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首页> 外文期刊>Ultrasonics, Ferroelectrics and Frequency Control, IEEE Transactions on >Contrast agent response to chirp reversal: simulations, optical observations, and acoustical verification
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Contrast agent response to chirp reversal: simulations, optical observations, and acoustical verification

机译:对比剂对线性调频反转的响应:模拟,光学观察和声学验证

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Active response of a microbubble is characterized by its resonance behavior where the microbubble might oscillate after the excitation waveform has been turned off. We investigate in this paper an excitation approach based on this resonance phenomenon using chirps. The technique, called chirp reversal, consists in transmitting a first excitation signal, the up-sweep chirp (UPF) of increasing frequency with time, and a second excitation signal, the down-sweep (DNF) that is a replica of the first signal, but time reversed with a sweep of decreasing frequency with time. Simulations using a modified Rayleigh-Plesset equation were carried out to determine bubble response to chirp reversal. In addition, optical observations and acoustical measurements were carried out to corroborate the theoretical findings. Results of simulations show differences between bubblesiquest oscillations in response to up-sweep and down-sweep chirps mainly for transmitted center frequencies above the bubbles resonance frequency. Bubbles that are at resonance or far away from resonance engender identical responses. From the optical data, the larger bubbles showed different dynamics when up-sweep or down-sweep chirps were transmitted. Smaller bubbles (< 2 mum diameter) appear to be less sensitive to frequency sweep at 1.7 MHz center frequency. However, driven at a higher center frequency, smaller bubbles tend to be more sensitive. These results were confirmed through the acoustical measurements. We concluded that simulations and experimental data show that significant differences might be observed between bubblesiquest responses to UPF and DNF chirps. We demonstrate in this study that, for an optimal use of chirp reversal, the transmit frequency should be higher than the resonance frequency of the contrast microbubbles.
机译:微泡的主动响应的特征在于其共振行为,其中在关闭激励波形后微泡可能会振荡。我们在本文中研究了一种基于chi的共振现象的激励方法。该技术被称为线性调频反向,包括发射第一激励信号,随时间增加频率的上扫线性调频(UPF)和第二激励信号,即下扫频(DNF),它是第一信号的副本,但时间随着频率的降低而倒转。进行了使用改进的Rayleigh-Plesset方程的模拟,以确定气泡对线性调频反向的响应。另外,进行了光学观察和声学测量以证实理论发现。仿真结果表明,主要针对高于气泡共振频率的传输中心频率,气泡响应上升和下降的线性调频振荡之间的差异。处于共振或远离共振的气泡会产生相同的响应。从光学数据来看,当传输上扫或下扫chi时,较大的气泡显示出不同的动力。较小的气泡(小于2毫米的直径)似乎对1.7 MHz中心频率的扫频不太敏感。但是,以较高的中心频率驱动时,较小的气泡往往更敏感。这些结果通过声学测量得到证实。我们得出的结论是,模拟和实验数据表明,在对UPF和DNF线性调频脉冲的气泡请求响应之间可能会观察到显着差异。我们在这项研究中证明,对于an反向的最佳使用,传输频率应高于对比微泡的共振频率。

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