Palti Y, Ganot G, Stämpfli R
Biophys J. 1976 Mar;16(3):261-73. doi: 10.1016/S0006-3495(76)85686-X.
The kinetics of potassium conductance changes were determined in the voltage clamped frog node (Rana esculenta), as a function of conditioning prepotential. The conditioning potential duration varied from 1 to 50 ms and the amplitude between -60 and +130 mV (relative to rest). The conductance kinetics were determined at a single test potential of +20 mV (depolarization) by means of the slope of log [ninfinity - nt] vs. time relationship which defines the time constant of the process (tau). The values of tau, after conditioning hyperpolarizations, were around 5 ms, up to 10 times greater than values obtained following a strong depolarization. The tau vs. pre-potential curve was sigmoid in shape. These differences were only slightly dependent on [K+]0 or conditioning pulse duration. The steady-state current values were also found to be a function of conditioning potential. After conditioning hyperpolarizations, the log [ninfinity - nt] vs. time curve could not be fitted by a single exponent regardless of the power of n chosen. The prepotential dependency of potassium current kinetics is inconsistent with the Hodgkin-Huxley axon model where the conductance parameters are assumed to be in either one of two possible states, and where the rate of transfer from one state to the other follows first order kinetics. In contrast the described kinetics may be consistent with complex multistate potassium "channel" models or membranes consisting of a number of types of channels.
在电压钳制的食用蛙(Rana esculenta)神经节中,测定了钾离子电导变化的动力学,作为预处理电位的函数。预处理电位的持续时间在1至50毫秒之间变化,幅度在-60至+130毫伏之间(相对于静息电位)。通过log [∞ - nt]与时间关系的斜率来确定在+20毫伏(去极化)的单一测试电位下的电导动力学,该斜率定义了该过程的时间常数(τ)。预处理超极化后,τ值约为5毫秒,比强去极化后获得的值大10倍。τ与预处理电位的曲线呈S形。这些差异仅略微依赖于[K+]0或预处理脉冲持续时间。稳态电流值也被发现是预处理电位的函数。预处理超极化后,无论选择n的幂次如何,log [∞ - nt]与时间曲线都不能用单一指数拟合。钾离子电流动力学对预处理电位的依赖性与霍奇金-赫胥黎轴突模型不一致,在该模型中,电导参数被假定处于两种可能状态之一,并且从一种状态转移到另一种状态的速率遵循一级动力学。相比之下,所描述的动力学可能与复杂的多状态钾“通道”模型或由多种类型通道组成的膜一致。