The effects of external pH on calcium channel currents in bullfrog sympathetic neurons.

We have investigated the effects of external pH (pHo) on whole-cell calcium channel currents in bullfrog sympathetic neurons. The peak inward current increased at alkaline pHo and decreased at acidic pHo. We used tail currents to distinguish effects of pHo on channel gating and permeation. There were large shifts in the voltage dependence of channel activation (approximately 40 mV between pHo and 9.0 and pHo 5.6), which could be explained by binding of H+ to surface charge according to Gouy-Chapman theory. To examine the effects of pHo on permeation, we measured tail currents at 0 mV, following steps to + 120 mV to maximally activate the channels. Unlike most previous studies, we found only a approximately 10% reduction in channel conductance from pHo 9.0 to pHo 6.4, despite a approximately 25 mV shift of channel activation. At lower pHo the channel conductance did decrease, which could be described by binding of H+ to a site with pKa = 5.1. In some cells, there was a separate slow decrease in conductance at low pHo, possibly because of changes in internal pH. These results suggest that changes in current at pHo > 6.4 result primarily from a shift in the voltage dependence of channel activation. A H(+)-binding site can explain a rapid decrease in channel conductance at lower pHo. The surface charge affecting gating has little effect on the local ion concentration near the pore, or on the channel conductance.     

A kinetic analysis of the electrogenic pump ofChara corallina: I. Inhibition of the pump by DCCD

Summary The current-voltage curve of theChara membrane was obtained by applying a slow ramp depo- and hyperpolarization by use of voltage clamp. With the progress of poisoning by DCCD (dicyclohexylcarbodiimide) theI–V curve moved by about 50 mV (depolarization) along the voltage axis, reducing its slope, and finally converged to thei _d -V curve of the passive diffusion channel. Changes ofi _p -V curve of the electrogenic pump channel could be obtained by subtracting the latter from the former.The sigmoidali _p -V curve could be simulated satisfactorily by adopting a simple reaction kinetic model. Kinetic parameters of the successive changes of state of the H⁺ ATPase could be evaluated. Changes of these kinetic parameters during inhibition gave useful information about the molecular mechanism of the electrogenic pump.Depolarization of the membrane potential, decrease of membrane conductance, and decrease of pump current during inhibition of the pump with DCCD are caused mainly by the decrease of conductance of the pump channel. The decrease of this pump conductance is caused principally by a marked decrease of the rate constant for releasing H⁺ to the outside.     

ATP inhibition and rectification of a Ca2+-activated anion channel in sarcoplasmic reticulum of skeletal muscle.

We describe ATP-dependent inhibition of the 75-105-pS (in 250 mM Cl-) anion channel (SCl) from the sarcoplasmic reticulum (SR) of rabbit skeletal muscle. In addition to activation by Ca2+ and voltage, inhibition by ATP provides a further mechanism for regulating SCl channel activity in vivo. Inhibition by the nonhydrolyzable ATP analog 5'-adenylylimidodiphosphate (AMP-PNP) ruled out a phosphorylation mechanism. Cytoplasmic ATP (approximately 1 mM) inhibited only when Cl- flowed from cytoplasm to lumen, regardless of membrane voltage. Flux in the opposite direction was not inhibited by 9 mM ATP. Thus ATP causes true, current rectification in SCl channels. Inhibition by cytoplasmic ATP was also voltage dependent, having a K(I) of 0.4-1 mM at -40 mV (Hill coefficient approximately 2), which increased at more negative potentials. Luminal ATP inhibited with a K(I) of approximately 2 mM at +40 mV, and showed no block at negative voltages. Hidden Markov model analysis revealed that ATP inhibition 1) reduced mean open times without altering the maximum channel amplitude, 2) was mediated by a novel, single, voltage-independent closed state (approximately 1 ms), and 3) was much less potent on lower conductance substates than the higher conductance states. Therefore, the SCl channel is unlikely to pass Cl- from cytoplasm to SR lumen in vivo, and balance electrogenic Ca2+ uptake as previously suggested. Possible roles for the SCl channel in the transport of other anions are discussed.     

