The Action Potentials and Currents on the I-V Plane in the Molluscan Neuron

The action potentials and the corresponding transmembrane currents, directly recorded in the F1 neuron of Helix aspersa by the Self-clamp Technique, were plotted on the I-V plane to represent the real electrical cycle of the cell membrane during activity. The membrane electrical cycle, experimentally obtained, agreed in several aspects with a similar cycle obtained from calculated data on the giant axon of Loligo, but not for the sign, with the consequence of a different localization, as far as voltage and time are concerned, of the negative impedance period. The negative impedance proved to be −614 ± 181 Ω cm² and corresponded to the late phase of the repolarization after the action potential peak. A constant positive impedance was found of 522 ± 131 Ω cm² during the ascending tract of the action potential. These two results are in contrast with previous analyses. The simultaneous availability of the conjugate voltage and current directly measured signals led to the immediate representation of the membrane total conductance in its real time course during activity, in agreement with the Hodgkin and Huxley predictive model. The peak conductance was 1.9 ± 0.7 mmho/cm² in this preparation. The electrical work spent to sustain a single active event proved to be 70 ± 19 nJ/cm². A vectorial representation of the membrane electrical activity is proposed to describe analytically the characteristic behaviour of excitable cells, as well as a new method that utilizes the only action potential to measure the threshold potential in spontaneously discharging cells. The proposed new experimental protocol, based on the use of the Self-clamp Technique, proved to be faster, easier, more productive when compared with the conventional methods; it could be used advantageously in the electrophysiological studies on excitable cells both to define the basic conditions of the investigated preparation and to directly evaluate the effects of subsequent pharmacological stimulations.     

Sodium Movements in Perfused Squid Giant Axons : Passive fluxes

Sodium movements in internally perfused giant axons from the squid Dosidicus gigas were studied with varying internal sodium concentrations and with fluoride as the internal anion. It was found that as the internal concentration of sodium was increased from 2 to 200 mM the resting sodium efflux increased from 0.09 to 34.0 pmoles/cm²sec and the average resting sodium influx increased from 42.9 to 64.5 pmoles/cm²sec but this last change was not statistically significant. When perfusing with a mixture of 500 mM K glutamate and 100 mM Na glutamate the resting efflux was 10 ± 3 pmoles/cm²sec and 41 ± 10 pmoles/cm²sec for sodium influx. Increasing the internal sodium concentration also increased both the extra influx and the extra efflux of sodium due to impulse propagation. At any given internal sodium concentration the net extra influx was about 5 pmoles/cm²impulse. This finding supports the notion that the inward current generated in a propagated action potential can be completely accounted for by movements of sodium.     

Modeling and simulation of ion channels and action potentials in taste receptor cells

Based on patch clamp data on the ionic currents of rat taste receptor cells, a mathematical model of mammalian taste receptor cells was constructed to simulate the action potentials of taste receptor cells and their corresponding ionic components, including voltage-gated Na⁺ currents and outward delayed rectifier K⁺ currents. Our simulations reproduced the action potentials of taste receptor cells in response to electrical stimuli or sour tastants. The kinetics of ion channels and their roles in action potentials of taste receptor cells were also analyzed. Our prototype model of single taste receptor cell and simulation results presented in this paper provide the basis for the further study of taste information processing in the gustatory system.     

Dynamics of chloride and potassium currents during the action potential in Chara studied with action potential clamp

TheCl^– and K⁺ currents underlying the action potential (AP) in the giant alga Chara were directly recorded with the action potential clamp method. An electrically triggered action potential was recorded and repetitively replayed as command voltage to the same cell under voltage clamp. The resulting clamp current was close to zero. Only the initial rectangular current used for stimulation was approximately reproduced by the clamp circuit. Inhibition of Cl^– channels with niflumic acid or ethacrynic acid and of K⁺ channels with Ba²⁺ evoked characteristic compensation currents because the amplifier had to add the selectively inhibited currents. Integration of the compensation currents revealed a mean flux through Cl^– and K⁺ channels of 3.3 10^–6 and 2.1 10^–6 mole M^–2 AP^–1 respectively. The dynamics of CI^– and K⁺ channel activation/inactivation were obtained by converting the relevant clamp currents to ionic permeabilities using the Goldman-Hodgkin-Katz current equation. During the AP the Cl^– permeability reaches a peak 370 ms, on average, after termination of the stimulating pulse. The following inactivation proceeds 3.6 times slower than the activation. The increase in K⁺ permeability lags behind the rise in Cl^– permeability, reaching a peak approximately 2 s after the latter.     

