Development and Function of the Voltage-Gated Sodium Current in Immature Mammalian Cochlear Inner Hair Cells

Inner hair cells (IHCs), the primary sensory receptors of the mammalian cochlea, fire spontaneous Ca²⁺ action potentials before the onset of hearing. Although this firing activity is mainly sustained by a depolarizing L-type (Ca_V1.3) Ca²⁺ current (I _Ca), IHCs also transiently express a large Na⁺ current (I _Na). We aimed to investigate the specific contribution of I _Na to the action potentials, the nature of the channels carrying the current and whether the biophysical properties of I _Na differ between low- and high-frequency IHCs. We show that I _Na is highly temperature-dependent and activates at around −60 mV, close to the action potential threshold. Its size was larger in apical than in basal IHCs and between 5% and 20% should be available at around the resting membrane potential (−55 mV/−60 mV). However, in vivo the availability of I _Na could potentially increase to >60% during inhibitory postsynaptic potential activity, which transiently hyperpolarize IHCs down to as far as −70 mV. When IHCs were held at −60 mV and I _Na elicited using a simulated action potential as a voltage command, we found that I _Na contributed to the subthreshold depolarization and upstroke of an action potential. We also found that I _Na is likely to be carried by the TTX-sensitive channel subunits Na_V1.1 and Na_V1.6 in both apical and basal IHCs. The results provide insight into how the biophysical properties of I _Na in mammalian cochlear IHCs could contribute to the spontaneous physiological activity during cochlear maturation in vivo.     

Maturation and fertilization of the sea urchin oocyte: An electrophysiological study

Some electrical properties of the sea urchin oocyte during germinal vesicle breakdown (GVBD) and fertilization have been studied using two intracellular electrodes. Oocytes with distinct germinal vesicles have resting potentials of ?70 to ?90 mV and the specific membrane resistance may range from 3 to 10 kΩ·cm². Around rest the I–V relationship is concave toward the axis origin and the membrane is K⁺ selective. A second electrical state, of lower potential and higher resistance, preexists in the membrane. Following GVBD, the K⁺-selective system is lost and the oocyte attains the characteristics of the second state with a resting potential of ?10 to ?50 mV and specific membrane resistance of 10–50 kΩ·cm². At rest the I–V relationship tends to be convex toward the axis origin. The majority of sea urchin eggs (which have undergone GVBD and completed meiosis) have a resting state of ?10 to ?30 mV; 10–50 kΩ·cm². The I–V relationship around rest is convex toward the axis origin and the resting potential is sensitive to changes of Na⁺, Cl^?, and K⁺ in the external medium. There is probably no major change in the electrical properties of the oocyte during the completion of meiosis. A small percentage of eggs from suboptimal animals have high resting potentials of ?70 to ?90 mV and specific membrane resistance of 5–50 kΩ·cm². Such eggs have predominantly K⁺-selective membranes and we suggest that they are either underripe or aged. The first electrical event across the egg plasma membrane during fertilization is a step-like depolarization which occurs about 2 sec after the attachment of the fertilizing spermatozoon to the vitelline layer. There is no change—at the level of the light microscope—either in the egg surface or in the behavior of the spermatozoon until the second event, the fertilization potential (FP), is initiated 11 sec later. The cortical reaction occurs simultaneously with the FP and during the rising phase of the FP the spermatozoon stops gyrating around its point of attachment. Oocytes, which do not have cortical granules, upon insemination exhibit step events but no FP; in contrast artificially activated eggs, either spontaneous or induced by the ionophore A23187, give rise to only the FP. We suggest that the FP is the electrical result of the modification of the egg plasma membrane during cortical exocytosis.     

The influence of different membrane components on the electrical stability of bilayer lipid membranes

A good understanding of cell membrane properties is crucial for better controlled and reproducible experiments, particularly for cell electroporation where the mechanism of pore formation is not fully elucidated. In this article we study the influence on that process of several constituents found in natural membranes using bilayer lipid membranes. This is achieved by measuring the electroporation threshold (V_th) defined as the potential at which pores appear in the membrane. We start from highly stable 1,2-diphytanoyl-sn-glycero-3-phosphocholine (DPhPC) membranes (V_th ∼ 200 mV), and subsequently add therein other phospholipids, cholesterol and a channel protein. While the phospholipid composition has a slight effect (100 mV ≤ V_th ≤ 290 mV), cholesterol gives a concentration-dependent effect: a slight stabilization until 5% weight (V_th ∼ 250 mV) followed by a noticeable destabilization (V_th ∼ 100 mV at 20%). Interestingly, the presence of a model protein, α-hemolysin, dramatically disfavours membrane poration and V_th shows a 4-fold increase (∼ 800 mV) from a protein density in the membrane of 24 × 10^− 3 proteins/μm². In general, we find that pore formation is affected by the molecular organization (packing and ordering) in the membrane and by its thickness. We correlate the resulting changes in molecular interactions to theories on pore formation.     