Ionic selectivity, saturation, and block in a K+-selective channel from sarcoplasmic reticulum

The open-channel conductance properties of a voltage-gated channel from sarcoplasmic reticulum were studied in planar phospholipid membranes. The channel is ideally selective for K+ over Cl- and for K+ over Ca++. In symmetrical 1 M solutions, the single-channel conductance (in pmho) falls in the order: K+ (214) > NH4+ (157) > Rb+ (125) > Na+ (72) > La+ (8.1) > Cs+ (< 3). In neutral bilayers, the channel conductance saturates with ion activity according to a rectangular hyperbolic relation, with half-saturation activities of 54 mM for K+ and 34 mM for Na+. Under symmetrical salt conditions, the K+:Na+ channel conductance ratio increases with salt activity, but the permeability ratio, measured by single-channel bi-ionic potentials, is constant between 20 mM and 2.5 M salt; the permeability ratio is equal to the conductance ratio in the limit of low-salt concentration. The channel conductance varies < 5% in the voltage range -100 to +70 mV. The maximum conductance varies K+ and Na+ is only weakly temperature dependent (delta H++ = 4.6 and 5.3 kcal/mol, respectively), but that of Li+ varies strongly with temperature (delta H++ = 13 kcal/mol). The channel's K+ conductance is blocked asymmetrically by Cs+, and this block is competitive with K+. The results are consistent with an Eyring-type barriers as it permeates the channel. The data conform to Lüger's (1973. Biochem. Biophys. Acta. 311:423-441) predictions for a "pure" single-ion channel.     

K+-selective channel from sarcoplasmic reticulum of split lobster muscle fibers

The patch clamp technique has been used to study channels in a membrane inside a cell. A single muscle fiber is skinned in relaxing saline (high K+, low Ca2+ with EGTA and ATP), leaving the native sarcoplasmic reticulum (SR) membrane exposed for patching. Fibers are dissected from the second antenna remotor muscles of the American lobster, Homarus americanus. Transmission and scanning electron microscopy confirm the large volume fraction of SR (approximately 70%) and absence of sarcolemma in this unusual skinned preparation. The resting potential of the SR was measured after the resistance of the patch of membrane was broken down. It is near 0 mV (-0.4 +/- 0.6 mV). The average input resistance of the SR is 842 +/- 295 M omega. Some 25% of patches contain a K+-selective channel with a mean open time of seconds and the channel displays at least two conducting states. The open probability is weakly voltage dependent, large at zero and positive potentials (cytoplasm minus SR lumen), and decreasing at negative potentials. The maximal conductance of this channel is 200 +/- 1 pS and the substate conductance is 170 +/- 3 pS in symmetrical 480 mM K+ solution. The current-voltage relation of the open channel is linear over a range of +/- 100 mV. The selectivity is similar to the SR K+ channel of vertebrates: PK/PNa is 3.77 +/- 0.03, determined from reversal potential measurements, whereas gamma K/gamma Na is 3.28 +/- 0.06, determined from open-channel conductance measurements in symmetrical 480 mM solutions. Voltage-dependent block in the lobster SR K+ channel is similar to, but distinct from, that reported for the vertebrate channels. It occurs asymmetrically when hexamethonium is added to both sides of the membrane. The block is more effective from the cytoplasmic side of the channel.     

Use of weak acids to determine the bulk diffusion limitation of H+ ion conductance through the gramicidin channel.

The addition of 2 M formic acid at pH 3.75 increased the single channel H+ ion conductance of gramicidin channels 12-fold at 200 mV. Other weak acids (acetic, lactic, oxalic) produce a similar, but smaller increase. Formic acid (and other weak acids) also blocks the K+ conductance at pH 3.75, but not at pH 6.0 when the anion form predominates. This increased H+ conductance and K+ block can be explained by formic acid (HF) binding to the mouth of the gramicidin channel (Km = 1 M) and providing a source of H+ ions. A kinetic model is derived, based on the equilibrium binding of formic acid to the channel mouth, that quantitatively predicts the conductance for different mixtures of H+, K+, and formic acid. The binding of the neutral formic acid to the mouth of the gramicidin channel is directly supported by the observation that a neutral molecule with a similar structure, formamide (and malonamide and acrylamide), blocks the K+ conductance at pH 6.0. The H+ conductance in the presence of formic acid provides a lower bound for the intrinsic conductance of the gramicidin channel when there is no diffusion limitation at the channel mouth. The 12-fold increase in conductance produced by formic acid suggests that greater than 90% of the total resistance to H+ results from diffusion limitation in the bulk solution.     

