游离心肌细胞晚钠通道爆发型开放模式的电位依赖性

应用膜片箝技术记录豚鼠游离心室肌细胞钠通道电流,发现除极可引起晚钠电流爆发型开放,而复极可终止爆发型活动。爆发型模式的通道电流不仅有浓度依赖性和电位依赖性,其开放时间常数也随箝制电位变正而增大。多步阶梯式除极和斜线除极的实验结果首次表明电位变化愈迅速、除极步数愈多,爆发型出现的机率也就愈高。     

海葵毒素对心肌钠通道开放模式、动作电位及心电图QT间期的影响

应用膜片箝技术记录游离豚鼠心肌细胞钠通道电流, 细胞内微电极技术记录心室乳头肌的动作电位和心电图机记录豚鼠的心电图。使用与心肌细胞钠通道有高度亲和力的海葵毒素(sea anemone toxin, ATXⅡ)改变钠通道开放的动力过程, 从三个水平来研究钠通道、动作电位、心电图变化的关系, 并试图探讨长QT综合征(long QT syndrome, LQTs)的发病机制。结果显示: ATXⅡ使钠通道的开放频率增加, 钠通道中“长时间开放模式”的开放时间常数增大, 动作电位的持续时间APD50和APD90也分别增加了23%和27%。 ATXⅡ使动物心电图QT间期延长18.6%, QTc (校正的QT间期)增大18.9%。这些结果提示, 钠通道动力过程的变化对动作电位和心电图QT间期有重要影响, 钠通道功能或结构的变异可能是临床上部分长QT综合征产生的原因。     

海葵毒素对心肌钠通道开放模式，动作电位及心电图QT周期的影响

应用膜片箝技术记录游离豚鼠心肌细胞的钠通道电流,细胞内微电极技术记录心室乳头肌的动作电位和心电图机记录豚鼠的心电图,使用与心肌;细胞钠通道有高度亲和力的海葵毒素（sea anemone toxin,ATXⅡ）改变钠通道开放的动力过程,从三个水平来研究钠通道,动作电位,心电图变化的关系,并试图探讨长QT综合征（long QT syndrome,LQTs)的发病机制,结果显示,ATXⅡ使钠通道的开放频率增加,钠通道中“长时间开放模式”的开放时间常数增大,动人电位的持续时间APD50和APD50也分别增加了23％和27％,ATXⅡ使动物心电图QT间期延长18．6％,QTc(校正的QT间期）增大18．9％,这些结果提示,钠通道动力过程的变化对动作电位和心电图QT间期有重要影响,钠通道功能或结构的变异可能是临床上部分长QT综合征产生的原因。     

晚钠电流在获得性心血管病合并心律失常发生中的作用及其意义

心肌细胞的晚钠电流出现于动作电位的复极期,正常心肌细胞存在内源性晚钠电流,幅度小;晚钠电流幅度增大可见于长QT综合征3、4、9、10和12型,也见于多种病理及药物作用下,导致动作电位时程延长,诱发恶性室性心律失常,如尖端扭转型室性心动过速等;同时由于平台期延长,钙离子内流时间延长,改变心肌收缩力并参与钙相关心律失常的发生。近年来,随着对心血管疾病及其合并心律失常发病机制的深入认识,发现越来越多的获得性心血管疾病患者心律失常的发生与晚钠电流异常增大相关,极大地扩大了晚钠电流相关心律失常的范畴,选择性晚钠电流抑制剂已成为抗心律失常药物新的亚类。     

乌拉坦对大鼠海马CA1神经元电压门控钠通道和动作电位的作用

乌拉坦对兴奋性和抑制性配体门控通道具有广泛的可检测的作用.作者运用全细胞膜片钳技术研究乌拉坦对wistar大鼠海马CA1神经元电压门控钠通道和动作电位的作用.结果发现乌拉坦可逆并剂量依赖性地抑制钠电流和动作电位,其中,在10mmol/L浓度时可减小钠电流强度达38%,使激活曲线向去极化方向移动,并延长钠通道失活后的恢复时间,降低动作电位的幅值.这些结果表明乌拉坦对电压门控钠通道的抑制作用可能是乌拉坦全身麻醉作用的机制之一.     

