Alicata D A, Rayner M D, Starkus J G
Békésy Laboratory of Neurobiology, Pacific Biomedical Research Center, Honolulu, Hawaii.
Biophys J. 1990 Apr;57(4):745-58. doi: 10.1016/S0006-3495(90)82595-9.
Schauf and Bullock (1979. Biophys. J. 27:193-208; 1982. Biophys. J. 37:441-452), using Myxicola giant axons, demonstrated that solvent substitution with deuterium oxide (D2O) significantly affects both sodium channel activation and inactivation kinetics without corresponding changes in gating current or tail current rates. They concluded that (a) no significant component of gating current derives from the final channel opening step, and (b) channels must deactivate (during tail currents) by a different pathway from that used in channel opening. By contrast, Oxford (1981. J. Gen. Physiol. 77:1-22) found in squid axons that when a depolarizing pulse is interrupted by a brief (approximately 100 microseconds) return to holding potential, subsequent reactivation (secondary activation) is very rapid and shows almost monoexponential kinetics. Increasing the interpulse interval resulted in secondary activation rate returning towards control, sigmoid (primary activation) kinetics. He concluded that channels open and close (deactivate) via the same pathway. We have repeated both sets of observations in crayfish axons, confirming the results obtained in both previous studies, despite the apparently contradictory conclusions reached by these authors. On the other hand, we find that secondary activation after a brief interpulse interval (50 microseconds) is insensitive to D2O, although reactivation after longer interpulse intervals (approximately 400 microseconds) returns towards a D2O sensitivity similar to that of primary activation. We conclude that D2O-sensitive primary activation and D2O-insensitive tail current deactivation involve separate pathways. However, D2O-insensitive secondary activation involves reversal of the D2O-insensitive deactivation step. These conclusions are consistent with "parallel gate" models, provided that one gating particle has a substantially reduced effective valence.
绍夫和布洛克(1979年,《生物物理杂志》27卷:193 - 208页;1982年,《生物物理杂志》37卷:441 - 452页)利用黏液虫巨轴突证明,用重水(D₂O)进行溶剂置换会显著影响钠通道的激活和失活动力学,而门控电流或尾电流速率没有相应变化。他们得出结论:(a)门控电流的任何显著成分都并非来自通道最终打开步骤;(b)通道在尾电流期间失活的途径必定与通道打开时所采用的途径不同。相比之下,牛津(1981年,《普通生理学杂志》77卷:1 - 22页)在鱿鱼轴突中发现,当一个去极化脉冲被短暂(约100微秒)回到保持电位打断时,随后的再激活(二次激活)非常迅速,并且几乎呈现单指数动力学。增加脉冲间隔会导致二次激活速率恢复到对照的S形(一次激活)动力学。他得出结论:通道通过相同途径打开和关闭(失活)。我们在小龙虾轴突中重复了这两组观察结果,证实了先前两项研究所得出的结果,尽管这些作者得出了明显相互矛盾的结论。另一方面,我们发现短暂脉冲间隔(50微秒)后的二次激活对D₂O不敏感,尽管较长脉冲间隔(约400微秒)后的再激活恢复到类似于一次激活的D₂O敏感性。我们得出结论:对D₂O敏感的一次激活和对D₂O不敏感的尾电流失活涉及不同途径。然而,对D₂O不敏感的二次激活涉及对D₂O不敏感的失活步骤的逆转。这些结论与“平行门”模型一致,前提是一个门控粒子的有效价大幅降低。