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脂质囊泡内微粒的动力学:受限空间内的运动。

Dynamics of microparticles inside lipid vesicles: movement in confined spaces.

机构信息

Centre for Drug Delivery Research, The School of Pharmacy, University of London, London WC1N 1AX, UK.

出版信息

J Drug Target. 2010 Dec;18(10):821-30. doi: 10.3109/1061186X.2010.526228. Epub 2010 Oct 29.

DOI:10.3109/1061186X.2010.526228
PMID:21029030
Abstract

Microparticles and nanoparticles used in drug delivery frequently depend on their movement in confined spaces such as cells. Liposomes containing small numbers of 1-µm diameter polystyrene particles were used to study the dynamics of their movement within the confined space of the liposome interior. The analysis of the trajectories of single and multiple entrapped particles revealed that the particles were largely localized toward the periphery of the liposome with a rare presence in the centre. Interparticle interactions were studied by calculating interparticle distances, ranging from close to zero to around 8 µm with a mean of ∼4 µm. The diffusion coefficient of a single entrapped particle was D = 0.27 × 10(-9) cm(2) s(-1) when compared with 5.1 × 10(-9) cm(2) s(-1) free in water. When more than one particle was entrapped, the calculated diffusion coefficients were D = 0.61 × 10(-9) cm(2) s(-1) for two particles, D = 1.26 × 10(-9) cm(2) s(-1) for three particles, and D = 1.3 × 10(-9) cm(2) s(-1) for multiple particles). Particle movement was found to be distinctly faster at the periphery (average velocity 21.4 μm s(-)1) than at the centre of the vesicle (average velocity 14.2 μm s(-1)). These results demonstrate the significance of particle-particle interactions as well as particle-surface interactions, which is evident here in some systems by particle aggregation close to the liposome membrane.

摘要

用于药物递送的微粒和纳米颗粒通常依赖于它们在细胞等受限空间中的运动。本文使用含有少量 1-µm 直径聚苯乙烯颗粒的脂质体来研究它们在脂质体内部受限空间内的运动动力学。对单个和多个包裹颗粒的轨迹分析表明,颗粒主要定位于脂质体的外围,很少存在于中心。通过计算颗粒间的距离来研究颗粒间的相互作用,范围从接近零到约 8 µm,平均值约为 4 µm。与在水中自由扩散的 5.1×10(-9) cm(2) s(-1)相比,单个包裹颗粒的扩散系数 D = 0.27×10(-9) cm(2) s(-1)。当有多个颗粒被包裹时,计算得到的扩散系数为:两个颗粒时 D = 0.61×10(-9) cm(2) s(-1),三个颗粒时 D = 1.26×10(-9) cm(2) s(-1),多个颗粒时 D = 1.3×10(-9) cm(2) s(-1))。与囊泡中心(平均速度 14.2 μm s(-1))相比,颗粒在囊泡外围的运动速度明显更快(平均速度 21.4 μm s(-1))。这些结果表明了颗粒-颗粒相互作用以及颗粒-表面相互作用的重要性,在某些系统中,靠近脂质体膜的颗粒聚集就证明了这一点。

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