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骨骼肌中的肌节长度-张力关系。

The sarcomere length-tension relation in skeletal muscle.

作者信息

ter Keurs H E, Iwazumi T, Pollack G H

出版信息

J Gen Physiol. 1978 Oct;72(4):565-92. doi: 10.1085/jgp.72.4.565.

DOI:10.1085/jgp.72.4.565
PMID:309929
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC2228549/
Abstract

Tension development during isometric tetani in single fibers of frog semitendinosus muscle occurs in three phases: (a) in initial fast-rise phase; (b) a slow-rise phase; and (c) a plateau, which lasts greater than 10 s. The slow-rise phase has previously been assumed to rise out of a progressive increase of sarcomere length dispersion along the fiber (Gordon et al. 1966. J. Physiol. [Lond.]. 184:143--169;184:170--192). Consequently, the "true" tetanic tension has been considered to be the one existing before the onset of the slow-rise phase; this is obtained by extrapolating the slowly rising tension back to the start of the tetanus. In the study by Gordon et al. (1966. J. Physiol. [Lond.] 184:170--192), as well as in the present study, the relation between this extrapolated tension and sarcomere length gave the familiar linear descending limb of the length-tension relation. We tested the assumption that the slow rise of tension was due to a progressive increase in sarcomere length dispersion. During the fast rise, the slow rise, and the plateau of tension, the sarcomere length dispersion at any area along the muscle was less than 4% of the average sarcomere length. Therefore, a progressive increase of sarcomere length dispersion during contraction appears unable to account for the slow rise of tetanic tension. A sarcomere length-tension relation was constructed from the levels of tension and sarcomere length measured during the plateau. Tension was independent of sarcomere length between 1.9 and 2.6 microgram, and declined to 50% maximal at 3.4 microgram. This result is difficult to reconcile with the cross-bridge model of force generation.

摘要

青蛙半腱肌单纤维等长强直收缩过程中的张力发展分为三个阶段

(a) 初始快速上升阶段;(b) 缓慢上升阶段;(c) 持续超过10秒的平台期。此前认为缓慢上升阶段是由于沿纤维的肌节长度离散度逐渐增加所致(Gordon等人,1966年。《生理学杂志》[伦敦]。184:143 - 169;184:170 - 192)。因此,“真正的”强直张力被认为是缓慢上升阶段开始前的张力;这是通过将缓慢上升的张力外推到强直收缩开始时得到的。在Gordon等人(1966年。《生理学杂志》[伦敦]184:170 - 192)的研究以及本研究中,这种外推张力与肌节长度之间的关系给出了熟悉的长度 - 张力关系的线性下降支。我们检验了张力缓慢上升是由于肌节长度离散度逐渐增加这一假设。在张力的快速上升、缓慢上升和平台期,沿肌肉任何区域的肌节长度离散度均小于平均肌节长度的4%。因此,收缩过程中肌节长度离散度的逐渐增加似乎无法解释强直张力的缓慢上升。根据平台期测量的张力水平和肌节长度构建了肌节长度 - 张力关系。在1.9至2.6微米之间,张力与肌节长度无关,在3.4微米时降至最大张力的50%。这一结果难以与力产生的横桥模型相协调。