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Flow estimation using subharmonics of microbubbles

机译:使用微泡的子态测量的流程估计

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It has been observed that the subharmonic signal of the microbubbles has a significant contrast-to-tissue ratio. The flow velocity can be evaluated precisely even without wall filter for subharmonics since the vessels containing the microbubbles would be distinguishable from the surrounding tissues. However, the microbubble cannot generate the subharmonics unless the applied pressure exceeds the required onset threshold. Moreover, it will undergo cavitation if the acoustic pressure is over the cavitation threshold. While the microbubble moves through the sample volume, there are three different regions inside the excitation beam. The beam-weighted pressure is below the onset threshold, between the onset and cavitation thresholds, and over the cavitation threshold. Since the subharmonics can occur only when the beam-weighted pressure is between the onset and cavitation thresholds, the observation time for subharmonics is shorter than that for the fundamental. Our numerical results showed that the onset threshold is very close to the cavitation threshold. Moreover, some microbubbles are found to generate subharmonics and undergo cavitation simultaneously. Our mathematical analysis showed that the consecutive received signals would have very low correlation for the subharmonics. The experimental data from the Levovist/spl reg/ suspension were used to verify the theoretical predictions. It can be shown that the absolute value of the normalized autocorrelation (first lag) of Doppler signals for the subharmonics was much smaller than the fundamental and the second harmonics when the emitted frequency is 2.1 MHz and the acoustic pressure is 0.8 Mpa. In addition, it is found that the correlation value is always below 0.3 when the emitted frequency is swept from 1.5 to 2.5 MHz and the applied pressure is varied from 0.1 to 1.6 Mpa.
机译:已经观察到微泡的子发声信号具有显着对比度与组织比。流速可以精确地,即使没有进行分谐波壁滤波器进行评估,因为含微泡的容器将是从周围组织区分开来。然而,除非施加的压力超过所需的开始阈值,否则微泡不能产生子发行物。此外,如果声压在空化阈值上,它将发生空化。虽然微泡移动通过样品体积,但激发束内部有三个不同的区域。光束加权压力低于起始阈值,在开始和空化阈值之间,并且在空化阈值上。由于仅当射线加权压力在开始和空化阈值之间时,因此才能发生次汞,因此子发行物的观察时间短于基本基础的观察时间。我们的数值结果表明,开始阈值非常接近空化阈值。此外,发现一些微泡来产生亚烃类和同时进行空化。我们的数学分析表明,连续接收的信号对子发行的相关性非常低。来自Levovist / SPL REG /悬架的实验数据用于验证理论预测。它可以示出,多普勒信号的分谐波的标准化自相关(第一滞后)的绝对值比基本和第二谐波小得多当发射频率为2.1兆赫和的声压为0.8MPa。另外,发现当发射频率从1.5到2.5MHz扫描时,相关值始终低于0.3,并且施加的压力变化0.1至1.6MPa。

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