抗钠-钙交换体α-1重复序列(117-137)抗体对心肌钠-钙交换电流及钙电流的抑制作用(英文)

本研究旨在探讨抗钠-钙交换体(Na+-Ca2+ exchanger,NCX)α-1重复序列(117-137)抗体对大鼠心肌细胞钠-钙交换电流的影响。实验用合成的α-1重复序列(117-137)肽免疫大鼠制备抗α-1重复序列(117-137)抗体;应用全细胞膜片钳技术,在急性分离的心肌细胞上观察抗α-1重复序列(117-137)抗体对大鼠心肌细胞钠-钙交换电流的影响,同时还观察了其对大鼠心肌细胞L型钙通道、电压门控钠通道和豚鼠心肌延迟整流钾通道电流的影响;最后,采用EMBOSS Pairwise Alignment Algorithms软件对NCXα-1重复序列和L型钙通道(1076～1096)的氨基酸序列进行了比较。结果显示,抗α-1重复序列(117-137)抗体对大鼠心肌细胞Na+-Ca2+交换电流呈现剂量依赖性的抑制作用。在钳制电压为+50和-100mV时,其抑制外向和内向钠-钙交换电流的IC50分别为18.9和22.4nmol/L。此外,该抗体还对L型钙通道电流具有抑制效应(IC50=22.7nmol/L),对电压门控钠通道和延迟整流钾通道电流则无明显影响。通过氨基酸序列比对发现,NCX α-1重复序列(117-137)与L型钙通道IIIS5-S6序列(孔环)之间具有23.8%的相似性。以上结果表明,抗NCX α-1重复序列(117-137)抗体是心肌NCX的一种抑制性抗体,同时也可以抑制L型钙通道。     

多不饱和脂肪酸对成年雪貂心肌钾通道的作用

本研究是在成年雪貂的心肌上研究多不饱和脂肪酸（PUFA）对电压门控钾通道的效应。我们观察到,n-3 PUFA能抑制短时性外向钾电流（Ito)和延迟整流钾电流（IK),而对内向整流钾电流（IK1）则没有明显影响。二十二碳六烯酸（DHA）对Ito和Ik能产生浓度依赖性的抑制作用,其IC50分别为7.5和20μmol/L,但不影响IK1。二十碳五烯酸（EPA）对这三种钾通道的作用与DHA相似。花生四烯酸（5或10μmol/L)先引起IK的抑制,然后引起IK,AA的激活;用环氧合酶抑制剂消炎痛可以阻断花生四烯酸激活IK,AA的作用。不具有抗心律失常作用的单不饱和脂肪酸和饱和脂肪酸都不明显影响这些钾通道的活性。上述实验结果证明,n-3 PUFA能抑制心肌细胞的Ito和IK,但和我们以前报道的PUFA对心肌钠电流和钙电流的作用相比,其对Ito和IK抑制作用的效能较低。n-3 PUFA的抗心律失常效应可能与它们抑制心肌钠、钙、钾通道的作用有关。     

一种改进的人体心房肌细胞分离方法

本研究旨在探讨稳定的人体心房肌细胞分离方法,并观察分离的正常窦性心律（normal sinus rhythm,NSR）患者右心房肌细胞基本电生理特性。XXIV型蛋白酶和V型胶原酶两步法进行单个人体心房肌细胞分离,常规全细胞膜片钳技术记录正常的L-型钙通道电流（L-type calcium current,ICa-L）、钠通道电流（sodiumcurrent,INa）、瞬时外向钾通道电流（transient outward potassium current,Itol）和内向整流钾通道电流（inward rectifier potassium current,Ik1）。此方法分离的人体心房肌细胞数量多,细胞膜光滑,折光性强,横纹清楚,耐钙,可用于膜片钳实验的占分离细胞总数的50％-60％。该方法简单、稳定、可靠,酶用量少,分离的心肌细胞质量好,数量多,并能记录到多种离子通道电流,表明其具有正常的电生理功能,适合膜片钳实验。     