Single-Channel Analysis of a Delayed Rectifier K+ Channel in Xenopus Myelinated Nerve

Single-channel properties of a delayed rectifier voltage-gated K⁺ channel (I-type) were investigated in peripheral myelinated axons from Xenopus laevis. Channels activated between −60 and −40 mV with a potential of half-maximal activation, E₅₀, at −47.5 mV. Averaged single-channel currents activated with a time delay at all membrane potentials tested. Time to half-maximal activation decreased from 80 to 1.6 msec between −60 and +40 mV. The channel inactivated monoexponentially with a time constant of 10.9 sec at −40 mV. The time constant of deactivation was 126 msec at −80 mV and 16.9 msec at −110 mV. In symmetrical 105 mm K⁺, the single-channel conductance (γ) was 22 and 13 pS at negative and positive membrane potentials, respectively, at 13–15°C. In Na⁺-rich solution with 2.5 mm extracellular K⁺γ was 7 pS and the reversal potential was negative to −80 mV, indicating a high selectivity for K⁺ over Na⁺. γ depended on extracellular K⁺ concentration (K _D = 19.6 mm) and temperature (Q ₁₀= 1.45). External tetraethylammonium (TEA) reduced the apparent single-channel current amplitude at all potentials tested with a half-maximal inhibiting concentration (IC₅₀) of 0.6 mm. Open probability of the channel, but not single-channel current amplitude was decreased by extracellular dendrotoxin (DTX, IC₅₀= 6.8 nm) and mast cell degranulating peptide (MCDP, IC₅₀= 41.9 nm). In Ringer solution the membrane potential of macroscopic I-channel patches was about −65 mV and depolarized under TEA and DTX. It is concluded that besides their activation during action potentials, I-channels may also stabilize the resting membrane potential. Received: 2 June 1995/Revised: 13 October 1995     

Redox potentials of the oriented film of the wild-type, the E194Q-, E204Q- and D96N-mutated bacteriorhodopsins

The redox potentials of the oriented films of the wild-type, the E194Q-, E204Q- and D96N-mutated bacteriorhodopsins (bR), prepared by adsorbing purple membrane (PM) sheets or its mutant on a Pt electrode, have been examined. The redox potentials (V) of the wild-type bR were −470 mV for the 13-cis configuration of the retinal Shiff base in bR and −757 mV for the all-trans configuration in H₂O, and −433 mV for the 13-cis configuration and −742 mV for the all-trans configuration in D₂O. The solvent isotope effect (ΔV=V(D₂O)−V(H₂O)), which shifts the redox potential to a higher value, originates from the cooperative rearrangements of the extensively hydrogen-bonded water molecules around the protonated CN part in the retinal Schiff base. The redox potential of bR was much higher for the 13-cis configuration than that for the all-trans configuration. The redox potentials for the E194Q mutant in the extracellular region were −507 mV for the 13-cis configuration and −788 mV for the all-trans configuration; and for the E204Q mutant they were −491 mV for the 13-cis configuration and −769 mV for the all-trans configuration. Replacement of the Glu¹⁹⁴ or Glu²⁰⁴ residues by Gln weakened the electron withdrawing interaction to the protonated CN bond in the retinal Schiff base. The E204 residue is less linked with the hydrogen-bonded network of the proton release pathway compared with E194. The redox potentials of the D96N mutant in the cytoplasmic region were −471 mV for the 13-cis configuration and −760 mV for the all-trans configuration which were virtually the same as those of the wild-type bR, indicating that the D to N point mutation of the 96 residue had no influence on the interaction between the D96 residue and the CN part in the Schiff base under the light-adapted condition. The results suggest that the redox potential of bR is closely correlated to the hydrogen-bonded network spanning from the retinal Schiff base to the extracellular surface of bR in the proton transfer pathway.     

