Sun Yang, Zhao Shukui, Dayton Paul A, Ferrara Katherine W
Department of Biomedical Engineering, University of California Davis, Davis, CA 95616, USA.
IEEE Trans Ultrason Ferroelectr Freq Control. 2006 Jun;53(6):1130-7. doi: 10.1109/tuffc.2006.1642511.
Rayleigh-Plesset analysis, ultra-high speed photography, and single bubble acoustical recordings previously were applied independently to characterize the radial oscillation and resulting echoes from a microbubble in response to an ultrasonic pulse. In addition, high-speed photography has shown that microbubbles are destroyed over a single pulse or pulse train by diffusion and fragmentation. In order to develop a single model to characterize microbubble echoes based on oscillatory and destructive characteristics, an optical-acoustical system was developed to simultaneously record the optical image and backscattered echo from each microbubble. Combined observation provides the opportunity to compare predictions for oscillation and echoes with experimental results and identify discrepancies due to diffusion or fragmentation. Optimization of agents and insonating pulse parameters may be facilitated with this system. The mean correlation of the predicted and experimental radius-time curves and echoes exceeds 0.7 for the parameters studied here. An important application of this new system is to record and analyze microbubble response to a long pulse in which diffusion is shown to occur over the pulse duration. The microbubble response to an increasing or decreasing chirp is evaluated using this new tool. For chirp insonation beginning with the lower center frequency, low-frequency modulation of the oscillation envelope was obvious. However, low-frequency modulation was not observed in the radial oscillation produced by decreasing chirp insonation. Comparison of the echoes from similar sized microbubbles following increasing and decreasing chirp insonation demonstrated that the echoes were not time-reversed replicas. Using a transmission pressure of 620 kPa, the -6 dB echo length was 0.9 and 1.1 micros for increasing and decreasing chirp insonation, respectively (P = 0.02). The mean power in the low-frequency portion of the echoes was 8 (mV)2 and 13 (mV)2 for increasing and decreasing chirp insonation, respectively (P = 0.01).
瑞利 - 普莱斯方程分析、超高速摄影以及单气泡声学记录先前已被分别应用于表征微气泡对超声脉冲的径向振荡及产生的回波。此外,高速摄影已表明微气泡在单个脉冲或脉冲序列作用下会因扩散和破碎而被破坏。为了开发一个基于振荡和破坏特性来表征微气泡回波的单一模型,研发了一种光声系统,用于同时记录每个微气泡的光学图像和背向散射回波。联合观测提供了将振荡和回波的预测结果与实验结果进行比较的机会,并识别由于扩散或破碎导致的差异。利用该系统可能有助于优化造影剂和超声脉冲参数。对于此处研究的参数,预测的和实验得到的半径 - 时间曲线及回波的平均相关性超过0.7。这个新系统的一个重要应用是记录和分析微气泡对长脉冲的响应,其中显示在脉冲持续时间内会发生扩散。使用这个新工具评估微气泡对频率递增或递减线性调频脉冲的响应。对于从较低中心频率开始的线性调频脉冲激励,振荡包络的低频调制很明显。然而,在频率递减线性调频脉冲激励产生的径向振荡中未观察到低频调制。比较频率递增和递减线性调频脉冲激励后类似大小微气泡的回波表明,回波不是时间反转的复制品。使用620 kPa的发射压力,频率递增和递减线性调频脉冲激励时, - 6 dB回波长度分别为0.9微秒和1.1微秒(P = 0.02)。频率递增和递减线性调频脉冲激励时,回波低频部分的平均功率分别为8(mV)²和13(mV)²(P = 0.01)。