Huang C L
Physiological Laboratory, University of Cambridge, United Kingdom.
J Gen Physiol. 1996 Apr;107(4):515-34. doi: 10.1085/jgp.107.4.515.
The effects of the ryanodine receptor (RyR) antagonists ryanodine and daunorubicin on the kinetic and steady-state properties of intramembrane charge were investigated in intact voltage-clamped frog skeletal muscle fibers under conditions that minimized time-dependent ionic currents. A hypothesis that RyR gating is allosterically coupled to configurational changes in dihydropyridine receptors (DHPRs) would predict that such interactions are reciprocal and that RyR modification should influence intramembrane charge. Both agents indeed modified the time course of charging transients at 100-200-microM concentrations. They independently abolished the delayed charging phases shown by q gamma currents, even in fibers held at fully polarized, -90-mV holding potentials; such waveforms are especially prominent in extracellular solutions containing gluconate. Charge movements consistently became exponential decays to stable baselines in the absence of intervening inward or other time-dependent currents. The steady-state charge transfers nevertheless remained equal through the ON and the OFF parts of test voltage steps. The charge-voltage function, Q(VT), shifted by approximately +10 mV, particularly through those test potentials at which delayed q gamma currents normally took place but retained steepness factors (k approximately 8.0 to 10.6 mV) that indicated persistent, steeply voltage-dependent q gamma contributions. Furthermore, both RyR antagonists preserved the total charge, and its variation with holding potential, Qmax (VH), which also retained similarly high voltage sensitivities (k approximately 7.0 to 9.0 mV). RyR antagonists also preserved the separate identities of q gamma and q beta species, whether defined by their steady-state voltage dependence or inactivation or pharmacological properties. Thus, tetracaine (2 mM) reduced the available steady-state charge movement and gave shallow Q(VT) (k approximately 14 to 16 mV) and Qmax (VH) (k approximately 14 to 17 mV) curves characteristic of q beta charge. These features persisted with exposure to test agent. Finally, q gamma charge movements showed steep voltage dependences with both activation (k approximately 4.0 to 6.5 mV) and inactivation characteristics (k approximately 4.3 to 6.6 mV) distinct from those shown by the remaining q beta charge, whether isolated through differential tetracaine sensitivities, or the full approximation of charge-voltage data to the sum of two Boltzmann distributions. RyR modification thus specifically alters q gamma kinetics while preserving the separate identities of steady-state q beta and q gamma charge. These findings permit a mechanism by which transverse tubular voltage provides the primary driving force for configurational changes in DHPRs, which might produce q gamma charge movement. However, they attribute its kinetic complexities to the reciprocal allosteric coupling by which DHPR voltage sensors and RyR-Ca2+ release channels might interact even though these receptors reside in electrically distinct membranes. RyR modification then would still permit tubular voltage change to drive net q gamma charge transfer but would transform its complex waveforms into simple exponential decays.
在将时间依赖性离子电流降至最低的条件下,研究了莱克多巴胺受体(RyR)拮抗剂莱克多巴胺和柔红霉素对完整的电压钳制青蛙骨骼肌纤维膜内电荷动力学和稳态特性的影响。一种假设认为,RyR门控与二氢吡啶受体(DHPRs)的构象变化存在变构偶联,这将预测这种相互作用是相互的,并且RyR修饰应影响膜内电荷。两种药物在100 - 200微摩尔浓度下确实改变了充电瞬变的时间进程。它们独立消除了qγ电流所显示的延迟充电阶段,即使在保持在完全极化的 - 90 mV保持电位的纤维中也是如此;这种波形在含有葡萄糖酸盐的细胞外溶液中尤为突出。在没有介入内向或其他时间依赖性电流的情况下,电荷运动始终变为指数衰减至稳定基线。然而,通过测试电压阶跃的开启和关闭部分,稳态电荷转移仍然相等。电荷 - 电压函数Q(VT) 大约偏移了 +10 mV,特别是在那些通常发生延迟qγ电流的测试电位处,但保留了陡度因子(k约为8.0至10.6 mV),这表明存在持续的、强烈电压依赖性的qγ贡献。此外,两种RyR拮抗剂都保留了总电荷量及其随保持电位的变化Qmax(VH),其也保留了类似的高电压敏感性(k约为7.0至9.0 mV)。RyR拮抗剂还保留了qγ和qβ种类的各自特性,无论它们是由其稳态电压依赖性、失活还是药理学特性定义的。因此,丁卡因(2 mM)降低了可用的稳态电荷运动,并给出了浅的Q(VT)(k约为14至16 mV)和Qmax(VH)(k约为14至17 mV)曲线,这是qβ电荷的特征。这些特征在暴露于测试药物后仍然存在。最后,qγ电荷运动显示出强烈的电压依赖性,其激活(k约为4.0至6.5 mV)和失活特性(k约为4.3至6.6 mV)与其余qβ电荷所显示的不同,无论是通过丁卡因敏感性差异分离,还是将电荷 - 电压数据完全近似为两个玻尔兹曼分布的总和。因此,RyR修饰特异性地改变了qγ动力学,同时保留了稳态qβ和qγ电荷的各自特性。这些发现提出了一种机制,通过该机制横向管电压为DHPRs中的构象变化提供主要驱动力,这可能产生qγ电荷运动。然而,它们将其动力学复杂性归因于变构偶联,通过这种偶联,DHPR电压传感器和RyR - Ca2+释放通道可能相互作用,即使这些受体位于电特性不同的膜中。然后,RyR修饰仍将允许管电压变化驱动净qγ电荷转移,但会将其复杂波形转变为简单的指数衰减。