Single-channel analysis of the anion channel-forming protein from the plant pathogenic bacterium Clavibacter michiganense ssp. nebraskense

The anion channel protein from Clavibacter michiganense ssp. nebraskense (Schürholz, Th. et al. 1991, J. Membrane Biol. 123: 1-8) was analyzed at different concentrations of KCl and KF. At 0.8 M KCl the conductance G(V_m) increases exponentially from 21 pS at 50 mV up to 53 pS at V_m = 200 mV, 20°C. The concentration dependence of G(V_m) corresponds to a Michaelis-Menten type saturation function at all membrane voltage values applied (0-200 mV). The anion concentration K_0.5, where G(V_m) has its half-maximum value, increases from 0.12 M at 50 mV to 0.24 M at 175 mV for channels in a soybean phospholipid bilayer. The voltage dependence of the single channel conductance, which is different for charged and neutral lipid bilayers, can be described either by a two-state flicker (2SF) model and the Nernst-Planck continuum theory, or by a two barrier, one-site (2B1S) model with asymmetric barriers. The increase in the number of open channels after a voltage jump from 50 mV to 150 mV has a time constant of 0.8 s. The changes of the single-channel conductance are much faster (<1 ms). The electric part of the gating process is characterized by the (reversible) molar electrical work ΔG^θ_el = ρZ_gFV_m ≈ -1.3 RT, which corresponds to the movement of one charge of the gating charge number |Z_g| = 1 across the fraction ρ = ΔV_m/V_m = 0.15 of the membrane voltage V_m = 200 mV. Unlike with chloride, the single channel conductance of fluoride has a maximum at about 150 mV in the presence of the buffer PIPES (≥5 mM, pH 6.8) with K_0.5 ≈ 1 M. It is shown that the decrease in conductance is due to a blocking of the channel by the PIPES anion. In summary, the results indicate that the anion transport by the Clavibacter anion channel (CAC) does not require a voltage dependent conformation change of the CAC.     

Transmembrane potential measurements on plant cells using the voltage-sensitive dye ANNINE-6

The charging of the plasma membrane is a necessary condition for the generation of an electric-field-induced permeability increase of the plasmalemma, which is usually explained by the creation and the growth of aqueous pores. For cells suspended in physiological buffers, the time domain of membrane charging is in the submicrosecond range. Systematic measurements using Nicotiana tabacum L. cv. Bright Yellow 2 (BY-2) protoplasts stained with the fast voltage-sensitive fluorescence dye ANNINE-6 have been performed using a pulsed laser fluorescence microscopy setup with a time resolution of 5 ns. A clear saturation of the membrane voltage could be measured, caused by a strong membrane permeability increase, commonly explained by enhanced pore formation, which prevents further membrane charging by external electric field exposure. The field strength dependence of the protoplast’s transmembrane potential V _M shows strong asymmetric saturation characteristics due to the high resting potential of the plants plasmalemma. At the pole of the hyperpolarized hemisphere of the cell, saturation starts at an external field strength of 0.3 kV/cm, resulting in a measured transmembrane voltage shift of ?V _M?=??150 mV, while on the cathodic (depolarized) cell pole, the threshold for enhanced pore formation is reached at a field strength of approximately 1.0 kV/cm and ?V _M?=?450 mV, respectively. From this asymmetry of the measured maximum membrane voltage shifts, the resting potential of BY-2 protoplasts at the given experimental conditions can be determined to V _R?=??150 mV. Consequently, a strong membrane permeability increase occurs when the membrane voltage diverges |V _M|?=?300 mV from the resting potential of the protoplast. The largest membrane voltage change at a given external electric field occurs at the cell poles. The azimuthal dependence of the transmembrane potential, measured in angular intervals of 10° along the circumference of the cell, shows a flattening and a slight decrease at higher fields at the pole region due to enhanced pore formation. Additionally, at the hyperpolarized cell pole, a polarization reversal could be observed at an external field range around 1.0 kV/cm. This behavior might be attributed to a fast charge transfer through the membrane at the hyperpolarized pole, e.g., by voltage-gated channels.     

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.     