HCO 3 - and OH-transport across the plasmalemma ofChara

Internodal and whorl (branch) cells of the green alga,Chara corallina Klein ex Willd., em. R.D.W., were studied with the extracellular vibrating probe for measuring transmembrane ion currents, and with an extracellular pH microprobe for measuring the surface pH profile. Bands of positive inward current (OH^- efflux) 1–3 mm wide were separated by wider bands of outward current (HCO ₃ ^- influx) along the length of the cell. The measured peaks of inward current ranged from 20 to 60 A cm^-2 (98 m from the cell surface) which would correspond to a surface ionic flux of 270–800 pmol cm^-2 s^-1. The peaks of outward current (HCO ₃ ^- influx) ranged from 10 to 30 A cm^-2 which would correspond to a surface ionic flux of 140–400 pmol cm^-2 s^-1. The inward current bands matched the regions of surface alkalinity very well. The outward current (HCO ₃ ^- influx) was reduced at least 10-fold in low-HCO ₃ ^- medium, with a commensurate readjustment in the strength and pattern of inward current (OH^- efflux). (Although these experiments involved a manipulation of the external pH, it is felt that the main adjustment in current patterns was in response to the reduction in exogenous HCO ₃ ^- ). The presence of the vibrating probe perturbed the inward current region when vibrating with a 26-m amplitude, but this perturbation was eliminated when a 7-m amplitude was used. The perturbation was usually observed as a reduction in the number of inward current peaks with an increase (approximate doubling) in the amplitudes of the one or two remaining peaks. Both the inward and outward currents were light-dependent, falling off within seconds of light removal.     

Blocking action of Nephila clavata spider toxin on ionic currents activated by glutamate and its agonists in isolated hippocampal neurons

The blocking action ofNephila clavata spider neurotoxin, or JSTX, on ionic currents activated by L-glutamate and its agonists when applied to the membrane of neurons isolated from the rat hippocampus was investigated using a concentration clamp technique. Crude JSTX venom was found to block L-glutamate-, quisqualate, and kainate-activated ionic currents induced by activating non-N-methyl-D-aspartate (non-NMDA) membrane receptors. Following the effects of JSTX, ionic currents activated by L-glutamate and its agonists declined to 34–36% of their initial value with no recovery during JSTX washout. An active fraction of JSTX at concentrations of 10^–4–10^–5 produced almost total but partially reversible blockade of ionic currents. The action of JSTX became less effective during depolarization. The concentration dependence of JSTX-induced blockade of kainate-activated ionic currents was investigated and the velocity constants of interaction between the toxin and glutamate receptors obtained. It is postulated that JSTX interacts with chemically-operated non-NMDA ionic channels, blocking their transition into a number of their possible open states.A. A. Bogomolets Institute of Physiology, Academy of Sciences of the Ukrainian SSR, Kiev. Translated from Neirofiziologiya, Vol. 21, No. 2, pp. 152–160, March–April, 1989.     

Membrane potential of the unfertilized sea urchin egg

The membrane potential, specific resistance, and potassium selectivity of the unfertilized Strongylocentrotus purpuratus egg were determined by two independent methods: tracer flux and microelectrode. The potassium influx was 0.50 ± 0.2 pmole/cm²· sec, which was greater than the sodium, chloride, and calcium influxes by factors of 4, 7, and 75, respectively. By means of the constant-field equations, the flux data were used to calculate membrane potential (?70 mV) and specific resistance (420 kΩ · cm²). The effect of the external potassium concentration on the sodium influx was determined and the results closely fit the result expected if the membrane behaved as a potassium electrode. Microelectrode measurements of the potential and resistance were ?75 ± 3 mV and 380 ± kΩ · cm².     

