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青蛙横纹肌的细丝晶格。松弛和僵直肌肉A带中的径向力、晶格稳定性和细丝压缩。

Filament lattice of frog striated muscle. Radial forces, lattice stability, and filament compression in the A-band of relaxed and rigor muscle.

作者信息

Millman B M, Irving T C

机构信息

Department of Physics, University of Guelph, Ontario, Canada.

出版信息

Biophys J. 1988 Sep;54(3):437-47. doi: 10.1016/S0006-3495(88)82977-1.

Abstract

Repulsive pressure in the A-band filament lattice of relaxed frog skeletal muscle has been measured as a function of interfilament spacing using an osmotic shrinking technique. Much improved chemical skinning was obtained when the muscles were equilibrated in the presence of EGTA before skinning. The lattice shrank with increasing external osmotic pressure. At any specific pressure, the lattice spacing in relaxed muscle was smaller than that of muscle in rigor, except at low pressures where the reverse was found. The lattice spacing was the same in the two states at a spacing close to that found in vivo. The data were consistent with an electrostatic repulsion over most of the pressure range. For relaxed muscle, the data lay close to electrostatic pressure curves for a thick filament charge diameter of approximately 26 nm, suggesting that charges stabilizing the lattice are situated about midway along the thick filament projections (HMM-S1). At low pressures, observed spacings were larger than calculated, consistent with the idea that thick filament projections move away from the filament backbone. Under all conditions studied, relaxed and rigor, at short and very long sarcomere lengths, the filament lattice could be modeled by assuming a repulsive electrostatic pressure, a weak attractive pressure, and a radial stiffness of the thick filaments (projections) that differed between relaxed and rigor conditions. Each thick filament projection could be compressed by approximately 5 or 2.6 nm requiring a force of 1.3 or 80 pN for relaxed and rigor conditions respectively.

摘要

利用渗透收缩技术,测量了松弛状态下青蛙骨骼肌A带细丝晶格中的排斥压力与细丝间距的函数关系。在剥皮前使肌肉在乙二醇双四乙酸(EGTA)存在下达到平衡时,化学剥皮效果有了很大改善。晶格随着外部渗透压的增加而收缩。在任何特定压力下,松弛肌肉中的晶格间距都小于强直状态下肌肉的晶格间距,但在低压时情况相反。在接近体内发现的间距时,两种状态下的晶格间距相同。在大部分压力范围内,数据与静电排斥相符。对于松弛肌肉,数据接近厚丝电荷直径约为26 nm时的静电压力曲线,这表明稳定晶格的电荷位于厚丝突起(重链肌球蛋白S1片段,HMM-S1)沿长度的大约中间位置。在低压下,观察到的间距大于计算值,这与厚丝突起远离丝主干的观点一致。在所有研究条件下,无论是松弛状态还是强直状态,在短和非常长的肌节长度下,通过假设排斥性静电压力、弱吸引力压力以及松弛和强直状态下不同的厚丝(突起)径向刚度,可以对细丝晶格进行建模。每个厚丝突起在松弛和强直状态下分别可被压缩约5或2.6 nm,分别需要1.3或80 pN的力。

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