睫状体色素上皮细胞容积激活性氯电流

为研究睫状体色素上皮 (pigmentedciliaryepithelial,PCE)细胞容积激活性Cl-电流的特性 ,用膜片箝全细胞记录技术记录了猪的低渗液诱发的容积激活性Cl-电流。此电流外向占优势 ,几乎没有时间依赖性失活 ,电流 电压曲线显示此电流反转电位 (- 6 3± 0 5mV)很接近氯离子平衡电位的计算值 (ECl=0mV)。电流的激活依赖于细胞内ATP ,细胞外ATP抑制外向电流和内向电流 ,但外向电流抑制率大于内向电流抑制率 (92 %比 74% ,P <0 0 1)。氯离子通道阻断剂tamoxifen抑制外向电流和内向电流 ,两个抑制率几乎相等 (85 %比 87% ,P >0 0 5 )。此电流特性与其他类型细胞的P糖蛋白相关电流很相似。结果提示PCE细胞容积激活性Cl-电流的形成可能与P糖蛋白有关     

Investigation of burst generation by the electrically coupled cyberchron network in the snail Helisoma using a single-electrode voltage clamp

This paper describes the results of investigating burst generation by the cyberchron network in the snail Helisoma. The cyberchron network is composed of approximately 20 electrically coupled neurons and controls the feeding behavior of the snail. The electrical coupling between network members has made it particularly difficult to distinguish between the importance and involvement of single-cell and network properties in burst generation by this system. The present investigations utilized the new single-electrode voltage clamp to examine the membrane properties and network interactions of the cyberchron neurons: (1) A slow outward current is activated by moderately large depolarizing commands (?40 to 0 mV) and does not undergo inactivation decay (i.e., decline in magnitude) during a command potential step maintained for 10 sec or more. The lack of inactivation of the outward current in cyberchron neurons appears to be due to the dominating role of a Ca-dependent K current. (2) There are two functionally distinct classes of cyberchrons—current generator cyberchrons and follower cyberchrons. (3) Primary current generator cyberchrons have membrane properties similar to endogenous bursting neurons (e.g., persistent inward Ca current and negative resistance region in I–V plot) and appear to provide the main driving and timing current for the rest of the network. (4) The vast majority of cyberchrons are secondary current generator cyberchrons with membrane properties which exhibit inward-going rectification and appear to burst as a result of regenerative excitation with one another and the primary current generator cyberchrons. (5) The second class of cyberchrons are driven by the electrical synaptic input from the current generator cyberchrons, do not exhibit inward-going rectification, and are called follower cyberchrons. (6) Burst termination is due to activation of a slow outward tail current in most cyberchrons during the burst (probably Ca-activated K current) which causes a hyperpolarization in individual cyberchrons, terminating the burst. (7) Decay of the outward tail current causes the cyberchrons to depolarize, which activates the persistent inward Ca current in the primary current generator cyberchrons, starting the burst cycle anew.     

人胎儿鼻咽上皮细胞的背景氯电流

采用膜片钳和图像分析技术,研究人胎儿鼻咽上皮细胞背景电流的特性及其与容积激活性氯电流的关系。在等张溶液中,可记录到一背景电流,该电流呈微弱的外向整流性,无明显时间依赖性失活,其翻转电位为(?0.73±1.7)mV(n=21),接近氯离子平衡电位(?0.9mV)。细胞外高张刺激(440mOsmol/L)明显抑制此电流(59.6±7.1)%,而低张刺激(160mOsmol/L)则诱发细胞产生容积激活性氯电流。氯通道阻断剂tamoxifen和5-硝基-2-(3-苯丙胺基)苯甲酸[5-nitro-2-(3-phenylpropylamino)benzoicacid,NPPB]显著地抑制背景电流并使细胞基础容积增大。上述结果表明,人胎儿鼻咽上皮细胞的背景Cl?电流是背景电流的重要成分,此Cl?电流与容积激活性氯电流及细胞基础容积调节有关。     

Flow-activated chloride channels in vascular endothelium. Shear stress sensitivity, desensitization dynamics, and physiological implications