Ionic currents of the nodal membrane underlying the fastest saltory conduction in myelinated giant nerve fibers of the shrimp Penaeus japonicus

The myelinated giant nerve fiber of the shrimp, Penaeus japonicus, is known to have the fastest velocity of saltatory impulse conduction among all nerve fibers so far studied, owing to its long distances between nodal regions and large diameter. For a better understanding of the basis of this fast conduction, a medial giant fiber of the ventral nerve cord of the shrimp was isolated, and ionic currents of its presynaptic membrane (a functional node) were examined using the sucrose-gap voltage-clamp method. Inward currents induced by depolarizing voltage pulses had a maximum value of 0.5 μA and a reversal potential of 120 mV. These currents were completely suppressed by tetrodotoxin and greatly prolonged by scorpion toxin, suggesting that they are the Na current. Both activation and inactivation kinetics of the Na current were unusually rapid in comparison with those of vertebrate nodes. According to a rough estimation of the excitable area, the density of Na current reached 500 mA/cm². In many cases, the late outward currents were induced only by depolarizing pulses larger than 50 mV in amplitude. The slope conductance measured from late currents were mostly smaller than that measured from the Na current, suggesting a low density of K channels in the synaptic membrane. These characteristics are in good harmony with the fact that the presynaptic membrane plays a role as functional node in the fastest impulse conduction of this nerve fiber.     

Voltage clamping with single microelectrodes: Comparison of the discontinuous mode and continuous mode using the Axoclamp 2A amplifier

Summary The voltage clamp technique is a powerful method for studying the physiology of excitable membrane. This technique has made possible the determination of ionic responses generated by activation of either receptor-mediated or voltage-dependent processes. The development of the whole-cell, tight-seal voltage clamp method has allowed the analysis and examination of membrane physiology at the single cell level. The method allows the characterization of voltage-dependent ionic conductances both at the macroscopic (whole-cell) and at the microscopic (unitary conductance or single channel) level in cells less than 10 µm in diameter, a feat difficult to achieve with conventional fine-tipped micropipettes.In this paper, several methologies used for culturing neuronal and non-neuronal cells in the laboratory are described. A comparison between the two modes of voltage clamp using blunt-tipped patch-microelectrodes, the switching (discontinuous) and the non-switching (continuous) modes, of the Axoclamp-2A amplifier is made. Some results on membrane currents obtained from neuronal and non-neuronal cells using the single electrode whole-cell tight-seal voltage clamp is illustrated. The possible existence of two inactivating K⁺ currents, one dependent on Ca⁺⁺ the other is not, is discussed.     

Opposite regulation of KCNQ5 and TRPC6 channels contributes to vasopressin-stimulated calcium spiking responses in A7r5 vascular smooth muscle cells

Physiologically relevant concentrations of [Arg⁸]-vasopressin (AVP) induce repetitive action potential firing and Ca²⁺ spiking responses in the A7r5 rat aortic smooth muscle cell line. These responses may be triggered by suppression of KCNQ potassium currents and/or activation of non-selective cation currents. Here we examine the relative contributions of KCNQ5 channels and TRPC6 non-selective cation channels to AVP-stimulated Ca²⁺ spiking using patch clamp electrophysiology and fura-2 fluorescence measurements in A7r5 cells. KCNQ5 or TRPC6 channel expression levels were suppressed by short hairpin RNA constructs. KCNQ5 knockdown resulted in more positive resting membrane potentials and induced spontaneous action potential firing and Ca²⁺ spiking. However physiological concentrations of AVP induced additional depolarization and increased Ca²⁺ spike frequency in KCNQ5 knockdown cells. AVP activated a non-selective cation current that was reduced by TRPC shRNA treatment or removal of external Na⁺. Neither resting membrane potential nor the AVP-induced depolarization was altered by knockdown of TRPC6 channel expression. However, both TRPC6 shRNA and removal of external Na⁺ delayed the onset of Ca²⁺ spiking induced by 25 pM AVP. These results suggest that suppression of KCNQ5 currents alone is sufficient to excite A7r5 cells, but AVP-induced activation of TRPC6 contributes to the stimulation of Ca²⁺ spiking.     