白介素1β对大鼠皮层神经元钠电流的急性作用

白介素1β(Interleukin-1β,IL-1β)是重要的促炎细胞因子,在多种中枢神经系统的损伤和疾病过程中发挥关键作用。电压门控的钠通道是神经元中最重要的离子通道之一,是产生再生性动作电位的基础,决定了神经元的兴奋性等电学性质,也与多种中枢疾病过程相关。然而,现在还没有直接关于IL-1β与中枢钠通道的相互关系的研究。在该研究中,使用全细胞膜片钳记录测定了IL-1β对培养的皮层神经元钠电流的急性作用,并分析了由此对动作电位的影响。结果显示,IL-1β对钠电流幅度只有较小的抑制,而显著降低钠通道的半激活电压,不改变激活的斜率因子和失活性质,这个作用引起动作电位阈值显著降低。这些结果提示在损伤和疾病过程中,快速释放的IL-1β可能会增加神经元兴奋性,从而恶化神经损伤过程。     

脊神经损伤后钠电流的变化及其离子通道机制

目的:检测脊神经切断大鼠背根节(DRG)神经元重复放电能力和钠电流的变化,并研究介导其电流变化的钠通道亚型的表达情况。方法:脊神经切断术后2～8d慢性痛大鼠模型背根节急性分离,对中等直径DRG神经元运用全细胞膜片钳技术记录神经元放电和钠电流的变化。对背根节神经元进行RT-PCR检测,分析其钠通道亚型的表达情况。结果:电流钳下,实验组DRG神经元在电流刺激下产生重复放电,而对照组神经元多诱发单个动作电位,电压钳记录发现实验组背根节神经元快钠电流和持续性钠电流幅值均明显大于对照组,PCR结果显示,Nav1.3、Nav1.7和Nav1.8通道亚型mRNA表达显著增高。结论:钠通道介导了脊神经受损模型的DRG神经元兴奋性增高,持续性钠电流可能通过调节阈下膜电位振荡的产生调节神经元兴奋性。     

脊神经损伤后钠电流的变化及其离子通道机制

目的：检测脊神经切断大鼠背根节（DRG）神经元重复放电能力和钠电流的变化,并研究介导其电流变化的钠通道亚型的表达情况。方法：脊神经切断术后2～8d慢性痛大鼠模型背根节急性分离,对中等直径DRG神经元运用全细胞膜片钳技术记录神经元放电和钠电流的变化。对背根节神经元进行RT-PCR检测,分析其钠通道亚型的表达情况。结果：电流钳下,实验组DRG神经元在电流刺激下产生重复放电,而对照组神经元多诱发单个动作电位,电压钳记录发现实验组背根节神经元快钠电流和持续性钠电流幅值均明显大于对照组,PCR结果显示,Nav1.3、Nav1.7和Nav1.8通道亚型mRNA表达显著增高。结论：钠通道介导了脊神经受损模型的DRG神经元兴奋性增高,持续性钠电流可能通过调节阈下膜电位振荡的产生调节神经元兴奋性。     

培养的新生大鼠交感神经元膜电学性质及电压门控通道的膜片箝研究

在培养的新生大鼠颈上神经节交感神经元标本上,用全细胞电流箝及电压箝技术观察记录了交感神经元膜电学参数及电压门控性通道电流。用全细胞电流箝测得下列平均值：静息电位,－５１±６ｍＶ;输入阻抗,１４３２±３８９ＭΩ;时间常数,１３０±３２ｍｓ;动作电位幅度,９６±１０ｍＶ,超射值,４２±６ｍＶ。培养早期即可记录到自发或诱发的动作电位,大多数动作电位后跟随快或慢的后超极化电位。在电压箝状态下可分别记录到电压门控钠、钾、钙通道电流。钾电流以延迟整流型为主,钙电流只有高电压激活,缓慢失活的Ｌ或Ｎ型,未能记录到低电压激活,快速失活的Ｔ型钙电流。     