Although activation of outward rectifying Cl(-) channels is one of the fastest responses of endothelial cells (ECs) to shear stress, little is known about these channels. In this study, we used whole-cell patch clamp recordings to characterize the flow-activated Cl(-) current in bovine aortic ECs (BAECs). Application of shear stress induced rapid development of a Cl(-) current that was effectively blocked by the Cl(-) channel antagonist 5-nitro-2-(3-phenopropylamino)benzoic acid (100 microM). The current initiated at a shear stress as low as 0.3 dyne/cm(2), attained its peak within minutes of flow onset, and saturated above 3.5 dynes/cm(2) approximately 2.5-3.5-fold increase over pre-flow levels). The Cl(-) current desensitized slowly in response to sustained flow, and step increases in shear stress elicited increased current only if the shear stress levels were below the 3.5 dynes/cm(2) saturation level. Oscillatory flow with a physiological oscillation frequency of 1 Hz, as occurs in disturbed flow zones prone to atherosclerosis, failed to elicit the Cl(-) current, whereas lower oscillation frequencies led to partial recovery of the current. Nonreversing pulsatile flow, generally considered protective of atherosclerosis, was as effective in eliciting the current as steady flow. Measurements using fluids of different viscosities indicated that the Cl(-) current is responsive to shear stress rather than shear rate. Blocking the flow-activated Cl(-) current abolished flow-induced Akt phosphorylation in BAECs, whereas blocking flow-sensitive K(+) currents had no effect, suggesting that flow-activated Cl(-) channels play an important role in regulating EC flow signaling.     

The pacemaker current in cardiac Purkinje myocytes

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).     

Potassium channels regulated by inositol 1,3,4,5-tetrakisphosphate and internal calcium in DDT1 MF-2 smooth muscle cells

This study was carried out to determine the intracellular components responsible for the transmembrane current evoked by stimulation of H1-histaminergic receptors in DDT1 MF-2 smooth muscle cells. Histamine elicited an outward current that was reversed below the K+ equilibrium potential and passed voltage-independent K+ channels. A histamine concentration-dependent rise in outward current and in cytoplasmic-free Ca2+ with similar time courses was observed. The histamine-induced current was not found after depletion of internal Ca2+ stores, suggesting a coupling between internal Ca2+ and K+ current. The time course of the initial increase in inositol (1,4,5)-trisphosphate (Ins (1,4,5)P3) caused by histamine differs from that of the internal Ca2+ response. However, a significant concentration-dependent increase in inositol (1,3,4,5)-tetrakisphosphate (Ins (1,3,4,5)P4) was seen during the whole stimulating period. The role of internal Ca2+, Ins (1,4,5)P3, and Ins (1,3,4,5)P4 on the outward current was also examined by the addition of these substances directly to the cytoplasm. Internal application of Ca2+ increased the amplitude and duration of the histamine-induced current whereas internal EGTA suppressed the outward current. Internal Ins (1,4,5)P3 did not affect the histamine-induced K+ current, Ins (1,3,4,5)P4 inhibited the outward current, and the combination of Ins (1,3,4,5)P4 and Ca2+ abolished this response. The noradrenaline response evoked under normal conditions is not reflected by a change in transmembrane current or a change in Ins (1,3,4,5)P4 but is associated with an increase in Ins (1,4,5)P3 and internal Ca2+. Stimulation of alpha 1-adrenoceptors, however, also evoked an outward current after the addition of Ins (1,3,4,5)P4 intracellularly. It is concluded that K+ channels, carrying the histamine outward current, are activated from the combined action of internal Ca2+ and Ins (1,3,4,5)P4.     