Membrane transport in stomatal guard cells: The importance of voltage control

Potassium uptake and export in the resting conditions and in response to the phytohormone abscisic acid (ABA) were examined under voltage clamp in guard cells of Vicia faba L. In 0.1 mM external K+ (with 5 mM Ca2(+)-HEPES, pH 7.4) two distinct transport states could be identified based on the distribution of the free-running membrane voltage (VM) data in conjunction with the respective I-V and G-V relations. One state was dominated by passive diffusion (mean VM = -143 +/- 4 mV), the other (mean VM = -237 +/- 10 mV) exhibited an appreciable background of primary H+ transport activity. In the presence of pump activity the free-running membrane voltage was negative of the respective K+ equilibrium potential (EK+), in 3 and 10 mM external K+. In these cases VM was also negative of the activation voltage for the inward rectifying K+ current, thus creating a strong bias for passive K+ uptake through inward-rectifying K+ channels. In contrast, when pump activity was absent VM was situated positive of EK+ and cells revealed a bias for K+ efflux. Occasionally spontaneous voltage transitions were observed during which cells switched between the two states. Rapid depolarizations were induced in cells with significant pump activity upon adding 10 microM ABA to the medium. These depolarizations activated current through outward-rectifying K+ channels which was further amplified in ABA by a rise in the ensemble channel conductance. Current-voltage characteristics recorded before and during ABA treatments revealed concerted modulations in current passage through at least four distinct transport processes, results directly comparable to one previous study (Blatt, M.R., 1990, Planta 180:445) carried out with guard cells lacking detectable primary pump activity. Comparative analyses of guard cells in each case are consistent with depolarizations resulting from the activation of an inward-going, as yet unidentified current, rather than an ABA-induced fall in H(+)-ATPase output. Also observed in a number of cells was an inward-directed current which activated in ABA over a narrow range of voltages positive of -150 mV; this and additional features of the current suggest that it may reflect the ABA-dependent activation of an anion channel previously characterized in Vicia guard cell protoplasts, but rule out its function as the primary mechanism for initial depolarization.(ABSTRACT TRUNCATED AT 400 WORDS)     

An outward-rectifying potassium channel in primary cultures of sweat glands from cystic fibrosis subjects

We have previously described a high conductance calcium-activated 'maxi K' channel in primary cultures of human eccrine sweat gland cells both from normal subjects and those with cystic fibrosis. In further studies we have now identified a potassium-selective channel of much lower conductance which shows outward-rectification and which is present in sweat glands isolated from cystic fibrosis subjects. In experiments with inside-out patches using symmetrical pipette and bath solutions containing 140 mM K+ the channel showed an outward slope conductance (at +50 mV) of approximately 26 pS and an inward conductance (at -50 mV) of approximately 11 pS. When K+ in the bath was replaced by Na+ the reversal potential shifts to reveal a permeability ratio PK/PNa approximately 40 Unlike the maxi-K+ channel, the outward-rectifying channel does not show sensitivity to Ca2+. Channels were found in cells cultured from the glands of four out of five cystic fibrosis subjects. In cells cultured from 30 subjects who did not have cystic fibrosis, an outward-rectifying potassium channel was seen in only one out of approximately 3000 patches.     

Conduction and blocking properties of a predominantly anion-selective channel from human platelet surface membrane reconstituted into planar phospholipid bilayers

We have investigated the basic properties of a predominantly anion-selective channel derived from highly purified human platelet surface membrane. Single channels have been reconstituted into planar phospholipid bilayers by fusion of membrane vesicles and recorded under voltage-clamp conditions. The channel is found to have the following properties: (i) Channel activity occurs in bursts of openings separated by long closed periods. (ii) The current-voltage relationship is nonlinear. Channel current is seen to rectify, with less current flowing at positive than at negative voltages. Rectification may be due to asymmetric block by HEPES/Tris buffers. In 450 mM KCl, 5 mM HEPES/Tris, pH 7.2, the single channel conductance at -40 mV is approximately 160 pS and at +40 mV is approximately 90 pS. (iii) The conductance-concentration relationship follows a simple saturation curve. Half maximal conductance is achieved at a concentration of approximately 1000 mM KCl, and the curve saturates at a conductance of approximately 500 pS. (iv) Reversal potentials interpreted in terms of the Goldman-Hodgkin-Katz equation indicate a Cl: K permeability ratio of 4:1. (v) The channel accepts all of the halides as well as a number of other anions. The following sequence of relative anion permeabilities (in the presence of K+) is obtained: F- less than acetate- less than gluconate- less than Cl- less than Br- less than I- less than NO3- less tha SCN-.(vi) Cations as large as TEA+ are permeant. (vii) Current through the channel is blocked in the presence of DIDS, SITS and ATP, but not by Zn2+.     

