Barr R C, Plonsey R
Biophys J. 1984 Jun;45(6):1191-202. doi: 10.1016/S0006-3495(84)84268-X.
This paper reports on a simulation of propagation for anisotropic two-dimensional cardiac tissue. The tissue structure assumed was that of a Hodgin-Huxley membrane separating inside and outside anisotropic media, obeying Ohm's law in each case. Membrane current was found by an integral expression involving partial spatial derivatives of Vm weighted by a function of distance. Numerical solutions for transmembrane voltage as a function of time following excitation at a single central site were computed using an algorithm that examined only the portion of the tissue undergoing excitation at each moment; thereby, the number of calculations required was reduced to a large but achievable number. Results are shown for several combinations of the four conductivity values: With isotropic tissue, excitation spread in circles, as expected. With tissue having nominally normal ventricular conductivities, excitation spread in patterns close to ellipses. With reciprocal conductivities, isochrones approximated a diamond shape, and were in conflict with the theoretical predictions of Muler and Markin; the time constant of the foot of the action potentials, as computed, varied between sites along axes as compared with sites along the diagonals, even though membrane properties were identical everywhere. Velocity of propagation changed for several milliseconds following the stimulus. Patterns that would have been expected from well-known studies in one dimension did not always occur in two dimensions, with the magnitude of the difference varying from nil for isotropic conductivities to quite large for reciprocal conductivities.
本文报道了对各向异性二维心脏组织传播的模拟。假设的组织结构是由霍奇金-赫胥黎膜分隔内外各向异性介质,且在每种情况下都遵循欧姆定律。膜电流通过一个积分表达式得出,该表达式涉及由距离函数加权的Vm的部分空间导数。使用一种算法计算了在单个中心部位激发后跨膜电压随时间变化的数值解,该算法仅检查每个时刻正在经历激发的组织部分;从而,所需的计算量减少到一个很大但可实现的数量。给出了四种电导率值的几种组合的结果:对于各向同性组织,激发如预期那样呈圆形传播。对于具有标称正常心室电导率的组织,激发以接近椭圆形的模式传播。对于互易电导率,等时线近似为菱形,这与穆勒和马尔金的理论预测相矛盾;计算得出的动作电位波峰的时间常数,与沿对角线的部位相比,沿轴的部位之间存在差异,尽管膜特性在各处都是相同的。刺激后传播速度在几毫秒内发生变化。在一维中著名研究中预期的模式在二维中并不总是出现,差异的大小从各向同性电导率时的零到互易电导率时的相当大不等。