Isolation and characterization of I(Kr) in cardiac myocytes by Cs+ permeation

Isolation of the rapidly activating delayed rectifier potassium current (I(Kr)) from other cardiac currents has been a difficult task for quantitative study of this current. The present study was designed to separate I(Kr) using Cs+ in cardiac myocytes. Cs+ have been known to block a variety of K+ channels, including many of those involved in the cardiac action potential such as inward rectifier potassium current I(K1) and the transient outward potassium current I(to). However, under isotonic Cs+ conditions (135 mM Cs+), a significant membrane current was recorded in isolated rabbit ventricular myocytes. This current displayed the voltage-dependent onset of and recovery from inactivation that are characteristic to I(Kr). Consistently, the current was selectively inhibited by the specific I(Kr) blockers. The biophysical and pharmacological properties of the Cs+-carried human ether-a-go-go-related gene (hERG) current were very similar to those of the Cs+-carried I(Kr) in ventricular myocytes. The primary sequence of the selectivity filter in hERG was in part responsible for the Cs+ permeability, which was lost when the sequence was changed from GFG to GYG, characteristic of other, Cs+-impermeable K+ channels. Thus the unique high Cs+ permeability in I(Kr) channels provides an effective way to isolate I(Kr) current. Although the biophysical and pharmacological properties of the Cs+-carried I(Kr) are different from those of the K+-carried I(Kr), such an assay enables I(Kr) current to be recorded at a level that is large enough and sufficiently robust to evaluate any I(Kr) alterations in native tissues in response to physiological or pathological changes. It is particularly useful for exploring the role of reduction of I(Kr) in arrhythmias associated with heart failure and long QT syndrome due to the reduced hERG channel membrane expression.     

Possible existence of transient TTX-sensitive chloride current in the membrane of isolated cardiomyocytes

Cardiomyocytes enzymatically isolated from rat and guinea pig ventricular tissue were investigated under conditions of intracellular perfusion and voltage clamp at 18-20 degrees C. Perfusion with 135 mmol/l Tris(HF), pH 7.2 was used to eliminate outward potassium currents. The dependence of inward current (elicited by depolarizing pulses from a holding potential level of--120 mV) on low external TTX concentrations (from 10(-13) to 10(-10) mol/l) was studied. Similar TTX concentrations increased the amplitude of the inward current and changed its kinetics in a large number of cells tested. The effect was fully reversible. The effect could be evaluated in a net form by digital subtraction of the current obtained after the application of a low external TTX concentration from the initial current in a TTX-free solution. The TTX concentration dependence of the difference current could be fitted by one-to-one binding curve with Kd = (1.0 +/= 0.4) x 10(-12) mol/l. TTX-induced current changes were absent in low sodium or chloride-free external solutions. The outward current (a block of which by TTX produced the inward current changes observed) showed a reversal potential consistent with the chloride nature of such a current. The existence of a transient TTX-sensitive Na-dependent potential gated chloride current in the membrane of isolated cardiomyocytes is postulated.     

非洲爪蟾卵母细胞GABAB和GABAc受体介导的电流反应

实验应用双电极电压箝技术,在具有滤泡膜的非洲爪蟾(Xenopuslaevis)卵母细胞上记录到γ-氨基丁酸(γ-aminobutyricacid,GABA)-激活电流。此GABA-激活电流的特点及有关GABA受体类型的研究和分析如下(1)在35.5%(55/155)的受检细胞外加GABA可引起一慢的浓度依赖性的外向电流。(2)GABAA受体的选择性拮抗剂bicuculline(10     

Three kinds of currents in the canine betaine-GABA transporter BGT-1 expressed in Xenopus laevis oocytes

The cloned canine betaine-GABA cotransporter BGT-1 has been heterologously expressed in Xenopus laevis oocytes in order to characterize its electrophysiological properties. Voltage-clamp experiments on transfected oocytes reveal the presence of three types of membrane current which are absent in non-injected oocytes: (i) an organic substrate-independent current (uncoupled current); (ii) a transport-associated current, seen upon addition of betaine or GABA; (iii) presteady-state currents induced by voltage changes. The three kinds of current are analogous to those reported in structurally similar cotransporters. The transport-associated current is strictly dependent on the presence of Na(+). The good correlation between the amount of charge underlying the presteady-state currents and the transport-associated current indicates that both processes are due to the activity of the transporter.     

Barium currents in developing skeletal muscle cells of normal and mutant mice foetuses with 'muscular dysgenesis'.