白细胞介素-6对新生大鼠海马神经元电压依赖离子通道和NMDA电流的影响

目的: 研究白细胞介素-6对海马神经元电压依赖离子通道和NMDA电流的影响.方法: 应用全细胞膜片钳技术观察IL-6对电压依赖性钠通道电流(INa),延迟整流性钾通道电流(IK),电压依赖性钙通道电流(ICa),NMDA(N-methyl-D-aspartate)受体通道电流的影响.结果: 50 ng/ml IL-6作用24 h后IK 和ICa明显减小,Cm明显增大.50,500 ng/ml时减小NMDA电流.结论: IL-6通过作用于电压依赖钾通道,钙离子通道及NMDA通道影响神经元功能.     

成年蜜蜂脑神经细胞的培养和电生理特征

为了研究杀虫剂等对蜜蜂毒性作用的神经机制,需在体外建立成年蜜蜂脑神经细胞的分离培养和电生理记录技术并研究其正常电生理特征,而对成年蜜蜂脑神经细胞的分离培养和电生理特性的研究报道甚少。我们采用酶解和机械吹打相结合的方法获得了数量较多且活力较好的成年意大利蜜蜂Apis mellifera脑神经细胞,并用全细胞膜片钳技术研究了成年意大利蜜蜂脑神经细胞对电流和电压刺激的反应,获得了成年意蜂脑神经细胞的基本电生理特征以及钠电流和钾电流的特性。全细胞电流钳的记录结果表明,在体外培养条件下,细胞无自发放电发生,注射电流后仅引起细胞单次放电,引起细胞放电的阈电流平均为60.8±63 pA; 细胞动作电位产生的阈电位平均为−27.4±2.3 mV。用全细胞电压钳记录了神经细胞的钠电流和钾电流。钠电流的分离是在电压刺激下通过阻断钾通道和钙通道实现。细胞的内向钠电流在指令电压为−40～−30 mV左右激活,−10 mV达峰值,钠通道的稳态失活电压V_1/2为−58.4 mV; 外向钾电流成份至少包括较小的快速失活钾电流和和较大的缓慢失活钾电流（占总钾电流的80%）,其半激活膜电位V_1/2为3.86 mV,无明显的稳态失活。结果提示缓慢失活钾电流的特征可能是细胞单次放电的机制之一。     

心肌细胞电压依赖性钾通道的研究进展

心肌细胞电压依赖性钾通道的研究进展周军,周兆年（中国科学院上海生理研究所上海２０００３１）在心肌,分布较多且研究较为深入的电压依赖性钾通道（ＶＤＰＣ）主要是短暂外向钾通道Ｉｔｏ、延迟整流钾通道ＩＫ和内向整流钾通道ＩＫ１,它们共同参与心肌动作电位的复极...     

白细胞介素-6对新生大鼠海马神经元电压依赖离子通道和NMDA电流的影响

目的 :研究白细胞介素 6对海马神经元电压依赖离子通道和NMDA电流的影响。方法 :应用全细胞膜片钳技术观察IL 6对电压依赖性钠通道电流 (INa) ,延迟整流性钾通道电流 (IK) ,电压依赖性钙通道电流 (ICa) ,NMDA(N methyl D aspartate)受体通道电流的影响。结果 :5 0ng/mlIL 6作用 2 4h后IK和ICa明显减小 ,Cm明显增大。 5 0 ,5 0 0ng/ml时减小NMDA电流。结论 :IL 6通过作用于电压依赖钾通道 ,钙离子通道及NMDA通道影响神经元功能。     