Voltage- and time-dependent K+ channel currents in the basolateral membrane of villus enterocytes isolated from guinea pig small intestine

Patch-clamp studies were carried out in villus enterocytes isolated from the guinea pig proximal small intestine. In the whole-cell mode, outward K+ currents were found to be activated by depolarizing command pulses to -45 mV. The activation followed fourth order kinetics. The time constant of K+ current activation was voltage-dependent, decreasing from approximately 3 ms at -10 mV to 1 ms at +50 mV. The K+ current inactivated during maintained depolarizations by a voltage- independent, monoexponential process with a time constant of approximately 470 ms. If the interpulse interval was shorter than 30 s, cumulative inactivation was observed upon repeated stimulations. The steady state inactivation was voltage-dependent over the voltage range from -70 to -30 mV with a half inactivation voltage of -46 mV. The steady state activation was also voltage-dependent with a half- activation voltage of -22 mV. The K+ current profiles were not affected by chelation of cytosolic Ca2+. The K+ current induced by a depolarizing pulse was suppressed by extracellular application of TEA+, Ba2+, 4-aminopyridine or quinine with half-maximal inhibitory concentrations of 8.9 mM, 4.6 mM, 86 microM and 26 microM, respectively. The inactivation time course was accelerated by quinine but decelerated by TEA+, when applied to the extracellular (but not the intracellular) solution. Extracellular (but not intracellular) applications of verapamil and nifedipine also quickened the inactivation time course with 50% effective concentrations of 3 and 17 microM, respectively. Quinine, verapamil and nifedipine shifted the steady state inactivation curve towards more negative potentials. Outward single K+ channel events with a unitary conductance of approximately 8.4 pS were observed in excised inside-out patches of the basolateral membrane, when the patch was depolarized to -40 mV. The ensemble current rapidly activated and thereafter slowly inactivated with similar time constants to those of whole-cell K+ currents. It is concluded that the basolateral membrane of guinea pig villus enterocytes has a voltage-gated, time-dependent, Ca(2+)-insensitive, small-conductance K+ channel. Quinine, verapamil, and nifedipine accelerate the inactivation time course by affecting the inactivation gate from the external side of the cell membrane.     

Depolarization increases the single-channel conductance and the open probability of crayfish glutamate channels.

We have studied the voltage sensitivity of glutamate receptors in outside-out patches taken from crayfish muscles. We found that single-channel conductance, measured directly at the single-channel level, increases as depolarization rises. At holding potentials from -90 mV to approximately 20 mV, the conductance is 109 pS. At holding potentials positive to 20 mV, the conductance is 213 pS. This increase in single-channel conductance was also observed in cell-attached patches. In addition, desensitization, rise time, and the dose-response curve were all affected by depolarization. To further clarify these multifaceted effects, we evaluated the kinetic properties of single-channel activity recorded from cell-attached patches in hyperpolarization (membrane potential around -75 mV) and depolarization (membrane potential approximately 105 mV). We found that the glutamate dissociation rate constant (k_) was affected most significantly by membrane potential; it declined 6.5-fold under depolarization. The rate constant of channel closing (k(c)) was also significantly affected; it declined 1.8-fold. The rate constant of channel opening (k(o)) declined only 1.2-fold. The possible physiological significance of the depolarization-mediated changes in the above rate constants is discussed.     