The ontogenesis of Ca channel activities was studied in the developing myotubes of normal mice and mutant mice foetuses with 'Muscular Dysgenesis'. The ionic current through Ca channels was measured with Ba2+ as charge carrier using the whole cell clamp technique. All dissociated myotubes from foetuses (14th to 18th day of gestation) showed two distinct inward Ba currents: a low threshold, transient current (T-type) and a high threshold sustained current. In normal myotubes, T-type current density increased from the 14th day to the 16th day of gestation. After day 16, T-type current density decreased gradually until birth. Similar changes in T-type current density were observed in developing dysgenic myotubes where the current density was about 40% of that measured in normal myotubes throughout the prenatal period studied. The high threshold sustained current (L-type current) density increased gradually with age in normal myotubes while absent in dysgenic muscle. The latter, regardless of age, showed a high threshold current (Idys) which is distinct from the L-type current. Idys density did not change during the prenatal myogenesis period studied.     

Steady-state and dynamic properties of cardiac sodium-calcium exchange. Ion and voltage dependencies of the transport cycle

Ion and voltage dependencies of sodium-calcium exchange current were studied in giant membrane patches from guinea pig ventricular cells after deregulation of the exchanger with chymotrypsin. (a) Under zero-trans conditions, the half-maximum concentration (Kh) of cytoplasmic calcium (Cai) for activation of the isolated inward exchange current decreased as the extracellular sodium (Nao) concentration was decreased. The Kh of cytoplasmic sodium (Nai) for activation of the isolated outward exchange current decreased as the extracellular calcium (Cao) concentration was decreased. (b) The current-voltage (I-V) relation of the outward exchange current with saturating concentrations of Nai and Cao had a shallow slope (twofold change in approximately 100 mV) and a slight saturation tendency at very positive potentials. The outward current gained in steepness as the Nai concentration was decreased, such that the Kh for Nai decreased with depolarization. The decrease of Kh for Nai with depolarization was well described by a Boltzmann equation (e alpha.Em/26.6) with a slope (alpha) of -0.06. (c) Voltage dependence of the outward current was lost as the Cao concentration was decreased, and the Kh for Cao increased upon depolarization with a Boltzmann slope of 0.26. (d) The I-V relation of the inward exchange current, under zero-trans conditions, was also almost linear (twofold change in approximately 100 mV) and showed some saturation tendency with hyperpolarization as the Cai concentration was decreased. The Kh for Cai decreased with depolarization (Boltzmann slope, -0.10). Voltage dependence of the inward current was decreased in the presence of a high (300 mM) Nao concentration. (e) In the presence of both Na and Ca on both membrane sides, the I-V relations with saturating Nai show sigmoidal shape and clear saturation at positive potentials. Measured reversal potentials were close to the equilibrium potential expected for a 3 Na to 1 Ca exchange. (f) Nai and Cai interacted competitively with respect to the outward current, but in a mixed competitive-noncompetitive fashion with respect to the inward current. (g) Cai inhibited the outward exchange current in a voltage-dependent manner. The half-effective concentration for inhibition (Ki) by Cai increased upon depolarization with a Boltzmann slope of 0.32 in 25 mM Nai and 0.20 in 100 mM Nai. (h) Nai also inhibited the inward exchange current voltage dependently. The Ki decreased upon depolarization (Boltzmann slope, -0.11 at 3 microM Cai and -0.10 at 1.08 mM Cai).(ABSTRACT TRUNCATED AT 400 WORDS)     

