Vassalle M, Yu H, Cohen I S
Department of Physiology and Biophysics, State University of New York, Stony Brook 11794, USA.
J Gen Physiol. 1995 Sep;106(3):559-78. doi: 10.1085/jgp.106.3.559.
It is generally assumed that in cardiac Purkinje fibers the hyperpolarization activated inward current i(f) underlies the pacemaker potential. Because some findings are at odds with this interpretation, we used the whole cell patch clamp method to study the currents in the voltage range of diastolic depolarization in single canine Purkinje myocytes, a preparation where many confounding limitations can be avoided. In Tyrode solution ([K+]o = 5.4 mM), hyperpolarizing steps from Vh = -50 mV resulted in a time-dependent inwardly increasing current in the voltage range of diastolic depolarization. This time-dependent current (iKdd) appeared around -60 mV and reversed near EK. Small superimposed hyperpolarizing steps (5 mV) applied during the voltage clamp step showed that the slope conductance decreases during the development of this time-dependent current. Decreasing [K+]o from 5.4 to 2.7 mM shifted the reversal potential to a more negative value, near the corresponding EK. Increasing [K+]o to 10.8 mM almost abolished iKdd. Cs+ (2 mM) markedly reduced or blocked the time-dependent current at potentials positive and negative to EK. Ba2+ (4 mM) abolished the time-dependent current in its usual range of potentials and unmasked another time-dependent current (presumably i(f)) with a threshold of approximately -90 mV (> 20 mV negative to that of the time-dependent current in Tyrode solution). During more negative steps, i(f) increased in size and did not reverse. During i(f) the slope conductance measured with small (8-10 mV) superimposed clamp steps increased. High [K+]o (10.8 mM) markedly increased and Cs+ (2 mM) blocked i(f). We conclude that: (a) in the absence of Ba2+, a time-dependent current does reverse near EK and its reversal is unrelated to K+ depletion; (b) the slope conductance of that time-dependent current decreases in the absence of K+ depletion at potentials positive to EK where inactivation of iK1 is unlikely to occur. (c) Ba2+ blocks this time-dependent current and unmasks another time-dependent current (i(f)) with a more negative (> 20 mV) threshold and no reversal at more negative values; (d) Cs+ blocks both time-dependent currents recorded in the absence and presence of Ba2+. The data suggest that in the diastolic range of potentials in Purkinje myocytes there is a voltage- and time-dependent K+ current (iKdd) that can be separated from the hyperpolarization-activated inward current i(f).
一般认为,在心脏浦肯野纤维中,超极化激活内向电流i(f)是起搏电位的基础。由于一些研究结果与这一解释不一致,我们采用全细胞膜片钳方法研究单个犬浦肯野心肌细胞舒张期去极化电压范围内的电流,该标本可避免许多混淆因素的限制。在台氏液([K+]o = 5.4 mM)中,从Vh = -50 mV开始的超极化步骤在舒张期去极化电压范围内导致一个随时间增加的内向电流。这个随时间变化的电流(iKdd)在约-60 mV时出现,并在EK附近反转。在电压钳制步骤中施加的小的叠加超极化步骤(5 mV)表明,在这个随时间变化的电流发展过程中斜率电导降低。将[K+]o从5.4 mM降至2.7 mM使反转电位向更负值移动,接近相应的EK。将[K+]o增加到10.8 mM几乎消除了iKdd。Cs+(2 mM)在EK正电位和负电位时均显著降低或阻断了随时间变化的电流。Ba2+(4 mM)在其通常的电位范围内消除了随时间变化的电流,并揭示了另一个随时间变化的电流(可能是i(f)),其阈值约为-90 mV(比台氏液中随时间变化的电流阈值负> 20 mV)。在更负的步骤中,i(f)大小增加且不反转。在i(f)期间,用小的(8 - 10 mV)叠加钳制步骤测量的斜率电导增加。高[K+]o(10.8 mM)显著增加i(f),而Cs+(2 mM)阻断i(f)。我们得出以下结论:(a) 在没有Ba2+时,一个随时间变化的电流确实在EK附近反转,且其反转与K+耗竭无关;(b) 在不存在K+耗竭且iK1不太可能失活的EK正电位时,该随时间变化电流的斜率电导降低;(c) Ba2+阻断这个随时间变化的电流,并揭示另一个阈值更负(> 20 mV)且在更负电位时不反转的随时间变化电流(i(f));(d) Cs+阻断在没有和存在Ba2+时记录到的两种随时间变化的电流。数据表明,在浦肯野心肌细胞舒张期电位范围内存在一种电压和时间依赖性K+电流(iKdd),它可以与超极化激活内向电流i(f)区分开来。