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单个心肌纤维中的被动张力和主动张力。

Passive and active tension in single cardiac myofibrils.

作者信息

Linke W A, Popov V I, Pollack G H

机构信息

Center for Bioengineering, University of Washington, Seattle 98195.

出版信息

Biophys J. 1994 Aug;67(2):782-92. doi: 10.1016/S0006-3495(94)80538-7.

Abstract

Single myofibrils were isolated from chemically skinned rabbit heart and mounted in an apparatus described previously (Fearn et al., 1993; Linke et al., 1993). We measured the passive length-tension relation and active isometric force, both normalized to cross sectional area. Myofibrillar cross sectional area was calculated based on measurements of myofibril diameter from both phase-contrast images and electron micrographs. Passive tension values up to sarcomere lengths of approximately 2.2 microns were similar to those reported in larger cardiac muscle specimens. Thus, the element responsible for most, if not all, passive force of cardiac muscle at physiological sarcomere lengths appears to reside within the myofibrils. Above 2.2 microns, passive tension continued to rise, but not as steeply as reported in multicellular preparations. Apparently, structures other than the myofibrils become increasingly important in determining the magnitude of passive tension at these stretched lengths. Knowing the myofibrillar component of passive tension allowed us to infer the stress-strain relation of titin, the polypeptide thought to support passive force in the sarcomere. The elastic modulus of titin is 3.5 x 10(6) dyn cm-2, a value similar to that reported for elastin. Maximum active isometric tension in the single myofibril at sarcomere lengths of 2.1-2.3 microns was 145 +/- 35 mN/mm2 (mean +/- SD; n = 15). This value is comparable with that measured in fixed-end contractions of larger cardiac specimens, when the amount of nonmyofibrillar space in those preparations is considered. However, it is about 4 times lower than the maximum active tension previously measured in single skeletal myofibrils under similar conditions (Bartoo et al., 1993).

摘要

从化学去表皮的兔心脏中分离出单个肌原纤维,并将其安装在先前描述的装置中(Fearn等人,1993年;Linke等人,1993年)。我们测量了被动长度-张力关系和主动等长力,两者均按横截面积进行归一化。肌原纤维横截面积是根据相差显微镜图像和电子显微镜照片中肌原纤维直径的测量值计算得出的。在肌节长度约为2.2微米之前的被动张力值与在较大心肌标本中报道的值相似。因此,在生理肌节长度下,负责心肌大部分(如果不是全部)被动力的成分似乎存在于肌原纤维内。在2.2微米以上,被动张力继续上升,但不像在多细胞制剂中报道的那样陡峭。显然,在这些拉伸长度下,除肌原纤维之外的结构在决定被动力的大小方面变得越来越重要。了解被动张力的肌原纤维成分使我们能够推断肌联蛋白的应力-应变关系,肌联蛋白是一种被认为在肌节中支持被动力的多肽。肌联蛋白的弹性模量为3.5×10⁶达因/厘米²,该值与报道的弹性蛋白的值相似。在肌节长度为2.1 - 2.3微米时,单个肌原纤维的最大主动等长张力为145±35毫牛/毫米²(平均值±标准差;n = 15)。当考虑那些制剂中非肌原纤维空间的量时,该值与在较大心脏标本的固定端收缩中测量的值相当。然而,它比先前在类似条件下单个骨骼肌肌原纤维中测量的最大主动张力低约4倍(Bartoo等人,1993年)。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f378/1225421/40464d83bbb0/biophysj00072-0298-a.jpg

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