白介素1β抑制培养的大鼠皮层神经元钠电流峰值和动作电位幅度

白介素1β(interleukin-1β,IL-1β)是重要的促炎细胞因子,在中枢神经系统的生理学和病理学过程中发挥关键作用。电压门控钠通道是可兴奋细胞电学活动的基础,控制神经元的兴奋性和动作电位。最近的研究又显示了IL-1β与电压门控通道之间的相互作用。为考察中枢神经元中IL-1β与电压门控钠通道之间的相互作用,本研究使用10ng/mL的IL-1β处理培养的大鼠皮层神经元24h,通过电压钳技术测定电压门控钠电流,结果表明IL-1β处理抑制钠电流幅度,但不改变其激活和失活性质。与电压钳记录结果相一致,电流钳记录表明IL-1β降低动作电位幅度但不影响阈值。这些结果显示长时间的IL-1β处理可以抑制电压门控钠电流,这种抑制作用减小了动作电位幅度,这可能改变神经元的电学性质、突触传导等基本功能,并提示了IL-1β在神经系统损伤和疾病中作用的新的思路。     

Two modes of gating during late Na+ channel currents in frog sartorius muscle

Na+ currents were measured during 0.4-s depolarizing pulses using the cell-attached variation of the patch-clamp technique. Patches on Cs-dialyzed segments of sartorius muscle of Rana pipiens contained an estimated 25-500 Na+ channels. Three distinct types of current were observed after the pulse onset: a large initial surge of inward current that decayed within 10 ms (early currents), a steady "drizzle" of isolated, brief, inward unitary currents (background currents), and occasional "cloudbursts" of tens to hundreds of sequential unitary inward currents (bursts). Average late currents (background plus bursts) were 0.12% of peak early current amplitude at -20 mV. 85% of the late currents were carried by bursting channels. The unit current amplitude was the same for all three types of current, with a conductance of 10.5 pS and a reversal potential of +74 mV. The magnitudes of the three current components were correlated from patch to patch, and all were eliminated by slow inactivation. We conclude that all three components were due to Na+ channel activity. The mean open time of the background currents was approximately 0.25 ms, and the channels averaged 1.2 openings for each event. Neither the open time nor the number of openings of background currents was strongly sensitive to membrane potential. We estimated that background openings occurred at a rate of 0.25 Hz for each channel. Bursts occurred once each 2,000 pulses for each channel (assuming identical channels). The open time during bursts increased with depolarization to 1-2 ms at -20 mV, whereas the closed time decreased to less than 20 ms. The fractional open time during bursts was fitted with m infinity 3 using standard Na+ channel models. We conclude that background currents are caused by a return of normal Na+ channels from inactivation, while bursts are instances where the channel's inactivation gate spontaneously loses its function for prolonged periods.     

迷走神经对家兔在体心脏心室肌细胞跨膜电位的影响

本研究观察了电刺激迷走神经对家兔在体心脏心室肌细胞跨膜电位的作用及钾通道阻滞剂氯化四乙基铵对这一作用的影响。结果表明,在自然心率条件下,迷走神经刺激可使静息电位(RP)、动作电位振幅(APA)和0相最大上升速率(dv/dt)_(max)增加,动作电位时程(APD)缩短。冠脉注射氯化四乙基铵使心室肌细胞复极过程明显延长,迷走神经刺激不再引起 RP、APA 增大,动作电位时程不再缩短,(dv/dt)_(max)反而减小。这些结果提示,迷走神经刺激对正常心室肌细胞跨膜电位的影响可能是通过外向 K~ 流增加引起的。     

A study of the molecular sources of nonideal osmotic pressure of bovine serum albumin solutions as a function of pH.

Two types of the late Na channels, burst and background, were studied in Purkinje and ventricular cells. In the whole-cell configuration, steady-state Na currents were recorded at potentials (-70 to -80 mV) close to the normal cell resting potential. The question of the contribution of late Na channels to this background Na conductance was investigated. During depolarization, burst Na channels were active for periods (up to approximately 5 s), which exceeded the action potential duration. However, they eventually closed without reopening, indicating the presence of slow and complete inactivation. When, at the moment of burst channel opening, the potential was switched to -80 mV, the channel closed quickly without reopening. We conclude that the burst Na channels cannot contribute significantly to the background Na conductance. Background Na channels undergo incomplete inactivation. After a step depolarization, their activity decreased in time, approaching a steady-state level. Background Na channel openings could be recorded at constant potentials in the range from -120 to 0 mV. After step depolarizations to potentials near -70 mV and more negative, a significant fraction of Na current was carried by the background Na channels. Analysis of the background channel behavior revealed that their gating properties are qualitatively different from those of the early Na channels. We suggest that background Na channels represent a special type of Na channel that can play an important role in the initiation of cardiac action potential and in the TTX-sensitive background Na conductance.     

