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超声造影剂后向散射对声压的依赖性:理论与实验

The dependence of ultrasound contrast agents backscatter on acoustic pressure: theory versus experiment.

作者信息

Sboros V, MacDonald C A, Pye S D, Moran C M, Gomatam J, McDicken W N

机构信息

Department of Medical Physics and Medical Engineering, University of Edinburgh, Royal Infirmary of Edinburgh, UK.

出版信息

Ultrasonics. 2002 May;40(1-8):579-83. doi: 10.1016/s0041-624x(02)00175-0.

Abstract

Experimental investigations have not fully explored the interaction between ultrasound beams and microbubble contrast agents. Moreover theoretical investigations have not solved the problem of the microbubble oscillation. A simple in-vitro system based on a commercial scanner (ATL UM9) was used to insonate (3 MHz transmission) diluted contrast suspensions of Definity and Quantison at different acoustic pressures (0.27-1.52 MPa). The experimental data were referred to a blood mimicking fluid in order to extract an estimate of their scattering cross-section. The results were compared with the solutions of the three main bubble oscillatidn models, Rayleigh-Plesset, Herring and Gilmore. Non-linear solutions of the above models were produced numerically using the Mathematica Package Software. The experiments showed that both agents provided a linear increase in scattering cross-section with increasing acoustic pressure. The thick shelled Quantison provided an increasing number of scatterers with increasing acoustic pressure, which proved that free bubbles leaked out of the shell. At high acoustic pressures both Quantison and Definity scattering cross-sections were almost identical, and were probably that of a free bubble. The Rayleigh-Plesset model provided a scattering cross-section almost independent of acoustic pressure. On the contrary the scattering cross-sections calculated by the Herring and Gilmore models solutions displayed a definite dependence on acoustic pressure of an order higher than one, which is slightly higher than the order of dependence exhibited by the experimental data. However, the increase of the experimentally measured scattering cross-section with acoustic pressure was sharper than the calculated one by the above two models. This is most probably due to the fact that the models simulated damped and not free bubble oscillations. In conclusion the Rayleigh-Plesset model was inadequate in describing the bubble oscillations even at small diagnostic acoustic pressures. The Herring and Gilmore models could simulate the dependence of the scattering cross-section of encapsulated microbubbles on acoustic pressure. However the contribution of free bubble oscillations has still to be modelled.

摘要

实验研究尚未充分探索超声束与微泡造影剂之间的相互作用。此外,理论研究也未解决微泡振荡问题。基于商用扫描仪(ATL UM9)构建了一个简单的体外系统,用于在不同声压(0.27 - 1.52 MPa)下对Definity和Quantison的稀释造影剂悬浮液进行超声照射(3 MHz发射)。将实验数据与仿血液流体进行对照,以估算其散射截面。将结果与三种主要气泡振荡模型(瑞利 - 普莱斯方程、赫林模型和吉尔摩模型)的解进行比较。使用Mathematica软件包对上述模型的非线性解进行数值计算。实验表明,两种造影剂的散射截面均随声压增加呈线性增加。厚壳的Quantison随着声压增加产生的散射体数量增多,这证明有游离气泡从壳中泄漏出来。在高声压下,Quantison和Definity的散射截面几乎相同,可能是游离气泡的散射截面。瑞利 - 普莱斯模型给出的散射截面几乎与声压无关。相反,赫林模型和吉尔摩模型解计算出的散射截面显示出对声压有明确的高于一阶的依赖性,略高于实验数据所显示的依赖阶数。然而,实验测量的散射截面随声压的增加比上述两个模型计算的更陡峭。这很可能是因为模型模拟的是阻尼气泡振荡而非自由气泡振荡。总之,即使在小诊断声压下,瑞利 - 普莱斯模型也不足以描述气泡振荡。赫林模型和吉尔摩模型可以模拟包封微泡散射截面与声压的依赖性。然而,游离气泡振荡的贡献仍有待建模。

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