Purified ryanodine receptor from skeletal muscle sarcoplasmic reticulum is the Ca2+-permeable pore of the calcium release channel

The ryanodine receptor of rabbit skeletal muscle sarcoplasmic reticulum was purified by immunoaffinity chromatography as a single approximately 450,000-Da polypeptide and it was shown to mediate single channel activity identical to that of the ryanodine-treated Ca2+ release channel of the sarcoplasmic reticulum. The purified receptor had a [3H]ryanodine binding capacity (Bmax) of 280 pmol/mg and a binding affinity (Kd) of 9.0 nM. [3H]Ryanodine binding to the purified receptor was stimulated by ATP and Ca2+ with a half-maximal stimulation at 1 mM and 8-9 microM, respectively. [3H]Ryanodine binding to the purified receptor was inhibited by ruthenium red and high concentrations of Ca2+ with an IC50 of 2.5 microM and greater than 1 mM, respectively. Reconstitution of the purified receptor in planar lipid bilayers revealed the Ca2+ channel activity of the purified receptor. Like the native sarcoplasmic reticulum Ca2+ channels treated with ryanodine, the purified receptor channels were characterized by (i) the predominance of long open states insensitive to Mg2+ and ruthenium red, (ii) a main slope conductance of approximately 35 pS and a less frequent 22 pS substate in 54 mM trans-Ca2+ or Ba2+, and (iii) a permeability ratio PBa or PCa/PTris = 8.7. The approximately 450,000-Da ryanodine receptor channel thus represents the long-term open "ryanodine-altered" state of the Ca2+ release channel from sarcoplasmic reticulum. We propose that the ryanodine receptor constitutes the physical pore that mediates Ca2+ release from the sarcoplasmic reticulum of skeletal muscle.     

Ca2+ currents in cerebral artery smooth muscle cells of rat at physiological Ca2+ concentrations

Single Ca2+ channel and whole cell currents were measured in smooth muscle cells dissociated from resistance-sized (100-microns diameter) rat cerebral arteries. We sought to quantify the magnitude of Ca2+ channel currents and activity under the putative physiological conditions of these cells: 2 mM [Ca2+]o, steady depolarizations to potentials between -50 and -20 mV, and (where possible) without extrinsic channel agonists. Single Ca2+ channel conductance was measured over a broad range of Ca2+ concentrations (0.5-80 mM). The saturating conductance ranged from 1.5 pS at 0.5 mM to 7.8 pS at 80 mM, with a value of 3.5 pS at 2 mM Ca (unitary currents of 0.18 pA at -40 mV). Both single channel and whole cell Ca2+ currents were measured during pulses and at steady holding potentials. Ca2+ channel open probability and the lower limit for the total number of channels per cell were estimated by dividing the whole-cell Ca2+ currents by the single channel current. We estimate that an average cell has at least 5,000 functional channels with open probabilities of 3.4 x 10(-4) and 2 x 10(-3) at -40 and -20 mV, respectively. An average of 1-10 (-40 mV and -20 mV, respectively) Ca2+ channels are thus open at physiological potentials, carrying approximately 0.5 pA steady Ca2+ current at -30 mV. We also observed a very slow reduction in open probability during steady test potentials when compared with peak pulse responses. This 4- 10-fold reduction in activity could not be accounted for by the channel's normal inactivation at our recording potentials between -50 and -20 mV, implying that an additional slow inactivation process may be important in regulating Ca2+ channel activity during steady depolarization.     

Anion permeation in an apical membrane chloride channel of a secretory epithelial cell

Single channel currents though apical membrane Cl channels of the secretory epithelial cell line T84 were measured to determine the anionic selectivity and concentration dependence of permeation. The current-voltage relation was rectified with single channel conductance increasing at positive potentials. At 0 mV the single channel conductance was 41 +/- 2 pS. Permeability, determined from reversal potentials, was optimal for anions with diameters between 0.4 and 0.5 nm. Anions of larger diameter had low permeability, consistent with a minimum pore diameter of 0.55 nm. Permeability for anions of similar size was largest for those ions with a more symmetrical charge distribution. Both HCO3 and H2PO4 had lower permeability than the similar-sized symmetrical anions, NO3 and ClO4. The permeability sequence was SCN greater than I approximately NO3 approximately ClO4 greater than Br greater than Cl greater than PF6 greater than HCO3 approximately F much greater than H2PO4. Highly permeant anions had lower relative single channel conductance, consistent with longer times of residence in the channel for these ions. The conductance sequence for anion efflux was NO3 greater than SCN approximately ClO4 greater than Cl approximately I approximately Br greater than PF6 greater than F approximately HCO3 much greater than H2PO4. At high internal concentrations, anions with low permeability and conductance reduced Cl influx consistent with block of the pore. The dependence of current on Cl concentration indicated that Cl can also occupy the channel long enough to limit current flow. Interaction of Cl and SCN within the conduction pathway is supported by the presence of a minimum in the conductance vs. mole fraction relation. These results indicate that this 40-pS Cl channel behaves as a multi-ion pathway in which other permeant anions could alter Cl flow across the apical membrane.     