利诺吡啶对豚鼠耳蜗外毛细胞和Deiters细胞钾电流的抑制

为探讨KCNQ家族钾通道在耳蜗外毛细胞和Deiters细胞的功能性表达,我们观察并记录了KCNQ家族钾通道阻滞剂利诺吡啶对豚鼠耳蜗单离外毛细胞(outer hair cells,OHCs)和Deiters细胞总钾电流的影响。采用酶孵育加机械分离法分离豚鼠耳蜗单个OHCs和Deiters细胞：运用膜片钳技术,在全细胞模式下记录正常细胞外液中8个外毛细胞和5个Deiters细胞的总钾电流,并观察100μmol／L和200μmol／L利诺吡啶对外毛细胞和Deiters细胞总钾电流的影响。结果观察到,在正常细胞外液中的单离外毛细胞,可记录到四乙基二乙胺敏感的外向性钾电流和静息膜电位附近激活的内向性钾电流(the K^ current activated at negative potential,IKa)两种钾电流,而在单离Deiters细胞中只记录到外向整流性钾电流。在细胞外液中,加入100μmol／L利诺吡啶后,OHCs中的四乙基二乙胺敏感的钾电流峰电流成分被抑制,稳态电流幅值减小,且电流的失活时问常数明显延长;在细胞外液中加入100μmol／L和200μmol／L利诺吡啶后,OHCs的内向性钾电流IKa被完全抑制;而细胞外液中利诺吡啶终浓度为200μmol／L时,Deiters细胞的外向整流性钾电流幅值无明显变化。由此我们推测,KCNQ家族钾通道存在于豚鼠耳蜗外毛细胞,其介导的钾电流是四乙基二乙胺敏感的钾电流的组成部分,并构成全部的IKn,其功能是介导细胞内K^ 外流和防止细胞过度去极化;KCNQ家族钾通道不存在于豚鼠耳蜗Dciters细胞。     

钙激活性氯离子通道的电生理研究

目的:研究大鼠肺动脉平滑肌细胞上钙激活性氯离子通道的电流、电压电流关系等电生理特性.方法:采用急性酶分离法(胶原酶Ⅰ型和木瓜蛋白酶)分离出单个肺动脉平滑肌细胞,应用膜片钳技术,测定各组大鼠肺动脉平滑肌细胞上钙激活性氯离子通道电流和电压电流.结果:急性酶分离法能成功分离出适用于膜片钳记录的单个大鼠肺动脉平滑肌细胞,并测到稳定的钙激活性氯离子通道电流,该电流表现出时间、电压及钙离子依赖性,并呈外向整流特征.结论:大鼠肺动脉平滑肌细胞的钙激活氯离子通道具有时间依赖性、钙离子依赖性和电压依赖性,并具有外向整流特征.     

心肌细胞钾通道的分子学多样性

电压调控性钾通道和内向整流性钾通道是心肌细胞两类主要的钾通道,对心肌细胞动作电位的形成起重要的作用。对其分子生物学结构的多样性的研究,有助于进一步弄清其功能并为寻找理想的抗心律失常药物提供理论指导。     

Statistical properties of ion channel records. Part I: relationship to the macroscopic current

Macroscopic ion channel current can be derived by summation of the stochastic records of individual channel currents. In this paper, we present two probability density functions of single channel records that can uniquely determine the macroscopic current regardless of other statistical properties of records or the stochastic model of channel gating (presented often with stationary Markov models). We show that H(t), probability density function of channel opening events (introduced explicitly in this paper), and D(t), probability density function of the open duration (sometimes has named dwell time distribution as well), determine the normalized macroscopic current, G(t), through G(t) = P(t) - H(t) * Q(t) where P(t) is the cumulative density function of H(t), Q(t) is the cumulative density function of D(t), * is the symbol of convolution integral and G(t) is the macroscopic current divided by the amplitude of single channel current and the number of single channel sweeps. Compared to other equations for the macroscopic current, here the macroscopic current is expressed only in terms of the statistical properties of single channel current and not the stochastic model of ion channel gating or a conditioned form of macroscopic current. Single channel currents of an inactivating BK channel were used to validate this relationship experimentally too. In this paper, we used median filters as they can remove the unwanted noise without smoothing the transitions between open and closed states (compare to low pass filters). This filtering leads to more accurate measurement of transition times and less amount of missed events.     