Simulation of the undiseased human cardiac ventricular action potential: model formulation and experimental validation

Cellular electrophysiology experiments, important for understanding cardiac arrhythmia mechanisms, are usually performed with channels expressed in non myocytes, or with non-human myocytes. Differences between cell types and species affect results. Thus, an accurate model for the undiseased human ventricular action potential (AP) which reproduces a broad range of physiological behaviors is needed. Such a model requires extensive experimental data, but essential elements have been unavailable. Here, we develop a human ventricular AP model using new undiseased human ventricular data: Ca(2+) versus voltage dependent inactivation of L-type Ca(2+) current (I(CaL)); kinetics for the transient outward, rapid delayed rectifier (I(Kr)), Na(+)/Ca(2+) exchange (I(NaCa)), and inward rectifier currents; AP recordings at all physiological cycle lengths; and rate dependence and restitution of AP duration (APD) with and without a variety of specific channel blockers. Simulated APs reproduced the experimental AP morphology, APD rate dependence, and restitution. Using undiseased human mRNA and protein data, models for different transmural cell types were developed. Experiments for rate dependence of Ca(2+) (including peak and decay) and intracellular sodium ([Na(+)](i)) in undiseased human myocytes were quantitatively reproduced by the model. Early afterdepolarizations were induced by I(Kr) block during slow pacing, and AP and Ca(2+) alternans appeared at rates >200 bpm, as observed in the nonfailing human ventricle. Ca(2+)/calmodulin-dependent protein kinase II (CaMK) modulated rate dependence of Ca(2+) cycling. I(NaCa) linked Ca(2+) alternation to AP alternans. CaMK suppression or SERCA upregulation eliminated alternans. Steady state APD rate dependence was caused primarily by changes in [Na(+)](i), via its modulation of the electrogenic Na(+)/K(+) ATPase current. At fast pacing rates, late Na(+) current and I(CaL) were also contributors. APD shortening during restitution was primarily dependent on reduced late Na(+) and I(CaL) currents due to inactivation at short diastolic intervals, with additional contribution from elevated I(Kr) due to incomplete deactivation.     

Effects of Na(+) channel and cell coupling abnormalities on vulnerability to reentry: a simulation study

The role of dynamic instabilities in the initiation of reentry in diseased (remodeled) hearts remains poorly explored. Using computer simulations, we studied the effects of altered Na(+) channel and cell coupling properties on the vulnerable window (VW) for reentry in simulated two-dimensional cardiac tissue with and without dynamic instabilities. We related the VW for reentry to effects on conduction velocity, action potential duration (APD), effective refractory period dispersion and restitution, and concordant and discordant APD alternans. We found the following: 1). reduced Na(+) current density and slowed recovery promoted postrepolarization refractoriness and enhanced concordant and discordant APD alternans, which increased the VW for reentry; 2). uniformly reduced cell coupling had little effect on cellular electrophysiological properties and the VW for reentry. However, randomly reduced cell coupling combined with decoupling promoted APD dispersion and alternans, which also increased the VW for reentry; 3). the combination of decreased Na(+) channel conductance, slowed Na(+) channel recovery, and cellular uncoupling synergistically increased the VW for reentry; and 4) the VW for reentry was greater when APD restitution slope was steep than when it was flat. In summary, altered Na(+) channel and cellular coupling properties increase vulnerability to reentrant arrhythmias. In remodeled hearts with altered Na(+) channel properties and cellular uncoupling, dynamic instabilities arising from electrical restitution exert important influences on the VW for reentry.     

