Aliev Mayis K, Tikhonov Alexander N
Institute of Experimental Cardiology, Cardiology Research Center, Moscow, Russia.
Mol Cell Biochem. 2004 Jan-Feb;256-257(1-2):257-66. doi: 10.1023/b:mcbi.0000009873.37245.54.
The purpose of this work was the development of a basal mathematical model for the diffusion of low-molecular metabolites in a skeletal muscle cell. A three-dimension diffusion of low-molecular particles was simulated by a Monte-Carlo method (random walks of diffusing molecules). The model takes into account the following structural elements: (i) a regular lattice of actin and myosin filaments inside a myofibril; (ii) the membranes of sarcoplasmic reticulum and mitochondria surrounding the myofibrils; (iii) a set of myofibrils inside a skeletal muscle cell. We simulated diffusion of particles in the bulk of intracellular water phase and their reflections from the rigid surfaces of intracellular structures. The model allowed to calculate the apparent coefficients of particle diffusion in the axial and radial directions, Dparallel(app) and Dperpendicular(app), respectively. In accordance with experimental data from literature, the coefficient Dparallel(app) was independent of time. The coefficient of radial diffusion Dperpendicular(app) decreased with time to steady state values similar to that determined by the NMR diffusion spectroscopy methods. The interactions of diffusing particles with thin and thick filaments of myofibrils could explain the decrease in the Dperpendicular(app) value by a factor of 20%. The collisions of particles with myofilaments began to reveal themselves as a gradual decrease in the Dperpendicular(app) value at early stages of diffusion (t1/2 approximately equal to 0.05 microsec). The contribution of particle reflections from the membranes of sarcoplasmic reticulum and mitochondria to the retardation of the radial diffusion was about of 20-30%, depending on porosity of a membranous shield around the myofibril. For conventional sizes of a membranous shield (diameter 2 microm), the interactions of particles with the shield caused a decrease in the Dperpendicular(app) value with a half-time t1/2 approximately equal to 0.5 msec. This time is essentially lower by a factor about of 100 than that found in published NMR measurements. When we considered diffusion of particles inside a cell compartment confined to impermeable membranous shield, the reflection of particles from this shield led the drastic decrease in the radial diffusion coefficient (Dperpendicular(app) --> porportional to when t --> porportional to). This pattern of the Dperpendicular(app)(t) time-course might be expected in the NMR measurements on skeletal muscle tissue where a sarcolemma represents an impermeable shield for ATP and PCr molecules.
这项工作的目的是开发一个用于模拟低分子代谢物在骨骼肌细胞中扩散的基础数学模型。采用蒙特卡洛方法(扩散分子的随机游走)模拟了低分子颗粒的三维扩散。该模型考虑了以下结构要素:(i)肌原纤维内肌动蛋白和肌球蛋白丝的规则晶格;(ii)围绕肌原纤维的肌浆网和线粒体膜;(iii)骨骼肌细胞内的一组肌原纤维。我们模拟了颗粒在细胞内水相主体中的扩散以及它们从细胞内结构刚性表面的反射。该模型能够分别计算颗粒在轴向和径向上的表观扩散系数,即Dparallel(app)和Dperpendicular(app)。根据文献中的实验数据,系数Dparallel(app)与时间无关。径向扩散系数Dperpendicular(app)随时间下降至稳态值;该稳态值与通过核磁共振扩散光谱法测定的值相似。扩散颗粒与肌原纤维的细肌丝和粗肌丝之间的相互作用可以解释Dperpendicular(app)值下降20%的原因。在扩散早期(t1/2约等于0.05微秒),颗粒与肌丝的碰撞开始表现为Dperpendicular(app)值逐渐下降。肌浆网和线粒体膜对颗粒的反射对径向扩散延迟的贡献约为20% - 30%,这取决于围绕肌原纤维的膜状屏障的孔隙率。对于常规尺寸的膜状屏障(直径2微米),颗粒与屏障的相互作用导致Dperpendicular(app)值下降,其半衰期t1/2约等于0.5毫秒。这个时间比已发表的核磁共振测量结果低约100倍。当我们考虑颗粒在由不可渗透的膜状屏障限定的细胞区室内扩散时,颗粒从该屏障的反射导致径向扩散系数急剧下降(当t趋于无穷时Dperpendicular(app)趋于零)。在对骨骼肌组织进行核磁共振测量时,预计会出现这种Dperpendicular(app)(t)时间进程模式,因为肌膜对ATP和PCr分子来说是不可渗透的屏障。