Gating currents from neuronal KV7.4 Channels: General features and correlation with the ionic conductance

The K_V7 (KCNQ) subfamily of voltage-gated K⁺ channels consists of five members (K_V7.1- K_V7.5) giving rise to non-inactivating, and slowly activating/deactivating currents mainly expressed in cardiac (K_V7.1) and neuronal (K_V7.2- K_V7.5) tissue. In the present study, using the cut-open oocyte voltage clamp, we studied the relation of the ionic currents from homomeric neuronal Kv7 channels (K_V7.2-K_V7.5) with the gating currents recorded after K⁺ conductance blockade from the same channels. Increasing the recording temperature from 18{degree sign}C to 28{degree sign}C accelerated activation/deactivation kinetics of the ionic currents in all homomeric K_V7 channels (activation Q10s at 0 mV were 3.8, 4.1, 8.3, and 2.8 for Kv7.2, Kv7.3, Kv7.4 and Kv7.5 channels, respectively), without large changes in currents voltage-dependence; moreover, at 28{degree sign}C, ionic currents carried by K_V7.4 channels also showed a significant increase in their maximal value. Gating currents were only resolved in K_V7.4 and K_V7.5 channels; the size of the ON gating charges at +40 mV was 1.34 ± 0.34 nC for K_V7.4, and 0.79 ± 0.20 nC for K_V7.5. At 28{degree sign}C, K_V7.4 gating currents had the following salient properties: 1) similar time integral of QON and QOFF, indicating no charge immobilization; 2) a left-shift in the V1/2 of the QON/V when compared to the G/V (≈ 50 mV in the presence of 2 mM extracellular Ba²⁺); 3) a QON decay faster than ionic current activation; and 4) a rising phase in the OFF gating charge after depolarizations larger than 0 mV. These observations suggest that, in K_V7.4 channels, VSD movement is followed by a slow and/or low bearing charge step linking to pore opening, a result which may help to clarify the molecular consequence of disease-causing mutations and drugs affecting channel gating.     

Changes in Cell Length During Action Potentials in Chara

Changes in cell length during excitation in Chara were recordedsimultaneously with extracellular action potentials. Cells stimulatedin artificial pond water (APW) gave a diphasic change in celllength ; that is, a transient shortening followed by a delayedextension. When a cell was stimulated 1–3 min after aprevious shortening, the extension phase was not evident, andthe amplitude of the shortening was always larger than the previousone. Cells stimulated in moist air gave shortenings with muchlarger amplitudes and much greater durations compared with thosein APW. From such marked differences in both amplitude and durationbetween the two types of shortening it is suggested that theshortening might be caused mainly by an osmotic water movementduring excitation. Net water loss during a single action potentialwas calculated from the cell shortening to be 1.076 nl cm^–2per impulse or 59800 pmol cm^–2 per impulse, which couldbe caused by a local enhancement of ionic concentration justoutside the plasmalemma of about 0.74 mN.     

Quantification of Transmembrane Currents during Action Potential Propagation in the Heart

The measurement, quantitative analysis, theory, and mathematical modeling of transmembrane potential and currents have been an integral part of the field of electrophysiology since its inception. Biophysical modeling of action potential propagation begins with detailed ionic current models for a patch of membrane within a distributed cable model. Voltage-clamp techniques have revolutionized clinical electrophysiology via the characterization of the transmembrane current gating variables; however, this kinetic information alone is insufficient to accurately represent propagation. Other factors, including channel density, membrane area, surface/volume ratio, axial conductivities, etc., are also crucial determinants of transmembrane currents in multicellular tissue but are extremely difficult to measure. Here, we provide, to our knowledge, a novel analytical approach to compute transmembrane currents directly from experimental data, which involves high-temporal (200 kHz) recordings of intra- and extracellular potential with glass microelectrodes from the epicardial surface of isolated rabbit hearts during propagation. We show for the first time, to our knowledge, that during stable planar propagation the biphasic total transmembrane current (I_m) dipole density during depolarization was ∼0.25 ms in duration and asymmetric in amplitude (peak outward current was ∼95 μA/cm² and peak inward current was ∼140 μA/cm²), and the peak inward ionic current (I_ion) during depolarization was ∼260 μA/cm² with duration of ∼1.0 ms. Simulations of stable propagation using the ionic current versus transmembrane potential relationship fit from the experimental data reproduced these values better than traditional ionic models. During ventricular fibrillation, peak I_m was decreased by 50% and peak I_ion was decreased by 70%. Our results provide, to our knowledge, novel quantitative information that complements voltage- and patch-clamp data.     

