Borejdo J, Burlacu S
Baylor Research Foundation, Baylor University Medical Center, Dallas, TX 75226.
J Muscle Res Cell Motil. 1991 Aug;12(4):394-407. doi: 10.1007/BF01738594.
F-actin was electrophoresed in capillary tubes filled with agarose gel. The use of capillary imparted high resistance on the gel allowing the use of high enough concentration of salts to keep F-actin polymerized, and allowed the application of high electric fields without liberating considerable amount of heat. The intensity profile of the electrophoretic band of F-actin showed a peak, which in 1% agarose in the electric field of 17.8 V cm-1 at 0 degree C, migrated at 3.4 cm hr-1. Microscopic observation of actin filaments extracted from different positions along the gel showed that during electrophoresis filaments distributed themselves in such a manner that the longest polymers migrated slowest and the shortest migrated fastest. Using this observation we calculated the weight and number distributions of filament lengths from corresponding experimental intensity profiles. Phalloidin-labelled F-actin oriented in the gel upon application of an electric field. F-actin showed unusual orientational response: it oriented rapidly when the field was applied, but relaxed very slowly when the field was removed. Orientation of F-actin varied within an electrophoretic band, longest polymers showing the best orientation and short oligomers and monomers not orienting at all. The degree of orientation increased with the size of the electric field. When F-actin was labelled with phalloidin before electrophoresis, it was no longer able to migrate in the gel, but the electric field oriented it in the same way as when it was labelled after the electrophoresis. These results show that the electrophoresis of F-actin in agarose fractionates it according to its length, that by using electrophoresis it is possible to rapidly obtain distribution of filament lengths, and that F-actin migrates in agarose by the process of reptation.
F-肌动蛋白在填充有琼脂糖凝胶的毛细管中进行电泳。毛细管的使用使凝胶具有高电阻,从而能够使用足够高浓度的盐来保持F-肌动蛋白聚合,并允许施加高电场而不会释放大量热量。F-肌动蛋白电泳带的强度分布显示出一个峰值,在0℃下17.8V/cm的电场中,1%琼脂糖中的F-肌动蛋白以3.4cm/h的速度迁移。对从凝胶不同位置提取的肌动蛋白丝进行显微镜观察表明,在电泳过程中,丝的分布方式是最长的聚合物迁移最慢,最短的迁移最快。利用这一观察结果,我们从相应的实验强度分布计算出丝长度的重量和数量分布。施加电场时,鬼笔环肽标记的F-肌动蛋白在凝胶中定向。F-肌动蛋白表现出不同寻常的定向响应:施加电场时它迅速定向,但去除电场时松弛非常缓慢。F-肌动蛋白的定向在电泳带内有所不同,最长的聚合物表现出最佳的定向,而短的寡聚物和单体根本不发生定向。定向程度随电场强度的增加而增加。在电泳前用鬼笔环肽标记F-肌动蛋白时,它不再能够在凝胶中迁移,但电场以与电泳后标记时相同的方式使其定向。这些结果表明,F-肌动蛋白在琼脂糖中的电泳根据其长度对其进行分离,通过电泳可以快速获得丝长度的分布,并且F-肌动蛋白在琼脂糖中通过蛇行过程迁移。