Electrical characteristics of the apical and basal-lateral membranes in the turtle bladder epithelial cell layer

(1) The active transport of Na⁺ across the turtle bladder epithelial cell layer consists of a passive entry step through a Na⁺-selective path in the apical membrane and an active extrusion step through Na⁺ pump-containing path in the basal-lateral membrane together with some back-leakage through the paracellular spaces and tight junctions between the epithelial cells. This hypothesis has now been verified qualitatively and to some extent, quantitatively by the use of an intracellularly-located microelectrode in conjunction with a conventional assembly of extracellularly-located macroelectrodes mainly in short-circuited bladders bathed by Na⁺-rich Ringer media. Under these conditions, the intracellular potential (V_sc) averaged 38.4 mV with the cell electronegative; the fractional resistance of the apical membrane ($\text{?R}{}_{\mathrm{<mtext>a</mtext>}}$) averaged 0.55; while the concomitant transepithelial parameters, short circuiting current (I_sc) and electrical conductance (G_t), average 68.6 μA/cm² and 0.98 mS/cm², respectively. (2) The relation between these parameters and the transepithelial flow of Na⁺ (orI_sc) is evoked by blocking Na⁺ entry into the cell (by the mucosal addition of amiloride or removal of mucosal Na⁺). Amiloride-induced blockade of the Na⁺ entry step results in a rapid hyperpolarization of the cell interior during which V_sc = —79.1 mV and $\text{?R}{}_{\mathrm{<mtext>a</mtext>}}\text{= 0.92}$. I_sc and G_t (equivalent to the shunt conductance under these conditions) averaged 5 μA/cm² and 0.35 mS/cm², respectively. The entire process is reversible on re-admission of Na⁺ entry into the cell. (3) A slow depolarization of the cell interior in the period of blocked transapical Na⁺ entry is opposite to that expected from an electroneutral Na⁺-K⁺ exchanging pump; but instead is the predictable response of an electrogenic Na⁺ pump in parallel with a passive K⁺-selective conductance in the basal-lateral membrane. (4) The electrogenicity concept is substantiated after pretreatment of the bladder with serosal ouabain, which changes the response of V_sc to amiloride (from the aforementioned biphasic response) to a step-function response, attributable mainly to the development of a slowly dissipating K⁺ diffusion potential across the basallateral membrane. (5) Under open-circuit conditions, the electronegativity of cell to mucosa (V_a) is a linear inverse function of the electropositivity of serosa to mucosa (V_t). For V_t ? 100 mV, V_a is positive; and for V_t between ?30 and 90 mV, V_a is negative.     

The electrogenic sodium pump of the frog retinal pigment epithelium

Summary It was previously shown that ouabain decreases the potential difference across anin vitro preparation of bullfrog retinal pigment epithelium (RPE) when applied to the apical, but not the basal, membrane and that the net basal-to-apical Na⁺ transport is also inhibited by apical ouabain. This suggested the presence of a Na⁺–K⁺ pump on the apical membrane of the RPE. In the present experiments, intracellular recordings from RPE cells show that this pump is electrogenic and contributes approximately –10 mV to the apical membrane potential (V _AP). Apical ouabain depolarizedV _AP in two phases. The initial, fast phase was due to the removal of the direct, electrogenic component. In the first one minute of the response to ouabain,V _AP depolarized at an average rate of 4.4±0.42 mV/min (n=10, mean ±sem), andV _AP depolarized an average of 9.6±0.5 mV during the entire fast phase. A slow phase of membrane depolarization, due to ionic gradients running down across both membranes, continued for hours at a much slower rate, 0.4 mV/min. Using a simple diffusion model and K⁺-specific microelectrodes, it was possible to infer that the onset of the ouabain-induced depolarization coincided with the arrival of ouabain molecules at the apical membrane. This result must occur if ouabain affects an electrogenic pump. Other metabolic inhibitors, such as DNP and cold, also produced a fast depolarization of the apical membrane. For a decrease in temperature of 10°C, the average depolarization of the apical membrane was 7.1±3.4 mV (n=5) and the average decrease in transepithelial potential was 3.9±0.3 mV (n=10). These changes in potential were much larger than could be explained by the effect of temperature on anRT/F electrodiffusion factor. Cooling the tissue inhibited the same mechanism as ouabain, since prior exposure to ouabain greatly reduced the magnitude of the cold effect. Bathing the tissue in 0mm [K⁺] solution for 2 hr inhibited the electrogenic pump, and subsequent re-introduction of 2mm [K⁺] solution produced a rapid membrane hyperpolarization. We conclude that the electrogenic nature of this pump is important to retinal function, since its contribution to the apical membrane potential is likely to affect the transport of ions, metabolites, and fluid across the RPE.     