Na-K pump current in the Amphiuma collecting tubule

There is strong evidence supporting the hypothesis of an electrogenic Na-K pump in the basolateral membrane of several epithelia. Thermodynamic considerations and results in nonepithelial cells indicate that the current carried by the pump could be voltage dependent. In order to measure the pump current and to determine its voltage dependence in a tight epithelium, we have used the isolated perfused collecting tubule of Amphiuma and developed a technique for clamping the basolateral membrane potential (Vbl) through transepithelial current injection. The transcellular current was calculated by subtracting the paracellular current (calculated from the transepithelial conductance measured in the presence of luminal amiloride) from the total transepithelial current. Basolateral membrane current-voltage (I-V) curves were obtained in conditions where the ratio of the pump current to the total basolateral membrane current had been maximized by loading the cells with Na+ (exposure to low-K+ bath), and by blocking the basolateral K+ conductance with barium. The pump current was defined as the difference of the current across the basolateral membrane measured before and 10-15 s after the addition of strophanthidin (20 microM) to the bath solution. With a bath solution containing 3 mM K+, the pump current was nearly constant in the Vbl range of -20 to -80 mV (52 +/- 5 microA.cm-2 at -60 mV) but showed a marked voltage dependence at higher negative Vbl (pump current decreased to 5 +/- 9 microA.cm-2 at -180 mV). In a 1.0 mM K bath, the shape of the pump I-V curve was similar but the amplitude of the current was decreased (24 +/- 4 microA.cm-2 at -60 mV). In a 0.1 mM K bath, the pump current was not significantly different from 0. Our results indicate that the basolateral Na-K pump generates a current which depends on the extracellular potassium concentration. With physiological peritubular concentration of K+ and in the physiological range of potential, the pump activity, measured as the pump-generated current, was independent of the membrane potential.     

Contribution of R domain phosphoserines to the function of CFTR studied in Fischer rat thyroid epithelia

The regulatory domain of cystic fibrosis transmembrane conductance regulator (CFTR) regulates channel activity when several serines are phosphorylated by cAMP-dependent protein kinase. To further define the functional role of individual phosphoserines, we studied CFTR containing previously studied and new serine to alanine mutations. We expressed these constructs in Fischer rat thyroid epithelia and measured transepithelial Cl(-) current. Mutation of four in vivo phosphorylation sites, Ser(660), Ser(737), Ser(795), and Ser(813) (S-Quad-A), substantially decreased cAMP-stimulated current, suggesting that these four sites account for most of the phosphorylation-dependent response. Mutation of either Ser(660) or Ser(813) alone significantly decreased current, indicating that these residues play a key role in phosphorylation-dependent stimulation. However, neither Ser(660) nor Ser(813) alone increased current to wild-type levels; both residues were required. Changing Ser(737) to alanine increased current above wild-type levels, suggesting that phosphorylation of Ser(737) may inhibit current in wild-type CFTR. These data help define the functional role of regulatory domain phosphoserines and suggest interactions between individual phosphoserines.     

Determination of RNA orientation during translocation through a biological nanopore

We investigate single-molecule electrophoretic translocation of A(50), C(50), A(25)C(50), and C(50)A(25) RNA molecules through the alpha-hemolysin transmembrane protein pore. We observe pronounced bilevel current blockages during translocation of A(25)C(50) and C(50)A(25) molecules. The two current levels observed during these bilevel blockages are very similar to the characteristic current levels observed during A(50) and C(50) translocation. From the temporal ordering of the two levels within the bilevel current blockages, we infer whether individual A(25)C(50) and C(50)A(25) molecules pass through the pore in a 3'-->5' or 5'-->3' orientation. Correlation between the level of current obstruction and the inferred A(25)C(50) or C(50)A(25) orientation indicates that 3'-->5' translocation of a poly C segment causes a significantly deeper current obstruction than 5'-->3' translocation. Our analysis also suggests that the 3' ends of C(50) and A(25)C(50) RNA molecules are more likely to initiate translocation than the 5' ends. Orientation dependent differences in a smaller current blockage that immediately precedes many translocation events suggest that this blockage also contains information about RNA orientation during translocation. These findings emphasize that the directionality of polynucleotide molecules is an important factor in translocation and demonstrate how structure within ionic current signals can give new insights into the translocation process.     

