纤溶过程中纤维蛋白网络和血浆凝块的原子力显微镜

A. Blinc, J. Magdić, J. Frič, I. Muševič
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引用次数: 26

摘要

摘要利用原子力显微镜(AFM)对纤维蛋白纤维溶解的超微结构进行了实时研究。在玻璃表面制备纯化的薄纤维蛋白凝胶和血浆凝块,并在AFM液体细胞中覆盖等渗盐水或肝素化血浆。通过将纤溶酶或重组组织型纤溶酶原激活剂(rt-PA)引入洗浴凝块的溶液中来启动纤溶。在Nanoscope III原子力显微镜上以轻叩或接触模式连续实时进行显微镜观察。单幅图像的采集时间为2 ~ 8 min,成像时间长达1 h,视场范围为128 × 128 μm ~ 0.7 × 0.7 μm,分辨率为512 × 512像素。在最小的视野中,纤维蛋白纤维是由直径40-70纳米的球体组成的。纤维蛋白原溶液中NaCl浓度对纯化凝胶中复合纤维蛋白纤维的直径影响较大:150 mmol/l NaCl溶液中复合纤维蛋白纤维直径为250±155 nm, 50 mmol/l NaCl溶液中复合纤维蛋白纤维直径为1.42±0.19 μm。血浆凝块由粗纤维和穿插的细纤维组成。富血小板血浆凝块的粗纤维和细纤维的直径明显小于贫血小板血浆凝块的相应纤维类型(620±195 nm vs 965±200 nm, 195±30 nm vs 260±60 nm)
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Atomic force microscopy of fibrin networks and plasma clots during fibrinolysis
Abstract We have used atomic force microscopy (AFM) in order to study the ultrastructure of fibrin fibre dissolution in real time. Thin purified fibrin gels and plasma clots were prepared on glass surfaces and overlaid with isotonic saline or heparinized plasma in an AFM fluid-cell. Fibrinolysis was initiated by introducing plasmin or recombinant tissue-type plasminogen activator (rt-PA) into the solution bathing the clots. Microscopy was performed serially in real time on the Nanoscope III Atomic Force Microscope operating in the tapping or contact mode. The acquisition time for a single image was 2–8 min and the clots were imaged for up to 1 h with fields of view ranging from 128 × 128 μm to 0.7 × 0.7 μm with a resolution of 512 × 512 pixels. In the smallest fields of view fibrin fibres were seen to be composed of globules 40–70 nm in diameter. The diameter of composite fibrin fibres in purified gels depended on the concentration of NaCl in the fibrinogen solution: 250 ± 155 nm in 150 mmol/l NaCl vs. 1.42 ± 0.19 μm in 50 mmol/l NaCl. Plasma clots were composed of thick fibres with interspersed thinner fibres. In clots from platelet-rich plasma both the thick and the thin fibres had significantly smaller diameters than the corresponding fibre types in clots from platelet-depleted plasma (620 ± 195 nm vs. 965 ± 200 nm, and 195 ± 30 nm vs. 260 ± 60 nm, P
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