Bumetanide Hyperpolarizes Madin–Darby Canine Kidney Cells and Enhances Cellular Gentamicin Uptake by Elevating Cytosolic Ca2+ Thus Facilitating Intermediate Conductance Ca2+-Activated Potassium Channels

Loop diuretics such as bumetanide and furosemide enhance aminoglycoside ototoxicity when co-administered to patients and animal models. The underlying mechanism(s) is poorly understood. We investigated the effect of these diuretics on cellular uptake of aminoglycosides, using Texas Red-tagged gentamicin (GTTR), and intracellular/whole-cell recordings of Madin–Darby canine kidney (MDCK) cells. We found that bumetanide and furosemide dose-dependently enhanced cytoplasmic GTTR fluorescence by ~60 %. This enhancement was suppressed by La³⁺, a non-selective cation channel (NSCC) blocker, and by K⁺ channel blockers Ba²⁺ and clotrimazole, but not by tetraethylammonium (TEA), 4-aminopyridine (4-AP) or glipizide, nor by Cl^? channel blockers diphenylamine-2-carboxylic acid (DPC), niflumic acid (NFA), and CFTR_inh-172. Bumetanide and furosemide hyperpolarized MDCK cells by ~14 mV, increased whole-cell I/V slope conductance; the bumetanide-induced net current I/V showed a reversal potential (V _r) ~?80 mV. Bumetanide-induced hyperpolarization and I/V change was suppressed by Ba²⁺ or clotrimazole, and absent in elevated [Ca²⁺]_i, but was not affected by apamin, 4-AP, TEA, glipizide, DPC, NFA, or CFTR_inh-172. Bumetanide and furosemide stimulated a surge of Fluo-4-indicated cytosolic Ca²⁺. Ba²⁺ and clotrimazole alone depolarized cells by ~18 mV and reduced I/V slope with a net current V _r near ?85 mV, and reduced GTTR uptake by ~20 %. La³⁺ alone hyperpolarized the cells by ~?14 mV, reduced the I/V slope with a net current V _r near ?10 mV, and inhibited GTTR uptake by ~50 %. In the presence of La³⁺, bumetanide-caused negligible change in potential or I/V. We conclude that NSCCs constitute a major cell entry pathway for cationic aminoglycosides; bumetanide enhances aminoglycoside uptake by hyperpolarizing cells that increases the cation influx driving force; and bumetanide-induced hyperpolarization is caused by elevating intracellular Ca²⁺ and thus facilitating activation of the intermediate conductance Ca²⁺-activated K⁺ channels.     

A study of the current-voltage relationships of electrogenetic active and passive membrane elements in riccia fluitans

Potassium- and proton-dependent membrane potential, conductance, and current-voltage characteristics (I–V curves) have been measured on rhizoid cells of the liverwort Riccia fluitans. The potential difference (E_m) measured with microelectrodes across plasmalemma and tonoplast is depolarized to the potassium-sensitive diffusion potential (E_D) in the presence of 1 mM NaCN, 1 mM NaN₃, or at temperatures below 6°C. Whereas the temperature change from 25°C to 5°C decreases the membrane conductance (g_m) from 0.71 to 0.43 S ? m^?2, 1 mM NaCN increases g_m by about 25%. The membrane displays potassium-controlled rectification which gradually disappears at temperatures below 5°C. The potassium pathway can be described by an equivalent circuit of a diode and an ohmic resistor in parallel. In the potential interval of E_D ± 100 mV the measured I-V curves roughly fit the theoretical curves obtained from a modified diode equation. ⁸⁶Rb⁺(K⁺)-influx is voltage sensitive: In the presence of 1 mM NaCN, ⁸⁶Rb⁺-influx follows a hyperbolic function corresponding to a low conductance at low [K⁺]_o and high conductance at high [K⁺]_o. On the contrary ⁸⁶Rb⁺-influx is linear with [K⁺]_o when pump activity is normal. It is believed that there are two K⁺-transport pathways in the Riccia membrane, one of which is assigned to the low conductance (0.2 S · m^?2), the other to a temperature-dependent facilitated diffusion system with a higher conductance (7.7 S · m^?2). The electrogenic pump essentially acts as a current source and consumes about 39% of the cellular ATP-turnover. In the presence of 30 μM CCCP the saturation current of 0.1 A · m^?2 is doubled to about 0.2 A · m^?2, and the electromotive force of ?360 mV switches to ?250 mV. It is suggested that this may be due to a change in stoichiometry from one to two transported charges per ATP hydrolyzed.     

