Maughan D W, Godt R E
Biophys Struct Mech. 1980;7(1):17-40. doi: 10.1007/BF00538156.
The elastic behavior of mechanically skinned skeletal muscle fibers in relaxing solution is modelled using equations developed by Flory (1953) for the elasticity of non-biological polymers. Mechanically, the relaxed skinned fiber is considered to be a semi-crystalline network of inextensible polymer chains, which are periodically cross-linked and which are bathed in an aqueous medium. We consider (1) configurational elastic forces in the network, (2) entropic forces due to mixing of polymer and water, (3) electrostatic forces due to fixed charges on the muscle proteins and mobile charges in the bathing solution, and (4) compressive forces due to large colloids in the bathing solution. Van der Waals forces are not considered since calculations show that they are probably negligible under our conditions. We derive an expression which relates known quantities (ionic strength, osmotic compressive pressure, and fiber width), experimentally estimated quantities (fixed charge density and volume fraction of muscle proteins), and derived quantities (concentration of cross-links and a parameter reflecting the interaction energy between protein and water). The model was tested by comparison with observed changes in skinned fiber width under a variety of experimental conditions which included changes in osmotic compressive pressure, pH, sarcomere length, and ionic strength. Over a wide range of compressive pressure (0-36 atm) the theory predicted the nonlinear relation between fiber width and logarithm of pressure. The direction and magnitude of the decrease in width when pH was decreased to 4 could be modelled assuming the fixed charge density on the protein network was 0.34 moles of electrons per liter protein, a value in accordance with the estimates of others. The relation between width and sarcomere length over the complete range of compressive pressures could be modelled with the assumption that the number of cross-links increases somewhat with sarcomere length. Changes of width with ionic strength were modelled assuming that increasing salt concentration both increased the electrostatic shielding of fixed charges and decreased the number of cross-links. The decrease of fiber width in 1% glutaraldehyde was modelled by assuming that the concentration of crosslinks increased by some 10%. The theory predicted the order of magnitude but not the detailed shape of the passive tension-length relation which may indicate that, as with non-biological polymers, the theory does not adequately describe the behavior of semi-crystalline networks at high degrees of deformation. In summary, the theory provides a semiquantitative approach to an understanding of the nature and relative magnitudes of the forces underlying the mechanical behavior of relaxed skinned fibers. It indicates, for instance, that when fibers are returned to near their in vivo size with 3% PVP, the forces in order of their importance are: (elastic forces) approximately (entropic forces) greater than (electrostatic forces) approximately (osmotic compressive forces).
利用弗洛里(1953年)为非生物聚合物弹性所推导的方程,对处于松弛溶液中的机械剥制骨骼肌纤维的弹性行为进行了建模。从力学角度来看,松弛的剥制纤维被视为一个由不可伸展的聚合物链组成的半结晶网络,这些链会周期性交联,并浸泡在水性介质中。我们考虑了以下因素:(1)网络中的构型弹力;(2)聚合物与水混合产生的熵力;(3)肌肉蛋白质上的固定电荷与浸泡溶液中移动电荷产生的静电力;(4)浸泡溶液中大分子胶体产生的压缩力。由于计算表明在我们的条件下范德华力可能可忽略不计,因此未予以考虑。我们推导了一个表达式,该表达式关联了已知量(离子强度、渗透压和纤维宽度)、实验估计量(固定电荷密度和肌肉蛋白质的体积分数)以及推导量(交联浓度和反映蛋白质与水之间相互作用能的一个参数)。通过与在各种实验条件下(包括渗透压、pH值、肌节长度和离子强度的变化)观察到的剥制纤维宽度变化进行比较,对该模型进行了测试。在较宽的压力范围(0 - 36个大气压)内,该理论预测了纤维宽度与压力对数之间的非线性关系。当pH值降至4时宽度减小的方向和幅度可以通过假设蛋白质网络上的固定电荷密度为每升蛋白质0.34摩尔电子来进行建模,该值与其他人的估计相符。在整个压力范围内,宽度与肌节长度之间的关系可以通过假设交联数随肌节长度略有增加来进行建模。宽度随离子强度的变化通过假设盐浓度增加既增加了固定电荷的静电屏蔽又减少了交联数来进行建模。在1%戊二醛中纤维宽度的减小通过假设交联浓度增加约10%来进行建模。该理论预测了被动张力 - 长度关系的量级,但未预测其详细形状,这可能表明,与非生物聚合物一样,该理论在高变形程度下不能充分描述半结晶网络的行为。总之,该理论为理解松弛剥制纤维力学行为背后的力的性质和相对大小提供了一种半定量方法。例如,它表明当用3%聚乙烯吡咯烷酮使纤维恢复到接近其体内大小时,按重要性排序的力为:(弹力)近似(熵力)大于(静电力)近似(渗透压)。