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青蛙离体肌纤维“等长”舒张过程中肌节动力学的激光衍射研究。

Laser diffraction studies of sarcomere dynamics during 'isometric' relaxation in isolated muscle fibres of the frog.

作者信息

Edman K A, Flitney F W

出版信息

J Physiol. 1982 Aug;329:1-20. doi: 10.1113/jphysiol.1982.sp014287.

DOI:10.1113/jphysiol.1982.sp014287
PMID:6982971
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1224764/
Abstract
  1. A study has been made of changes in sarcomere length and tension which occur during relaxation from isometric (;fixed ends') tetani in isolated muscle fibres of the frog. Sarcomere lengths were calculated from measurements of the separation of the zero-to-first-order intensity maxima in diffraction patterns generated by illuminating small segments of fibre with a He-Ne laser. Diffraction spectra were recorded continuously on cine-film using the method of ;streak' photography.2. Many sarcomeres in a muscle fibre are found to undergo active shortening during relaxation, at the expense of others located elsewhere which become passively extended. The time of onset of changes in sarcomere length coincides with the well known ;shoulder' on the tension record, and their amplitude is maximal at the time when isometric force approaches zero. The original pattern of sarcomere lengths is only re-established after tension has disappeared.3. The variability in the pattern of sarcomere length changes during relaxation was studied in a sample of twenty fibres, by making ;streak' recordings from successive 1 mm segments along the entire length of each fibre. This survey showed that segments which elongate are located predominantly, though not exclusively, close to the fibre ends. The fractional length of the fibre which underwent shortening was found to vary considerably in different preparations. In many ;streak' recordings the first order line fragmented into several distinct intensity maxima.4. The effects of varying the initial fibre length on the time course of the tension decay and on the accompanying changes in sarcomere length were studied. The range of fibre lengths investigated corresponded with sarcomere spacings of 1.9-3.2 mum. The rate constant, R, for the exponential (later) component of the tension decay decreased with increasing fibre length and this was accompanied by a reduction in the mean amplitude of sarcomere shortening [Formula: see text] and lengthening [Formula: see text]. However, the time interval during which sarcomeres shortened or elongated increased, and so the mean velocities of sarcomere length changes ([Formula: see text] and [Formula: see text]) also displayed an inverse dependence upon fibre length.5. The effects of altering temperature (0-20 degrees C) on the time course of the changes in sarcomere length and tension were investigated. The time to onset of the length changes, t(1), the time to maximum amplitude, t(2), and the time to full recovery, t(3), all decreased exponentially with increasing temperature, but to differing extents. Temperature co-efficients for the velocity of sarcomere length changes during the interval t(2) - t(1) and for the fast tension decay were 2.47 ([Formula: see text]), 2.54 ([Formula: see text]) and 2.45 (R). The rate of the slow tension decay (before the tension ;shoulder') also increased with temperature, with a Q(10) of 2.43.6. The complex patterns of sarcomere length changes seen during relaxation appear to be due to variations in the duration of mechanical activity in different fibre segments. A model is presented which shows that the characteristic form of the tension decay can be accounted for by the progressive emergence of local inequalities in the relative strengths of adjacent sarcomeres, as relaxation proceeds.
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a63c/1224764/082910144e72/jphysiol00674-0032-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a63c/1224764/082910144e72/jphysiol00674-0032-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a63c/1224764/082910144e72/jphysiol00674-0032-a.jpg
摘要
  1. 对青蛙离体肌纤维等长(“固定两端”)强直收缩后松弛过程中肌节长度和张力的变化进行了研究。肌节长度通过测量用氦氖激光照射纤维小段产生的衍射图样中零级到一级强度最大值之间的距离来计算。衍射光谱采用“条纹”摄影法连续记录在电影胶片上。

  2. 发现肌纤维中的许多肌节在松弛过程中会主动缩短,代价是位于其他部位的肌节被动延长。肌节长度变化开始的时间与张力记录上众所周知的“肩部”一致,其幅度在等长力接近零时最大。只有在张力消失后,肌节长度的原始模式才会重新建立。

  3. 通过对每根纤维全长上连续的1毫米小段进行“条纹”记录,研究了20根纤维样本在松弛过程中肌节长度变化模式的变异性。这项研究表明,伸长的小段主要(但并非唯一)位于纤维末端附近。发现不同标本中发生缩短的纤维部分长度差异很大。在许多“S条纹”记录中,一级线分裂成几个明显的强度最大值。

  4. 研究了改变初始纤维长度对张力衰减时间进程以及伴随的肌节长度变化的影响。所研究的纤维长度范围对应于1.9 - 3.2微米的肌节间距。张力衰减指数(后期)成分的速率常数R随纤维长度增加而降低,同时肌节缩短[公式:见原文]和延长[公式:见原文]的平均幅度也减小。然而,肌节缩短或延长的时间间隔增加,因此肌节长度变化的平均速度([公式:见原文]和[公式:见原文])也呈现出与纤维长度的反比关系。

  5. 研究了改变温度(0 - 20摄氏度)对肌节长度和张力变化时间进程的影响。长度变化开始的时间t(1)、达到最大幅度的时间t(2)以及完全恢复的时间t(3),均随温度升高呈指数下降,但下降程度不同。在t(2) - t(1)区间内肌节长度变化速度的温度系数以及快速张力衰减的温度系数分别为2.47([公式:见原文])、2.54([公式:见原文])和2.45(R)。缓慢张力衰减(在张力“肩部”之前)的速率也随温度升高,Q(10)为2.43。

  6. 松弛过程中观察到的肌节长度变化的复杂模式似乎是由于不同纤维段机械活动持续时间的差异所致。提出了一个模型,该模型表明,随着松弛的进行,相邻肌节相对强度局部不平等的逐渐出现可以解释张力衰减的特征形式。

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