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嵌套微泡的惯性空化阈值。

Inertial cavitation threshold of nested microbubbles.

作者信息

Wallace N, Dicker S, Lewin Peter, Wrenn S P

机构信息

Department of Chemical Engineering, Drexel University, Philadelphia, PA, USA.

Department of Chemical Engineering, Drexel University, Philadelphia, PA, USA.

出版信息

Ultrasonics. 2015 Apr;58:67-74. doi: 10.1016/j.ultras.2014.12.004. Epub 2015 Jan 7.

Abstract

Cavitation of ultrasound contrast agents (UCAs) promotes both beneficial and detrimental bioeffects in vivo (Radhakrishnan et al., 2013) [1]. The ability to determine the inertial cavitation threshold of UCA microbubbles has potential application in contrast imaging, development of therapeutic agents, and evaluation of localized effects on the body (Ammi et al., 2006) [2]. This study evaluates a novel UCA and its inertial cavitation behavior as determined by a home built cavitation detection system. Two 2.25 MHz transducers are placed at a 90° angle to one another where one transducer is driven by a high voltage pulser and the other transducer receives the signal from the oscillating microbubble. The sample chamber is placed in the overlap of the focal region of the two transducers where the microbubbles are exposed to a pulser signal consisting of 600 pulse trains per experiment at a pulse repetition frequency of 5 Hz where each train has four pulses of four cycles. The formulation being analyzed is comprised of an SF6 microbubble coated by a DSPC PEG-3000 monolayer nested within a poly-lactic acid (PLA) spherical shell. The effect of varying shell diameters and microbubble concentration on cavitation threshold profile for peak negative pressures ranging from 50 kPa to 2 MPa are presented and discussed in this paper. The nesting shell decreases inertial cavitation events from 97.96% for an un-nested microbubble to 19.09% for the same microbubbles nested within a 2.53 μm shell. As shell diameter decreases, the percentage of inertially cavitating microbubbles also decreases. For nesting formulations with average outer capsule diameters of 20.52, 14.95, 9.95, 5.55, 2.53, and 1.95 μm, the percentage of sample destroyed at 1 MPa was 51.02, 38.94, 33.25, 25.27, 19.09, and 5.37% respectively.

摘要

超声造影剂(UCAs)的空化作用在体内既会产生有益的生物效应,也会产生有害的生物效应(Radhakrishnan等人,2013年)[1]。确定UCA微泡惯性空化阈值的能力在超声造影成像、治疗剂开发以及对身体局部效应的评估方面具有潜在应用价值(Ammi等人,2006年)[2]。本研究评估了一种新型UCA及其通过自制空化检测系统测定的惯性空化行为。两个2.25 MHz的换能器相互呈90°角放置,其中一个换能器由高压脉冲发生器驱动,另一个换能器接收来自振荡微泡的信号。样品室置于两个换能器焦点区域的重叠处,微泡在此处暴露于每个实验由600个脉冲序列组成的脉冲发生器信号,脉冲重复频率为5 Hz,每个序列有四个四周期的脉冲。所分析的制剂由包裹在聚乳酸(PLA)球形壳内的、被二硬脂酰磷脂酰胆碱聚乙二醇-3000单层包被的SF6微泡组成。本文呈现并讨论了在50 kPa至2 MPa的峰值负压范围内,壳直径和微泡浓度变化对空化阈值分布的影响。嵌套壳使惯性空化事件从未嵌套微泡的97.96%降至嵌套在2.53 μm壳内的相同微泡的19.09%。随着壳直径减小,惯性空化微泡的百分比也降低。对于平均外囊直径分别为20.52、14.95、9.95、5.55、2.53和1.95 μm的嵌套制剂,在1 MPa下样品被破坏的百分比分别为51.02%、38.94%、33.25%、25.27%、19.09%和5.37%。

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