Pennefather P S, Zhou W, DeCoursey T E
Faculty of Pharmacy, University of Toronto, Toronto, Ontario M5S 2S2, Canada.
J Gen Physiol. 1998 Jun;111(6):795-805. doi: 10.1085/jgp.111.6.795.
A simple kinetic model is presented to explain the gating of a HERG-like voltage-gated K+ conductance described in the accompanying paper (Zhou, W., F.S. Cayabyab, P.S. Pennefather, L.C. Schlichter, and T.E. DeCoursey. 1998. J. Gen. Physiol. 111:781-794). The model proposes two kinetically distinct closing pathways, a rapid one favored by depolarization (deactivation) and a slow one favored by hyperpolarization (inactivation). The overlap of these two processes leads to a window current between -50 and +20 mV with a peak at -36 mV of approximately 12% maximal conductance. The near absence of depolarization-activated outward current in microglia, compared with HERG channels expressed in oocytes or cardiac myocytes, can be explained if activation is shifted negatively in microglia. As seen with experimental data, availability predicted by the model was more steeply voltage dependent, and the midpoint more positive when determined by making the holding potential progressively more positive at intervals of 20 s (starting at -120 mV), rather than progressively more negative (starting at 40 mV). In the model, this hysteresis was generated by postulating slow and ultra-slow components of inactivation. The ultra-slow component takes minutes to equilibrate at -40 mV but is steeply voltage dependent, leading to protocol-dependent modulation of the HERG-like current. The data suggest that "deactivation" and "inactivation" are coupled through the open state. This is particularly evident in isotonic Cs+, where a delayed and transient outward current develops on depolarization with a decay time constant more voltage dependent and slower than the deactivation process observed at the same potential after a brief hyperpolarization.
本文提出了一个简单的动力学模型,以解释随附论文(Zhou, W., F.S. Cayabyab, P.S. Pennefather, L.C. Schlichter, and T.E. DeCoursey. 1998. J. Gen. Physiol. 111:781 - 794)中描述的类HERG电压门控钾离子电导的门控机制。该模型提出了两条动力学上不同的关闭途径,一条快速途径受去极化(失活)促进,另一条缓慢途径受超极化(失活)促进。这两个过程的重叠导致了在 -50 至 +20 mV 之间出现一个窗电流,其峰值在 -36 mV 处,约为最大电导的 12%。与卵母细胞或心肌细胞中表达的HERG通道相比,小胶质细胞中几乎不存在去极化激活的外向电流,如果小胶质细胞中的激活在负向发生偏移,这一点就可以得到解释。正如实验数据所示,当以 20 秒的间隔逐渐使钳制电位更正(从 -120 mV 开始)而不是逐渐更负(从 40 mV 开始)来确定时,模型预测的可用性对电压的依赖性更强,且中点更正。在该模型中,这种滞后现象是通过假设失活的缓慢和超慢成分产生的。超慢成分在 -40 mV 时需要数分钟才能达到平衡,但对电压的依赖性很强,导致类HERG电流出现依赖于实验方案的调制。数据表明,“失活”和“失活”是通过开放状态耦合的。这在等渗 Cs⁺ 中尤为明显,在去极化时会出现延迟且短暂的外向电流,其衰减时间常数比在短暂超极化后在相同电位下观察到的失活过程对电压的依赖性更强且更慢。