Gilliam F R, Starmer C F, Grant A O
Department of Medicine, Duke University Medical Center, Durham, North Carolina 27710.
Circ Res. 1989 Sep;65(3):723-39. doi: 10.1161/01.res.65.3.723.
Lidocaine block of the cardiac sodium channel is believed to be primarily a function of channel state. For subthreshold potentials, block is limited to the inactivated state, whereas above threshold, block results from the combination of open- and inactivated-state block. Since, in the absence of drug, inactivation develops with time constants that vary from several hundred milliseconds to a few milliseconds as potential is varied from subthreshold to strongly depolarized levels, we would predict a similar voltage dependence of at least a fraction of block. Prior theoretical analyses from our laboratory suggest that there should be a direct parallel between blockade determined with a single pulse and trains of pulses. We tested these predictions by measuring the blockade of sodium current in cultured atrial myocytes during exposure to 80 microM lidocaine. We selected two test potentials for most of our studies, -80 mV, which was clearly in the subthreshold range of potentials, and -20 mV, which was close to the peak of the current-voltage curve. With single pulses of increasing duration, block developed with a single exponential time course and with time constants that decreased from 694 +/- 117 msec at -80 mV to 373 +/- 54 msec at -20 mV. In the absence of drug, inactivation developed with a time constant 176 +/- 17 at -80 mV and 2.9 +/- .5 msec at -20 mV. Despite the much slower onset of inactivation at -80 mV, no second-order delay in block development was observed. This suggests that at -80 mV block is occurring to a channel conformation that is accessed without delay rather than the classical inactivated state. We compared the kinetics of block during a single continuous pulse with trains of pulses at -20 mV. The rate of block onset was faster during the pulse trains, suggesting an element of "activated state" block. We computed shifts in apparent inactivation from observed steady-state blockade. The computed shifts agree well with those observed, indicating that shifts in apparent inactivation result largely from voltage-sensitive equilibrium blockade. The classical states described in the Hodgkin-Huxley formalism may be too restrictive to fully describe the voltage- and time-dependent block of cardiac sodium channels.
利多卡因对心脏钠通道的阻滞作用被认为主要取决于通道状态。对于阈下电位,阻滞作用仅限于失活状态,而在阈上电位时,阻滞作用则是由开放状态和失活状态阻滞的共同作用导致的。由于在无药物的情况下,随着电位从阈下变化到强去极化水平,失活以时间常数发展,时间常数从几百毫秒到几毫秒不等,因此我们可以预测至少一部分阻滞作用会有类似的电压依赖性。我们实验室之前的理论分析表明,单脉冲和脉冲序列所确定的阻滞作用之间应该存在直接的平行关系。我们通过测量培养的心房肌细胞在暴露于80微摩尔利多卡因期间钠电流的阻滞情况来检验这些预测。在大多数研究中,我们选择了两个测试电位,-80毫伏,该电位明显处于阈下电位范围,以及-20毫伏,该电位接近电流-电压曲线的峰值。随着单脉冲持续时间的增加,阻滞作用以单指数时间进程发展,时间常数从-80毫伏时的694±117毫秒降至-20毫伏时的373±54毫秒。在无药物的情况下,失活的时间常数在-80毫伏时为176±17毫秒,在-20毫伏时为2.9±0.5毫秒。尽管在-80毫伏时失活的起始要慢得多,但未观察到阻滞发展的二阶延迟。这表明在-80毫伏时,阻滞作用发生在一个无需延迟即可进入的通道构象上,而不是经典的失活状态。我们比较了单个连续脉冲期间的阻滞动力学与-20毫伏时的脉冲序列期间的阻滞动力学。脉冲序列期间阻滞起始的速率更快,这表明存在“激活状态”阻滞的因素。我们根据观察到的稳态阻滞计算了表观失活的偏移。计算得到的偏移与观察到的偏移非常吻合,表明表观失活的偏移主要是由电压敏感的平衡阻滞导致的。霍奇金-赫胥黎形式体系中描述的经典状态可能过于局限,无法完全描述心脏钠通道的电压和时间依赖性阻滞。