Utilization of the Vibrating Probe and Ion-Selective Microelectrode Techniques to Investigate Electrophysiological Responses to Wounding in Pea Roots

This paper examines the ionic composition of wound-induced electricalcurrents in higher plant tissue, using two non-injurious electrophysiologicaltechniques. By simultaneous recording of K⁺, H⁺ , and Ca²⁺ ionfluxes with extracellular ion-selective microelectrodes, wehave determined that a Ca²⁺ influx (2.4 µA cm^–2),a small H⁺ influx (0.17 µA cm^–2) and a large K⁺efflux (16 µA cm^–2) occur immediately after woundingin roots of Pisum sativum L. var. Greenfeast. Using an extracellularvibrating probe at the wound site, net ion currents of 26 µAcm^–2 were measured 5 min after wounding. In a more concentratedbathing medium (1/4 rather than 1/16 strength Hoagland's solution),net ion currents of 59 µA cm^–2 were measured, andthese would appear to be the largest extracellular currentsthat have been measured in plants. We made a quantitative comparisonof the summed ion fluxes with the net ion currents and thisrevealed that ion fluxes, in addition to those measured here,occur after wounding. Key words: Wounding, ion flux, electric current, calcium, potassium     

Characterization of the plasma-membrane H+-ATPase from Vicia faba guard cells

Stomatal movement is controlled by external and internal signals such as light, phytohormones or cytoplasmic Ca²⁺. Using Vicia faba L., we have studied the dose-dependent effect of auxins on the modulation of stomatal opening, mediated through the activity of the plasma-membrane H⁺-ATPase. The patch-clamp technique was used to elucidate the electrical properties of the H⁺-ATPase as effected by growth regulators and seasonal changes. The solute composition of cytoplasmic and extracellular media was selected to record pump currents directly with high resolution. Proton currents through the ATPase were characterized by a voltage-dependent increase in amplitude, positive to the resting potential, reaching a plateau at more depolarized values. Upon changes in extracellular pH, the resting potential of the cell shifted with a non-Nernst potential response (±21 mV), indicating the contribution of a depolarizing ionic conductance other than protons to the permeability of the plasma membrane. The use of selective inhibitors enabled us to identify the currents superimposing the H⁺-pump as carried by Ca²⁺. Auxinstimulation of this electroenzyme resulted in a rise in the outwardly directed H⁺ current and membrane hyperpolarization, indicating that modulation of the ATPase by the hormone may precede salt accumulation as well as volume and turgor increase. Annual cycles in pump activity (1.5–3.8 μA · cm^-2) were expressed by a minimum in pump current during January and February. Resting potentials of up to -260 mV and plasmamembrane surface area, on the other hand, did not exhibit seasonal changes. The pump activity per unit surface area was approximately 2- to 3-fold higher in guard cells than in mesophyll cells and thus correlates with their physiological demands.     

Effect of nonachlazine on transmembrane ionic currents in the frog atrial trabeculae

The effect of the antianginal drug nonachlazine displaying antiarrhythmic properties on transmembrane ionic currents in the frog atrial fibers was studied in experiments on isolated trabeculae of the frog atria. The transmembrane ionic currents were measured by a voltage clamp technique based on a double sucrose gap arrangement. Nonachlazine (1.03 X 10(-5) mol/l) decreased the amplitude of the fast inward current whatever the magnitude of membrane potential. The drug inhibited the slow inward current and prevented the adrenaline-increased permeability of the slow sodium-calcium channel if external sodium ions were replaced by choline chloride. Nonachlazine (1.03 X 10(-5) mol/l) diminished the amplitude of the inward ionic current in a calcium-free medium as well. The stimulatory effect of prostacycline (2 X 10(-7) mol/l) on the fast inward ionic current was inhibited by nonachlazine. The data obtained suggest that the antiarrhythmic effect of nonachlazine might be linked with the inhibition of the fast sodium inward current and the slow calcium inward current.     