Coupling between voltage sensor activation,Ca2+ binding and channel opening in large conductance (BK) potassium channels

To determine how intracellular Ca(2+) and membrane voltage regulate the gating of large conductance Ca(2+)-activated K(+) (BK) channels, we examined the steady-state and kinetic properties of mSlo1 ionic and gating currents in the presence and absence of Ca(2+) over a wide range of voltage. The activation of unliganded mSlo1 channels can be accounted for by allosteric coupling between voltage sensor activation and the closed (C) to open (O) conformational change (Horrigan, F.T., and R.W. Aldrich. 1999. J. Gen. Physiol. 114:305-336; Horrigan, F.T., J. Cui, and R.W. Aldrich. 1999. J. Gen. Physiol. 114:277-304). In 0 Ca(2+), the steady-state gating charge-voltage (Q(SS)-V) relationship is shallower and shifted to more negative voltages than the conductance-voltage (G(K)-V) relationship. Calcium alters the relationship between Q-V and G-V, shifting both to more negative voltages such that they almost superimpose in 70 microM Ca(2+). This change reflects a differential effect of Ca(2+) on voltage sensor activation and channel opening. Ca(2+) has only a small effect on the fast component of ON gating current, indicating that Ca(2+) binding has little effect on voltage sensor activation when channels are closed. In contrast, open probability measured at very negative voltages (less than -80 mV) increases more than 1,000-fold in 70 microM Ca(2+), demonstrating that Ca(2+) increases the C-O equilibrium constant under conditions where voltage sensors are not activated. Thus, Ca(2+) binding and voltage sensor activation act almost independently, to enhance channel opening. This dual-allosteric mechanism can reproduce the steady-state behavior of mSlo1 over a wide range of conditions, with the assumption that activation of individual Ca(2+) sensors or voltage sensors additively affect the energy of the C-O transition and that a weak interaction between Ca(2+) sensors and voltage sensors occurs independent of channel opening. By contrast, macroscopic I(K) kinetics indicate that Ca(2+) and voltage dependencies of C-O transition rates are complex, leading us to propose that the C-O conformational change may be described by a complex energy landscape.     

Allosteric voltage gating of potassium channels II. Mslo channel gating charge movement in the absence of Ca(2+).

Large-conductance Ca(2+)-activated K(+) channels can be activated by membrane voltage in the absence of Ca(2+) binding, indicating that these channels contain an intrinsic voltage sensor. The properties of this voltage sensor and its relationship to channel activation were examined by studying gating charge movement from mSlo Ca(2+)-activated K(+) channels in the virtual absence of Ca(2+) (<1 nM). Charge movement was measured in response to voltage steps or sinusoidal voltage commands. The charge-voltage relationship (Q-V) is shallower and shifted to more negative voltages than the voltage-dependent open probability (G-V). Both ON and OFF gating currents evoked by brief (0.5-ms) voltage pulses appear to decay rapidly (tau(ON) = 60 microseconds at +200 mV, tau(OFF) = 16 microseconds at -80 mV). However, Q(OFF) increases slowly with pulse duration, indicating that a large fraction of ON charge develops with a time course comparable to that of I(K) activation. The slow onset of this gating charge prevents its detection as a component of I(gON), although it represents approximately 40% of the total charge moved at +140 mV. The decay of I(gOFF) is slowed after depolarizations that open mSlo channels. Yet, the majority of open channel charge relaxation is too rapid to be limited by channel closing. These results can be understood in terms of the allosteric voltage-gating scheme developed in the preceding paper (Horrigan, F.T., J. Cui, and R.W. Aldrich. 1999. J. Gen. Physiol. 114:277-304). The model contains five open (O) and five closed (C) states arranged in parallel, and the kinetic and steady-state properties of mSlo gating currents exhibit multiple components associated with C-C, O-O, and C-O transitions.     