High-conductance K+ channel in pancreatic islet cells can be activated and inactivated by internal calcium

Summary The Ca²⁺-activated K⁺ channel in rat pancreatic islet cells has been studied using patch-clamp single-channel current recording in excised inside-out and outside-out membrane patches. In membrane patches exposed to quasi-physiological cation gradients (Na⁺ outside, K⁺ inside) large outward current steps were observed when the membrane was depolarized. The single-channel current voltage (I/V) relationship showed outward rectification and the null potential was more negative than –40 mV. In symmetrical K⁺-rich solutions the single-channelI/V relationship was linear, the null potential was 0 mV and the singlechannel conductance was about 250 pS. Membrane depolarization evoked channel opening also when the inside of the membrane was exposed to a Ca²⁺-free solution containing 2mm EGTA, but large positive membrane potentials (70 to 80 mV) were required in order to obtain open-state probabilities (P) above 0.1. Raising the free Ca²⁺ concentration in contact with the membrane inside ([Ca²⁺]_i) to 1.5×10^–7 m had little effect on the relationship between membrane potential andP. When [Ca²⁺]_i was increased to 3×10^–7 m and 6×10^–7 m smaller potential changes were required to open the channels. Increasing [Ca²⁺]_i further to 8×10^–7 m again activated the channels, but the relationship between membrane potential andP was complex. Changing the membrane potential from –50 mV to +20 mV increasedP from near 0 to 0.6 but further polarization to +50 mV decreasedP to about 0.2. The pattern of voltage activation and inactivation was even more pronounced at [Ca²⁺]_i=1 and 2 m. In this situation a membrane potential change from –70 to +20 mV increasedP from near 0 to about 0.7 but further polarization to +80 mV reducedP to less than 0.1. The high-conductance K⁺ channel in rat pancreatic islet cells is remarkably sensitive to changes in [Ca²⁺]_i within the range 0.1 to 1 m which suggests a physiological role for this channel in regulating the membrane potential and Ca²⁺ influx through voltage-activated Ca²⁺ channels.     

Voltage dependent potassium fluxes and the significance of action potentials in Acetabularia

Membrane potential, V_m, and K⁺(⁸⁶Rb⁺) fluxes have been measured simultaneously on individual cells of Acetabularia mediterranea. During resting state (resting potential approx. ?170 mV) the K⁺ influx amounts to 0.24–0.6 pmol · cm^?2 · s^?1 and the K⁺ efflux to 0.2–1.5 pmol · cm^?2 s^?1. According to the K⁺ concentrations inside and outside the cell (40 : 1) the voltage dependent K⁺ flux (zero at V_m = E_K = ?90 mV) is stimulated approx. 40-fold for V_m more positive than E_K.It is calculated that during one action potential (temporary depolarization to V_m more positive than E_K) a cell looses the same amount of K⁺, which leaks in during 10–20 min in the resting state (V_m = ?170 mV). Since action potentials occur spontaneously in Acetabularia, they are therefore suggested to have a significant function for the K⁺ balance of this alga.     

Amplification of small signals by voltage-gated sodium channels in drone photoreceptors

Summary Photoreceptor cells of the drone,Apismellifera , have a voltage-gated Na⁺ membrane conductance that can be blocked by tetrodotoxin (TTX) and generates an action potential on abrupt depolarization: an action potential is triggered by the rising phase of a receptor potential evoked by an intense light flash (Autrum and von Zwehl 1964; Baumann 1968). We measured the intracellular voltage response to a small (9%), brief (30 ms) decrease in light intensity from a background, and found that its amplitude was decreased by 1M TTX. The response amplitude was maximal when the background intensity depolarized the cell to –38 mV. With intensities depolarizing the cell membrane to –45 to –33 mV the average response amplitude was decreased by TTX from 1.2mV to 0.5mV. TTX is also known to decrease the voltage noise during steady illumination (Ferraro et al. 1983) but, despite this, the ratio of peak-to-peak signal to noise was, on average, decreased by TTX. The results suggest that drone photoreceptors use voltage-gated Na⁺ channels for graded amplification of responses to small, rapid changes in light intensity.Abbreviations TTX tetrodotoxin - V _i intracellular potential with respect to the bath - V _o extracellular potential - V _m,V _i-V _o approximate transmembrane potential - S amplitude of the voltage response to an 8.9% decrease in light intensity - N voltage noise, usually measured as root mean square voltage deviation as described in Methods     

