包被微泡的脂质分布和粘度

K. Kooiman, M. Emmer, T. Kokhuis, J. Bosch, H. D. de Gruiter, M. V. van Royen, W. V. van Cappellen, A. Houtsmuller, A. V. D. van der Steen, N. de Jong
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引用次数: 14

摘要

超声造影剂由直径在1到10微米之间的充满气体的涂层微泡组成。在超声场中,类似大小的微气泡的反应有很大差异。不均匀涂层性能被认为是根本原因。到目前为止,这种涂层的特性,如粘度,已经在超声场中使用振动微泡装置进行了动态研究。本研究的重点是在静态设置中确定脂包微泡涂层的粘度。涂层的粘度是通过光漂白后荧光恢复(FRAP)测量荧光脂质的迁移率来确定的。我们发现表面剪切粘度为8×10−6 kg/s,与微泡大小无关。此外,我们发现涂层中的脂质分布是不均匀的,并且在不同的微泡中存在差异。总之,本研究表明涂层的静态表面剪切粘度可以独立地确定,现在可以用于微泡动力学模型。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Lipid distribution and viscosity of coated microbubbles
Ultrasound contrast agents consist of gas-filled coated microbubbles with diameters between 1 and 10 µm. Within an ultrasound field, high differences in responses of similar sized microbubbles have been reported. Heterogeneous coating properties have been suggested to be the underlying cause. Until now, properties of this coating, like viscosity have been studied dynamically using a set-up of vibrating microbubbles in an ultrasound field. This study focuses on determining the viscosity of the coating for lipid-coated microbubbles in a static set-up. The viscosity of the coating was determined by measuring the mobility of a fluorescent lipid using Fluorescence Recovery After Photobleaching (FRAP). We found a surface shear viscosity of 8×10−6 kg/s that was independent of the microbubble size. In addition, we found that the lipid distribution in the coating was heterogeneous and varied from microbubble to microbubble. In conclusion, this study shows that the static surface shear viscosity of the coating can be determined in an independent way which can now be used in microbubble dynamics models.
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