PACEMAKER OSCILLATIONS IN HEART AND BRAIN: A KEY ROLE FOR HYPERPOLARIZATION-ACTIVATED CATION CHANNELS

Rhythmic activity of single cells or multicellular networks is a common feature of all organisms. The oscillatory activity is characterized by time intervals of several seconds up to many hours. Cellular rhythms govern the beating of the heart, the swimming behavior of sperm, cycles of sleep and wakefulness, breathing, and the release of hormones. Many neurons in the brain and cardiac cells are characterized by endogenous rhythmic activity, which relies on a complex interplay between several distinct ion channels. In particular, one type of ion channel plays a prominent role in the control of rhythmic electrical activity since it determines the frequency of the oscillations. The activity of the channels is thus setting the “pace” of the oscillations; therefore, these channels are often referred to as “pacemaker” channels. Despite their obvious important physiological function, it was not until recently that genes encoding pacemaker channels have been identified. Because both hyperpolarization and cyclic nucleotides are key elements that control their activity, pacemaker channels have now been designated hyperpolarization-activated and cyclic nucleotide–gated (HCN) channels. The molecular identification of the channels and the upcoming studies on their properties in heterologous systems will certainly enhance our understanding of “pacemaking” in physiological systems. This review gives a brief insight into the physiological importance of these channels and sums up what we have learned since the first cloning of genes succeeded (for recent reviews, see also Clapham 1998; Luüthi and McCormick 1998a; Biel et al. 1999; Ludwig, Zong, Hofmann, et al. 1999; Santoro and Tibbs 1999). (Chronobiology International, 17(4), 453–469, 2000)     

The enantiomer pair of 24S- and 24R-hydroxycholesterol differentially alter activity of large-conductance Ca2+-dependent K+ (slo1 BK) channel

24S-hydroxycholesterol (HC) is most abundant oxysterols in the brain, passes through blood brain barrier, and is therefore regarded as an intermediary for brain cholesterol elimination. We reported that large-conductance Ca²⁺- and voltage-activated K⁺ (slo1 BK) channels are suppressed by this oxysterol, which is presumably intercalated into cell membrane to access the outer surface of the channel. Such an outer approach would make it difficult to interact with the inner, ion-conducting part of the channel. The present findings showed that 24R-HC, the racemic counterpart of 24S-HC, also suppressed slo1 BK channel but in a different voltage-dependent manner. There was a difference between the effects of the two enantiomers on activation kinetics but not on deactivation kinetics. It is suggested that the chirality contributes to the efficacy of channel blockers that act from outer lipophilic parts of channels, as with those which act on the inner, ion-permeable surface.     

Allosteric Effects of Permeating Cations on Gating Currents during K+ Channel Deactivation

K⁺ channel gating currents are usually measured in the absence of permeating ions, when a common feature of channel closing is a rising phase of off-gating current and slow subsequent decay. Current models of gating invoke a concerted rearrangement of subunits just before the open state to explain this very slow charge return from opening potentials. We have measured gating currents from the voltage-gated K⁺ channel, Kv1.5, highly overexpressed in human embryonic kidney cells. In the presence of permeating K⁺ or Cs⁺, we show, by comparison with data obtained in the absence of permeant ions, that there is a rapid return of charge after depolarizations. Measurement of off-gating currents on repolarization before and after K⁺ dialysis from cells allowed a comparison of off-gating current amplitudes and time course in the same cells. Parallel experiments utilizing the low permeability of Cs⁺ through Kv1.5 revealed similar rapid charge return during measurements of off-gating currents at E_Cs. Such effects could not be reproduced in a nonconducting mutant (W472F) of Kv1.5, in which, by definition, ion permeation was macroscopically absent. This preservation of a fast kinetic structure of off-gating currents on return from potentials at which channels open suggests an allosteric modulation by permeant cations. This may arise from a direct action on a slow step late in the activation pathway, or via a retardation in the rate of C-type inactivation. The activation energy barrier for K⁺ channel closing is reduced, which may be important during repetitive action potential spiking where ion channels characteristically undergo continuous cyclical activation and deactivation.     