General anesthetics modulate GABA receptor channel complex in rat dorsal root ganglion neurons

The effects of halothane, isoflurane, and enflurane on ionic currents induced by bath application of gamma-amino-butyric acid (GABA) were studied with the rat dorsal root ganglion neurons maintained in primary culture. The whole-cell patch clamp technique was used to record the current. In normal neurons before exposure to anesthetics, GABA at low concentrations (1-3 x 10(-6) M) induced a small sustained inward current. At higher concentrations (3 x 10(-5) M-1 x 10(-3) M), GABA induced a large inward current, which decayed to a steady-state level (desensitization). Halothane (0.86 mM), isoflurane (0.96 mM), and enflurane (1.89 mM), each equivalent to the respective 2 minimum alveolar concentration (MAC) units, augmented the sustained current evoked by 3 x 10(-6) M GABA to 330-350% of control and the peak current evoked by 3 x 10(-5) M of GABA to 136-145% of control. The decay phase of the current was accelerated by the anesthetics, the time for the current to decline to 70% of the peak being reduced to 23-39% of control. In contrast, the densitized steady-state current evoked by high concentrations of GABA was decreased by anesthetics. In conclusion, general anesthetics exert a dual effect on the GABA receptor channel complex: to potentiate the nondesensitized (both peak and sustained) current and to suppress the desensitized steady-state current. The potentiation of the GABA receptor channel response may be a primary action of anesthetics leading to surgical anesthesia.     

Induction of two K+ currents by complement component C5a in mouse macrophages.

Puff application of complement component C5a (5 x 10(-8) M) onto peritoneal macrophages from thioglycollate-stimulated mice induced two kinds of outward current at a holding potential of -68 mV, a slowly-rising sustained outward current and a spike-like transient outward current. Quinidine (2 x 10(-4) M) and tetraethylammonium (10(-2) M) partially suppressed both types of outward current. Charybdotoxin (2 x 10(-6) M) markedly suppressed the spike-like outward current. Reversal potentials in bath solutions of different external K+ concentrations were dependent only on K+ concentrations. The transient current was not suppressed in Ca(2+)-free EGTA-containing solution, but was completely abolished in BAPTA-containing solution. One kind of single channel responding to C5a, which has a single-channel conductance of 29 pS, was recorded from cell-attached patches. These results suggest that C5a activates a Ca(2+)-dependent and another type of K+ current.     

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.     

Steady-state and dynamic properties of cardiac sodium-calcium exchange. Sodium-dependent inactivation

Sodium-calcium exchange current was isolated in inside-out patches excised from guinea pig ventricular cells using the giant patch method. The outward exchange current decayed exponentially upon activation by cytoplasmic sodium (sodium-dependent inactivation). The kinetics and mechanism of the inactivation were studied. (a) The rate of inactivation and the peak current amplitude were both strongly temperature dependent (Q10 = 2.2). (b) An increase in cytoplasmic pH from 6.8 to 7.8 attenuated the current decay and shifted the apparent dissociation constant (Kd) of cytoplasmic calcium for secondary activation of the exchange current from 9.6 microM to < 0.3 microM. (c) The amplitude of exchange current decreased synchronously over the membrane potential range from -120 to 60 mV during the inactivation, indicating that voltage dependence of the exchanger did not change during the inactivation process. The voltage dependence of exchange current also did not change during secondary modulation by cytoplasmic calcium and activation by chymotrypsin. (d) In the presence of 150 mM extracellular sodium and 2 mM extracellular calcium, outward exchange current decayed similarly upon application of cytoplasmic sodium. Upon removal of cytoplasmic sodium in the presence of 2-5 microM cytoplasmic free calcium, the inward exchange current developed in two phases, a fast phase within the time course of solution changes, and a slow phase (tau approximately 4 s) indicative of recovery from sodium-dependent inactivation. (e) Under zero-trans conditions, the inward current was fully activated within solution switch times upon application of cytoplasmic calcium and did not decay. (f) The slow recovery phase of inward current upon removal of cytoplasmic sodium was also present under the zero-trans condition. (g) Sodium-dependent inactivation shows little or no dependence on membrane potential in guinea pig myocyte sarcolemma. (h) Sodium-dependent inactivation of outward current is attenuated in rate and extent as extracellular calcium is decreased. (i) Kinetics of the sodium-dependent inactivation and its dependence on major experimental variables are well described by a simple two-state inactivation model assuming one fully active and one fully inactive exchanger state, whereby the transition to the inactive state takes place from a fully sodium-loaded exchanger conformation with cytoplasmic orientation of binding sites (E1.3Ni).