Bovendeerd P H, Arts T, Huyghe J M, van Campen D H, Reneman R S
Department of Biophysics, University of Limburg, Maastricht, The Netherlands.
J Biomech. 1992 Oct;25(10):1129-40. doi: 10.1016/0021-9290(92)90069-d.
The dependence of local left ventricular (LV) mechanics on myocardial muscle fiber orientation was investigated using a finite element model. In the model we have considered anisotropy of the active and passive components of myocardial tissue, dependence of active stress on time, strain and strain rate, activation sequence of the LV wall and aortic afterload. Muscle fiber orientation in the LV wall is quantified by the helix fiber angle, defined as the angle between the muscle fiber direction and the local circumferential direction. In a first simulation, a transmural variation of the helix fiber angle from +60 degrees at the endocardium through 0 degrees in the midwall layers to -60 degrees at the epicardium was assumed. In this simulation, at the equatorial level maximum active muscle fiber stress was found to vary from about 110 kPa in the subendocardial layers through about 30 kPa in the midwall layers to about 40 kPa in the subepicardial layers. Next, in a series of simulations, muscle fiber orientation was iteratively adapted until the spatial distribution of active muscle fiber stress was fairly homogeneous. Using a transmural course of the helix fiber angle of +60 degrees at the endocardium, +15 degrees in the midwall layers and -60 degrees at the epicardium, at the equatorial level maximum active muscle fiber stress varied from 52 kPa to 55 kPa, indicating a remarkable reduction of the stress range. Moreover, the change of muscle fiber strain with time was more similar in different parts of the LV wall than in the first simulation. It is concluded that (1) the distribution of active muscle fiber stress and muscle fiber strain across the LV wall is very sensitive to the transmural distribution of the helix fiber angle and (2) a physiological transmural distribution of the helix fiber angle can be found, at which active muscle fiber stress and muscle fiber strain are distributed approximately homogeneously across the LV wall.
利用有限元模型研究了局部左心室(LV)力学对心肌肌纤维取向的依赖性。在该模型中,我们考虑了心肌组织主动和被动成分的各向异性、主动应力对时间、应变和应变率的依赖性、左心室壁的激活顺序以及主动脉后负荷。左心室壁中的肌纤维取向通过螺旋纤维角来量化,螺旋纤维角定义为肌纤维方向与局部圆周方向之间的夹角。在第一次模拟中,假设螺旋纤维角的透壁变化从心内膜处的+60度到中层的0度,再到心外膜处的-60度。在该模拟中,在赤道水平处,发现最大主动肌纤维应力从心内膜下层的约110 kPa变化到中层的约30 kPa,再到心外膜下层的约40 kPa。接下来,在一系列模拟中,反复调整肌纤维取向,直到主动肌纤维应力的空间分布相当均匀。使用心内膜处螺旋纤维角为+60度、中层为+15度、心外膜处为-60度的透壁过程,在赤道水平处,最大主动肌纤维应力从52 kPa变化到55 kPa,表明应力范围显著减小。此外,左心室壁不同部位肌纤维应变随时间的变化比第一次模拟中更为相似。得出的结论是:(1)左心室壁上主动肌纤维应力和肌纤维应变的分布对螺旋纤维角的透壁分布非常敏感;(2)可以找到一种生理透壁分布的螺旋纤维角,在此情况下,主动肌纤维应力和肌纤维应变在左心室壁上近似均匀分布。