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Modeling of nonlinear viscous stress in encapsulating shells of lipid-coated contrast agent microbubbles

机译:脂质包裹的造影剂微泡封装壳中的非线性粘性应力建模

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A general theoretical approach to the development of zero-thickness encapsulation models for contrast microbubbles is proposed. The approach describes a procedure that allows one to recast available rheological laws from the bulk form to a surface form which is used in a modified Rayleigh-Plesset equation governing the radial dynamics of a contrast microbubble. By the use of the proposed procedure, the testing of different rheological laws for encapsulation can be carried out. Challenges of existing shell models for lipid-encapsulated microbubbles, such as the dependence of shell parameters on the initial bubble radius and the "compression-only" behavior, are discussed. Analysis of the rheological behavior of lipid encapsulation is made by using experimental radius-time curves for lipid-coated microbubbles with radii in the range 1.2-2.5 mu m. The curves were acquired for a research phospholipid-coated contrast agent insonified with a 20 cycle, 3.0 MHz, 100 kPa acoustic pulse. The fitting of the experimental data by a model which treats the shell as a viscoelastic solid gives the values of the shell surface viscosity increasing from 0.30 x 10 (8) kg/s to 2.63 x 10 (8) kg/s for the range of bubble radii, indicated above. The shell surface elastic modulus increases from 0.054 N/m to 0.37 N/m. It is proposed that this increase may be a result of the lipid coating possessing the properties of both a shear-thinning and a strain-softening material. We hypothesize that these complicated rheological properties do not allow the existing shell models to satisfactorily describe the dynamics of lipid encapsulation. In the existing shell models, the viscous and the elastic shell terms have the linear form which assumes that the viscous and the elastic stresses acting inside the lipid shell are proportional to the shell shear rate and the shell strain, respectively, with constant coefficients of proportionality. The analysis performed in the present paper suggests that a more general, nonlinear theory may be more appropriate. It is shown that the use of the nonlinear theory for shell viscosity allows one to model the "compression-only" behavior. As an example, the results of the simulation for a 2.03 mu m radius bubble insonified with a 6 cycle, 1.8 MHz, 100 kPa acoustic pulse are given. These parameters correspond to the acoustic conditions under which the "compression-only" behavior was observed by de Jong et al. [Ultrasound Med. Biol. 33 (2007) 653-656]. It is also shown that the use of the Cross law for the modeling of the shear-thinning behavior of shell viscosity reduces the variance of experimentally estimated values of the shell viscosity and its dependence on the initial bubble radius. (C) 2008 Elsevier B. V. All rights reserved.
机译:提出了开发用于对比微泡的零厚度封装模型的一般理论方法。该方法描述了一种程序,该程序允许人们将可用的流变规律从本体形式转换为表面形式,该形式用于控制对比微气泡径向动力学的修改的Rayleigh-Plesset方程中。通过使用所提出的程序,可以对封装的不同流变律进行测试。讨论了现有的壳模型对脂质包裹的微泡的挑战,例如壳参数对初始泡半径和“仅压缩”行为的依赖性。通过使用半径为1.2-2.5μm的脂质包裹的微泡的实验半径时间曲线来分析脂质包裹的流变行为。曲线是用20个周期,3.0 MHz,100 kPa声脉冲声化的研究性磷脂涂层造影剂获得的。通过将壳视为粘弹性固体的模型对实验数据进行拟合,得出在以下范围内壳表面粘度值从0.30 x 10(8)kg / s增加到2.63 x 10(8)kg / s。气泡半径,如上所示。壳表面弹性模量从0.054 N / m增加到0.37 N / m。提出这种增加可能是由于脂质涂层具有剪切稀化和应变软化材料的特性。我们假设这些复杂的流变特性不允许现有的壳模型令人满意地描述脂质封装的动力学。在现有的壳模型中,粘性和弹性壳项具有线性形式,其中假定作用在脂质壳内部的粘性和弹性应力分别与壳的剪切速率和壳的应变成比例,并且比例系数不变。本文进行的分析表明,更通用的非线性理论可能更合适。结果表明,使用非线性理论计算壳的粘度可以模拟“仅压缩”行为。例如,给出了一个以6个周期,1.8 MHz,100 kPa声脉冲声化的2.03μm半径气泡的仿真结果。这些参数对应于de Jong等人观察到的“仅压缩”行为的声学条件。 [超声医学。生物学33(2007)653-656]。还表明,使用克罗斯定律对壳粘度的剪切稀化行为进行建模可以减少壳粘度的实验估算值的变化及其对初始气泡半径的依赖性。 (C)2008 Elsevier B. V.保留所有权利。

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