concentrations, surfactant-shelled Sonazoid produced a much larger IC dose after shell destruction than did either biSpheres or Optison (p<0.01). Thick-shelled biSpheres had the highest fragmentation threshold and produced the lowest IC dose. More than two and five acoustic cycles, respectively, were necessary for the thin- and thick-shell biSpheres to reach a steady-state fragmentation threshold.
对比剂微泡破坏在多种新型诊断和治疗应用中具有重要意义。微泡破坏的压力阈值由外壳材料决定,而微泡发生惯性空化(IC)的倾向则取决于超声造影剂(UCA)的气体和外壳特性。在不同声学条件下,测定了三种具有不同外壳和气体特性的特定UCA(Optison、Sonazoid和biSpheres)的超声破碎阈值。还比较了这些制剂或其衍生物在破碎后产生的、具有IC特征的声发射,采用累积宽带噪声发射(IC“剂量”)进行比较。白蛋白外壳的Optison和表面活性剂外壳的Sonazoid具有较低的破碎阈值(在1.1 MHz时平均分别为0.13和0.15 MPa,在3.5 MHz时分别为0.48和0.58 MPa),而聚合物外壳的biSpheres具有明显更高的阈值(在1.1 MHz时平均分别为0.19和0.23 MPa,在3.5 MHz时,薄壳和厚壳biSpheres分别为0.73和0.96 MPa,p<0.01)。在初始浓度相当的情况下,表面活性剂外壳的Sonazoid在外壳破坏后产生的IC剂量比biSpheres或Optison都大得多(p<0.01)。厚壳biSpheres具有最高的破碎阈值,产生的IC剂量最低。薄壳和厚壳biSpheres分别需要超过两个和五个声周期才能达到稳态破碎阈值。