Heterogeneity of conductance states in calcium channels of skeletal muscle

The single channel conductance of the dihydropyridine (DHP)-sensitive calcium channel from rabbit skeletal muscle transverse tubules was analyzed in detail using the planar bilayer recording technique. With 0.1 M BaCl2 on both sides of the channel (symmetrical solutions), the most frequent conductance is 12 pS, which is independent of holding potential in the range of -80 to +80 mV. This conductance accounts for approximately 80% of all openings analyzed close to 0 mV. Two additional channels of conductance 9 and 3 pS are also present at all positive potentials, but their relative occurrence close to 0 mV is low. All channels depend on the presence of agonist Bay K 8644 and are inhibited by the antagonist nitrendipine. The relative occurrence of 9 and 3 pS can be increased, and that of 12 pS decreased, by several interventions such as external addition of cholesterol, lectin (wheat germ agglutinin), or calmodulin inhibitor R24571 (calmidazolium). The 9- and 3-pS channels are also conspicuous at positive potentials larger than +40 mV. We suggest that 9- and 3-pS channels are two elementary conductances of the same DHP-sensitive Ca channel. Under most circumstances, these two conductances are gated in a coupled way to generate a channel with a unitary conductance of 12 pS. Interventions tested, including large depolarizations, probably decompose or uncouple the 12-pS channel into 9 and 3 pS.     

Regulation of the hyperpolarization-activated K+ channel in the lateral membrane of the cortical collecting duct [published erratum appears in J Gen Physiol 1995 Sep;106(3):579]

An intermediate-conductance K+ channel (I.K.), the activity of which is increased by hyperpolarization, was previously identified in the lateral membrane of the cortical collecting duct (CCD) of the rat kidney (Wang, W. H., C. M. McNicholas, A. S. Segal, and G. Giebisch. 1994. American Journal of Physiology. 266:F813-F822). The biophysical properties and regulatory mechanisms of this K+ channel have been further investigated with patch clamp techniques in the present study. The slope conductance of the channel in inside-out patches was 50 pS with 140 mM KCl in the pipette and 5 mM KCl, 140 mM NaCl (NaCl Ringer''s solution) in the bath. Replacement of the bath solution with symmetrical 140 mM KCl solution changed the slope conductance of the channel to 85 pS and shifted the reversal potential by 55 mV, indicating that the selectivity ratio of K+/Na+ was at least 10:1. Channel open probability (Po) in inside-out patches was 0.12 at 0 mV and was increased by hyperpolarization. The voltage-dependent Po was fitted with the Boltzmann''s equation: Po = 1/[1 + exp(V-V1/2)zF/RT], with z = 1.2 and V1/2 = -40 mV. Addition of 2 mM tetraethylammonium or 500 mM quinidine to the bath blocked the activity of the K+ channel in inside-out patches. In addition, decrease in the bath pH from 7.40 to 6.70 reduced Po by 30%. Addition of the catalytic subunit of protein kinase A (PKAc; 20 U/ml) and 100 microM [corrected] MgATP to the bath increased Po from 0.12 to 0.49 at 0 mV and shifted the voltage dependence curve of channel activity toward more positive potentials by 40 mV. Two exponentials were required to fit both the open-time and the closed-time histograms. Addition of PKAc increased the long open-time constant and shortened the long closed-time constant. In conclusion, PKA-mediated phosphorylation plays an important role in the regulation of the voltage dependence of the hyperpolarization-activated K+ channel in the basolateral membrane of CCD.     