Action potential characterization in intact mouse heart: steady-state cycle length dependence and electrical restitution

Transgenic mice have been increasingly utilized to investigate the molecular mechanisms of cardiac arrhythmias, yet the rate dependence of the murine action potential duration and the electrical restitution curve (ERC) remain undefined. In the present study, 21 isolated, Langendorff-perfused, and atrioventricular node-ablated mouse hearts were studied. Left ventricular and left atrial action potentials were recorded using a validated miniaturized monophasic action potential probe. Murine action potentials (AP) were measured at 30, 50, 70, and 90% repolarization (APD(30)-APD(90)) during steady-state pacing and varied coupling intervals to determine ERCs. Murine APD showed rate adaptation as well as restitution properties. The ERC time course differed dramatically between early and late repolarization: APD(30) shortened with increasing S1-S2 intervals, whereas APD(90) was prolonged. When fitted with a monoexponential function, APD(30) reached plateau values significantly faster than APD(90) (tau = 29 +/- 2 vs. 78 +/- 6 ms, P < 0.01, n = 12). The slope of early APD(90) restitution was significantly <1 (0.16 +/- 0.02). Atrial myocardium had shorter final repolarization and significantly faster ERCs that were shifted leftward compared with ventricular myocardium. Recovery kinetics of intracellular Ca(2+) transients recorded from isolated ventricular myocytes at 37 degrees C (tau = 93 +/- 4 ms, n = 18) resembled the APD(90) ERC kinetics. We conclude that mouse myocardium shows AP cycle length dependence and electrical restitution properties that are surprisingly similar to those of larger mammals and humans.     

A novel LQT-3 mutation disrupts an inactivation gate complex with distinct rate-dependent phenotypic consequences

Inherited mutations of SCN5A, the gene that encodes Na(V)1.5, the alpha subunit of the principle voltage-gated Na(+) channel in the heart, cause congenital Long QT Syndrome variant 3 (LQT-3) by perturbation of channel inactivation. LQT-3 mutations induce small, but aberrant, inward current that prolongs the ventricular action potential and subjects mutation carriers to arrhythmia risk dictated in part by the biophysical consequences of the mutations. Most previously investigated LQT-3 mutations are associated with increased arrhythmia risk during rest or sleep. Here we report a novel LQT-3 mutation discovered in a pediatric proband diagnosed with LQTS but who experienced cardiac events during periods of mild exercise as well as rest. The mutation, which changes a single amino acid (S1904L) in the Na(V)1.5 carboxy terminal domain, disrupts the channel inactivation gate complex and promotes late Na(+) channel currents, not by promoting a bursting mode of gating, but by increasing the propensity of the channel to reopen during prolonged depolarization. Incorporating a modified version of the Markov model of the Na(V)1.5 channel into a mathematical model of the human ventricular action potential predicts that the biophysical consequences of the S1904L mutation result in action potential prolongation that is seen for all heart rates but, in contrast to other previously-investigated LQT-3 mutant channels, is most pronounced at fast rates resulting in a drastic reduction in the cells ability to adapt APD to heart rate.     

Modulation of single cardiac sodium channels by DPI 201-106

Single sodium channel currents were analysed in cell attached patches from single ventricular cells of guinea pig hearts in the presence of a novel cardiotonic compound DPI 201-106. The mean single channel conductance of DPI-treated Na channels was not changed by DPI (20.8 +/- 4 pS, control, 3 patches; 21.3 +/- 1 pS with DPI, 5 mumol/1,3 patches). DPI voltage-dependently prolongs the cardiac sodium channel openings by removal of inactivation at potentials positive to -40 mV. At potentials negative to -40 mV a clustering of short openings at the very beginning of the depolarizing voltage steps can be observed causing a transient time course of the averaged currents. Long openings induced an extremely slow inactivation. Short openings, long openings and nulls appeared in groups referring to a modal gating behaviour of DPI-treated sodium channels. DPI-modified Na channels showed a monotonously prolonged mean open time with increased depolarizing voltage steps, e.g. the open state probability within a sweep was increased. However, the number of non-empty sweeps was decreased with the magnitude of the depolarizing steps, e.g. the probability of the channel being open as calculated from the averaged currents was voltage-dependently decreased by DPI (50% decrease at -50.7 +/- 9 9 mV, 3 patches). Short and long openings of DPI-modified channels could be separated by variation of the holding potential. The occurrence of long Na channel openings was much more suppressed by reducing the holding potential (half maximum inactivation at -112 +/- 8 mV, 4 patches) than that of short openings (half maximum inactivation at -88 +/- 8 mV, 4 patches). Otherwise, short living openings completely disappeared at potentials positive to -40 mV where the occurrence of long openings was favoured. The differential voltage dependence of blocking and activating effects of DPI on cardiac Na channels as well as the differential voltage dependence of the appearance of short and long openings refers to a modal gating behaviour of cardiac Na channels.