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. Magdic , J. Fric , I. Musevic
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引用次数: 26

摘要

我们使用原子力显微镜(AFM)实时研究纤维蛋白纤维溶解的超微结构。在玻璃表面上制备薄的纯化纤维蛋白凝胶和血浆凝块,并在AFM流体细胞中用等渗盐水或肝素化血浆覆盖。纤维蛋白溶解是通过将纤溶酶或重组组织型纤溶酶原激活剂(rt-PA)引入浸泡血栓的溶液中来启动的。在以轻敲或接触模式操作的Nanoscope III原子力显微镜上连续实时进行显微镜检查。单个图像的采集时间为2–8分钟,血栓成像时间长达1小时,视野范围为128×128μm至0.7×0.7μm,分辨率为512×512像素。在最小的视野中,纤维蛋白纤维由直径为40–70 nm的球组成。纯化凝胶中复合纤维蛋白纤维的直径取决于纤维蛋白原溶液中的NaCl浓度:在150 mmol/l NaCl中为250±155 nm,在50 mmol/l的NaCl中为1.42±0.19μm。血浆凝块由粗纤维和稀疏纤维组成。在来自富含血小板的血浆的凝块中,粗纤维和细纤维的直径均显著小于来自贫血小板的血浆凝块中相应纤维类型的直径(620±195 nm对965±200 nm,195±30 nm对260±60 nm,两种比较的P<0.001)。无论是由纤溶酶还是rt-PA引发,粗纤维和细纤维的纤溶主要通过给定部位整个纤维厚度的横向切片进行。用2.5 U/ml纤溶酶完成纤维切片的时间在薄纤维蛋白纤维和厚纤维蛋白纤维之间没有差异(7.6±3.7分钟对6.4±4.2分钟)。在低浓度纤溶酶(0.17U/ml)的情况下,一些纤维蛋白纤维在被切割之前沿着其整个观察到的长度变得更薄。较厚纤维的纤维变薄速度是较薄纤维的3倍。我们得出的结论是,“穿透”模式是纯化凝胶和血浆凝块中纤维蛋白溶解的主要方式,导致纤维断裂的蛋白水解在厚复合纤维蛋白纤维中比在薄复合纤维蛋白中更有效。
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

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< 0.001 for both comparisons). Fibrinolysis of both thick and thin fibres proceeded predominantly by lateral section of the whole fibre thickness at a given site, regardless of whether it was initiated by plasmin or by rt-PA. The time to complete fibre section by 2.5 U/ml of plasmin did not differ between thin and thick fibrin fibres (7.6 ± 3.7 min vs. 6.4 ± 4.2 min). With a low concentration of plasmin (0.17 U/ml) some fibrin fibres became thinner along their entire observed length before they were cleaved. The rate of fibre thinning was 3-times faster in the thicker fibres than in the thinner ones. We conclude that the ‘cut-through’ pattern is the predominant way of fibrinolysis in purified gels and in plasma clots, and that proteolysis leading towards fibre cleavage proceeds more efficiently in thick than in thin composite fibrin fibres.

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