Calcium channel currents in pars intermedia cells of the rat pituitary gland. Kinetic properties and washout during intracellular dialysis

Ca channel currents in primary cultured pars intermedia cells were studied using whole-cell recording with patch pipettes. Experiments were carried out at 18-21 degrees C in cells internally dialyzed with K-free, EGTA-containing solutions and in the presence of 10 mM Ca or 10 mM Ba in the external solution. Ca and Ba currents depended on the activity of two main populations of channels, SD and FD. With Ca as the charge carrier, these two populations differed in their closing time constants at -80 mV (SD, 1.8 ms; FD, 110 microseconds), apparent activation levels (SD, -40 mV; FD, -5 mV), half-maximal activation levels (SD, +5 to +10 mV; FD, +20 to +25 mV), half-times of activation at +20 mV (SD, 2.5-3.5 ms; FD, 1.0-1.3 ms), and time courses of inactivation (SD, fast; FD, slow). Functional FD channels were almost completely lost within 20-25 min of breaking into a cell, whereas SD channels retained most of their functional activity. In addition, the conductance-voltage curve for FD channels shifted approximately 15 mV toward more negative membrane potentials within 11-14 min under whole-cell recording. At that time, 60-70% of the FD channel maximum conductance was lost. However, the conductance-voltage curve for SD channels shifted less than 5 mV within 25 min. The addition of 3 mM MgATP and 40 microM GTP to the internal solution slowed down the loss of FD channels and prevented the shift in their activation curve. It was also found that the amplitude of the current carried by FD channels tends to increase as a function of the age of the culture, with no obvious changes in the kinetic properties of the channels or in SD channel activity.     

A kinetic analysis of the electrogenic pump ofChara corallina: III. Pump activity during action potential

Summary The current-voltage curve (I–V curve) of theChara membrane was obtained by applying a slow ramp hyper- and depolarization by use of voltage clamp. By inhibiting the electrogenic pump with 50m DCCD (dicyclohexylcarbodiimide), theI–V curve approached a steadyI–V curve within two hours, which gave thei _d -V curve of the passive diffusion channel. Thei _p -V curve of the electrogenic pump channel was obtained by subtracting the latter from the former. The sigmoidali _p -V curve could be simulated satisfactorily with a simple reaction kinetic model which assumes a stoichiometric ratio of 2. The emf of the pump (E _p ) is given as the voltage at which the pump current changes its sign. The conductance of the pump (g _p ) can be calculated as the chord conductance from thei _p -V curve, which is highly voltage dependent having a peak at a definite voltage. The changes of emf and conductance during excitation were determined by use of the current clamp (I=0). Since theE _p andg _p (V) are known, the changes, during excitation, of emf (E _d ) and conductance (g _d ) of the passive diffusion channel can be calculated. The marked increase of the membrane conductance and the large depolarization during the action potential are caused by the marked increase of the conductance of the passive diffusion channel and the large depolarization of its emf. The conductance of the electrogenic pump decreases to about half at the peak of action potential, while the pump current increases almost to a saturated level.     

Neuronal membrane potential is mildly depolarized in the anoxic turtle cortex

Neuronal membrane potential (E_m) regulates the activity of excitatory voltage-sensitive channels. Anoxic insults lead to a severe loss of E_m and excitotoxic cell death (ECD) in mammalian neurons. Conversely, anoxia-tolerant freshwater turtle neurons depress energy usage during anoxia by altering ionic conductance to reduce neuronal excitability and ECD is avoided. This wholesale alteration of ion channel and pump activity likely has a significant effect on E_m. Using the whole-cell patch clamp technique we recorded changes in E_m from turtle cortical neurons during a normoxic to anoxic transition in the presence of various ion channel/pump modulators. E_m did not change with normoxic perfusion but underwent a reversible, mild depolarization of 8.1 ± 0.2 mV following anoxic perfusion. This mild anoxic depolarization (MAD) was not prevented by the manipulation of any single ionic conductance, but was partially reduced by pre-treatment with antagonists of GABA_A receptors (5.7 ± 0.5 mV), cellular bicarbonate production (5.3 ± 0.2 mV) or K⁺ channels (6.0 ± 0.2 mV), or by perfusion of reactive oxygen species scavengers (5.2 ± 0.3 mV). Furthermore, all of these treatments induced depolarization in normoxic neurons. Together these data suggest that the MAD may be due to the summation of numerous altered ion conductance states during anoxia.