Intracellular Ca(2+) oscillations induced by over-expressed Ca(V)3.1 T-type Ca(2+) channels in NG108-15 cells

T-type Ca²⁺ channel family includes three subunits Ca_V3.1, Ca_V3.2 and Ca_V3.3 and have been shown to control burst firing and intracellular Ca²⁺ concentration ([Ca²⁺]_i) in neurons. Here, we investigated whether Ca_V3.1 channels could generate a pacemaker current and contribute to cell excitability. Ca_V3.1 clones were over-expressed in the neuronal cell line NG108-15. Ca_V3.1 channel expression induced repetitive action potentials, generating spontaneous membrane potential oscillations (MPOs) and concomitant [Ca²⁺]_i oscillations. These oscillations were inhibited by T-type channels antagonists and were present only if the membrane potential was around −61 mV. [Ca²⁺]_i oscillations were critically dependent on Ca²⁺ influx through Ca_V3.1 channels and did not involve Ca²⁺ release from the endoplasmic reticulum. The waveform and frequency of the MPOs are constrained by electrophysiological properties of the Ca_V3.1 channels. The trigger of the oscillations was the Ca_V3.1 window current. This current induced continuous [Ca²⁺]_i increase at −60 mV that depolarized the cells and triggered MPOs. Shifting the Ca_V3.1 window current potential range by increasing the external Ca²⁺ concentration resulted in a corresponding shift of the MPOs threshold. The hyperpolarization-activated cation current (I_h) was not required to induce MPOs, but when expressed together with Ca_V3.1 channels, it broadened the membrane potential range over which MPOs were observed. Overall, the data demonstrate that the Ca_V3.1 window current is critical in triggering intrinsic electrical and [Ca²⁺]_i oscillations.     

Leak Current Rectification in Myxicola Giant Axons : Constant field and constant conductance components

Early leak current, i.e. for times similar to the time to peak of the transient current was measured in Myxicola giant axons in the presence of tetrodotoxin. The leak current-voltage relation rectifies, showing more current for strong depolarizing pulses than expected from symmetry around the holding potential. A satisfactory practical approximation for most leak corrections is constant resting conductance. The leak current-voltage curve rectifies less than expected from the constant field equation. These curves cannot be reconstructed by summing the constant field currents for sodium and potassium using a P_Na/P_K ratio obtained in the usual way, from zero current constant field fits to resting membrane potential data. Nor can they be reconstructed by summing the constant field current for potassium with that for any other single ion. They can be reconstructed, however, by summing the constant field current for potassium with a constant conductance component. It is concluded that the leak current and the resting membrane potential, therefore, are determined by multiple ionic components, at least three and possibly many. Arguments are presented suggesting that ion permeability ratios obtained in the usual way, by fitting the constant field equation to resting membrane potential data should be viewed with skepticism.     

The ionic basis of the resting potential of molluscan unstriated muscle

Summary The membrane potential (Vm) of unstriated, non-spiking fibres from the buccal retractor muscle of the opisthobranch molluscPhiline aperta is primarily determined by the distribution of the potassium ion across the membrane. In salines where potassium is varied and chloride remains constant or nearly so, the membrane potential varied with log external K⁺ with a slope of 50.6 (±2.3) mV per decade. In chloride-free salines the slope was 48.5 mV per decade. The experiments were conducted at temperatures of 18–20° C.A ten-fold reduction in external chloride concentration depolarised the fibres by around 10 mV, indicating that chloride permeability makes some contribution to Vm. In salines where [K]₀·[Cl]₀ is constant the Nernst slope was 55.8 mV per decade compared with the theoretical value of 58 mV.The experimental data suggest that the internal potassium concentration of the fibres is 247±31 mM and pNa/pK is 0.01, giving a predicted value of Vm in sea water of –72 mV. The membrane potential of 90 fibres measured in sea water was –74.2±1.3 mV. The membrane contains an electrogenic sodium pump which contributes 4–5 mV to the membrane potential.