Extracellular pH Modulates the Voltage-dependent Ca2+ Current and Low Threshold K+ Current in Hair Cells

Extracellular protons have been shown to modulate voltage-activated ionic channels. It has been proposed that synaptic modulation by exocytosed vesicular protons would be a characteristic feature of ribbon-type synapses. Type-I hair cells have a calyceal afferent junction with a diffusionally restricted synaptic cleft. These led us to study the action of extracellular pH changes on the voltage-activated Ca²⁺ and K⁺ currents evaluated using a whole-cell patch clamp in isolated cells. The amplitude of the Ca²⁺ and the K⁺ current were reduced by extracellular acidification, but without significant changes with extracellular alkalization. A shift in the voltage dependence to a more positive membrane potential was achieved at pH < 6.8. Our results shows that the presynaptic K⁺ and Ca²⁺ currents are modulated by protons, indicating that protons released along with an afferent neurotransmitter would participate as a feedback mechanism in type-I hair cells. Special issue article in honor of Dr. Ricardo Tapia.     

Chloride conductance of denervated gastrocnemius fibers from normal goats

Membrane potentials, cable parameters, and component resting ionic conductances of gastrocnemius fibers from normal goats were measured in vitro at six to 32 days following denervation by section of the tibial nerve. Denervated fibers were depolarized an average of 11.6 ± 1.5 mV (six preparations) from the control mean of 62.1 ± 1.0 mV (124 fibers) over the period studied. Fibrillation, tetrodotoxin-resistant action potentials, and anodebreak excitation were present in the denervated preparations after 13 days. The control cable parameters from 124 fibers (13 preparations) were membrane resistance, 1052 ± 70 ω·cm² and membrane capacitance, 6.2 μF/cm². In denervated fibers membrane resistance increased two to three times in the 13 to 32 day period; membrane capacitance increased about 50% in normal solution at eight to nine, 27–28, and 32 days. Myoplasmic resistivity was assumed to be 112 Ωcm. Measurements were made at 38°C. Component resting conductances were determined from the cable parameters in normal and chloride-free solution. Mean chloride conductance G_Cl and mean potassium conductance G_K of control fibers were 776 ± 49 μmhos/cm² and 175 ± 15 μmhos/cm² (92 fibers), respectively. Following denervation G_Cl increased slightly at six to nine days then fell to low values at 16 to 32 days that were close to or indistinguishable from zero. G_K increased significantly to 372 ± 40 μmhos/cm² and 499 ± 90 μmhos/cm² at 16 to 20 and 32 days, respectively. It was concluded from these findings that G_Cl and G_K of mammalian skeletal muscle are controlled by factors from the nerve and/or muscle action potentials. Goat muscle is different from frog muscle in which G_Cl does not change and G_K decreases during denervation.     

The capacitance of skeletal muscle fibers in solutions of low ionic strength

The capacitance of skeletal muscle fibers was measured by recording with one microelectrode the voltage produced by a rectangular pulse of current applied with another microelectrode. The ionic strength of the bathing solution was varied by isosmotic replacement of NaCl with sucrose, the [K] [Cl] product being held constant. The capacitance decreased with decreasing ionic strength, reaching a value of some 2 µF/cm² in solutions of 30 mM ionic strength, and not decreasing further in solutions of 15 mM ionic strength. The capacitance of glycerol-treated fibers did not change with ionic strength and was also some 2 µF/cm². It seems likely that lowering the ionic strength reduces the capacitance of the tubular system (defined as the charge stored in the tubular system), and that the 2 µF/cm² which is insensitive to ionic strength is associated with the surface membrane. The tubular system is open to the external solution in low ionic strength solutions since peroxidase is able to diffuse into the lumen of the tubules. Twitches and action potentials were also recorded from fibers in low ionic strength solutions, even though the capacitance of the tubular system was very small in these solutions. This finding can be explained if there is an action potential—like mechanism in the tubular membrane.     

Phase Plane Trajectories of the Muscle Spike Potential

To facilitate a study of the transmembrane action current, the striated muscle spike potential was recorded against its first time derivative. The specialized recording methods are described, as well as several mathematical transformations between a coordinate system in V, t, and the present coordinate system in V, dV/dt. The particular properties of the present recording method permitted an estimation for the “sodium” potential in muscle fibers at +39 mv. The maximum membrane conductance during spike production is in the order of 150 to 200 mmhos/cm². The changes in the shape of the recorded response indicate that the ionic currents and membrane conductances are reduced by Tris buffer or hypertonic Ringer's fluid. However, no marked changes in the properties of active membrane were observed when chloride ion was replaced by sulfate.