A mutant KcsA K(+) channel with altered conduction properties and selectivity filter ion distribution

The selectivity filter of K(+) channels is comprised of a linear queue of four equal-spaced ion-binding sites spanning a distance of 12A. Each site is formed of eight oxygen atoms from the protein. The first three sites, numbered 1-3 from the extracellular side, are made of exclusively main-chain carbonyl oxygen atoms. The fourth site, closest to the intracellular side, is made of four main-chain carbonyl oxygen atoms and four threonine side-chain hydroxyl oxygen atoms. Here we characterize the effects of mutating the threonine to cysteine on the distribution of ions in the selectivity filter and on the conduction of ions through the filter. The mutation influences the occupancy of K(+) at sites 2 and 4 and it reduces the maximum rate of conduction in the limit of high K(+) concentration. The mutation does not affect the conduction of Rb(+). These results can be understood in the context of a conduction mechanism in which a pair of K ions switch between energetically balanced 1,3 and 2,4 configurations.     

Histidine scanning mutagenesis of basic residues of the S4 segment of the shaker k+ channel

The voltage sensor of the Shaker potassium channel is comprised mostly of positively charged residues in the putative fourth transmembrane segment, S4 (Aggarwal, S.K., and R. MacKinnon. 1996. Neuron. 16:1169-1177; Seoh, S.-A., D. Sigg, D.M. Papazian, and F. Bezanilla. 1996. Neuron. 16:1159-1167). Movement of the voltage sensor in response to a change in the membrane potential was examined indirectly by measuring how the accessibilities of residues in and around the sensor change with voltage. Each basic residue in the S4 segment was individually replaced with a histidine. If the histidine tag is part of the voltage sensor, then the gating charge displaced by the voltage sensor will include the histidine charge. Accessibility of the histidine to the bulk solution was therefore monitored as pH-dependent changes in the gating currents evoked by membrane potential pulses. Histidine scanning mutagenesis has several advantages over other similar techniques. Since histidine accessibility is detected by labeling with solution protons, very confined local environments can be resolved and labeling introduces minimal interference of voltage sensor motion. After histidine replacement of either residue K374 or R377, there was no titration of the gating currents with internal or external pH, indicating that these residues do not move in the transmembrane electric field or that they are always inaccessible. Histidine replacement of residues R365, R368, and R371, on the other hand, showed that each of these residues traverses entirely from internal exposure at hyperpolarized potentials to external exposure at depolarized potentials. This translocation enables the histidine to transport protons across the membrane in the presence of a pH gradient. In the case of 371H, depolarization drives the histidine to a position that forms a proton pore. Kinetic models of titrateable voltage sensors that account for proton transport and conduction are presented. Finally, the results presented here are incorporated into existing information to propose a model of voltage sensor movement and structure.     

Built for speed

Many of us were taught in high school biology that the action potential waveform in nerves and other excitable tissues was generated by an initial rapid influx of external Na⁺ ions across the plasma membrane, followed by an outward movement of intracellular K⁺ ions. The former event, mediated by voltage-gated Na⁺ channels, is responsible for the fast depolarizing upstroke of the action potential, while voltage-gated K+ channels are responsible for the subsequent repolarizing phase, which largely controls action potential duration. Although Hodgkin and Huxley described the fundamental importance of this sequential activation process more than 60 y ago, the molecular and structural details underlying the faster activation of voltage-gated Na⁺ (Nav) vs. K⁺ (Kv) channels have yet to be fully resolved.     

Activation of Shaker Potassium Channels : I. Characterization of Voltage-dependent Transitions

The conformational changes associated with activation gating in Shaker potassium channels are functionally characterized in patch-clamp recordings made from Xenopus laevis oocytes expressing Shaker channels with fast inactivation removed. Estimates of the forward and backward rates for transitions are obtained by fitting exponentials to macroscopic ionic and gating current relaxations at voltage extremes, where we assume that transitions are unidirectional. The assignment of different rates is facilitated by using voltage protocols that incorporate prepulses to preload channels into different distributions of states, yielding test currents that reflect different subsets of transitions. These data yield direct estimates of the rate constants and partial charges associated with three forward and three backward transitions, as well as estimates of the partial charges associated with other transitions. The partial charges correspond to an average charge movement of 0.5 e₀ during each transition in the activation process. This value implies that activation gating involves a large number of transitions to account for the total gating charge displacement of 13 e₀. The characterization of the gating transitions here forms the basis for constraining a detailed gating model to be described in a subsequent paper of this series.